. 'M. * W IS. jZ f Vefticai J^orce Ma^iet a/iJ t/w Bararn.e(jer rroni, m9 Feb? JG. 0 tx> F// //. 0. n Solnr Ti/nt'. Greenwich Ma^neti/xil aiuL Mp-O'i rvlogtcal Obsen'olion^s , ISJ/J . 'Plate ■*!§ ^ Si >V C<> • ' ' • ‘ Harorncter y- ' 4 ■ 4 ir ■umiiKiirnnnii li ^//rV n Pliolvfjmpliic Rfrorr/ of (fu chancjes of i/u I fi<' Roy‘f(l Oh.s'cox'a loTy , (jr'octiH'tcIi , ('t-caiwith (Trexnmcli Maff^xOral and J'Jpti'orolfjjicu I ()lMer\ atun.s , JS'jj . fUl, :i ’_Jiiill) rh( i‘invii(c((T (Jiif/ Diy^ Bad) riicfnioifKlf'/' dm MB Bf/ iS.BB u> Frd iC. zy. ‘('inr 'll HU'. DESCRIPTION OF THE GALVANIC CHRONOGRAPHIC APPARATUS OF THE ROYAL OBSERVATORY, GREENWICH. [Foi'ming the Appendix to the Greemmch Observations^ 1856 . ) LONDON; PRINTED BY GEORGE EDWARD EYRE AND WILLIAM SPOTTISWOODE, PRINTERS TO THE QUEEn’s MOST EXCELLENT MAJESTY. FOR HER MAJESTY’S STATIONERY OFFICE. 1857 . DESCRIPTION 01<' THE GALVANIC CHRONOGRAPHIC APPARATUS OT* THE ROYAL OBSERVATORY, GREENWICH. The practical introduction of Galvanic Chronographic Apparatus, in a form available for the purposes of an Observatory, is entirely due (so far as I am aware) to American Astronomers. The history of its successive steps of advance in the United States is given, with due reference to official documents, in the Annals of the Astronomical Observatory of Harvard College, Vol. I. Part I. It was from a letter of Dr. Locke to myself, dated 1849 , January 13 , that I first became acquainted with the system pro- posed by that gentleman ; and from a letter of Professor Mitchel, dated 1849 , July 10, that I received details of Professor Mitchel’s method, though I was aware that his attention had been for some time directed to the subject. The method of Dr. Locke contemplated the keeping a galvanic battery in constant action during those portions of time in which no signals (whether for clock-seconds or for moments of observation) were exhibited ; the battery-action being suspended for the instant in which the signal is given. Professor Mitchel’s method employed the battery only for giving the signal. This appeared to me preferable, both for diminution of the consumption of battery-elements, and for the superior distinctness of the signal. The fillets employed by Dr. Locke appeared to me entirely inapplicable to the uses of an Observatory, where more than 500 feet would be required for a single evening ; they are not, however, essential to his principle. Professor Mitchel’s specimens exhibited the second-signals as dots in a radial arrangement, the measures of time being taken along the circumferences of successive circles, and thus representing equal portions of time by different measures of space, according to the radius of the circle on which they fell. This appeared to me likely to lead to inconvenience ; it is not, however, necessarily connected with the system. B 2 [iv] Description of the Galvanic Chronographic Apparatus On reviewing these matters, it appeared to me that the objeets to be obtained, in order to make tlie principle of chronographic registration useful at the Royal Observa- tory, must be the following : — 1 . The record must be made by dots or punctures, following each other in a spiral line upon a sheet of paper wrapped round a cylinder, which revolves, nearly or exactly^ in a definite time of convenient period as referred to sidereal reckoning. 2. jSIeans must be provided for interrupting at pleasure that movement upon which the sequence of spirals depends, and at the same time interrupting the action of the galvanic battery, in order that paper may not be unnecessarily consumed Mhen obser- vations are discontinued. 3. Means must be provided for distinctlj’- separating the records of observations made before and after such discontinuance. 4. An important result would be attained if the regulation of the movement could be made so perfect, that the instrument itself, while maintaining the motion of the barrel, could itself be used as transit-clock, 5. Supposing this object to be not attained, it is still very desirable that the barrel revolve with great uniformity, in order that the punctures of different turns of the spiral corresponding to the same second of transit-clock-time but in different minutes, should be arranged in a straight line as nearly as possible parallel to the barrel-axis, for the sake of focility of reading. With these guiding principles, the apparatus was arranged in the form which I now proceed to describe. Figure 1 is a view of the whole apparatus from the south. (The dial-plate of the clock faces the east.) It is to be remarked that the barrel is protected by a jointed case of plate-glass, and that the clock and the pendulum are inclosed in boxes whose sides consist of glass pannels, and thus the whole which is represented in Figure 1 is actually at once visible to the eye, except only a part of the pendulum-suspension, which is indicated by dots. A is the cast-iron platform which supports the whole of the apparatus except the pendulum. It is an inverted tray, strongly ribbed ; its upper surface was planed by the planing-engine. The height of the upper surface above the floor of the room is 3 ft. 4 in. B,B, are two of the four posts which support A. They are connected by diagonal braces below the range of this view; C is a box, through MRich the clock-weight descends. D, D, two standards, whose pedestals arc screwed upon A, which support the anti- friction wheels on which the pivots of the barrel rest. E, the Great Barrel, revolving in 2 minutes of sidereal time. It is of brass, and is covered with a layer of woollen cloth. A sheet of paper is wetted, and in this state is OF THE Royal Observatory, Greenwich, [v} wrapped round the cloth, and its folding edges are united by cement ; when the paper becomes dry, its surface is tight and smooth. To remove the paper, the cemented edges are wetted. Six similar barrels are provided, in order that when one is fully charged, another may be substituted for it without delay. F is the toothed wheel of 300 teeth upon the eastern end of the barrel. G, G, two standards which carry the support of the pinion that drives F, the two guides of the sliding pricker-frame, the two long screws which give motion to the piicker-frame, and the apparatus for ungearing the long screws, and for suspending the galvanic action. H, the pinion of 30 teeth, revolving in 12 seconds, which drives the wheel F. It receives motion from the clock. I, the spindle of H. It is not a spindle of a wheel of the clock, but is connected with a spindle of a wheel of the clock in the same line by a clutch, which acts at the beginning of the connexion by friction, and finally makes a firm union. J, J, the two guides of the sliding pricker-frame. K, the upper of the two long screws by which the pricker-frame is made to travel. The screw-thread is removed from a few inches of that end of the screw which is visible in this view, in order that, if from inadvertence the revolution of the screw should be permitted to continue after the arrival of the pricker-frame at the west end of the screw, the power of the screw to continue its longitudinal motion should cease, and there should be no danger of breaking the frame of the instrument. L is a balanced winch for occasionally turning the screw K by hand, when it is not connected with the clock. M, M, is a spindle of a wheel of the clock, connected with K, when necessary, by a clutch. It revolves in ten minutes. N is the lower of the two long screws. It is connected (as regards rotatory motion) with K by toothed wheels on the outside of the vrestern standard G, so that it necessa- rily revolves in the same time as K. 0, O, is the wooden frame of the box of plate-glass which covers the barrel. 1 , P, &c. aie brass hinge-pieces screwed to the plate-glass with intervening layers of vulcanized caoutchouc. Q, Q, two handles fixed in the bottom of the lower piece of plate-glass. To open the box, the lower plate is turned upwards and over till its handles Q rest upon the upper plate, and then the two plates are turned up together into a vertical position, in which they are retained by a wooden hook, omitted in this Figure, but shown in Figure 2. R is a system of four galvanic wires, by which power is given to the two galvanic magnets wdiieh drive the two prickers that make the punctures on the barrel. Two of the wires with one magnet have relation to the circuit which is completed at every second b}'- the action of the transit-clock, and thus, by means of one of the prickers, impress on the barrel a puncture at every second ; the other two are in the eircuit which is completed by the touch of the observer’s finger, and thus, by means of the other [vi} Description of the Galvanic Chronographic Apparatus pricker, impress on the barrel a puncture at the instant of each observation. (It will be mentioned below that two wires, acting by one galvanic magnet and one pricker, are sufficient for both those offices, but that four wires and two prickers are convenient.) The wires pass over fixed bearers near the ceiling of the room, while their lower ends partake of the motion of the frame carrying the galvanic magnets and prickers, as it slides from one end of the barrel to the other. The descriptions attached to the four wires correspond to the nomenclature of attachments in the map of wires, &c. preserved in the Observatory. S, a piece of wood attached to the ceilmg of the room, with four rounded openings through which the wires pass. T, a wooden case inclosing the four wires in their descent to the floor, on their way to the batteries in the basement, and to the subterraneous passage to the transit-room. One of them rises again to the gearing-rheotome X, and again descends through the |loor. V, the observation-rheotome, or small apparatus for interrupting or completing the circuit of the observation-current. There is a similar apparatus, the transit-clock- rheotome, beneath the platform A (not shown in the plates), for interrupting or com- pleting the circuit of the current produced by the beats of the transit-clock ; this is employed in the operation of ruling lines upon the barrel E. W is one of the transit-clock- wires, which, having been led from the contact-spring in the transit-clock, rises up through the floor to the gearing-rheotome X. X is the gearing-rheotome. It is so connected with apparatus, to be described below, that the same movement which puts the long screw K in connexion with the clock- spindle M, does at the same time complete the circuit through X ; and when the con- nexion of K and M is broken, the circuit through X is also broken. The other wire which descends from X through the floor is not seen in this view. The details of the clock will be described in the explanation of subsequent figures, Y is the wooden frame of the glass case of the clock. Z is the vertical spindle which is put in motion by the clock and revolves in two seconds. a is the radial arm carried by Z, moving in a horizontal plane and acting on the pendulum-spike h. b is the stone pillar which rises through the room to support the northern pivot of the polar axis of Shuckburgh’s equatoreal in the room above. c is the large cast-iron bracket which carries the suspension-piece of the clock- pendulum. It embraces two sides of the pier b, and is fixed to each side by a single strong screw. d is a flat iron plate sliding upon the top of c, and adjusted horizontally by three screws, of which two are seen in the view. The suspension-piece of the pendulum is attached to its lower surface, and passes downwards through a large opening in the horizontal part of the bracket c. OP THE Royal Observatory, Greenwich. {vii} e, a case inclosing the pendulum-suspension. f, the suspension arches of the pendulum, to be described hereafter. The suspension- apparatus permits the pendulum to move in every direction. g, the pendulum ; it is a compensation pendulum, with steel rod and quicksilver in an iron cistern. Upon the steel rod there is a small sliding weight, for adjustment of rate. h, the spike at the bottom of the pendulum cistern, on which the radial arm a of the clock acts ; by this action the circular motion of h or the conical motion of g is main- tained. i, the wooden frame of the glass case which incloses the pendulum. Figure 2 is a view of the apparatus from the east side. k shows the position of the plate-glass-covering of the Barrel, when it is opened. 1, a wooden hook, for retaining the plate-glass in a safe position. in, the dial-plate of the clock ; it shows hours to 24, minutes to 60, and seconds to 60. The seconds-hand travels with a uniform smooth motion. n, a small slider guided by two screws, partly hidden in Figure 2 by the dial-plate, but exhibited completely, and on a larger scale, in Figure 2 Its explanation will be best understood from the following : — Figuie 2 (^), the slider n as seen from above. In the process of ruling lines on the bairel, it is necessary to slide one of the clock-spindles lengthways, so as to ungear or detach its wheel from the pinion in which it acts. By withdrawing a locking-lever at the distant end of the spindle, the separation is permitted 5 and by pushing forward the slider n or o, whose inclined end acts on the near end of the spindle, the spindle is forced endways, and is letained in the position to which it is so forced ; and the separation of the wheels is thus effected. ^ p, a lever, by pushing which in the longitudinal direction of the barrel-axis, the circuit is completed at the rheotome X, and at the same time K is put in connexion with M ; or, by pushing in the opposite direction, the galvanic circuit and the spindle connexion are both broken. The lever is seen more completely in Figures 12 and 14. q, a small piece of wood, attached by a hinge to the wooden frame of the cover of the barrel. When it is lifted, the lever p can be moved from one position (as that of completing circuit, &c.) to the other position (as that of breaking circuit, &c.), or mce versa ; but when q is dropped, the lever p is retained immoveably in the position (which ever it may be) in which it is placed. It is seen more clearly in Figures 3 and 12. r, s, two brass cylinders attached to the clock frame, carrying two glass cylindrical vessels nearly filled with water. t, V, two silken cords, passing over pullies. Their upper ends are fastened so as to act horizontally on the frame of the “ intermediate wheel ” in the chronometric governor, and their lower ends sustain weights in the water (conical cups carrying {viii} Description op the Galvanic Chronographic Apparatus shot), the preponderance of one of which over the other defines, in the chronometric governor, the power which maintains the conical movement of the pendulum g. Figure 3 is a representation of the apparatus as viewed from above. w is a piece of plate-glass covering the greater part of the large opening in the back part of the roof of the box covering the Barrel. X is a narrow opening which is left for the system of wires R to travel along, as the pricker-frame travels from one end of the barrel to the other. A portion of the pricker-frame is seen imperfectly through w and x. y, y, two screws acting in the plate d, and supporting the two primary suspension- springs of the pendulum. They are visible in this view through holes in the plate which covers d. z, a small piece of wood attached to the box by hinges, by lifting which the gearing- rheotome X is discovered. Figure 4 represents the principal train of the clock, as viewed from the east. a is the wcight-line-barrel. h is the weight-line (a wire-rope). It supports the weight by a sheaf of two pullies (a single pully also being attached to the lower side oi the platform A), and lises into the clock at c. The tension upon b is about 21 lbs., and it descends 8-4; inches in one hour. c is the rising part or return of the weight-line. It is attached to the going-lever m, on which it acts with a tensile force as nearly as possible equal to that with which h acts upon a. d is the barrel-ratchet of 48 teeth. e, e, the barrel-clicks, their centers of motion being on the wheel h. f the going-ratchet of 80 teeth, forming part of the wheel h. g, the going-click, whose center of motion is in the fixed clock-plate. h, the barrel wheel of 96 teeth, revolving in 2 hours. i, the pinion of 32 teeth, in which it works. ;, the second wheel of 48 teeth revolving in 40 minutes. k, the lantern pinion of 12 teeth in which it works. /, the sliding-frame which carries the center of motion of i andy. m, the going-lever, on which the tension of the return of the weight-line c acts. 71 , the center of motion of 711 , fixed in the clock-plate. 0, the guide fixed to the clock-plate, in which the end-rod of I slides ; the other end of / being jointed to the lever m, and therefore requiring no guide. The action of the lever in, slider I, and click g, is the following. As the clock con- tinues going in the ordinary Avay, successive teeth of the ratchet pass undei the click g*. The slider t is kept in position by three forces, namely, the pressure of the teeth of OF THE Royal Observatory, Greenwich. i" ix 1i against the teeth of i (as produced immediately by the weight-line (5»), the reaction of the teeth of k against those of /, and the pressure of the lever m (produced by the return of the weight-line c), acting to thrust the slider endways. The position taken by the slider under this action is definite ; as, if it slide too far to the left, the moment of the action of c upon the lever m is increased, and tends to bring it to the right ; or the contrary, if it is too far to the right. But when the winch is applied to Avind up the cord, the pressure of h upon the wheel h ceases entirely. The pressure of c and m continue, and the portion of this pressure which is throAvn upon the teeth of i pushes the wheel Jb backwards, till a tooth of f lodges against g. Then the rotation of k is kept up by the action of the teeth of /, in the movement which is caused by the pressure of m upon the slider /, and which carries I towards the right, the wheels i and j at the same time revolving in the bush which is fixed in 1. The effect of this movement is that the Avheel j does for the time revolve round that tooth which is in bearing on the teeth of the Avhecl h (iioav firmly fixed) ; and thus revolving, it maintains the motion of k as in the ordinary state. The line c during this time is descending. As soon as the pressure of the hand on the Avinch is relieved, h presses i and I to the left ; and, as the moment of the action of c cn m has been diminished by the change of position of m, the pressure of h on I overcomes it and forces the lever m to the left, raising the cord c, and restoring all to their original state. It Avas intended at first to use a smaller pinion for ^ and a larger Avheel fory, Avith the purpose of making the barrel a go for 8 days ; and the lever ?)i and guide o Avere accom- modated to this. But it AVRS found that an inconveniently heavy Aveight Avould be required, and the Avheels Avere so changed as to make the barrel go 2 days only. pis a wheel of 70 teeth revolving in 10 minutes. The spindle of this Avheel is M, which is connected bv a clutch Avith the lonq- screw K. 7, the pinion of 7 teeth in Avhich p acts. r, a wheel of 40 teeth, revolving in one minute. This Avheel carries the seconds- hand. s, the pinion of 8 teeth in Avhich it acts. if, a contrate Avheel of 48 teeth, revolving in 12 seconds. The spindle of this wheel is connected by a friction-clutch Avith I, the spindle of the large pinion H, Avhich acts in F to drive the Barrel E. It is upon the near end of the spindle of t that the slider n or o acts. When the locking lever at the distant end of the spindle (to be hereafter described) is removed, and the slider n or o is forced, the contrate wheel t is pushed out of its gearing with the pinion u, but s is not detached from gearing with r, nor H from F, and thus the Barrel can be turned with great rapidity without any interference with the movement of the pendulum or the wheels immediately connected with it. «, a pinion of 8 teeth with vertical spindle, revolving in 2 seconds, a fly attached to u, consisting of a bar loaded at its extremities, a bevelled wheel of 50 teeth on the same spindle. Gueenwicii Obsek\wtion.s, 1856 . — Appendix. ^ {xj Description of the Galvanic Chronographic Apparatus the flat friction-plate on the same spindle. It receives the friction which, in a modification of the chronometric-governor, regulates the expenditure of power, and leaves a uniform force to act on the wheels that maintain the rotation of the pendulum. y, the bevelled “ intermediate wheel” of 50 teeth. Its center of motion is carried by the moveable frame on which the fine cords t and v act. In rotation round its center, it is driven by w. z, a bevelled wheel of 50 teeth attached to the vertical spindle Z. It is driven hjy. «, «, a, three anti-friction wheels which support the upper part of Z. One of them is carried by a spring. i6, the cock which carries the upper pivot of u, a:, and w, the lower pivot of Z, and the center of motion of the moveable frame that carries the center of motion of y. It will be remarked that there is no connexion between w and except by the action of the “ intermediate wheel ” y ; and that iv and 2 ; revolve in opposite directions. y, the arch-head of the moveable frame, with a groove in which the cords t and v act. A hole which is seen in /3 is made for the purpose of allowing the end of the arch- head to pass freely through (3. £, a cup loaded with a piece of lead, connected with the arch-head by a flexible spring, and travelling by means of a wheel upon the curved lever. e, the curved lever, to be described hereafter. K, the near or eastern pivot of the curved lever. The axis of the curved lever is in the direction perpendicular to the clock-face. is used in other figures to denote the distant or western pivot of the curved lever, a counterpoise for the curved lever. 0, the pressure-pin fixed in the lower side of the curved lever. This pin presses upon the friction-plate .r. The amount of its friction depends on the position of the arch-head y and the weight S. When S has travelled so far upon the curved lever as to be far removed from the axis of which '( is the pivot, the pressure of S upon the friction- plate, and the consequent friction, are so great as to stop the clock. When 8 is nearly above the axis, as in the view, the pressure and friction are insignificant. 1 , I, the tAvo brass cups in water, partly loaded with shot, suspended from t and v. Figure 5 is the dial-train. X, a pinion of 12 teeth, on the same spindle as /r, p, and M, revolving in 10 minutes. A a wheel of 72 teeth, revolving in one hour and carrying the minute hand. jj. a wheel revolving in 24 hours and carrying the hour hand. No further explanation is necessary. Figure 6 is a view of the upper or regulating part of the clock, from the south. V is an index, pointing to a graduation upon the arch-head, which gives a measure of OF THE Royal Observatory, Greenwich. (xi] the position of the arch-head, and of the consequent position of the weight S, and of the friction which the pressure-pin 0 produces on the revolving friction-plate x. Figure 7 is a horizontal plan of the regulating part of the clock, ^ is the western pivot of the curved lever. Figure 8 is a horizontal plan of the friction-plate and curved lever only. Figure 9 is a horizontal plan of the arch-head and parts connected with it only. The action of the regulating-part may now be explained. It must be understood that the weight hanging on the cord v is greater than that hanging on the cord t. Let the excess be W. This will have the elfect of pushing the center of the intermediate wheel y towards the south with a force n x W, where n is the proportion of the radius of the arch-head to the distance oiy from the center of the arch-head. In the ordinary state of things, with the arch-head resting tranquil, there must be a pressure — exerted by the teeth of w upon those of y, and a pressure — g — exerted in the opposite direction by the teeth ofy upon those of which implies a pressure of ” exerted by the teeth of 2 ; upon those of^ in the same direction as the first ; and thus all the forces sustained hyy balance. But as we cannot assert that the magnitude of the weight acting upon the barrel a is such as to produce exactly the pressure — 2 — the teeth of w, we must apply a Aveight to the barrel which will, unless it is reduced, produce a force greater than - 2 — the teeth of w, and we must have some means of reducing that 91 X force on the teeth of iv to the value — 2 “’ '^'he means of reducing is given in the friction of the presure-pin 0 upon the friction-plate x, produced by the weight S. The arch-head therefore w^hen tranquil must rest in one certain definite position, which draws the weight S to such a position upon the curved lever, that the pressure of the pressure- pin 0 upon the friction-plate x exactly consumes the excess of force derived from the t X W weight-barrel, and leaves the due pressure — 2 — 3,ct on the teeth of y. Suppose now, from inequality in action of the weight-line on the weight-barrel, friction in the train, resistance of the Great Barrel, or any other cause not higher in the wheel-work than w, the force which acts on w; is suddenly increased, so as to accelerate the revolution of v, ?x, and x. The rotation of 2 ^ will not be immediately affected, for it is connected by the arm a with the heavy pendulum, whose inertia is very great. Consequently the acceleration of the rotation of v, w, and 2 ;, will carry the wheel y and its center towards the north, or the arch-head towards the south ; it will therefore draw the weight 8 further along the curved lever so as to be farther from the axis ? ; it will therefore increase the pressure of S upon x, and the consequent friction ; and will UNIVErtSiTY OF C 2 ILLINOIS LIBRARY [xii] Description of the Galvanic Chronographic Apparatus thus reduce the power derived from the train of wheels till the remainder which acts • • • • • 7?- X W t • upon ?/ is diminished to its proper value —2 — 5 which the arch-head will be tranquil. It is easy to observe this effect by any arrangement which impresses either greater foj'ce or greater resistance on the wheel-train or Great Barrel. If the Barrel is put out of balance, by altering one of the adjusting-weights to be hereafter mentioned, the arch-head y is seen to slide backwards and forwards under the index v, the period of its oscillation coinciding exactly with the time of rotation of the Barrel. By this arrangement, therefore, the maintaining power upon the wheel y is sensibly constant, and that upon the arm a, which immediately maintains the motion of the pendulum, is affected by the friction, &c., only of the wheels y, z, and of the anti- friction wheels « « «. The only resistance to the motion of the pendulum arises from the resistance of the air and the friction of the suspension. The inclination of the pendulum-rod to the vertical soon becomes such that these forces balance ; and will frequently remain sensibly unaltered during many hours or days. It is, however, much affected by small irregularities in the friction of y, 0, &c. When we wish to increase the inclination of the pendulum, which is to be done by increasing the maintaining power upon the wheel y, the process is, not to alter the weight upon the barrel-line (supposed to be great enough or greater than is absolutely necessary), but to put a small shot into the northern cup i. This overcomes the force actually exerted by w upon y, draws the arch-head towards the north, and causes S to travel along the curved lever so as to diminish the pressure of fl upon x, and the con- sequent friction ; and the force exerted by w upon y gradually increases till it becomes equal to the new or increased value of — after which the arch-head remains quiet, as before. The object of suspending the cups 1, 1, in water, is to impede the sudden movement of the arch-head (which implies an irregular motion cither of the pendulum or of the Great Barrel) without offering the slightest impediment to its slow movement. Figure 10 is a horizontal plan of the upper part of the clock, showing the radial arms, &c. Four arms are represented, of which two are mere counterpoises to the others. They have been planned with different intentions. The straighter arms, whose concave sides precede in the ordinary motion, were so shaped in order that the action of the pressing surface of a upon the spike of the pendulum, friction included, might be truly in the direction of a tangent to the circle described. The more curved arms, whose convex sides precede, were so shaped in order that, when the inclination of the pendulum is large, the friction might have some effect in diminishing the resolved part of the force OF THE Royal Observatory, Greenwich. {xiii} of gravity on the pendulum (which, at large inclinations, is too great for isochronism) ; the arrangement has not been sensibly beneficial. The small projections from the sides of a are lumps of solder which have been affixed for the purpose of measuring degrees of inclination of the pendulum-rod. The inclina- tion usually maintained is about 3.^-°. Figure 1 1 is a perspective view from below of the suspension of the pendulum. arc two pieces of split metal, connected with the suspension plate d, through Avhich the primary suspension-springs pass. These springs, however, are not supported by 0, but by two screws y y, represented in Figure 3. TT, TT, the two primary suspension springs. p is an arched piece of brass suspended by v, tt. 0 - is a piece of brass arched in the opposite direction, and, as regards its horizontal plan, at right angles to p. It is firmly connected with p, and is in fact cast with it. It supports the secondary suspension-springs. T, r, the two secondary suspension-springs. u, an arched piece of brass, suspended by r, t, in which the pendulum rod g is fixed. The attachments of the springs are so adjusted that the top and bottom of the secondary springs are at precisely the same height as the top and bottom of the primary springs. It is evident that, by the combination of the flexures of the two pairs of springs, the pendulum is free to move in all directions, exactly as if it were suspended from the point -which is the intersection of the line joining the top of tt tt, with the line joining the top of r t. The pendulum, in its motion, always turns the same side towards the north. Figure 12 is a view, from the south, of the mechanism between the clock and the Great Barrel.
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