C9 *> 8 1 \ ' «\ Vi, '„ ^ W o_ ^ v* ^ ' V ■0. '**<$ 0> ^ s ■ ^ v^ .I ■{ .0 0. 'V v- \V , ^ &S * c_ oo x » . \ «***. * t^HL^ This Book is the property of the General Electric Company and must be returned to the Assistant General Foreman when you leave the Testing Department. No. Instructions FOR Testing Electrical Apparatus Copyright 1914 by General Electric Company GENERAL ELECTRIC COMPANY TESTING DEPARTMENT SCHENECTADY, N. Y. 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The result of these three angular changes is a change in the phase relation in the watt- meter. The total change rarely exceeds 2 degrees, and is fre- quently less than 30 minutes. At or near unity power-factor its effect on the reading is inappreciable; but at a very low power- factor large errors may result. Correction for Phase Angle Correction of wattmeter readings for errors due to phase angle of wattmeter, current transformers, and potential trans- formers, may be made as follows: — A — Single-phase circuits. (1) Correct all instruments for scale error. (2) Obtain a, the equivalent phase angle of the wattmeter, from the certificate. (This is very small for the P and P3 watt- meters, and can usually be neglected.) (3) Select £, the phase angle between the primary and (reversed) secondary currents of the current transformer, from the certificate, using the reading of the ammeter in series with the wattmeter. (4) Select 7, the phase angle between the primary and (reversed) secondary voltages of the potential transformer from the certificate, using the reading of the voltmeter in parallel with the wattmeter. (5) Determine cos 2 , the apparent power-factor from the readings of the ammeter, voltmeter and wattmeter (corrected according to Xo. 1) by the formula ^ , . Watts Power-factor = — - w volts X amperes (6) Add algebraically a, /3 and 7, using the signs as given in the certificates. (7) Select the correction factor from Tables 1 or 2. In these tables a series of values of ( a-\-(5-\-y) is given in the left hand column; in the first line across the top of the columns is given a set of values of the apparent power-factor (cos 02-) The correction factor is found in the column under the proper apparent power-factor in line across the page from the proper value of ( a +0+7). For values lying between those given in the tables, interpolation will give sufficient accuracy for most cases. Table 1 should be used when ( a + +7) is a positive angle and the power-factor of the circuit supplying the wattmeter is lagging, or when ( a +/3 +7) is a negative angle and the power- factor of the circuit is leading. Table 2 should be used when ( a +/3 +7) is a positive angle and the power-factor is leading, or when ( a +/3 +7) is a negative angle and the power-factor is lagging. (8) True watts = wattmeter reading corrected according to (1) X certified ratio of current transformers X certified ratio of potential transformer X correction factor for phase angle. 55 If the greatest accuracy or values outside the limits of the table are required, the following method may be used: Follow (1), (2), (3), (4) and (5) as given herewith. If cos 6 represents the true power-factor of the circuit, being considered a positive angle for lagging current and a negative angle for lead- ing current, 0=02 + (a+/3+ 7 ) Then True watts = wattmeter reading corrected according to (1) X certified ratio of current transformer X certified ratio of potential transformer X — cos 6 2 — is the correction factor given in Tables 1 and 2. Co$ 02 s B — Three-phase three-wire circuits with currents and voltages balanced. When two wattmeters or a polyphase wattmeter are used with similar current transformers whose secondaries are equally loaded and not interconnected the total watt reading may be corrected for phase angle by the same method as on single-phase, using the apparent power-factor of the three-phase circuit which is Total wattmeter reading 3 X volts (delta) X amperes of one line instrument corrections being applied as per (1). C — Other polyphase circuits. On three-phase four-wire circuits, three-phase three-wire circuits, whose currents or voltages are unbalanced, and two- phase circuits each wattmeter should be treated as a separate single-phase instrument obtaining the apparent power-factor from its reading and of the voltmeter and ammeter in the same phase, consequently using a different correction factor for each wattmeter. On a three-phase three-wire circuit using the two- wattmeter method, it should be noted that the current is fre- quently leading in one wattmeter and lagging in the other. MEASUREMENT OF POWER-FACTOR Watts The power-factor of a single-phase circuit = . , b ^ volts X amps. It is usually obtained by using the readings of the voltmeter, ammeter and wattmeter. In a balanced three-phase circuit, the power-factor may be obtained from the two wattmeter readings. If a is the phase angle, the power-factor = cos a, and R is the ratio of the smaller to the greater wattmeter reading, Tana=—~y/3 56 The principle of the General Electric Company balanced three-phase power-factor meter uses this fact. The elements are so combined into one instrument that the position of the pointer depends on the ratio of the watts. The instrument is quite accurate, and independent of frequency. The volt-amperes in a balanced three-phase circuit are equal to the product of the amperes per line, the volts between lines, and the square root of three. 57 CHAPTER 3 ASSEMBLY OF MACHINES FOR TEST HANDLING MATERIAL When erecting large apparatus for test, methods of handling and transportation are of prime importance. Each piece of apparatus must of course be handled with reference to its special construction. Practically all of the handling of the larger machines and parts is done by the crane men and crane followers, but each test man should become familiar with the correct methods of handling such material and see that such work is carried on in the approved manner. There is a great difference between ropes and slings used for hoisting. In ropes the wear can always be seen by the strands becoming frayed, loose, or cut. A chain, except for a few bruises, will not show any signs of weakness, even though, at the same time, it may be full of small cracks which cannot be seen by the naked eye, or it may be much crystallized by long use. Care should be used in every case to see that satisfactory slings and ropes are used to lift apparatus. There are many varieties of hitches and knots, some of which are shown on the following pages. Wire cable slings occupy a very important place in hoisting and have been found very satisfactory when carefully used. In using slings of any kind care should be taken to see that one section does not lie on top of another and thus put an undue strain on the outer section. It often happens when a rope sling is used double that the ends of the rope are passed through the double part. Unless this is done carefully the effect of only one part will be obtained instead of two. Increased Stresses Due to Angle of Slings When a weight is lifted by two or more slings connected to the crane hook and making an angle with each other, the increase in the stress of the individual slings must be considered. On account of this angle between the two sets of slings the stresses on each set is greater than half the total load, and increases very rapidly as the angle between the sling and the work is decreased. An angle of 45 degrees between the sling and the work makes the stress in each sling % of the total weight, and the collapsing force between the two points of attachment to the work is equal to Yi the weight. This collapsing force acts in a direct line between the two points of attachment. If the work is ring shaped, it would tend to deform the ring. A spreader of suffi- cient stiffness should be used between these two points to resist this collapsing force. It will be seen that eyebolts are not suitable for attaching the slings to the work unless a spreader is used to relieve them of this side pull, which would put a heavy bending moment on the shank of the bolt. 58 Reducing the angle between the sling and the work to 30 degrees makes the stress in each sling equal to the total weight and the collapsing force is also equal to the total weight. Such a small angle should never be used if avoidable. The following tables show how the safe load becomes very much smaller when the slings are used at an angle instead of a straight pull. SAFE LOAD IN LB. ON MANILA ROPES AND SLINGS Two Part Sl/ng Two Part Sling Two Port Sling Two Port Si in g Rope i i A Diam. / \ y/\ in In. / \ / \ ^^\^ Vertical Looc/ 60° Angle 45"Ang/e xn"Angle> V?. 500 435 355 250 % 1000 870 710 500 Vx 1500 1300 1065 750 V* 2000 1750 1420 1000 1 3000 2600 2125 1500 IK 4000 3475 2830 2000 IV? 5000 4340 3540 2500 1U 8000 6940 5665 4000 2 10000 8680 7080 5000 2H 13000 11285 9200 6500 2V 2 16000 14880 11325 8000 SAFE LOAD IN LB. ON WIRE CABLE OR SLINGS Two Port Sling Two Part Sling Two Part Sling Two Port Sling Wire i i A Cable Diam. in In. A /\ /^ Vertical Load 60 "Angle 45°Angre 30°Angle V?, 4000 3470 2830 2000 % 6500 5625 4590 3250 u 9000 7800 6350 4500 Vh 12000 10400 8500 6000 1 16000 13870 1 1300 8000 IK 24000 20800 17000 12000 iy 2 38000 32900 26900 19000 w 50000 43300 35300 25000 2 64000 55500 45250 32000 59 SAFE LOADS FOR EYEBOLTS When it is necessary to use eyebolts for lifting loads no greater strain should be allowed than given in the table on page 61, which gives the safe load in pounds up to and including bolts 2 3^ in. in diameter. It should be understood that to obtain the greatest strength from an eyebolt, it must fit reasonably tight in the hole into which it is screwed, and the pull applied in a line with the axis of the screw. Eyebolts should never be used if considered the least faulty. They should never be painted when used for miscellaneous lifting, as paint is very apt to cover up flaws. They should be tested occasionally by tapping gently with a hammer but not sufficient to bend or to otherwise injure them. If it does not impart a good ring one of two things is the reason. It may fit too loosely in the hole, or there may be a flaw. Where a bolt is to be used for anything like its maximum load it should be screwed in tight with a bar and given a gentle tap with a bar or hammer to see if it imparts a solid feeling. If not, it should not be used. The strains set up in an eyebolt when used at an angle are very severe, due to the bending action of the bolt, and it is very liable to break where it is screwed into the work. This is shown very clearly by the table on page 61, that gives the safe load when used for a direct pull, and also shows how the strength of the bolt rapidly decreases according to the angle that may be used. SAFE LOAD ON ROPES AND CHAINS The tables on page 62 give the safe loads which may be put on manila rope, wire cables, and chains. The first column gives the diameter of the rope or chain, the second column gives the safe load which the rope or chain is to carry singly. In a sling where the strain is carried by two ropes or chains, the load given in third column should be used. In a sling where four parts of the rope or chain carry the load, the figures in the fourth column should be used. Figures are in tons of 2000 lb. each. The figures given in the above table are for cases in which the slings are in constant use and subjected to ordinary shop practice. Where cables of known high tensile strength are used these figures may be increased proportionately. The loads for manila rope should be used only when the rope is in fairly good condition; when badly chafed or worn the load should be reduced in proportion. As there are a great many different kinds of material to handle in the various parts of the Works, and in order to familiarize those engaged in the actual handling of these materials, a short table of the weights of the various materials is given on page 62. The weights of cast iron, steel, copper and lead are given in pounds per cubic foot. The weights of wood, concrete, stone, earth, brick, mortar and marble are also given in pounds per cubic foot. The weight of shafts is given per lineal foot. 60 H H N «1 IC OC r- — lOiOlOXOCCOOO i-i (N C^ LC I> O tJ- IV) - OOOOOOOOOO - ' .£ * OOOOOOOOOO ™ n -r .&<; -"H^xCXNOh t ^ ^ ^ * f S ) 4r^ ^5 / > i ?* / s <*> / $ / x . O /O eo 30 40 SO GO 70 30 £>0 /00 Pressure /6s. £>. pe/~s0 N £V0 400 £0O dOO /OOO0PO /600 2000 Rubbing Speed in feet per minute Fig. 43 SAFE MAXIMUM PRESSURE ON BEARINGS FOR EACH SPEED not dip into it. If this instruction is observed satisfactory lubrication will be obtained for all ordinary bearing pressures and rubbing speeds. For high bearing pressures, or high speeds, some form of forced lubrication is used. The oil is forced into the bearing either on the bottom, or the lower quarter and enters the bearing at a point such that the revolving shaft draws the oil under the shaft. Oil from forced lubricated bear- ings is usually returned to an external cooling tank, where its temperature is reduced before being again pumped into the bearing. Oil rings and forced lubrication are occasionally used on the same bearings, so that if the oil pressure fails the rings supply enough oil to prevent danger, until the oil pres- sure can be restored. A properly designed bearing may run hot from the following causes: Oil rings sticking; scarcity or poor quality of lubricating oil; excessive local pressure in the bearing; insufficient relief on the sides of the bearings; improper alignment and exces- sive belt pull, or current flowing from frame to shaft. The remedy for the greater part of these troubles is obvious. In the case of excessive local pressure in the bearing, or insuffi- 86 cient relief on the side of the bearing, the remedy is to remove the high spots on the babbitt or bearing metal with a scraper and increase the side clearance. Allowable bearing pressures, speeds, etc., are given in Figs. 41, 42 and 43. Before starting a machine all bearings must be filled with the proper amount of oil. Bearings should be inspected to see the}* have not been carelessly filled, viz., that oil has not been spilled on the bearing housing, or bearing shell, or upon other parts associated with the bearing, otherwise, a false impression may be obtained as to oil leakage or throwing when under test. To give the bearing a critical test for oil leaking Fig. 44 TYPES OF OIL GAUGES or throwing, the dividing line between cap and bearing pedestal and between bearing brackets, should be painted with whit- ing. The end of the commutator or field spider adjacent to the bearing should also be given a white coating, so that it is possible to detect, after a comparatively short run, the slightest leakage or throwing of oil. Bearings with the end of the bearing shell visible should be filled with oil until it touches the lower part of the shell at the end of the bearing housing. Where the end of the bearing shell cannot be seen the bearing should be filled to within Y% in. of the top of the visible portion of the oil gauge glass; in the case of sight gauges to within 3^8 in. of the top of the gauge. In the case of overflow gauges having no glass, a record of the distance of the oil level from the top of the gauge must be made, in every case, upon the Testing Record. Gauges with glass tubes so placed as to show the oil level (Fig. 44a) are used on bearings of large machines, and stand pipe gauges (Fig. 44b) on small and medium size machines. Overflow gauges (Fig. 44c) are those with the top of the stand pipe fitted with a hinged cap. Oil gauges on most induction motors are of the overflow type, and should be filled to within tV in. of the overflow. As 87 already stated, no oil must be spilled upon the bearing parts. In filling bearings a funnel must be used and the oil inserted through the sight holes for the oil rings, or through the opening above the shaft at the end of the bearing housing. During test no oil should be allowed to leak or be thrown from the bearings upon the rotating parts, or windings. This is especially true with reference to commutating machines, where it is important that lubricating oil be kept away from the commutator, brushes and fittings. Should oil-leaking or throwing on these parts be detected during the test, the test should immediately be discontinued and the cause of leakage removed. If bearings under test rise in temperature 40 degrees cent, or more, above the room temperature, it should be reported to the office as a defect, since no properly designed bearing should heat above 40 degrees rise under normal conditions. It will usually be found that a greater temperature rise is due to a faulty bearing. Thrust Bearings There are two classes of thrust bearings; those which depend upon a film of oil between two flat plates, and those which have either hardened rollers or balls rolling between two hardened surfaces. The first class may be sub-divided into (a) those which are supplied with oil under pressure and (b) those which revolve in a bath of oil. In both these classes the bottom plate is stationary and the top one rotates with the shaft. In the pressure thrust bearing the two plates are recessed for about half their diameter and the remaining annular ring is scraped or ground to a true surface. Scraping is perhaps pref- erable to grinding as in a ground plate there is a possibility of particles of the abrasive becoming imbedded in the surfaces and causing them to cut. The bottom plate usually rests upon a spherical surface which allows the plates to align themselves in their proper relative positions. The oil is led from the pump or accumulator to the recess between the plates and the pressure raised until the plates separate and the oil passes out between the plates and up along the shaft to the overflow where it escapes and returns to the pump or cooling tank. It is obvious that the pressure per sq. in. required to separate the plates is a function of the superincumbent weight and the area of the bearing plates. The limit of allowable pressure per sq. in. on this type of bearing is the capacity of the pumps or accumulator, as the friction is purely fluid friction and the plates do not come in contact with each other. If an accumulator is not used it is necessary to interpose between the pump and the thrust bearing some form of baffler which will cause a back pressure on the pump above that required to separate the plates of the thrust bearing. This difference in pressure between the two sides of the baffler should be from 25 to 40 per cent of the pressure required to lift the plates. For example; if it requires 1000 lb. per sq. in. to separate the plates, the pump should show a pressure of from 1250 to 1400 lb. per sq. in._ This insures a uniform flow of oil through the plates, which condition is 88 absolutely necessary for correct operation of this class of thrust bearing. The amount of oil which should be passed through a pressure thrust bearing varies with the diameter of the plates and this amount in gallons should be about 100 per cent of the diam- eter of the plates in inches. Thus a 20 inch thrust bearing requires about 20 gallons per minute. In operating this kind of a thrust bearing some reserve source of oil pressure, such as a spare pump, should be at hand in case of the failure of the one in service. Both pumps should be on the line constantly and each pump should be capable of supplying the necessary amount of oil to the bearing. If one pump fails the other can carry the load while repairs are being made. A check valve should be placed in the line from each pump so that the oil cannot escape if a valve or some other vital part of the other pump should fail. The other style of plate bearing revolves in a bath of oil and is grooved in such a way that the top plate draws a film of oil between itself and the bottom plate. A type of thrust bearing of this kind is a segment bearing. The novel feature of this bearing is a series of adjustable surfaces mating with a continuous thrust collar. The parts carrying these adjustable surfaces are referred to as "shoes" or "segments" and are free to adjust themselves, thus bringing about uniform distribution of load over the entire bearing surface and, further, and more important, adjust themselves at a slight angle with the collar and thus glide or skim over the oil film which adheres to it. The "shoes" consist of heavy steel blocks faced with babbitt, their upper faces forming the adjustable bearing surfaces. Each "shoe" fits into a recess in the body casting and is mounted on a spherical topped block in contact with another spherical topped block below, which provide the adjustment to running conditions. Below each shoe seat is an adjustable wedge for raising and lowering to bring about a uniform distribution of load. Machines equipped with bearings of this type require a con- siderable amount of power to start, consequently, they are usually assembled in the Testing Department with a pressure step bearing underneath them so that they may be easily started. The "step-block" is then lowered until the machine is supported from the upper thrust bearing. Unusual care should be exercised in first starting bearings of this type and the machine should be brought to speed very slowly to be very certain that the bearing is operating properly. ROLLER BEARINGS The roller type of thrust bearing (see Fig. 45) consists of several hardened steel rollers held in a brass retainer and arranged radially to the shaft. The rollers revolve between hardened and ground steel plates, one of which is stationary and the other revolving with the shaft. In this form of bearing the oil is not ' 89 under pressure but must be supplied quite liberally. The oil must enter as close to the shaft as possible so that the centrifugal force may throw the oil out across the surface of the disks. Rapid starting of a new roller bearing often causes trouble by scoring or drawing the temper because the hardened steel plates as they come from the grinder are not in proper condition for a bearing surface. This trouble can be avoided by lapping the plates or by running several hours at slow speeds thus giving the plates a chance to smooth themselves. The amount of oil that should pass through a bearing of this type is very indefinite. Fig. 45 VERTICAL ROLLER THRUST BEARING The sole function of the oil is to keep the bearing cool and just what this amount may be for a particular bearing is hard to predict but will probably be from 10 to 14 gallons per minute on bearings up to 30 in. diameter. In any special case it is better to be guided by the advice obtained direct from the manu- facturers of the roller bearing in question. Roller bearings have been made as large as six feet across the disks and carry 2,500,000 lb. Balance of Rotating Parts Static Balance Rotating parts are usually balanced by putting them on a shaft and laying the shaft on two parallel rails called balance ways. The balance ways must be carefully leveled and well supported to prevent deflection from the weight of the piece to be balanced. After the correct amount of balance weight has been determined, a suitably formed weight is made and securely 90 fastened to the inside of the rim, or at a point at the same distance from the center as that at which the temporary weights were supported. The weights should be so fastened that they will not produce a shearing stress on the bolt or other fastening holding them in place. In revolving fields the weight should be placed on the inside of the rim. In this case the bolt has only to keep the weight from falling out when the machine is at rest. On d-c. armatures, pockets are generally provided into which melted lead is poured and hammered into place. On slow speed machines it is not necessary to get accurate balance, especially on heavy fields. On a 2000 or 3000 kw. field running about 120 rev. per min. an unbalanced weight of 50 lb. would probably not be noticed. Vertical machines must be more accurately balanced than horizontal ones. Dynamic Balance A field with good static balance will not necessarily be in good balance when running. It is often necessary to rebalance a rotor dynamically after the machine is assembled. The shaft must be straight before any balancing is done. This can be determined by holding a pointer or pencil to the shaft and revolving the shaft slowly. If the pointer touches all points, the shaft is straight and the work of balancing may proceed. If it does not touch all around, the shaft is sprung and must be straightened before the rotor is balanced. On very heavy rotors it is not possible to balance them statically as a whole, because their weight will press the shaft sufficiently into the ways to prevent the rotor from taking its natural position. In this case the parts are balanced separately as carefully as possible and the whole is afterwards dynamically balanced, if necessary. To locate roughly the position proper for balancing, hold a pencil or chalk so that the high side of the shaft strikes it as the shaft revolves at normal speed. On a rigid shaft this mark will indicate the heavy side, but on a flexible shaft it will prob- ably show the light side of the rotating part. Put some weight on the side opposite the mark and try again. If the balance is better, the weight is in the proper place and the mark will be found to extend further around the shaft. If the balance is worse, the weight is on the wrong side. If the mark is found to have moved, weight should be added at the new point. If the mark is found on just the opposite side, too much weight has been added. Pulleys Pulleys are made of various materials such as cast iron, steel, steel rims with cast iron centers, wood rims with cast iron centers, paper rims with cast iron centers, etc. Paper pulleys are in common use, especially in the smaller sizes and when not subjected to dampness, they are preferable to cast iron or steel on account of their higher coefficient of friction. Steel pulleys have the advantage over cast iron in that they will stand a higher speed, are much lighter and are not liable to 91 have hidden cracks or flaws. A pulley should be made with a bore of such size that it will go on the shaft without pressure and should be held in place with set screws. All pulleys, especially cast iron ones, should be rigidly inspected frequently for cracks or other flaws. A speed of 5000 ft. per min. produces a tensile stress of about 1200 lb. per sq. in., which is the usual working stress allowed for cast iron pulleys. There are men detailed in the Testing Department whose business it is to inspect all pulleys after they are put on machines and again before machines are started. The practice of having pulleys inspected each time before a machine is started, must be rigidly adhered to. It is very essential that the shaft extend clear through the hub of the pulley. This will give the pulley a maximum working strength and will insure its not coming off the machine while it is running. The set screws in these pulleys must be inspected to see that they are in good condition, that the threads are not damaged, and that they extend through the hub to the key in the shaft. Flange pulleys are cast iron pulleys with a steel center. These are readily adapted to any machine by first fitting a coupling to the shaft and then bolting this flange pulley to the coupling. New centers are readily obtained for these pulleys so that they may be easily kept in first class condition. It is good practice to operate pulleys between 4000 and 5000 ft. per min. When not in use, they must be placed in the store-house provided for that purpose. Belts Leather belts are much used in the Testing Department and a considerable amount of power is transmitted by them. In no case, however, should a belt carry more than 400 kw. When- ever possible, endless belts must be used, as they are stronger and do not cause fluctuations in the electrical instruments as do laced belts. Laced belts must be examined very carefully before starting a test to see that the lacings are in first class condition, and all belts must be inspected before being used to see that they are riveted properly and in no way defective. The size of belt to be used must be carefully calculated by the Head of Section, and in no case should it be left to the judgment of the shop men. The belts must never be wider than the pulley, nor be allowed to run with one end overlapping the edge of the pulley, as this will surely injure the belts. They should be run with the tight side on the bottom if possible, and must be kept free from oil as this reduces the capacity very much and causes slipping on the pulley. Quarter turns in belts must be avoided if possible as this stretches the belts on one side and greatly reduces their capacity. Under no conditions is a belt to be overloaded; if it breaks it may seriously damage apparatus or injure men working in the vicinity. Belts, must, therefore, be regarded as sources of danger and possible accident. When not in use they must be returned to the store-house where they will be inspected and repaired by a man employed for that purpose. Whenever belts are running near an aisle, or passage way, guards must be so placed that men cannot fall, be thrown, or 92 drawn into them. The testing tables should never be set in a line with a running belt and work should be so arranged that an employee must not work continuously in line with belts, unless proper mechanical guards are provided. Whenever a belt is found defective, it must be returned to the repair shop for repairs. HP KM 3e/t /6 20 24 28 32 36 W/'dth -2oly- 3p/y 44 48 32 36 60 64 68 72 76 80 inches 4-p/y 4« 3p/y ~ Fig. 46 WIDTH OF LEATHER BELTS Fig. 46 and the data on page 94 show the carrying capacity of leather belts of various widths and thicknesses "when running at speeds of from 1000 to 5000 ft. per minute. It is not per- missible to operate a belt in the Testing Department at a higher velocity than 5500 ft. per minute. When a belt is started for the first time it must be very carefully watched to see that it runs properly on the pulley, 93 and has the proper tension. Under no circumstances must an employee lean against, sit or stand upon, or pass through a belt even though it is not running. It is equally important that neither tools, nor articles of any description be laid upon belts after they are placed on the pulleys. DATA IN CONNECTION WITH WIDTH OF LEATHER BELTS The curves in Fig. 46 have been plotted from the following data: Coefficient of friction =0.4. Arc of contact = 165°. Weight of leather belting = 56 lb. per cubic foot. Centrifugal force =0.012 F 2 (with velocity in ft. per second.) 7\ = 1. T 2 =0.316. Ratio tight over slack side=-^- ■L 2 3.1643. Torque or pull = Ti- T 2 =0.684. Greatest tension = T x +0.012 F 2 . Average thickness per ply = tf in- Working tension per sq. in. =275 lb. for laced belting. H.p. or kw. per inch in width of f% in. thick. 1.05 1.56 2.03 2.46 2.855 3.18 3.447 3.63 3.73 .783 1.163 1.514 1.835 2.129 2.372 2.57 2.71 2.78 Width of Belt Up to 6 in. 6 in. to 20 in. 20 in. to 40 in. 40 in. to 60 in. 60 in. to 80 in. Up to 2 in. 2 in. to 5 in. 5 in. to 10 in. 10 in. to 36 in. Above 36 in. Up to 2 in. 2 in. to 5 in. 5 in. to 10 in. 10 in. to 24 in. 24 in. to 36 in. Above 36 in. for 1000 ft. per minute, for 1500 ft. per minute, for 2000 ft. per minute, for 2500 ft. per minute, for 3000 ft. per minute, for 3500 ft. per minute, for 4000 ft. per minute, for 4500 ft. per minute, for 5000 ft. per minute. Curves Plotted with the Following Thickness 1 ply belting varying from ^ in. to •& in. 2 ply belting varying from ^ in. to ^f in. 3 ply belting varying from -jjf in. to f| in. 4 ply belting varying from f| in. to §J in. 5 ply belting varying from f£ in. to l-^- in. Belts are to be Used in the Following Widths varying by \i in. varying by Yi in. varying by 1 in. varying by 2 in. varying by 4 in. Pulley Face to Exceed Width of Belt + h + y 2 + ^ 74 + 1 +iy 2 + 2 94 Before starting a test, the man responsible for the test must see that no one is in contact with the belt, and that nothing has been left lying upon it or where it may fall into it, while running. Truing Commutators The condition of a commutator determines to a great extent the satisfactory operation of the unit in service. A true periphery and a perfectly smooth surface are two requisites to satisfactory service. To secure these conditions is the aim of all commutator truing devices. There are two methods now recognized for truing commutators, viz., a turning tool and slide rest, sup- plemented by sandpaper, or some form of commutator grinder. In turning commutators some sort of a slide rest with a tool holder must be provided. In the Testing Department there are several sizes built on the same general plan, but differing principally in the length. The slide rest is held rigidly in such a position that the point of the tool is about on a level with the center of the commutator and movable parallel to the surface thereof. A very sharp diamond-point tool and a fine feed should be used. The cutting speed should be about 350 ft. per min. The end play must be eliminated by some means, usually by tying a board in such a position that it holds the armature securely against one oil deflector. After the commutator has been trued up as carefully as possible with the tool the final finish is obtained with either sandpaper or carborundum paper. Emery in any form should never be used because of the metallic particles which it contains. The objection to turning commutators is: first, that the cutting tool breaks the mica instead of cutting it; second, because of the different densities in mica and copper, the tool does not give a perfectly uniform surface and leaves the commutator bars a little higher in the center than on the edges; third, it is neces- sary to take a deep cut with the tool to get the required "bite" for cutting; fourth, the tool must be supplemented with sand- paper; fifth, the tool wears rapidly and must be replaced by another or re-ground during the process of turning. This is especially true when turning a commutator when the machine is run as a motor. When a tool is replaced in the middle of a cut it is difficult to prevent a score or a slight ridge being left where the new cut begins which can be removed only by taking another cut off the whole length of the commutator. This results in great waste of copper and decreases the life of the commutator. In truing a grooved commutator, that is, one from which the side mica has been cut out, it is very difficult to keep from carry- ing the copper across the slots when using a turning tool. This, of course, would necessitate cutting out the bridges of copper which on a commutator of any size means a considerable loss of time. The other, and perhaps the better method of truing com- mutators is with a commutator grinder. This consists essentially 95 of a small motor geared to a spindle which carries an abrasive wheel, the whole being carried on a slide rest similar to that used in turning commutators. The advantages of a commutator grinder over a turning tool are many; there is only one dis- advantage. The commutator can be ground with the machine running at normal speed and carrying full voltage. The grinder does not have to be so rigidly supported as the turning tool, and there is no danger of gouging the commutator as is the case with a turning tool. Grooved commutators can be ground with practically no bridging of the copper between bars. A com- mutator grinder can be installed, and the commutator ground without shutting down the machine. The commutator grinder produces an absolutely true surface from the fact that the grinding is done when the armature is running at normal speed. It is often the case that a commutator which runs true at slow speed will run eccentric at normal speed. Another important feature of the commutator grinder is the arrangement for catching all the copper dust. This consists essentially of a hood enclosing the grinding wheel leaving just enough opening for the wheel to come in contact with the commutator. A discharge pipe fitted with an ejector using compressed air produces a vacuum sufficient to draw all the chips away from the wheel and deposit them in a bag which is fastened to the end of the suction pipe. The disadvantage of a grinder is that it cannot remove copper as rapidly as a turning tool, and if the commutator has been allowed to become deeply grooved by the wear of the brushes, time would perhaps be saved by turning it, rather than grinding it. On the other hand, if the commutator is given the attention due it and attended to before the grooves become of appreciable depth, it will not only be better for the commutator to be ground, but it will prevent the necessity of removing a large amount of copper as would have to be done if the com- mutator were turned. Correcting End Play If a machine is properly leveled the rotor will revolve without rubbing either oil deflector when there is no field on the machine. If this is found to be the case, but that when field is put on the rotor pulls either one way or the other, it shows that the magnetic center of the field and armature do not lie in the same plane. This may be caused by the rotor being out of place on the shaft, or by the stator being out of its proper position on the base. It is evident that the defective end play may be corrected by moving either the rotor or frame. Whichever is found wrong should be made right, although perhaps it might be cheaper to move the stator than the rotor. The stators of the larger machines are not doweled till after the machines have been set up and tried out for both air gap and end play. If the machine were being installed outside where there were no facilities for pressing the shaft in or out of the rotor, the best 96 and certainly the cheapest way of correcting end play would be to move the frame on the base and redowel. If there is not sufficient clearance between the frame holding- down bolts and the holes in the feet, the holding-down bolts could have the body turned down as far as the depth of the thread, the reduced part being made of a length about Y± in. greater than the thickness of the foot and measured from the under side of the head. This will allow a much greater move- ment of the stator and w^ill not weaken the bolt if it is not reduced below the root of the thread. This method of correcting end play is sometimes used in the Testing Department, but after test the defect is always remedied by the shop, so that the proper position of the stator may be obtained without the use of the reduced bolts. 97 CHAPTER 4 PREPARATION OF APPARATUS FOR TEST ; INSPECTION; WIRING; OBSERVA- TIONS DURING OPERATION Preliminary Inspection It is the aim to have all apparatus delivered to the Testing Department from the manufacturing department in a completed condition including fittings and all other parts. When apparatus is delivered, the man in whose charge it has been placed should make a very careful inspection for mechanical defects and should see that all parts as assembled check with the Testing Instructions. The following are some defects which may appear: Copper bridges formed between the bars over the side mica of the com- mutator, due to improper turning; bent end conductor or com- mutator leads; improper brush staggering; damaged insulation of armature and field spools; broken insulating boards on fields; insufficient clearance between bare electrical terminals or conductors and ground; poor joints between electrical conductors; loose terminals; bus rings or other connections improperly sup- ported; brush pigtails too long or touching the armature risers; too little clearance between a brush stud or various parts of fittings and ground; incorrect spring pressure; defective spacing of collector ring taps; defective spacing of lubricating brushes, etc. It should be noted that laminated pole tips are not bent and that cast pole tips are of approximately uniform thickness on all the main poles of the machine. All oil rings in each bearing should be visible through the bearing cap oil cover and the bearings should be properly filled with oil as described on page 87. See that the brushes on collector rings ride properly on the rings and do not overlap. In fact a test man should place himself in the position of the customer and if anything about the machine does not appear right he should report it to the Head of Section. It is the duty of the Head and Assistant Heads also to look over the apparatus, but the man in charge of the machine will be held directly responsible. The Head or Assistant Head of Section must place the brushes of d-c. machines on the mechanical neutral and sign the Testing Record to that effect. The above inspection should also be made on all machines upon which changes have been made by the shop to make sure that no foreign material has lodged in the machine. Wiring Though a great deal of the wiring in testing work is tempo- rary, it must always be done as neatly as possible, due regard being paid to safety. All circuits should be protected by signs or barriers, where there is danger of any one coming in contact 98 with them. Conspicuously lettered danger signs are used to indicate the nature of the circuit. In addition to this, white tape is used around cables or apparatus carrying high voltages. After a tester has completed the wiring of a machine, he should notify the Head of Section, or Assistant Head of Section, to inspect the same. The Head of Section, or Assistant Head of Section, must then assure himself that it is satisfactory, and if so, enter his approval upon the Testing Record sheet and sign his name. The following general rules should always be followed in wiring apparatus for test. First, procure the print of connec- tions, which will be furnished by the Head of Section. The apparatus must then be connected up in accordance there- with. A copy of this print is sent to the customer with the apparatus, to help him in its installation. Checking the wiring during test serves the double purpose of detecting errors in the print, or wrong connections in the apparatus. It is consequently of considerable importance. In wiring apparatus for test, all the wiring should be com- pleted before any of the circuits are connected to the source of power, to prevent the necessity of handling live circuits while wiring. Where possible, one hand only should be used for connecting or disconnecting low voltage live circuits where an intervening switch cannot be used for making final connections. It must always be remembered that any circuit may become grounded and that some circuits are permanently grounded. The 125, 250, and 500 volt direct current shop circuits are permanently grounded. Hence, in all cases, circuit breakers must be wired on the positive side of the "125 volt" and "500 volt shop" circuits. As the "250 volt shop" is a part of the three- wire system with grounded neutral, a circuit breaker must be used on each side. Opening direct current motor and synchronous motor fields is likely to break down the insulation of the apparatus, and in the case of a d-c. motor, the motor will run away. Wher- ever binding posts and connectors, as used for rheostats and small fields, are employed, a length of unbroken insulation should be stripped from the end of the temporary field wire, so that the portion stripped can be passed through the binding post and bent back over the terminal. A complete loop is thus formed which prevents the circuit being broken, even though the clamping screw in the binding post or terminal works loose. It is not safe to insert in the binding post the bare end of a wire which has previously been used, since it may be fractured. When a motor field is wired through the field ammeter switch, the wire leading to the switch terminal and thence to the ammeter should be continuous, the switch simply serving to short-circuit the leads near the ammeter terminals. Motor field circuit breaking switches must be located so that they cannot be opened accidentally. The field switches must be provided with a holding clip, or other fastening. Single-pole switches must always be used in all field circuits. 99 In all cases, circuit breakers must be used for breaking direct currents of appreciable value. Oil switches must like- wise be used on all alternating current circuits, when currents and voltages of any magnitude are in question. Never break an alternating current circuit either by water box, or by an ordinary air-break switch, otherwise abnormal voltages may be produced and strain the insulation of the apparatus. All direct current generator and motor armature circuits must, therefore, contain a circuit breaker of sufficient capacity to open the maximum current delivered by the machine under test. When "feeding back" tests are made on direct current machines, two circuit breakers must be used, one in the supply circuit, and one in the motor-generator circuit through which the load energy is exchanged between the machines. All transformers with iron cases must have their cases grounded by a substantial wire, or cable, leading to ground. This lead must be substantially connected to the transformer case and to ground, so that it cannot be accidentally discon- nected. Temporary switches, circuit breakers, etc., should never be attached to a test table or switchboard which is permanently equipped. They should be mounted on rheostat stools, or temporary stands. All temporary cables and wiring must be properly insulated from iron floors, frames, and ground. High voltage alternating current lines must be carried at a sufficient height so that they cannot come in contact with men walking under them. This also applies to disconnecting and oil switches. Cables must be kept a sufficient distance apart to take care of the potential difference between them. They must be mechanically supported so they cannot drop from their fastenings to the floor. High tension wires must be carried to the testing table from the rear. They must not be car- ried over the heads of men working at the test table. All wires and circuits carrying more than 600 volts, must be regarded as high voltage. No one must approach closer than 1 foot to high voltage circuits, since many circuits possess sufficient capacity or voltage to arc over before contact is made. Starting Up Before starting a machine for the first time, the tester must assure himself that all instructions contained in Chapter 3, and in the preceding paragraphs have been rigidly followed in reference to the mechanical and electrical conditions, the wiring of the various circuits, lubrication, etc. The belt lacings must be watched to prevent them opening during test. Pulleys must be inspected by the regularly appointed Pulley Inspector to make sure they are securely fastened on the shaft and that they are mechanically strong. All keys, set screws, or other rotating parts which may catch in the clothing, or injure others must be properly protected. All keyways must be provided with covers or guards. All shafts carrying one-half of a solid coupling must have that part boxed in, so that workmen may 100 not come in contact with the sharp edges which usually exist. No loose articles must be allowed inside any rotating or station- ary parts. All belts must be guarded by substantial guards. If a machine has been standing for any length of time, before it is started again the same precautions must be observed. These points are strongly emphasized in reference to all ver- tical apparatus, where the danger of dropping things into a machine, while running, or of workmen leaving tools in danger- ous places on or about the machine is very much greater than with horizontal apparatus. When apparatus is first started it should be brought to speed very slowly and carefully watched to see that every- thing is correct as the speed increases to normal value. Reliable tachometers, or speed indicating devices must be used in starting to prevent a dangerous increase of speed. Oil rings must be examined at slow speed to see if they are carrying sufficient oil to the bearings. In the majority of cases, oil rings should turn when the machine is running at 34 normal speed, and should properly lubricate the bearings. The balance of the rotating parts should be carefully noted until the machine has reached its normal rated speed. If the apparatus does not run without vibration the matter should be reported as a defect. The vibration must be remedied before the test proceeds. Vibration due to the running of the machine may indicate lack of balance, whereas it may be really due to improper alignment, or to springing of the shaft. When unbalancing occurs in operating machines running above 1200 rev. per min. correction must be made by dynamic balancing as in Chapter 3. Preparation for Heat Runs Heat runs are taken primarily to determine the amount of temperature rise on the different parts of a machine while run- ning under a specified load. This rise in temperature is measured either by the rise in resistance of the current carrying parts or by means of thermometers, or both. The results obtained by the rise in resistance, as a general rule, are used only as a check on the results obtained by reading thermometers placed on the different parts, the temperature rise of which it is desired to determine. Guarantees, except in special cases, are always based on the rise by thermometer. Thermometers should be carefully examined for broken mercury columns before being placed on a machine. They should not be inverted and in no case should they be placed on a machine so that the bulb is on a higher level than the other end. Before starting a heat run thermometers should be placed on the stationary accessible parts of the machine indicated by the Testing Record. Each thermometer should be attached with the bulb in contact with the part of which the temperature is required and should have the bulb covered with a sufficient amount of putty to secure it to the machine and to shield it 101 from being affected by the surrounding air. Extreme care must be exercised regarding the amount of putty so used, as too much putty is as bad as too little. Just enough should be used to do the work required. There should be no restriction of the natural windage of the machine or radiation from the coil whose temperature is being measured. Thermometers which are to register the temperature of air ducts should be so placed that the bulbs cannot make contact with the iron laminations while the machine is running. Ther- mometers which are liable to be shaken off by continued action of windage, or slight vibration, should be securely fastened to the machine. When placing thermometers on field coils, care should be taken tosee that they are not placed on the fiber strips protecting the outside terminals. These fiber strips run from one terminal to the other and form a non-conducting wall between the coil and its outside insulation, and thus do not represent the true temperature of the coil. Coils above the horizontal center line of the machine should be used as the top of the machine is usually somewhat hotter than the bottom. On small machines two thermometers will be sufficient on the coils, but larger machines should have at least four. One thermometer will be sufficient on the frame of small machines, but two or more should be used on the large units. At least two thermometers should be used on the laminations ard ducts of small machines, and at least four should be used on larger machines. Any large machine requiring a considerable floor space should have the room temperature taken at four or more different near-by points, and at a sufficient distance away so as not to be affected by the windage and radiation of the machine. The machine should be shielded from currents of air coming from adjacent pulleys, belts and other machines, as unreliable results are obtained when this is not done. A very slight current of air will cause great discrepancies in the heating results, con- sequently a suitable canvas screen should be used to screen the machine under test, or the machine causing the draught should be shut down. Great care must be used, however, to see that such screen does not interfere with the natural ventilation of the machine under test. Care must always be taken to see that sufficient floor space is left between machines to allow free circulation of air. During the progress of the heat run the different parts of the machine should be carefully watched for excessive heating of any part, including the bearings. A sufficient number of ther- mometers and amount of putty should be made ready to take all the final temperatures of the revolving parts after the machine is shut down, and the man in charge of the machine, if it is a large one, should obtain temporarily several extra men to help apply the thermometers and record the results. On shutting down, thermometers should be placed on all the revolving parts as specified on the Testing Record. 102 All small commutators should have at least two, and large ones at least six thermometers applied at different points extending the whole length of the commutator from the arma- ture risers to the outer end. The thermometers must be applied as speedily as possible, and the resistances of the various circuits measured immediately after the machine stops. If any thermometer shows an un- usually high temperature as compared with others it must be immediately checked by placing other thermometers on the same part. Reliable results depend directly upon promptness and speed, and nothing should be allowed to interfere with the carrying on of this work. To avoid repetitions of runs the machines must be shut down quickly. Readings should be taken of all thermometers every two minutes until they begin to fall. In calculating the rise of temperature the room temperature should be taken as the average of the last two readings recorded during the heat run. Temperature Coils In order more accurately to determine the temperatures of the inaccessible windings of large machines, coils of small wire known as "temperature coils" are sometimes imbedded in the slots with the main winding. The rise in temperature of the main winding is found from the rise in resistance of these tem- perature coils and, consequently, accurate measurement of the cold resistances of these coils is of the utmost importance. During the heat run, readings should be taken of the resistances of these coils at the same time that the thermometer readings are taken. All readings must be very carefully made as a small error made in the resistances of these coils makes a very appre- ciable difference in the final temperature obtained. The rise in temperature mav be calculated from the formula given on page 112. OBSERVATIONS AND COMMENTS DURING OPERATION. REPORTING AND CORRECTING DEFECTS On all Testing Records a number of questions are given concerning the operation and condition of the machine during the test, which should be intelligently answered by the men conducting the test. A close watch should be made for undue heating of bearings. While running under load, no bearing should rise more than 40 deg. cent, above the room temperature. In case such a rise occurs, the bearing should be scraped and the test repeated. Any machine showing a bearing temperature rise of 25 deg. cent., during an "equivalent load" run, should have the run continued till bearing temperatures are practically constant, unless the temperature continues to rise rapidly. In any case, note should be made if the bearing temperatures rise above these limits and the fact should be reported as a defect. 103 A record should be made of any oil throwing or leakage during test, and the matter reported at once. In the case of oil throwing on d-c. machines, the test should be discontinued until the defect is remedied. All covers must be assembled in place so that it is impossible for any foreign matter accidentally to get into the machine. All staging around machines must be substantial and secure. End play should be tried both with and without field on the machine. This matter should be recorded on the Record Sheet. If the end play is. defective it may be repaired as given on page 96. During a heat run, machines set upon shop blocking should have the blocking and holding-down bolts examined at least every 24 hours to prevent the machine from pulling over or the bearings from loosening. Any connections not checking with the connection print or wiring diagram should be reported. All machines should be carefully watched for any unbalanc- ing or change in alignment. A defect of this nature may appear after the machine has been running for some time even though the balance and alignment may have seemed perfect at the beginning of the run. Record should be made of binding bands, commutator shrink ring or any other part running out of true. Commutators sometimes become noisy during operation, due to brush friction. This may be remedied by a slight occa- sional lubrication of the commutator surface. The noise may be due to the brushes chattering, in which case no lubrication must be used, but the defect reported at once. Chattering may be caused either by poor commutator surface or an improper setting angle of the brushes. One or two brushes may glow and become very hot on a stud carrying a number of brushes, while the other brushes run cool and without sparking. This is known as selective com- mutation and is due to difference in brush pressure, composition or contact resistance which cause some of the brushes to carry more than their share of the current, thus overheating them and giving poor commutation. In order to remedy this difficulty, it is usually necessary to change either the brushes or brush pressures, or possibly both. The brushes should be examined to see that they do not stick in their holders. Collector rings with rough joints, eccentric collector rings or ones running out of true should be reported at once. Unless the line circuit of a machine or the circuit supplying excitation to the fields is grounded, grounds developing in the armature, fields, or fittings during test may not at once become apparent. During the high potential test any defect of this nature is readily shown, however, and should be reported at once in order that repairs may be made immediately. The spacing and alignment of field poles, especially in the case of com mutating pole machines, should receive the most 104 careful attention. Poor alignment is usually indicated when the air gap is measured. The checking of polarity (see page 111) at once indicates the reversal of any field coils. In three-phase machines the reversal of any phase will cause a considerable unbalancing in the voltage across phases. The reversal of one coil will be shown in a similar manner, but the unbalancing is not so pronounced. In quarter-phase machines these defects will be shown by the phase rotation test only. See page 172. The test of balancing voltage and cur- rent and of phase rotation should, therefore, be carefully taken. Stationary Apparatus The instructions already given in reference to rotating apparatus very largely apply to stationary apparatus. The following points must also be carefully observed in testing the latter, including transformers, regulators, compensators, switches, relays, etc. Careful inspection must be made for mechanical or elec- trical defects when preparing stationary apparatus for test. The precautions already given in reference to wiring should be followed. All valves, tripping devices, contacts and insulation should be examined. Wherever cases or receptacles are oil filled for insulation purposes, see that the proper amount of oil is put into them before test. During the test the tanks and receptacles must be carefully inspected for oil leakage, due to blow holes in castings, oil plugs, oil gauges, or due to siphoning through the leads. Adjustments of springs, weights, contacts, gauges and air gap clearances must be made before testing, so far as is practicable. Xo metallic particles must be allowed to drop or be thrown into transformers, regulators, etc., during test; otherwise breakdowns of insulation may result. When testing stationary apparatus, it is rarely possible to tell from inspection whether the apparatus is "alive" or not. Hence there is all the more reason, on high voltage apparatus, to make use of signs and barriers, to eliminate danger and pre- vent shocks. 105 CHAPTER 5 TESTING RECORDS For the purpose of recording the results of standard tests, various Testing Records are used to suit the different classes of apparatus. Before a standard test is made, the tester must provide himself with one of the Testing Records. He should immediately fill in all blanks and headings, with all the data concerning the machine which can be entered before the test is started. All entries must be made at once upon the Testing Record and never on "scrap paper." These Testing Records (which should contain all the results of the standard test) must be checked at the conclusion of each test to insure con- sistency of readings and that full and complete explanations have been made concerning the machine under test. One man is appointed in each section to approve the results of each individual test immediately upon its completion. In all cases the written approval of this man must be obtained for each test before the next test is started. The completeness of these records is of the greatest impor- tance, since they are used when passing the machine for ship- ment and are finally filed in the Data Department, where they are accessible for reference for the Designing Engineer and others who desire to know the characteristics of the particular machine. It is, therefore, necessary to make accurate, neat and orderly entries on the Testing Record, and supplement them with sufficient data fully to inform any one who has not personally taken part in the test. Then, if reference is made to them afterwards, no question can arise as to the meaning of any of the readings or observations made. In general, the Testing Record is intended to be a complete and accurate history of the individual machine while in test and, therefore, every effort must be made to carry out this idea. Special tests must be recorded on special Record Sheets. As these tests are special and often involve new or peculiar conditions, careful notes and explanations, with diagrams if necessary, should be entered to make clear the conditions under which the test was conducted. The date of making the test, together with the name of the individual making it must always be recorded on all Testing Records and Record Sheets. In addition, whenever exhibition tests are made for our own Engineers, or for a customer's Engineer the Record Sheet must give the names of the Engineers who witness the test. Records of tests taken under the direction of a customer's Engineer must be plainly marked so that they may be distinguished from any other tests which may be taken on the machine. It is frequently necessary to furnish the cus- tomer with "certified copies" of tests in lieu of his sending an Engineer to witness the tests and check up the guarantees. Wherever Engineering instructions request "certified copies" 106 of the test, all the necessary tests and information must be recorded on the Record Sheet so that "certified copies" can be made, demonstrating that all guarantees have been met. The reasons for all check tests should be plainly stated on the Testing Record. When tests have been finished, all records in reference to them are sent to the Calculating Room, and such calculations made as required. Curves showing the characteristics of machines are plotted and filed with the corresponding Record Sheet. It is the function of the Calculating Room also to check up results on the Testing Records with those of duplicate machines already shipped; and, where necessary, to refer Testing Records on newly designed machines to the Engineering Department for their approval before passing the machine for shipment. As soon as the Calculating Room is assured, that the test proves that a given piece of apparatus is satisfactory and has the characteristics required for our guarantees, it approves the Testing Record and the machine is listed on the "Daily Test Report." The "Test Report" is issued daily, copies being sent to all persons interested in the shipment of the machine. It is the offi- cial notification that the apparatus is satisfactory in all respects and may be shipped. The majority of apparatus tested is listed upon this "Test Report." Certain small mechanisms and parts which only require a slight electrical test are passed for shipment, bearing the Testing Department stamp only, to show that they have been officially tested. Since the system of passing apparatus is largely founded on the test records, it is essential that these records be com- plete in every detail. 107 CHAPTER 6 METHODS OF CONDUCTING STANDARD TESTS In the manufacture of armatures and fields for electrical apparatus, many of the "faults and weaknesses" of material and errors of workmen can be disclosed by what may be termed "stationary testing." Faults and weaknesses may arise as follows: Through a wrong application of insulation, or through mechanical, faults in it. The use of wrong material for con- ductors, leads, etc. Wrong assembly or connections — workmen's mistakes. Direct current armatures are tested for grounds, short-cir- cuits, open -circuits, and high resistance joints before being sent to the Testing Department. In testing for grounds a high potential is applied between winding and core; the potential depending upon the class of apparatus tested. When a ground develops in test, if it cannot be located by inspection it must be referred to the Armature Department. In no case is it to be located by smoking the insulation. /K -0-31 Fig. 47 TESTING FOR GROUNDS If a low resistance ground has developed it may be quickly and accurately located by the following method: A low voltage current is passed through the armature winding from a com- mutator bar to the one adjacent to it, which is sufficient to give a readable deflection on a galvanometer or milli- voltmeter (as shown in Fig. 47). A line is connected to a galvanometer to ground, the other galvanometer connection being placed on one of the commutator bars. Then pass the supply and galvanometer leads from segment to segment, until a full deflection is obtained and zero reading when the leads are moved one segment further. The grounded coil then lies between the bars, for which full deflection was obtained. 108 A "bar to bar" test is usually made to disclose short-circuits open-circuits, and other similar faults. For this test the wind- ings connected to two adjacent commutator segments have their resistance measured by the "drop of potential method," as indicated in Fig. 48. Storage batteries should be used and a special electro-magnetic D'Arsonval galvanometer. With this arrangement readings can be obtained rapidly, as the instrument is "dead beat." Measuring the ohmic resistance of the winding will some- times reveal a wrong connection, which, on a bar to bar measure- ment, would give a uniform deflection all around the commutator. Series or wave windings may sometimes have all the conductors joined in series, but in the wrong order, so that the armature is inoperative. In the case of multiple or lap windings, double, triple or even quadruple spiral re-entrant windings are possible, whereas a single spiral is required. In taking a resistance measurement for brush to brush or a running resistance of the armature, see that the measurement is made from the proper commutator segments. For multiple or lap windings, the resistance measured from diametrically opposite points divided by half the number of poles squared will give the true running resistance, while with a series or wave winding the W tiffi-P 1r*" Fig. 48 TESTING FOR OPEN CIRCUIT resistance should always be taken at points 180 electrical degrees apart. For example, take a four-pole armature with a lap winding and 360 commutator segments. This should have its resistance measured between bars Xo. 1 and No. 181. The resistance divided by four will give the running resistance. With a wave winding on the same armature, the resistance measurement should be taken between bars No. 1 and No. 91, this resistance being the true running resistance. Alternating current armatures and fields are similarly tested for grounds, short-circuits, open- circuits, wrong connections, polarity, etc. In testing for grounds the same methods and similar apparatus are used as for direct current machines, except that with alternating current the voltages generated and used are usually higher and, consequently, the testing 109 voltages are correspondingly higher and greater care must be taken in testing. All high potential tests must be made with carefully calibrated electrostatic voltmeters that have been checked with a spark gap. The testing equipment should be as near the apparatus as possible, since the additional capacity of testing lines may raise the voltage at the receiving end much above that at the generating end. Unless this precaution is taken, excessive voltages may be applied which may damage the insulation. In case a ground develops a resistance measure- ment will generally locate the point at which it occurs, unless each phase has two or more multiple circuits. In the latter case it may be more readily located by opening one or more cable joints and separating the circuits. A measurement may then be taken in the following manner: First, measure the resistance of the grounded circuit or phase. Second, measure the resistance to ground by connecting one line to ground. Third, measure the other end of the resistance to ground, by connecting one measuring line at the other ter- minal of the phase and one to ground. If all measurements have been accurately made the sum of the second and third will be equal to the first, and the location of the ground will be as far from one terminal as the measured resistance from that terminal to ground is of the total resistance of the circuit. This test is shown in Fig. 49, which represents a single circuit, or phase, of an alternating current machine, with a I Fig. 49 TEST FOR GROUNDS ON AN A-C. ARMATURE ground as shown. If the resistance between A and B is one ohm, between A and G 0.35 ohm and between B and G 0.65 ohm, the location of the ground is 35/100 of the distance between A and B, from A. As 10 coils are in the circuit the measurements show that the fourth coil is grounded, counting from A. In the case of an alternating current winding the ohmic resistance measurement will not always detect a wrong con- nection, such as a reversed coil, pole section, or phase; since, although the copper resistance would be measured correctly the total winding might be partly reversed and, therefore, inoperative. Such faults may be discovered by a polarity or impedance test, with alternating current. For this purpose a :single-phase current can be used, since a reading may be taken 110 on the different circuits, or between pairs of terminals succes- sively by shifting the testing lines until the whole windings have been tested. Short-circuited coils on moderate size machines can be readily tested by using a wound electro-magnetic yoke excited with alternating current. This yoke is dropped over a portion of the armature coil after the coils have been placed in their slots. The yoke and armature form an alternating current transformer, "with the yoke winding as primary, and the arma- ture coil as secondary. If there is a short-circuited turn, layer or coil in the armature, the magnetizing current in the yoke winding rises. If the current is maintained a short time, the insulation on the short-circuited section will warm up appreci- ably, or burn sufficiently to indicate the defective coil. On larger size alternator armatures, tests may be made for short-circuits by passing alternating current through the armature coil itself. In this case it is usually necessary to increase the reactance of the coil by placing a magnetic bridge over its armature slots after it has been assembled in the core. The above tests may be made with the apparatus at rest. The Armature Department, therefore, uses them for detecting faults and correcting them before delivering the parts to the Testing Department. These faults can be more readily cor- rected when apparatus is being wound, with a resulting saving in time and cost. It is, however, sometimes necessary to test by these methods, after apparatus has been received in the Testing Department, in order to locate faults which have developed later. As soon as the spools are assembled on a machine and before the frame is taken from the spool assembly stand the windings should be tested electrically for resistance and high potential. They should also be tested for polarity of the poles by exciting the field coils. These tests check the assembly of spools and their position upon the frame. In testing field coils for polarity all field windings must be tested separately to ascertain that the series, shunt and commutating pole windings are wound and assembled so as to give the required polarity. Polarity may be tested by use of a compass, but the compass must not be carried too near to the poles, as it may be demagnetized, or even reversed. To test for the opposite polarity of alternate poles, bridge two pole tips with a piece of soft iron. If the polarity of the poles differs the piece will be strongly attracted, whereas if the poles are of the same polarity much less attraction will be exerted. Drop on Spools With a given current flowing through the field the voltage drop on any one spool of a direct current machine should in no case be more than 4.5 per cent higher or lower than the average drop, and on alternating current machines no spool should vary more than 7 per cent either way from the average. If the drop is outside of these limits, the matter should be referred to the office for instructions. The field spools for 111 alternating current apparatus are assembled on the field spider in the Armature Department, hence it is necessary to take only a resistance measurement per spool before using them for a test. In recording drop on the spools of alternating current machines, they should be numbered in a clockwise direction facing the collector end, and beginning at the spool next to the opening in the field for spool No. 1. In direct current machines spool No. 1, either main or corn- mutating is always the top spool or the next adjacent in a clock- wise direction facing the commutator end. Resistance When testing a machine a very careful record must be kept of the resistances of all windings. Most armatures when delivered to test are fitted with equalizer rings which make it impossible to obtain the true armature resistance. The Arma- ture Department's tag attached to the armatures when received in the Testing Department gives the armature resistance which was obtained before the connection of the equalizer rings. The tester must, therefore, record on the Testing Record the measure- ment of resistance from this tag. The armature resistance is rarely measured in the Testing Department. Such cases are specified when required. The shunt field resistance is obtained by the "drop method," using an ammeter and voltmeter. This measurement is required on each machine before a test is started. For measuring the series field resistance a special galvanometer measuring set must be used, with which the various testing sections are provided. As a considerable amount of the resist- ance of a series field may consist of the contact resistances between the spools, all connections must be carefully cleaned and clamped tightly together, before taking the resistance. After the heating test on any machine, the resistances of the various parts are again measured and the rise in temperature may be calculated by the following method: Let Rh = hot resistance of copper measured at the temperature h- Rti = cold resistance of copper measured at the temperature h. Then * 2 = (238+*i) -^7 -238 Kt\ The rise obtained from this formula should then be corrected according to the standard rules of the A.I.E.E. for variations from 25 deg. cent, in the observed room temperature. Insulation Resistance A measurement of the insulation resistance is occasionally taken upon direct current machines and alternators. The government requires this measurement in most cases. An insulation resistance measurement is frequently taken on alternators of 2300 volts and above. On commercial apparatus generally, the measurement of insulation resistance, however, is unnecessary, since the materials used have ample dielectric 112 strength and the slight leakage which a low insulation resist- ance would indicate is unimportant. This test when required is taken by the "d-c. voltmeter method of measuring high resist- ance" as given on page 42. In case the insulation resistance is lower than required, due to dampness, the machine should be baked either by the method described for making equivalent load tests (page 144) or by placing the machine in a baking oven. High Potential Test This test is taken by applying an alternating voltage between the various windings of a machine and from the current carrying parts to ground. Fig. 2 shows the connections for one of the standard high potential testing sets. Unless otherwise specified all high potential tests should be taken as given on the Standing Instructions for the machine in question. When the high poten- tial test is applied to a moderate or large sized machine or piece of apparatus, such machine must be entirely surrounded by white tape and should have placed on it in a conspicuous place the standard high potential signs to make doubly sure that no one comes in contact with it. A sufficient number should stand guard around it to make sure that no one is injured. On small apparatus the standard high potential signs should be used and but one man need stand as guard. Small machines need not be surrounded with white tape. After finishing the high potential test all oil and disconnecting switches must be opened before the high potential testing cables leading to the apparatus are handled. All temporary and high potential testing cables must be disconnected from the testing transformers or high voltage source at the conclusion of the test. Adjustment of Speed Limiting Device Many d-c. machines are equipped with a device for limiting the speed in case of loss of field or any other condition which might cause excessive speed. These devices must be adjusted to operate at 15 per cent above the normal speed of the machine under test (10 per cent for shop machines). This device is a centrifugal device in which a revolving weight acts against a spring and operates a switch connected in the circuit of the low voltage trip coil of the circuit breaker. Figs. 51a and 51b give diagrammatic views of the latest type of this device. In order that it may operate properly the follow- ing adjustments must be made: With the weight moved outwards to the maximum distance, a clearance of ye in. as shown in Fig. 51b must be allowed between the centrifugal weight and the link when the switch is open. This clearance must be allowed in order to prevent the weight from hammering the switch after it has been forced open. With the switch blade wide open and with the weight at its maximum distance outwards, there must be y& in. clearance between the nearest point of the switch and the centrifugal weight. A clearance of 34 in. must be allowed between the switch blade and the clips when the switch blade is in its extreme "out" position, as shown in Fig. 51b. 113 The adjustments of the clearance of the switch and centrif- ugal weight can be obtained by finishing their respective stops (on the short end of the switch and the hook shaped stops on the ring), to the proper dimensions. If too much material has already been removed from the stop, it may be drilled and tapped for a screw or plug which can then be finished to the proper dimensions. All of the clearances given are the minimum that are obtained when the weight is rotating. After these clearances have been adjusted, the spring should be adjusted, if necessary, so that the centrifugal weight strikes the switch and forces the switch blade from the clips when the speed has reached the specified limit. The springs are adjusted Fig. 50 SPEED LIMITING DEVICE (EARLIER TYPE) so that the weight operates on the switch when the speed has risen 15 per cent above normal. The method of spring attach- ment and therefore of adjustment will be clear from the figures. The switch shown in Fig. 50 is arranged to short-circuit the low voltage trip coil of the circuit breaker and should be adjusted with the clearances shown in Figs. 52a, b, c. In this case the revolving weight drives the switch blade into the switch con- tacts. Figs. 52a, b, c also show diagrammatically a type of switch which is adjusted by varying the notch in which the loose end of the spring is placed. The number of the notch in 114 Not Less than Not Less Te 'when Fig. 51a We/ght /s Outer Pos/t/a Fig. Sib DETAILS OF SPEED LIMITING DEVICE (LATER TYPE) 115 Fig. 52a 3" — 1 ^~-- /Voc/ess Cfta/7 /e 1 O) o Fig. 52b Fig. 52c DETAILS OF SPEED LIMITING DEVICE (OLD TYPE) 116 which correct adjustment is obtained must be recorded, and the speed at which it trips; also the tripping speed and number of the notch on each side of the correct one. The notches are numbered beginning at the one nearest the pivot. In adjusting any speed limiting device several check readings must be taken at the final position to make certain that the device is set at the proper point. Adjustment of End Play Device Many machines, especially synchronous converters, are equipped with an end play device to cause an even wearing of bearings, commutator and collector rings. These devices are Fig. 53 MAGNETIC END PLAY DEVICE of two types, viz., magnetic and mechanical. Before any adjust- ments are made great care must be used to see that the machine is perfectly level, that it floats in the mid position of its end play with field on, and that it has the correct amount of end play. The magnetic end play device, see Fig. 53, causes the armature to oscillate by the same principle as is used in an electric bell. It should be wired as shown in Fig. 54, using a source of supply whose voltage equals the normal voltage of the machine under test. To adjust the device set contact (A) by means of the thumbscrew (T) until it firmly touches contact (B). This is done with the armature in the mid position of its end play. When the contacts come together the circuit is closed through the coil and the electromagnet pulls the end of the shaft toward it. When the shaft comes toward the magnet it pushes the rod 117 (R) against the arm carrying contact (B) which opens the circuit, releasing the magnetic pull on the end of the shaft so that the armature is pulled back in the other direction by the field of the machine. The momentum of the armature carries it beyond the mid position of the end play and the contacts come together again. The pull of the electromagnet is not exerted fully until the armature has traveled away from the device some distance beyond the mid position. The pull is then established and causes the armature to return to mid ruse /?es/s£0/7ce 3a< Cos?&er7Sers /M&gnet Co// MavMe firm ^ 7/7SU/ateGf Spring fuse Fig. 54 CONNECTION DIAGRAM FOR MAGNETIC END PLAY DEVICE position. This cycle is then repeated. A rheostat is provided to adjust the magnetic pull of the device to that of the fields, so that the armature may oscillate the full distance of end play allowed without bumping the bearings. After final adjustment has been obtained, the amount of resistance included in the rheostat should be measured and recorded on the Testing Record. A condenser is connected across the contact to suppress the spark when the circuit is opened. The bushing through which the push rod passes should not be lubricated, as it is provided with specially prepared graphite for self-lubrication. The mechanical end play device is shown in Fig. 55, and consists of a ball running in a raceway held in a block which is held in a shell. This shell is screwed into a three armed casting which is bolted to the end of the pillow block of the machine. This ball makes contact with a plate on the end of the shaft 118 of the machine. The shell in which the raceway block is held should be screwed into the position at which the ball will just make contact with the plate when the armature is in the mid position of its end play. The ball must be in its lowest position and the spring which" is in the shell must not be set up tight but must have sufficient play to take up the force of the end thrust. As the center line of the raceway block is at an angle Fig. 55 MECHANICAL END PLAY DEVICE with the center line of the shaft, the friction between the ball and plate will cause the ball to be carried up and during the revolution it will throw the shaft its full distance. The ball will then fall back and the pull of the field will cause the arma- ture to return and the cycle to be repeated. Adjustment should be made of the tension of the spring so that the armature will swing through the range of its end play and yet not bump the bearings. It may be necessary to change springs. When the exact position of the ball has been determined, the shell may be held in place by screwing down the plug in the side of the three armed spider. Saturation In order to ascertain the characteristics of the magnetic circuit, a test known as "saturation" is made. The character- istic curve may be obtained by either of the following methods: "generator saturation," or "motor saturation." 119 Generator Saturation The test usually made is "generator saturation." To obtain a saturation curve by this method, the machine is driven as a generator, preferably at normal speed. If, however, a set of readings is known for one speed, they can be obtained for any other by direct proportion. Hence a saturation curve taken at any constant speed at once gives the saturation curve at any other speed. The brushes of direct current machines should always be set on the neutral point and the machines run preferably at no-load speed when taking a no-load saturation curve. In taking a saturation curve on polyphase alternating cur- rent generators, a reading of the voltage across each phase must be taken at normal field current, to see if the phases are properly balanced. If they do not balance, they must be made to do so. On synchronous converters careful readings must be taken of the direct voltage, as well as the alternating voltage between all phases with the field excitation giving normal voltage. The phase voltages must also be closely balanced. The usual method of taking a generator saturation curve is to hold the speed constant, and then increase the field current step by step until at least 125 per cent of the normal voltage of the machine is reached, taking readings at each step simulta- neously, of volts armature, volts field, and amperes field. After reaching the maximum value of the field current, without open- ing the field, reduce the current gradually in four or five steps, and again take readings to determine the value of the residual magnetism at various points along the curve. Special care must be taken to insure accurate readings at and above normal voltage, since with alternating current generators, this is the portion of the curve used for calculating the regulation under load. Whenever saturation curves are taken, a record of the air gap from iron to iron must be made upon the Record Sheet, together with the armature and field specifications. Motor Saturation When it is inconvenient or impossible to drive the machine as a generator, a "motor saturation " may be made. In this case the machine is operated as a free running motor. The driving power must be furnished from a variable voltage circuit. A certain voltage is impressed upon the armature and the motor field weakened or increased in the case of direct current machines to give normal speed, and a record made of the volts armature, amperes armature, amperes field, volts field, and speed. The starting voltage should be at least 50 per cent lower than the normal voltage of the apparatus. The applied voltage at the armature should be increased by steps to 25 per cent above normal value, and the field increased correspondingly to keep the speed constant, the same readings being recorded at the various steps as before. Readings should also be taken at 120 three or four points as the impressed voltage and field current are lowered to approximately the values at the beginning of the test. Care should be taken when testing direct current apparatus, as unstable electrical conditions may develop, and excessive speeds result. The circuit breaker in the armature circuit of the motor driving the machine must, therefore, be accessible to the tester reading the speed. -Mil ' i ixf $11 i |^ T § 1 ! f ^'T 1 ! '1 . sT r /00[ \ 7 | i ^ S 4 It / Jl itzti z : X / JZJZ ± I 300 it it 7 -i i~ / 40C / 1 ^t-ui it it it-K X j \ JOO 1 IE Zt It it tilt ■ It *,00 / | ■"»/ _ ~^~ ~r- 7tlt If If "TO ' f -I ... L , 1/ T ^- -4- Xl£ — „± ± 1 <0 20 40 60 80^ /OO 120 /Jmper&s rie/d Fig. 56 SATURATION CURVE ON A 500 KW., 600 VOLT, 20 POLE, 360 R.P.M. 3-PHASE, 60 CYCLE, A-C. GENERATOR On alternating current apparatus, the machine is run as a motor and the impressed voltage varied as already described. The speed is independent of the motor field in this case, and instead of regulating the motor field for speed it should be regulated to give mimimum input current at each voltage. Readings should be taken of voltage impressed, amperes arma- ture, amperes field, and volts field. With induction motors it is only necessary to impress variable voltages at constant fre- quency and record readings of impressed volts armature, amperes armature, and speed. 121 The calculation of saturation tests is very simple, as it consists only in applying instrument correction factors and ratios, and plotting upon coordinate paper, volts armature as ordinates and amperes field as abscissae. Fig. 56, and Calcu- lation Sheet No. 1, show the results of a saturation test made by either of the above methods. Core Loss Three methods are used to measure the core losses on rotating direct current apparatus and alternating current synchronous apparatus. They are known as follows: "running light core loss," "belted core loss," and "deceleration core loss." The following conditions must be obtained with direct current apparatus in order to give satisfactory results: Brushes must be shifted on the commutator to the mechanical neutral point. They must have their normal tension and the commutator must be clean, so that the normal operating commutator and brush friction values are obtained. This test, wherever pos- sible, must be made after all the others have been finished, in order to have a glossy commutator with its surface in good operating condition. The driving power should be supplied from a variable voltage circuit that is not subject to sudden fluctuation. Readings must not be taken when the rotating parts are accelerating or decelerating. Running Light This test is made by running the machine free as a motor. It is made on most d-c. generators and motors which are given a running test and occasionally on alternating current syn- chronous apparatus. When "running light" tests are made on direct current generators, the observations must be made with full load field flux. The potential applied to the armature must be equal to the normal rated voltage of the generator increased by the IR drop in the armature at full load. With this voltage im- pressed, the field current is varied until normal speed is obtained, when careful readings must be made of armature current, armature voltage, field current, field voltage and speed. If the machine in test is a direct current motor, the voltage applied to the armature should be equal to the normal rated voltage of the motor, less the IR drop in the armature under full load. The field current is then adjusted to give normal speed and electrical and speed readings taken, as outlined above for direct current generators. The power supplied to machines running free will equal that absorbed in bearing friction, brush friction, windage, and core loss, when the armature PR losses have been sub- tracted. In making records of these tests, the Testing Record must clearly show whether the running light current consists of the armature current plus the shunt field current, or whether it is the armature current alone. To check this point, open 122 the armature circuit with the shunt field circuit closed, and note whether any current is indicated on the ammeter reading the power supplied. If no current is indicated, the reading indicates the armature current alone, otherwise, the running light current is equal to the sum of the armature and field currents. To obtain ''running light" core loss tests, only a single field winding must be used for excitation; this must be a shunt field winding. In the case of series wound motors the field should be sepa- rately excited and extreme care should be taken to see that the motor does not lose its field. In order to obtain running light core loss upon alternating current synchronous machines (in which class synchronous converters are not included as the core loss test on these ma- chines is similar to that on direct current machines), they should be operated as synchronous motors at the proper frequency and rated voltage. For the best results, both frequency and voltage must have a steady value. With normal voltage on the armature, the direct current field should then be varied until minimum armature current is obtained. Readings should then be taken of amperes and volts of all the phases. At minimum input current unity power-factor is obtained and, therefore, the power to drive such machines will be the volt-ampere input. Wattmeters may be used in addition to check the volt-ampere readings. This measurement includes friction and windage losses, together with open-circuit core loss, plus the I 2 R loss in the armature. If the value of the core loss need not be separated from the other losses, the test is useful for checking up full load efficiencies. Belted Core Loss By means of the ' ' belted core loss' ' method the core loss can be separated from the bearing friction, brush friction and windage. A small direct current motor is used to drive the machine under test as a generator at its rated speed. A belt drive between these machines is most commonly used, but wherever great accuracy or a high speed is necessary, direct drive by means of a coupling is often used. The driving motor for this test should be such that good commutation is obtained for all loads required by the core loss test with a fixed setting of the brushes; and with the maximum volts on the machine under test, it should carry not more than 50 per cent of its normal rated capacity. Ordinarily a good rule to follow is to select a motor, the rated capacity of which is approximately 10 per cent of the rated output of the machine under test. When the brush setting to give the best possible commutation at all loads has been obtained, the brushes should be left in that position throughout the test. The commutator surface should be in first class condition and should have the brushes closely fitted to it. The belt should be of minimum width and weight to carry the load without slipping. When testing motor-generator sets, 123 synchronous converters and other machines that do not require belts in practice, the tension of the belt must be kept as low as practicable so that the bearing friction is not increased on account of belt pull. Endless belts should always be used in preference to laced belts. The diameter of the pulleys should be so selected that the driving motor will run at or near its rated speed when the machine under test is running at its normal speed. The driving motor should have its field separately excited from a constant source and other wiring so arranged that readings may be taken of amperes armature, volts armature, amperes field and speed. The volt-wires should be firmly attached to brushes on two adjacent studs. The brushes so used should be insulated from the holders so that the true volts armature may be obtained. Previous to starting the test, careful resistance measurements must be made of the armature of the driving motor. The machine under test should be wired as a separately excited generator with provision for reading volts armature, volts field, amperes field and speed. The test should then be carried out as follows: The field of the driving motor should be adjusted to about normal value and held constant, and the speed regulated by varying the voltage applied to the armature terminals. Careful readings should be taken to make sure that no belt slipping occurs. This is done by taking simultaneous readings of speed of both the driving motor and the machine under test: (a) with no field on the machine under test, (b) with normal field excitation. The two readings of speed should be identical. The machines should be run a sufficient length of time to allow the friction to become constant. This will be the case when the input to the driving motor becomes constant when driving the machine under test without any field excitation. Throughout the entire test, readings must be taken at abso- lutely constant speed when the rotating parts are neither accel- erating nor decelerating. Readings should be taken as follows: (a) Take the input to the driving motor with no field on the machine under test and with all brushes down on the commu- tator. (b) Take the input with field on the machine under test to give normal volts with all brushes down on the commutator. (c) Take the input with all brushes raised from the com- mutator and with the same field current in the machine under test as for the preceding reading. (d) Take the input with all brushes raised and with no field on the machine under test. The difference between the first and fourth readings is brush friction. The difference between the second and first readings and also the difference between the third and fourth readings is core loss. The core loss should be the same with the brushes down as with the brushes up, and the two results obtained 124 should check within 6 per cent before proceeding with the test. Starting with zero field on the machine under test observations of the input to the driving motor should be made at various values of the field up to that which will give 125 per cent normal voltage, and at least half the readings should be taken between 90 per cent and 110 per cent of the normal voltage. The "friction, reading" with zero field excitation on the machine under test should be repeated at least three times during the progress of the test; namely, at the beginning, again near the mid point of the curve and finally at the end of the test. ' | j : ! 1 ' "' i tt ~\ It t7 ^ 1 1 1 A f\ , / it in / rl / / ^o / * _ 1 o i ft y TT^ * y ^ J V h- <=>? yj 44- 1 Fig. 57 OPEN CIRCUIT CORE LOSS ON A 500 KW., 600 VOLT, 20 POLE, 360 R.P.M. 3-PHASE, 60 CYCLE, A-C. GENERATOR As the amperes field of the machine under test are increased the volts armature of the driving motor should also increase because of the increased IR drop in the armature. The driving motor should then be unbelted and a "running light " reading taken on it as follows: Without changing the brush shift hold the same amperes field as was held during the core loss test and take a reading of the input to the motor to give the same speed as was read on the driving motor at the beginning of the test. The volts armature should be lower than for anv reading taken during the core loss test. To check the results of the core loss as the test proceeds the power input to the driving motor required bv the core loss at a given excitation should be plotted agains't volts armature generated. This should give a curve similar to Fig. 57. Correcting the motor input at the various field strengths by deducting the PR loss in the armature of the driving motor and subtracting the power input to the driving motor with zero field on the machine in test, the core loss is left corresponding to 125 By subtracting the "running light " input to the driving motor from the input with zero field on the machine in test, the bearing friction and windage losses of the machine under test are obtained. No pulsation or sudden variations must occur in the arma- ture current of the driving motor which might vitiate the power readings. It is advisable to wire an inductive winding in series with the armature of the driving motor in order to steady the motor armature current. / f O / J / / -4000 / / / / / SOOO / 1/ / r / / / y ,> V' /ooo s >1 s\ /oo 200 SOO too SOO 6O0 700 Fig. 58 SHORT CIRCUIT CORE LOSS ON A 500 KW\, 600 VOLT, 20 POLE 360 R.P.M., 3-PHASE, 60 CYCLE, A-C. GENERATOR In making out reports of core loss the following data regarding the machine under test should be recorded on the Testing Records in addition to the electrical readings already mentioned: viz., circumference of commutator; circumference of shunt and series field spools; height of shunt and series field spools; number and width of commutator bars; size and material of brushes; number of studs and brushes per stud; brush pressure per brush; rating of driving motor together with its armature and frame number; type and rating and serial number of the machine under test. On series motors core loss tests should be taken at several different speeds covering the range of the speed curve. The method used is identical with that described above and will be considered in connection with railway and series motor tests. 126 Synchronous alternating current machines generally have loss measurements taken as outlined above on open-circuit (see Calculation Sheet No. 2), and also with the armature of the machine under test short-circuited. In the latter case the increase in power supplied by the driving motor over that required by the friction loss is plotted as ordinates against the amperes armature as abscissas, or the open-circuited arma- ture voltage due to a given excitation. A curve is obtained /O 20 30 40 50 60 70 SO SO /OO //O /20 Seconcfs Fig. 59 DECELERATION CURVES ON A 3000 KW., 2300 VOLT, 720 R.P.M. 60 CYCLE, 3-PHASE, A-C. GENERATOR similar in character to the open-circuited core loss curve. Such test is commonly known as "short-circuited core loss." Fig. 58 shows the results of such tests after all correction factors have been applied. In making this test careful measurements must be made of the resistance of the short-circuited armature circuit including all leads, before and after the test, since to obtain the true short-circuited core loss the PR loss must be subtracted. Observations should be made with the short-circuited armature current at least 200 per cent of its normal full load value. (See 127 Calculation Sheet No. 3.) Care must be taken not to overheat the windings. Deceleration Core Loss It is often necessary to determine the core loss, friction and windage losses of large machines when it, is impracticable to employ the "belted core loss" method. The "running light" reading alone does not allow the separation of the core loss from friction and windage. A method known as the "deceleration core loss" is used for this purpose. Such tests 90 80 70 60 X40 20 10 _L t / f 7 7 7- / / jT y s^ ^^ ^.^^ i *" r ~* "800 J200 /600 2000 Vo/ts /Ir/nati/re 2400 Fig. 60 OPEN CIRCUIT CORE LOSS CURVE FROM DECELERATION CURVES IN FIG. 59 are employed regularly on turbine-driven units, and it is very convenient to use them in connection with certain vertical waterwheel-driven generators, and other exceptionally large horizontal alternators and direct current machines with a considerable flywheel capacity. A running light reading at normal speed and normal voltage should be taken to give the driving power necessary under that condition. Where this is not practicable, the moment of inertia of the rotating part must be known. This can be very accurately calculated for the majority of machines from their mechanical dimensions, as given by the working drawings. The test is as follows : First drive the machine with no field at a little above normal speed, and then suddenly cut off the driving power and observe the deceleration, then do the same 128 thing with full field on the machine. In the first case the decelera- tion is due to the retarding force (friction and windage), in the second case due to these factors plus core loss. Readings of the speed of the rotating parts should be taken at sufficiently frequent intervals to obtain a uniform and reliable curve. A set of these curves is shown in Figs. 59 and 60. With the aid of these curves together with a "running light" test, or a calculation of the kinetic energy of the rotating parts, a determination of the value of the core loss, and also of the friction and windage, is readily made. The following is a brief derivation of the formulae used in calculating such results by either method. If W = weight. r = radius of gyration. Si = speed in r.p.m. at time 7\ Sa = speed in r.p.m. at time TV Wr 2 = flywheel effect. Then the kilowatts loss may be found from the following: *2308 (S^-Sf) 1 . . . , , .. , o , c. — — Wr- - _ = kw. lost in decelerating from Si to S 2 with any particular field excitation. * This formula gives the average power loss from Si to Sz and may be derived as follows: If M = mass v =linear velocity at radius of gyration 03 = angular velocity 5 = speed in r.p.m. corresponding to angular velocity g =32.2 ft. per sec. per sec. £ = kinetic energy at speed 5 and time T Ei = kinetic energy at speed Si and time Ti Ei = kinetic energy at speed S2 and time Ti P = power 1 W The kinetic energy of a moving body at any instant is — Mv 2 . M = — and for a rotating body v=ru> and co =— — . b(J. 1 W W / ?7rS\ 2 Hence E =-- M& = ^-(raj2) =~ I r =^) =0.00017 Wr*S*. I Ig Ig \ oU / £1 =0.00017 Wr 2 Si 2 (1) £•2=0.00017 Wr°- S2 2 (2) The energy consumed between Ti and T2=Ei—Ei but for (1) and (2) £1 -Ei =0.00017 Wr* (Si 2 -S2 2 ) in foot lb. Energy Power Time .-. P=|i-^- 2 = 0.0001 7 Wr* ( ;!f y? ft. lb. per sec. /« — il (J2 — i l) Multiplying by the proper constants to reduce to kilowatts we have kw .0.00017 W,: ^M x^| Xi -^ Wr-- ^=^ which is (T2 — T1) 1000 00O 10 10 (T2 — T1) the average power loss for speeds from Si to S2. (Continued on page 130) 129 If T z and T* are respectively the times at which the speeds S\ and 52 occur with no excitation on the machine, then in this rt. 1 "I 2308 W 2 W-Sf) case the loss m kw. = ■ Wr 2 -?= , _ T , §The kw. core loss is then the difference between the results obtained from the above two formulae. With deceleration core loss records the same data must be entered upon the record sheets that are required in connection with the belted core loss method. Calculation Sheets 2 and 3 show the standard method of calculating test results, open- circuited and short-circuited, taken by the belted core loss method. Calculation Sheet 4 shows the method employed in calculating results of deceleration core loss, either by using the value of Wr 2 , or the running light test. Input- Output Test It is sometimes required that the efficiency of a machine, or motor-generator set be measured by the input-output method. The measurement of the power input to the motor or the output from the generator is then required. The efficiency of the set will then equal To find the loss at any particular speed use the following method: E =0.00017 Wr 2 S 2 . If ds is the infinitely small change of speed during the infinitely short time dt then f . "p-moi;™* ) _ . 00034 Wr , s « or a _ KS is dt dt dt dt dt But — =- is a rate of change of energy or power and -3- =P dt dt Having obtained a deceleration speed-time curve we can get. P for any value of 5. Since -r - is the slope of the curve and can be obtained by drawing at the tangent to the curve where 5 has the desired value. Substituting values of 5 and -7- in the above equation gives the value of P. dt § If the kw. ' 'running light " has been obtained, , .. • r ..,, 2308 _. . (Si* -52*) v WrKSt-Sf) kw "running light" =- T7 r- Wr 2 -y= 7F -^- = Ki Wr 2 = 10'° (T2-T1) (T2-T1) kw. "running light " (7^2 — Ti) also kw. friction = Ki(5i2-5 2 2 ) KiWr 2 (Si 2 -S2 2 ) (Ti-Tz) or substituting for Wr 2 kw friction =7^ =rr Xkw. "running light." {Ti— Ta) Hence knowing the "running light," the friction can be calculated and the core loss separated from the "running light." 130 Total output of generator total input to motor The efficiency of the generator equals Total output of generator input to motor — motor losses The efficiency of the motor equals Output of generator +generator losses input to motor In the case of induction motors, input-output test is some- times taken by the string brake method, which is discussed in Chapter 12." The input-output method of measuring efficiency is one of the most difficult tests which the Test Dept. is called upon to make, and is subject to considerable inaccuracy. This method of the direct measurement of the efficiency of a machine should preferably be made by using a duplicate machine for power or for load. This is especially true of motor-generator sets. The two sets should be wired up for feed back test and the electrical losses supplied to the direct current machine, unless it is possible to secure a source of alternating current whose wave form is identical with that of the alternating current motor under test. Great care must be exercised in wiring the machines for this test. The voltmeters, reading the voltage of the input and the output, should be wired as near to their respective machines as possible. The secondaries of the current transformers should be wired directly to the instruments and not through any switches or contacts of any kind, and the wiring must be continuous, i.e., without an}' splices. The alternating current wattmeters, reading the input, must be placed some distance apart. All instruments should be carefully tested for stray fields. If the machines have series fields, these must be disconnected. Before the machine is started the wiring must be thoroughly inspected by the Head of the Section or one of his assistants. The complete set of instruments, transformers, etc., must be specially calibrated before this test is commenced. No reading should be taken until the instrument pointers are steady and extreme care must be taken to have all readings simultaneous. Xo man should read more than two instruments and preferably there should be one man for each instrument reading directly the input and the output. The resulting errors from the input-output method are likely to be large, since any inaccuracy in instruments, or personal errors in reading, influence the results directly. The errors in reading the instruments maybe partially eliminated by taking several readings at each load and using the average of all these readings. Even with the best conditions for making the input-output test it is still much more preferable to ascertain efficiency by measuring the losses directly. By adding all the losses to the output at any 131 load the input at that load may be obtained, The output divided by this result gives the per cent efficiency. The same per cent errors in instruments or instrument readings in loss measurement test influences the results of the efficiency calcula- tions only indirectly; consequently the latter method is superior for ordinary testing. Shunt F/'e/d vvw Tora6/ea/?d -+- Exc/tat/o/7 OCo/T?fmi£at/ng/ye/d * 'WWW Commutat/f?0 —F/ * -j .4. ^L _JL £ X 7 T v I I r 7 I I t L <25? -*? 60 SO /oo /20 /"TO ,^ • i L< ^ ■j ,"t ,' i ~* ' § ,*-' i n4 - iLQ. S$ s To ] £r --V -i i -I 1_ -\ -s J " * FrictionD. c dCoreloss n \ | i J )( I />»fiky?,J,JLl/>/* „^ Brus/i/rktionAC. /k, r (/cf-4 20 60 ^ GO /OO AtO Fig. 70 EFFICIENCY AND LOSSES ON A 100 KW., 6 POLE, 275 R.P.M. 525/575 VOLTS, COMPOUND WOUND D-C. GENERATOR 148 armature, as shown in Fig. 71. Tests are made as on other d-c. generators with the following additional special points: In compounding a machine, care should be taken to have the shunts in each half of the series field of approximately the same size, and when the correct compounding has been obtained "shunt balance readings" should be taken as follows: Remove the shunt from one side of the series field and take readings at no load and full load. Replace this shunt and repeat the readings for the other half of the series field. The line voltage obtained on these two readings should check. -vV\AAA/W Shunt Ffrkt Fig. 71 THREE- WIRE GENERATOR Unbalanced Readings If unbalanced readings are required, a compensator should be wired as in Fig. 71. A reading should be taken at no load normal voltage. With no change in the field and holding con- stant speed, \i load should then be thrown on one side of the line and the voltage read from the neutral to each side of the line. Volts and amperes line, volts and amperes field should also be read. One-quarter load should then be put on the other side of the line, giving a balanced load, readings being taken as before. The load should then be increased to 3^ load on one side, this procedure being continued until 125 per cent balanced load is obtained and readings taken at each step. Instructions some- times call for 50 per cent unbalancing, in which case the load is increased 50 per cent at each step instead of 25 per cent. Revolving Compensator One type of three-wire generator has its compensator mounted directly on the shaft at the back of the armature and is equipped with only one slip ring. COMMUTATING POLE GENERATORS General Notes The general instructions covering mechanical inspection, measurement of air gaps, drop on spools, etc., applying to all other generators must be followed in testing machines with 149 commutating poles. The function of the commutating pole is to improve commutation and in testing, commutation is, there- fore, important. The pole spacing should check within -^ in. as specified on page 82. The commutating poles produce the necessary flux for neutralizing the effect of armature reaction. This flux prevents the shifting of the neutral point between no load and full load which occurs in d-c. machines not equipped with them. In addition it aids the current reversal in the armature coils at commutation. To obtain the proper reversal without sparking at normal current requires a definite number of ampere turns in the commutating field.. The brushes are placed on the mechanical neutral, and if the machine is properly com- pensated the mechanical neutral will check with the electrical neutral. Baking Commutators Commutators of commutating pole machines are baked according to the method on page 144. The brushes must never be shifted under load, so as to produce sparking and heating. They must always be shifted at no-load to insure their not being set beyond the safe limit of no-load commutation, thus rendering it possible for the machine to flash over if the load is suddenly removed. In all cases, the Head of Section or his assistant must be consulted before the brushes on any com- mutating pole machine are shifted far from the neutral. It must also be remembered that the armature must not be short-circuited through the commutating pole winding when baking a commutator, as in this case the majority of machines will build up as series generators, and the armature current can- not be controlled. Locating the Neutral Referring to Fig. 72, one armature coil contained in a pair of slots in the armature core and the corresponding commutator segments are marked for the convenience of the Testing Depart- ment. The coils are marked with red paint, and the ends of the corresponding commutator bars are stamped with the letter " O. " In a machine with full pitch winding the two red marked arma- ture conductors (A) forming a coil will come one pole arc apart, and in setting the brushes these conductors should be placed directly under the centers of the commutating poles as shown, and the brushes shifted until the center of the brush rests on the center line of the commutator segment corresponding. On a fractional pitch winding the two red conductors will not span a full pole arc, and hence they should be so located that they are equi-distant from the center of their respective" poles as shown by the dotted lines B-B, and the brushes set as above. If there is more than one coil per slot, there will be a corresponding num- ber of commutator segments stamped O-O, but the middle one should be used. After the brushes are set the usual tests for building up, saturation, etc., may be continued. 150 Shunt Adjustment It is the aim of the Engineers to design the commutating field so that it will operate without a shunt; however, it is some- times necessary to shunt out some of the current to obtain the proper compensation for satisfactory commutation. A thorough trial should be made, however, with full commutating field. In adjusting for commutation, a compound wound machine may be Fig. 72 DIAGRAM SHOWING MARKING OF ARMATURE AND COMMUTATOR FOR LOCATING MECHANICAL NEUTRAL run with full series field. If the commutation is not satis- factory at full commutating field about ten per cent of full load current should be shunted. If the commutation is improved more current should be shunted until sparkless commutation (Xo. 1, see Fig. 62) is obtained at all loads up to fifty per cent overload unless otherwise specified. If the commutation is not improved by shunting current the Head of Section should be notified. Sometimes a slightly better effect is obtained by shifting the brushes forward or backward from the neutral point. This, however, should only 151 be done after all other adjustments have failed, and permission has been obtained from the Head of Section. If none of these methods gives satisfactory results the trouble may be due to a weak field. This can be ascertained by separately exciting the commutating field and sending a larger current through it than would otherwise be obtained with normal load on the machine. If such procedure improves the commutation the fact must be referred to the Engineers to have changes made. The iron grid shunts used on the larger machines should be placed so that the edges of the grids are in a vertical position and as near as possible to the position they are to occupy when in actual operation. Care should be taken to see that they contain ample current carrying capacity and do not heat up. If they are allowed to heat excessively the amount of current shunted changes, and thus destroys the commutation of the machine. When the final brush position has been determined it should be marked with a chisel. On the larger machines a trammel should be made by the shop to assist the customer to assemble the brushes in a correct position. This trammel consists of a steel bar pointed on the ends and of the correct length to mark the distance from two points in the magnet frame to the point on the commutator on which the brushes on one stud should be placed. After the proper adjustment has been obtained an ammeter should be wired in and the amount of current shunted carefully measured. Inductive Shunt Any condition which would suddenly under-excite the corn- mutating field or make it inactive would make the machine sensitive and cause bad sparking at the brushes. If the corn- mutating field is equipped with a grid or German Silver shunt and the machine becomes short-circuited, the inductance of the commutating field forces the instantaneous heavy overload current through the non-inductive shunt and leaves the com- mutating field without sufficient excitation to neutralize the armature reaction. The electrical neutral immediately shifts and bad commutation results. To eliminate this trouble an inductive shunt is sometimes used across the terminals of the commutating field in series with the non-inductive shunt. This shunt will be used only when called for by the Engineers, but when so specified it should be in circuit while the commutating field is being adjusted for com- mutation. The inductive shunt is of low resistance, and is de- signed to have an inductance greater than the commutating field. If the machine has an inductive _ shunt and flashing or violent sparking is produced by throwing a heavy load on and off quickly, try adjusting the air gap of the inductive shunt. With a given winding on the core, the inductance of the shunt may be varied by changing the air gap and the relative induc- 152 tance of the shunt and commutating winding be thus altered. If the current read on the meter in the shunted circuit quickly falls to zero when a heavy load is thrown off by tripping a breaker, and the brushes show sparking, there is too little inductance in the shunt and its air gap should be decreased. The air gap should be adjusted so as to give minimum sparking when the machine is operating with a highly fluctuating load. Motor Operation Some machines are required to run as motors as well as generators. When such operation is specified they are equipped with a switch for reversing the series field, so that they may run as accumulative compound wound motors. Such machines should be tried under load as motors and have shunts adjusted as specified above. If possible the same shunt should be used for motor operation as was obtained when the machine was operating as a generator. In no case should a machine be passed for both motor and generator operation unless it will operate satisfactorily under both conditions without changing the brush position. Compounding, Etc. After satisfactory commutation has been obtained the machine should be compounded and other tests taken as des- cribed for generators without commutating poles. THREE-WIRE COMMUTATING POLE GENERATORS Commutating pole machines equipped for three-wire oper- ation should be adjusted similarly to the above. Care must be taken to see that the shunts on each half of the commutating field are approximately equal. EXCITERS Exciters are tested in the same manner as other direct cur- rent generators, as previously explained. All 125 volt exciters must give at least 175 volts with full shunt field at no load. Most 125 volt compound wound exciters are compounded at both the rated voltage and at 80 volts. On small exciters the brushes are usually shifted ahead of the neutral point to obtain the compound at 125 volts and a shunt placed across the series field for the 80 volt condition. The latter is only an approxi- mate setting and no attempt is made to get extremely accurate results. Stability Test Direct connected exciters should be given a Stability Test. With rated no-load voltage on the alternators, raise and lower the speed 2 per cent above and below normal, noting and recording the voltage change in each case. The change in voltage should not exceed 6 per cent of normal no-load voltage in either case. The no-load voltage setting should always be made with a rising field. 153 THREE- WIRE BALANCER SETS In the operation of three-wire circuits the load often tends to become heavier on one side than the other with a consequent unbalancing of the voltage. To obviate this, small motor- generator sets called "balancer sets" are used. In its most common form the balancer set. consists of two similar machines on one shaft or with their shafts coupled together and their armatures connected in series across the out- side mains. Each machine is wound for one-half the voltage between the outside mains, and their combined rating in amperes is made equal to the probable difference in load between the two sides of the system. This unbalanced load is carried by the neutral wire taken from the balancer at the point where the two armatures are connected. When the load on the system is balanced, the two machines run as motors in series across the outside lines, no work is done, and the only current used is that necessary to overcome the losses of the machines running free. As soon as one side of the system becomes more heavily loaded than the other, the drop in voltage on this side will be the greater and the voltage impressed on the machine on this side reduced. The other machine, having the higher voltage, will tend to run faster than the first and drive it as a generator. The machine operating as a motor will act as a load on its side of the system, lowering the voltage on that side, while the generator will supply current to and raise the voltage on the heavily loaded side. The combined current of the two machines equals the unbalanced load of the system and the total effect is to restore the voltage balance of the system. As the unbalanced load on the system may shift from one side to the other, this action of the balancer must also shift. Either machine may at any instant be operating as a motor and the next instant as a generator. As the direction of rotation is always the same it is impossible to tell, without knowing how the load is balanced, which is the motor and which the generator. Balancer sets are adjusted by loading one side at a time with the required current in the neutral wire. Fig. 73 shows the connections for a compound wound, corn- mutating pole balancer set connected for loading in the Testing Department. These sets may be shunt wound, shunt wound with commutating poles, or compound wound with commutating poles. Balancer sets should receive the same preliminary inspection and tests as d-c. generators and motors, and after being wired according to the correct diagram, should be adjusted for com- mutation, field balance, speed and compounding. Commercial and Adjustment test consists of balancing tests and the operation of the set to demonstrate that it is a duplicate electrically of machines of the same type already shipped and that it is free from manufacturing defects. Balancing tests consist of adjusting both machines of the set so that the voltage across each machine shall always be balanced within 2 per cent. The sum of the two voltages will be equal to the applied voltage. The wiring on balancer sets must be 154 done as carefully as that for motors as either end of the set may be operating at any time as a motor. The same precautions, therefore, must be exercised as when operating a motor. for/ob/e rT&s/s to/ice TC/rca/i Greater ^yVWVWVW— ' Fig. 73 WIRING DIAGRAM FOR TESTING BALANCER SET VL = Impressed volts line VA, VAi = Volts machine A and Ai VF, VFi = Volts shunt field A and Ai AL = Amperes line AA, AAi = Amperes armature A and Ai AF, AFi = Amperes shunt field Aand Ai AN = Amperes neutral Shunt Wound Sets On shunt wound sets the fields are cross connected and should be adjusted and the brushes shifted to such a position that the proper voltage balance is obtained. One side of the set is loaded at a time as shown in the figure. Satisfactory com- mutation and speed must also be obtained, and when such condi- tion has been established with one side running as a generator. 155 the set should be reversed and the other side adjusted to cor- respond. When both sides have been properly adjusted the set should operate with either end running as a motor. Shunt Wound Sets with Commutating Poles If the set is equipped with commutating poles, it should be adjusted with the brushes placed on the mechanical neutral as on other commutating pole machines. After good com- mutation has been obtained (by adjusting a shunt in the com- mutating field, if necessary), the proper voltage balance should be obtained. It should not be necessary to shift the brushes from the mechanical neutral, but if a balanced condition cannot other- wise be obtained the Head of Section should be notified im- mediately. Compound Wound Sets with Commutating Poles On these sets, the commutating field should be adjusted for commutation and the shunt and series fields adjusted for the proper voltage balance, after satisfactory commutation has been obtained. It should be noted that on a compound wound balancer set the machine operating as a motor runs as a dif- ferentially wound machine while the other acts as an accumula- tive compound wound generator. Therefore, care should be taken in adjustment as the set may have enough series field to cause it to speed up to a dangerous point. HEAT RUNS, ETC. After the set has been adjusted the heat runs should be taken by loading one side for the specified time with the required current flowing through the neutral wire. All readings of voltage and current should be carefully checked to see that they are consistent. Saturation may be taken by operating each machine as an individual generator. Core loss may be taken on a set with three or more bearings by the method of belted core loss previously described, the belt being run over the coupling between the machines. On two bearing sets the core loss is obtained by a series of "running light" readings on each machine as follows: With one end operating as a shunt motor read the input with no voltage on the other (a) with brushes down, (b) with brushes up; then (c) with normal voltage on the generator end with brushes down. These readings should then be repeated with the set reversed. From these the core loss of the set may be calculated. SPECIAL TESTS consist of saturation, core loss, input-output, commutation and field balancing tests. INPUT-OUTPUT TEST consists of taking careful measurement of the input and output of the set when connected .as during the heat runs. COMPLETE TEST consists of field balance and adjustment, normal and overload heat runs, core loss or input-output, and commutation tests. 156 CHAPTER 8 DIRECT CURRENT MOTORS The tests on direct current motors may be divided in the same manner as for generators. Preliminary Tests are practically the same as those taken on d-c. generators and the instructions included in Chapter 7 should be carefully followed. When the machine has been wired according to the correct print, the wiring should be checked by the Head of Section, or his assistant, and it is absolutely necessary that the machine should operate in the proper direction of rotation when so connected. Make provision for reading volts and amperes line, volts and amperes field and speed. Direct current motors may be loaded by the methods given in Chapter 7 or by belting to generators. Starting After setting the brushes on the mechanical neutral and observing instructions contained in Chapter 4, page 98, the machine may be started. You must be absolutely certain that there is a full field on any motor before attempting to start it. On starting, the speed of the machine must be carefully followed with a tachometer and the circuit breaker must immediately be opened if the speed rises above the prescribed limits. With the starting rheostat, or water box in the "off" posi- tion the terminals of the rheostat or box must be attached across the open main switch AFTER the circuit breaker has been closed. The lower terminal should be attached first. The resistance across the main switch may then gradually be cut out, and if the speed of the motor is all right, should be entirely cut out and the main switch closed. If the motor tends to run above normal speed, the circuit breaker must be opened and the motor shut down. The connections should be carefully checked to see that the field is wired properly. It may be that the field has been connected directly across the main switch. If such is the case the field current will fall rapidly as the starting resist- ance is cut out and the motor will speed up. To test for incorrect connections in the field, observe the volts field during starting. These will drop if the field is incorrectly connected. Trouble may also be experienced due to reversed polarity, etc., which may be traced out as noted under d-c. generators. MOTORS WITHOUT COMMUTATING POLES Adjustment for Speed and Commutation After the motor has been started it should be adjusted for commutation by shifting the brushes back of the mechanical neutral. This shift is necessary as the electrical neutral of a motor is shifted by the armature reaction in a direction opposite to the direction of rotation. When shifting brushes for com- mutation the speed of the motor must be carefully watched. With no-load normal voltage and full field a speed reading should 157 be taken, the brushes being shifted so that when full load is on, the speed is not less than 7 per cent below nor more than 3 per cent above normal rated speed. With the machine hot the speed must not vary more than 5 per cent either way from the normal rated speed, consequently the full load speed with the machine cold must be within the limits as given above. The same precautions regarding brush fit and the condition of the commutator should be used as for d-c. generators. All compound wound motors should be adjusted with full series field. If this cannot be done, the fact should be referred to the Head of Section. The speed must come within 4 per cent of the rated speed when the machine is hot. Differentially com- pound wound motors should be loaded with care since the series field may be strong enough to overcome the shunt field and cause the machine to speed up and run away. The no-load speed of accumulative compound wound motors should be carefully watched as it may be considerably higher than the rated speed. When the correct running position has been found it should be marked with a chisel and the number of bars shift from the neutral point recorded on the Testing Record. Speed Regulation Speed regulation may be defined as the ratio of the drop in speed from no load to full load divided by the full load speed. On a load run this regulation must not exceed 6 per cent. Heating Tests After the correct adjustment has been obtained the heating tests may be started. The general instructions in Chapters 4 and 7 should be followed carefully. Motors may be loaded by belting to generators, feeding back, or by the circulating current methods described in Chapter 7. In using the method shown in Fig. 65, if the machines are motors, the same connections should be made and the machines thrown together. The voltage of the system must be held by the machine running as a generator. The only correct way of obtaining load is by changing the speed of the set, the brushes having previously been set in the running position. Usually the speed will have to be decreased and the difference between full load and no-load speed will be the normal drop in speed for the motors. Cases have occurred where the speed of the motor, due to armature reaction, increased during the load. In "feeding back," this fact is shown by the motor taking an overload at no-load speed in which case the speed of the loss supply must be increased. In using the method shown in Fig. 66, if two shunt motors are being tested, one machine should be run at normal voltage, current, speed and with full field; the other should be run as a generator with a little higher current and slightly stronger field than it would have under normal condition. The fields of the generator may have to be connected in multiple. The motor should be started first from the electrical loss supply circuit and its brushes shifted for commutation and speed. 158 After exciting the field of the generator and adjusting the voltage between the machines to zero the circuit may be closed. The machines should then be loaded by increasing the field cur- rent of the generator. The brushes must always be shifted carefully while the machines are under load, for a slight change in shift will at once change the load. During the heat run the speed will rise and the field current will fall. After the heat run has been finished and all motor readings taken, the wiring should be changed and the motor readings taken on the machine which ran as a generator. The circulating current method is used particularly in the testing of series or railway motors. In the latter case the machines are geared to the same shaft. i T T ~sj v L T\ ^^~^pp^J^^ ~T v * == "— -— »^_ t \ A -4-X^ - V ^r X 2w v ^t \ >^ \r ^$t \ ^< ^c- + ^ N ^ ^^ S y i. jc ± ^^a± l 3l j 7 A -4 21 _,^ A 1 Xy> _i$t t . J32 - " -£-- 4- -4 ->?W- -^~ 1 m i t y x + h ' ' r I *' 4 -t IL . ± IT :^„: ± . ~ ± 20 40 €0 GO Amperes Ltr. m m fi*0 7000^ [ | ' | | | } l | j | n~T ii" 1 Jrl | y^^Ji ! X" ^^ it ^-^r sm ! ir -^ « W pt&fT $" T $_ _|_ ± i _._41 „ -^h — 1. .AV <$- 1 i i - $ ia- «t j 1 s^t ii __l!l " 1 1 j N f j £ 4~ - 1 K 1 p »'***' '■" • — L_ »_ 1 _ _ l__ ra „-.j£ ="-\j,j_ - '» 1 ■ ! » i — 1 i - — [-) A XJfr\ 4 1 X - ™_ h _±Lrf £.F)e/J j „ ,,-f'' J tttt TXP T \ r m 1 IWfiAt&rtT 1 i l i m Tl mi ii ^-6aX7/vvc-iVi>/?_I_ _ «= +t -fir lu iy 1 1 tj „ i i lu.jgff-Pr — +r- J4J- f(<\*y¥ i H-T- -T 1 M -J j T|| 1 f / >' 1 1 \ / / S 44p/?./?M. f \ / p. c! n«onf600Vo/ts ^ st 7 Ztt > 7 - - 4 ^£*z S ^ T/4 / ^< *' U. I—-* C- — ^ yPjoj^, V / / S ^^4^wgfc i tj y ^ t-h S-** jIK/^ 7 ■ttft/Z' ti%YS L//y r /2S Amperes A/or/n&/ ^Y/ ~^ 40 OO /20 /60 /Iw/oeres Fig. 76 CORE LOSS AND SPEED CURVE OF A 50 H.P., 500 VOLT RAILWAY MOTOR 200 240 Commutating tests on series railway motors should be made by holding normal voltage and operating the machine at loads varying from 33 ^ per cent to 200 per cent normal load. On series commutating pole motors, Interruption Tests are taken. These consist in opening and closing the motor circuit, while the machine is running at various loads and speeds. The machine should stand such tests without arcing over at a 164 line voltage as high as 125 per cent normal. The loads are varied from 33 }/& per cent to 200 per cent normal. Mill motors are tested for commutation by suddenly reversing the direction of rotation under various loads. DEVELOPMENT TESTS consist of General Tests and Special Tests, and are made when an entirely new type of machine is being developed. SPECIAL TESTS consist of speed curves, core loss, and satura- tion tests. In taking a speed curve two similar motors are mounted on a testing stand, the pinion of each meshing in the same gear on a shaft. One motor drives the other as a separately excited generator and is run loaded until the motor is heated to about 50 deg. cent. rise. The speed curve is then taken on the motor rotating in both directions, the voltage being held constant. The resistance of both armature and field should be measured both before and after taking the curve. Core loss should be taken as on any other machine by the belted method, except that the test should be made at about five speeds. Fig. 76. The lowest speed should correspond to about 175 per cent full load amperes (taken from speed curves) and the highest at about 200 per cent full load speed. During this test the machine is separately excited. A saturation curve may be taken as on any other machine by separately exciting the field. Saturation curves at different speeds mav be obtained from data taken during the core loss test. The speed curves, core losses and saturation are calculated as previously explained. The speed curves and core losses should be plotted on the same sheet against amperes line as abscissae and rev. per min. and watts as ordinates. From these two sets of curves another can be developed, which will give the core loss of the motor at any speed or current. The Thermal Characteristic should be obtained by making a series of heat runs at varying amperes, allowing sufficient time to get a temperature rise of 75 deg. cent, on any part except the commutator. Each run should be made at the same constant voltage, the current value for each run varying from 50 to 150 per cent normal. If a sufficient number of heat runs be taken on a sufficient number of motors of the same class, type and form, the horse-power rating for 75 deg. cent, rise may be obtained for any length of run from one-half hour to continuous running. Before starting a heat run, cold resistances and tem- peratures should be taken. After the motor has run continuously for the allotted time, amperes and volts having been held constant with all covers off, and all openings unrestricted, it is shut down, hot resistances measured, and all temperatures taken. The results of the thermal heat run should be plotted, one curve for armature and one for field, against time in hours as abscissas and degrees cent, rise as ordinates. Through zero and the plotted points corresponding to the different loads, lines should be drawn. The intersections of these lines with the line 165 of 75 deg. cent rise gives the time the motor takes to attain 75 degrees rise with the load corresponding to the plotted point through which the line was drawn. From these curves another curve should be plotted with time as abscissa? and amperes load as ordinates. This is an ampere time curve for 75 deg. cent. rise. too 70 *<*) -i I §50 MM 1 „, lt:/7m t 4/t'j?/sf> j Cem&7?/sel /CoM.63'frAse Com.ttJt'/se \ / ''toMSSTTtee — -gfeSkr 1 1 7 ^x^~- m Mi aW $Y o^d^"" §L$l j&^xl^t^>p^- -wr w ^$rvJf vf 1> ^ %1 Y/Z^ +t 7~/4? ±jS-?4S -3-y ? it / \ 1 j 3 4 /SO %/60 /40 /ZO /00 80 60 40 \ \ v \ s, V \ \ t V <> p k *m n /Ts\y *%r n- 4Z /i./z 'Ovfot/t 01 L £// -fff~ 2 3 <4 /ioctrs /?un Fig. 77 THERMAL CHARACTERISTICS OF A 100 H.P., 600/1200 VOLT RAILWAY MOTOR On the same sheet as the ampere time curve is plotted, a curve should be drawn with time as abscissae and horse power as ordinates, the horse power being calculated from the standard 75 deg. cent, characteristics. See Fig. 77. 166 In loading railway motors, as in the Speed Curve, two motors are geared together on the same shaft (see Fig. 78), one running as a motor at the rated voltage and full load current and driving the other as a separately excited generator. The separately excited field of the generator is in series with the motor field, thus giving a normal full load excitation. The armature of the generator is connected to a water box, the resistance of which is varied until full load on the motor is obtained. The run is made for one hour, after which temper- atures are taken. Motor [=|)j^a^j: JT==rt =#=) Generator "&O-0OOOO0O" fte/a 1 Fig. 78 CONNECTIONS FOR LOADING TWO RAILWAY MOTORS Resistances are measured and high potential applied both before and after the test, and, before starting, the speed should be checked in both directions of rotation. The circulating current method is often used in making this test. One out of every fifty of all types of motors should receive the one hour load run. All 600 volt commutating pole motors, excepting those receiving the one hour load run, should be run under load for ten minutes in each direction of rotation. Other motors having their characteristics well established should receive commercial tests. COMMERCIAL TESTS consist in running a motor light for a short period. It is the practice to run four motors in parallel, the fields being connected in series and separately excited by 167 a current equal to full load current of the motor. (See Sketch of Connections in Fig. 79.) With normal voltage held constant across the armatures, the motors are run light for five minutes in each direction of rotation, readings of speed, armature and field current being recorded. With rated voltage across the motors, the fields should be weakened until about twice normal speed is attained. Under these conditions the machine should be run in each direction for five minutes, the same readings as above being recorded. Resistance measurements cold only are taken. High poten- tial tests must be made after this run. Booster <& F/W/ F/e/SJ FMJZ Fi6>M4\ Fig. 79 CONNECTIONS FOR RUNNING LIGHT ON RAILWAY MOTORS Care must be taken that the resistance at 25 degrees cent, and speed come within the prescribed limits already mentioned. STANDARD EFFICIENCY TESTS on all series motors with the exception of railway motors are made by the method of losses and the calculation is identical with that of any other motor. In this case, of course, the amperes armature equals amperes line. See page 433. In making an INPUT-OUTPUT TEST the motors are geared and connected as for the Load Heat Run and are usually run under full load for one hour up to ordinary working temperatures and to get the bearings in good running condition. Before the load is put on, a careful measurement of the armature and field resistances of the motor, and of the armature of the gener- 168 ator is taken by the drop in potential method. Three differen measurements of each should be made with as many different values of current, which should be near the normal load current. Holding constant normal voltage, 12 or 15 different loads ranging from as low as possible to 150 per cent load should be put on, the direction of rotation being such that the motor tends to lift from its bearings. Readings at each load should be taken of the amperes, volts armature and speed of the motor and amperes and volts armature of the generator. The direction of rotation should then be changed and several check points taken in speed and amperes, after which the machine should be shut down and hot resistance measurements made. /300 \ /200 .Vi J/OO ^ /ooo /oo 900 30 800 30 7O0 70 600 60 \ \ V \ s, s -%Cc >Li KC . %c?/?. -f % i ct Vo n j 1 ^ > s s , V 1 1 ^f. ft I 30 /20 Fig. 80 INPUT-OUTPUT CURVES ON A 100 H.P., 600 VOLT, RAILWAY MOTOR Tractive effort The Calculation Sheet 8 and Fig. 80 show the method of working and plotting the data obtained from the input-output test. Unless otherwise specified the tractive effort and miles per hour are calculated for 33 in. wheels. The formulas used are: ,,.. , R. p. m. X diameter of wheels in inches X-n- Miles per hour = — ■= : ,^„^ Gear ratio X 1056 Amps. X volts X efficiency X 252 Miles per hour X 500 The gear ratio is that between the gear and pinion. From these characteristics new ones should be plotted, as shown in Fig. 81, the PR being corrected for 75 deg. cent, rise, and the gear loss assumed as 5 per cent at full load. If the gear loss from test has to be changed at full load, it should be changed in the same ratio throughout the curve. (See Calculation Sheet 9.) COOLING OFF TESTS are made by running the motor under full load, with covers off, for one hour, shutting down and reading temperatures as the machine cools down. For the first hour 169 after the machine is shut down, the following temperatures are read every fifteen minutes: the armature, commutator, field, frame, air in the motor, and room temperatures. After the first hour temperatures should be taken every half hour until the temperature of the hottest point is not more than 25 degrees cent, above the surrounding atmosphere. The results of the cooling off test should be plotted to time as abscissas and degrees centigrade rise as ordinates. The curves for armature, field, commutator, frame and air in the motor, should all be plotted on one curve sheet. ' uu ""rag 1) L, %c?/? = = = = = ~ — % * v s' & 2^ v 70 25^ ^ 7 £ S h f S A*' 3M «&£ v fe §u t ^ d 6& ^ 1 ^ f "■-- T&- ^2000 K 2/7^ 40 \- ^ >£**&,<».- 5? ?> ^ \ S* 30 ^ £ ?!* ^ 7 &/OO0^ /O 20 4L -j ** t **" o o /?U-I^ /20 /GO Amperes 200 260 Fig. 81 SPEED, TRACTIVE EFFORT, EFFICIENCY ON A 100 H.P., 600 VOLT RAILWAY MOTOR DYNAMOTORS Dynamotors are used to supply current at one-half the line voltage of a system and consist of an armature having two distinct windings and commutators rotating inside a common magnetic circuit, having a shunt winding and also a series winding so connected that it is active only during the period of starting. The tests ordinarily taken consist of dynamic balance of the armature in a special frame, a one hour heat run at rated output and running light readings with normal con- nections (but with the ground connection removed) and also at reduced voltage with the series field only. After these tests are finished the dynamotor should be thrown directly on the line and starting characteristics and commutation noted. Core loss when called for, should be taken by the method of motor core loss. Calculation Sheet 27 shows results of a motor core loss on this type of machine. 170 Input-output efficiency is calculated from the readings taken with the machine connected as for a heat run. Calculation Sheet 26 shows results of such test. VENTILATION TESTS Ventilation tests are sometimes taken on Railway Motors. The double pitot tube method is ordinarily used and the velocity and quantity of air delivered calculated using the weight of the standard air. In this cas e V=401oV h 3 at the center of the pipe. Q =3654^4 V I13 using the average velocity as given in Chapter 16, page 313. 17 CHAPTER 9 ALTERNATING CURRENT GENERATORS The tests on Alternating Current Generators may be divided as follows: Preliminary tests, commercial tests, heating tests, special tests, input-output tests, over-speed test, wave form, location of keyway, voltage regulation and static tests. Preliminary Tests consist of drop on spools, resistance measurement, air gap and fitting of collector brushes. The pre- cautions specified in Chapter 4 should be carefully followed. COMMERCIAL TESTS consist of excitation and other readings at no load necessary to demonstrate that the machine is a dupli- cate of the same type already shipped and that it is free from manufacturing defects. After the machine has been started a saturation curve should be taken as described in Chapter 6, page 120, the curve being taken up to full excitation voltage on the field. Care should be used to see that the voltages in the various phases are balanced. Synchronous impedance may then be taken. The object of this test is to determine the field current necessary to produce a given armature current when the machine is running short- circuited. Since the regulation of the machine is calculated from the impedance and saturation curves, care should be taken that consistent results are obtained. The armature . should first be short-circuited; then with the machine running at normal speed and a weak field current, the current in each phase should be read. The field current should be increased gradually until 150 per cent normal arma- ture current is reached, readings being taken simultaneously of amperes armature and field and volts field. Care should be taken not to overheat the windings. Although the speed in this test should be held normal a small variation therefrom will not affect the curve, because e.m.f. -E in the formula, current = = '— A = / „ ^ ^et the term R 2 Impedance VR 2 +L 2 W 2 is small compared with L 2 W 2 , and as E and W vary propor- tionally to the speed, the current remains practically constant. In the calculation of synchronous impedance all readings should be corrected for the constants of instruments and ratios used and a curve plotted on the same sheet as the saturation curve, amperes or ampere turns field being plotted as abscissae and amperes armature as ordinates. See Calculating Sheet 7 and Fig. 82. Phase rotation should be taken after these tests are finished by using a "Phase Rotation Indicator" described in Chapter 2, page 25. See Fig. 12. The terminals of the machine under test whether three-phase or quarter-phase should be connected to the corresponding terminals of the indicator. The indicator should operate on the residual voltage of the alternator but if it will not, a small field current should be applied to the machine 172 under test and the voltage should gradually be brought up to a small amount and the magnet of the meter should revolve in the same direction as the rotor of the machine under test when facing the head end. Be careful not to burn out the indicator. If it rotates in the opposite direction (a) for a quarter-phase machine, a phase is reversed; (b) for a three-phase machine, either a phase is reversed or the wrong leads have been brought out. The head end of a machine is the end at which the coil to coil /OOO S 900 _ f / BOO ./ r l**> / / *m / r / / y ' / / \300 §200 / / / / /oo / / °t / 1 A 2 s4/n 'pert s / JO %vfc f QS wrth' Revolving Shunt Connect -Studs land 3 to the some Phase on I Q and QB Connect Stud 3 to beginning of Phase / Connect Stud 4 to beginning op Phase 2 Fig. 83 CONNECTION BLOCKS whether there is any appreciable current flow from this source. A high reading a-c. ammeter should be connected to low resist- ance leads, one of which is in contact with the revolving shaft, and the other securely fastened to the frame of the machine.. 174 If an appreciable reading is obtained on the instrument, the fact should be reported as a defect to be remedied by insulating the bearing-standard from the base. V d Lead End J i ^ uuu Lead £nd } I 3 5 7 ?z:zz--s A O Machines With Revolving Shunt 5 ■ -^H s - Commutator Col lee tor for A T Machines Col lector Studs hove odd numbers, Commutator Studs have ever, numbers Fig. 84 CONNECTION BLOCKS All machines rated 1000 kv-a. and above must be furnished with insulation under the bearing pedestal. HEATING TESTS Before starting these tests instructions in Chapter 4 regarding thermometers, etc., should be carefully followed. The heating 175 tests on a-c. generators may be divided into two parts; load tests and equivalent load tests. actual ACTUAL LOAD TESTS Actual load tests may be taken by the water box method or feeding-back method. The water box method is similar to that described for d-c. generators. Boxes must be used in each phase and care must be taken to keep the currents in the various phases balanced. The boxes in the different phases of a three-phase machine should be connected in "Y", and the leads from the generator under test should be run to the blades. Not more than 2300 volts should be applied to the standard water box. Machines requiring a higher voltage than this should have transformers placed in the line. In the various sections there are several water boxes good for more than 2300 volts and these should be used whenever possible, rather than transformers. Fig. 85 GRAPHICAL DETERMINATION OF CURRENTS FOR A POWER-FACTOR HEAT RUN Very often it is required to load an a-c. generator at a specified power-factor. In such case a synchronous motor should be connected across the terminals of the generator under test in multiple with the water boxes and should ordinarily be run light, having its field excited to give the required leading or lagging current in the armature circuit of the generator under test. If the latter machine is to be run at leading power-factor the field of the synchronous motor must be excited with a current above its normal excitation for unity power-factor. The machine under test is accordingly run below normal excita- tion. If a lagging power-factor is specified the conditions are reversed. Wattmeters must be used to determine the power- factor of the circuit. The amount of current to be held in the armature circuit of the synchronous motor floating on the line may be determined graphically as follows. Referring to Fig. 85: Let AB = full load current of the generator under test (for a normal load heat run.) 176 Draw angle BAC=the angle whose cosine is the power- factor to be held. Draw BC perpendicular to AC. Lay off CD = minimum input current for the synchronous motor running light. Then BD is the current to be held in the armature circuit of the synchronous motor and AD is the amount of current to be carried by the water boxes. Thus, by holding the synchro- nous motor current at BD (varying the field if necessary) and loading the generator under test on the water boxes until AD amperes are obtained the load of the specified power-factor is obtained and the heat run may be taken. OV Fig. 86 SHIFTING OF PHASES SHOWN DIAGRAMMATICALLY "Feeding Back" Method Two similar alternators may be tested under actual load by direct connecting their shafts and supplying the losses mechanically. It is, however, necessary to shift the stators with respect to each other so that the machines will remain continually out of phase with each other. The vector difference of the voltages thus generated by the two machines will cause a current to flow which may be varied by changing the relative positions of the stators. For example, consider a three-phase machine the phases of which are shown diagrammatically in Fig. 86. The machines should be run at normal speed, with the fields separately excited to a value corresponding to the load at which it is desired to make the test. The value of this excita- tion should be calculated from the saturation and synchronous 177 impedance curves. With points a and a r connected together the voltage across b and b' should be read, the circuit closed and the value of the current flowing observed. Knowing the voltage between phases a-b, a'-b', and between b and b', the angle of phase displacement may be readily obtained. Should the armature current be considerably greater or less than that desired a further trial will be necessary. The current value will vary nearly as the angle of dis- placement so that an approximate value of the angle desired can be found from the value of current and angle previously ascertained. When the value of this angle has been ascertained, the phase displacement should be changed, so as to obtain it as closely as possible. With the machines still connected together as they were originally, the angle of phase displacement pre- viously found will be increased 120 electrical degrees by con- necting a' and b. If a' and c are connected, a still further displacement of 120 degrees is obtained. If with any of these connections, the field of one machine be reversed, a still further displacement of 180 degrees is made. With the connection which gives the nearest value of armature current to that required, a further adjustment may be made by shimming the stator of either or both machines up on one side and taking shims out on the other side. The circuits should then be closed and the heat run made for the specified time. Even with the angles of phase displacement possible with -the various combinations of con- nections and field reversals it may not be practicable to get the desired armature current. In this case, unbolt the coupling and shift the rotor of one machine around one or more bolt holes. The "cut and try" operation should then be repeated. Although thus "cut and try" method is not the best one to use it gives very satisfactory results, especially where it is necessary to make an actual full load test. Two frequency changer sets consisting of a-c. generators and synchronous motors may also be given an actual load run by shifting the phases of the generators or motors with respect to each other. The losses in the sets should be supplied electri- cally from the synchronous motor end. The stators of the gener- ators or motors are usually held in cradles, so that they may be rotated to run in phase with other machines, consequently it is necessary only to turn the frames in their cradles to obtain the proper shift. Each different load of course requires a definite relative position of the two stators. The fields should be excited with the field currents necessary for the test as found from the saturation and synchronous impedance curves. One set will operate direct and the other inverted. If a run is required at a specified power-factor the generator of the set operating inverted should have its field excited at such a value that the specified power-factor is obtained on the gener- ator of the set operating normally. Wattmeters should be used to determine the power-factor. 178 EQUIVALENT LOAD TESTS Equivalent Load Tests may be subdivided into "Open Circuit Heat Run," "Short Circuit Heat Run," "Open Delta Heat Run" and "Zero Power-Factor Heat Run." The Open-Circuit Heat Run as its name implies consists in running the generator at no load and with a field current which gives a predetermined percentage over normal voltage. The run should be continued until the temperatures are constant and the machine then shut down and the final temperatures recorded. The resistance of the field should be measured care- fully both before and after the run. Volts armature and speed should be held constant and readings taken of volts and amperes field. The Short-Circuit Heat Run consists of running the machine until temperatures are constant with its armature terminals short-circuited through an ammeter and with sufficient excitation in the field to obtain a given percentage over normal current in the armature. Amperes armature and speed should be held constant and readings taken of amperes and volts field. Final temperatures should be recorded and the resistance of the armature both before and after the run carefully measured. The Open Delta Heat Run is sometimes made on large three- phase alternators. The phases of the machine should be connected in delta, one side of which is left open. The machine should be run up to speed, the field excited and the voltage across the opening in the delta measured with a potential transformer and voltmeter. This voltage should be approximately zero. The armature should then be wired to a source of direct current sufficient to supply the amount necessary. One side of the open delta should be grounded to protect the armature of the direct current machine from static strain. The other armature terminals should be carefully insulated. Due to harmonics which may exist in the legs of the delta, an alternating cross-current may flow in the winding. This should be measured by an a-c. ammeter and current transformer (if necessary) inserted in the armature circuit. The amount of circulating direct current necessary is then found as follows: Let / = normal rated current of machine under test. V = normal rated voltage of machine under test. ^ T rated kv-a. then / = ;= V3 V Let I\ = amount of cross current found with field excited as specified above. h= amount of direct current required. Then P = Ii>+I 2 * I 2 2 =P-Ii 2 When this value has been determined the voltage of the machine supplying the circulating direct current should be increased until the desired current is obtained. The field of the alternator under test should then be excited to the value necessary to give normal no-load voltage, and the run continued until tempera- 179 tures are constant. Careful record should be made of volts armature, volts and amperes field, direct- and alternating- current amperes armature, and speed. /oo 90 BO 70 \eo % 20 /o 11- -4- -4- ■ ~~-W- — X X ^ ^ v J_ J_ i y\. _J_ J. _|_ .3. Z .«_ >§ ">5i ^ ^ J. yL. A_ / 't r H I I r f t . eo so /20 /40 1 220 | j 1- ZOO 1 t \ J_ lot M i- >»- /eo i pt t 1" r /SO s_ N» "W 4- l r ?r ei o ss MO \/20 X/00 eo eo <*o fr/ct/o/j 7/1 c/ Mb da 'J*' 20 ¥r\ A r#^ ^T L £f A / 0/7C OS zo <40 /ZO /<*o 60 eo /a Fig. 87 EFFICIENCY AND LOSSES ON A 5000 KW., 11,000 VOLT, 257 R.P.M. 60 CYCLE, 3-PHASE A-C. GENERATOR The Zero Power-Factor Run is another excellent method of making an equivalent load run and is often used where two machines of approximately the same rating are available. The 180 generator under test is run as a synchronous motor with its field excited to give full load current. The field is usually over- excited, but there may be cases when under-excitation is specified or a test may be called for in which the field will be intermittently over- and under-excited. Readings should be recorded of amperes armature, volts armature, amperes and volts field and speed, and the run continued until all temperatures are constant. Final temperatures should then be taken and the resistances of both field and armature carefully measured. SPECIAL TESTS consist of saturation, synchronous impedance, open- and short-circuit core loss and wave form. On turbine driven generators air readings will be taken to determine the pressure and amount of air circulating in the various parts of the machine. INPUT-OUTPUT TEST, OVER-SPEED TEST and WAVE FORM have been described in Chapter 6. COMPLETE TEST consists of special tests and heating tests. STANDARD EFFICIENCY TEST is made by the method of losses. Page 437 and Calculation Sheet 14 and Fig. 87 show the method of calculating and plotting results. LOCATION OF KEYWAY It is often required that two machines whose revolving parts are on the same shaft, or are to be direct connected shall operate in series or multiple. In such case the generated voltages must be in phase with each other, and in order to make sure of this fact the key-ways of the machines must be definitely located with respect to each other. This is done by connecting the fields of the two machines in series and exciting them from the same source of power. The revolving parts are then adjusted and the keyways so located, that upon suddenly opening the field switch, no "kick" is obtained upon a voltmeter connected across any particular phase of either machine. This position can best be determined in the following way: Set the rotating part of the first machine with respect to the stationary part so that no "kick" is obtained on a voltmeter across any one phase when the field circuit is suddenly opened. Then set the other machine so that zero "kick" is obtained on that phase which is to be connected to the phase of the first machine on which zero "kick" was obtained. A definite marking should be made upon the machines so that the shop may cut the key-ways in such position that the relative position of the rotors will always remain the same. VOLTAGE REGULATION A test of the voltage regulation of alternating current gener- ators is sometimes made, but more frequently is calculated from the saturation and synchronous impedance curves. In actually determining the regulation, the machine is subjected to normal load with normal voltage held on the armature. With the field excitation held constant, the load is suddenly thrown off and the armature voltage observed. The difference between this voltage and normal voltage divided by the normal voltage is 181 the per cent voltage regulation. Very often, especially on large machines, it is found impossible to run the machine at actual load on account of limited facilities. In such cases it becomes necessary to calculate the voltage regulation from the saturation and synchronous impedance test. This is done as follows: Let V = normal line voltage. / = normal line amperes R =hot resistance between lines. r . ^ , , . rated kv-a. I for three-phase machines = 7^ Vs v T , , , . rated kv-a. I for two-phase machines = -r-== 2V = voltage drop in armature for three-phase machines. v = IR = voltage drop in armature for two-phase machines. Let ai = amperes field on saturation curve corresponding to(F+»). a 2 = amperes field on synchronous impedance curve corresponding to J. The amperes field required to produce n ormal ra ted voltage with full load on the generator will be a s = var+^2 2 . Let Fi=the voltage on the saturation curve corresponding to a 3 . Vi — V Then per cent regulation = — ^ — If it is desired to calculate the regulation of the machine at a power-factor less than unity then I becomes- — ? — - — per cent power-factor and as becomes Vai 2 +a 2 2 — 2a x a 2 sin where = the angle whose cosine is the power-factor. STATIC TESTS Some perfectly standard a-c. generators are given what is known as "Static Test." The resistance and polarity of the field spools are measured and the stationary armature is con- nected to an alternator of the correct frequency and the voltage necessary to overcome the impedance of the winding is measured at several different current values up to 200 per cent normal. Care should be taken not to overheat the windings. For this test the machine is not assembled in bearings, but the field is placed inside the armature and the air gap measured, after which, the field is removed and the impedance test taken. WAVE FORM Wave form is taken with the oscillograph and ordinarily at no load. The Engineers may, however, specify a full load test. In this case the machine is usually "dead-loaded" to eliminate the effect of the wave form of other machines. 182 CHAPTER 10 SYNCHRONOUS MOTORS The tests on synchronous motors may be divided as follows: Preliminary Tests; Commercial Tests; Heating Tests; Special Tests; Input-Output; Over-Speed; Wave Form; and Torque Tests. Preliminary Tests consist of drop on spools, resistance measurement, air gap and fitting of collector brushes. The instructions in Chapter 4 should be carefully followed. When a machine is run as a synchronous motor extreme care should be used in starting it to see that the field circuit is open and that the voltmeter switch is not closed. The special switch designed for this case must always be used. The field of the synchronous motor acts as the secondary of a transformer, and the voltage induced across the rings at starting may be enough to cause serious injury As the machine comes to synchronism this induced voltage falls to zero and the field switch may then be closed. COMMERCIAL TESTS consist of excitation and other readings at no load necessary to demonstrate that the machine is a duplicate electrically of machines of the same type already shipped and that it is free from manufacturing defects. Synchronous motors are ordinarily run as a-c. generators when commercial tests are taken. HEATING TESTS Heating Tests on synchronous motors as on other machines consist of actual load tests and equivalent load tests. In making an actual load test the machine is usually excited with a current to give minimum input on the armature as found from the phase characteristic curves which are taken as follows: PHASE CHARACTERISTIC The machine must be operated from some a-c. source of correct frequency and at constant voltage. A reading of amperes input on all phases should be taken with zero field on the motor, where possible. Starting with a weak field and reading volts and amperes armature and volts and amperes field, the field should be increased by small steps until the point of minimum input armature current is found. Increasing the field current beyond this point increases the amperes armature. On a no-load phase characteristic curve, the watts input at the lowest point should check very closely with the sum of the core loss, friction and windage losses, since the power-factor is unity on synchro- nous motors at this point and the amperes field must equal that found for normal voltage on the saturation curve. These points must be checked with each other to see that they agree. With a weak field the current is lagging and with a strong field it is leading. In taking a no-load phase characteristic the current should rise to a value of at least 50 per cent of full load alter- nating current. A load phase characteristic should be taken in a similar manner to the no-load. The output is held constant and the amperes load recorded in addition to the readings noted above. 183 Care must be taken not to overheat the windings. It is impossible to obtain a zero field point during the full load characteristic, since the current would be so large as dangerously to heat the machine and the torque not sufficient to carry full load output. /oo 90 GO X 70 % 40 JO /O X \ X \ \ X X x \ \ Xl t / i f t R t m i M t W- i /O £0 30 4-0 GO Fig. 88 PHASE CHARACTERISTIC CURVES ON A 187 KV-A., 2300 VOLT, 720 R.P.M., 3-PHASE, 60 CYCLE, SYNCHRONOUS MOTOR All readings should be corrected for instruments and shunt ratios and a curve plotted between amperes field as abscissae and amperes armature as ordinates. See Calculating Sheet 10 and Fig. 88. 184 ACTUAL LOAD TESTS The actual load test on a synchronous motor is usually made by belting or direct connecting the motor to a d-c. shop generator and exciting the field of the motor for minimum input as found above. In taking a power-factor heat run, the field of the synchronous motor should be over-excited to give the required power-factor unless otherwise specified. Wattmeters should be used to determine the power-factor. Synchronous motors which are parts of Frequency Changer sets may be given an actual load run as explained under a-c. generators. EQUIVALENT LOAD TESTS Synchronous motors are usually run as a-c. generators when being given equivalent load test. Sometimes a synchronous motor is given an equivalent load run by loading it on a d-c. generator and running at reduced voltage, having the load brought up to cause full load current to flow in the armature, and having the field held at the value which may be specified. SPECIAL TESTS On synchronous motors consist of starting test, saturation, no load and full load phase characteristics, synchronous impedance, core losses and wave form. Saturation, synchronous impedance, core losses and wave form are taken as for a-c. generators. Starting Tests Starting tests are taken as follows: If the motor is of a new type and rating, starting tests should be made both with and without a compensator. In all cases, however, the motor should first be tested without the compensator. The center line of one pole should be placed in line with the center line of the frame. At the head end of the motor a distance of 180 electrical degrees should be marked off in a clockwise direction from this line. The total length of the scale used should be %$ of the distance between the center lines of adjacent poles for three-phase machines, 3^ for two-phase machines and ^i for six-phase machines. The scales should be divided into five equal parts, each division line being numbered. On each one of these scale divisions the center line of the marked pole should be placed and the motor started. Thus five tests are made to insure that the motor will not stick in any position. See Fig. 89. With one pole moved to position No. 1 and the machine at rest, sufficient current should be sent through the armature to give a reasonable reading of amperes and volts on the various phases and induced volts on the field. The induced volts field should be read with a potential transformer and a-c. voltmeter. The readings with the machine at rest are taken to determine which phase gives the maximum readings of current and voltage so that the latter can be read at the moment of starting. 185 With the instrument switches adjusted to give the maximum reading, the armature current should be increased until the motor starts. Volts armature, amperes armature and induced volts field should be read simultaneously. The starting volts should now be held constant until the motor comes to synchronism, the time required to reach this point being recorded. The machine attains synchronism when the induced -volts on the field fall to zero. Then the machine should be shut down and the tests repeated from each of the other four positions. Enough time must be allowed between readings so as not to overheat the machine and the current must be left on only so long as is necessary to obtain a reading. "1*^ Pole, Fig. 89 METHOD OF DIVIDING POLE ARC FOR STARTING TEST ON A 3-PHASE MACHINE If a motor shows a tendency to remain at half speed the alternating voltage should be increased until the motor breaks from half speed and comes up to synchronism. The voltage required to break the motor from half speed should then be held and recorded until full speed is reached. All starting tests should be recorded on a special record sheet provided for the purpose and a sketch made showing the starting positions. If the motor sticks at half speed a record should be made of this fact. If the test is required with a compensator, the motor should be set with its field in the position where the highest starting current is taken and allowed to rest in that position for at least six hours until the oil is well pressed out of the bearings. This is done in order to obtain the worst starting conditions likely to occur in normal operation. Connections should then be made to the lowest tap of the compensator and with normal voltage held on the line, the starting switch of the compensator should be closed. If the motor fails to start, the voltage must at once be switched off and connections made with the next higher taps on the compensator and so on until the motor starts. Readings 186 2000 VO /aoo so /600 so J400 -'O . /ZOO %60 %*/O0O si SO ^ S " J£ "t s " -+S "" 2 : 4 N* \ N w ^ > s A >k\< ? t 20 40 60 GO %Loae/ /OO /20 /40 22 20 m /6 /4 u -3- ,>.U A ) < -^C2fisXj?esD.C\- .C.£.fye/d- mm. 20 40 eo go /OO /20 /*o Fig. 95 EFFICIENCY AND LOSSES ON A 300 KW, 600 VOLT, 750 R.P.M., 25 CYCLE, 3-PHASE SYNCHRONOUS CONVERTER Starting tests should be made from several different positions of the armature with respect to the field. A scale, corresponding to the distance between collector ring taps, should be laid off on the armature, divided into five equal parts. A point of reference is marked on the field, opposite to which the marked 199 positions of the armature are placed for the successive starts. These positions should be numbered and a sketch showing the numbering be made on the Record Sheet. Having brought point No. 1 opposite the reference point, the a-c. switches should be closed and a moderate field put on the alternator, sending about one-half normal full load current through the converter. Read volts and amperes in the various phases. As it will be impracticable to read all phases at once during the start, cut the ammeter into that phase which shows the highest current and the voltmeter across the phase which indicates the highest voltage, so as to get the maximum readings at the instant of starting. Increase the field of the generator until the armature begins to revolve, when volts and amperes input and induced volts on the field should be read. The voltage across the collector rings should then be held constant, until the converter reaches synchronism, the time required to reach this point from the start being noted. There are several methods of determining whether the ma- chine is in synchronism. One is, the induced volts field will fall to zero; another, the voltmeter across the armature will read a definite voltage, which would vary from a negative to a positive reading if the machine were below synchronism. Readings should be taken on all phases, of volts and amperes after the machine has reached synchronism. The machine should then be shut down, the armature brought to position No. 2 and the test repeated. In this manner all five points should be taken. After these tests have been taken, the time required to bring converter to synchronism should be taken by throwing one-half voltage across the collector rings. Core Losses are taken with the converter running as a gener- ator and results recorded as given in previous chapters. A reading should be taken of the volts across the collector rings as a check on the no load ratio. Calculation Sheet 25 shows the results of a core loss taken by the motor core loss method. STANDARD EFFICIENCY TEST is made by the method of losses. Page 435 and Calculation Sheet 13 shows the method used in calculating the efficiency of a converter. See Fig. 95. COMPLETE TESTS consist of normal and overload heat runs and special tests. Other tests which may be called for on synchronous con- verters are: Compounding Test with Reactance When a converter is required automatically to deliver a con- stant direct voltage, with a load subject to sudden changes, a compound wound machine is used with a definite reactance inserted between the converter and the line. Such reactances must be tested with the machines for which they are designed. A constant voltage is possible, since an alternating current pas- sing through a reactance will increase the potential if leading, and decrease it if lagging. By adjusting the shunt field so that about 20 per cent lagging current flows at no load and the current 200 at full load leads slightly, the strength of the series field can be adjusted so as to give the same voltage at no load and full load. A compound wound converter, running with reactance, must be compounded like a direct current generator. Unless other specific instructions are issued in reference to compounding, hold con- stant the voltage of the alternator by which the converter is driven. Adjust the shunt field to give the correct no-load voltage, then, without touching the field rheostats, put on full load and read the direct volts. If the machine over-compounds, the series field is too great, and gives too much leading current. In this case a shunt must be adjusted across the terminals of the series winding to shunt a portion of the current. On this compounding test, all readings are taken and adjustments made as on a direct current generator without touching the field rheostats after the no-load adjustment is made. Pulsation Tests Since the torque of a converter need only be great enough to overcome that due to its own losses, it is very sensitive to changes in line conditions, viz., excessive line drop or speed changes of the driving unit. Line drop alone will start a machine pulsating, in many cases. Once started the pulsation generally increases rapidly, till the machine falls out of step or flashes over. To prevent pulsation, copper or brass bridges are located between the poles, which act as a short-circuited secondary and oppose sudden changes of the input armature current. Converters of new design are tested for pulsation by inserting a resistance per phase, between them and the driving alternator. The drop through this resistance corresponds to the line drop which will probably occur in practice. Usually 15 per cent drop is used. If two machines are tested together each machine would have 15 per cent drop between it and the driving alternator or there would be 30 per cent between the two machines as shown in Fig. 96. With the two machines running in synchronism self-excited and with the fields adjusted to give minimum input, observe the voltmeters on the d-c. end of the two machines. Any slight pulsation will be shown by these instruments at once. Hold the direct volts constant on one machine throughout the test. With one field held at minimum input value, reduce the field current in the other machine to about one-half minimum input value. If no pulsation is noted, take a full set of readings on both machines, then reduce the field current of the other machine to one-half minimum input value, and watch for pulsation on both machines which now take a heavy lagging current. Take a full set of readings under these conditions. Next adjust the field of the first machine again to the minimum input value, watch for pulsation and take readings. With this field held at minimum input, change the field of the other machine from its value at one-half minimum input to twice the minimum input value, observe and read. The other field is then brought up to twice normal value, readings are taken and the effect of 201 the heavy leading current in each machine noted. Leaving one field over excited, weaken the other field so as to get half minimum input, look for pulsation and take a full set of readings. Next adjust both fields for minimum current and raise and lower one field about once a second between the extreme values used above and repeat this test for the other machine. If no pulsation develops with the high line drop under these extreme conditions the machines are satisfactory. Dynamometer Board Alternator A A Resistance Resistance. Fig. 96 CONNECTIONS FOR PULSATION TEST Input-Output Efficiency Test Input-output tests on small machines are made with the machine running as a converter, dead loaded on a water box. Larger machines are tested in pairs, one machine feeding back on the other with electrical loss supply. The machines are wired exactly in a similar manner to that used in a heat run (circulating current method) special atten- tion being given the wiring to see that no unbalancing occurs in either the a-c. or the d-c. circuits. On the machine running as a converter, wattmeters are connected in the a-c. end, between the converter and the transformers and preparation made for reading d-c. armature and field current and volts. If current transformers are used with the wattmeters, duplicate trans- formers must be used in the other phases of the machine to prevent unbalancing caused by the resistance and inductance of the transformers. With the machine running in synchronism at rated speed with zero load, and all meters connected, hold constant the alternating volts impressed on the converter and take careful readings of all instruments. Then read the current and volts in each phase, as a check on the wiring and balancing of all phases. Also carefully check all instruments for stray fields. Any instruments so affected must be protected by iron shields or their location changed. With full load, repeat 202 the test for stray fields, since any instrument affected will give misleading and erroneous results. With the no-load minimum input field current held constant, carefully read the a-c. input, as shown by the wattmeters, as a check on the no-load losses. As efficiency is usually guaranteed at \i, 3^2, Z A, 1> M and 1^ load, careful readings must be taken at these loads. Each time the load is changed, the converter field excitation must be changed to the minimum input value for that load. This is shown when the sum of the wattmeter readings is exactly equal to the kv-a. input. To obtain this condition every time usually requires several trials and considerable time, so that an efficiency test made in this way is more expensive than when made by the separate loss method. The likelihood of error is also greater. INVERTED CONVERTERS The speed of a converter, running from the a-c. side, is deter- mined by the line frequency. The same machine running as an inverted converter and delivering alternating current operates as a d-c. motor. Its speed depends upon the field excitation and load, and it will deliver a variable frequency, particularly if compound wound. When run inverted, a compound wound machine should have its series field almost, if not entirely, short-circuited when part of its load is inductive, since a lagging alternating current will weaken the field and increase the speed, sometimes causing a runaway. For this reason, care must always be taken when running a converter inverted, to see that sufficient field excitation has been obtained to prevent excessive speed, particularly when another machine is operated as a converter from the inverted machine. SPLIT POLE CONVERTERS The field poles of split pole converters consist of two or more separate and independent parts each equipped with its own field coil. The ratio of the converter is changed by varying the relative strengths of the main and auxiliary wind- ings. The transformers should never be connected delta primary with diametral secondary because of the harmonic current that may flow if this connection be used. The testing instruc- tions will include, besides the regular tests to be made, the volts to be held across the collector rings and the range through which the direct volts are to be varied by means of the auxiliary field. All preliminary tests are taken as for standard converters and the following tests are modified according to instructions below. Phase Characteristics Phase characteristics should be taken under three different conditions of excitation. NO-LOAD PHASE CHARACTERISTICS (a) Hold the direct volts constant and vary the main field with the regulating and compensating fields unexcited. (b) Hold the alternating volts specified in the testing instructions and with the main field only, find the main field 203 current for minimum input. (This may check with [a].) Set the main field rheostat to give minimum input current as just determined and vary the compensating field while using the regulating field to maintain the direct volts constant at the lowest limit. (c) Same as (b) except it is taken at the highest limit of direct volts. NOTE. — In case there is no compensating winding take curves corresponding to (b) and (c) by holding the direct volts constant with the regulating field while varying the main field. FULL LOAD PHASE CHARACTERISTICS The full load phase characteristics should be taken in the same manner as the no load, except that in all cases the current in the d-c. end should be held at the value necessary to give the rated output of the machine at the voltage on which the kilo- watt rating is based. Voltage Range Curves Voltage range curves are taken by holding the impressed volts constant and, with the main field rheostat set for minimum input current as found in (a) of the phase characteristics varying the current in the regulating field to obtain the specified range of direct voltage. Minimum input current must at all times be maintained by varying the compensating field. NOTE. — In case there is no compensating winding two curves should be taken. (1) Holding the main field rheostat constant. (2) Holding minimum input current by changing the main field rheostat. Curves are plotted with direct volts line as ordinates and amperes regulating field as abscissae. Similar curves should be obtained for full load conditions. Core Loss and Saturation Two core loss tests are required to cover the various condi- tions of operation. (1) Vary the direct volts by means of the main field only with the auxiliary field unexcited. This test is the same as for a standard machine. (2) Holding^ the alternating volts constant at the value specified in the instructions and with the main field rheostats in the position determined from (1) for obtaining the specified alternating volts, vary the regulating and compensating wind- ings to change the direct volts throughout the range. (It will be found necessary to vary the compensating winding in order to hold the specified alternating volts.) NOTE. — If there is no compensating winding, change the main field rheostat to hold the alternating volts constant. Saturation curves should be taken under the same conditions as core loss. 204 Running Light Readings Running light readings from the d-c. end should be taken under three different conditions. (a) Holding the specified alternating voltage using the main field onlv, and allowing the direct volts to come what they will. (b) Holding the minimum direct volts and the specified alternating volts by varying the regulating field, and varying the compensating field to obtain correct speed. (c) Taken in the same manner as (b) except at the maxi- mum direct volts. Heating Tests The heat runs should be made by holding the specified alternating voltage, varying the regulating field to obtain the desired direct voltage and adjusting the compensating winding to obtain minimum input. The main field rheostat should remain in the position found in obtaining the specified alternating voltage with normal current output and minimum current input when the compensating and regulating fields are unexcited. On those machines not equipped with compensating field, the main field must be varied to obtain minimum input. COMMUTATING POLE CONVERTERS The brushes of the commutating pole converter should be set on mechanical neutral for best commutation. This point is located by placing the armature bars, which are painted red, central with respect to a main pole, and then setting the brushes so that the center of the brush comes over the center of the red mark on the commutator as specified under "Commutating Pole Generators" in Chapter 7. It sometimes may be necessary to shift the brushes slightly forward to secure a falling voltage characteristic under load. When adjusting the commutating field on a converter, in order to determine whether it has the proper field strength, run the machine at full load or as near this value as possible, and take the drop from the pigtail of one brush to various points on the commutator under the brush. If the drop is the same to all points under the brush the adjustment is cor- rect, but if it is higher on the trailing side the commutating field is weak and if higher on the leading side, the field is too strong. Most commutating pole machines have a brush raising device to lift all except two pilot brushes from the commutator during the period of starting from the a-c. end. This device should be carefully examined to see that it operates satisfactorily, that it does not bind, that it raises all the brushes (except the pilot brushes) well off the commutator and that it allows all the brushes to make proper contact on the commutator with plenty of allowance for the wear of brushes. The pilot brushes are for the purpose of getting field on the machine and correcting reversed polarity if necessary. 205 Converters with A-C. Boosters Commutating pole converters which have an a-c. booster are equipped with an auxiliary shunt winding on the commutat- ing poles. The strength of this field is controlled by means 'echanica.Ho Connected. Fi e. /a /?h&osta.t Fig. 97 CONNECTIONS OF A-C. BOOSTER FIELD AND AUXILIARY SHUNT COMMUTATING FIELD WITH CONTROL FOR SYNCHRONOUS CONVERTER HAVING COMMUTATING POLES AND A-C. BOOSTER of a double-dial rheostat, which is mechanically connected and operated with the double-dial rheostat in the booster field, and an auxiliary resistance which is divided into steps that are 206 controlled by contactors. These contactors are set to operate at various loads thus changing the resistance in the shunt commutating field according to the load on the converter. (See Fig. 97.) The double dial rheostat takes care of any change in commutating field strength made necessary because of a change of the direct voltage of the converter. The contactor-controlled resistance is set for the maximum value of auxiliary field which will give good commutation at no load. The load is then increased to the maximum value which can be carried with good commutation at this field strength. The first contactor should be adjusted to close at this value (which will be about 40 per cent normal load) and the auxiliary field strength thus increased to the greatest value permissible without sparking. The load should then be increased to the maximum which will not cause sparking at this setting (which will be about 85 per cent normal load) and the second contactor adjusted to close at this point. The same operation should be repeated for the other two contactors which should be set to close at about 110 per cent and 130 per cent normal load. The only phase characteristics which need be taken on this type of machine are those with the booster field unexcited and are the same as those described for standard converters. The voltage range curves should be taken at no load and full load with the alternating volts held constant and are similar to those for split pole machines without compensating windings. The booster field is used in place of the regulating field. Core loss and saturation curves should be taken. (a) With the main field of the converter excited (booster not excited). (b) With the booster field excited and the converter not excited. The alternating and direct voltage of the converter should be read in each case. Other tests should be taken as previouslv described. MOTOR CONVERTERS A motor converter consists of a standard synchronous con- verter and an induction motor. The induction motor has a wound rotor with taps brought out to a set of common rings that take the place of the collector rings for both motor and converter. The voltage of the induction motor rotor is the alternating voltage of the converter. The advantage of the motor converter is that high tension (up to 13,000 volts) may be applied on the stator of the induction motor, the rotor delivering low voltage to the converter. Hence the intervening bank of transformers always necessary with a synchronous converter are not required. No reduction of power-factor is caused by the induction motor, since unity power-factor may be maintained with the motor converter by proper adjustment of the field of the synchronous converter. Caution should be observed when when staiting a motor converter to see that it does not exceed synchronous speed. This synchronous speed is always the syn- chronous speed of a machine having a number of poles equal to the sum of the number of poles on the synchronous converter and induction motor forming the motor-converter. 207 CHAPTER 12 INDUCTION MOTORS The tests made on an Induction Motor either for Engineering information, or for checking guarantees may be divided as follows: Preliminary tests; commercial tests; heating tests; special tests; input-output tests. Preliminary test consists of air gap, resistance measure, and inspection as contained in the instructions in Chapters 3 and 4 which should be carefully followed. Special measuring scales are used in taking the air gap of Induction Motors, as noted on page 83, Chapter 3. Great care should be used in taking both the stationary and revolving gap measurements. Ordinarily there should be as many points measured as there are openings in the end shield. On machines equipped with pedestal bearings at least eight equally spaced points should be taken. Resistance measure is generally made between terminals. On some machines the separate phases are each brought out to a terminal block. Whenever the resistance is measured per phase it should be clearly indicated on the record sheet. Quarter-phase machines are usually measured between terminals 1-3 and 2-4. Detailed descriptions of the apparatus and methods used in resistance measurements are given in Chapter 2. When a motor is delivered to test it bears a tag on which the resistance between terminals as measured by the Armature Department, is written. This value is generally accepted by the Testing Department and the machine need not be re-measured except when heat runs or special tests are to be made. All heat runs and special tests should be preceded by a resistance measurement taken when the machine is cold and a careful measurement by thermometer of the machine windings. Commercial Tests Commercial tests consist of preliminary tests, excitation readings, stationary impedance, and voltage ratio on Form M and Form P motors. The excitation readings consist of taking running light readings of volts and amperes with normal voltage impressed on the stator. The windings of phase wound rotors must be short circuited. Form L and Form P rotors should be short-circuited by means of the short-circuiting switch provided on the motor; Form M rotors should be short-circuited by con- necting the brush-holders together with a short cable. The brushes should be sanded to a good fit to reduce the -contact resistance as much as possible. In starting, the voltage should be applied gradually or in steps, the lowest being about one- quarter of the normal voltage. The majority of motors should start on one-fourth normal voltage with the rotor short-circuited. The voltage necessary to start must be recorded. The bearings must be watched carefully to detect any undue heating, especially in the case of high speed machines. End play must be tried out, both with and without voltage applied to the stator. A tachom- eter reading of speed should be taken and recorded to show 208 that the motor is running at the correct speed for the frequency of the circuit used, and also as a rough check on the frequency of the driving alternator. After the motor has been run for several minutes to show up any defects the readings of volts and amperes should be made and recorded. Care should be taken to detect any unbalancing in the voltage or current in the different phases. Stationary Impedance consists of taking readings of volts and amperes, at normal rated amperes, with the rotor short- circuited and blocked with the clamping device furnished for this purpose. On Form K motors, this value will be practically the same for any position of the rotor. On motors having phase wound rotors, it is necessary to vary the position of the rotor, with respect to the stator, in order to obtain the max- imum and minimum effects. Normal amperes is first obtained with any convenient position of the rotor, and the corresponding voltage is held constant during the shifting of the rotor position. This voltage is generally found to be about one-fifth of the rated voltage of the motor, a fact which will serve to detect any gross error which might be made in testing. On Form L motors, a reading must also be taken and recorded with the resistance in. Close attention must be given to current and volt- age balance on the different phases and much care must be used to avoid applying excessive currents and damaging the winding. Voltage ratio readings must be taken and recorded on all Form M and Form P motors. This consists in applying normal voltage to the stator winding, and measuring the voltage be- tween rings on the rotor winding, the rotor being open-circuited and held stationary. The primary exciting current must also be read and recorded. HEATING TESTS Heating tests generally taken on Induction Motors may be divided into actual load runs and equivalent load runs. ACTUAL LOAD RUNS The actual load runs may be sub-divided into normal load, overload, crane motor, and intermittent heat runs. They are usually made by belting or direct connecting the motor to a d-c. shop generator and holding normal voltage and the speci- fied current. The instructions in Chapter 4 relating to thermom- eters should be followed carefully. Readings should be taken every half hour on normal load runs, and every fifteen minutes on overload and crane motor runs. Crane motor heat runs are taken on motors designed for intermittent service and are generally made holding normal voltage and current for a half hour. In some cases the runs extend over a period of one hour. Readings should be taken every fifteen minutes. Intermittent heat runs are usually made according to instruc- tions from the Engineering Department. The Induction Generator method is sometimes employed in making load runs on Induction Motors. Two similar induction 209 motors are belted together and run in parallel from the same alternator which supplies the losses. See Fig. 98. In order to get full load in both machines, the diameter of the pulleys must differ by a percentage equal to double the full load per cent slip. In starting, the switches A are closed and the motor allowed to come up to speed, until the speed of the motor running as a generator is above synchronism. The alternator field is opened momentarily, while the switches B are closed. The circuit in the alternator field is then closed again, and full load current flows through the two machines. No changes in Fig. 98 INDUCTION GENERATOR METHOD OF FEEDING BACK load can be made without changing the pulley ratio and it is absolutely necessary that this ratio be correct in order to obtain full load. Several modifications of this method are possible. The shafts of the two machines may be direct connected or belted together and one winding of the machine to act as the induction generator be separately excited with either alternating or direct current and the other winding connected to water boxes. In this method the induction generator cannot be a Form K machine. Another modification sometimes used is to wire the induction generator to the synchronous motor of a motor-generator set and load the set, the field of the synchronous motor being adjusted to supply the exciting current for the induction gener- ator. Slip readings should be taken during all heat runs as des- cribed on page 217. EQUIVALENT LOAD RUNS Equivalent load runs are generally made on large motors which it would be difficult to load on account of the large amount of power required. The heating due to iron losses is obtained by running the motor light at normal voltage until the temperatures of the various parts become constant, readings being taken and recorded as in actual load heat runs. The heat- 210 ing due to copper losses is obtained by running the motor under partial load at a voltage less than normal, and holding normal and overload currents. From the results obtained in these tests the temperatures which would be obtained under actual load con- ditions may be approximately determined. SPECIAL TESTS Special tests consist of excitation curves, impedance curves, slip curve, stationary torque test and starting tests. The excita- tion, impedance and slip curves are very important, since it is from these curves that the data are taken for the calculation of the characteristic curves of the induction motor. These curves are generally accompanied by torque tests and occasionally by starting tests. Excitation Curves consist of a series of readings of volts, amperes and watts, taken at different voltages when the motor is running light, the frequency of the applied voltage remaining constant. The motor should be so located that all conditions affecting its operation remain unchanged throughout the test. A solid foundation is necessary to prevent vibration at full speed. The driving alternator should be at least three-fourths of the kilo- watt capacity of the motor. It should be driven by an endless belt or by direct connection to its driving motor to avoid pulsa- tions in the instrument readings. The transformers and other apparatus must be connected so that the alternator is working under normal conditions, since satisfactory wattmeter readings cannot be obtained if the alternator is run too low on its satura- tion curve. Transformers when used must be well balanced and must not be forced beyond their voltage range. The alter- nator used should have a sine waveform. The testing table must be adapted for wattmeters. If the voltage be too high for direct reading on the wattmeters and voltmeters, multipliers or potential transformers must be con- nected between the points measured and the instrument; similarly, if the current be too high for direct reading, current transformers must be used in the wattmeter and ammeter circuits. On motors of less than 20 h.p., the potential lines must be attached on the generator side of the testing table, since, if they are attached to the motor side of the table or to the motor terminals, the exciting current of the potential transformers passes through the wattmeters. Although this current is small, it may be quite an appreciable percentage of the exciting current of a small motor, and the error involved may cause an abrupt break in the curve whenever a potential transformer ratio is changed. In the case of large motors, the exciting current of the potential transformer is so small in comparison with that of the motor, that the incidental errors are negligible. When multipliers are used the above precautions may be disregarded since they are non-inductive. On large motors the potential leads should be connected to the motor terminals to eliminate the line drop in switches and cables leading from the table to the motor. The 211 current leads to the wattmeters and ammeters should be twisted together throughout their length and should be free from sharp bends or loops. All connections must be bright and clean. The short-circuiting switches must always be closed when instru- ments are changed. On circuits of more than 500 volts all instruments must be discharged to eliminate static charge. Do not ground the secondary circuits of the potential trans- formers. The iron cases of oil-insulated potential transformers should be connected together and grounded. Each man should become thoroughly familiar with the characteristics and limi- tations of instruments and transformers as explained in detail in Chapter 2. In starting up, the same precautions should be observed as in commercial tests. After preliminary inspection of wiring, bearings, etc., the line switches of the testing table should be closed. Always see that the wattmeter short-circuiting switches are closed in starting, or whenever a change is made in the generator field excitation. The exciter field switch should be closed, and the voltage brought up gradually until the motor starts and reaches normal speed. The motor should then be inspected to see that it is operating normally. The amperes and volts in the different phases should be read, and any unbal- ancing discovered and a few check readings made with a dif- ferent set of instruments. The end play must be tried out, since defective end play may cause friction losses, which would render the excitation curves inaccurate. Small motors should be run about 1^ hours and larger ones at least 2J^ hours, in order to obtain constant friction, before beginning the curves. In taking an excitation curve on a quarter-phase motor both wattmeters read positive. However, in the case of a three-phase motor, one wattmeter reads negatively through the upper portion of the curve. It is, therefore, necessary to deter- mine the algebraic signs of the readings of both wattmeters before beginning the curve. Adjust the circuit so that both wattmeters show a positive deflection on the scale, then open one of the phases in which a wattmeter current coil is connected and observe the other instrument. If the needle drops off the scale below zero, the instrument reads negatively. If the needle drops to some value above zero the reading is positive. This process must then be repeated for determining the sign of the other wattmeter. In taking the data for the curves, the frequency of the alternator must be held constant. A value of about 125 per cent normal volts should be used for the first reading. Readings of volts, amperes, watts, and frequency must be made and recorded. The volts should then be decreased in steps to give 15 or 20 points on the curve, down to a value of 10 or 15 per cent normal volts. At this point the motor becomes unstable. As readings are taken on the descending curve, the instrument with the negative sign will read less than the positive reading instrument, and its readings fall off more rapidly, becoming less and less until zero is reached and its sign changes. When it becomes positive 212 its current leads must be interchanged. The two most important points on the excitation curve are amperes and watts at normal voltage, and friction watts. These readings determine the core loss of the motor. Several readings only a few volts apart §4000 75 3500 65 3000 55 2500 45 2000 35 1500 25 1000 15 500 -E t I -Z tt It 17 + t-r-t- + 4 U /Jr MUhttsj 1/ t-j 7 -E 4 1 t t-f -t / I/Amps. J // /aMmps. # t afHb^ V J Jl f -X 7 z y A -J- / Z + y /- T s t a -^ ■**- ^7 ==r y S ^ s> ^=_->" j v 100 200 300 400 500 600 Vo/tS Fig. 99 EXCITATION CURVES ON A 100 H.P., 6 POLE, 500 R.P.M., 440 VOLT, FORM M, 3-PHASE INDUCTION MOTOR should be taken on each side of normal voltage. The volts and amperes in the different phases should be read at normal volts, and at two or three other points in the curve as a check on the phase balance of the motor. These readings should be recorded. 213 As the lowest point on the curve is approached, a large number of readings should be taken, since it is from these readings that the friction watts of the motor are determined. In many cases hunting begins at low voltage. This causes the wattmeter needle to swing with a slow beat. Reliable readings can generally be obtained between beats but care must be used to avoid taking readings when the motor is accelerating or decelerating. Bad cases of hunting are not numerous. As a check on the three-phase curve, single- phase readings of several points around normal volts should be taken on the two phases in which the wattmeters are connected. Volts, amperes and watts should be read as in the three-phase curve, A few check readings should also be made with a different set of instruments. Before shutting down, curves should be plotted using volts as abscissae, and amperes and the algebraic sum of the wattmeter readings, as ordinates. The single-phase amperes are theoretically 1.73 times the three-phase or twice the quarter-phase amperes. Practically, however, the single- phase amperes have a value from 1.4 to 1.8 times the polyphase, for either three-phase or quarter-phase motors. The single- phase excitation watts generally come about 10 per cent higher than the polyphase on account of higher PR losses, the iron losses being practically the same whether the motor is running single-phase or polyphase. The temperature of the laminations should be recorded at the end of the test. The calculation of the excitation curves is done in the Cal- culating Room. The instrument readings are corrected by means of the calibration curves furnished by the Calibrating Laboratory. The data are then worked up, and the curves plotted. The data of a calculated excitation test are shown on Calculation Sheet No. 16. Fig. 99 shows a typical set of excita- tion curves, plotted from this data. Impedance Curves consist of a series of readings of volts, amperes and watts, taken at different values of current, when the rotor is blocked and short-circuited, the frequency of the applied voltage being constant. The test table arrangement is the same as that for the excitation curve. The rotor of a squirrel cage (Form K) motor is a sym- metrical bar winding; therefore, the impedance of the motor is practically the same for any position of the rotor relative to the stator. In Forms L, M, and P motors having phase-wound rotors the impedance varies with different posi- tions of the rotor relative to the stator. It is therefore neces- sary to determine the rotor positions at which the impedance is maximum and minimum so that the rotor may be blocked on an average position for the impedance curves. For accomplish- ing this, a position curve is taken. Before taking the position and impedance curves, the rotor must be short-circuited. This is accomplished in Forms L and P motors by means of the short-circuiting switch and in the Form M motor either by a short cable connected directly to the collector rings, or by short- circuiting the brush-holders, using metallic brushes in order to reduce the contact resistance to a minimum. 214 Position Curve. In taking the position curve, an angular distance should be marked off on the end shield, equivalent to one-half of a pole pitch for quarter-phase motors, or two thirds of a pole pitch for three-phase motors. This space should then be pointed off into about ten equal parts. A pointer should be attached to the motor shaft or pulley so that its outer end will pass over the division marks. The pointer is first set on position Xo. 1 and the rotor blocked so that it cannot move from that position. The switches should then be closed uv -■ /34 J~ L 131 fY -i 4 -^v ,28 X -, h- J 4^ t V %m t v- f 4 I t t t 4 *\/?d -i I L — . t /u 7 i t r 7 W t A 1 ± W 4 4 \4 mi 4 ^ t At IZ0 Zt AT ^ na h \t 118 eh 1 lb 1 M I 2 3 4 5 6 7 8 9 /Position Fig. 100 POSITION CURVE ON A 100 H.P., 500 R.P.M., 25 CYCLE, 440 VOLT, FORM M, 3-PHASE INDUCTION MOTOR (Test Taken at 63 Volts) and the impressed voltage increased gradually, until a value of about normal amperes is obtained. Volts and amperes on all three phases should be read and recorded to make certain that there is no unbalancing on the different phases. Holding the same volts as in position Xo. 1 the rotor should be turned until the pointer is over position Xo. 2 where the amperes should again be read. This is repeated on each of the succeeding posi- tion?. A curve should then be plotted between position number as abscissae, and amperes as ordinates (when this curve is plotted for Engineering Data, the ordinates used are the amperes at normal volts found by multiplying by the ratio ,t \ ■ . ). The rotor is blocked for the Impedance -oltage used in test/ * Curve on the position which gives an average value of current. See Fig. 100 and Calculation Sheet 17. 215 fe Impedance Curve Having blocked the rotor in any convenient position, in the case of a squirrel cage rotor, or on the average position as shown S * r 1* 4 | | 7 ZdnS L- 340^ f- 8 3 7 7/7/7 1 i 7 7 t ■' *■ 7/T/7 ' / Lk)U J y r £ 7 / f / //C / .r c \34>Watbs S34>JrnD y J ' > "' f- / / J J //drfrnps I4U f— ' Jr ■x. i j X tXXl inn 1 / / /ft watts IUU fry/ 2 ... J s n £f) , J i -XT / -XT. T \a 70 -XX -XX n n£*dL— ' "0 10 ZO 50 4C 50 60 70 60 90 /00 //0 120 /30 Vo/ts Fig. 101 IMPEDANCE CURVE ON A 100 H.P., 500 R.P.M., 25 CYCLE, 440 VOLT, FORM M, 3-PHASE INDUCTION MOTOR by the position curve in the case of a phase-wound rotor, the impedance curve may now be taken. The readings of volts, amperes and watts should be taken beginning at the lower part 216 of the curve, the current readings increasing in steps until a a value of 150 per cent normal amperes is reached. Up to this point about 12 or 15 readings should be taken, special care being used to get several good readings at and near normal amperes. Above the 150 per cent normal ampere point the wattmeter read- ings may be discontinued, the curve of volts and amperes alone being extended with several points, to a value of 300 per cent normal amperes. Great care must be used not to overheat the motor windings. A set of phase-balance readings should be taken at normal amperes. Single-phase check readings should be made on the two phases in which the wattmeters are con- nected, at a voltage equal to that necessary to obtain normal amperes on the three-phase curve. The single-phase impedance amperes should be times the three-phase at the same volt- age. The single-phase impedance watts should be Y2 the three- phase at the same voltage. In taking the curve data, the cur- rent should not be held on the motor any longer than is neces- sary to secure a reading. After each reading the exciter switch should be opened until ready to take the next reading, thus keeping the temperature of the motor more nearly uniform. Final temperatures of the rotor conductors should be recorded. Curves should be plotted using volts as abscissae, with amperes and the algebraic sum of the watts as ordinates. The volt-ampere curve is a straight line, curving slightly upward on the higher values. Single-phase amperes are practically equal to the polyphase, in the case of quarter-phase motors; or about 86 per cent of the polyphase for three-phase motors. Single-phase watts should be about one-half of the polyphase, for either quarter-phase or three-phase motors. The calculation of the impedance curves is done in the Calculating Room. The data of a calculated impedance test is shown on Calculation Sheet No. 19. Fig, 101 shows a typical set of impedance curves, plotted from the data given there. Slip Curve. There are several methods employed by the Testing Department for measuring the slip of induction motors, among which the following are the more important: First, by means of a slip indicator; second, by means of an arc lamp and revolving disk; third, by means of a voltmeter; and fourth, by means of a revolution counter. The method employing the slip indicator is the one most commonly used. The construction and operation of this instru- ment are described in detail in Chapter 2, page 27. The arc light and revolving disk method is a good one but it requires more time to set up the apparatus than does the slip indicator method. A disk (see Fig. 102) having as many white and as many black sectors as there are poles on the motor, is attached to the shaft of the motor, so that it revolves with it. This disk is illuminated by an alternating current arc lamp which is operated from the same alternator as the motor. Assume a six pole 60 cycle motor running at the synchronous speed of 1200 r.p.m. or 20 revolutions per second. Then 20X6 or 120 217 black sectors pass a stationary point on the circumference of the disk, in one second. As the frequency is 60 cycles, the arc lamp will give 120 maximum illuminations per second. The black sectors, would therefore appear to be stationary. Practically, the induction motor cannot run at synchronous speed, and the slip, at each maximum illumination will cause each black sector to lie a small angle behind that seen by the previous illumination. These successive differences in position appear as sectors rotating backwards, which can be followed by the eye. The difference between the actual speed and the synchronous speed of the motor can be counted. Fig. 102 DISK FOR MEASURING SLIP OF SIX-POLE MOTOR The voltmeter method affords a very accurate and con- venient scheme for measuring the slip of motors having collector rings. The alternating voltage drop across the brushes is read by means of a low reading d-c. voltmeter. Every time the rotor slips an angular distance of two poles behind the synchro- nous revolving field of the stator, a complete voltage cycle is generated in the rotor winding. The d-c. voltmeter will be deflected in a positive direction every alternate half wave or once everjr cycle. Therefore, by counting the number of positive beats per minute of the voltmeter and dividing this value by one half the number of poles, the slip of the motor is obtained in revolutions per minute. The method employing^ a revolution counter is generally used in the case of high speed machines where it is not possible to measure the slip by any of the methods above described. It consists in reading the number of revolutions of the rotor for a known interval of time by means of a revolution counter. The difference between the speed thus measured, and the synchro- nous speed, gives the slip of the motor in rev. per min. Several readings should be taken and averaged, when this method is employed. In all of the foregoing methods for taking slip, it is very neces- sary that the load and impressed voltage on the motor, and the 218 frequency of the driving alternator, remain constant while the readings are taken and in each case the speed must be checked with a speed counter. Slip readings must always accompany heat runs. When special tests are made, a slip curve should always be taken. This curve must have readings at no load, and at 50, 75, 100 > t J 1 - T 7 " y ZaZ' ti Z - / f J / I t / _ ! / y / / T / I f / ZL z_ y ^t 7T_ AO m 120 160 » 200 220 Fig. 103 SLIP CURVE ON A 100 H.P., 500 R.P.M., 25 CYCLE, 440 VOLT, FORM M, 3-PHASE INDUCTION MOTOR and 125 per cent of normal load amperes. Sometimes it is not possible to hold normal voltage on the motor on account of the large amount of power necessary. In such cases the highest obtainable voltage should be held and the voltage and current should be reduced from normal in the same proportion. The motor should always be heated to its normal running tempera- ture at the time the slip readings are taken. All readings of volts, amperes, and slip must be recorded. A typical calculation 219 of a slip curve may be found on Calculation Sheet No. 18. Fig. 103 shows a slip curve plotted from the data given. Stationary Torque Tests. Two methods are employed for measuring stationary torque, one in which a spring balance is used, the other in which a special torque indicator is used, each in con- nection with a lever arm attached to the shaft. The first method applies to motors having squirrel cage rotors, in which the torque is practically constant for varying positions of the rotor relative to the stator. The second method is used on motors having phase-wound rotors, in which the torque is not constant for all positions of the rotor. T S Fig. 104 MEASUREMENT OF TORQUE BY MEANS OF SPRING BALANCE In the first method the lever is clamped to the pulley or shaft as shown in Fig. 104. The size and length of the lever depends on the rating of the motor, the lever and spring balance being chosen to give a maximum reading at about % of the capacity of the balance used. Torque at 1 ft. radius = — In estimating the length of lever needed, allowance should be made for at least 175 per cent of full load torque. The balance and length of lever L should be chosen to make ( W-\- F-\- T) (see below) equal to at least twice (W+F). Let the point of attachment to the lever be at X. Then XF = the length of the lever arm. On the frame of the motor, a mark should be made at M, correspond- ing to the position of the pointer P, when the distances TX and SY are equal. If the weight of the lever is not sufficient to over- come the friction of the bearings and allow it to turn downward of its own weight, attach the additional weight, W. Open all line switches, thus doing away with any torque effect resulting from residual magnetism of the alternator field. By means of a suitable windlass, raise the lever slowly, pulling vertically on the spring balance H. As the pointer passes the mark M read the tension as indicated by the balance. Call this reading (W-{-F), W being the force due to the weight of the lever and F 220 the force due to bearing friction of the motor. Raise the lever until the pointer is some distance beyond M, then lower it slowly allowing the force of gravity to pull it toward the floor. When the pointer passes the mark M, the spring balance should again be read. Call this reading (W — F). The lever should be moved as steadily as possible, otherwise the tension indicated by the spring balance will fluctuate. Several readings should be taken as described above. Now close the line switches and bring up the line current gradually to a value of 200 per cent normal amperes. In so doing, watch the motor carefully to see that it does not tend to turn in the wrong direction. Take readings in the same manner as that just described. Call the reading taken as the lever is raised (W+F+T) t and that taken as it is lowered (W—F+T), T being the force due to the stationary torque of the motor. The readings should be recorded as follows: Volts Amperes (W+F) (W-F) (W+F+T) (W-F+T) T. Solving for the value of T, and knowing the length of the lever arm in feet, L, the stationary torque is calculated from the formula Stations To rqU e=(^L^y Xi xr Care must be taken to see that the motor does not overheat. To get reliable readings the frequencv of the alternator must be held constant. If any variation of (W+F+T) and W-F+T) should occur with change of rotor position, the maximum and minimum values should be recorded. As a check on the readings taken, the lever should be loosened and the rotor turned to a different position relative to the stator. Here the lever should be again clamped to the shaft or pulleys and readings of (W+F+T) and (W—F+ T) taken. This should be repeated for several dif- ferent positions. The temperature of the rotor conductors must be taken and recorded at the end of the test. The second method of taking torque applies to Forms L, M and P motors having phase- wound rotors. The data is taken by mean of a special torque indicator described in detail in Chapter 2, page 29. The indicator must be fastened to the lever arm so that the rope pulls vertically upward on the instrument. The cord used should have no tendency to twist when decreasing in length. In taking the torque cards, the diagram need cover but one pole-phase, to represent a complete torque cycle of the motor. The purpose of the indicator is to show the minimum torque effect exerted by the motor. On Form L motors two torque cards should be taken; one with the secondary starting resistance in, the other with it all cut out. A current of one-half normal amperes should be held for the reading with resistance in. Normal amperes should be held for the card taken with the resistance cut out. The motor should be carefully watched to see that the secondary resistance does not become too hot. Temperatures of the rotor must be recorded. On Form M and Form P motors, torque cards are generally taken with different values of secondary resistance. Sometimes 221 the secondary resistance is changed by changing the leads to the grids, and often by means of a controller. Whenever the test is made with a controller, a torque card should be taken for each controller position. The current held for these cards should be as near normal as the heating of the motor and grids will permit. The grids must not be allowed to become too hot, since this would lead to unreliable results, on account of the 600 _, s i - \ ^ \ ^20 j &,„ 1 -T~ 9//p r - Power Factor - / 90 ?»- = -^- = - ^, CN / ^ X- ^ te s §80 -f y 7 >? ^7/7-T 7- y \— = "*\J fl 4 S A J \nt t -,* ~ '* it h s \wtl ^ \50 —t ^ % T s^ ^ - 3i^ n Z 30 ! MP %mt ^ \^w ^**~ ' % -<*^ n 60 IZO 160 ZOO Z40 nroutput Z80 500 400 \ i 3Z0 360 ' Fig. 105 CHARACTERISTIC CURVES OF A 100 H.P., 500 R.P.M., 25 CYCLE, 440 VOLT, FORM M, 3-PHASE INDUCTION MOTOR rapid change in resistance with change of temperature. Tempera- tures of the rotor and grids should be recorded for each card taken. Calculation Sheet 22 shows the results of this test Starting tests are closely associated with the torque tests just described. They are generally taken according to instruc- tions given by the Engineering Department. Characteristic curves of the Induction Motor are calculated from the data obtained from the special tests. The data of a calculation are shown on pages 439 to 445 and Calculation Sheets 20 and 21. The corresponding characteristic curves are given in Fig. 105. The data used in the calculation are taken from the excitation curves (Fig. 99), the Impedance Curves (Fig. 101) and the slip curve (Fig. 103). 222 COMPLETE TESTS consist of normal and overload heat runs and special tests. SPECIAL OVERLOAD HEAT RUN consists of bringing the machine to normal load temperatures, then applying 50% overload for two hours and recording temperatures, then applying 25% over- load until constant temperatures are reached and recording temperatures. LONG COMMERCIAL TEST consists of taking equivalent load heat runs, readings of excitation and stationary impedance. GENERAL TESTS consist of taking excitation and impedance tests with wattmeters, single-phase, at points near normal volt- age and normal current respectively. Fig. 106 DIAGRAM OF APPARATUS USED IN TAKING INPUT-OUTPUT BY THE STRING BRAKE METHOD STANDARD EFFICIENCY AND POWER-FACTOR TESTS consist of calculating from general or special tests the efficiency and power-factor at any load. INPUT-OUTPUT "EFFICIENCY AND POWER- FACTOR TESTS con- sist of determining the efficiency and power-factor directly by the input-output method with wattmeters. They can be made either by the "String Brake" or "Electri- cal Load" methods. Neither of these methods is particularly accurate nor are they recommended. In certain cases, however, these tests are made on Induction Motors. String Brake Method In Fig. 106 L is a lever or scale beam suspended at the point ,Y. From T the small platform A is suspended, on which cali- brated weights are placed. P is a flat faced pulley on the shaft of the motor running in the direction shown by the arrow, i.e., toward the lever L. One end of a small rope is attached at B, which is wound one or more times around the pulley. The other end is made fast to a spring balance G. A strip bearing a mark is located at K so that when the point of the lever L comes opposite to the mark, the lever is in a horizontal position at an angle of 90 degrees to the force exerted by the pulley. 223 Since the stress along a rope is transmitted through its center, adjust the brake until the points M and N are a distance apart equal to the diameter of the pulley plus the diameter of the rope, one-half the diameter of the rope being added to each side of the pulley. This adjustment must be carefully made and care taken to see that nothing moves to throw the brake out of line or proper adjustment. When ready, slip one turn of the rope off the pulley but leave it attached at B and G, then balance the lever until the pointer on the end comes to rest at the mark K. This balancing of L must be repeated each time the rope is changed. The motor should be run light for at least one hour before the test proper is commenced, so that friction may become constant. Since speed is one of the important factors in the output of the motor it should be taken very carefully. Running light readings should now be taken on the motor. The voltage impressed on the motor should be held constant as well as the impressed frequency. Attach a small weight to the spring balance to give enough tension on the spring for a reading on the balance of a quarter or half a pound. This "no load" scale reading must be recorded and subtracted from all subsequent readings taken. Put a small weight on A and pull up on the spring balance G until the pointer on lever L reaches K. Then when the motor volts and speed of the generator are normal and all meters are steady, read and record volts, amperes, watts, weights on A, spring balance reading and speed given by the tachometer. A reading should also be taken of the slip. Add more weight to A and take another reading, continuing in this manner until the breakdown load of the motor is reached. For an induc- tion motor the readings should be recorded in the following manner: Volts Amps. + Watts -Watts Weight Tension on A on balance Speed Slip of Motor A rope of small diameter gives better results than a larger one, even though it may require more time to make the tests on account of having to renew it more frequently. On motors up to 20 h.p. a }/i in. oiled hemp rope is best and a Y2 in. rope can be used up to 50 h.p. The rope will last longer, usually, if doubled and two strands used in parallel. The rope turns around the pulley should all lie closely and evenly together on the face of the pulley. The tension read on the balance G will vary with the temperature of the rope and may differ widely with different loads. The additional weight put on A each time should be such as to give from fifteen to twenty readings between no load and breakdown. When the breakdown point has been reached and complete readings taken and recorded the diameter of the pulley should be carefully measured. 224 (Weight on A ) — (tension on balance) -("no load ' ' reading on balance) = actual load in pounds = P. (Normal speed) —(slip) = actual speed of motor. R = (Radius of pulley in inches) +(3^ diameter of rope.) 5 = Speed in revolutions per minute. _, , . Watts Power-iactor = 77- Then H.P. l-RXPXS Volts Xamps. 12X33,000 _™ . H.P. output X746 Efficiency = =r— — : \\ atts input When making any special test, the tester should see that the tests check among themselves before handing them in. Efficiency by the "Electrical Load" Method Consider Fig. 107; let if be the motor and L the load machine. This should be of about an equal capacity and be belted to rfies/stonce To Measuring Instruments and l/'ne To Water Box orSu/tati/e Motor Source of Current Fig. 107 CONNECTIONS FOR MEASURING INPUT-OUTPUT BY "ELECTRICAL LOAD" the motor M. It should be a direct current machine, and must be separately excited from a suitable source of energy. To take the efficiency test, connect M so that the total input can be obtained. Separately excite the field of L, con- necting an ammeter and a variable resistance in circuit. Connect the armature of L to a water-box or a motor the load of which can be varied, placing an ammeter in the circuit and a voltmeter across the brush terminals. If the test involves a considerable range of speeds, run M over that range, and hold the field current of L constant, its value being such that the speeds or loads required for M can be obtained. Having made the necessary connections, etc., keep the field current of L constant at its predetermined values. Vary the load on L by changing the water resistance or the load on the 225 motor to which it is connected, to suit the testing conditions required on M. The efficiency of M may be required for a series of speeds or loads. Read the input and speed of M, and the volts and amperes of L, keeping the field of L constant and noting its value. The "counter torque" must now be obtained to complete the calculations. To obtain this, disconnect M, connect L to a source of current which can be varied so as to give L different speeds, keeping L separately excited. Run L as a motor driving M, keeping the field current of L constant with the same value it had when L was used as a generator. Vary the speed of L so that the speed of M can be varied slightly below its previous minimum speed to slightly above its maximum speed. Take a number of readings at varying speeds, reading volts and amperes input of L and speeds of L and M. If the electrical efficiency alone is desired (case A), sufficient readings have been taken. If the commercial efficiency is desired (Case B), take off the belt from L, and run it light as a motor. Vary its speed from slightly below to slightly above the speeds used before when running as a motor, and take a number of readings at different speeds, reading volts and amperes input and speed, separately exciting L, with the same current used in the two previous cases. The necessary readings are now complete for calculating the efficiency. Case A Let Wm be the total input of M. Let Wl be the product of volts and amperes read for L. Let Fm be M's friction, windage, etc. Let Fl be L's friction, windage, etc. Divide the belt friction equally between L and M including this in Fm and F/. Let R be the hot resistance of Us armature, which must be measured. Let / be the current in L's armature. Then electrical efficiency = ==. where CT is the mechanical losses in L and M and the belt loss. Case B Commercial efficiency = == where CT is the mechanical losses of L including belt loss. In running the counter torque curves, the field of L must be held constant throughout, and readings must not be taken when accelerating. HIGH POTENTIAL TESTS should be taken on all induction motors as called for in the Engineering Instructions. 226 CHAPTER 13 STEAM TURBINES Since the horizontal type of turbine has almost entirely sup- planted the vertical type, the following instructions and illustra- tions will refer principally to the horizontal machines. How- ever, the work of operating and testing is practically the same for both types, except in certain features which will be dealt with separately, and the instructions may, in general, be con- sidered as applying to both types. Nomenclature Due to the radical differences in construction of the steam turbine from that of any other prime mover, there are many parts more or less unfamiliar to the average engineer. To secure uniformity in the designation of parts, thus avoiding any uncertainty and unnecessary cTelay, Figs. 108 and 109 should be carefully studied until thoroughly familiar. The number of stages of both vertical and horizontal machines is indicated by the following form letters. Xo. of Stages Vertical Horizontal Xo. of Stages Vertical Horizontal 1 A 7 M P 2 B C 8 Q R 3 D E 9 S T 4 F G 10 u W 5 H J 11 AA 6 K L 12 BB CC Generators are indicated thus: Type Form ATB Vertical ATB Horizontal CC Horizontal T HT T Tests Tests on a steam turbine may be divided into two classes, Commercial Tests and Special Tests. For commercial tests the turbine is assembled in Building No. 60, and is operated non-condensing at practically no load, and without regard to any definite steam pressure or super- heat. The tests consist of dynamic balance, adjustment of operating and emergency governors, and the inspection of the 227 Fig. 108 VERTICAL TURBINE AND GENERATOR 228 PARTS OF VERTICAL CURTIS TURBINE AND GENERATOR (See Fig. 108) 1 Condenser base 2 Intermediate holder 3 Turbine head 4 Steam chest 5 First stage nozzle 6 Operating valve 7 Generator stool 8 Coupling 9 Ends of field coils 10 Field core 11 Armature core 12 Armature spider 13 Armature coils 14 Coil supporting rings 15 Ventilating fan 16 Top bearing bracket 17 Top bearing 18 Collector and brush-holder 19 Operating governor 20 Governor dome 21 Governor beam 21 Governor beam 22 Governor rod 23 Governor dome stool 24 Ventilating hood 25 Mid bearing cap 26 Mid bearing 27 Pilot valve chest 28 Hydraulic cylinder 29 Head end carbon packing rings 30 First stage wheel 31 Exhaust end carbon packing rings 32 Packing ring dome 33 Guide bearing 34 Step bearing 35 Intermediate buckets 36 Nozzle diaphragm 37 Cam shaft 38 Emergency governor 39 Shaft 40 Field spider 229 230 £ W « H w H c/J •— i H O < O N o o H Pi o ^ i _ i o ^ 03 -^ >> o w tx o O, a S S-d 0) ^3 o G'd o o > ,_ be a 'w a o IS £ ° g as > g £ £^2mOOKKPhO 03 rj 03 c OcoOPhOOW „ 03 .S rt o ^ ^^ d fcuo aj w P 03 u, » C3 8 £T ; u *" >.b 03 '&.£A NNNNNNNNNNNfOfO«5W)(?)«5fnrO 'H to 03 C G 03 oj a> a 'C< 03 03 rj A) o 3~3 rt3 s c s x tm ^0 W .S-S.S Zf nj 03 03 *1 t/1 1— I •— I ^ 03 u'O'd o ■^'c6l>-OOOOX'XOOO^)^)X)'-HCOCOiOCDO'-iI>CNlcOCO t-h T-i (MhhCMhcOCnKMCOCO^ *-• .is 15 kO ic »0 lO iO CM CM lO t-I Cm'cm'cMCMCMCM lOiO CO »C iC l> »0 03 O 00 O CM ^ si °5 to io >o I>LOiOiOiOl>t>iO io»o HC^HHrtHHHNNHNNNWMCOPO^^^^ be 4) u pq lO lO c^coco^^^^^^OioiTtcNioiasiooooo^Looooio o CO ooooooooooooooooooooooo OOOOOOOOOOOOIMiOOiOOiOiOiOiOiCiO MXM»OLO(MLO00CaNO5ffiNNaNiONNNNNN ID o bo cd X iO C^^C^^^'^^'^TttTt'^-^^^TtiiO | *0 ^f lO lO CO CO z as 750 1500 1500 2500 3500 3750 5000 9000 14000 15000 20000 500 500 800 1000 1000 1500 2000 2250 3000 5000 5000 8000 239 SEALING STEAM SEC TION A AA -A A -A A GZZZZZ* \ Fig. 114 CARBON PACKING (FLOATING RING TYPE) 1 Carbon packing casing (half) 2 Clamp bolt for (1) 3 Carbon ring segment 4 Retaining bolts for casing 5 Stop for carbon rings 6 Bracket for (5) 6 Garter spring 8 Alloy packing ring 9 Retaining ring 10 Drain to 2nd stage shell 11 Drain to 3rd stage shell 12 Drain to atmosphere 13 Supporting spring 240 In turning oil on the step bearing proceed as follows: Open the valve until the step is raised and note the gauge pressure. Then close the valve, allowing the step blocks to come together again. Now open the valve very slowly, and watch the gauge. Hold the pressure between 90 and 95 per cent of that required to raise the step, and watch for oil leakage at the drain from the step. At this pressure the step will not be raised, and if the blocks are parallel the leakage between them will be practically nothing. However, if the blocks are not quite parallel there will be an opening on one side which will allow a considerable flow of oil. Having ascertained that the step blocks are all right the valve should then be opened to give about a quarter of the required flow, and the step bearing and pipes allowed to become warm. This must be done since the oil will not drain away from the step rapidly enough to prevent flooding when cold. The oil in the supply tank is kept at a temperature of 45 to 51 deg. cent, and a short time should be sufficient to warm up the bearing and drains. The valve may then be opened the full six turns. A table of the flow and probable pressures for various machine capacities is given on page 239. This table is calculated for machines that are completely assembled. It is usually necessary to readjust the baffler between the periods of adjusting wheel and field balance. Oil leaks in the step bearing should be carefully watched for, and remedied before starting the machine. Carbon Packing Rings The carbon packing rings (see Fig. 114) should have enough steam to lubricate, and to seal in case vacuum is used. Too much steam is injurious. The right amount will be indicated by the escape of a little vapor from the drain leading from the carbon ring casing. This drain should always be left open. It sometimes happens that, through insufficient steam lubrica- tion or other cause, the carbon rings tend to grip the shaft, become very noisy and throw the machine into vibration. When this occurs, which is more often on horizontal than on vertical types, a very thin solution of graphite and water should be introduced into the carbon casing. One or two applications will effectually remove the trouble. The graphite must never be mixed with oil, nor made into a thick solution with water, as it then becomes gummy, and causes the rings to stick in the casing and hold away from the shaft. When this happens the rings cannot seal. Trip Rigging Before starting a machine, try the trip rigging on the emer- gency throttle valve to see that it will trip the valve easily See Fig 115. 241 Top of Vo/i/e fO f?o not t/'gtitentT/anc/s /7?ore tnar? necessary f£ % /j — J* !6- /8- 15- Pressure Control P/ue? To Latch on '^mergence/ 6~oye/~nor 7urn /ntn/s direct /'or? if to open wOen iei/er f | isnoo/red up \ 7urnintnis direction to c/ose i/n/ve wnen /erer/'s noo/redup, u/sotono/se si/ding nut on a" /e yen /or engaging ///to no o/r after vo/re i?as /been trippe Section "Z-£" Loo/ring Down Fig. 115 THROTTLE VALVE AND EMERGENCY GOVERNOR TRIP RIGGING 1 Valve bonnet 11 Trip bell crank 2 Valve body 12 Large gland 3 By-pass nut 13 Small gland 4 By-pass valve cover 14 Sliding nut 5 By-pass valve 15 Yoke 6 Valve spool 16 Trip handle 7 Valve stem 17 Trip hook 8 Valve seat 18 Lever for sliding nut 9 Trip spring Valve stem bushing 19 Handwheel 242 Wheel Balance Before the main valve is opened to admit steam into the line to the emergency throttle, the exhaust valve should be opened. This will obviate any danger of excessive steam pres- sure on the turbine shell should the throttle valve leak. Cold machines, in being started, should have enough steam given them to start them revolving at once. Otherwise the steam may distort the wheels, due to local heating. As soon as a machine starts to revolve, place one end of a wrench or bar against the intermediate holder, and rest the ear against the other end, and listen for rubbing. If the wheels seem to be running clear, bring the speed up to about 50 rev. per min., and then shut steam off completely. Listen for rubbing as before and at the same time notice whether the speed dimin- ishes rapidly or not. The time that a machine should run before stopping varies greatly with the size and type, hence it is left largely to the judgment of the man in charge of the machine as to whether it is operating as it should. It is not necessary to let the machine come to a stop to see if it is run- ning freely, as any marked diminution of speed can be noticed in a minute or two. Heat the machine up thoroughly before bringing it to normal speed by allowing it to run at about one fourth normal speed for fifteen to thirty minutes, depending on the size. When well heated, bring to normal speed (if the balance permits) and note the balance, or amount of vibration, on the bearings and on the intermediate holder. If the balance is good enough at normal speed it should then be tried at 110 per cent normal speed. Balance at 110 per cent speed should be as good, or nearly as good as at normal. Some machines are in good balance when they come to test, but more often they have to be balanced dynamically. Before beginning wheel balance, the method of numbering the balance weight holes should be understood. It is impracticable to mark the wheel alongside the holes themselves, as the steam would soon efface the marking, so the following method is used: On horizontal machines, holes for introducing balance weights into the wheels are provided in the turbine head and in the exhaust chamber. The wheels are revolved until a hole in the wheel is in line with the hole in the exhaust chamber. This is considered hole No. 1. A definite point of reference is made on the middle bearing in line with this hole, and a mark made on the coupling also in line. This locates hole No. 1 and should be permanently indicated by a prick punch mark on the coupling. The wheels are now slowly revolved and the location of each balance weight hole is marked on the coupling with chalk or whiting. Beginning with No. 1 the holes are numbered, always in the direction of rotation. In vertical machines the holes are numbered in a slightly different manner. The coupling is not assembled during wheel balance, so a key- way is selected to locate hole No. 1, this key-way being indicated by a prick punch mark. The balance weight hole in the wheel nearest in line with the key- way is 243 brought under the hole in the turbine head and No. 1 marked on the bearing under the key-way. Revolve the wheels slowly and mark under the key- way on the bearing the location of each hole. Numbering on the bearing must be against rotation in order that the numbering on the wheels themselves may be in the direction of rotation. All turbines revolve counter clockwise facing the steam inlet end. Before beginning work on balance, the shaft should be painted with whiting, at both ends when accessible. When the machine is up to speed or at as high a speed as the vibration will permit mark the shaft lightly with a pencil. The pencil line will appear heavier in one place which is generally opposite or nearly opposite the side that requires additional weight. Place a weight in the side indicated, in either the first or last stage wheel, depending on which showed the greater amount of unbalancing as indicated by the pencil mark. Use a fair sized weight, e.g., one two inches long. Bring the machine up to as high a speed as the balance will permit and note the balance of all parts. Then move the weight one-quarter way around the wheel and try the balance again. Proceed thus until both first and last wheels have been tried. Then continue trials in. the holes in which the best balance was noted, using larger or smaller weights as may seem necessary. No rigid rule can be set down for the size and use of weights in balancing. It is a matter which must be left entirely to the judgment of the test man. A balance record similar to that given on page 245 should be kept, and on this an accurate record of weights used and the per cent balance should be noted. From this record it is evident that weights in hole No. 7 gave the best results in "quartering," hence it was then only necessary to try slight variations and changes in the neighbor- hood of hole No. 7 to obtain a perfect balance. A number of things may influence the balance of wheels at the start which are not due to an actual unbalancing of the wheels themselves. (1) The carbon packing rings may be gripping the shaft. This has already been discussed, and the proper remedy ex- plained. (2) The diaphragm packing rings may be rubbing on the shaft or wheel hubs. That surface of the packing ring that bears against the shaft consists of a series of V-shaped grooves. When there are indications of rubbing at this point, the turbine should be run continuously at a speed at which there is a slight vibra- tion. This will in a short time wear a clearance between the rings and shaft and remove the source of trouble. This method should be followed in all cases in which a turbine vibrates at low speeds, and for which no other cause can be found. (3) The wheels may be rubbing at the circumference. When this is the case it should be reported at once, and an investi- gation made. (4) There may be water in the turbine. See that all drains are free. If, when opened, neither water nor steam escapes, it 244 * BALANCE HOLE NUMBERS PER CENT BALANCE 1 n 2' 2 Wl 3 light 4 2" 2" 5 6 1" 7 2" 2" 2" 2" 2" 2" 8 2" 2" 9 10 2" 11 12 v be 4u i— iW Is I 93 95 54 I 90 94 55 I 92 95 93 I 97 97 95 I 93 95 94 I 93 94 93 I 95 97 96 I 92 95 92 I 98 99 98 I 99 100 98 I 100 100 100 " O "Indicates the outside, or first stage wheel. "I" Indicates the last stage wheel. Note — Italics indicate pencil notations by the one doing the balancing. 245 is evident there is a stoppage somewhere, and all valves and piping should be carefully examined. CA UTION. Do not run wheels with loose weights. Be sure that all weights are tight, and that none project so far on either side of the wheel as to strike any stationary parts. Field Balance The method employed in balancing the field is practically identical with that used in balancing the wheels. In this case the numbers may be painted directly alongside each balance weight screw hole, beginning at the field leads and numbering in the direction of rotation. When the field leads are brought out on opposite sides of the shaft, hole No. 1 should be indicated by a prick punch mark. On a later type of field the balance weight screw holes are replaced by a dove-tail groove in which are carried the heads of the bolts securing the weights. It will be necessary on this type to divide the groove into a number of equal sections, or "loca- tions" which should be numbered as are the screw holes on the older type of field. Twenty-four is the most convenient number of "locations" to use. On the older type of field the balance should be obtained by the use of one weight only in each end of the field. If this is impossible and more than one weight is necessary the weights must be concentrated, not scattered or counter-balancing each other. On the later type with the groove, the procedure is some- what different. Here the balance weights are always used in pairs, i.e., a pair of weights in each end of the field. The weights of any one pair must always be equal in size and similar in shape and each weight must be secured by at least two bolts. When a balance is finally obtained the size of the weights of a pair should have been so selected that the weights are located approxi- mately 60 deg. to 90 deg. apart. This method of balancing allows of a very wide range of adjustment. By bringing the weights together or moving them further apart along the groove any effective value from zero to a maximum may be obtained, and the resultant value may be placed in any position desired. If the weights have been selected as directed there will be ample latitude for further adjustment should it become necessary at any time. In all field balance work the shaft should be painted with whiting at each end of the field, and indications of the direction and amount of unbalancing made as described under the head of "Wheel balance." These indications should be used as a guide in the location of weights throughout all balance work, but the knowledge of how to do this must be gained by experience as the significance varies with every machine. CAUTIONS 1. Balance weights must fit tightly, all bolts be inf place and drawn up tightly. 246 2. Weights must fit firmly for their full length against the outer side of the slot. 3. Xo balance weight should be used whose thickness is more than twice the depth of the balance weight slot. 4. Weights should never be superimposed. In loading machines for shutting down, do not load them single-phase. The foregoing instructions on the balancing of alternator fields will also apply, in a general way, to the balancing of direct current armatures. The weights used in direct current arma- tures are of different shapes, and are secured in various ways, but the method employed in obtaining a balance is the same as that used in balancing turbine fields and revolving fields. Before beginning balance work on any generator, all wiring should be completed and cold resistance measurements taken. One condition to be watched in all balance work is the number of operating valves that are held open. Only just so many valves as are necessary to bring the machine up to speed should be used. If a greater number of valves is opened a greater amount of steam is required to do the same work. This is wasteful, and in the case of large machines the steam pressure in the mains may be so reduced by the excessive flow as to let the step-accumulator down, causing considerable damage if not stopped at once. This rule in regard to the number of valves opened should, in fact, be observed in the starting of machines at all times, especially those of larger sizes. The only case in which it cannot apply is in the testing of operating governors to be described later. Too much importance cannot be attached to the main- tenance of steam pressure. Low steam pressure may, through the loss of pressure in the step-accumulator oil system as just referred to, damage the wheels of a vertical turbine to such an extent as to require an entirely new set of wheels. Governor Tests EMERGENCY GOVERNORS After the wheels are balanced and before the field is assembled, the emergency governor should be adjusted and tested. There- after it should be tripped at least once every twenty-four hours, and a record made in a folder provided for this purpose. Emer- gency governors are known as Type E. There are two forms now used. Form D, the eccentric ring type (Fig. 116) is used on all machines of 2000 rev. per min. and under, and Form E, the plunger type (Fig. 117) used on the higher speed machines. The Form D governor is shown in Fig. 116 in its normal concentric position before operating. In operating, the ring (1) moves out eccentrically against the spring (13) coming in contact with the trip finger (9) (Fig. 118) thereby releasing the emergency throttle valve. The adjusting nut (8) (Fig. 116) over the spring screws on to the spindle (4). The thread is right- handed, so that by turning the nut to the right more tension is 247 ^^»5-^ Fig. 116 EMERGENCY GOVERNOR (FORM D), (DOUBLE RING TYPE, HORIZONTAL TURBINES) Emergency governor ring 8 Emergency governor guide 9 block 10 Emergency governor spring 12 box 13 Emergency governor spindle Emergency governor stop 14 Bushing for (2) 15 Collar for (3) Adjusting nut for (4) Guide pin for (1) Cotter pin for (5) Bushing for (3) Emergency governor spring Support for (13) . Rivet for (1), (2) and (3) 248 Fig. 117 EMERGENCY GOVERNOR,*PLUNGER TYPE (FORM E) 1 Governor plunger 2 Tension adjusting bushing 3 Guide bushing 4 Retaining nut for spring 5 Adjusting nut for spring 6 Governor spring 7 Cotter pin for retaining nut 8 Pin for adjusting nut 9 Clamping collar for governor 10 Dowel pin for clamping collar 11 Holes for spanner wrench 12 Cap screw for clamping ring 240 Fig. 1 EMERGENCY GOVERNOR AND THRUST BEARING 1 Pillow block or stand- 17 Stationary plate, front ard thrust 2 Gear casing 18 Adjusting shims, front 3 Shaft thrust 4 Gauge board 19 Bearing cap bolt 5 Lock nut for gears 20 Bearing cap 6 Spiral gear 21 Bearing 7 Emergency governor 22 Babbitt lining 8 Deflector 23 Bearing packing ring 9 Emergency governor trip 24 Air deflector finger 25 Oil guard 10 Emergency governor con- 26 Adjusting shims, back necting rod to throttle thrust valve 27 Revolving plate, back 11 Emergency governor rig- thrust ging bell crank 28 Roller cage, back thrust 12 Cover plate 29 Stationary plate, back 13 Emergency trip finger rod thrust 14 Thrust nut 30 Water drain sight cup 15 Revolving plate, front 31 Bearing standard dowel thrust pin 16 Roller cage, front 32 Dowel pin nut thrust 33 Bearing standard bolt 250 given to the spring and the speed at which the governor operates is increased. The nut (8) is held in position by a lock-screw, which goes through one of the holes in the nut and screws into a stationary plate below. This screw must always be replaced after it has been removed to make an adjustment of the governor. The Form E governor is shown in Fig. 117. Here, instead of an eccentric ring, we have a plunger (1) to strike the trip- finger. The entire mechanism is contained in a bored out sec- tion of the shaft, and held in place by the two clamping rings (9,9). The adjusting nut (5) over the spring, does not turn, but is moved in or out by turning the bushing (2). Since the nut has a right-hand thread, turning the bushing to the left, forces the nut in, puts more tension on the spring, and increases the speed at which the governor will operate. The bushing (2) is held in position and prevented from turning by the clamp rings (9), hence these rings must be loosened before any effort is made to move the bushing. The rings are clamped by four cap screws in the holes (12). All emergency governors must be adjusted to trip at 10 per cent above the normal speed of the machine, with an allowable variation of 3^2 per cent either high or low. The speed at which they return to their normal position must be, on the Form D, between 90 per cent and 100 per cent of normal speed, and on the Form E, between 100 and 101 per cent. After the proper adjustment has been obtained, the governor must be tripped five or six times in succession, and the operation of all parts of the trip rigging noted. There should be no lag to any of the parts, and the valve should close quickly. Any defect must be reported at once. Fig. 118 shows the assembly of a Form D governor and the arrangement of the trip rigging. This illustration also gives a good idea of the arrangement of the thrust bearing and adjusting shims of the roller type of thrust. Fig. 119 shows the arrangement of a later type of thrust bearing known as the "Block" type. This is the type of thrust also shown in the illustration of a general turbine assembly, Fig. 109. A third arrangement of a thrust bearing, known as the "Ring" type is shown in Fig. 120. The Ring type and the Block type thrusts are interchangeable. Either may be as- sembled in the outer housing (9) Fig. 119. OPERATING GOVERNOR The operating or main governor is known as Type M gover- nor, Form C, and is shown in Fig. 121. On vertical machines the governor is set directly on the top of the main shaft, see Fig. 108, but on horizontal machines it is driven from an auxiliary shaft connected to the main shaft by a worm and gear. See Fig. 122 and Fig. 123. This auxiliary shaft also drives the gear oil pump. After the gear pump is assembled and operative the steam driven oil pump should not be used except when starting and stopping the machine. 251 >52 ,^ CD CU co -i^> C *3 2 o _c 33 X co V CO CO 3^ CO ,"J^ O^ o^ jS O co 3^ ? ? >?S? o .5 -c •r 1 ^ CD co O i^ i^ o X X »-H 1 CD CD > ti — i 05 O CO OnJ £ 05 CD 3 t-i -£T3 +3 jj*C n 1 — ' +J C +3 .ts ^, I '32 ■rPb.33 2 s ft u bua ££££ £ o o c £ 'co co ° 2 :2 u «-> j £ ^£ ) cr> ^ C Nf*J^ ID ON00O 253 Fig. 120 RING TYPE THRUST BEARING 1 Alloy thrust rings 2 Thrust bearing shell 3 Thrust bearing 4 Bolts 5 Shims for adjusting clearance of wearing shoe 6 Wearing shoe 7 Set screw for shaft nut 8 Shaft nut 254 Before beginning governor tests the machine should be run for a short time with the governor holding speed to ascertain that all parts of the governor and hydraulic rigging function properly, that there is no sticking in any part, and that there is no hunting in the governor itself. Any defects noted should be reported at once and the necessary corrections made before proceeding with the governor test. OPERATING GOVERNOR TEST Fasten a pointer on the machine in some convenient place where it will be near the piston or connecting rod (No. 14, Fig. 122). Paint the section of rod opposite the pointer with a coat of whiting. Move the pilot valve by hand, opening all the operating valves. As the last valve opens so that the roller 12 (Fig. 124) just rises over the point of the cam (14) make a mark on the whiting opposite the pointer. Then lower the pilot valve stem so that the valves close, and as the last valve is just closed make a second mark on the whiting opposite the pointer. The foregoing refers to high pressure machines only. Machines designed to operate on both high and low pressure steam are provided with a low pressure butterfly valve, Fig. 125, whose operation precedes that of the high pressure valves. Hence the two marks must include the total travel of the piston rod (2), necessary to operate both the high pressure valves and the butterfly valve. The first mark is located as described above. The second mark is made when the piston or connecting rod (2), Fig. 125, has, by means of the cam (8) and connecting rod (10) brought the butterfly valve to the "closed position" as indicated by dotted lines. The length of the connecting rod (10) should be so adjusted as to give a compression on the spring (5) of from s5 to tV in. Having located the two limit marks, divide the intervening space into five equal parts, thus obtaining six marks. In order to bring the speed above the point at which the governor would normally hold the speed, and so make each mark on the scale pass the pointer, it is necessary to block open one or more valves. Before any valves are blocked open, and with the. governor holding speed, check the tachometer.' This is done preferably by holding the speeder on the end of the gover- nor spindle (8), "Fig. 121, rather than on the end of the main shaft. Take a two minute reading. The proper governor speed may be determined from the ratio of the worm and gear. The tachometer, which is always belted, should be provided with a pulley of such diameter as to give a reading well up on the scale. All is now ready for the actual governor tests and adjust- ments. Speed readings should be taken as the marks on the scale pass the pointer, first as the machine is brought above normal speed, and again as it falls below normal. The first readings are taken with the synchronizing spring (27), Fig. 121, set in mid-position; that is/ with the plug (26) Fig. 121, set at the mid-position of its travel. All adjustments 255 Fig. 121 OPERATING GOVERNOR 1 Governor dome 21 Thrust plate for (19) 2 Governor lever 22 Worm wheel 3 Governor bracket 23 Worm 4 Weights 24 Supporting plate for worm 5 Fulcrum block for (15) wheel 6 Links 25 Handwheel 7 Yoke for (6) 26 Plug for synchronizing 8 Spindle or connection rod spring 9 Spring for universal joint 27 Synchronizing spring 10 Lower spring plug 28 Limit switch base 11 Main spring 29 Limit switch details 12 Adjusting nut for (11) 30 Trunnion for lever 13 Adjusting plate 31 Nut for (30) 14 Key for (13) 32 Stop for weight 15 Knife edge for (4) 33 Studs for lever bracket 16 Transmission roller bear- 34 Nuts for (33) ing 35 Lead screw for (26) 17 Lever bracket 36 Shaft for worm 18 Roller bearing for lever 37 Knife edge bearing block 19 Bracket for synchronizing for (4) and (7) gear 38 Knife edge for (6) 20 Bracket for worm gear 39 Upper spring plug 40 Stop blocks 256 P Q M o a o w C rt > C as .22 £« o co ■«* in vo t* 0) p — +-> , «« o o nS ■ Q S£ ^ 0) > e e o 0) o o m ri oocoou N00OO -I CM biO a as "2 "5 .si 5£ HI Ml g. c ^ S b '- _^; _o _o -^ ii a o S 2 2 C5 * ^ H H H > w O ^h m ro ^ m o 2.",; Fig. 123 GEAR PUMP AND CASING (OUTSIDE TYPE PUMP) (See page 259) 258 PARTS OF GEAR PUMP AND CASING (Outside Type Pump) (See Fig. 123) 1 Gear casing 2 Spiral gear driver 3 Turbine shaft and keys 4 Spiral gear driven 5 Lower bushing (governor end) 6 Governor and pump shaft 7 Bronze thrust plate for governor 8 Steel thrust plate for governor 9 Upper bushing (governor end) 10 Keys for (4) and (6) 11 Steel thrust plate for spiral gear 12 Upper bushing for (6) pump end 13 Upper bushing for (14) pump end 14 Idler shaft for pump gear 15 Bolt for (1) and (16) 16 Pump casing 17 Stuffing gland for pump suction 18 Stuffing box packing 19 Pump gear 20 Plug in bottom of casing 21 Bottom bushings for (6) and (14) pump end 22 Pump discharge 23 Pump suction 259 / Fig. 124 HIGH PRESSURE CONTROLLING VALVE 1 Adjusting screw for valve spring 2 Supporting plate for (1) 3 Spring supporting plate (adjustable) 4 Controlling valve spring 5 Stud for spring supporting plate, with nut 6 Frame for controlling valve, with bolts 7 Guide plate for valve stem 8 Upper cup for (7) 9 Thrust pin 10 Lower cup for (11) 1 1 Controlling valve lever 12 Cam roller for lever 13 Spindle for cam roller with nut 14 Cam with key 15 Cam shaft 16 Cam shaft bracket with bearing cups and bolts 17 Gland for packing 18 Nut for stuffing box 19 Gnide plate and stuffing box for valve stem 20 Valve stem 21 Valve (wing type) 22 Valve seat 23 Valve casing 24 Pin for (20 and (21) 260 P OSIT ION OF BUTTERFLY VALVE WHEN FIRST HIGH PRESSURE VALVE STARTS TO OPE^ FULL OPEN POSITION Fig. 125 ARRANGEMENT OF HYDRAULIC GEAR ON MIXED PRESSURE TURBINE 1 Cam shaft for high pressure valves 2 Piston rod 3 Pilot valve chest 4 Hydraulic cylinder 5 Spring 6 Cam roller 7 Slot for cam roller (6) 8 Cam plate 9 Cam lever 10 Connecting rod for butterfly valve 261 -2/ ( gjio @ /8 +-/Q m& Fig. 126 HYDRAULIC OPERATING CYLINDER AND PILOT VALVE (HORIZONTAL TURBINES) Pilot valve stem guide Pilot valve pivot clamp Pilot valve middle bushing Pilot valve end bushing Pilot valve seat bushing (hardened steel) Floating lever Differential lever Link for (18) Rod end — adjustable Connection to governor lever 1 Hydraulic cylinder 12 2 Cylinder head 13 3 Stuffing gland for (2) 14 4 Nut for stuffing box 15 5 Piston 16 6 Piston ring 7 Piston rod 17 8 Piston rod nut 18 9 Pilot valve 19 10 Pilot valve chest 20 11 Pilot valve stem 21 262 of the governor must be made with the spring in this position. On a properly adjusted governor a set of readings similar to the following is obtained. Marks Accelerating Decelerating Lag 1728 1725 3 1740 1736 4 1748 1743 5 1757 1752 5 1770 1767 3 1790 1786 4 Tachometer reading = 1750 Speed of machine = 1800 The requirements to be met are as follows: (1) Normal speed must be between readings No. 3 and No. 4. (2) The total regulation, that is, the difference between reading No. 6 accelerating and reading No. 1 decelerating, must be between 3.6 and 4.0 per cent of normal speed. (3) The "lag" is the difference in the readings accelerating and decelerating for the same mark on the rod and must not exceed an average of 0.4, or a maximum for any one reading of 0.5 per cent of normal speed. If the speed or regulation of the :rnor is not correct, it can be adjusted by varying the tension on the main governor spring (11), Fig. 121, or by changing weights in the pockets of the governor weights (4), Fig. 121. Increasing the tension on the main spring will raise the speed and decrease the regulation. Decreasing the tension lowers the speed and increases the regulation. Increasing the weight in the pockets of the governor weights lowers the speed without appreciably affecting the regulation. If the lag is excessive take a set of readings on the governor rod (17), Fig. 122, with the rod disconnected from the piiot valve. This will indicate whether the excess lag is in the gover- nor or in the hydraulic rigging. See Fig. 126. In either case the lag should be corrected before proceeding. After the gover- nor has been properly adjusted, take three sets of readings using the scale or marks laid out on the piston rod, the synchro- nizing spring being in mid-position. Then take two sets of readings on each of the two limit positions of the synchronizing spring: " Spring all in " (maximum compression) and "spring all out " (minimum compression). Bafflers The step bearing baffler, Fig. 127, is furnished with all vertical machines, having replaced the old style baffler (Fig. 113), now used only as a part of the permanent testing equipment. The baffler frame is first tested for sand holes and porous places in the casting. It is carefully painted over the entire surface with whiting, filled with oil, and kept under a pressure of 2500 lb. per sq. in. for 24 hours. If at the end of this time 263 Fig. 127 STEP BEARING BAFFLER (ADJUSTABLE) 1 Head (inlet end) 2 Plug for blowoff 3 Strainer (gauze mesh) 4 Barrier frame 5 # Adjusting screw 6 Head (outlet end) 7 Washer (inlet end) 8 Strainer frame 9 Baffler screw 10 Washer (outlet end) 264 there is no indication of oil anywhere on the whiting, the baffler is completely assembled with strainer and plug. The plug^ or screw (9), Fig. 127, has a thread with a taper- ing depth of groove which allows of a wide range of adjustment. The deepest grooves should be assembled at the discharge end. The following table shows the approximate flows for given pressure drops across the baffler and various adjustments of the adjusting screw (5), Fig. 127. The temperature of the oil is •50 deg. cent. FLOW IN GALLONS PER MINUTE \^ Length ^^^^ of Drop ^^---^"A" 2 In. 3 In. 4 In. 5 In. 6 In. 7 In. 8 In. lb. per sq-t n. ^^~~^~ 50 1.0 2.2 3.1 4.4 6.0 8.0 12.5 75 1.5 2.9 4.2 5.4 7.6 10.7 16.8 100 1.9 3.4 5.0 6.5 9.0 12.7 20.5 125 2.2 3.9 5.5 7.4 10.1 14.5 24.0 150 2.4 4.4 6.3 8.4 11.2 15.6 27.5 "A" is the distance between the end of the plug and the baffler head. See Fig. 127. Stage Valves In most of our multi-stage vertical turbines, valves are pro- vided which open additional second stage nozzles at times of overload. The usual arrangement of this valve is shown in Fig. 128. The pipe (16) connects with the first overload valve on the operating valve casing. When the operating valve is opened steam is admitted to the upper side of the piston (14) and the stage valve (2) is forced open against the spring (5). This valve should open quickly and positively, and should close in the same way. The only test made on the assembled stage valve is to open and close the controlling valve a few times, and note that the stage valve acts properly and operates without sticking. Also the travel of the stem or indicator rod (8) should be measured. A modification of this valve carries the spring outside of the casing, but the operation is essentially the same. GENERATORS Sectional views of vertical and horizontal turbo-generators ai^ shown in Figs. 129 and 130. The scheme of ventilation of the turbine generator is rad- ically different from that of other types of generators. Referring to Fig. 129, air is drawn in through an opening in the side of the hood (9), forced by the fans (21), through the air gap and out through the ducts in the armature laminations (1) to the 265 Fig. 128 STAGE VALVE (See page 267) 266 PARTS OF STAGE VALVE. (See Fig. 128) 1 Casing for stage valve 2 Valve and piston 3 Valve seat 4 Cylinder lining 5 Spring 6 Cylinder head 7 Adjusting screw 8 Indicator rod 9 Balance-cylinder head and stuffing-box 10 Gland for stuffing-box 11 Spring seat 12 1 12 r Rings for piston 13 Indicator 14 Balance piston 15 Packing ring for balance piston 16 Admission from overload operating valve 17 Drain for valve 2G7 Fig. 129 VERTICAL GENERATOR SECTION 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 Armature punching section 16 Armature punching space block (outside) 17 Armature punching space block (inside) 18 Armature spider 19 Armature flange (top or lower) 20 Armature key 21 Armature coil 22 Bearing bracket (upper) 23 Ventilating hood 24 Floor plates 25 Generator base and middle bearing bracket 26 Pole piece revolving 27 Revolving field spider 28 Field spider rings 29 Shaft 30 Field coil support End flange Field coil retaining bolts Retaining rings Field coil Fan Air deflector (upper) Air deflector (lower) Collector lead supports Brush-holder studs Collector Field lead Brush-holder lead Binding bands Coupling 268 space between the laminations and the armature shell (4) and thence downward to be discharged through openings in the gen- erator base (11). The ventilation scheme on the horizontal generator, Fig. 130, is similar to that on the vertical, except that air is drawn in from below at both ends. The air is forced by the fans through the air gap and out through the laminations, and may be dis- charged at either the top or bottom of the armature as the customer may require. On small machines of 1000 kw. and less, the fans are usually omitted from the field. On machines in test, where a bottom discharge is called for, the opening at the bottom of the armature is temporarily blocked off, and the air taken from the top. Otherwise, a more or less elaborate arrangement of air ducts would be necessary to prevent the hot discharged air from being drawn in and circulated through the armature over and over again. Generator Tests ALTERNATORS Generator tests comprise the lesser part of the work on tur- bine sets. On standard machines, and those for stock, the only tests usually required are saturation and synchronous impedance curves, phase rotation, current leakage from shaft to pillow block, field and armature measurements, and high potential tests. These tests are invariably made on every machine. In addition to the above, heat runs, either open circuit and short circuit, or a "zero power-factor" run may occasionally be called for. Other tests much less frequently made are ven- tilation tests, motor core loss, phase characteristic, armature impedance with rotor removed, open-delta heat runs, zero- excitation heat runs and full load heat runs. As all the above mentioned tests except ventilation tests and "zero-excitation runs" have been dealt with elsewhere in this book no further mention is necessary except such details as may need special attention due to slightly different condi- tions that may be found on turbine generators. Before beginning generator tests all pipe joints, and joints about the gear casing, pump and bearings where there is a possibility of oil leakage, should be carefully painted with whiting so that any leaks existing may be located during the progress of generator tests. The limits to which saturation and synchronous impedance curves are to be run, and the values of voltage and current held on open- and short-circuit heat runs are varied from time to time under instructions from the turbine generator Engineers, hence, the book of "Special Instructions" previously referred to should be consulted for this data. Cold Measurements Under the head of "field balance" reference was made to taking cold measurements on the generator. This should be 269 270 » Fig. 131 WATER COLUMNS ON GAUGES The water column on the gauges should be measured and entered on the testing Record Sheet with the number of the gauge. The water column is measured from the top of the siphon coil to the center of the gauge and recorded as + or — WC in inches. (See Fig. 131.) U-tubes are used to read all vacuum and pressures of a few inches. These consist of a thick glass tube with }/% in. bore bent in the shape of a U, and mounted in a wooden case carrying a brass scale. (See Fig. 132.) The scale is graduated in inches with a zero at the center and numbered each way to read at least 16 in. The tube is then rilled with mercury. The U-tube is connected up through a heavy rubber tube. The glass tube should be clean and free from water and the connections should be free from air leaks. These may be detected by turning the cock off, leading to the vacuum being measured, and noting if any perceptible fall of the column occurs. Both columns should be read and added together. Never read one 276 and multiply by two. When the U-tube is disconnected both columns should stand at the same level. When reading vacuum the U-tube may be left connected to the machine, but it should be disconnected after each pressure reading, or the tube will gradually fill with water. Fig. 133 ABSOLUTE PRESSURE GAUGE Absolute pressure gauges are used only on the high vacuum of the exhaust, to check the U-tube. These are made of a thin glass tube bent in the shape, of a U with one end longer than the other. The longer end is bent over and brought down below the bottom of the U. (See Fig. 133.) The short leg of the U and a couple of inches of the other leg is completely filled with mercury, which is then boiled out and the top sealed. The whole tube is then mounted in a wooden case carrying a brass scale graduated in inches. The lower end is connected to the vacuum to be measured by a heavy rubber tube. Normally the difference in the heights of the two columns will be six to eight inches, but with a high vacuum on the lower end they will tend to equalize. The upper column has an absolute vacuum on it so that the difference in the height of the two columns represents the difference between the vacuum 277 being read and an absolute vacuum, or the absolute back pres- sure. The sum of the readings on the absolute gauge and the U-tube should check the barometer reading within less than 0.1 in. The mercury in the end ,open to the atmosphere slowly oxidizes and when this takes place the absolute gauge will record a smaller back pressure than is actually present. The gauge should be placed above the opening into the vacuum space and the rubber tube kept free from loops or water may lodge in it and be carried over on the top of the mercury when the vacuum is broken. If this occurs, the gauge must be sent to the laboratory and cleaned and refilled. The gauge must always be kept in a vertical position and never laid down or carried horizontally, or air will get into the sealed end. Turn on to vacuum very slowly and never take it off suddenly, or the mercury may break the sealed end. Temperatures The temperatures to be read are: Steam pipe (near pressure gauge), All stage shells (when called for), Air (near U-tubes and absolute gauges). The temperature of the initial steam is read as nearly as possible to the pressure gauge, the thermometer-well being placed diametrically in the steam pipe. Steam is available at any pressure up to 200 lb. gauge, and of varying quality. For running tests, which require high pressure arid low superheat, it is sometimes necessary to inject a spray of water into the steam. This is done at a considerable distance from the turbine in order to get a good mixture of water and steam. When dry steam is specified, it is best to hold about 15 deg. superheat; for, if a lower superheat be held, the temperature may drop to the saturation point where the condition of the steam cannot be determined without a calorimeter. " " ' When the testis finished, always shut off injection water to avoid filling the steam pipe with water, as this would cause a water hammer when steam is again turned on. In cases where it is necessary to read the temperature in the various stages, the thermometer wells should be located near the gauge and in the path of the steam; special precautions being taken so that the revolving part of the turbine will not strike the thermometer well. The temperature of the air near all U-tubes and absolute gauges is taken in order to correct the length of the mercury column to the same temperature as that at which the barometer reading is read. The man reading temperatures should fill the thermometer wells with mercury and be sure that there are no broken mercury columns in the thermometers in use. A thermometer should be placed as low in the well as possible with the readings to be taken, but do not have the mercury column below the point of immersion as vaporization of the mercury in the thermometer may take place. 278 Flow There are two methods in common use of measuring the quantity of steam to be consumed: The first is to weigh the water after the steam has been condensed in a surface condenser. The second is to measure the steam flow by means of a steam flow meter. The first method is the one most commonly used in the Testing Department, although in nearly all cases a flow meter is installed and readings recorded. Flow Tanks After the steam has been condensed in the surface condenser it is pumped from the hot well to the flow tanks where it is weighed. These tanks should be of sufficient capacity to hold the amount of steam condensed during six minutes. They are mounted one above the other. Both outlet pipes should be equipped with quick closing valves which shut perfectly tight. The upper tank is used as a reservoir, when taking weights on the lower, which is mounted on a pair of platform scales. To measure the amount of condensed steam, proceed as follows: Close the upper tank outlet valve on an even six minutes. Then close the lower tank outlet and balance the scale. This reading is called "tare." The upper valve is then opened, and closed after exactly six minutes have elapsed from the first closing. After closing, the scale is again balanced, and this reading is called "gross." The difference between the "gross" and "tare" is the "net" reading which when multiplied by 10 gives the flow per hour. After taking the "gross" reading, the lower valve is opened and the water allowed to run to waste. The valve is then closed and the "tare" again taken. This cycle is repeated as long as the test continues, care being taken to close the upper valve at exactly each six minute interval. If the flow is extremely rapid, readings may be taken at four or even three minute intervals. Slight variations will occur due to irregular pump or condenser action, but the average of a number of readings will give accurate results with constant conditions. At least five readings should be obtained for each load, or operating condition. Before taking any readings, the scales should be carefully inspected to see that the platform and the scale beam move freely. The scales should be calibrated frequently. This can be done by balancing the scales and then adding a 50 lb. standard weight. These should be placed on each of the four corners of the platform. The scales should be thoroughly overhauled occasionally and all knife edges kept sharp. When not in use the weight should be taken off the knife edges, by throwing the lever to the off position. Load There are two methods of obtaining load; one with an electric generator, and the other by the use of a water brake. 279 When an electric generator is used, the load is measured by means of wattmeters; ammeter and voltmeter readings being taken as a check. » te a, .5 ft .S c*22 $ .Es > .2 OJ b r;Mb g rt o"3 ,3 ft"£ 5 Mn ^ 6 F ft £ '-5^ *S. « Si 3.c 8***431 ef ^ >°^i J |l . h Jsh&ihfi NNNNNXxxxx'XxxMMaaaiafflacaoooocoooo Z O- iS'^^CCsriaCCCCCrt «« J2 aa o ^ 2 w: ■ To To ~ if C*CO "* »0 CD NWC.O-iN«^C!ONXCl OHO«-*tt rtrirnnHH rtHHMNJlNNNMONN ec re re re ~ ^ OQKKCoc ■-I m co ■* *Q co r- oo os c — eq s 287 ENGINE Single cylinder engines are used with generators from 2% to 60 kw. capacity, and vertical tandem compound engines with machines from 25 to 75 kw. capacity. The engines are standard commercial machines. See Fig. 135. Steam Pressures The ratings of the standard single cylinder engines are based on the steam pressures given in the following table and those designed for 80 lb. steam pressure can be operated at pressures up to 125 lb. either condensing or non-condensing. If higher boiler pressures are used a suitable reducing valve must be placed in the steam line to give the desired pressure. For steam pressures of less than 80 lb., single cylinder engines are fitted with large cylinders, to operate at pressures ranging from 35 to 60 lb. The tandem compound engines are designed to operate economically at 125 lb. condensing or 140 lb. non-condensing. Unless otherwise advised by Engineering instructions, all engines must be tested at the pressures given in the tables on pages 289 to 292 inclusive. These tables are a complete list of all types of engines manufactured. Lubrication Two systems of lubrication are used, gravity and forced. In the gravity system all the main bearings of the engine are lubricated from an oil reservoir attached to the engine (refer to Fig. 136) ; each bearing being provided with an adjustable sight feed for regulating the flow of oil. The waste oil collects in a bedplate reservoir, from which it can be drained, filtered and used over again. The bearings of the governor and valve gear are lubricated by compression grease cups. In the forced system the lubricant is passed under pressure to the various parts of the engines. The base of the engine forms an oil tank to which is attached a small plunger pump driven by an eccentric on the shaft. The oil is forced through grooves in the main bearings, drilled holes in the shaft connecting these grooves with the crank pin. The oil is also forced to the wrist pin through the pipe on the side of the connecting rod. The passages in the crosshead pass the oil from the wrist pin to the guides. After passing through the bearings the oil is collected in the base, where it settles and is used over again. The bearing caps must be set up tight and the main bearing liners must be close to the shaft; otherwise too much oil leakage will occur before reaching the last bearing. To prevent the entrance of foreign matter a strainer is attached to the suction valve of the pump. When the crank chamber is inspected, no waste, dirt or other matter must be allowed to enter and mix with the oil. When cleaning the oil chamber, canvas and not waste should be used, since the latter clogs the strainer. Only mineral oil should be used for lubricating. Since the oil passes through the bearings repeatedly, it gradually loses its lubricating properties, becoming thick and gritty. It should, 288 SINGLE VERTICAL CYLINDER ENGINE SETS, GRAVITY LUBRICATION TYPE DIMENSIONS IN INCHES Dia. Dia. Dia. Ex- haust Pipe Volts Full Amp. Full Steam Pres- Classification Cyl- inder Stroke Steam Pipe Load Load Lb. MP 4- 2 3^-700 3 Mi 3 % 1 110 23 80 MP 4- 3 -700 3K 3 % 1 110 27 100 MP 4- 4 -600 4^ 4 1 IV 110 36 80 MP 4- 5 -600 4K 4 1 Wa 110 45 100 MP 4- 7 -550 5 4H Wa m, 110 64 80 MP 4- 8^-550 5 4^ Wa IV?, 110 77 100 MP 6-10 -450 QV?, 5 IV?, 2 110 91 80 MP 6-12^-450 W, 5 IV?, 2 110 114 100 MP 6-15 -400 8 6 2 2V? 110 136 80 MP 6-17K-400 8 6 2 2V?, 110 160 100 MP 6-20 -360 9 7 2 V?, 3 125 160 80 MP 6-25 -360 9 7 2 V? 3 125 200 100 MP 6-30 -305 11 8 3 m 125 240 80 MP 6-35 -305 11 8 3 3V?, 125 280 100 MP 6-40 -305 11 8 3 SV2 125 320 125 Generators can be wound for 110, 125 or 250 volts. SINGLE VERTICAL CYLINDER ENGINE SETS, FORCED LUBRICATION TYPE DIMENSIONS IN INCHES Classification Dia. Dia. Dia. Volts Full Amp. Full Steam Pres- Cyl- inder Stroke Steam Pipe haust Pipe Load Load Lb. MP 4 -7 -550 5 4^ IV IV? 110 64 80 MP 4- 8^-550 5 4H IVa IV?, 110 / i 100 MP 6-10 -475 sv?, 5 IV 2 110 91 80 MP 6-12^-475 QV?, 5 IV? o 110 114 100 MP 6-15 -425 8 6 2 2V 110 136 80 MP 6-15 -425 6 6 2 ' 2Vo 110 136 150 MP 6-17V 2 -425 8 6 2 2V 110 160 100 MP 6-17^-425 6 6 2 2V 110 160 175 MP 6-20 -400 9 7 2V? 3 125 160 80 MP 6-25 -400 9 7 2 V? 3 125 200 100 MP 8-30 -315 11 8 3 33^ 125 240 80 MP 8-35 -315 11 8 3 3V 125 280 100 MP 6-40 -315 11 8 3 3 V 125 320 125 MP 8-50 -280 12 11 3H 4 125 400 100 MP 6-60 -280 12 11 sy 2 4 125 480 125 Generators can be wound for 110, 125 or 250 volts. 289 co w te o te w p te o o °te te o w o co fe P w H O W te o o H CJ W Ptf S* -; ■'.' 3«S ^ >w (D £3 . oooo rt cn,0 ■^t" 1 "^ ^ ^ " <8i-3 1— 1 T— 1 1— 1 T-H 4) oooo S3 d O X o o cm cm ^ co > Q "JO CO I> 05 O oooo C lOOO ^n -^ ^ r^ CO II ioiooio «C cm co to t^ '« 1 1 1 1 cS CO CO CO CO o pl, cm PhPh SEES CO W te »—i o te w p te P o ft § o « o pq co ^ O o £~ CO H w CO p W H o W CO te . te p o H o w to to io to io io cm cm cm cm cq cm o o o ooo O OO O to to ^oowtoco CO CM Oi io O O t-i i-i CM ^ (X) to to to to to to CM CM CM CM CM CM -I CO CO ^ to CO 3^^ \^ ^ ■H rH CM CM CO CO ^ CO!> 00 00 o 0) Ph J-l CD G Oi O CM ^ 00 IOCONNO OO OOOO to to o o o to IO tJH ^ t^ tjh CO I I I I I I 00 CO ^ CM O O * t-h (M CO to O I I I I I 7 co co oo oo oo oo PL, PL, PL, PL, PL PL, a cu CD 290 *3 co W H H W co CO c 5 a >>>.:>,>.>>>> >> >,_, 4_>.|j + j.ij.tj.(j.|j+o'-0'X3' , £j'0'^J hi o w C •r; -r -r - r •r •£ - r -r cd 00 |2j .-i^H^H^^^c^C^C^C^CvqCMtM ■»-> to \(N\N\(N\N \N Q-SS OqtMtMtMCOCOCO^^TfT^cOCO H t/i •So \CN\N \N\Cl>000000i-iT-i I So HH a Ih /p>e &r>c/ Vo/ve Fig. 138 PISTON ROD PACKING action. If the tension on this spring is not sufficient, the length of the indicator cards will vary; the higher the speed of the engine the greater will the variation be. The pressure of the pencil upon the paper can be adjusted by screwing the handle in and out. The line should not be heavy as this will cause unnecessary friction. After the diagram has been taken, close the cock and take the atmospheric line; then disconnect the cord to avoid excessive wear on the drum. 297 The following notes should be made on the card and any- other data which it is proper to add: Date Time Requisition No. Dia. of Rod Kw. Capacity Cylinder Card No. Boiler Pressure Stroke Exhaust Pressure Clearance Revolutions per min. Scale of Spring Volts Engine No. Amperes Cylinder No. Pounds of water per kw-hr. Dia. of Cylinder A trifle more lead at the crank end of the valve should be given at no load, as at % or full load the average pressure on either side of the piston will be found to be. practically equal, due to the angularity of the connecting rod. Various adjustments will be necessary to obtain the best diagram and operation of the engine. Packing In all single cylinder engines, up to and including the 30 kw. size, the Garlock Spiral Packing is used in both piston rod and valve stem stuffing boxes, and in the valve stem stuffing boxes of all engines, the leakage being taken up by tightening the brass nut on the box. In the piston rod stuffing boxes of the tandem-compound, cross-compound and of the single cylinder 50 kw. engine, United States Metallic Packing is used. Fig. 138 shows the "Double" type which is commonly used, but in some machines the "Single Junior" packing is employed. The general con- struction of the two packings is similar. The packings consist of vibrating cups A and A , receiving the packing rings 1, 2 and 3. These rings are in halves and, in assem- bling the packing, the joints should be broken. The vibrating cups rest upon rings B and B, which have a spherical bearing, so that the packing will follow the rod in any position. The steam pressure forces the packing down in the cups and against the piston rod, thereby preventing steam leakage. The coil springs C and C assist this pressure, at the same time holding the pack- ing in place and preventing the rings from following the rod at the moment of reversing. If the packing has been taken out for examination, the ground surfaces should be cleaned and freed from grit before reassembling. The box holding the packing is drilled and tapped for a % i n - waste pipe and fitted with a globe valve which should always be open. General Instructions An engine unit should not be considered mechanically nor electrically perfect, until the tests have so proved. Testers should familiarize themselves with every detail of design and operation, thereby helping toward the production of the most 298 reliable piece of apparatus. After the inspection in the Engine and Testing Department the unit is dismantled and thoroughly overhauled, touched up and re-inspected, preparatory to final shipment. GENERATOR The tests taken on the generator are duplicates of those described in preceding chapters. All standard d-c. generators are given only compounding tests and adjustment of shunts. On standard a-c. generators saturation and synchronous imped- ance are taken. If core losses are called for they are taken as previously described, the generator being either disconnected from its engine and assembled in shop bearings or the connecting rod, etc., of the engine is dismantled and a driving belt slipped over the engine flywheel. 299 CHAPTER 15 GENERAL ELECTRIC TEST TRACKS As the work on the General Electric Test Tracks is almost entirely experimental a large number of the tests require special instructions. The following rules, however, have been issued relative to the operation of trains on these tracks, as well as instructions for obtaining data, in testing apparatus. No test should be started nor should changes be made in any test without instructions from the office of the Supervisor of Test Tracks. All data should be recorded upon special record sheets and supplementary column sheets, or upon the special form sheets provided for that test. All data sheets should contain the name of the man in charge of the test, and date of test, while all supplementary column sheets should also contain in the upper right hand corner the number of the record sheet to which they belong. ELECTRIC LOCOMOTIVES Special form sheets are printed for testing locomotives, which should be carefully filled out. The procedure of testing is as follows : 1st. Inspect motors, contactor compartments, rheostat compartments, controllers, etc., for loose material, scrap wire, etc. Examine all bearings to see that they are properly lubri- cated, including motors, air compressors, dynamotors and all operating parts. 2nd. Ring out wiring to see that all connections are accord- ing to the wiring diagram. Inspect the wiring to see that all terminals are properly soldered and secured with lock washers; also that all parts of both the main and auxiliary circuits are properly insulated and that all wiring is so secured as to prevent the insulation being cut by chafing. 3rd. Take clearance measurements to see that the locomo- tive conforms to the clearance diagram. 4th. See that the current collecting devices are in proper condition and satisfactory for operation. Where third rail shoes are used this should include the pressure on the rail in the running position as well as the measure- ments showing the position of the shoe with respect to the third rail. On trolley poles and bases it should include the pressure of the wheel on the wire at some given angle of the trolley pole. This can be taken with a small spring balance attached to the trolley rope. It is well to note what this pressure is, both going up and coming down, to insure that the base does not have an undue amount of friction. On pantograph trolleys the pressures of the pans, or rollers, against the wire should be taken as on trolley poles and wheels. Where rollers are employed as collecting devices it should be 300 carefully noted -whether the rollers are free to revolve and whether they are in every way satisfactory to operate. 5th. Connect to the power circuit and try out the lighting circuit, including headlights. Pump up the air pressure and try out the air brakes, adjust all valves, gauges, etc., according to the air brake diagram and inspect all air piping for leaks. 6th. Check with the wiring diagram the contactors that are closed, both forward and reversed on each notch of one controller and if there are two controllers check in one direction of the second controller. For some typical connections see DS prints No. 15466, 28765, 28234, 29302, 39188. These prints are on file in the Testing Section office. 7th. Determine the rotation of the motors, each motor or pair of motors separately and with all motors cut in. This should be done in both directions on each combination. 8th. Measure the resistance of each step of the starting resistance to see that it agrees with the specification. This should be done by applying the air brakes so that the locomotive does not move and having an ammeter wired in the motor circuit. Put the controller on the first point with the main switch closed so that the current will pass through the motor circuit. Simultaneous readings should be taken of the current flowing and the voltage drop across the various steps of resist- ances. The voltmeter leads should be applied at the con- tactors, or controller fingers to which the resistances are attached in order to make an additional check on the wiring. Care should be taken not to keep the current on longer than is absolutely necessary to take each reading so as to avoid an increase in resistance due to heating. 9th. Where a blower is used for forced ventilation of the motors the distribution of air to the different motors should be taken, holding constant the voltage of the trolley and reading volts line, amperes input to the blower motor, speed of the blower motor and the air pressure at some given point on the motor so that the volume of air going through the motor can be obtained by comparing these results with the result of tests previously made on the test stand. Before starting this test an inspection should be made to make sure that all motor covers are on, air outlets from the motors open and that the air inlet and outlet of the blower are free from any obstruction. 10th. Run for tests on bearings and note the operation of all auxiliary parts. This test should be started at slow speed and the speed increased as soon as the temperature of the bearings will permit, to the maximum speed at which the locomotive is to be run and continued at this speed for several miles, or until the bearings and all operating parts are in satis- factory operating condition. 11th. Make a wheel slipping test by bringing the controller up, point by point, until the wheels slip and read volts line and amperes to the motor on each step of the controller. This test should be made in both directions with and without sand and with all the various combinations of motor cutout switches. 301 It is necessary to take readings on each point, beginning with the first, only once for each combination and after this the controller should be immediately brought to the point next below the one at which the wheels slip and readings taken at this point and continued as before until the wheels slip again. The controller should be thrown off as soon as the wheels start to slip so as to damage the track as little as possible. The wheels should not be allowed to slip more than once in the same spot otherwise a false indication of tractive coefficient might be ob- tained. 12th. Remove all grounds and take insulation and high potential test. These should include all the wiring and all parts of the electrical equipment. Mounting Motors on Trucks Before mounting motors on trucks, the following measure- ments should be taken: Compare bore of gears with size of axle for gears ; compare bore of axle liners with size of axle for liners ; compare the distance between wheel hubs with the length of the motor; axle liner flanges and gear hub; compare the distance between the center of axle and suspension bar face on- truck with the distance between the axle box centers and face of motor under nose suspension. After these dimensions have been checked, and the motors have been found to fit on the truck, the key for the gear should be fitted in the key- way and the gear put on, care being taken to get the right side of the gear next to the hub of the wheel, and to see that all lock washers and cotter pins are in place. The motor should then be hoisted by the two lugs opposite the axle bearings with a two hook chain, and the motor placed on the axle without axle linings. The motor can then be lowered in place, by allowing it to revolve around the axle until the nose suspension rests on the suspension bar. The chains can then be hooked in the two lugs nearest the axle bearings and raised enough to allow the axle linings to be put in place. The axle caps, gear cover and strap fastening the motor to the suspension bar can then be put on and the installation is complete. Before the motors are put into service or the car run as a trailer, the motor bearings and gears should be properly lubri- cated. Trolley Bases Test sheets should contain the following data: Number and size of spring (outside diameter, free length, number of turns and size of wire). Position of tension adjusting screw during test. Length of pole from pivot to center of trolley wheel. Style of harp and wheel. Length and tension of springs with pole, in horizontal and 45 degree positions. Pull Curve This curve is taken by measuring the vertical pull in pounds at the center of the trolley wheel for different heights of the wheel. 302 The "height" of the wheel is the vertical distance of the center of the trolley wheel above its position when the pole is hori- zontal. (For pantograph trolleys the height is the distance of the top of the pan above its position when locked.) In taking this test a rope should be fastened about the wheel and readings of pounds pull taken, both going up and coming down. Service Heat Runs on Motors These heat runs are made on motors under as nearly as possible the same conditions as will obtain in service. By making a number of heat runs under various conditions data is obtained from which the thermal characteristics of the motor are determined. These curves show the relation between the ratio of distribution of losses (ratio between watts loss in field and in armature) to the degree (Centigrade) rise per watt loss for the armature and for the field. The instructions for the test include the following points: (a) Weight of train. (b) Line voltage to be held. (c) Accelerating current required. (d) Schedule (includes length of run, time power is on, time of coasting, time of braking, and time of lay-over). The following readings must be taken before starting the test: Resistance of field, total and partial. resistance of armature. In order to facilitate the measurement of armature resist- ance during the run, resistance readings are taken between commutator bars nearer to each other than the distance between brushes. These bars should be marked or the resistance taken with a templet, in order that all measurements can be made between the same points or including the same number of bars. The ratio between the partial resistance to the total resistance is a constant from which the total resistance can be calculated. The following must also be taken during the test: Air temperature, velocity and direction of wind, readings during test (taken every hour), field resistance, partial resistance of armatures of alternate motors, temperature by thermometer of field spools and frame, and air temperatures. During the run a record is kept of the schedule, direction of wind, weather conditions and all points of any interest in connection with the runs. Records of the line voltage and amperes motor are taken with graphic recording meters for a couple of runs in each direction during the hour. When the temperatures of the motors have become constant, the test is stopped. Besides the regular hourly readings the following temperatures are taken: Armature core surface, and conductors; commutator; field spools; frame. These readings should be taken indoors in order to avoid all draughts. Train Friction Train friction curves show the relation between the train or car friction expressed in pounds per ton and speed in miles per hour. 303 There are two methods by which car friction may be obtained, coasting tests and free running. Friction from Coasting Curves The. test should be made on a straight and preferably level track. The car is accelerated to a speed slightly greater than the highest speed called for on the friction curve and allowed to coast. Speed should be measured with a speed recording instrument. Runs should be made in both directions. From the rate of retardation at any point the retarding force is calculated which represents the total car friction at that speed. The weight of the car plus the flywheel effect of the revolving parts is the weight that tends to keep the car moving. When geared motors are used, a test should be made to obtain the rate at which the armature will slow down due to the friction of its own bearings in order that it may be known whether the flywheel effect of the armature will be sufficient to overcome the friction of its own bearings and furnish power to assist in keeping the car moving, or whether the car will have to furnish power to keep the armature revolving. The type of motor and the gear ratio should be given, together with any information that can be obtained, regarding the type of car, arrangements of wheels, wheel base of truck, etc.; if possible a photograph, or a sketch showing the cross section of the car, or locomotive should be included. Friction by Free Running With the car running at constant speed, readings of speed, volts line and amperes should be taken, preferably with graphic recording meters. The input to the motors, minus their elec- trical losses, gives the power absorbed in friction at a given speed. It is very difficult to get accurate results by this method on account of the difficulty of keeping the car speed absolutely constant. The test sheets should contain the following data: Weight of car or train. Diameter of wheels and speed of car. The number, rating and serial numbers of motors, and gear ratio, must be given. Operating Rules Each man, when starting work on the Test Tracks, is given a copy of the "Operating Rules." These must be carefully learned and implicitly followed at all times. 304 CHAPTER 16 BLOWERS Commercial Tests consist of the operation of the blower for such a length of time as is necessary to demonstrate that no electrical or mechanical faults exist. In case the motor is of sufficient power to drive the fans with unrestricted inlet and outlet it is so tested, but in most cases the motor is provided for a certain specified pressure and volume delivered from the fans and will not operate the fan with unrestricted inlet and outlet without overloading the motor. In such cases the load on the motor can be limited by partially obstructing the inlet to the fan by means of a blower or other restriction so that the motor will not be subjected to an excessive load. Standard Heat Run consists of the operation of the machine with air delivery restricted for a specified time or until constant temperatures of the motor are reached. This restriction may be for the purpose of bringing the load on the motor to a specified amount or may be a restriction to give the required air delivery for which the fan is to be supplied. Minimum Speed Heat Run consists of a heat run at full field with unrestricted inlet and outlet for a specified time or until constant temperatures are reached. Maximum Air Delivery Heat Run consists of operating the blower at full speed with the inlet and outlet unrestricted for a specified time or until constant temperatures of the motor are reached. Endurance Run consists of running the machine for 48 hours with the specified restriction of blower inlet and outlet. In case of ventilating fans for the Government, this consists of a 40 hr. run in addition to the 8 hr. " Normal Air Deliverv Heat Run." General Tests consist of the following: (a) Running the machine with air delivery restricted for a specified time, or until constant temperatures of the motor are reached. (b) 48 hr. endurance run (40 hr. in addition to the normal air delivery heat run). (c) Heat run at full field with unrestricted inlet and outlet for a specified time, or until constant temperatures are reached. (d) Air measurements to determine the delivery of the blower. Special Tests consist of general tests on the blower to obtain air delivery under different conditions of opening and under different speeds. Complete Tests consist of the following: (a) Running the machine with air delivery restricted for a specified time, or until constant temperatures of the motor are reached. (b) 48 hr. endurance run. 305 (c) Heat run at full field with unrestricted inlet and outlet for a specified time, or until constant temperatures are reached. (d) Tests on the blower to obtain air delivery under differ- ent conditions of opening and under different speeds. 1. DOUBLE PITOT TUBE OR GOVERNMENT METHOD This test is made in accordance with Government specifi- cations issued by the Navy Department under the cognizance of the Bureau of Construction and Repair. For making air tests in accordance with this method using double Pitot tubes, a testing pipe preferably of galvanized iron having the same shape and size as the outlet of the fan and a length equal to twenty times the diameter of the pipe, if round, or twenty times the average of the width and depth, if rectangu- lar, should be connected to the fan outlet. This pipe should be smooth and carefully fitted to the fan in order to avoid any unnecessary obstruction to the free passage of the air. It is sometimes inconvenient to use a pipe of exactly the same shape as the fan outlet, and in many cases it would be permissible to use a pipe of nearly the same area connected to the fan outlet by an adapter gradually changing from the size of the outlet to the size of the pipe. The double Pitot tubes should be supported in the middle of the test pipe half way between the two ends and should be parallel to the sides of the pipe and pointing toward the fan. All connections between the Pitot tube and the Manometer or U-tube should be carefully made to avoid any possible leakage, as a very small leakage in the connections of these rubber tubes might seriously affect the reading of the manometer. In making the measurements the exact area of the pipe where the Pitot tube is located should be carefully measured allowing for curvature of the sides of the pipe which sometimes takes place when the pipe is made of thin material and the pres- sure in the pipe is considerable. When the area of this pipe differs from the area of the outlet of the fan, the results should be corrected accordingly, as the air velocity will be greater in a smaller pipe and the static pressure less, but the total impact pressure will not be affected except by the increased friction of the smaller pipe. A suitable damper or door should be placed at the end of the testing pipe so that the size of the opening may be adjusted to obtain the proper pressure and volume. Care should be taken to run the fan at rated speed as nearly as possible, but where this is impracticable, correction may be made for small varia- tions in speed by correcting the volume in proportion to the speed and the pressure in proportion to the square of the speed. The most accurate results are obtained by using a nest of Pitot tubes connected to floating manometers which consist of metal cans floating in water, divided into as many air tight compartments as there are Pitot tubes ; but it is more convenient to use a single tube in the middle of the pipe, in which case, according to the U.S. Navy rules, the velocity determined by 306 the Pitot tube should be divided by 1.10 to obtain the assumed average velocity through the whole pipe. In calculating the horse power the total impact pressure is used without any reduction, although to be strictly consistent the velocity head due to the average velocity of the pipe added to the static pressure should be used. When the blower is provided with a straight inlet a con- siderable loss is occasioned by vena contracta which will not take place when the inlet piping is finally installed on the fan. If the fan were tested with nothing added to the inlet, the efficiency shown by the test would be too low and it is desirable to put a short cone or bell on the inlet of the blower in making the efficiency test unless the fan is built with a cone inlet. Use of Air Table When conducting a fan test the temperature of the air in the testing room should be taken by two Fahrenheit thermom- eters, placed near the fan. One should hang free in the air, and the other, with its bulb wrapped in thin cloth, should be sus- pended over a small receptacle filled with water so that the cloth will be saturated. The temperature of the water must be the maximum that it will naturally attain in the room, Corrected barometer reading must also be recorded on the test sheet. The method of finding the weight of air from the air tables mentioned in the specifications, is as follows: On the page containing the dry bulb reading as recorded on the test sheet, note the barometer reading corresponding to the first three figures of the corrected barometer reading recorded on the test sheet. In the column under the dry bulb temperature and opposite the barometer reading, the corresponding weight of saturated air is given. The weight of air found in the table must then be corrected to correspond with the corrected barometer reading found in test. This correction will be found in the second line from the top of the page. Correction must also be made for the difference between the wet and dry bulb temperatures by adding to the weight of air already obtained the number in the third sub-division of the column under the dry bulb temperature which corresponds to the difference between the wet and dry bulb reading. This reading will be found in the second sub- division of the column. Example Given barometer reading 30.15 in. Dry bulb reading 67° F. Wet bulb reading 59° F. Under the column showing the dry bulb temperature of 67° and opposite the barometer reading of 30.1, the weight of air is given as 0.07517. The addition for each 0.01 of an inch of barometer is given as 2.6 in the second line from the top of the page. Multiply this by 5, i.e., by the excess of the corrected barometer reading over that selected in the table; the result is 13, which must be added to the weight of air previously found. 307 The wet bulb depression is the difference between 67° and 59°, or 8°. The number opposite 8 is 23. This must also be added, making the total weight of air 0.07553. All pressure readings should be corrected for standard air (see page 309) by multiplying the actual pressure obtained by the ratio of the weight of standard air to the weight of air at the time of test. The readings of horse, power input to the fan should also be multiplied by this ratio. Pressure and Horse Power Curves by Double Tube Method A pressure curve may be taken by the double tube method as follows: The opening at the outer end of the discharge pipe should be closed and pressure and power readings taken. Under this condition the static and impact pressures should be exactly the same since no air passes through the fan. Readings should then be taken by increasing the opening by suitable increments from closed to wide open, measuring the opening each time. The speed of the fan should be held constant throughout the test. The air readings and electrical input readings should be taken simultaneously. It will be noted that in a test which is made with a pipe on the discharge side of the fan, the reading of the impact tube is always greater than the static reading. If the pipe is on the suction side the readings will be negative and the greater numeri- cal value will be given by the static side of the tube. This should be considered as the value for impact pressure of the fan. The smaller value is given by the impact tube and should be treated as static pressure when considering the capacity of the fan. If readings are taken by means of a U-tube, the reading of both sides of the tube should be given on the test sheet. The test sheet should always specify whether the readings were taken by the U-tube or by a manometer. If by a manometer, the manometer constant should be recorded and must always be used in working up the test. CALCULATION OF FAN TESTS BY THE DOUBLE TUBE METHOD A fan test of this kind should be recorded in the following form of the standard column paper provided for this purpose. The same abbreviations should always be used to avoid confusion. TYPE OF FAN SERIAL NUMBER DATE... Motor Rating Double Tube Test, Taken at R.P.M. No. hi hi h 3 *S V Q hl+hf ht+h f Air H.P. Fan H.P. EfL 1 2 3 4 I Wet Bulb °F. Barometer... ....in. Dry Bulb °F. Wt. of Air lb. Effective area of Pipe = Sq. Ft. 308 The first column gives the number of the reading. The second and third show the impact and static readings taken from the test sheet and corrected for standard air. The fourth column shows the velocity head or the difference between hi and h 2 . The fifth column is friction which must be calculated from the velocity head bv the formula H = ^- X 0.000 16 lv 2 . ab TT hf= w?r-^, where h/ equals friction loss in inches of water, / is oy./o \ the length of pipe in feet between the fan and the Pitot tube. a = length of long side of pipe in feet. b = length of short side of pipe in feet. i» = average velocity in feet per second. The friction loss should be added to both the static and impact readings before the curves are plotted, but it does not affect the volume. The sixth column showing the air velocity at the center of the pipe may be obtained from the curves shown on prints C-4487-A, B, C, and D. It may also be obtained from the formula V=1097-*|— Where to = weight of air per cu. ft. in pounds. This gives the velocity at the center of the tube. For the average velocity use 91 per cent of this value or use the same formula with a constant of 997 instead of 1097. The volume must be given in the seventh column. It is obtained by multiplying the average velocities given in column six by the area of the pipe. The horse power in the air can be calculated from the formulas .. , PXQ PXQ hXQ Air h ' p - = 33000 ° r 3667 ° r 6345 . The horse power input to the fan is the horse power output of the motor. Unless instructions are issued to the contrary, all fan tests for Government work should be plotted with pounds per sq. ft., horse power input to fan, and efficiency as ordinates; and volume in cu. ft. per minute as abscissae. Both static and impact pres- sure should be plotted. The tester should carefully date and sign each test sheet, and should include sufficient data to distinguish all sheets used on the same test. For instance, electrical readings are usually placed on one sheet and fan pressure readings on another, therefore, each of these sheets should state the name and number of the fan, the rating of the motor, the speed at which the test was taken and the method used. The Calculating Room must see that this data is placed on the Calculation Sheet. The sheet on which the curves are plotted should give the name, type and number of fan, rating of the motor, speed at which the test was taken, and the method employed. Curves should always be plotted across the width of the sheet. 309 2. CONE METHOD OF TEST The following method of conducting a fan test is used only when a short convenient method is required for purposes of comparison. In this method of test an adapter is used, where it is necessary, to change the fan outlet from rectangular to cir- cular, a cone being placed on the circular end. This cone is made up of sections about two feet in length, the sides of which slope about two inches to the foot. Readings are taken by a single Pitot tube, the open end of which is held flush with the opening in the outer end of the cone and pointed against the stream of air. Pressure is registered as before, by a manometer or U-tube. The readings are taken, one at the top, one at the bottom, and one at each side of the cone at a distance from the edge of the pipe of about % of the diameter of the opening. A reading is also taken in the center of the cone opening. The average of these five readings represents the impact pressure produced by the fan, and is taken as the velocity head. The velocity may be obtained from the curve or from the formula given for the double tube test. The static pressure may be obtained as follows: Divide the volume of each opening by the area of the fan opening, which gives the outlet velocity V\. The corresponding velocity head can then be obtained from the curve. The velocity head sub- tracted from the impact pressure gives the static pressure. The static pressure should be plotted as well as the impact pressure. These tests should be plotted with pressures in inches of water, h.p. inputs to the fan, and efficiencies, as ordinates; and volumes as abscissae. The following form should be used for tabulating the results of calculations: TYPE OF FAN SERIAL NUMBER DATE Motor Rating Cone Test Taken at R.P.M. No. hi V Ae Q Vi h s hi Air H.P. Fan H.P. Eff. 1 2 3 Wet Bulb °F. Barometer in. Dry Bulb °F. Wt. of Air. lb. After the curves are plotted, the efficiency, as given by the calculations, should be checked, with the efficiency obtained from the curves. This will correct any discrepancy between the efficiencies as obtained from the curve and as calculated. 310 3. THE BOX METHOD The box method of testing fans is as follows: The fan is arranged to discharge directly into a large box which has a sufficient capacity to reduce the air velocity to a minimum. An opening is made in the side of the box at right angles to the opening into which the fan discharges, and cones are attached similar to those used in the cone test. Readings are taken by the same method and readings should also be taken of the box pressure by a U-tube connected to a pipe inserted through a hole in the side of the box. The end of the pipe should be flush with the inside of the box to avoid eddy currents. The pressure shown by this pipe will be somewhat higher than that registered at the end of the cone, and both pressures should be corrected for standard air and plotted on the final curve sheet. The volume must be calculated as in the cone test, but the pressure obtained in the box is taken as the static pressure produced by the fan, since the velocity head is lost in the box. To obtain the impact pressure the volume obtained should be divided by the area of the opening of the fan, and the cor- responding velocity head taken from the curve. This velocity head should be added to the static pressure shown by the cone readings. For transformer ventilation it is customary to calculate the pressure in ounces, measured at the cone opening. The following form should be used in tabulating the calcula- tions: TYPE OF FAN SERIAL NUMBER DATE Motor Rating... Box Test Taken at R.P.M. NO. /J2 P v Ae Q Vi hz hi Air H.P. Fan ' -pa: H.P. btt - 1 2 3 4 Wet Bulb °F. Dry Bulb °F. Barometer in. Wt. of Air..... lb. Fan h.p. should be calculated from the static pressure and the efficiencv obtained will be the static efficiencv. FORMULAE FOR BLOWER TESTS h\ = Impact head in inches of water. h 2 = Static head in inches of water. h 3 = Velocity head in inches of water — hi — hi. h= Total head in inches of water =/*i+ Ay w = Weight of air in test in pounds per cu. ft. 311 B = Barometer reading. h f = Head lost in friction in the pipe from the Pitot tube to the fan, in inches of water. H/ = Head lost in friction in the pipe from the Pitot tube to the fan, in feet of air. Hz = Velocity head of the air in feet of air. . a = Length of long side of pipe in feet. b = Length of short side of pipe in feet. / = Coefficient of friction =0.00008 for ordinary piping. This value should be used in determining the friction loss between the fan and Pitot tube, but for determining the amount of pressure required to overcome the resistance of air piping, it is usually safer to use a coefficient of 0.00010. I = Length of pipe in feet from Pitot tube to fan. v = Mean velocity of air in ft. per sec. V = Velocity of air in ft. per min. Q = Volume of air in cu. ft. per min. P = Pressure of air in lb. per sq. ft. . -p , . . . PX16 P p = Pressure of air in ounces per sq. in. = . = -^. A =Area of pipe in sq. ft. A e = Effective area of pipe in sq. ft. =A XK K = Constant for effective area of pipe =0.94 for the Cone Method. Eff = Efficiency. w = Weight of air in test in pounds per cu. ft. Weight of 1 cu. ft. of air at 30 in. Bar; 70 deg. F and 70 per cent humidity = 0.07465 lb. This is taken as standard air. Wefght of water = 62.36 lb. per cu. ft. at 62 deg. F. Weight of a column of water 1 ft. sq. and 1 in. high = ' = 5.2 lb. at 62 deg. F. Weight of a column of standard air 1 ft. sq. and 1 ft. high = 0.07465 lb. Weight of a column of any other air 1 ft. sq. and 1 ft. high = w. xt 1 x- 1 .j-x 0.07465X5X530, ^ u Neglecting humidity w = 30X ( 46 q +1 o j for Fahr - at i ,■ i. ■/■, 0.07465X5X294, _ , Neglecting humidity w = 30 x (273 +^ °)~ Therefore, to change from feet of air to inches of water 5 2 divide by - _ ' Anr =69.73 for standard air. 0.0/465 5 2 or divide by — — for any other air. w H f hf= 5.2 312 ab For round or square pipe JHy-=4/-j- o 2 where d = diameter in feet. / / — Jo. 2 hz \hz v =\/2 ^ 3 = 8.02 \ Hz= 8.02 J— ^~ = 18.28-J- F =60 f=60v2 £# 3 =481.2\/#3 = 1097 —at the center of the pipe. $"'« = -i015\/liz for standard air. P =9 p = o.2Xh Therefore 9 p=5.2Xh P = IT32 = °- 577 * <2 =rx.4,= Fxxi av. vel. I . = 0.94 J Ihz =3654.0 A \/hz, using t*ot//d£>e aVfecteaf /n case or^oz/ure or^o/tape on motor or- tnroupn tran&for/ner to motor /cads Cat>/e C/a/np SacAr f/nper B/oc/c CyZ/rtcfer front /7/?aerfi/oc# Fig. 155 CONNECTIONS OF QUARTER-PHASE HIGH VOLTAGE TYPE NR STARTING COMPENSATOR WITH NO-VOLTAGE AND OVERLOAD RELAY 348 Fig. 156 CONNECTIONS OF THREE-PHASE, TYPE I, INDUCTION MOTOR AND TYPE NR, FORM A2 STARTING COMPENSATOR WITH NO-VOLTAGE RELEASE ONLY Generator Fig. 157 CONNECTIONS OF THREE-PHASE TYPE I, INDUCTION MOTOR AND TYPE NR, FORM A3 STARTING COMPENSATOR, WITH NO-VOLTAGE AND OVERLOAD RELEASE 349 Connect to a /otv tens/on circuit lyh/ch wot/A* be affected /n case of faik//e of yo/tage on the motor or through transformer to motor /eads Fig. 158 CONNECTIONS OF CR HIGH VOLTAGE THREE-PHASE STARTING COMPENSATOR WITH NO-VOLTAGE AND OVERLOAD RELEASE Fig. 159 CONNECTIONS OF QUARTER-PHASE, TYPE IQ, INDUCTION MOTOR AND TYPE NR, FORM A3 STARTING COMPENSATOR WITH NO-VOLTAGE AND OVERLOAD RELEASE 350 lowest voltage tap is next to the core). Standard compensators for motors up to and including 17 h.p. have 50, 65, and 80 per cent taps; those for motors above 17 h.p. have 40, 58, 70 and 85 per cent taps. The ratios obtained should agree to within 3 per cent of the above. In determining ratios see that both the primary and secondary instruments are on the same phase. In checking the ratio of quarter-phase compensators, join leads A' and A' (see Fig. 154), apply 100 volts to the lines A and A, and read the voltage on the taps between the motor leads B, B and each tap. These compensators are tested "open delta." Magnetizing Current Magnetizing current is measured at normal primary voltage and frequency. The alternator used should operate at normal voltage. The exciting current at normal voltage and frequency should, on 60 cycle compensators, not exceed 25 per cent, and, for 40 and 25 cycle compensators, it should not exceed 30 per cent of the full load current of the motor, assuming in the smaller sizes, the motor to operate at 75 per cent efficiency and in the larger sizes at 80 per cent. On special compensators, covered by Engineering Notices, the magnetizing current should be taken at 20 per cent above normal potential as well as at normal. In making this test hold the voltage constant across one phase and read the current in all three legs, then hold the current constant in one leg and read the three-phase voltage, or instead of holding current in one leg, two voltmeters may be used, one to hold the voltage constant, and the other to read the three-phase voltage. Owing to the fact that these machines are used for starting duty only, a high current and magnetic density is employed. Therefore, a very small change in frequency or potential makes a con- siderable difference in the exciting current, and care must be exercised to see that the voltage and frequency are normal. Quarter-phase compensators are tested "open delta." It will be noted that on three-phase compensators one leg will read slightly lower than the other two, which should be balanced. This is due to leakage caused by the high magnetic density and the close proximity of the iron case and supporting straps. Heat Runs Short-circuit the motor leads and apply sufficient voltage to the line leads to force the required current through the coils. This current should be held constant for one minute and the impedance volts read in each phase during this period and on each set of taps. The value of the current will be given in the standard Engineering Brief, or in Engineering Notices covering special cases. Thirty minutes should elapse between successive heat runs on the same compensator up to and in- cluding 200 h.p. ; above this size one hour should be allowed. A thermometer should be placed on each coil and the temper- 351 atures watched until they attain a maximum after each run and this value should be recorded. Directly after the close of each run the tap leads should be changed to the next tap. Heat runs should always be started on the tap next to the core. On large compensators it sometimes happens that there is not sufficient power available to make the heat run as called for. In this case upon permission from the Engineering Dept. the following alternative may be used: Hold half the current called for, and hold it four times as long. This will give an equivalent heating. After the completion of the heat run the taps should be taped up after placing the tap leads on the second set of taps. All compensators should be sent out with the tap leads on this tap. Insulation Tests The double potential and the high potential tests should be applied after all other tests are completed and the compensator is assembled with the taps taped up. The frequency should be high in order to keep the magnetizing current below the normal current for which the compensator is designed. In case the normal voltage of the compensator is so high that it is impossible to secure double potential, one set of taps may be connected to the line and voltage applied, which shall be double the voltage for which the tap is designed. All compensators up to and including 550 volts normal rating should receive 2500 volts insulation tests from windings to core and frame for one minute; those from 550 to 4000 volts should receive 7500 volts; those for 4000 volts should receive 10,000 volts; those above 4000 volts, double normal potential. In applying the high potential tests all leads should be connected together. 352 CHAPTER 20 MINE AND INDUSTRIAL LOCOMOTIVES MINING LOCOMOTIVES Mining locomotives (LM type) are built for various gauges in sizes of 3 to 20 tons. With, the exception of an occasional 3-motor, 6-wheel type they are all 2-motor, 4-wheel locomotives and are equipped with either 250 or 500 volt series wound, totally enclosed motors mounted directly on the axles and driving through double reduction gearing. The controllers are of the "R" type, which have a separate cylinder for forward and reverse in which is incorporated a commutating switch that permits starting the locomotive with motors either in series or in parallel. Before being sent to the Locomotive Department the various parts of the equipment are tested separately; the motors being subjected to the standard test for railway motors and the con- trollers, circuit breaker, etc. being subjected to the regular tests in force in their respective departments. The test of the locomotive proper is, therefore, principally a bearing run, a check of the wiring connections and a general inspection to see that all parts operate properly, that clearances are sufficient and that the apparatus is properly located. Unless otherwise specified, tests should be conducted as follows: 1. Anchor the locomotive securely on the testing stand that is provided in the Locomotive Section and operate it on all points of the controller, forward and reverse, both series and parallel, to assure that connections have been properly made. Caution: As these are series motors running practically without load, power should be thrown off as quickly as possible when checking with the controller in the "parallel" position. 2. Make a bearing run of 15 minutes duration in each direction at full "series" position of the controller. 3. Measure and record the resistances of the several rheostat steps. A 20 per cent variation from the values given in the DS print is allowable. 4. Make a careful general inspection to see that the brakes, sand rigging, headlights and circuit breaker operate properly; that the wiring cables are clamped securely and that they do not interfere with the access to the motor bearings or other parts; see that the rheostat terminals have good clearances to "ground" on the locomotive frame and check up carefully all questions on the testing record. Cable Reels Many locomotives, particularly the 5 and 6 ton sizes are equipped with motor-driven cable reels. The purpose of the reel is to permit operation over those portions of the mine roads that are not provided with trolley wires. The reel 353 rotates with its axis vertical and is driven by a four pole, series wound, vertical motor which is wired directly across the line in series with a permanent resistance to protect it from an injurious rush of current when the motor is stalled. The outer end of the cable is hooked over the trolley wire and as the locomotive moves forward the reel motor is overhauled and acts as a series generator, its counter torque producing sufficient tension in the cable to pay it out evenly. As soon as the loco- motive starts back and slackens up on the cable, the motor action comes into play and winds up the cable; the action is analogous to that of a spring having infinite length. Test as follows: 1. Measure and record the cold resistance of the armature, field and permanent rheostat. 2. Check the polarity. 3. Check for satisfactory operation by mounting the reel equipment on the shop locomotive that is provided for this purpose and run it out on the test track. At least five trials should be made running the full length of the cable. The reel should pick up and wind the cable compactly when the locomotive is running on the full series point of the controller. 4. When the reel equipment is mounted on its own loco- motive, check the rotation (looking at the top of the reel) as follows: If the motorman's seat is on the left hand side of the locomotive the rotation should be counter-clockwise. If the seat is on the right hand side of the locomotive the rotation should be clockwise. Winding Devices For hauling cars out of mine slopes where the grade is too steep for locomotive operation some locomotives are equipped with winding devices. These consist of a vertical axis cable drum fitted with 400 to 600 ft. of flexible steel cable and driven by a series wound, totally enclosed motor. Test as follows: 1. Give the drum and motor a 15 minute bearing run, holding them down to moderate speed by applying the band brake on the drum. 2. See that the brake and clutch levers operate readily and that the clutch engages properly. 3. With the clutch disengaged, see that the cable can be hauled out by hand easily. Use a spring balance and record the pull required; this must not exceed 45 lb. 4. Measure and record the resistance of the starting rheostat. INDUSTRIAL LOCOMOTIVES Industrial locomotives (LS type) are built for various gauges and in sizes from 3 to 25 tons. They are practically all of the single truck, 4-wheel, 2-motor type. The electrical equipment in general is the same as for the mine locomotives and they differ only in the mechanical arrangement of the 354 frames. With the exception of the larger sizes (15 to 25 tons) the test should be conducted in the same manner as for the mining locomotives. Those of 15 tons and above are, as a rule, built for the standard gauge (56 3^2 in.) and are equipped with cabs, air brakes and MCB couplers. Instead of using the testing stand in the Locomotive Section, these should be tested on the General Electric Company test tracks and the general instructions in force there will apply. STORAGE BATTERY LOCOMOTIVES Storage battery locomotives (C.S.B. and L.S.B. types) are at present built in various sizes, from 2^ to 8 tons. These as a rule will be single truck, 4 wheels, with either one or two motors, and for various gauges from 24 in. to 563^ in. The equipment differs from the standard mine (L.M.), and industrial (L.S.) types, in having low voltage automobile type motors, driving the wheels by double reduction gearing in place of the regular 250-500 volt motors. The storage battery will usually consist of 44 "lead acid" cells or 70 to 80 Edison cells, all connected in series for an average discharge potential of 85 volts. After the battery is in proper condition of charge as herein- after described, the locomotive should be placed on the testing stand and test conducted in the same manner as before described for mining (L.M.) and industrial (L.S.) type, i.e., operate on all points of the controller forward and reverse to see that all connections are properly made, make 15 minute bearing runs in each direction; measure the resistance of the rheostat; and make a general mechanical inspection of brakes, sand rigging, headlights, wiring, etc. When a locomotive has been delivered to test, each and every cell should be carefully inspected to see that the electro- lyte is at the proper level. This level varies for the different types and makes. For the "Lead Acid" battery (distinguished by a rubber jar) the level of the liquid should be Y2 in. above the plate, for the Edison (distinguished by metal jars) the level of the liquid should be Y2 in. above the plates for the A-4 and A-6 types, and y % in. for the A-8, A-10 and A-12 types. Caution: Gas may be present in the cells. Do not use a match, candle or other open flame to inspect. The lead cell batteries may be easily inspected by removing the cover or the soft rubber plug. For determining the height of liquid in Edison cells the method illustrated in Fig. 160 will be found convenient. If the liquid is low, sufficient pure distilled, water should be added; never use water suspected of containing the slightest impurities as very great damage to the battery may result. After ascertaining if the liquid is at the proper height see that the several battery trays or crates are properly connected in series, as otherwise a portion of the battery might easily be ruined. 355 Since it is impossible here completely to describe the various methods of charging the several types of batteries, due to the fact that the several manufacturers recommend slightly different procedure, the following brief summary must suffice for the first charge while the battery is temporarily in our care: The battery should be placed on charge at the normal rate as given with the instructions that accompany each battery. For lead Fig. 160 QUICK METHOD OF DETERMINING PROPER LEVEL OF ELECTROLYTE ABOVE PLATES batteries when the voltage has reached a value of 2.55 volts per cell (112 volts for 44 cells) the charging should be discon- tinued. For Edison batteries, charge at the normal rate as given on the name plate for 7 hours or until the voltage has reached a value corresponding to 1.85 volts per cell. When all tests have been completed, the locomotive may be shipped without recharging, as the running light test will as a rule use but little of the battery charge. Fig. 161 shows the proper method of connecting a battery to the line for charging. 356 Vo/t meter Ammeter Fig. 161 DIAGRAM SHOWING GENERAL METHOD OF CHARGING BATTERIES The trays are first connected in series, i.e., the. negative of one tray to the positive of the adjoining tray. The current flows from the positive wire of the current supply, into the positive terminal of the first tray (in this case on the right) ; through the positive and out of the negative of each cell and each tray in turn and returns to the current supply from the negative of the last cell. The voltmeter is connected inside the resistance or rheostat, to show the battery voltage only. 357 CHAPTER 21 PORCELAIN INSULATORS Insulators are of two distinct types; link insulators and bushings. The Link Insulators are those used for either strain or suspension work and have holes, called cableways, for fastening the cables. Bushings comprise all other kinds of porcelain insulators which are cylindrical in form, and serve as conduits. Inspection Before testing, all insulators should be given a rigid inspec- tion for mechanical defects, such as cracks, flaws, warping, chipping and non-uniformity in color of glaze. Methods Used in Applying High Potential In applying high potential to porcelain insulators, they are placed on a rack which holds twelve, and these are tested together. In the larger type requiring a special test, it will be found advantageous to use two racks at once. The Link Insulators have cableways on either side between which the potential is applied. This can be done by using two spiral springs which can be pushed through the cableways and hooked upon themselves, thus making the insulator take the same position as it does in service. In testing bushings, a pipe or spring is laid through the center of approximately the same size as the hole. A piece of metal foil or spring is then wound around the outside at the middle point. The potential test is then applied between the metal parts. Routine Potential Tests on Insulators for Switchboard Depart- ment Potential values, where called for, should be determined by the needle gap and striking distance curve C-845. (See Fig. 186.) This determination should be made under testing conditions with the insulators connected to the transformer. (The capacity currents taken by some insulators and the oscillating discharge passing over their surface sometimes seriously affect the trans- formation ratio.) Where arc-over values only are specified, the tester must see that the testing outfit and conditions will not facilitate arc-overs. Insulators in production and not listed in Eng. Brief 10761A should be called to the attention of the Engineering Department. Any insulators listed showing serious discrepancies from the results of specified tests, without defects being apparent, should be referred to the Engineering Department before proceeding further. 358 Tests are called for by letters having the following signifi- cance: 11 A" Apply potential between central stud filling the insulator bore, and the foil band around the outside of insulator. Foil should be so located as to bring the maximum tax (stress) through that section of the insulator which is under maximum stress in service. If the outer surface is not completely glazed foil should be placed on the unglazed surface. " B " Includes ' ' Blind ' ' Insulators. Apply potential between the stud and foil around the opposite end of insulator, the foil being located to give approximately service conditions. " C" Apply potential between foil located inside and outside the insulator on the unglazed parts. "D" Apply potential between spiral springs coiled in cableways. ".4," "B," " C" and "D" tests consist of a flash-over voltage applied instantaneously and a 90 per cent flash-over voltage applied for 30 seconds. TUBES Wet process porcelain tubes must be tested at 20,000 volts per each y% in. thickness applied for 30 seconds between central stud and foil covering the outside completely except at ends where the foil is omitted to obtain the necessary striking dis- tance. 359 CHAPTER 22 TRAIN CONTROL APPARATUS Inspection and High Potential Tests Before testing any apparatus, a careful inspection must be made for any mechanical defects. Any part of apparatus that will be subjected to a difference of potential must be given a high potential test, corresponding to that specified in the Engineering Briefs. AIR BRAKE APPARATUS This includes valves, governors, strainers, cylinders, and all other parts that make up the braking system of a car or train. VALVES Air valves are manufactured under the following type letters: A, S, VL, E, and TE. The A and S are motorman's valves, different forms of which are used for straight air and emergency brake systems. The VL is a pressure reducing valve used for automatic air brake systems, and reduces the main air reservoir pressure to a lower and constant pressure. Type E includes all emergency valves. One of the most important is the Form E, used with automatic air brake systems in connection with the pilot valve located in the controller. It exhausts the train pipe whenever the pilot valve is opened, thus applying the brakes to the car or train. Magnet valves are included under the Type TE. They are used for remote control. The Form B is used for operating pantograph trolleys. Mechanical Inspection Each valve is given a careful inspection to see that all the pipe connections have good threads. In the Types A and S, the fit of the handle should not be too loose. There should be only enough clearance to allow it to be easily removed. The handle should move over the different positions with compara- tive ease and be removable only in the lap position. Air Valve Tests Every casting, which will be subjected to air pressure in service, should be tested for porosity. This is done by immersing the casting under pressure in water. Where this cannot be done, cover the casting, under air pressure, with soap suds. Water must be used in every case to determine the amount of leakage, and all castings showing a continuous leakage must be rejected. After assembly, each valve should be subjected to an air pressure and operated as near as possible at the service pressure. All parts should then be again tested for leaks by immersing 360 in water or by covering the part with soap suds, while under pressure. Valves with metal stem seats are provided with ground stems. The stem and hood are inspected before being assembled on the valve body. GOVERNORS Governors automatically keep the air pressure of the braking system within a certain range by opening and closing the com- pressor motor circuit. Operating Test Each governor is stamped with the type letters and numbers; the letters represent the style of the governor, and the numbers represent the capacity and range at which it will operate. The first number indicates the minimum opening pressure in pounds per square inch. The second number denotes the maximum opening pressure. The third denotes the variation in the opening and closing pressures. The tests are similar in all governors and consist of connecting them to a source of compressed air, the compressor motor circuit being wired through the governor tested. The governor should then be adjusted to open the circuit at the minimum opening pressure and close it as soon as the pressure is reduced by an amount equal to the given pressure range. It must then be tested for maximum opening pressure and should again close when the pressure is varied through the amount equal to the normal range. All parts under pressure should be examined for leaks. Type ME 65-100-10 Form A Governor This governor is designed for use with a large compressor, the circuit of which is made or broken by a contactor or con- tactors controlled by the governor. The test is similar to that given above, except that the main circuit of the com- pressor is broken by the contactors controlled by the governor instead of by the governor direct. STRAINERS Strainers are used in air brake systems to catch scale and small particles that would interfere with the operation of any of the apparatus. They are tested with air pressure and exam- ined for leaks. CONTROLLERS The R, K, C and T controllers comprise the principal types, All others are modifications of the above. • The R and K types make and break the main motor circuit within the controller. The Type C controller makes and breaks a circuit which operates contactors that open and close the motor circuits. With a contactor box on each car and the control circuits connected in parallel, the motor circuits for a whole train can be controlled with one controller. Type T is used with induction motors, generally being used to cut out resistance in the rotor circuit of Type M motors. 361 Inspection The development of each cylinder and its fingers should be examined to see that they check with the DS diagram. The fingers should make good contact on the segments of the cylinder and in the order shown. Controllers having several auxiliary fingers in series should be tested to see that these fingers make and break contact simultaneously. All auxiliary release knobs should open the auxiliary contact fingers when released at any position of the handle. -The main cylinder and reversing cylinder should interlock, so that the reversing handle cannot be thrown when the controller is in any but the "off" position. When the reversing handle is in the removable position, the main cylinder should be locked in the "off" position. All controllers should receive a careful inspection for mechanical defects. All cables passing through the frame of the controller should pass through an insulating bushing, except in the case of Type R controllers for mining locomotives. There should be sufficient clearance between points at different potentials and between all current-carrying parts and frame. Operating Test All controllers should be connected and operated under service conditions as nearly as possible. Those controllers which operate the main motor circuit should be connected and operated with a motor or motors with the proper resistance in circuit, to check the wiring and the blow-outs on the different fingers. Carefully note whether the arc blows in the proper direction and ruptures satisfactorily when turning the con- troller to the "off" position. When the controller is not adapted to motors used in the testing department, the complete develop- ment and wiring of the controller should be carefully checked with the DS diagram. Those built to operate contactors should be connected to the latter and operated, noting the direction the arc blows as in other controllers. When turning the con- troller to the "on" position the auxiliary finger or fingers should make contact first, and should break last when turning to the "off" position, unless otherwise stated on the Engineering Brief for that particular type or form of controller. Where a separate blow-out is used for the auxiliary fingers, it should be carefully tested. The auxiliary fingers, whether fitted with a blow-out coil or not, should break the total current of the controller in any position, when the auxiliary release knob is released. Automatic and Semi-Automatic Controllers Several types of the C controllers have their cylinders fitted with a spring and governor so that when the handle of the controller is turned to the "full on" position, the spring is wound up sufficiently to rotate the cylinder. The governor should be adjusted so that the cylinder will rotate in the specified time. The governor is fitted with a small magnet coil which 362 should lock and hold the cylinder in any position when the specified current is passed through the coil. Pilot Valves Many C controllers are fitted with pilot valves operated by the auxiliary release knob. This pilot operates a valve for an emergency operation of the brakes. They should be con- nected to an emergency valve which should trip whenever the auxiliary release knob is released. The reversing handle should interlock with the valve in the "off" position, and should prevent tripping of the emergency valve. The valve should operate quickly without leakage when closed. REVERSERS Reversers used in Type M control are operated by solenoids energized through the reversing cylinder to the controller. The segments on the rocker arm are so arranged that a move- ment from one extreme position to the other changes connections and reverses the armature or field circuits of the motors. Operating Test The operating test consists of connecting the inductive resistance specified between the first and third fingers, one side of the shop to the third finger, with the other side connected alternately to the two solenoid coils. Under these conditions the reverser should operate quickly and throw completely over, without rebounding. It should be operated on the different voltages specified. The arc formed on the control fingers must be blown outward from the fingers and should rupture immedi- ately. This should be noted. The coil resistances should be measured and should check within 10 per cent of that specified in the Engineering Briefs. Spools for Supply Shipments After the high potential test, the resistance of each spool should be measured and should check within 8 per cent either way, from that specified in the Engineering Briefs. MS SWITCHES MS switches are made up for the control of various car or train circuits, and are in most instances equipped with magnetic blowouts. Quick-break operation on some types is also employed. Each switch should be examined for mechanical defects such as broken or loose parts. The switch should work freely and should not stick or bind in any position. It should make good contact when closed. Switches designed to open the main current should be given a blow-out test, consisting of breaking a specified current in order to see that the arc is blown outward, and ruptures satisfactorily. All switches should be given a high potential test between parts of opposite polarity when a blade or blades are open. 363 CUT-OUTS Cut-outs for train control service are used to cut out the control circuits of individual cars from the rest of the train, one cut-out being placed on each car. Besides seeing that the fingers make good- contact on the contact segments, all fuses should be "rung out" to see that they are in good condition. CONNECTION BOXES Connection boxes are used as splicing junctions where the wiring of the car is run through conduit. They consist of a metal box containing connection terminals to which wires may be easily connected or disconnected. They receive a high potential test only. MU TRIPPING SWITCHES These switches have a series coil through which the motor circuit is wired, and a small control switch through which the control circuit for the line contactors is wired. The series coil operates an armature fitted with a calibrated spring similar to a circuit breaker, so that if an excess of current is taken by the motors, the armature trips out the control circuit switch, opening the contactors in the motor circuit. Examine the compound box to see that it is not cracked or broken, and that all flat headed screws are center punched other than the removable screws used in fastening the cables. The control switch should work freely and make good contact when closed. The switch should open when the lever is thrown to the "off" position. All MU switches are calibrated for various tripping points. (See Engineering Briefs.) They are sent to the Test Dept. for calibration without the cover. The armature should be held in the operating position by means of a block of fiber or other non-magnetic substance, as though it rested against the cover. Marks are made to determine the relative positions of the cap of the calibrating springs for the different currents. The switches are then returned to the shop for stamping and assembly of cover, after which they are given a blow-out test, which consists of breaking a small inductive circuit with the switch to deter- mine the direction of the blow-out. A high potential test should be made between the series coil and the control switch, also between the switch blade and upper left-hand terminal when the switch is open. CONTACTORS Contactors are used for making and breaking the motor circuits on a car. They are operated by a solenoid which actuates a lever carrying one contact tip, the other tip is stationary, and iitted with a blow-out coil which helps to break the arc between the tips. 364 There are two distinct types of contactors: DB contactors which are used for direct current work, and DBA contactors which are used for alternating current work. The DBA contactors have a laminated armature and an E- or U-shaped laminated field with copper shading coils in the face of the outside leg, to prevent humming when the contactor is closed. An arbitrary number is assigned to each contactor, and form letters are used to indicate minor mechanical differences. A numeral follows the form letter to indicate the operating coil used, viz. DB-260-A-1. Inspection Each contactor should be examined carefully for mechanical defects, such as broken arc chutes, cotter pins, loose screws or bolts. Also note whether it bears the Mechanical Inspection Department's stamp. The contact tips when closed should make good contact over their full width. The copper shunt should be free from sharp kinks or bends and should not rub on any metal part having sharp or rough edges. All contac- tors must operate freely, and must not stick or bind in any position. TYPE DB CONTACTOR Commercial Tests From the tables given in the Engineering Briefs, see that specification on the spool corresponds with the stamping on the name plate. When hung in the proper position, the contactor should pick up and wipe contact at or below the current values given for the respective spools, care being taken that the contactor wipes full contact, as sometimes the pick up current is taken to be the same as that required for the wipe contact. To avoid this error, note that the first upward movement of the plunger only brings the contact tips together. This is called the pick up. The next movement wipes the contacts over one another, and also increases the pressure between them. The amount of this movement should equal or exceed that given in the Engi- neering Brief. Measurement of Spring Pressure Insert a strip of paper or cloth between the tips, and put enough current through the operating coil to close the contactor completely. Hang a spring balance from the screw heads holding the tip on the finger, and note the pull required on the spring balance to loosen the paper between the tips. Resistance Measurement of Spools The resistance of each coil should be measured and be within 8 per cent above or below the specified resistance at 25 deg. cent. 365 TYPE DBA CONTACTOR The pick up and wipe is similar to that in the DB contactors. As each DBA contactor, however, is connected directly across the line, it is tested for the operating voltage instead of the current. The voltage should be obtained by gradually raising the field on the alternator. The magnetizing current is measured at the proper frequency, and should be taken with the armature fully closed. The finger pressure should be taken as in the DB type. See that the contactor wipes on the same voltage at which it picks up. It should do so to protect the tips from freezing (welding together) due to insufficient contact area. The operating coil would also burn out, since with a-c. contactors the current is high until the contactor is closed. After the contactor has wiped, it should be perfectly noiseless. SPECIAL TESTS The test sheet should contain the following data: Coil specification (No. of turns and size of wire). Cold resistance and temperature of coil at which the cold resistance is taken. Number of coils in series or multiple during test. Finger Pressure This test is made by holding the contact fingers at full wipe position, attaching a spring balance to the screw which holds the finger to the jaw by means of a small loop of wire. A pull is then exerted through the spring balance until the fingers separate sufficiently to allow a thin strip of paper, placed between them, to be drawn out. The pull as recorded by the spring balance is taken as the finger pressure. The pressure of each finger should be measured separately. "Minimum Pick Up" and "Wipe" A contactor is at "pick up" position, when the armature is raised so that the fingers just make contact. At "wipe" position the contactor is fully closed. On a-c. contactors, two additional tests, regulation of alter- nator, and chattering and drop-out voltage are made in connection with the minimum pick up test. Regulation of Alternator With the armature blocked open, read the speed and voltage of the alternator both with and without the contactor in circuit. Repeat with the contactor blocked shut. Chattering and Drop-Out Voltage With the contactor picked up and fully wiped, note the minimum to which the voltage can be reduced before the con- tactor becomes noisy, and also note the voltage at which the contactor opens. 366 Saturation Curve This curve is taken at different voltages reading amperes and watts, readings being made both with the contactor closed and opened, or at such air-gaps as special instructions may require. Pull Curves on D-C. Contactors This curve is taken by holding a constant current and reading the pounds pull for different air gaps. The curve is taken in either of the following ways: First: By carefully adjusting the air gap, weighting down the plunger, and holding the amperes constant while weights are subtracted from the plunger until it picks up. Second: By weighting down the plunger and holding the amperes constant, while the air gap is gradually decreased until the plunger picks up. The air gap is then measured. A variation of this curve is sometimes made by holding a con- stant air gap and varying the amperes and weights. In connec- tion with the data for these curves, the length, diameter and weight on plunger should be given; the length of plunger being taken as the length from the butt end to the center of the hole in the lower end. The weight given in the table should be exclusive of the plunger and should be so stated on the Test Sheet. Pull Curves on A-C. Contactors The method of taking a pull curve on an a-c. contactor is more complex than on a d-c. contactor. In either case the pounds pull is dependent upon the ampere turns. In a d-c. contactor, however, the amperes at any voltage varies directly with the resistance of the coil and is independent of the plunger air gap, whereas in an a-c. contactor the amperes at any voltage does not vary with the resistance, but with the impedance. The reactance varies with the armature air gap. For this reason it is not desirable to hold the amperes constant. If, however, the voltage is held constant, an error will be caused due to the resistance of the coil being increased by heating. In tests where great accuracy is required, this error can be eliminated and all contactors can be compared upon a common basis by the following method: First: Measure the resistance of the coil cold. Second: Holding the voltage constant at that value at which the pull curve is desired, take an ampere air gap curve; i.e., read amperes at various air gaps. This curve should be taken as rapidly as possible to avoid undue heating of the coil. Third: Take a check reading of the resistance to see if the coil has been much heated. If the heating is slight, an average of the two readings should be taken as the resistance of the coil. Fourth: The ampere air gap curve thus obtained should be corrected for a temperature of 25 deg. cent, and replotted. 367 Fifth: Take a pull curve as given by the first method for d-c. contactors, holding the amperes constant corresponding to the different air gaps as obtained from the corrected ampere- air gap curve. In cases where the cold temperature of the coil happens to be within a few degrees of 25 deg. cent, the pull curve can be taken directly, holding the voltage at the value at which the curve is desired. Great care should be taken to prevent undue heating of the coil. The current must be on only for a sufficient time to obtain readings. At the completion of the test take another check reading of the resistance to determine the heating. Work Curve This curve is taken by measuring the pounds pull necessary to lift the plunger or armature at different air gaps, having the complete operating mechanism of the contactor and spring adjusted to give the finger pressure required. Speed Curve Speed curves are taken on contactors and relays to deter- mine the time a contactor takes to close or to open. For taking this curve, a special mechanism has been made which operates as follows: The contactor is set on a special stand and a mechanism is then fitted to the plunger of the contactor so that a pencil attachment operates along a vertical line. The pencil bears upon a sheet of sensitive paper which is secured to a cylindrical drum, revolving about a vertical axis. The drum is rotated by a small shunt motor operating at constant speed. Upon the periphery of the drum, contact fingers are fastened, which make and break the circuit through the contactor coil. The contactor is then operated through a number of cycles, and the mean curve is drawn. In this test the required voltage must be held across the coil without resist- ance in series, on account of the inductance of the circuit. Heat Runs This test is very similar to the heat runs made on other apparatus and consists in measuring the temperature of the coil or other part at frequent intervals, both by thermometer and resistance. It should be noted that, as the operating coils are well wrapped with twine or other binding, thermometers placed on the outside of the coils do not give a fair indication of the temperature of the interior of the coil. For this reason the temperature must be calculated from the rise of resistance. To get these readings as accurate as possible, care should be taken in measuring the cold resistance. All heat runs on coils should be made with coils assembled in the contactor frame, unless otherwise specified. All heat runs should be made holding the voltage constant. Life Tests Life tests on contactors are made generally to determine the effect of service on the wearing qualities of the various parts. 368 Before starting the test, the diameter of the hinge pins and hinge pin bearings, the maximum air gap, finger pressure, and all other parts of the contactor that will be affected by service, should be carefully measured. During the test a daily record should be kept of the number of operations, and of the operating failures of any of the parts. At the completion of the test, the parts measured at the beginning must be again measured to determine the amount of wear. FUSE BOXES Commercial Tests Fuse boxes are made of fiber or compound, and are fitted with terminal blocks, in which ribbon fuses may be readily placed. The principal test is high potential, for the value of which see Engineering Briefs. Fuse Boxes with Magnetic Blowout After the high potential test, a small fuse is placed across the terminal of these boxes. A current is then passed of suffi- cient capacity, and at sufficient voltage, to blow the fuse immed- iately. This is done to determine the direction of the blow- out. FUSES The test sheet should contain the catalogue number, ampere rating and dimensions of the fuse, also the style of box or holder in which the tests were made. Before starting the test, carefully inspect the fuses for defects, such as sharp bends, dents, burred holes, etc., discarding those that are not perfect, unless the test is being made to get an average curve on fuses from stock. Test to Determine Rating Connect a switch to the fuse box or holder, using a short- circuiting switch in multiple with both. If run off the shop circuit connect a water box in series. If run from the "booster," the current can be controlled from the booster field with a low resistance grid in series with the booster armature. With the series switch open, and the short-circuiting switch closed, adjust the current to the desired value, and hold as near constant as possible. Then close the series switch quickly and open the short-circuiting switch, and note the time by a stop watch it takes before the fuse blows. Fuses are rated at one- half the current at which they blow in thirty seconds. When a number of fuses are blown, the holder is likely to get very hot unless care is taken to cool it between tests. Ther- mometers should generally be placed on the fuse holder and the temperature kept below 75 deg. cent. Time-Current Curve To obtain time-current curves, fuses should be blown at current values which will blow the ribbons at periods varying from ten seconds to three minutes. 369 COUPLERS In train-control work, couplers are used to make temporary connections for the bus line, and control circuits between the cars of a train. Two parts are included in the complete coupling; the socket coupler, Type DA, and plug coupler, Type DC, which fits into the socket coupler. The contact terminals should be well fastened in the com- pound base, and the cover on the DA coupler should be held firmly closed by the spring. Couplers without cables are simply given a high-potential test, from the frame to each terminal, and between each terminal and the adjacent terminal. Sockets are placed at the ends of the car and cables run from them to the connection boxes in the car. When the socket is assembled with a cable, it is given the usual high potential test, and then each terminal is rung out with a lamp circuit to see that it is connected to the proper cable wire. CONTACTOR BOXES In the Type M or C control, instead of breaking the motor circuits in the controller, as is done in the K control, the con- troller operates a set of contactors assembled in a contactor box, which open and close the motor circuits. One contactor box is placed on each car, and the control circuits, besides being brought to the controllers of the car, are taken to couplers at either end of the car, from whence they can be connected by jumpers to other cars, and operated in multiple with them. The whole train is thus controlled from one controller. This control is manufactured either automatic or non-automatic. In non-automatic equipments, the motorman has full control of the acceleration of the car. In the automatic equip- ments, however, he does not control the resistance (accelera- tion) points. The automatic feature can readily be connected. One end of the cable is left open which can be afterwards con- nected to the connection boxes. The different wires are desig- nated by various colors. For the colors and numbers correspond- ing see the DS diagram. Inspection Each interlock should be carefully inspected to see that the rod is properly stamped, and that the disks agree with the Engineering Brief in regard to wipe and break. The terminal board and the terminals on all wires should be clearly and properly stamped and all wiring neatly done. The interlock rods should clear the back frame of the box by at least Y /i in. The name plate on each contactor and on the contactor box itself should be checked. Operation Test Each contactor box is connected to a controller and reverser, and operated so as to test all the control circuits. The main or motor circuits are rung out according to the DS diagram. 370 The operating voltage for each set of equipments should be obtained from Engineering instructions. The contactors should pick up and fully wipe on the minimum voltage, in the order specified. See that the arc is promptly ruptured on the inter- locks having magnetic blowouts. Potential Relay All automatic equipments having a potential relay should operate at a voltage higher than that at which the relay picks up. JUMPERS A jumper consists of two coupler plugs connected by a cable. It completes the circuits between cars. After the high-potential test, jumpers are "rung out" to see that the correct connections exist between the plugs as called for on the Engineering Notice. CIRCUIT BREAKERS There are several types of railway circuit breakers, the DB and MR representing the present standard. Most of the forms are fitted with a brush contact, auxiliary to the breaking finger contact, the latter being protected from the arc when opening by the contact fingers, which always open last. The AIR circuit breaker is closed manually by throwing the handle to the "on" position and can be tripped by throwing the handle to the "off" position, which gives a quick break open- ing. It is also arranged to trip out automatically on overloads. The DB circuit breakers are used for Type M control and are provided with solenoids for opening and closing. The coils are energized through a switch in the motorman's cab, the breakers themselves usually being under the car. Inspection All the cable terminal thimbles should be well fastened in the terminal blocks to prevent being lost in transportation. The arcing or secondary fingers should remain in contact when open- ing the circuit breaker, after the brush has opened contact by at least \i in. Both brushes and secondary fingers should make contact over their full width. All auxiliary switches on the cir- cuit breaker should be examined to see that they make good contact at the proper time. The copper shunts should be free from kinks or sharp bends. Calibration Each circuit breaker is calibrated for three tripping points. It is first tested for low tripping point, then for high point and finally for the intermediate point. It is left at the latter point, and the check nut is then set. Marks must be made designating the relative position of the cap of the calibrating spring for the different currents. Blow-Out Test Each circuit breaker is given a blow-out test in order to determine the direction of the arc. 371 RELAYS Railway relays can generally be classed under three heads: Current, potential and accelerating relays. Current Relays Current relays comprise all those which have their tripping coil in series with the circuit in which the current is to be con- trolled; the controlling circuits being wired through its disks or relays. Potential Relays Potential relays comprise all those having their operating coil shunt connected. These relays are used where a certain value of voltage is required for proper operation. Their func- tion is either to cut out resistance in control circuits, thus per- mitting lower voltage operation, or to transfer, or change control circuits. Accelerating Relays Accelerating relays are used with automatic control, their function being automatically to advance control connections. OPERATING TEST The relay should be able to break the specified amount of current on the contact studs, and if provided with a blow-out the arc should blow in the proper direction. The operating coil should operate the relay under the con- ditions specified in the Engineering instructions. The disks or arms should make good contact on the studs, and the wiring should be arranged in workmanlike fashion to prevent electrical or mechanical breakdowns in operation. 372 CHAPTER 23 PROJECTORS Projectors are designed for operation from direct current circuits and it is necessary to provide motor-generator sets or mercury arc rectifiers where only alternating current supply is available. Fig. 162 HAND CONTROL PROJECTOR The standard line of rheostats is designed with adjustments for line volts varying between 110 and 125 volts. When pro- jectors are operated in series or when one projector is operated from a line of greater than 125 volts potential, it is necessary to provide automatic cutouts with resistances equal to the resistance of the arc under normal conditions and rheostat capacity suffi- cient to take up the difference between the sum of the arc volt- ages and the line voltage. Inspection All projectors are inspected before the final test to see that the drum is balanced, that no bolts, screws, nuts, or cotter pins are missing, and that the rating on the name plate is correct. 373 Types of Control Hand — The hand control projector shown in Fig. 162 is controlled by handles on the rear of the drum and is provided with clamping devices for the horizontal and vertical planes. Fig. 163 PILOT HOUSE CONTROL PROJECTOR Pilot House — The pilot house control shown in Fig. 163 is operated from the inside of the pilot house by a controlling gear extending through the roof, the movement in both the hori- zontal and vertical planes being controlled by one handle. Rope Control — The rope control projector shown in Fig. 164 is operated by means of cables connected to the controlling gear of the projector. As the movements in both the hori- 374 zontal and vertical planes are controlled by a single handle the controlling gear may be placed in the pilot house, on the bridge, or at any other convenient place. Electric Control — -The electric control is of three types. First, the direct armature control in which the entire current for the motors is carried through the controller cable, the con- tacts in the controller being arranged to start, stop and reverse both the elevating and training motors, and so connected that the beam follows the movement of the controller handle. This control is employed in the 13 and 18 inch sizes. Fig. 164 ROPE CONTROL PROJECTOR Second, the rheostatic control in which the training and elevating motors are controlled from a distance through the con- troller cable, the controller being provided with resistances which give one or more speeds of training and elevating motors. Third, the synchronous control in which only the current required by the pilot motors is carried through the controller cable, the controller operating the pilot motors which in turn control the elevating and training motors. Adjustment A great deal of testing and adjusting of the electric control is done during the construction of the operating mechanism. For the synchronous control projectors, the pilot motors are connected and tested for polarity in accordance with Fig. 165, after which they are returned to the assembler for final connec- tion. The motor is then wired to a controller and if connected correctly the rotating field will take up 12 equidistant positions per revolution. After this test the pilot and training motors are assembled and wired, and thoroughly tested to insure the wiring being correct. When the projector is assembled the electric control is operated for some time to make sure that 375 III* III! v> i 1 1 + + + |,|,|,| + l + Uj «* i + + + 1 i iki4-'+!r!u ^r ¥ ■t- 1 1 1 +1 + + jJ !, j_!tj '■5 1 *© *> V) ^'<0 «>| ^ % ^j");(0!(oi^. : ^^! Mj«rt!% * % <0 jN|«fO»}§;5s]^i 9 <*5 B <: « * ^ Hill 0#€) 376 the connections are correct and that there are no mechanical faults in the training and elevating mechanism. Lamps are wired, adjusted and operated at the proper current and arc voltage, care being taken that the gap at the circuit breaker in the feeding magnet circuit is of the proper length, also that the screws limiting the motion of the pawls are properly set after which the feeding magnet armature spring may be adjusted so that the lamp will operate at its rated arc voltage. At the end of this test the lock nuts should be tightened and a general inspection of the mechanism made to see that everything is properly secured. With the lamp in position in the projector and in operation the position of the lamp should be adjusted by means of the Fig. 166 MEASUREMENT OF FOCAL DISTANCE focusing screw so that the beam will appear to be composed of parallel rays. Mirrors Referring to Fig. 166, the mirror A is held facing an object B approximately 100 feet from the mirror and a piece of ground glass or white card C is then moved backward and forward in the focus. When the focus is reached the image of the object is very distinct. The distance from the card to the center of the reflecting surface of the mirror is the focal length. Mirrors are tested for regularity of curvature and grinding by placing them in front of a large white screen on which horizontal black lines are drawn. The lens of the camera is placed back of the screen and through a hole in the center and the reflection of the right lines is photographed. Fig. 167 shows a mirror in which the curvature of the reflecting surface and the grinding is correct. Fig. 168 shows a mirror with irregularities in the reflecting sur- face which can be distinctly seen in the photographic test. Rheostats A rheostat or ballast is connected in series with the arc when it is operated from a constant potential circuit. The object of this resistance is to prevent fluctuations of the arc current. 377 Fig. 167 SHOWING CORRECT CURVATURE OF MIRROR 378 Fig. 168 SHOWING IRREGULARITIES IN CURVATURE 379 Carbons One per cent of all projector carbons are tested. The points to be observed are as follows: The kind of arc obtained, whether quiet or noisy, steady or wandering; the amount of refuse left in the lamp after the car- bons have been consumed, and the amount which the carbons burn out of focus. The table on page 381 gives the sizes of carbons, etc., for standard apparatus. SIGNAL APPARATUS Keyboards Keyboards must be wired and every combination tried, care being taken to see that the proper lamps light and that the con- tact switch makes contact so that the lamps light simultaneously. An insulation test is made at 500 volts. The cables are connected to the keyboard and every combination gone through to see that the connections are correct. The connections to the receptacles should be inspected to see that there are no loose ends of wire to short-circuit or ground the receptacle. Trucklight Controllers Trucklight controllers are wired and tested to see that the proper lamps light and that the pulsator works correctly. Diving Lamps Diving lamps are tested under water, as specified in the Government specifications for the apparatus, to see that leakage does not occur. 380 CO o O Oh Q < I> b- > >^ >^ >,>,>, >> J5 ,0,0.0,0,0.0,0 t/> «-[^--\irf\w\t\ eo\ Z i— < i— « o pq a o 0) (I- 1 b£ M GuO tX Vh 5-i »- J_ »- ^i I-, H o o o— '— • — — ' 35 'x PL, \N \p» iCOOOMNIN «3 i— i i—i i—i i—i >>>>>>>>:>,>>>> .O .0,0.0,0 .0.0 sssss ^ *-> — ' ^ getY//7c//hg ~Y Fig. 170 tf/g/? /o/iogetV/htf/rtg-y ft/ghl/o/iogeiY/hrf/ng-De/to ^owYo/iegeW/hd/ng - De/£a Fig. 171 ///gfrYo/togeW/ncting-Y Fig. 172 Mg/tto/togeW/hafog -0e/6o r 1 \ r ton>yc>/tage}Y/>7c///}g-£>/a/}7eir/c0/ towfo/tage Mhdfog -P/'a/netr/ca/ Fig. 173 Fig. 174 Figs. 169 to 174 STANDARD THREE-PHASE CONNECTIONS, THREE- PHASE SHELL TYPE TRANSFORMER Notes. — In effect, high voltage and low voltage windings are wound in opposite directions. Diagrams should be read facing low voltage side of transformer. voltage, place the voltmeter across X to Y so as to obtain a positive deflection; then move the voltmeter lead on X high voltage over to X low voltage and the one on Y high voltage to Y low voltage. Break the circuit and note the deflection of the voltmeter. If it is positive the polarity is correct. The other two phases must then be checked in the same way. In checking F-diametrical connections (Figs. 173 and 179) excite X to Y for checking phase 1 ; also for phase 2. For phase 388 w . : ahYo/tage lYthcf/'ng^ -0e/£a ten /a/tags -W/nct/rta -&&''£ Yo/tage W/hct/fyg-De/ia i.oiY Yo/£age 'YY/ha'/ng -Y U\M Fig. 178 rt/gfifo/ioge Mh&hg - Y \z \y \X £on> Yo/iage PY/haf/rig •£>/c7/7?etr/ca/ \1 J U Fig. 179 Kg* Yo/dogsW*?<7'>?g -Je/6a. £okv VoltogeMhc//'na-Dio/ne6ri5ol X'\ \X Y -■ Z*xH 1! H i Fig. 180 Figs. 175 to 180 STANDARD THREE-PHASE CONNECTIONS, THREE- PHASE CORE TYPE TRANSFORMERS Notes. — High voltage and low voltage winding wound in opposite direc- Xumbers 1, 2, 3 on diagrams refer to corresponding phases. Fig. 177a is for transformers having high voltage winding 5300 volts or less. Fig. 177b is for transformers having high voltage winding over 5300 volts. 389 1 transfer the lead from X high voltage to X low voltage and from Y high voltage to X' low voltage. For phase 2 transfer from Y high voltage to Y low voltage and from X high voltage to Y' low voltage. For phase 3 excite Z to X, then transfer from Z high voltage to Z low voltage and from X high voltage to Z' low voltage. In shell type delta-diametrical (Fig. 174), proceed as follows: For the left-hand phase excite X to Y high voltage and transfer from Y high voltage to X low voltage, and from X high voltage to X' low voltage. For the middle phase excite X to Z and transfer from X high voltage to Y low voltage and from Z high voltage to Y' low voltage. For right-hand phase excite Y to Z, transfer from Z high voltage to Z low voltage and from Y to Z' low voltage. For core type delta-diametrical (Fig. 180) proceed as follows: For phase 1, excite X to Z, transferring X high voltage to X low voltage and from Z high voltage to X' low voltage. For phase 2 excite X to Y, transfer from Y high voltage to Y low voltage and from X to Y' low voltage. For phase 3 excite Z to Y, transferring from Z high voltage to Z low voltage and from Y high voltage to Z' low voltage. Phase Rotation In addition to the polarity test it is necessary to check the phase rotation on all three-phase and six-phase transformers except on such as are run in parallel with one on which the test has already been made. The phase rotation meter should be connected to the high voltage side of the transformer and a relatively small voltage applied. This voltage should be sufficient to cause rotation of the meter but should not exceed 550 volts. The direction of rotation should be noted. Then the leads from the meter should be transferred straight across the transformer to the low voltage terminals. The transformer should again be excited with voltage sufficient to cause the meter to rotate end the direction of rota- tion should be noted. When the direction is the same on the low voltage as on the high voltage side, the result should be marked on the test sheet as "Standard." When it is opposite on the two sides, attention should be called to that fact on the test sheet. Six-phase transformers having double delta connections must have the rotation checked on each delta. Transformers having diametrical connection with the middle points of each phase brought out should have these points joined after which phase rotation should be checked by selecting ter- minals which will give two Y-connections. In addition to the test with the meter these transformers should have the neutrals connected together while the six voltages are read between each pair of consecutively numbered leads. These should all be of equal value and also should be equal to the voltage from any one of them to the neutral point. When the neutral points are not brought out a temporary delta connection should be made for the phase rotation test. 390 Ratio The ratio of a transformer is the ratio of voltage of the high voltage winding to the low voltage winding. The required voltages are given in the rating and are shown on the DS sketch. The ratio should be measured on at least one of each group of similar transformers and compared with the ratio shown by the DS sketch. The ratio of all other transformers in the group should be checked by running each in parallel with the one on which the ratio has been measured. The transformer should be operated at normal frequency or higher and at normal voltage or lower during the ratio test. An exception to this rule is made for transformers having capacities of 500 watts or less and with exciting current of more than 10 per cent. These should be tested at normal voltage and fre- quency. Where possible, it is best to make a ratio test by comparing the transformer with a standard of exactly the same ratio. The two should be connected in parallel on both sides and the high voltage winding excited while a voltmeter is used to read the difference in voltage between the two low voltage windings. When the above method is not applicable, two voltmeters should be used, one to read the low and the other to read the high voltage, the latter being stepped down through a potential transformer when necessary. Where voltages and scales will permit, the instruments should be interchanged between read- ings so as to eliminate errors. It is best to take at least two sets of readings, calculating the ratio from each and considering the average as the correct value. The parallel run should be made at normal frequency and normal voltage, the voltage being applied usually to the low voltage winding. A test for circulating current between the two high voltage windings should be made by closing and opening the circuit. If a spark is observed a further test should be made by measuring the amperes circulating through the high tension winding and by measuring the difference in voltage on open circuit. If no spark appears on the first test, it is best to make sure of the presence of voltage in the winding by touching the free high voltage terminal to the case (at reduced voltage). If the circulating current is more than 5 per cent of the rated current of the winding, attention should be called to the fact on the test sheet. On three-phase transformers it is preferable to use single- phase power and to measure the ratio of each phase separately. This is not possible when the neutral point of a Y-connection is not brought out. In such cases three-phase power must be used. On Y- diametrical transformers where the neutral point is not brought out, three-phase excitation must be used. Any inequality in the magnetizing characteristics of the three phases will result in distortion of the neutral, thereby causing unequal phase voltages. When such an inequality is found the diametric connection should be changed to a Y-connection and the phase voltages measured. If these are equal and of the proper value, 391 i.e., V3 times the diametric voltage, the ratio may be con- sidered as being correct. If the voltages are still unbalanced, however, the transformer should be returned to the Assembly Department so that the neutral point can be brought out. It should then be tested single-phase and if -the phase ratios are correct the transformer may be passed. The Y-connection may be made from the diametrical by referring to the standard connection diagrams previously referred to under polarity test. A variation of more than Y% of 1 per cent above or below the value shown on the DS sketch or connection label on stand- ard lighting transformers should be called to the attention of the Engineering Department. On other transformers the allowable variation is 1 per cent. Wattmeter Ammeter Primary Secondary Fig. 181 CONNECTIONS FOR IMPEDANCE TEST Checking Taps Nearly all transformers are provided with taps in one or both windings, so that a slight change in ratio or a low voltage for starting may be obtained. These tap voltages should be checked to determine whether they agree in voltage and in position with the DS sketch. This test may be made either by means of the "two voltmeter method" or by running the transformer in parallel with a standard transformer or with one on which the test has already been made. When two voltmeters are used, it is best to apply a low voltage to the full winding, then read the voltage from the terminals to the first tap, then between succes- sive taps of the same winding. Care should be taken in handling the voltmeter connected to the tap, because, although the voltage reading is low, the circuit to which it is connected may be several thousand volts above ground. If the opposite end of the circuit be grounded a severe shock may be obtained from the meter. On windings having low voltage taps at the ends it is some- times necessary to check their location by checking the polarity of each section of the winding. If the polarity of each is correct the taps are properly brought out. 392 Impedance The impedance of a transformer is measured by short- circuiting one of the windings and impressing an alternating e.m.f. on the other windings and taking simultaneous readings of amperes, volts, watts, and frequency. The impedance of transformers should be carefully measured for the following reasons: Transformers operating in multiple divide the load inversely as their impedance voltages; i.e., the one having the higher impedance will take the smaller part of the load and vice versa. When transformers of different types are operated in multiple, the impedance of one transformer must sometimes be increased by putting a reactive coil in the secondary circuit, and adjusting until the desired impedance is obtained. Impedance tests show whether a given arrangement of coils is satisfactory or not. If the arrangement is not satis- factory, excessive magnetic leakage will take place and high impedance voltage result. The impedance watts will also be high, due to excessive eddy current loss in the copper. Since regulation depends upon impedance to a great extent, a low impedance is very necessary for close regulation. The impedance voltage of lighting transformers varies from about 1 to 4 per cent while that of power transformers is usually from about 4 to 8 per cent. Transformers for operating syn- chronous converters are often provided with magnetic shunts in order to obtain high impedance, that is from 12 to 20 per cent. The impedance watts do not as a rule exceed 1 to 1 Y2 per cent of the total capacity of the transformer, although they are higher than the calculated I 2 R on account of the eddy current losses in the copper. The following method should be used in making the test: Place a thermometer on or very near the coil so as to obtain the exact temperature. Make a good short-circuit on one winding, using as short a cable as possible and one of ample cross section so that no appreciable losses will occur. Make the connections shown in Fig. 181. Adjust the current with the pressure circuits of the voltmeter and wattmeter open, then close the pressure circuits and take the reading of volts and watts. See Fig. 181. The watts should be corrected for the losses in the voltmeter, wattmeter and instrument transformers (if any are used). In measuring the impedance of three-phase transformers, the two wattmeter method should be used, a single set of instru- ments being transferred from one phase to the other by switches. The current should be adjusted so that the average value in the three lines is equal to the normal rated current. If the measured impedance watts exceed the calculated PR watts by more than 15 per cent, attention should be called to that fact on the test sheet. Core Loss and Exciting Current When the transformer is connected to a source of alternating e.m.f. a loss of energy takes place in the iron due to the cyclic reversals of the magnetic flux. This loss of energy is known as 393 core loss. Its value depends on the wave form of the impressed voltage as well as upon the value of that voltage. A peaked wave gives lower losses and a flat wave gives higher losses than a true sine wave. The core loss energy should therefore pref- erably be taken from a sine wave alternator operated at about its normal excitation. The core loss test is similar to the impedance test except that the voltage is applied to one winding, all others being open- circuited. It is usually preferable to apply voltage to the low voltage winding so as to avoid reading meters in high potential circuits. Care should be taken to see that the high tension cables are located so that no one can come in contact with them r^AAAAAAA/VW Pn Normal Secondary Vo/tage. ^AMA/WWS^ SMAAAMMH Fig. 182 CONNECTIONS FOR HEAT RUN and so that there is no danger of a short-circuit. During the test it is best to have the windings connected according to some one of the connections shown on the DS sketch. It is par- ticularly necessary to avoid leaving windings open at points where they would not be left open under operating conditions as it is sometimes possible to obtain excessive stresses between points of the same winding by leaving such connections open. The connection of instruments in measuring core loss should be the same as in the impedance test and the reading should be taken in the same way. In measuring the loss of three-phase transformers it is advisable to take three entirely separate sets of readings by the two wattmeter method, each of the three lines being used in succession as the neutral. The average value of the three sets of readings should be recorded as the true core loss. As alternators with perfect sine waves are very difficult to obtain, it is customary to correct the measured loss to a sine wave basis, by means of the core loss correction outfit. This outfit consists of a single winding on a small core, the sine wave loss of which has been carefully determined over a wide range of voltage. The outfit should be connected to the same source of power as the transformer under test, after which normal voltage should be applied to the latter. The loss in the standard core and the voltage across its terminals should be measured at the 394 same time as that of the transformer under test. The sine wave loss of the standard core at the same voltage should then be determined from the calibration curve. The ratio of the measured loss of the standard core to the reading taken from the calibration curve should be used to reduce the measured loss of the transformer under test to a sine wave basis. The exciting current may be corrected for wave shape by- carrying the test a little further. After the core loss correction has been determined, the voltage should be raised until the measured loss is equal to the corrected loss. The exciting cur- rent read at this voltage is approximately the true sine wave value. To Alternator Supplying Copper Losses wv*avvvvwiwwwivvw-^ To Tnree phase Alternator Supplying Core Loss Pr/mary Fig. 183 CONNECTIONS FOR HEAT RUN Heat Run The heat test may be conducted in several ways, all of which are intended to approximate as nearly as possible the actual operating conditions. The run with actual load may be made by using lamps, water rheostats or choke coils, but as this is very expensive except for small devices, some form of motor- generator method is usually employed. Fig. 182 shows the connections for testing two transformers by the motor-generator method. The secondaries of the two are connected in multiple and are then connected to an alter- nator which supplies the core loss and exciting current. The primaries are connected in series and opposing each other. If the transformers have the same ratio, the voltage from A to B will be zero. The secondary of an auxiliary transformer D is connected in series with the primaries and an alternator E is used to 395 supply the copper losses through this transformer D. The same method may be used for any even number of transformers, but it is not advisable to connect more than two high voltage units in this way, or more than six or eight units of any volt- age. The arrows show the direction of the load currents. Fig. 183 shows the connections for a heat run on three single- phase transformers. This method may also be used for one three-phase transformer when the windings can be connected in delta on each side. The three-phase alternator is used to Primary WWW\r^/VWV\r-> UvWV- 1 Secondary ^M^^^^^M^ WWW\r-^/WwJ S/WWV-J rWVWS Primary Secondary UT "LvvyvJ L^/d Lv\/\/\J A' A" , x^^a l^^t n/WW-nMAr-WWVn To Three-phase Alternator 8 To Three phase AILernatorA Fig. 184 CONNECTIONS FOR HEAT RUN, THREE-PHASE supply the core loss and exciting current. One of the deltas is opened and sufficient single-phase voltage is impressed to cause full load current to flow. The current circulates within the deltas and is entirely independent of the three-phase voltage impressed by the core loss alternator. Fig. 184 shows the connections for a heat run on two three- phase transformers in which three-phase current is used to supply the copper losses and three-phase voltage for the core loss. The auxiliary transformers A, A', A" may or may not be used depending on whether the voltage of the alternator B supplying the core loss is of the proper value or not. Auxiliary 396 transformers, B, B' and B" are used as series transformers to supply the impedance voltage. Fig. 185 shows connections for the heat run on two inter- changeable single-phase units designed for operation on "T" connected two-phase-three-phase circuits. It is the common practice to make such units interchangeable, each having the 50 per cent and 86.6 per cent taps so that either may be used as the main or the teaser. In actual operation the one used as the main has a somewhat heavier load than the teaser. How- ever, since either may be used as a main, the heat run should be made with the heavier load. The connections shown in Fig. 182 should not be used as with such a connection and with normal current in the winding for use on the two-phase circuit, the cur- rent in the three-phase side will be only 86.6 per cent of that --jgAVWvWMVWVVv 3 jYo/-/no/ Ko/toge. ¥¥ShamgL isyVW^WvHVWWvVV^ o Fig. 185 CONNECTIONS FOR HEAT RUN ON SINGLE-PHASE UNITS FOR OPERATION ON T-CONNECTED TWO-PHASE- THREE-PHASE CIRCUITS flowing under operating conditions. It is necessary to use con- nections shown in Fig. 185. The core loss is supplied in the regular manner and the normal current of the two-phase winding is supplied from alternator E through transformer D. An additional current is supplied from alternator / through trans- former H to the middle points F and G of the two three-phase windings. Since F and G are the middle points, no voltage is induced between them by the core loss alternator, and further- more, the current supplied by alternator / flowing in opposite directions in the two halves has no resultant effect upon the two-phase windings. The current from alternator J must be of such value as to produce a resultant current in the three- phase winding 15.5 per cent greater than that produced by alternator E alone. The frequency of alternator / must be different from that of alternator E so that the effect of the two currents in the three-phase winding will be equivalent to that obtained by adding them in quadrature. The methods described above are the ones most commonly used, but it is often necessary to modify them so as to fit special conditions. It will be noted that no provision has been made for making a heat run on a single transformer, except for such three-phase 397 units as can be connected delta on each side. As a rule such units cannot be given a normal load run without the use of actual load. However, there are other methods which may be used in special cases. Sometimes, it is possible to use a set consisting of two alternators on the same shaft, the transformer being connected between the two and the load current being adjusted by varying the alternator fields. Another method is applicable in case each winding is divided into two equal parts. The run may then be made by paralleling each winding separately and supplying core loss to one side and forcing the load current through each winding separately. In addition to the above, there are some compromise runs which approximate the load condition. One method of making a compromise run is by supplying double the normal core loss over a short period and then supplying double copper loss for an equal length of time, this cycle of operation being repeated until constant temperature conditions are reached. In connecting the transformers under test for the heat run, it is best to use the series connection of each winding, as this connection is preferable for resistance measurements. Care should be taken to see that the alternators and auxiliary trans- formers are of sufficient capacity to carry the normal load and the overload. In calculating the current necessary to supply the core losses, take the sum of the exciting currents of the trans- formers. To calculate the voltage required to supply the load current add together the impedance voltages of the transformers. Shop transformers should always be interposed between the loading alternator and the transformers under test, so as to avoid having high potentials on the switchboard and prevent breaking down the insulation of the alternator. Thermometers should be placed on air blast transformers, so as to obtain the temperatures of the air at intake of blower, air from primary coils, air from secondary coils, air from core at top and bottom and temperature of core at top and bot- tom. In placing thermometers on three-phase units, each phase should have as many thermometers as are ordinarily used on a single-phase transformer. On water cooled transformers, the temperature of the ingoing water, outgoing water, top oil, top of tank near oil level and bottom of tank should be determined. On self cooled oil immersed units, the temperature of top oil, top of tank near oil level and bottom of tank should be deter- mined. It is best to avoid changing the position of thermometers when taking readings. At the end of the run, especially in the case of air blast transformers, the thermometers on the core and coils should be carefully watched until the temperatures begin to fall. The maximum values should be recorded. When three or more transformers are available for the heat run, it is advisable to use one of them as a base for determining temperature rise. The resistance and temperature of this transformer should be carefully measured in comparison with that of the other units before the heat run is started. During the run, it should be screened from the heat given out by the 398 other units but should be subjected to the same cooling medium. That is, if it is an air blast unit, air should be forced through it; if a water cooled unit, water should be forced through its cooling coil; and if a self cooled type, it should be subjected to the same surrounding air conditions as the ones on the heat test. During the run, its temperature should be noted at the same time as that of the hot units, these values being used as base or reference temperatures. At the end of the run, the resistance of the hot and the "idle" units should be measured. The temperature rise is calculated from these final readings, a correction being made for any difference in the two initial resistances by multiplying the final resistance of the idle unit by the ratio of the initial resistance of the loaded unit to the idle unit. If an "idle" unit is not available, the reference temperatures should be as follows: On air blast transformers it should be the ingoing air; on water cooled units, the ingoing water temperature should' be used, and on self cooled transformers, the surrounding air temperature should be considered as the base. It is customary to overload self cooled transformers at the start of the heat run, so as to bring them up to operating tem- perature quickly. Air blast transformers are usually brought up to temperature on normal load, but without the use of the cooling agent. Water cooled units may be brought up on normal load, or slight overload without having water passing through the coils. As soon as approximately normal operating temperatures have been reached, the load is reduced to normal and the water started on the water cooled units or the air on the air blast. On water cooled transformers, the temperature of ingoing water should be adjusted to be approximately the same value as the room temperature at the start of the run. This value, when once decided upon should, however, be held throughout the run. The quantity of water should be adjusted so as to give a rise of exactly 10 deg. cent, in passing through the transformers. On air blast transformers, the air should be adjusted to the required pressure and both dampers should be left wide open. The quantity of air should be measured at the start of the run, and the quantity of water each hour during the run. The heat run should be continued until the rise of temperature is constant within one degree in three hours, this rise being deter- mined by means of thermometers. The load should then . be removed and resistances of hot and "idle" units measured. If the results do not seem to be consistent, the load should be replaced and the run continued until rises are again constant, after which a second set of resistance readings should be taken. The rise by resistance is calculated as follows: R h-Ro 0.0042 Ro where Rh =h.ot resistance. Ro = resistance at 0° cent. «, /#=hot temperature of winding. 399 The following variation of the formula is found to be service- able for slide rule calculations: Rh 238 +tH Rc~238+tc where Re = the cold resistance of the winding.. tc = temperature corresponding to this cold resistance. During the heat run the temperature of the hottest part of a transformer should not be allowed to exceed 100 deg. cent, unless specific instructions to the contrary have been received from the Engineering Department. Where terminals carrying more than 1000 amperes are used, the temperature of each should be measured at the end of the heat run. High Potential The application of a high potential to the insulation of a transformer is the only method of determining whether the dielectric strength is sufficient for continuous operation. Me- chanical examination amounts to little and measurement of insu- lation resistance is equally valueless, since insulation may show high resistance when measured by voltmeter with low voltage, but offer comparatively little resistance to the passage of high tension current. The voltage of the insulation test depends upon the voltage for which the windings are designed, and upon the conditions under which the transformer is to operate. This voltage is always specified on the Standing Instructions or test data card. As a general rule, the voltage is double the operating voltage of the winding with a minimum test voltage of 10,000 for the high voltage and 4000 for the low voltage wind- ing. The duration of the tests is always one minute, unless otherwise specified. In testing from the high voltage winding to core or to low voltage winding, the low voltage winding should always be grounded to the core for the following reasons: In testing between one winding and the core, a potential stress is induced between the core and the other winding, which may be much greater than the stress to which the insulation is subjected under normal operation and greater, therefore, than it is designed to withstand. In testing between the high voltage winding and the core the induced potential between the low voltage winding and core may be several thousand volts, and the low voltage winding may thus be broken down by an insulation test applied to the high voltage winding under conditions which would not exist in normal operation. During the test all leads on the same winding must be connected together. If only one terminal of a winding is connected to the testing transformer, the strain may vary throughout the winding and at some point may even be greater than at the terminal at which the voltage is applied. The charging current of a transformer varies with its size and design. This current may be measured by means of an ammeter placed in the low voltage circuit of the testing trans- 400 former. It will increase as the voltage applied to the insulation is increased. Inability to obtain the desired potential across the insulation may be due to large electrostatic capacity, or to the inability of the testing transformer to supply large capacity current at the voltage desired. In making the insulation test, it is essential that the voltage be brought up gradually. JO / 7- 4 / cQ / ae ' / ^ZLf / ^ / / \a<> i i: | /\ >'* 1 \ k /a 1 •% I / i 1 A / Jo / * i t / 1- / 1 V *• / / 4 J / f 2 • * / /> O 2 SO 4£> GO 0O /O0 /SO /40 /SO /0O 200 2SO B40 260 S0O 300 /f//OYO/6s - sqt/ore root o/ r /77&c7/7 $<2t/t?re Fig. 186 SPARK GAP CURVE The usual ways of controlling the voltage are as follows: 1st. By means of a resistance in series with the low voltage side of the testing transformer. Another resistance of such magnitude as to allow a flow of current at least five times the exciting current should be connected in multiple with the low voltage side, so as to maintain a smooth wave shape under all conditions. 2nd. By means of an induction regulator on the low volt- age side of the testing transformer. 3rd. By variation of the strength of the generator field. 401 The first method is not well suited to very high potential tests on account of the large amount of resistance required. The second and third methods are, however, suitable for any voltage. In applying the test voltage, it should be started at less than one quarter of the final value, should then be brought up during 30 seconds to the full value and after having been held the specified length of time should be reduced during about 15 seconds to less than one-quarter of its maximum value, after which the circuit may be opened. The spark gap should be as near as possible to the trans- former under test and on tests of more than 15,000 volts it should never be more than 20 feet away. Resistances should always be placed in series with this gap, but never between the testing transformer and the one under test. The value of the resistances placed in series with the gap should be such as to limit the current from }/i to 2 amperes in case of a discharge across the gap. This will require from 4 ohms to 3^2 ohm per volt, For tests of 10,000 volts or less, it is usually the practice to depend upon the ratio of the testing transformer in determin- ing the voltage that is to measure the voltage on the low voltage side, a spark gap being placed across to the high voltage side and being set at 10 per cent above the required voltage as a safety valve. For tests from about 10,000 to 50,000 volts, the gap should be set in accordance with the curve of arcing distance shown. (See Fig. 186.) The voltage should be raised slowly until the gap breaks, at which time the voltmeter reading should be noted. The voltage should then be reduced to zero, and the spark gap setting increased to 10 per cent above its former value. The voltage should then be brought up until the voltmeter reads the same value, this voltage being held for the specified length of time. For tests above 50,000 volts, it is not advisable to cause the spark gap to break with the full voltage on the transformer under test. For such tests, therefore, the gap is first set for the desired voltage, while the transformer under test is entirely disconnected. The gap is then broken and the voltmeter reading noted. Then the gap is set for % of the required voltage and the voltmeter read- ing obtained for the breaking of this gap. The transformer under test is then connected and the gap broken at the setting for % voltage. The voltmeter reading obtained with this last setting is then multiplied by the ratio of the readings for full and for % voltage with the transformer disconnected and this calculated voltage is held by voltmeter for the actual test, the spark gap being set at 15 per cent above this voltage during the test. The presence of moisture in the coils and insulation lowers the dielectric strength to such an extent that it is general practice to dry carefully all high voltage transformers before they are filled with oil. The drying-out run should ordinarily be made on all transformers having test voltages above 100,000 volts, and upon any transformer having test above 15,000 volts if it 402 has been standing in the factory for more than two or three weeks before test. The drying is ordinarily done by forcing a blast of air at about 80 deg. cent, through the transformer and this continued until the insulation resistance measured by the megger shows practically constant values. Transformers having high potential test voltages above 13,200 volts are filled with oil for the test. Care should be taken to see that the oil itself is of sufficient dielectric strength. Xo oil having strength of less than 20,000 volts between half inch disks 0.2 in. apart, should be used during the high potential tests. When the test voltage is higher, the strength of the oil should be correspondingly greater. For tests above 100,000 volts, the oil should show a dielectric strength of at least 40,000 volts. As the high potential test is made after the heat run, the oil has had an opportunity to free itself from air bubbles and to penetrate to every part of the transformer. In some cases, however, especially when the oil does not meet the requirements of dielectric strength, it is necessary to replace it before the high potential test. In such cases the transformer should be allowed to stand for some time before the test is applied. This period should be at least one hour for voltages of 50,000 and less, and at least 6 hours when the voltage is above 50,000. Induced Voltage Induced voltage is applied to transformers in order to test the insulation between turns and between sections of the wind- ings. The usual value of this test is twice normal voltage induced for a period of one mimvte, followed by one and one- half times normal voltage for five minutes. Low voltage trans- formers (5000 volts or less), usually have three times normal voltage applied for one minute. The source of power should have an approximate sine wave and a frequency such that the exciting current will not exceed 150 per cent of the rated load current of the excited winding. It is common practice to use a frequency of 200 cycles for 25 and 60 cycle transformers. The voltage may be controlled by any of the methods described for the high potential test. The voltage should be started at less than 34 oi the final value and should be brought up gradually to its full value. It should then be held for the specified length of time, after which it should be reduced slowly to less than l /i of the full value before the circuit is opened. During this test, windings designed for a voltage of over 1000 volts must be so arranged that all portions are connected together using one of the connections shown on the DS sketch. This precaution is necessary as otherwise excessive stresses might be induced between parts of the windings, which under normal operation would be subjected only to small voltages. If the winding has a rated voltage of more than 20,000 volts, it is best to use the full series connection during this test. Three-phase transformers designed for Y-connection having 403 voltage over 20,000 should ordinarily be connected for the highest Y-voltage during this test, although exception is made in the case of three-phase shell types for operation on Y-Y or Y- diametrical systems. Failures in Test When transformers fail between turns, between coils, between windings or from windings to other parts in such a manner that it becomes necessary to dismantle them, careful examination and tests should be made to determine whether failures in other parts have also occurred. Transformers failing under high potential should be given an induced voltage test before they are dismantled. This test should be made in the manner specified for the regular induced voltage test. Three-phase transformers failing in one phase should be given the full high potential test on the other two phases, one at a time, both windings of the two phases not under test being grounded. If the transformer is of shell type construction, induced voltage tests should also be made on each phase sepa- rately (whether or not they fail on high potential), with both of the other phases short-circuited. Three-phase shell type transformers failing between turns or between coils so that dismantling is necessary, should have the broken phase short-circuited on both high and low voltage windings, after which further induced voltage tests should be made on the other two phases. Single-phase voltage should be impressed on each phase separately while the other phase is short-circuited. Calculation of Efficiency The efficiency of a transformer is the ratio of its net power output to its gross power input, the output being at non-induc- tive load. The efficiency is to be based on the maximum volt- age and kv-a. rating, unless otherwise specified. It may be determined by either of two methods: 1. By the input-output method, or 2. By the loss method. The first method which requires the measurement of the input and output on normal load is not accurate on account of the small difference between the input and output, and is very seldom practicable because of the difficulty of obtaining full load. The loss method is, therefore, used exclusively for com- mercial work. The input includes the output together with the losses which are as follows: 1. The core loss which is determined by the core loss test. 2. The PR loss of the windings calculated from their resistances. The core loss may be measured either on the high voltage winding or on the low voltage winding. Rated voltage and frequency should be used. If the generator does not have a 404 sine wave, the loss should be corrected by means of the core loss correction outfit. The measurement of loss should be made at or near normal room temperature. The PR loss should be calculated from the measured resistance reduced to a room temperature of 25 deg. cent, unless otherwise specified. The rated current of each winding should be squared and multiplied by the resistance of that winding, the sum of these losses being added together to obtain the total I 2 R loss. See Calculation Sheets 29 and 30. The rated kv-a. of a transformer is to be considered the output and the losses are to be added to this value in order to obtain the input. For auto-transformers the core loss should be measured in the same way as on a transformer, and the PR loss of each sec- tion of the winding should be calculated from the rated current and resistance at 25 deg. cent. The total loss should be added to the rated output to obtain the input. The rated kv-a. of the auto-transformer is not the same as the output, but the output is always specified by the Engineers. Calculation of Regulation In constant potential transformers the regulation is the ratio of the rise of secondary terminal voltage from full load to no load (at constant primary impressed terminal voltage) to the secondary full load voltage. Regulation may be determined by loading the transformer and observing the rise in secondary voltage when the load is thrown off. This method is not satis- factory on account of the expense of making the test, and the small difference between no load and full load secondary volt- ages. Much greater reliance can be placed on results calculated from separate measurements of reactance drop and resistance, than on actual measurements of regulation. For non-inductive load, we have the following formula : (per cent IX) 2 Per cent regulation = per cent IR-\ — — — ^- — - — where per cent IR= total resistance drop expressed in per cent of rated voltage. Per cent IX = total reactance drop expressed in per cent of rated voltage. For lagging currents, we have the following: Per cent regulation = (per cent IR) P + (per cent IX) W+ [(per cent IX) P - (per cent IR) W] 2 200 where per cent IR= total resistance drop due to load currents expressed in per cent of rated voltage, per cent IX = total reactance drop due to load currents expressed in per cent of rated voltage. P = power-factor (cos 6) W = wattless factor (sin 0) 405 The following table gives the values of W, the wattless factor for various values of P, the power-factor: p w 1.00 0.95 0.312 0.90 0.436 0.85 0.526 0.80 0.60 0.75 0.66 0.70 0.714 0.60 0.80 The per cent IR is calculated from the rated current and the resistance at 25 deg. cent. It may be obtained conveniently by dividing the PR loss by ten times the rated kv-a. The per cent IX is calculated by taking the square of the per cent impedance volts, subtracting the square of the per cent IR and determining the square root. See Calculation Sheets 29 and 30. In auto-transformers the per cent IR drop should be cal- culated in the same way as for a transformer, and may be conveniently obtained by dividing the PR loss in watts by ten times the equivalent transformer capacity in kv-a. The per- cent IX drop should be calculated from the per cent impedance in the same way as for a transformer. The auto transformer should be connected as a transformer during the impedance test. These values of per cent IR and the per cent IX should then be multiplied bythe ratio rated voltage (h.v. winding) —rated voltage (l.v. voltage winding) rated voltage (high voltage winding) after which they should be used in the formulae given above for transformers. INDUCTION REGULATORS SINGLE-PHASE INDUCTION REGULATORS The IRS, or single-phase Induction Regulator, may be cooled by an air blast — it may be placed in a tank and be oil cooled — or it may be oil and water cooled. Regulators of this type are usually made for the control of single-phase lighting circuits. The primary winding is placed in slots on a movable core or armature, while the secondary winding is placed in slots on a stationary core. The regulator may be wound with any even number v of coils. The voltage induced in the secondary winding depends upon the relative position of the secondary with reference to the primary winding, the primary being in shunt and the secondary in series with the circuit to be controlled, the voltage of the circuit thus being increased or decreased accordingly. Single- 406 phase, as well as polyphase regulators have a distributed winding for both primary and secondary, but the maximum pole face which can be covered by an active winding in a single-phase regulator so as to produce the best results, is approximately 60 per cent. In the neutral position the secondary winding, therefore, encloses an area on the primary core not enclosed by an active primary winding and the impedance would be extremely high if no windings were provided. The slots of the primary not used for an active winding are, therefore, filled with a short-circuited winding, so that in the neutral position of the regulator the current forced through the secondary induces a current through the short-circuited winding which reacts upon the primary and reduces the impedance. Tests Required The following tests are made on single-phase regulators: Cold resistance. Ratio. Polarity. Core loss. Impedance. Heat run. High potential. Induced voltage. Xoise tests. Tests of auxiliaries. These tests are usually made in the order mentioned above. The order may be changed, however, if desired. It is considered desirable to have the high potential and induced voltage tests made last and in the order named. Cold Resistance Cold resistance should be measured by the methods described for transformers, care being observed to obtain accurate measure- ments if the rise by resistance is to be calculated at the end of the heat run. The resistance measurements should be reduced to a room temperature of 25 deg. cent., and entered on the test sheet. Ratio The ratio should be taken with normal voltage on the pri- mary, by reading the volts across the secondary with the armature in the limiting, maximum boosting, maximum lowering, and neutral positions. The feeder volts should be read in each position. The number of turns of the handwheel should be noted for each position, starting at a limiting position. Polarity Polarity should be checked against the DS sketch with the armature in the maximum boosting position. The regulator should boost the line voltage when the handwheel is revolving counter-clockwise. 407 Core Loss On this type of regulator with the permanent short-circuit on the armature, the core loss must be taken from the primary- winding. The power-factor will be low due to the air gap — - hence, considerable care must be taken in making the test. The core loss watts and the exciting current should be measured at normal voltage and frequency with the armature in both the maximum boosting and the neutral position. Impedance Impedance is always measured on the secondary winding as it is impossible to force full load current through the primary winding in the neutral position. With the primary short- circuited, full load current should be f orced.through the secondary and the voltage recorded with the armature in the neutral position, maximum boosting position, and position of maximum impedance. The positions should be recorded by giving the number of turns of the handwheel from a limiting position. Heat Run The ordinary commercial regulators are given a short- circuited heat run without oil. One of the windings is short- circuited, and the rotor placed in the maximum boosting or maximum lowering position. Currents of sufficient magnitude to produce a temperature rise of from 50 to 60 deg. cent, in 20 minutes, are held in the secondary. The values of currents for standard regulators are specified by the Engineers. In case a load run is required, the regulator is either con- nected as a transformer and placed on a non-inductive load, or in case two are available they are given a bucking run with the losses supplied from two sources of power. An idle unit is used as a basis for calculating temperature rises, if one is available. Oil immersed regulators should be filled with oil to the gauge line at room temperature. Thermometers should be placed in the tank between the second and third ribs — one at the bottom and one 2 in. below the gauge line. One thermometer should be placed in the top oil, the bulb being immersed about 1 3^ in. Room temperature should be recorded at three or four positions around the regulator. Normal voltage and frequency should be held on the pri- mary, and normal current in the secondary. Thermometer read- ings should be taken at hourly intervals, and resistance readings every two hours, primary and secondary being measured alternately. The normal load run should be followed by a 125 per cent load for 2 hours, unless otherwise specified. High Potential High potential test is made in the same way as on a trans- former. All leads must be connected to one or the other elec- trode of the high potential testing set. Standard 1100 to 2500 volt primary regulators are given a test of 7500 volts for one minute between windings, and from windings to frame. 408" Induced Voltage The induced voltage test consists of the application of three times normal voltage for 10 seconds to the primary winding, followed by double normal voltage for 5 minutes. The fre- quency should be sufficiently high to keep the exciting current within the full load current of the regulator. The armature should be placed in the maximum boosting or maximum lower- ing position. Noise Test Every regulator must be carefully tested for noise with normal excitation, frequency and load, while the armature is moved through its complete range. When the noise exceeds the standard which will be set from time to time, the regulator should not be passed without the approval of the Engineering Department. Tests of Auxiliary Apparatus The motor and limit switch should be connected in accord- ance with the DS sketch, after which they should be operated throughout the entire range without load or excitation on the regulator. A record should be made of the minimum volts re- quired to operate the motor, the amperes at normal voltage and the time required to operate it through the entire range. The tripping lugs should be adjusted during the test, so as to open the limit switch in such a way that the regulator will stop in the maximum boosting or maximum lowering position with allowance made for standard hunting. There must be suffi- cient allowance made to prevent the segment from coming against the stop pin when operating. When the tests have been com- pleted the bearings should be drained, washed out with kerosene oil, and the oil plugs screwed in tight. The brake shoes should be oiled, and the brake adjusted for hunting of approximately 1 per cent of the total range. The hunting should be recorded in turns of the hand wheel. The relay switch should be supplied with normal voltage at normal frequency, and the amperes measured with the armature in the middle position and in the normal operating position. A record should also be made of the resistance, and the minimum volts required to operate. The minimum volts should not exceed 80 per cent of normal. The connections should be checked against the DS sketch. The stationary contacts should be adjusted so that there is Y%vn. spring at the end of the face of the moving element when the armature is against the magnet coil. The stationary contacts must bottom in the holders which should be placed tight in the support. The switch should be given a double voltage test through the magnet winding for five minutes at approximately double frequency, with the magnet armature closed. A high potential test of 1000 volts should be applied for one miniate from windings to core, from contacts to frame, and between the contacts of the switches. 409 Special tests on motors will be called for by the Engineers when required. These include starting torque, impedance, heat run, minimum volts and amperes and watts with regulator loaded. The heat run is made by operating the. regulator at no load, reversing at limits during one hour. Normal voltage and frequency should be applied to the motor. The brakes should be set so as to allow a hunting of about 1 per cent of the total range of the regulator, and should be oiled to maintain this hunting throughout the run. The room temperature, rise in bearings, windings, laminations, rotor, commutator, and brake pulley, should be measured by thermometer, and the rise of windings by resistance. POLYPHASE INDUCTION REGULATORS Induction regulators of the IRQ, IRT and IRH types are used principally with synchronous converters, but are well adapted to control polyphase transmission circuits. As in the IRS type, they may be either air blast, oil cooled, or oil and water cooled. The primary winding is connected in shunt and the secondary in series with the circuit. In the polyphase induction regulator, the voltage induced in each phase of the secondary is constant, but by varying the relative positions of the primary and secondary, the effective voltage of any phase of the secondary on its circuit is varied from maximum boost to zero, and to maximum lower. Referring to Fig. 187 which represents "graphically the volt- age of the three phases of a three-phase or IRT regulator, AAA equals the line voltage or the e.m.f. impressed on the primary. This is shown by the large circle. Let BA, BA and BA equal the e.m.f. generated in the secondary coils and constant with the impressed e.m.f. This is shown by the three small circles on the circumference of the large circle. BBB shows the e.m.f. induced in the secondary coils directly in phase with the primary im- pressed e.m.f. This is the position of maximum boost. Posi- tions CCC represent the neutral position, and DDD the maximum lower position. EEE represents a position between neutral and maximum lower. By changing the position of the armature with respect to the field, the secondary voltage may be made to assume any phase relation with respect to the primary e.m.f.; it can be in series with it or directly opposed to it. This movement of the armature is obtained by means of a segment on the shaft which meshes with a worm on the small operating shaft. The regulator may be arranged for hand operation only, or can be motor- operated. Either a direct current or an induction motor may be used. The motor is controlled by a small double-pole double- throw switch, on the switchboard, to allow the voltage to be raised or lowered as desired. To stop the regulator on reaching the limits of regulation when moving in either direction, a limiting switch is provided, which opens automatically. If properly connected, this auto- matic cut off, however, does not interfere with movement in the 410 opposite direction, which can be obtained by the double-pole double-throw switch. Tests Required The following tests are required on all polyphase regulators: Cold resistance. Ratio. Polarity. Core loss. Impedance. Heat run. High potential. Induced voltage. Xoise test. a Fig. 187 REGULATOR DIAGRAM— THREE-PHASE The order of tests is immaterial, except that it is best to have the induced voltage test follow the high potential test, both of them being made after the other tests have been 'completed. It is also advisable to check the connection with the DS sketch after the tests are made, particularly where permanent con- nections are made by the Assembly Dept. after tests. Cold Resistance The resistance in each phase should be measured and the values at 25 deg. cent, calculated and reported on the test sheet. Ratio and Polarity Two separate tests are required in order to obtain the ratio and polarity; (1) ratio of secondary to primary turns, and (2) boost and lower and polarity. The ratio of turns must be checked by applying normal voltage at normal frequency to the primary and measuring the induced secondary voltages. The primary and secondary should then be connected to a source of supply as shown on the DS sketch, normal voltage being applied at normal frequency. The feeder voltage of each 411 phase should be measured with the armature in the extreme maximum boosting, neutral, maximum lowering and other intermediate positions. The position of the armature in each ease should be recorded in turns of the handwheel from one extreme position. The direction of rotation of the handwheel for boosting should be recorded. Standard regulators are designed for counter-clockwise rotation to boost the voltage. If the primary is incorrectly connected to the secondary, either an unbalancing of the feeder voltages will be noted, or with the feeder voltage balanced, the maximum boost, maximum- lowering, etc., will be found at wrong positions of the armature. It is possible, although very improbable, that such unbalancing may be due to reversed secondary leads. In any event, the proper connection must be determined and the leads plainly marked so that the necessary changes can be made by the Assembly Department. Core Loss The readings of core loss should be taken on the primary side with normal voltage applied at normal frequency. As the core loss is not the same in all positions of the armature, the maximum and minimum should be found and the readings taken at these points. The position of the armature should be recorded in turns of the handwheel from one extreme position. On IRH regulators having diametrical or double delta pri- mary connections, it will be more convenient to make the test with three-phase single delta temporary connections. The connection used should be noted on the test record. Impedance The impedance is usually measured by short-circuiting the secondary and applying sufficient voltage to the primary wind- ing to give full load current. As the impedance is not the same in all positions, the maximum and minimum readings should be obtained, and the position of the armature noted in each case. The impedance of an IRH regulator may be conveniently measured by connecting the primary, secondary, or both as three-phase. Heat Run It is customary to give standard regulators a compromise run with 150 per cent normal current and 125 per cent normal voltage for two hours, the proper cooling medium being used throughout. Hot resistances should be measured and the temperature rise calculated. Usually the secondary current is held at a specified value, but in case it is too large to measure it is considered satisfactory to hold the corresponding primary current calculated from ratio of turns. The ultimate heat runs are usually made with two regulators connected according to the motor-generator method, with the primaries in parallel and the secondaries in series so connected that the primary fields will rotate in the same direction. Normal 412 voltage is applied to the primary at the rated frequency. The armature of one regulator, called the generator, should be held in the maximum boosting position, while that of the other, the motor, should be adjusted until the proper secondary current is obtained. It is necessary to see that the currents in the pri- mary and secondary windings are balanced, particularly when the secondary current is large. The primary current will not be the same in both regulators. If the secondary current is too large to measure, the primary current of the one running as a generator should be calculated as follows: The theoretical primary current calculated from the ratio of turns should be added at an angle of 90 deg. to the magnetizing current measured at normal voltage. Under such a test, the heating of the regulator running as a generator will be equivalent to that under normal load con- ditions, whereas the heating of the other will be somewhat higher. Water cooled regulators should be run with the specified amount of water, which should be put in at about average room temperature, and the same temperature held throughout the run. Air-blast regulators should be furnished with air at the specified pressure. The quantity should be measured at the start of the run. The temperatures should be observed at oil level on the outside of the tank, at the bottom of the tank; also the tem- perature of the top oil inside the tank. On air-blast regulators, the temperature at the top of the tank and at a number of places on the windings should be observed. Care should be taken to avoid obstructing the passage of air. In case there are likely to be hot spots in the windings or connections, thermometers should be placed on them. Resistance of one primary and one secondary phase should be taken alternately every hour, unless the secondary resistance is too large. In that event, the primary should be taken every hour. The resistance of each phase should be measured at the end of the run, and the rise of temperature calculated from the increase in resistance. The proper number of single-phase regulators may be used instead of a polyphase regulator as the motor on a motor- generator run, provided they do not materially change the conditions of the polyphase unit under test. The heat run may also be made by putting dead load on the regulator, if necessary. High Potential The high potential test is usually made with the regulator hot. On standard 1100 or 2200 volt machines, 7500 volts is applied for one minute from primary to secondary and core, and from secondary to primary and core. On other regulators, the test voltage is specified. The same test voltage is applied between secondary phases and between primary phases if they can be separated. The test between phases should be made from phase 1 to phase 2, from phase 2 to phase 3, and from phase 1 to phase 3 independently — not from phases 1 and 2 to phase 3, 413 etc. The phase not connected during test should be short- circuited on itself. Induced Voltage Triple normal voltage should be applied for 10 seconds to the primary winding, followed by double normal voltage for 5 minutes. The frequency should be sufficiently high to keep the magnetizing current within full load current limits. The armature should preferably be placed in the maximum boosting position. If three-phase connections are used on an IRH regulator, care should be taken to see that the proper voltage is applied, viz. double volts per turn. Noise Test The noise test consists of operating the regulator with normal voltage and frequency, while the armature is rotated through all positions. If a short-circuited heat run is made, the armature should be moved over the full range during the run. If it is suspected that it may operate in a noisy manner under full load, a test should be made under as nearly full load conditions as can be obtained. Tests of Auxiliary Apparatus The operating motor and limiting switch should be connected in accordance with the DS sketch and normal voltage applied. The current and the time necessary to operate from maximum boost to maximum lowering position without load or excitation on the regulator should be noted. The minimum voltage required to operate the motor under such conditions should also be ascertained. The brake magnet, which is always designed for the same voltage and frequency as the operating motor, should have normal frequency voltage applied, and the current measured with the armature up. The maximum volts required to operate this device should also be determined, and the cold resistance should be measured. If the minimum voltage is more than 80 per cent of normal, the brake should not be passed for shipment. All auxiliary parts should be given a high potential test of 1000 volts for one minute from windings to frame and from active switch parts to iron supports. BR REGULATORS Modern central stations employ alternating current gen- erators of large capacity, each generator usually supplying two or more districts through independent feeders. One feeder may serve a business district, while another from the same generator may feed a residential district. As the compounding required on any of the feeders depends on the amount of load carried by the feeder, and as the load peak occurs at different times in different feeders, a device to regulate the feeder voltages independently is necessary. 414 Type IRS may be used, but the automatic BR feeder regulator has been expressly designed for this work. Fig. 188 shows the circuits. The automatic BR feeder regulators can change the line voltage quicker and with a smaller power consumption than other automatic types. The only moving part is a small and light switch arm. The friction of a number of small switch contacts constitutes the only turning resistance. The moving part of the switch carries a series of fingers, the majority of which are always in contact. See Fig. 189. Each finger is connected to a corresponding stationary collector ring by a brush, and the collector ring is connected to the line through a preventive resistance. The resistances connecting the fingers to the line prevent excessive exchange currents as the fingers pass from contact to contact, and vary the line volt- age uniformly. The regulator transformer is oil cooled. Tests Required The following tests are required: Cold resistance. Heat run. Ratio High potential. Core loss. Induced voltage. Impedance. Test of auxiliaries. Cold Resistance The cold resistance of the primary winding and of each half of the secondary winding should be measured exclusive of the preventive resistance. The resistance of each of the preventive resistances should be measured cold. The spring contacts should be insulated from the contact blocks by means of a thin sheet of fiber, and the resistance measured between the collector rings and the common connection. Ratio Ratio is taken at no load with full voltage on the primary, by reading the voltage across the secondary with the switch arm in maximum boosting and maximum lowering positions. The voltage should be read between the middle point of the secondary winding and each contact block. The polarity should also be checked against the standard sketches provided by the Engineering Department. Core Loss The magnetizing current and core loss readings should be taken at normal voltage and frequency with the switch contacts so arranged that each spring contact will cover one block only, or the contacts may be insulated from the blocks by means of a thin sheet of fiber. This arrangement is necessary as otherwise part of the secondary windings would be short-circuited through the preventive resistance and this loss would be included in the core loss reading. Impedance With the primary short-circuited and the switch arm in one extreme position, full load current should be forced through the secondary and the voltage and watts measured between the 415 middle point of the secondary winding and the contact block covered by the spring contacts, after which the readings should be repeated with the switch arm in the extreme position. The same readings should be repeated with the drop, and loss in the preventive resistances included. Heat Run The compromise heat run is made without oil, the primary being open-circuited and one-half of the secondary short- circuited, while current of sufficient magnitude is forced through the other half of the secondary to produce a rise of from 50 to 60 deg. cent, in 20 to 30 minutes. Resistance should be measured 416 at the end of the run and the rise by resistance calculated. The two halves of the secondary should be measured separately so as not to include the preventive resistance. The voltmeter leads should, therefore, be attached to the middle point of the two secondary coils and to the extreme contact blocks. 15^^/^ww^Swvww^W^ Tbfeec/er i 0/q/Sw/£c/) I I I I II I ^444- ■H* D/a/ Sw/ich flevefoped u \* 4 4 <4 Co//ector R/ngs Pnevent/ve /?es/s6o/7ce Fig. 189 BR REGULATOR An ultimate heat run may be made by the motor-generator method if two regulators are available at the same time. If only one is in test, it may be pumped back on a suitably arranged bank of transformers or it may be loaded on a water rheostat. In the latter case, apply voltage to the primary, connecting the secondary to a water box, adjusting until full load current is obtained. The switch must be in one of the extreme positions. 417 High Potential On 2200 volt regulators, a 7500 volt test for one minute should be applied from windings to ground. The test voltage will be specified on other regulators. Induced Voltage Three times normal voltage should be applied for one minute, followed by twice. normal voltage for five minutes. Tests of Auxiliaries The motor should be tested to determine the minimum volts required to operate it, and the current consumed when operating at normal voltage. The clutch coils should have tests to determine the resistance of each coil, minimum volts required to operate, and current consumed at normal voltage. With the motor and clutch coils connected to a line of rated voltage, the switch arm should be turned back and forth for one-half hour from one extreme position to the other. Operation should be watched closely and the time required for turning the switch arm from maximum boost to maximum lower should be measured. High potential tests should be made before assembly with the transformer parts as follows: A test of 1000 volts for one minute from clutch coils to frame, from active parts of limit switch to frame, from contact blocks to switch pot, from collector rings to support, from contact fingers to support, and between contact blocks. A test of 500 volts for one minute between collector rings and also between contact fingers. High potential test of 1000 volts should be applied for one minute between motor leads and frame, clutch coils and frame, and between active parts of limit switch and cover, when the final high potential test is made on the assembled regulator. REACTANCES At the present time reactances are built in several different types, the design depending principally upon the use to which the reactance is to be put. The largest sizes, called current limiting reactances, consist of a winding of bare copper cable on a cylindrical concrete core, the turns of this winding being insulated from each other by strips of wood, and the whole device being cooled by natural air circulation. Reactances of large size are also used in connection with the operation of synchronous converters, the design in this case being that of a polyphase unit wound on a laminated iron core and cooled by air blast or by oil circulation. The smaller reactances are used mostly in connection with the operation of mercury arc recti- fiers. These are wound on iron cores and are cooled by natural circulation of the air. 418 Tests Required The following tests are usually made on reactances: Cold resistance. Impedance. Heat run. High potential. Double or triple voltage. Where there are taps, it is necessary to check the tap ratio in the same way as on transformers. Cold Resistance No special instructions are needed for this other than those given for transformers. Impedance The impedance test consists of forcing normal current through the winding and reading the volts and watts. Care must be taken to have magnetic material removed at least 3 ft. from current limiting reactances during this test. Heat Run The heat run on current limiting reactances is made by forcing normal current at normal frequency through the wind- ings and continuing the run until temperatures become constant. Spirit thermometers only should be used to measure temperature. The heat run on reactances for use with mercury arc rectifiers usually consist of a 5-hour normal load run with a complete set of auxiliary apparatus connected to the mercury arc rectifier tube. A stability test is usually made at the same time as the heat run on reactances for rectifiers. This test consists in the deter- mination of the lowest value of direct current necessary to maintain the arc in the rectifier tube. High Potential The high potential test from windings to core is made accord- ing to the rules given for transformers. No special instructions are needed for reactances. Double or Triple Voltage This test is made in the same way as on transformers. The frequency is increased in order to keep the current within reasonable limits. SERIES LIGHTING TRANSFORMERS Series lighting transformers are used to insulate lamps from a high voltage series circuit. They range in capacity from 40 watts to 2000 watts and the standard ampere ratings are 4, 5.5, 6.6 and 7.5. As a rule, they are air cooled because the small capacity and low losses make it unnecessary to use oil as a 419 cooling medium. The primary winding is connected in series with a series arc or series incandescent circuit so that under all conditions of load on the secondary, the primary carries the full current of the circuit. For satisfactory operation of the incan- descent lamps connected to the secondary, it is desirable to obtain as near constant current in the secondary as possible. The tests required are: High potential. Resistance. Core loss and exciting current. Open circuit voltage. Impedance. Regulation. Heat run. Induced voltage. The high potential, resistance and impedance tests are made in the manner specified for constant potential transformers. Core loss should be measured at normal primary voltage and at normal primary current, the secondary being open- circuited in each case. The normal voltage is calculated by dividing the rated kv-a. by the rated current. The open-circuit voltage test is made by reading the voltage across the open-circuited secondary with normal current passing through the primary. Regulation test is made by putting various loads on the secondary with rated current passing through the primary and measuring the secondary voltage corresponding to each load. Readings should be taken at 34, H, Z A an d full voltage. Incan- descent lamps should be used for the load. The heat run is made with incandescent lamp load. The induced voltage test is made by applying three times normal voltage to the primary with the secondary open-cir- cuited. 420 CHAPTER 25 CALCULATION SHEETS The following calculations, which have been made with the slide rule, are intended to illustrate the method used in connec- tion with testing work. Every effort is made to avoid error but this Company does not guarantee their correctness nor does it hold itself responsible for any errors or omissions in these sheets. SATURATION ON A 500 KW., 600 V., 360 R.P.M., 60 CYCLE, 3-PHASE GENERATOR Volts Volts Amp. Speed Arm. Field Field R.P.M. 192 25 18.0 ' 360 228 29 21.0 360 253 32 23.2 360 304 38 29.0 360 416 52 40.0 360 495 62 48.9 360 542 70 55.1 360 579 75 59.8 360 597 597 \ 597 J 614 79 62.0 360 83 65.4 360 707 110 87.5 360 785 146 117.0 360 755 130 102.0 360 555 74 55.5 360 453 5/ 43.6 360 287 35 26.3 360 178 26 16.1 360 CALCULATION SHEET NO. 1 421 T)5 ooooocoooooooooooo COCOCOCOCOCOCOCOCOCOCOCOCOCOCOCOCOCO cocococococococococococococococococo d2 q q n- q cq -xF cq oq oq Ooon^oj c^ o co 06 ^' o o cd c Ci >fo cq q oq oq oq acoNM qqiocoioio do6»d(N'ocod^coHo^o66^6N oo oq cq co co ^ iO CO I> N N 00 00 O -h 31 xH (M ^ OhcDONO5OC<100(M CO H(MMC0 CO ^ iO tO LQ LQ CO CO CO I> o o co io co a>coco*o w io o (M o o i> <>j co co "tf co co i-h io co o oo cq co i> co ^ OOOOCONHOHNOICOO^HOONOOIX) 00 t-1 hhMcO ^ iO I> Oi OHH(MiO00 CO ^ lOiOiCOCOOO^O^OOOOOiOOOOiONiOiO 00 mSt oa^rHcoHooeqoMioooooNOrHioH co p? i-h ^iocooqooi>>oi>oq»o(Mioo3i>Ttico^ 1 '* ]>» '-■i I oooQOOHoocq^cooooooooiOH^N th CSJ r-H T-i t-< ,-H H y-i T-H H r-H CS| Oq CS) Cq iOifliCNO(MiCi«0(MC<10>0(MOiOCO>OiO SJ TjH^>ocot^oo^a>oqcoo^'- | co^co-^co °S o ooooooooo ooo ooooo io lOroOOOOOWfNiMOiOWOO'OOOOiO xfH cocoi>^cocqoco»ooooo 1> O00©OOH00(M^O0000OiOOH^n th Oq ,-H ,-H ,-H ,-1 rH rH t-H i-i cq C)'£ -& odcdidoidcdcdcqco'iddcdcdco'oo'idcqod c id !>I>000iOOl>'-i0qxtHC01>c0l>I>00'-HC0 rs ^h oi>'-ioqxtHcoi>coi>i>oo co s oqoq^ SB qtqqoqcotototocoo^totqoootoooo oo co co^' ^' ^' ^' co^' ^' io" id co io id co' co cd i> o co fe Ph fe CALCULATION SHEET NO. 2 422 o o > r tf o O o h o O Pi o H < B rococo cococoeocoeococotfococc &2 x <# p p oo co ooccoqio — ; — !N rt x os — ' o e o -^ I> (id << o o ue o *o O L e »-e >o»oio>oioo OS CD re X O O lO OS CD OS i-l CO ^_ ,_, ,_, _| ,_, oq £<, ^ ^ g5 i— i IQ 1M 00 -^ ■* CO ^CXCCC — OC0C0»0-«#r-IO»O"^l>C0'sf < I> iQ - e ^t O accnoco^ooHco^iNioo t- — eq re ^t >-e omh^x O O a z 5 p .pj -1 1 o»o»oo»ooo*qooooo»o »O00C0Tj00 -CCNC^^OX^^-i^O CO 0C CONCCi'Xi'OXC^N - a Le ko Le i_e iq io iq io iq io »o io ^e io c re ^t- L.e t^ o ce >< b io c x c :i c ic ei q ei ei id re* -r re' re -r id re' -f" id id -r i ~ to Friction Frid ion f> -u r V-. a; r/i 4-1 £ «J ^~ O 0} a) c n : i o ^2 l! O o o R w r/j r/) ■/ CU M L-; nt VI j-i — 0) 1 > ~ rt i- 1 c — " cc *— ' 1 1 o II 0< bua Q^S CALCULATION SHEET NO. 3 423 CALCULATIONS OF DECELERATION CORE LOSS ON A 3000 KW., 2300 V., 10-POLE, 60 CYCLE, 3-PHASE GENERATOR Moment of inertia is equal to 705,000 = Wr 2 . The normal speed of the turbine being 720, Si is taken equal to 730 and S 2 equal to 710. Consider curve taken with no field on the machine. (See Fig. 59.) r 3 or time corresponding to Si =61.6 seconds. T4 or time corresponding to 52=82.4 seconds. Ta-T z =82.4 -61.6 =20.8. (Si -St) Kw. loss 2308 Tr; , 9 W-S 2 *) 10 10 2308 X T A -T 3 705000 X 28800 2308 (Si+S.) 10 10 Ta 4700 10 10 Ta-T 3 Ta-Tz Substituting the value of Ta — Tz in the formula 4700 Kw. loss = 226 = Friction and Windage 20.8 For the curve taken with 77.4 amperes field current Ti-Ti =70.6 -52.1 =18.5 Kw. =-r5-^ = 254 = Core loss + Friction + Windage. 18.5 Curves taken with 103, 129 and 142 amperes field are calcu- lated similarly, and together with that taken at 77.4 amperes field include the constant friction loss and core loss. The two losses can be separated. Amp. Field Held Tz or Ti r 4 or T, - Tz or T 2 - Ti Si 5 2 Si 2 -S 2 2 Fric- tion Core Loss and Fric- tion Core Loss Volts from Satu- ration 61.6 82.4 20.8 730 710 28800 226 226 77.4 52.1 70.6 18.5 730 710 28800 226 254 28 1570 103 48.2 66.1 17.9 1 730 710 28800 226 266 40 1990 129 44.4 60.5 16.1 730 710 28800 226 292 66 2350 142 42.8 58.2 15.4 730 710 28800 226 306 80 2500 From the saturation curve the volts armature corresponding to the various field currents used can be obtained and a core loss curve plotted between volts armature as abscissae and core loss as ordinates. Si and S 2 are usually assumed at 2 per cent above and 2 per cent below normal speed. CALCULATION SHEET NO. 4 424 FIELD COMPOUNDING ON A 150 KW., 250 V. 225 R.P.M., D-C. GENERATOR 6 BARS BRUSH SHIFT 6-POLE, Volts Amp. Volts Amp. R.P.M. Arm. Arm. Field Field 250 226 10.8 225 250 150 240 11.65 225 250 300 270 12.90 225 250 450 300 14.3 225 250 600 334 15.9 225 250 750 370 17.6 225 CALCULATION SHEET NO. 5 PHASE CHARACTERISTICS ON A 300 KW., 600 V., 750 R.P.M. , 25 CYCLE 3-PHASE SYNCHRONOUS CONVERTER NO LOAD FULL LOAD 500 AMPS. D-C. Volts Volts Amp. Amp. Volts Volts Volts Amp. Amp. Volts D-C. A-C. A-C. Field Field D-C. A-C. A-C. Field Field 600 378 315 0.75 91 600 384 601 1.05 125 600 377 255 1.25 150 600 383.5 570 1.25 150 600 376 210 1.50 180 600 381 543 1.50 180 600 375 156 1.75 210 600 380 520 2.00 240 600 374 120 2.00 240 600 379 512 2.25 270 600 373 85 2.20 265 600 378 507 2.50 300 600 373 65 2.30 275 600 378 505 2.65 320 600 372 41 2.40 290 600 378 510 2.75 330 600 371 23 2.50 300 600 376 525 3.00 360 600 370 14 2.55 305 600 375 547 3.50 420 600 370 17 2.60 315 600 374 585 4.00 485 600 369 21 2.65 320 600 373 627 4.50 540 600 369 35 2.75 332 600 370 685 5.00 600 600 369 75 3.00 360 600 368 116 3.25 395 600 367 170 3.50 420 600 366 205 3.75 450 CALCULATION SHEET NO. 6 425 SYNCHRONOUS IMPEDANCE ON A 500 KW., 600 V., 20-POLE, 60 CYCLE, 3-PHASE GENERATOR Amp. Volts Amp. Speed Arm. Field Field R.P.M. 224 15.0 11.9 360 260 17.8 13.7 360 300 20.6 15.8 360 352 23.8 18.3 360 398 26.9 20.7 360 474 31.5 24.5 360 480 480 1 480 J 32.2 24.8 360 518 34.8 26.7 360 557 37.5 28.2 360 704 47.0 36.1 360 796 52.8 40.6 360 896 59.5 45.7 360 1000 66.5 51.1 360 CALCULATION SHEET NO. 7 426 LO 0030C o cc:i oq co o o o o O rf t-h O c; ccx OqOO o o ic co Oq CO Oq 00 ^t -H lo oq o Oi oi oq OS O CO CO CO co oq o ^ -h co oq o T— 1 1—1 H i—( " LO o x o o O OLOLO — i oq' o o o «o ON C O O O LO X LO -^ o rH i-H tcH co^^ X ^H t^ I> lO i-H Tjl tH X Oi CO X xo Oi co oq i> o OS OS l> X 1—1 tH LO OtCOO O O O CO OLO o o o o o coo; o OS — i — i x X o ic CO ^H O CD 1-1 1>- ^ LO X Tt< IOHH X O T}< o ^ LO C5 i-H T-l CO CO X l>CO CO CO "£ o^>oc O O C lo (MOO o o o 3 oa co O O Tf X X OSI> O oq oq co X> OSTf< oq i-h h to -ch x oq Oi CD CM ^ X i— i oq io LO lO-^ ^ ^ 10 ra LO O O CO o LO LO Ol O oq x o XX CO 3 C — C re co x x O CO lO ^ Oi X CO Oq CO OS CO CO CO i-H I oq co os ' T-l CO lo OS CO CO to DC co oq oq oq '— ' o 3 "3 ^r -~> . Jv . s . o . c 'C E II ^H -—^ •+ • a O .2 3 % gO £ nil . w i 1+2+ Veils Amps. R.P.M. . Wat Is Input ~^ ii r-§ • • • 3 S.S g §5 I . oq o Oil> oo do oqoqoqo & XOMN £ ONOH o HQOO S dodo 3^ ° ■^ -5 P r-. £ o C 3 e * c £ = Rio — Rn = armature, series field, series field shunt. " commutating field. " " shunt. Then the total IR drop=/ 4 Rt+I 4 R 5 +I s Rs+Iio Rio- Let Wi = Core loss watts taken from the core loss curve corresponding to Vl~\-IR for each load. W 2 = Watts brush friction from core loss test. If the value taken from test appears inconsistent, calculate W2 by the formula: W '= 33000 Where . F = Circumference of commutator in feet N =R.p.m. B = Number of brushes L =Lb. pressure per brush ix = Coefficient of brush friction for the particular type of brush used. In the case of engine- driven machines or those which are furnished without base, shaft or bearings, the bearing friction is omitted from the total losses, and is charged against the prime mover. In nearly every case it is preferable to use the calculated brush friction instead of that obtained from test. During a short test, the commutator and brush contact surface cannot get into as good condition as is obtained after a long period of commercial operation. Consequently, the brush friction test does not represent the conditions that will exist after the machine has been in operation for some time. The coefficient of friction determines the value of brush friction, which in turn is deter- 430 o >-0 3 OS § tO ^ OS iC I> 1> O H©C0O D lOiOt^COOCO^oi^f'iC^t o »c o o co i> io to oq os d oq i> i-h oq Tf i> oq o oq ^h i>^r to oq o oq oq co os co £ hom oq i-i co ^t co i>^Oi (X)Tt ^H t-( rH H- Tjl H o 5 i— I tO tO D o 3 ^_ ^ oq oq os .os t-0 i-l oonoo ii O»0^C0I>c6l>C006»0^ O'-h o MNOCNcir-Jd = g ONN N h C N O! O! h X CO to C\) tO LO O C OS CO i— i to i— t h t— i l~ ;c rc O ro c; ionoohh i— 1 CO *— 1 i> ■iS ^ ^ < oq oq OS i-i n w iC lO re 00 CO c c c ^«©ooq to oq d co co l>- oq od d to -* ctM O co ^ i-i co oi oq co d t^ co co ^x^hxcih io oq i> os Tt os o t^ os oq >Oh i-. to oq co NiN M oq i-h x i—i T—i i—i to 1 ^ £ Q tO IQ < r N CO -* <© rH OvJ oq oq o q o §S OONCOOOOXM'NOTt t^ t^ o H^OONNHOO cooo oi c n h a o h os i—i cs n o h i* m O'H - ft to io oq co i> '-i b- < « to * m o ■* CM x co co X Oq rf tO -h O - ioiOi-Hi>(Ncocqoo ^ ^ oq oq co q A W O O iot>c6oo«dos-^oco^H'* wo o co co co co* d t> od d nm^ t oq y-t -t oq — i r-H ro t-. coi-i oq oq x to Lt — cc oq i> D Oh i> 5 o — OS •H i-H Tf -t OS o*o©cocoood •o ti — o — — ■ \z ■ — ■ O] < "J ~j ~ ~ M X (N »; 3 ~ -'^ • © OJ U cd • • • • ■ — v- •— • R ■ — _ ' " ' '# 4 » »-i c v — a - ~ ~ ^ C .. cc w u> to -x ,-s ■-- J=. .~ < 22 ^ rV 1 {2 0. ft — ft ft — — a> 53 i-^^wft Ceo j o JoHU ^Pi c ^ IS": = F 0)0 o o tO ^ TO C3 03 g s so OOx XcOo CO CQ S OOx qoso d +i +j • c c G o o u ?o?o ° c Oqcq oq 2^ JH -*->-(-> w -y. -y. 'x '7. '-7. ooocqido6o»od io co co oq tjh i-h >-h i> co oo os oq co -tf *o oo (N oq to Oq rH rH CO CO O CO Oq CO Oq 00 OH HH00 IOH -H r^H CO CO qi> oq oqq oooooq»oi>.oooqo5oioo ococoioi>'-'oq»o»ocooocq r^i ^h to i-h i-h oq OS oq th i—i io CO ■* »0 O N d <*' O" O00 00 OS CO ioh cq q OOOOOiOiOOOCOOOHNiCO iO CO CO CO O i— lOS^CO^OOOi-t oq hio CO ^ IO o oo oq ioco ^ O »0 iO OS oq CO OSr-H th oq oq q lOOOLOoioioos^oq'oq'oso i>cocoi>»0'-'Ooqoqcooo ^h ^ io oq oq o oq hio CO ■*# IO . o os oq co' co r^ ooq oq as IO TjH 00 i> oq oq i-i t-h ioi>q i>q OOOCONOO^'dMN^O OCDCOCDHHOOH T-i CO io ^ >o oq t> oq i-h r^ w Volts Line Amperes Line Amperes Field Amperes Arm. IR . P^ l — i 1 bpeed Core Loss Brush Friction Bearing Friction PR Armature PR Brush IE Field . Total Losses . Kw. Input Kw. Output . H.P. Output . % Efficiency . Brush Density Brush Contact Res 3 Si pq u CD a CD Ph Co 4J ^OC/2 +j CD g as a tj: in &§■§ r-l ^j ■9 J? O^od 1— I t/3 4 CO o jh o do" Hw 4-» OS 7, «5X q id C3 oq «^\ a; CD - CO •w <+-< O is o O ™ ^ - %^, "~~"~~ ■- ~- ^ ■-■ — =. — — MOO 2000 3O0O 4000 FeeC per Aff/7v£e sooo Fig. 190 ►COEFFICIENT OF FRICTION OF A-C. BRUSHES The calculation of the a-c. brush contact resistance requires a measurement of the alternating current flowing in the arma- ture. This also varies in different types of machines. The following are the constants by which the direct current should be multiplied to obtain the alternating current. For Single-phase 1-41 Two-phase ....... 0.707 Three-phase 0.943 Six-phase 0.472 As with the d-c. brush contact resistance, a curve must be referred to of the a-c. contact resistance. This should be used and no direct measurement of resistance attempted. In every case the contact resistance should be calculated per ring, the total loss being obtained by multiplying by the number of rings. Brush contact area per ring = width of brush in inches X arc of contact in inches X the number of brushes. , , , , . Alternating current The brush density per ring == r- — ^ Q „ - nrr * fe Brush contact area per ring * Upper curve taken with copper collector rings. Lower curve taken with gun metal collector rings. 435 CO CO ooo 1> I> I> rH CD Ort< ■rH O r-< CO oo © ^ cq w q q ooooiOHTfOHiooodod ooqoonoi-ifMioooitoto COl>OSCOtOOqOs^H^ OS H rH oq coco (MOW (NOCOCOIO tHcocO coiONi- 1 CO COCO oq oq rH CO OO to CO to OS o o ooooHHoiowiooorldd OOOOOSCOHCONOOJ^^ lOoqoscO'stHcqiococo ©H 00 tO CO CO OOOCq'c^H/io^cH^H ooo ot> co co to rH CO to iO^!>i-icO CO O OS CD O O oooocDT-Hiootdioodcodd NCDOOiNHiOO'-iOsmM rHOSOSCO(N(NI>COCO ^ to 10 CO CO •OOIOWNCDO^'* NON 1> to CO CO LO CO CO CO COI> H CO ^ rH (N CO ^H oq to rH TH oo to co oq oq q q OHoocoHcoioo6^'d»odd ^H/ioostOiHoooqcooscqcq COCOOSCOrH(MTHC^CSJ CM CO to COCO OOOIM'lNOOO^'* to o to to CO CO CO to co oq cs) (M i> h co TjH i-H CM CO "* oq co rH to oo oo i> to os q q coooooi-itooi-Hcq'oscddd 10^005NHH10C005HH O CO OS CO (MO0HH to co co cq oq o cq cq oq co co to CD i-H HHNHCO CO Oq CSI th CO tO O O i> t(h oo to q q 03HooooHNio»ONo6o6dd OOOO1HHC0N00 00 (M rH OS co oq l> O 600 2.65 2.65 4760 1134 2654 CO oooo rHos do O OS rH TjH rH OS co oq CO o % Load . Volts Line . Amps. Line Amps. Shunt Field Amps. Arm. D-C. Amps. Arm. A-C. Core Loss . Brush Friction D-C. Bearing Friction PR Armature (.59 X D-C. PR) PR Brushes D-C. PR Shunt Field PR Rheostat . PR A-C. Brushes PR A-C. Brush Fric. Total Losses Kw. Output Kw. Input % Efficiency Brush Density [ ^_"£ Brush Contact f A-C Resis. { D-C 00 •« 3 -u m u rCl m 00^ G 5- a a pq ^ o "> ^00 o9 d9 S G rG G ^^ << / ^" — ^esi Ocl o biO 1 "! < CO 'C II o3 2) .tf = Vj X V LXlLX7o P-F. for three-phase machines K w IL= VlX2XV P-F and W b = 2V L XlLX% P-F. for two- phase machines 7i should be calculated for various power-factors as given under regulation. 437 o 2 ° M IOONNOOOOOOOOOIOCO NOHiOiOiOOOOOOO»ONO> HomiN oo»ohooo^(n^ i-i i-H N(M 1-1 OS lO iO CO CO i-i HTf COH(M(M i-i CM OON»0 00 00OOOOOOOOO OOCO^^h-^OOOOOOOi-iOi HONOOCOONNCD rH r-i CO CM CO lO I> CO CO ,_, ,_, ^ ^ rH CM OS OOi-iOO^^OOOOOOOO)CO >OOo:(MN(MOO(MOO(M00005 OH(M O i-i CM CO CO O CM lO CO i-H rH CO iO LO iO OS CM CM r-l rH ^ rH CM 00 iO i-O O lO Th CM CM o CM O CO CM rH i-H O O CM O O rH rH CO rH HrJ- CO ooooo^i> CO O O CO *0 CO 00 CO O O CO CM HH HIQIO^HH rH CM 00 oooo o o O CM OO O CM OO rH rH CO rH rH ^ IO OOOOOCM O O O O 00 lOOlO rH HH iO CM rH CM 00 ■0-U ^! . . . « 4J >* O a; t* o W rH rj g i» << B > O rH^H rnfeHMM^ CALCULATION SHEET NO. 14 438 Ph". o M w I- CM C f§ ^ o °g ,— ; IO ° J! ° 0?o r^ cm CM t/: t° ►H CM 00©0 CM i-H O CO CO CO CO CO 00 LO O O O (M CM rH rH b- LO 05OON(D»0(MC0 0i rHrHCOCMrHCOCCOO LO rH CO O CM 50 13200 19 51 69 13131 13700 00 CO COCO r-J MOON^CDOO^' OCDOONNWHiOOJ 1-|(MCOCMO^^LO CM CO CO CD CM LO CO LO LO O OJ O TjH LO O (MO LO CO CO O (M hoo CO CO CO CO CO CO CM t> O CM co cq cq ^ co o tooooo o i—i 028 000784 00001309 004393 00440609 001856 i—l cq 010435 431835 00010135 CO cq o to to OS OS cq oq ^ os co J> O CO 00 to ^ i> oo cq i-h t-H t-H t-H o cq os to co co i-H cq co to o tooooo 021 000441 000007362 004393 004400362 0013915 CO CO CO 010435 326735 000057 CO OS Cq o iO H lO N (M co «* i> o co to cq Tti co o cq co l— 1 T-H i— 1 O i— 1 OS t-H O H CO co b- t-h cq to ^ co o ^ cq co co t-h cq co ■* o coooooo T— I 014 000196 000003272 004393 004396272 0009279 • (M 010435 221535 00002533 CO to o o 14725 153011 04905 02341 07246 CO oo oo co cq t> cq o t> oo co cq OS OS OS 00 00 CO co o h cq cq o cq o oo o o n _ o, N + cm cc x xx lO iq x* OS OS OS X HOHOomroo o lOOiOO o o q CM d ^ o CM t^ o ' d d d d CO CM "^ O t^ X HO) X CO to CM X H f " r "^ '- h ' X O OS OS CM CO CM CM CO to to CM X "* (M Hffi OS OS CD I> r-( T— 1 X X CO CD tO X CO CO CO OS OS OS T— 1 xxxo Oi-h cm -* tP O rt X ox otjj o^ poo q CM CD cod ' d>d>Sd> HlO T}H O^ O i-H i-H Th COtHCO 1> OS r ' \ '** '^ OS lO tO tH ^ CD CM CM CM CM to co X CM OS t> CM ■^ O OS I>1> I> 1—1 X tO O l> O OS CM CM CO CO OS OS X 1> Kmc?:ocN q co o co q q q ic q to d cm : as © 'dodo X Tf TH O-HH OS O CD CO CO OS CO 1> f " l" '^ '^ o CO OS X X OS i> x cm ba Oi CO CD -t — x ea o tO X O 1— 1 -* co x ^ co Tf Tt Oa -^ OS q X X CM I> CO Tf X O X CM N C N C C C O CM O CM O O O OS CM q CD d do ' d>d><6<6 OS C<1 ffr co t> coc;n X CO CO CO CO ^ \ ' \ "^ "^ o CM CM CM CO »— 1 T— 1 T— 1 T— 1 w w * -S ,. ' t + + -6 ,-s £ + co f- 1 3i o Po (See note (See note II 1 II II II II II II II II s « ^ ^ £ H.P. orque H CALCULATION SHEET NO. 20 (Continued) 447 SUMMARY OF SPECIAL TEST EXCITATION RUNNING LIGHT Volts Amperes Watts • Polyphase Single-phase Friction watts 440 440 36.7 60.5 3026 3460 900 STATIONARY IMPEDANCE Polyphase Single-phase 118 102 4375 2050 Impedance amp. at rated volts =910. Max. =936. Min. = 810. Slip (S)=2.8 per cent at normal load of 440 volts, 118 amperes. Resistance between lines at 25 deg. cent. =0.071 ohms; at 65 deg. cent. =0.082 ohms. CALCULATION CONSTANTS E n = 254. X = 0.12926 Ih = 2.601 R = 0.041 Xi = 0.12926 I m = 36.7 JRi = 0.06627 X x 2 = 0.0167 e S o =249.26 £i 2 = 0.004393 PR= 143.4 go = 0.010435 Rt = 0.06377 Wx =1982.6 F =300 b = 0.14725 SUMMARY OF CHARACTERISTICS Per cent load . 50 75 100 125 Horse power . 50 75 100 125 Amperes line . 67 93 120 143 Per cent efficiency 90.4 , 91.6 91.8 9.1.1 Per cent power-factor . 81 88.8 92 92.9 CALCULATION SHEET NO. 21 448 o ft a* ft O Z o w ta -C ic t^ LO O- ^O tHOOCOCO^^+CD^OO En + lC LO LC LC lO l> I> CI IO t> C3 rooii>"^cdt>-ooo»H W ^ H; IC X! O N ^ LC * iC LO iC >C C lO lC lC lO 1> I> CI ININNN + 1 t- [^ I> I- l^ CO Tf Tf >-C CD CO I> LO LO + + li™*' LT*" LT"* Lf^ lO r> i> t> r^ i> cc d t- -1- 1- x x rn — '< r~ io - 1 - lc co CO t^ cc lo W+F W-F LCiCiCiOiOLOiOiCiO W N N N (M N (N (N N -r -t CO CO I> l> CO CO LC LC LC lC lC lC lC LT LC 'C N (M N CI (M CI N N -h OS t^ -t -f LC CI I> CO -frcrcrc-f-tCic3i'- J 1 1 I 1 1 1 1 1 1 -coaNCMr-ncco 0000000>1>»C C3 CI CI CI CI CI o X t^ CI N CI CI CI CI C, - -i Con- troller Pos. — Cl CI :c -r -f co I - X " Lewi- Arm. 2 ft. 2.292 ft. CI c 55 o CALCULATION SHEET NO. 449 22 w CO < H Ph i § r Ph' « v© J> (S P=f O Ph vo # n o ^§ o ro CO r O < £ fe CO o H CO w H W P C o H o & p 4) t) £ fc< »-lOt-i,-h0 CDOOiCKMt^i-ieOt^O^iO^CO COCO^^^h(MOOO»OOl>l?rHCO00 r-lrH0--ICOOOOOOCOO^C0«O00O5O(M-*t^000H> >-OCCOOO > ! ^iiOiOiOOCOOt^t^OO^ hooochnconhmohh OCOCOCOiOO OOlOONOOOWNNNffiO CDOO^-iCOCOOOSOSOOCD'-HOCO NQOJHNMN(MHO:05N(N t«A w2 OOOOOOiOOOOOOO OWON^OOHOiOiONOOO O^C0r-lO001>i0'-H>O-#C0 NCKNIMMHHHH >0O o 00 CO CO t-. cm CO Tf LO 1. Volts r Spool t^ -^ l> 00 CM o t^ 00 "* 00 ^* 00 -tf 00 ,_, p. CM 05 CO CM I> oo »o (M CO M lO 00 co Oi CM O CO OS cooq o H CO z ►J cn «3 CO CM 00 CO OS «- ' t> lO OS co c a> TJH O CM OS CO Ci CM lo OS 3 O O X LO LO -t CO CO — i CM cm O OOO LO O CM O co cm x x co as o cm lO COCOCO '-< LO CO CO CM rH CM CM r-t CM —I CM o o CO io -rf CO -h CM OOO Tf CO CO CO lo lO ^h CM CM O O OOO X o O X CO CT> OJ O CM CO CO CM to lO CO CO i-i CM -h CM CM h CM o o "t iO CO CO iO o lO CO CM iO ^ CM iO O X LO X -h — CO CM O OOO C3 O CM CM lO -t CO CO CM ^ CM CM la |i& |l& |1& oooo Koooo Pdoooo P^oqoq ">N SPTPiTCT NO 24. ft w '£ C P4oQOO CALCULATION SHEET NO. 24 451 MOTOR CORE LOSS AND SATURATION ON A 1000 KW., 600 V., 8-POLE, 375 R.P.M., 6-PHASE SYNCHRONOUS CONVERTER Direct Amp. Arm. Core Loss Volts Volts Arm. Amp. Field Speed IE I 2 R Arm. and Friction A-C. . Side 258 54 2.36 375 13920 30 13890 179 273 51 2.50 375 13910 20 13890 188 300 49 2.81 375 14710 20 14690 210 348 44 3.3 375 15300 20 15280 240 415 39.5 4.05 375 16400 10 16390 288 452 38.5 4.45 375 17400 10 17390 309 503 37.6 5.24 375 18900 10 18890 350 565 37 6.22 375 20900 10 20890 389 600 37 7.12 375 22200 10 22190 421 630 37.9 7.89 375 23850 10 23840 439 660 38.1 8.88 375 25100 10 23090 462 687 41.1 9.8 375 28200 10 28190 479 BRUSHES 600 35.5 7.1 375 21300 D-c. down, A-c. up 600 33.5 7.1 . 375 20100 D-c. up — (except 2), A-c. up 600 35.1 7.1 375 21050 D-c. up — (except 2), A-c. down D-c. brush friction — 1200. A-c. " " — 950. Total friction windage from curve 11800. Res. of armature at end of C.L. =0.0088. CALCULATION SHEET NO. 25 452 c 9, n^n^oo»coo^^ 0.2 ^^N00O33OH03 00 00 00MXO:0C3:^.00 00 ^m 3i2 CDOOWCONiO»00>0 ©x©i-i 10 oi co co co CO i- c x :i - i- 32 oi Lt po i — — M oj co oooooooooo ^'-CH^OCMOIOO NOJOONOCCXSCOOO ~> io^>aicocoair-iTfiooi> H r-l H N N (M CO •d o QJ p, ^cN'tCKNccDCOOCOOOO CD N N N 30 X C 1 , 35 O W as X N N iC C cqosb-b-<3»cco5TiH i-i cm h i-i i-h CM CM CO CO to 2? a«2 »o io t^ x co co NiQcOO-tXi-OXOJN m ro»oo6ai'-Hco»oi> t^' 05 > ^CON(N(MOOO>00«l t^ I> l> t> t^ I> b- CO CO CO NOiQOOOiC^W©'* OOCQMNHOOffiOOCO t^ t^ l> t^ O I- t^ co co CO Amp. Shunt Field O LO CO O X lO CM O iO O COCOCOCOMMCNCNt-^^ EN CM CM IN Ol CM CM 01 CM CM g oooooooooo q a d* CN^^iO»Ob-00O x co lo — co x m co ^h ci co -rf co cr. o oi -t -o cr. ic Ji U3 U3 l.0 iO l.0 >0 iO >0 u6 lO CALCULATION SHEET NO. 26 453 >0(M(M(M»00^0010 0005rHCq^COCCl>0000050 rHi-HrHT-lT-li-li-lr-li-ICQ OCOOCOOCD(MOOO(MCOO X^(MH0300NOCOCO(MIO (MOO^OJ^CDOCOMOOOO onooNOfflmoacooo r-it--C0I>C0»O00i-ii-tCOCO00 ioooio»ooo OCXMCOOOOOTtHcDOOOOOXM^ dddddddddddo COOiOOOiOOOO(NCO^»0© CBOOOHH(N(N(N(N(N(M NO(MON00OiO00OcD(M COt>-Oia>0»Oi-HCOt>.(NI>OOM Amp. Motor lOiOOOiOiOOOiOOiOO (MHO3500NCO>OT) ' *« v **Sfe*' - ****** x ^ W ,0* ^ * * * « / ,# I ^ **> s, - S Xi. - oo \0o. / v^ ^ • LIBRARY OF CONGRESS 111 029 827 700 1