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CHICAGO: The Jewelers' Publishing Co. 1884. 5^^ .Q'' Entered accovdinR to Act of Congress, in the year 18S3. by C. C. PIEBCE, in the Office of the Librarian of Congress, at Washington. PREFACE |fi[E DETACHED LEVER ESCAPEMENT forms one of the most interesting and important subjects for study in the whole range of the horological art, and is at the same time one of the most ditticult to treat fully, com- preliensively, and in such manner as to be easily understood. Realizing the paramount impdrtance to the work- ing watchmalier of a thorough comprehension of tlie Detached Lever Escapement, the principles of its construc- tion, the relation of its several parts and the methods of calculation Ijy which its relative proportions may be varied to produce certain results, the subscribers to the Prize Fund of the British Horological Institute resolved, in tlie month of January, 1864, that its first prize should be offered for the best treatise on this sul)j(jct. This prize, of the sum of thirty guineas, or about $150, was promptly announced in a circular issued to the members of the Institute, and at once attracted the attention of Muritz Grossmanu, then as now a resident of Glashutte, Saxony, a mem- ber of the Institute of many years standing, and a careful, painstaking, scientific horologist. He at once determined to com- pete for th» prize, the more readily arriving at this determination from the fact that he had long contemplated writing a series of works upon the several branches of practical horology, embodying the result of his experience and study, and the reception accorded this essay would serve as an index to the measure of success likely to attend such publications. Having been awarded the prize, Mr. Grossmaun, encouraged by many eminent horologists, concluded to publish the work in book form, preparatory to which he greatly elaljorated many portions of it and added the chapters on "Measuring Instru- ments," and "Materials Employed in Making Lever Escapements," thus increasing it to nearly double its original size. In April, 1866, it was published, and immediately assumed the importance of a standard text-book upon the sub- ject of which it treats. It has been widely read and consulted in this country as well as in Europe, the superior intelligence of American watchmakers enabling them to readily understand the work and appreciate its value; but the high price at which it has hitherto been held by European publishers has greatly limited its sale, while the difficulty of procuring it in large quan- tities at any price has rendered it an unprofitable publication for dealers to handle. Satisfied that a large edition, published at such a price as to place it within the reach of every working watchmaker in the country, would be appreciated by the craft, we have at great expense prepared this premium edition, and offer it to our patrons at a nominal price, making it the first of a series of technical works which, when completed, will embrace everything extant in the field of literature calculated to aid the workman in the profitable and pleasant pursuit of his calling. THE JEWELERS' PUBLISHING COMPANY, Chicago, March 1, 1884. H. A. PiiatCE, PresU TABLE OFCONTENTS. PNDEX. Page. Chapter I. Historical Notices of the Origin of the Detached Lever Escapement . 21 Chapter n. Preliminary Kemarks 23 Chapter m. General Observatioue on the Detached Lever Escape- ment 25 Chapter IV. Analysis of the Detached Lever Escapement — Its Parts and Their Various Coustruction— Classification 26 Chapter V. The Action of Wheel and Pallet 27 Chapter VI. The Action of Fork and Roller 30 Chapter VII, Combination of the Actions ^itj Chapter VIII. Description of Two Excellent Arrangements of the De- tached Lever Escapement 37 Chapter IX. Description of Some Special Constructions on Different Principles 40 Chapter X. Inetructious for Drawing Correct Escapements 43 Chapter XI. On the Respective Proportions of the Parts of the De- tached Lever Escapement and the Effects of Varia- tions in these Proportions 49 Chapter XII. Tables of Proportions 57 Chapter Xin. Procedure of Making a Correct Lever Escapement 89 Chapter XIV. On the Materials Employed for Making Lever Escape- ments 92 Chapter XV. On the Points to which the Examiner Should Direct his Attention lOU Chapter XVI. On the System of Measurement and the Measuring In- struments—Tables of Reduction lo:f DIAGRAMS. 1. A. Mudge's Lever Escapement. B. Rack Lever Escapement. 2. Lever Escapement with Ratchet Wheel and Circular Pallet. 3. Lever Escapement with Ratchet Wheel and Equidistant Lockings, 4. Pin Anchor. 5. A. Pin Anchor, jeweled. B. Pin Anchor, soUd jewels. 6. Lever Escapement with Club Wheel and Circular Pallet, visible jewels. 7. Lever Escapement with Club Wheel and Circular Pallet, improved. 8. Lever Escapement with Club Wheel and Equidistant Lockings. 9. Table Roller. 10. Double Roller and Spring Fork. 11. A. Two Pin Lever. B. Solid Impulse Lever. C. Jewel Roller Lever. 12. Enghfih Lever Escapement. 13. Lange's Lever Escapement with Analytical Construction of Lange's Improvement. 14. Resilient Lever Escapement. 15. Repellent Lever Escapement. 16. Pallet, 'Scaping over 2—5 teeth. 17. Pallet of C*' and 15° Lifting. 18. Illustration of the Procedure of Making Correct Escapements. 19. Measuring Instruments. 20. Measuring Instruments. THE DETACHED LEVER ESCAPEMENT. CHAPTER I. HISTOEICAI, NOTICKS OF THE ORIGIN OF THE DETACHED fST^^%a LEVER ESCAPEMENT. iJHE first trace of time-keeping by purely me- chanical means dates back to the Tenth centu- ry, when Gerbert, Bishop of Magdeburg (subse- quently Pope Sylvester II), is said to have constructed a clock going by weights and wheels. About the year 1370 Henry Vick, whom King Charles V of France called from Germany for this purpose, made a turret-clock, the first one of which we possess complete and positive information. Since the time of these first clocks the progress of horo- logy has been very great, but what has been done in this way has been chiefly in perfecting the escapement and the regulating parts, while the wheelwork of the train ha.s suf- fered but very little and comparatively unessential altera- tions. The invention of the pendulum as the regulating part of clocks and of the pendulum spring for portable timekeepers were the principal sources of transformation in the means employed for time-measuring. Any one who sees the clocks and watches of our day, would be inclined to suppose that the first clocks were con- structed with a pendulum as regulator, because this is evi- dently the most simple and certain system for clocks, and that the employment of the balance as a regulator has been suggested by the necessity of producing portable timekeep- ers, for which the pendulum would not answer. This is, however, not the case, for the first clocks we have any historical notices of had a verge escapement with a kind of rudimentary balance as a regulator, and the employ- ment of the pendulum for measuring the time was discov- ered nearly three centuries after the construction of Vick's clock, by Galileo. From this time clocks were made with the pendulum, but always with the verge escapement, this being the only one known at this period. This progress, important as it was, became much more so by another invention ensuing from it. The old vertical or verge escapement was very soon found unsatisfactory for clocks, by requiring too large an arc of oscillation. This circumstance led to the invention of the anchor pallets for clocks, by Hooke, about 16-50. From that time the possibility existed of employing a long, heavy pendulum with small arcs of vibration. An improvement of great value on Hooke's anchor pal- lets was Graham's dead-beat escapement, invented about the end of the Seventeenth century. Though the compara- tive value of Hooke's recoiling anchor and Graham's dead- beat escapement was a matter of earnest doubt among the most competent horologists of that time, the latter has de- cidedly superseded its rival, and is even now, in spite of all inventions of later date, the very best escapement for a good astronomical clock. 21 While these important imjjrovements were made on the ■escapement of clocks, watches were constructed mostly with the old vertical escapement. The great inaccuracy in the timekeeping of such watches, though amended as much as possible by the insertion of the fusee, created many contrivances of escapements with the principal view of giving more extension to the vibrations, and by doing so, making them more independent of the variable effect of the moving force and less liable to be disturbed by the external motion which a portable timekeeper is exposed to. Among these experiments we find a contrivance of Huy- ghens, in which the verge escapement is kept as it is, with the only difierence that the verge, instead of carrying the balance, has a wheel riveted on its axis, pitching into a pin- ion, which carries the balance. This was the first rough embodiment of the idea of increasing the arc of vibration by intervening mechanism. Another escapement witli this multiplication of vibra- tory movement is the rack-lever, invented by the Abbe Hautefeuille. It is almost identical with Hooke's recoiling anchor, but on the anchor axis is mounted a toothed rack, which pitches into a pinion forming the balance staS". This method, however, was soon abandoned, after the horizontal and the duplex escapements had been invented by Gral^ara and Dutertre. In these two dead-beat escapements the possibility oi larger vibrations was obtained, but during the excursions of the balance the tooth of the escape wheel was resting against a circular part of the balance axis. These escape- ments are very little influenced by the variations of the mo- tive force, but the tooth resting against the axis produces necessarily a considerable friction, increasing with the diam- eter of that circular part and with the extent of the vibra- tions. This friction, although diminished to the smallest amount po.ssible inthe duplex escapement, necessitates the application of oil on these parts, thus making the rate of the watch dependent on the quality of the oil and on all the changes by time and atmospheric influence to which even the best oil is subject. This occasioned the most earnest ef- forts to make the vibrations of the balance more independ- ent of the train and of the variable condition of the oil. Es- capements were constructed effecting this purpose more or less perfectly, one of which originated through taking up the idea of Huyghens and Hautefeuille of multiplying the arc of vibration by transmitting it to the balance through a-Iever. The recoiling anchor employed by Hautefeuille was converted into a reposing or dead-beat anchor. By the lever on the anchor axis the very small lifting arc of this latter was transferred to the balance in such a way as to multiply it considerably and to make all connection between these two parts cease immediately after the small arc of in- tersection had been performed, leaving the balance quite free for all the rest of its vibration. This escapement is the detached lever egcapement; it was invented by Mudge, about 1750, and it has served as prototype to all sorts of detached lever escapements known in our day. A description of Mudge's detached lever escapement will be given in Chapter V, with a diagram of its original form. This escapement was at the time of its invention not fully appreciated, for Mudge himself applied it to but two of his watches. Even at the beginning of our century it was but very little known, and the horizontal and duplex escapements prevailed for first-class watches. Since that time it has been more and more employed for better classes of watches, and has now got the better of its former rivals. Many modifications and improvements have been made on it, the most important of which will be described in the fifth and ninth chapters. 22 CHAPTER II. PRELIMINARY REMARKS. Before entering into tlie practical description and expla- nation of the lever escapement and its varieties, I think it right to say some words indicating the points of view from which I intend to treat the subject. In the first place, I deem it necessary to assume a neu- tral and cosmopolitan position, not merely dwelling on the inventions and contrivances in the lever escapement origi- nated in England and by English horologists, but describ- ing any construction of this escapement, no matter where it has been invented or kept in use. With respect to the order in which to describe the dif- ferent varieties of the lever escapement, I have thought it best to follow the historical arrangement as much as possi- ble, always fully describing and explaining those peculiari- ties which are good and commendable, and only indicating by a short description and diagram those which are of a merely historical value, and have not shown any practical advantage. In all the points where construction and calculation are concerned, I intend to take a quite different course from that hitherto in use. This deviation from the common way will be perceived through the whole extent of this treatise, and as I think this reformation of the method of measuring aind calculating the most important and useful part of it, I beg to explain here the motives that make me think so. The manufacture of clocks and watches, especially the latter, presents a peculiar difficulty by the reduced dimen- sions in which the parts of a watch must be constructed. The necessity of portability restrains the size allowed to a watch within very small limits, and even those horological i struments for which no such I'estriction would be imposed — for instance, box chronometers — are, for good reasons, very rarely made beyond a certain conventional size, which does not obviate the difficulty above mentioned. Now it is easy enough to draw any individual jiart of a watch on a large scale perfectly, according as scientific rules and good symmetry and harmony between the different parts may demand. But it is very difficult to transmit the exact proportions found in this way to the real dimensions of our work, without any essential alteration. Every oiher mechanician has the advantage that he may draw his work to the real size, and very often he is even obliged to draw on a smaller scale. Besides this, he has at his disposal measuring instruments of sufficient accu- racy to execute his work with the necessary exactness. But the watchmaker, on the contrary, cannot draw the objects of his manufacture except on a magnified scale, and those especially for which the greatest accuracy is required can only be drawn on a scale of 20 or '60 to 1, if the distinct illustration of all the particulars would be attained. The way and means of transferring the correct proportions of a good drawing to the real working size of watch-work are problems of great importance, though very little has been done till now to obtain a satisfactory result in this direction. The measuring instruments, gauges, calipers and tables for every special purpose, such as are resorted to by the majority of horologists and escapement makers, are very imperfect means. The measuring instruments are for the greater part not even of a sufficient accuracy and delicacy in their construction, and are in most cases quite independ- ent of any certain standard measure ; therefore they could not be used as a vehicle of mutual understanding on ques- tions of sizes and proportions, nor could they be employed 23 for any calculation or reduction of these sizes. The eccen- tric gauge of Roberts, for instance, though described and recomraended twice in the British Horological Journal, would be quite useless tor the two cases just mentioned. For iutercoiujaarison it would not do because it would prove a very difficult thing to construct a number of these gauges to give an identical measurement, for the slightest deviation from the true ditterence of centers, here one-tenth inch, would always produce a difference of twice the extent. For calculation or reduction it would not answer, because there is not the slightest connection with any standard meas- ure, and because the sizes measured by it are progressing in an increasing and decreasing ratio, so that it would be a very dangerous error to suppose, for instance, that the size 20 on this gauge would be a third of 60 or a half of 40. Besides, the range of sizes encompassed by this gauge is very limited, and will hardly exceed three or four millimetres when the f' '-^ion is extended up to 100 parts, and the delicacy of the division is not very great, for one degree of it corresponds to an average size of 0.04 m. The instrument is also not of a nature to be used for measuring very small and frail ob- jects, such as the ruby roller of a duplex escapement, etc., and altogether it is not to be recommended because the ec- centric principle is entirely defective for this purpose. Most of the gauges and tables now in use are made only for a certain number of cases and sizes, and leave the workman quite helpless when it is required to make an escapement with different numbers of teeth, uncommon angles of lifting and in larger or smaller sizes than usual. Besides, they are very seldom based upon scientific principles, and it is a question whether many of them are not altogether incorrect. As the Museum Committee of the British Horological Institute, by its announcement of March 20th, 1861, asked for information on the subject of a good and uniform sys- tem of measurement, beiug a member and a warm friend of the Institute, I thought it would be wrong not to give the description of a system known to me by many years' experience, and which I was sure would prove very useful when introduced into English watch manufacturing. I therefore sent in a paper, giving complete details on this subject, and for better illustration I also forwarded two nl the measuring instruments, as a donation for the museum. The paj)fr was puljlished in the Horological Journal, No. 55, March 2nd, 1863. I demonstrated in it that the pro- posed system was not only very suitable as a universal Standard of measuring in the watch trade, but more than chat, would at the same time be the means of applying mathematical principles directly to the practical execution of watchwork. Nobody will deny that though the advantages of a uni- form measurement are very imjiortant, the possibility of <»iuised U> injury, when falling into inexperienced hands, than the wheel with pointed teeth. Most of the ordinary escapements of this kind are made with a circular pallet; that is, the pallet-arms of e^^ual length, and the driving-planes at equal centre distances. There are the same reasoas for speaking agaiast this construction as already mentioned when treating of the escapement ^rith the ratchet wheel Still, the breadth of pallet-arms being considerably smaller, ajmpared to those of a ratchet-wheel escapement, the incorrectness of a circular pallet to a club- wheel escapement is comparatively less, and reduces itself in proportion to the part of the total lifting ailotteEMENT. As a sequel to the contents of the preceding chapters, we give here a description of the most advantageous con- structions of complete detached lever escapements, for the purpose of serving as a base for the following chapters, ex- plaining the respective proportions of the various parts of the escapement and the efiects of alterations in the same. The detached lever escapement, as it is made in the bet- ter English lever watches, is decidedly one of the best com- binations. We give in Diagram 12 an illustration of an escapement of this kind, standing at right angles. The escape wheel with ratchet teeth is made cf very good and hard hammered brass, and is usually polished. It would not be advisable to gild it, because by the common proce- Jure of gilding the brass would lose its hardness and elas- ticity. But even when merely electro-gilt, the thic cover of precipitated gold cannot give as hard and durable a surface as that of carefully hammered brass; and besides, nobody can be sure that the difierent chemical ingredients employed by the gilders for the processes of gilding and brushing may not be retained to some extent by the gold in such a loose state, and produce a pernicious influ'^nce on the oil. The pallet is made of steel, tempered, and has covered jewels. The lifting angle on the pallet varies from 8° to 12°. In the better English lever escapements of later days, 37 the lifting angle very seldom exceeds 10° from drop to drop, and this is the angle represented in all our diagrams. The lever is made of a thin, flat piece of steel, filed out on its sides merely to diminish its weight and give it a nice shape. The fork is the common fork of the doable roller already described, and carries on its lower side an index for the safety action, fixed to it by a screw and a steady pin. The lever is joined to the pallet by a plain staff, forming the axis of both, and by a pin fitted in a hole drilled through the lever and pallet near to the extremity of one arm of the latter. This j>iu prevents any displacement of the parts, which would, of '-'ourse, place the whole escapement out of going order. • The lever and index are tempered and the surfaces carefully polished, especially the acting parts of the fork. The balance staff has a shoulder, on which the balance is fitted and rivitcd. On the lower part of the balance staff and next to the balance a steel disc or roller with a collet projecting towards the balance is fitted, carrying the im- pulse pin. This latter firojects from the lower surface of the roller, is cylindrical, and flattened away one-third. The small detaining roller is fitted -jii the balance staff, a liitle lower than the lower extremity of the impulse pin, just to agree with the height of the index on the lever. The play of the lever is limited by two banking pins, whose place is near the fork end of the lever. In full plate watches, the pallet staff and escape pinion have their pivot holes in the tw .» plates, and may be of the full length allowed by the height of the frame. The bal- ance is hung between two cocks on the upper arid lower side of the upper plate. In i plate watches, the pallet staff and escape pinion must be brought under a small cock, to allow the balance above it the necessary freedom. Tiiey must then be very short, which is not advantageous, because the necessary side shake in the pivot holes has too much influence on the steadiness of the action. Therefore, it would be desirable to set the escapement in J plate movements in straight line because this arrangement allows a greater length of the es- cape pinion, while in full plate watches the escapement may be set in right angle just as well. This escapement, as it is used in England, may serve as a fundamental type in all the following chapters treating of the drawing, execution and proportions of the lever es- capement, and, in fact, all that can be said of this kind of lever escapement is in the same way more or less applicable to any other variety. Another arrangement of the lever escapement seems well deserving of a short description here, because it has a very good tendency to facilitate the manufacturing process and to make the parts of the least possible weight, without any prejudice to their solidity. This escapement is devised by A. Lange, and is found in almost all lever watches manu- factured in Glasshutte. (Saxony.) The escapement etands in straight line. The escape wheel is made of very hard hammered gold or aluminium-bronze, and has club teeth. The pallet and lever are but one piece, and of the same material as the wheel. The arm of the lever, opposite the fork end, which generally serves to establish the equipose, is suppressed here, and the fork arm made so thin aS to be counterpoised by the weight of the pallet. The fork end has the usual form, and the guard pin is formed by a thin pin of hard gold or aluminium-bronze \Nire, fixed into a very small square hole next to the bottom of the notch in the fork, and bent in a right angle towards the balance. The pallet has its locking faces at equal centre distances and in equal angles. The balance is compensated and hollowod out on both 38 sides to allow a little more height for the pallet arbor. On the upper side, tlie hollow is uot turned out close to the centre hole, thus leaving a pipe round this latter, to fit the pendulum collet on. 'j'^e hole, iu consequence of this, is rather long, but small ; and the balance staff is but a straight arbor fitted tightly into this hole. This saves the troul)le of turning a shoulder on both sides and riviting the balance upon it, besi'.lcs leaving the ])0ssibility of little alterations in the height of the balance staff by driving this latter a trifle further in or out. Every practical man who knows by experience the vexati jn of a balance not being Ii» proper height in an English watch, will agree that with this ar- rangement the detect is very easily removed, while in an English escapement another staff would be required. On the lower side of the balance the hollow is also not continued up to the centre liole, leaving a thicker part of the balance arm iu convenient length from the centre to receive the impulse pin, which has a triangular form. By these means the roller which in the other lever escapements carries the impulse pin, is dispensed with, and consequently the dead weight of the balance staff and the manufacturing expenses diminished A. small detaining roller completes* the ar- rangement. The banking is etiected by a pin projecting from the lower surface of the short or entrance arm, estab- lishing at the same time the equipoise between the short and long pallet arm. This pin plays iu a hole in the cock under the dial, or in the pillar plate, and the hole must be of just the size to allow the necessary freedom of escaping. This way of banking might be thought objectionalilo for the reasons mentioned in Chapter VI, but the lever in this es- capement being very thin and elastic, there is hardly any danger for the pivots and impulse pin. Besides, it has the advantage of not being liable to derangement by careless workmen, for the banking inn in the pallet is so strong as not to be easily bent. Diagram 1.3 gives an illustration of Lange's lever escapement. Mr. Lange has lately perfected the escapement in a way which deserves mention here. It is a natural defect of all lever escapements with inclined planes on the [)allet, that during the lifting action, l)y the gradual movement of the pallet, the angle in which the lifting plane stands to the wheel tooth is altered in every movement of the action. The result of this alteration is an unequal distribution of the lifting along the length of the lifting plane. When we suppose this length divided into a certain number of equal parts, the angularity performed by one of these parts will not be equal to that produced by any of the other parts. This change of position of the lifting planes would be less objectionable if it were of the same nature for both arms of the pallet; but this is uot the case. On the contrary, the angle of the lifting plane of the first arm increases coutiu- ually during the lifting action, while that of the second arm is gradually diminishing. The intended angle of lifting is performed, nevertheless, but is not equally distributed within the length of the lifting plane. The inclination of the lifting plane on the first arm will be the least at the beu'inniue of the lifting action, and that on the second arm will be greatest when the action begins. This defect may be noticed by the circumstance that in well-made lever watches, iu cases where the moving force is not suflicient, or its effect lessened by thickened oil and in- creased frictional resistance, the escapement has a tendency to set on the lifting face of the entrance arm when the pen- dulum spring is so adjusted that the balance stands right in the middle of action. To remove this defect, the ad- justment of the pendulum spring must be slightly altered. For better illustration, Diagram i:> shows an analytical sketch of the form which would be required for the two 39 driving planes to produce an equal distribution of the lift- ing action For tliis purpose, the angle of lifting, as well as the breadth of pallet, is divided into a certain number of equal parts, and corresponding to the curvature of the wheel circle, the parts of the lifting angle are delineated by arcs described with the radius of the wheel, but from cen- tres of increasing distance from the centre of the wheel. The points of intersection of the corresponding arcs indi- cate the form of the lifting faces, the first of which must be a convex curve, while the second must have a concave form. It is difficult to execute such curved lifting faces practi- cally, but the difficulties are happily sui'mounted, and it is a merit due to Mr. Lange to have invented and perfected this valuable improvement of the lever escapement. CHAPTER IX. DESCRIPTION OF SOME SPECIAL CONSTRUCTIONS ON DIF- fFEKENT PRINCIPLES. HE Resilient lever escapement is an invention of J. F. ^^ Cole, and may be considered as a successful solution of the problem of removing all the disagreeable even- tualities connected with the banking. Its principle consists in limiting the lockiug-faces on the wheel or pallet to a very small extent, just sufficient for a sound locking. The continuation of this locking iace stands at an angle to it, similar to the lifting angle, and this secondary lifting angle is for the purpose of leading the pallet back to its place of rest, if, in the case of banking, it has been pushed beyond its escaping arc. It is evident that an escapement" of this kind needs no banking pins, because by the elastic recoil pro- duced b/ the secondary lifting, the pallet and lever always return to the right place. Diagram 14, A and B illustrate the applications of the resilient princijjle most in use, the one with a ratchet wheel and the other with a club wheel. However, I do not think that these two ways of apply- ing the resilient system are the most commendable, because the inclined planes on the foresides of the teeth giving the resilient action, and the driving planes of the pallet, touch each other with very little divergence. This must result in a very detrimental influence upon the rate of a watch, be- cause if the oil is getting thick and glutinous, every approach of these nearly coinciding planes will produce a strong ad- hesion, thereby augmenting the unlocking resistance. This 40 disadvantage can be avoided by placing the resilient action in the pallet instead of the wheel teeth, in the \\'ay shown by Diagram 14 C, if a ratchet wheel is in question. With a club wheel, however, it would not be gaining anything, because the small inclined planes on the top of the wheel- teeth ^,'ould nearly coincide with the resilient faces of the anchor, thus creating the same danger of adhesion. Escapements with the lifting planes only on the wheel- teeth admit a very good resilient action if the foresides of their teeth are shaped in the way shown by Diagram 14, D. Watches with a good resilient escapement may be brought to strike violently against the banking by strong motions of the watch, or by an excess of moving power, and still there will not be the slightest exposure to any in- jury on the pivots or impulse pin, nor will they show any essential deviation in their rate, after having banked for some time. The repellent or anti-detached lever escapement of J. F. Cole is, as may be concluded by its name, quite a rever- sion of the ordinary principle. Tlie pallet of this escape- ment has the same lifting planes as any other, but the locking faces are different. They have no draw, nor are they concentric circles to the pallet centre, so as to give a dead rest ; they have on the contrary a small angularity, with a tendency to throw the pallet off, so that the escape- ment will run down if the balance be taken out. Instead of a fork, the lever has a thin pointed end, resting against the circumference of a jewel roller and giving the intpulse fo the balance, on the staff of which this roller is fixed by passing through a notch in the roller (Diagram 15) Tt is a great advantage of this escapement that it does not re- quire any safety parts or banking, and consequently it is nee of all the sources of error and failure connected there- •viih. 41 At first sight it causes a strange impression to see the greatest virtue of the lever escapement, the independence of its vibrations, thrown overboard so readily, with a view to perfecting it. Still, on close investigation, the idea is in many respects commendable, and well worth reflecting upon. The simplicity of this mechanism, and the removal of the danger of any external disturbance, are very important qualifications for its employment in pocket watches. The unlocking without any resistance is also a very val- uable economy of power, and must be esteemed so much the more, as in the detached lever escapement the unlock- ing resistance, which is one of the weak parts of it, cannot be removed. The repellent lever escapement requires also a much smaller amount of drop than the detached lever escapement, with the same safety of action, because it does not require the teeth of the escape wheel being undercut, thereby al- lowing the back slope of the teeth to be cut in a direction to leave sufficient liberty to the entering pallet arm. The only objectionable point is the friction on the roller during the excursion of the balanoe. This friction is very similar to that in the duplex escapement, but in this latter it is not supposed an impediment to good performance. On the con- trary, many watchmakers believe that a part of the super- iority of the duplex escapement is chiefly due to this fric- tion, which augments in the same rate as the moving force increases, and thus forms a kind of compensation of power. Apart from the fragility of the duplex escapement insep- arable from its nature, it would be the most resorted to of all the escapements ; and it seems that the repellent lever removes that natural defect. The chief object is to decide whether the friction of the repellent lever escapement is not greater than that of the duplex. The roller of the repellent lever must certainly be much larger thau the duplex roller, or the lifting angle would be disproportioually large. But in the repellent escapement the pressure of the lever end on the roller is but a small fraction of the force of the escape wheel, while the duplex wheel is pressing on its roller with the whole power trans- mitted by the train, only diminished by the greater diameter of the star wheel. A simple calculation will be sufficient to show tliat a comparison between the friction of both these escapements does not turn to the disadvantage of the repellent lever. To establish equal conditions for both, I will compare a duplex escapement, the imjjulse wheel of which has a di- ameter of 10 millimeters, and a repellent lever escapement with a wheel of the same size. The star wheel of the dujslex escapement of this size has a diameter of 13.0 m. and consequently, as the force is in the inverse ratio of the radius, the force with which tlie star tooth acts against the circumference of the roller is to the force of the upright teeth as 10-13, or supposing the force of the impulse wheel = 1, the pressure on the roller 10 is = rrr == 0.769. Tlie ruby roller in a duplex escapement of that size has a diameter of 0.77 m. The repellent escapement with a wheel of 10 m. diam- eter will have a middle length of pallet arm = 2.885 m. Supposing now the length of lever arm to be 3.08 m. and the lifting intended on the balance roller 40°, the diameter of this latter would be 1.54 m. or the double of the roller in the before mentioned duplex escapement. The pressure of the lever end is now to be ascertained, and we suppose the angle of the locking faces to be 10°, which ought to be sufficient for the repulsion. Tie pressure, being in the ratio of the sine of the angle, is in this case =: sin. 10° = 0.1736 (the force of the wheel always supposed =: 1). This amount is further diminished in the inverse ratio of the length of the pallet arm to the length of the lever arm. This latter being 2.885 m. and the former 3.08 m., the pressure of the lever end acting on , . , , , „ 0.1736 2.885 the circumference of the roller is = ttj^ = 0.162. Thus the pressure on the duplex roller is to that on the repellent roller as 0.769 to 0.162. The friction on both these rollei-s can be supposed in the ratio of the squares of the diameters, and as the roller of the repellent scapement is double the size of that of the duplex, is as 1-4. Therefore the frictional coefficient of the repellent roller must be multiplied by 4 to give the whole amount of comparative friction, 0.162 X 4 = 0.648 This number, compared to that of the duplex, shows clearly that the rei^ellent lever of the proportions supposed in this case is by no means at a disadvantage in point of friction. I have thought it not a«iiss to give this calculation here, because the comparison without it would be very uncertain, and might easily lead the student to underrate this inven- tion. When we consider, finally, that the repellent lever es- capement has not so much loss of power by the diminished drop of both the wheel and pallet action and that of lever and roller, and besides no loss of power by unlocking re- sistence, it may be considered as a rival to the detached lever escapement, even without taking into consideration the constructive advantage, and soundness of action. Comparing it to the duplex, and leaving the settled question of friction aside, the repellent lever has the advan- tage of giving an impulse at each vibration ; and though the transmission of the impulse in the direct way, as we have it in the duplex, be superior to that by the diagonal driving planes and intervening lever, the circumstance that 42 the duplex impulse requires fur the safety of its action a drop of about 10° before falling on the duplex pallet may be considered to make up for that deficiency. By omitting the fork and guard pin, the lever of tliis escapement may be constructed of very little weight, but it is necessary to establish carefully an exact equipoise of the pallet and lever, lest the escapement might go entirely out of action. There is one drawback, however, to this escapement. Though it will never set on the lifting, when properly made and kept in good order, it will not go on by itself when the notch in the roller stands in the centre line and the lever end is lying on the right or left side of the roller. This happens very easily, when the watch has gone down. In such cases, tlie watch requires, as well as the duplex watch, a small motion to make the balance vibrate. Diagram 15 B shows a pin anchor escapement upoa the repellent principle. CHAPTER X. INSTKUCTIONS FOK DRAWING CORRECT ESCAPEJIENTS. The correct way to draw the escapement is a very im- portant desideratum, especially for those who would like to give a solid and rational base to their endeavors in this part of watchmaking, because, for reasons best known to them- selves, practical working men do not like to undergo the trouble of developing the sizes and angles they require by mathematical calculations. For these persons the graphic way is the most convenient when any uncommon construc- tion or size of escapement is required, while for problems of frequent occurrence they may find it more convenient to go by the tables which will be found in Chapter XII For making a good and accurate drawing of a lever es- capement it is necessary to adopt a rather large scale, be- cause the lines of very small angles, as for instance 1° or li°, would nearly coincide if not diawn up to a certain length. Most of the before-mentioned diagrams are made with a radius of the escape wheel = 100 m., which is con- venient for drawing, and for the reduction of sizes. THE LEVER ESCAPEMENT WITH THE RATCHET WHEEL. Draw a circle with a radius of 100 m. in which the points of the wheel teeth are lying, and trace the line of centres a b. From this line set out to each side 30° with the aid of the protractor, and draw radii c and d to embrace this angle. These 60° form the escaping angle of the wheel, and correspond to 2* spaces between the teeth. (The wheel is 43 ahva3's supposcil to liave 15 teeth, though it might have any other number, and as the wliole circumference of a circle is — ^G0°, the space between two teeth is = -^^ — 24°). Tlu'ougli tlie two points of locking found by the intersection of the radii c and d with the circumlerence of the wheel, draw rectangular lines e and / to the radii, which of course are tangents to the circle, that is, lines touching the circum- ference but in one jjoiut. The point g, in which the tv,o tangents are crossing each other, falls into the centre line, and is the centre of motion for the pallet. The nest tiling to do is to mark the breadth of the pallet arms. This would in theory be equal to half the space between two teeth, or taking the space as 1-15 of the circumference of the wheel, 12° from the wheel centre. But in practice it is impossible to give this breadth to the arms, because no wheel can be made mathematically true in its division, and every moving part of the watch must have for the free movement of its pivots a certain shake. The points of the teeth, too, cannot be made perfectly sharp edges, nor can the slope on the back part of the teeth be hollowed out for the free passage of the delivery edge of the pallet. For all these reasons, a suiEcient quantity of drop is in- dispensable for the good and safe action of the escapement, and it will prove a good proportion to employ for this pur- pose 2° of the wheel's circumference, thus leaving but 10° of the 12° for the breadth of pallet arm. If a circular pallet is required (Diagram 2), tLdse 10° must be marked as 5° on each side of the radii c d. For forming an escapement with e-.juidistant lockings (Diagram 3), the 10° must be aj^plied to the right side of both the radii c and d. Through the points iu which the lines of these angles intersect the circumference of the wheel, the cii'cles /( and i, k and I, must be traced from the pallet centre, giving the theoretical outlines of the pallet arms. To form the driving planes, it is necessary to indi cate the angles of locking and lifting. Of the whole angle of movement (which, in all these drawings, we suppose to be 10°, though it might be more or less than that), li* must be reckoned for the locking, and the remaining 8^° serve for the driving action. Supposing the tooth on the outside of the pallet to be on the locking (which for the sake of uniformity will be so in all the drawings), the li° of the .yoking angle, as well as the 8}° of the lifting angle, must be taken towards the wheel centre on the entrance side. The lines m and n are drawn so as to embrace these angles. Pcrresponding to this position of the first pallet-arm, the d«>livery edge of the other arm must be in the periphery of the wheel, where the circle I is intersecting it. A line o must be drawn from the pallet centre to this point, and out- side from tlie tangent /the lines j) and q embracing the an- gles of 82 and li". The points where the lines m and n, and p, are crossing the circles h and i, k and /, when joined by straight lines, give the direction of the driving planes of the pallet. For the j^urpose of creating the draw, it is necessary to make the locking faces of tlie pallet deviate from the the- oretical circles h and k, which would only give a dead rest. Therefore a straight line r from the outer edge of the en- trance arm must be drawn, standing at an angle of 12° to the tangent of the circle h, which tangent is in this case identical with the radius c. The same angle of draw being required for the locking face of the other arm, a tangent s must be laid to the circle k in the inner edge of the driving plane on this arm (/ The locking face is drawn by a straight line t. in the angle of 12° to the tangent, from the inner edge of the driving plane. 44 To promote this drawing action and diminish friction on the lockings, it is necessary to give an inclination to the foreside of the teeth. An angle of about 24° to the radius will be what is required for this purjiose. The sloped back- face of the tooth must be made so as to give a solid tooth, and the lower part of the tooth may have any shape what- ever. The only thing rerpiired is to have the extremity of the tooth thin enough to enable the pallet to escape freely. For saving the trouble of marking these angles for each tooth separately', the following method is very convenient: Prolong the straight line forming the foreside of one tooth, and draw a circle from the centre of the wheel, to which this line is a tangent. Then draw from all the points of teeth straight lines touching this circle in but one point, and these are the foresides of the teeth and all in the same angle to the radial direction. The back lines of the teeth may be drawn in the same way. The delivery faces of the pallet arms are made parallel lines to the locking faces, and the rest of the outline of the pallet, which has nothing to do with the action, requires but a convenient shape. THE ESCAPEMENT WITH THE CLUB TEETH. Diagram 7 shows a club tooth escapement with circular pallet. Draw a circle with a radius of 100 m., in which the fore edges of the teeth are lying, and a line of centres a b, on each side of which set out 30° as before ; then trace the radii c and d and the tangents e and /. From the cross- ing point of these tangents, ff, which must he in the line of centres a b, draw a line v in an angle of 42° to one of the tangents, outside of the circle. These 4^° form the lifting angle for the inclined planes of the wheel teeth, and the remainder of the total lifting angle of 82° is assigned with 4° to the pallet. The outer edges of the teeth lie in a cir- cle drawn tlu'ough the crossing point of the lines v and c. The 12°, or half the s]>ace between two teeth after a subtraction of I3? of drop (Chapter V shows why with the club wheel a smaller quantity of drop is sufficient), equal to 105°, must be divided between the brcadtli of tooth and that of the pallet arm. Corresponding to their respective lifting angles, they might be made, the tooth 52" and the pallet arm 5". But this projiortion is not obligatory, and might be altered in any direction. The 5° of the l)readth of pallet arm must be set out with 21° ou each side of the radii c and d and the circles h and i, k and I drawn, as already described. The angle of total movement = 10°, leaves after the subtraction of l2° of locking, a total lifting of 8^°, divided so between wheel and pallet that the former performs 4J8 and the latter 4°. At first, the locking angle = 1J°, must be marked in- ward of the tangent e by the line m, and then the 4° of lifting by the line n. In the same way these two angles are marked on the other pallet arm outside the line 0, drawn through the crossing point of the circle I with the circum- ference of the wheel. The driving planes are drawn in the way already described. The locking faces of the pallet are made with the same drawing angle and in the same way as formerly mentioned when speaking of the ratchet wheel. The foreside of the teeth, too, is nuide witli the angle of 24" to the radius. To form the inclined planes of the teeth, set out the breadth of tooth = 5^°, to the left of the radius c; take the resulting size with the compass and mark it on each tooth to the left side. By drawing straight lines between the outer and the fore edges the inclined planes on the teeth are defined. The back of the teeth must be hollowed out in a suitable way for the free passage of the delivery edge 45 of the pallet, and the shape of the pallet made in the usual manner. (Diagram 7.) The pallet with equidistant lockings does not require this particular distribution of the lifting action, and in most cases the lifting angle is so divided that only about one- third of the total lifting is performed by the wheel teeth. In this case, the lifting will be 2it on the wheel and 6° on the pallet, and the respective breadths will be, for the tooth 3i° and for the pallet arm 7?. Draw the line v at an angle of 2}° to the tangent e, and the circle from the wheel centre passing through the cross- ing point of the line v and the radius c is the circle of the outer edges. Mark the inclined planes and fore sides of teeth in the way already described. Mark the 7° for the pallet arm to the right side of the two radii c and d. set out the locking angle = IP and the lifting angle of the pallet = 6°, and draw the circles and lines as already described. (Diagram 8.) Diagram 6 is an illustration of the circular pallet with the club wheel and the usual repartition of the lifting angle for better comparison of this way of executing with the one indicated by Diagram 7. THE PIN ANCHOR — DIAGRAM 4. Draw a circle of 100 m radius for the fore edges of the teeth, trace the line of centres, a h, and mark out on each side of it 30? ; draw the radii c and d and the tangents e and /, as before. Mark on each side of one of the radii li", double which, 25°, is the diameter of the pin. The tooth outside being supposed to be on the locking, the lock- ing angle of 1J° must be marked inside the circle by the line m, and the circle of the pin drawn from the crossing point of this line with the radius c. This done, the half of the space of 24" between two teeth must be divided. After subtraction of 2h° for the thickness of the pin and \l° for the drop, the remainder = 8? is the breadth of the tooth, Mark this angle on the circumference of the wheel to the left of the pin, and divide the wheel to give teeth in equal spaces and of equal breadth. The total angle of lifting is composed of two parts: the lifting on the inner half of the pin, and that on the inclined planes of the wheel teeth. The thickness of the jsin sup- posed to be equal to 2*° of the wheel, a lifting angle of about 2? on the anchor results from it, and the whole lift- ing angle being appointed = 8*°, the remaining 6i° must be performed by the wheel teeth. Mark this angle outside of the tangent e by the line v, and lay a circle from the centre of the wheel through the point where this line crosses the radius c. This circle embraces the outer edges of the teeth. Draw the inclined plane of one tooth, prolong the line of it, trace a circle to which this line is a tangent, and draw through all the fore edges of the teeth tangents to that circle, which give the inclined planes all in the same angle. The pin of the entrance arm standing at the locking, the pin of the other arm must accordingly be outside of the circle of the outer edges of the teeth. To mark this pin draw an arc from the crossing point of the radius d with the tangent /and set out half the thickness of the pin = li° on this arc, just outside of the outer circle of the wheel. This gives the centre of the pin. The foresides of the wheel teeth must now be drawn with the angles of draw = 15?, which is done in the way already indicated. The back lines of the teeth are made parallel to the locking face of the second following tooth, to give the an- chor pins freedom to enter into the space. The parallelism of the two lines mentioned is not essential, but it affords a 46 convenience in cutting the Avheel. To iinish the drawing, give a suitable shape to the anchor arms. THE JEWELED PIN ANCHOR. This escapement is to be draAvn in a very similar way, with the only exception that in this case the edge of the ruby pin can be made sufficiently thin as to produce no supplementary lifting angle, as the round pins in the pin anchor do. (Diagram 6, A and B). Draw the radii c and d and the tangents e and /, and inside of one tangent the locking angle = IJ", and outside of it the lifting angle = 82° by the lines m and n. Draw a circle through the crossing point of the line m and the radius c. Then set out 10° to the left of the locking radius for the breadth of tooth, leaving 2° for the drop. Draw the inclined planes of the teeth, give the foresides of the teeth the drawing angle of 15°, and shape the reverse in the way already explained. Trace the locking faces of the pallet jewels in a drawing angle of 10°, and shape the rest of the pallet and jewels appropriately. (In Figure B visible jewels are supposed, though they might be made as well covered in the usual way.) THE RESILIENT LEVEE ESCAPEMENT. The drawing of the resilient escapement, after what has been said, requires no further explanation. (Diagram 14, A— D.) THE REPELLENT LEVEE ESCAPEMENT. For drawing the repellent escapement trace the line of centres a b, and the radii c and d, in angles of 30° on each side of it. Mark the breadth of pallet arm = 101° on the right side of the radii c and d, and draw the circles h, i, k, and I. Mark the angle of locking =21° and that of lift- ing = 82° inside the tangent e and outside of the tangent /, and draw the driving planes of the pallet. Then mark an angle of 10° for the repulsion, outside of the tangent of circle h and inside of that of the circle Tc, and shape the pallet as usual (Diagram 15). The foresides of the teeth may be radial and the back slope just sufficient to give a solid tooth. THE TABLE ROLLER — DIAGRAM 9. Draw the line of centres, a b, and to the right and left side of it the lines e and d, at an angle of 5°, the sum of these angles being 10°, the total movement of pallet and lever which we suppose in all the diagrams. Mark on each of these lines the acting length of the lever by the points e and /, representing the edges of the notch in the fork. Take one-third of this length as radius and draw two arcs from the jjoints e and /. These two arcs cross in the line of cen- tres, and their crossing point t the wheel in this diagram is to that of a common size escape whtfei about as ?0 : 1. Cousequently the eSect of this increase of distance will be for a wheel of the size in the diagram = 0.9 m. When we compare now the diiference of 0.9 m. with the total extent of the arc of movement in the pallet over two teeth = 5.6 m. (See the table), we shall find that it is a loss of about i-6, or 16 per cent, of the intended total lifting effect. Escapements with a pallet scaping over three and more teeth, requiring exactly the same conditions for the freedom of their pivots, suffer of course under the same loss i.. nieclianical effect, but not so much to their disadvantage, for the alteration of 0.9 m. in the pitched distance is but 9 per cent, of the whole arc of movement of the pallet over three ^eth. The pallet over four teeth has under the same circumstances but a loss of 6 per cent., and that over five teeth li ses only 3.7 per cent, of the total amount of intended motion, by the same shake of the pivots. This diminution of the lifting eflect is, however, not so detriflaeatal as the loss on the locking. The extent of the locking arc when measured on the drawing is only 0.9 m. with the pallet scaping over two teeth, and consequently the whole locking action would be annihilated by the indis- pensable shake of the parts, and the necessity would urge a greater angle of locking. Thus the gain obtained on one side would be lost on the other. In all this, we have merely spoken of carefully sized pivot holes and carefully pitched pallets, and it must be perceived by the examples given that for a pallet over two teeth the slightest excess of shake in the holes, or the smallest deviation from the true pitch, would immediately produce the greatest irregularities in the action of the escapement, while the same defect would be of little consequence to a pallet over three teeth. In short, the pallet over three teeth is preferable, because those over more than three teeth wor k under mechanical disadvantages, further augmented by thickening oil, etc., and because the pallet over two teeth requires a greater accuracy of execution than could be af- forded under common cu'cumstances. The angle of lifting on the pallet is another very im- portant point, on which, nevertheless, opinions are very different. We see escapements with lifting angles varying from 6"^ to 12", and even more, and the question which of these angles is the best is a very natural one. Diagram 17 is intended to illustrate the effects of differ- ent lifting angles. One and the same pallet is represented with an angle of total movement of 6? from drop to drop, and with an angle of 15°. For the lifting of 6^ a locking angle of 1** has been adopted, while that of 15? shows a locking angle of li°. The lines belonging particularly to the angle of 6" are marked 1, and those referring to the angle of 15° are marked 2. The effects produced by these two extreme angularities are the foUowing: 51 The driving planes increase in length with the lifting angle, and at the same time they become more divergent from the direction in which the wheel acts. In both cases the whole power of the wheel is acting, but as the pallet with the longer arc is made to go through a wider distance, it is quite plain that the action at each point of this dis- tance cannot have the same energy, according to the great rule of mechanics that the force is in the inverse ratio to the velocity or to the distance to be })assed over. Besides, the friction on these hjuger and mure diagonal driving planes is also a disadvantage. On the other- hand, the reasons already mentioned wi'l apply here to prevent the construction of pallets with too short arcs. A pallet with 8? of total movement will re- quire the utmost rastriction of the locking angle, else th^s latter would form too great a part of the whole movement ; in consequence of which, this pallet would necessitate a very exact pitching and a most careful sizing of the pivot holes, because the least imperfection in these points would make the lockings unsafe and occasion considerable loss in the real eflect of the lifting. We liud the long arcs of movement in all the inferior classes of watches, and with good reason, especially when there are no jewel holes for the escape pinion and pallet axis, in which case a greater shake must be granted, because the brass holes cannot, for durability, be made so short or be rounded off, as a jewel hole may be. Short arcs, down to 8°, are em25loyed only in the very best and most carefully constructed watches. For escapements with the table roller it is not advisa- ble to emjjloy a pallet moving less than 10?, because the arc of intersection for the safety action is then too small to admit a perfect performance. The shape of the teeth may also be made an object of consideration. An alteration of this shape would be possi- ble by making the acting faces less inclined, and altering the back slopes accordingly. This would produce a shape similar t(> that in Mudge's escapemen' {See Diagram 1), and would be desirable by diminishing the drop which must necessarily be given to a ratchet wheel to make the delivery edges of the pallet pass freely the back slope of the tooth. But a very serious objection to such shape of teeth is that the friction on the locking would be considera- bly increased, because there would not be the point of the tooth, but a part of the acting face of it, lying against the locking face. The drawing action of the pallet would also be annihilated by approaching the acting face of the teeth to the radial direction. For this reason it is not advisable to make the inclination of the teeth less than 24° to the radius. The length of tho teeth, if the ILfting angle of the pal- let is not an uncommonly large one, may be 1-10 of the wheel's diameter. Any excess of length, especially with a ratchet wheel, would be of no use, and would put the durability of the wheel in danger. With respect to the form of the club teeth, the same considerations demand a sufficient inclination of their fore- sides. The objection of any loss of power by too much drop does not apply to the club wheel, because the possibil- ity of hollowing the back part of the tooth allows as close scaping as possible. The small inclined planes on the club teeth should be of such angle that the lifting on the pallet would be performed first, and that of the wheel tooth take place fifterwards, at the delivery edge. When the total lifting angle is divided so that its greatest part is assigned to the wheel, without giving at the same time more breadth to the teeth, the result will be that the lifting of the wheel tooth is performed first, by the inclined plane of the tooth 52 at the entrance edge, which is not so favorable as in the first method. The wheel teeth'of the pin anchor, and siraliar construc- tions, are bound, as to tlie forms of their fore faces, to the necessary drawing angle. The back part must be undercut to allow free passage to the pin during the slight recoil pro- duced by the drawing angle at the moment of unlocking. The lifting faces of the teeth may be made in dift'ereut ways. Some of these escapements have straight lifting faces, .some of them curves, although there seems no reason for a9 0.1 343 0.2753 0.1823 0.3'310 0.2107 0.3730 0.5425 0.087S 0.6774 5.0 4.95 2.89 3.76 2.01 0.77 1.38 0.01 !.(;() l.os 1.87 2.71 0.44 2.89 a.l 5.15 3.00 3.91 2.10 0.80 1.43 (i.:t.") I.(i7 1.13 l.!)4 2.82 0.46 3.00 5.4 5.35 3.12 4.06 2.18 0.83 1.49 O.'.IS 1.73 1.17 2.01 2.93 0.47 3.12 o.G 5.54 3.23 4.21 2.26 0.86 1.54 1.02 l.Sii 1.21 2.00 3.04 0.40 3.23 5.8 5.74 3.35 4.36 2.34 0.89 1.60 i.(k; l..S(i 1.26 2.1 1; 3.15 0.51 3.35 6.0 5.94 3.46 4..-.1 2.42 0.93 1.65 l.O'.l 1.93 ] M 2.24 3.26 0.53 3.46 6.2 6.14 3.58 4.G6 2.50 0.96 1.71 1.13 i.:i!i 1.34 2.31 3.36 0.54 3.58 6.4 6.34 3.70 4.81 2.58 0.99 1.76 1.17 2.05 1.39 2.39 :;.47 0.5li 3.70 6.6 6.53 3.81 4.96 2.66 1.02 1.82 1.2(1 2.12 1.43 2.46 3.58 0.58 3.81 0.8 6.73 3.93 5.11 2.74 1.05 1.87 1.24 2.18 1.47 2.54 3.69 0.60 3.93 7.0 6.93 4.04 5.26 2.82 1.08 1.93 1.28 2.25 1 ..52 2.61 3.80 0.61 4.C'4 7.2 7.13 4.16 5.41 2.90 1.11 1.98 1.31 2.31 1.56 2.69 3.91 o.o;; 4.16 7.4 7.33 4.27 5.56 2.98 1.14 2.04 1.35 2.38 1.60 2.76 4.01 0.05 4.27 7.6 7.52 4.39 5.71 3.06 1.17 2.09 1.39 2.44 1.65 2.84 4.12 0.(.. 4.39 7.8 7.72_ 4.50 5.86 3,14 1.20 2.15 1.42 2.51 1.69 2.91 4.23 0.68 4.50 8.0 7.92 4.62 6.02 3.22 1.23 2.20 1.46 2.57 1.73 2.98 4.34 0.70 4,62 8.2 8.12 4.73 6.17 3.30 1.27 2.26 1.49 2.63 1.78 3.06 4.45 0.72 4.73 8.4 8.32 4.85 6.32 3.38 1.30 2.31 1.53 2.70 1.82 3.13 4.56 0.74 4.85 8.6 8.51 4.97 6.47 3.46 1.33 2.37 1.57 2.76 1.86 3.21 4.67 0.76 4.97 8.8 8.71 5.08 6.62 3.54 1.36 2.42 l.(!0 2.83 1.91 3.28 4.77 0.77 5.08 9.0 8.91 5.20 6.77 3.63 1.39 2.48 1.64 2,89 1.95 3.36 4,88 0.79 5.20 9.2 9.11 5.31 6.92 3.71 1.42 2.53 1.68 2.95 1.99 3.43 4.99 0.81 5.31 9.4 9.31 5.43 7.07 3.79 1.45 2.59 1.71 3.02 2,04 3.51 5.10 0.83 5.43 9.6 9.50 5.54 7 22 3.87 1.48 2.64 1.75 3.08 2.08 3.58 5.21 0.85 5.54 9.8 10.0 9.70 5.56 7^37 3.95 1.51 2.70 1.79 3.15 2.12 3.66 5.32 0.86 5,66 9.90 5.77 7.52 4.03 1.54 2.75 1.82 3.21 2.17 3.73 5.43 0.88 5.77 59 The columns containing the circles of pallets require no explanation, after what has been said in Chapter V. The columns 5, 6 and 7 in Table I and 6, 7 and 8 in Table II indicate the lifting cireks. These circles will re- quire some explanation. The exact angle of inclination for the driving planes to give the intended lii'ting etteet can be very conveniently measured by the diameters of circles to which the prolong- ations of the driving planes are tangents, and in the next chapter it will be shown how to use these circles. In the tables they are for the sake of brevity called lifting circles, and their diameters are calculated for the three angles of movement: S'^, 10° and 12", as already mentioned. In Table II there are two diameters given in every column, because for a pallet with equidistant lockings the lifting circles for each pallet arm are not equal, as is the case w ith those of the circular pallet. The column 8 in Table I and 9 in Table II indicate the height of a segment, serving to determine the outer corners of the pallet. The diameter for the circle of this segment is that of the largest circle of pallet, and it must be imag- ined to be flattened away by a straight line, to show the height indicated in the table. The two last columns contain the breadth of pallet arms, which is the same for both the tables, and the distance of pitch for which the parts are intended, and which cannot be altered without making the escapement defective. • The following explanations may serve for the use of those who take an interest in the method of establishing these tables , but it may be repeated here that for the use of {he tables themselves it is by no means necessary to go through these calculations, because the tables are the results of them, and may be used by a person who knows nothing at all of mathematics. Another reason for giving these de- tailed explanations is to facilitate, to those who have had a good education, the solution of problems which are out of the common way. Besides, he who writes a book must be aware that it is dedicated to future times and to coming generations, and from all that has been said by the most competent English horologists there prevails the conviction that superiority in our time cannot be secured by mere practical skill, but on the contrary the task of our days must be to give to every workman p. good and thorough education, in order to enable him to apjily the aid of science directly to his practical pursuits. The calculations were originally made with live and six decimals, and the result shortened down to the more con- venient length of four decimals. Tliis will account for small differences that may be observed in the last decimals. All the angles in the following calculations have been rounded off, so that differences of less than 5' have been dropped, as they are too minute to perceptibly influence the working sizes. The woodcut diagrams accompanying these calcula- tions are merely meant to facilitate the understanding of the lines and augles spoken of. They serve for very dif- ferent angles and proportions, and it must be remarked here that the}' are not intended to give the proportions and angularities of each special case, but only to give a general impression of the part of the escapement just in question. TABLE I. COLUMNS ONE AND TWO. The column 2 contains the measured diameter of the escape wheel. This measured diameter is = the real diameter less the height of arc of the central angle of 24°, contained between two points of teeth. (See the dia- gram.) 60 Por a diameter of the. circle =n l,tlie height of arc of the angle of 24? is = 0.0109, of which number the last two decimals may be omit- ted. Consequently, the measured diameter of a wheel is =: the real dia- meter less 0.01, or in this case - 1—0.01=0.99. This is the ])ro]jortioiial number at tLe head of column 2. P'lir wheels of any greater or smaller number of teeth, the diHerence between measured and real diameter is dif- ferent, because the angle of 24° belongs only to the wheel of 15 teeth. d g = a d tang A. =0.5. taug- 30°. = 0.5. 0.5774.*) = 0.2887. f/(/is the radius of the locking ' circle, and con- seijuently the diameter of this circle must i)e: 0.2882=0.5774. The diameter of outer circle, as it has been previously explained, is= : 0.5774+0.0873 = 0.HH47. COLUMN THREE. The diameter of the outer circle of the (circular) ])allet is the sum of the diameter of the locking circle -|- the breadth of j)allet arm. This latter, equal to an arc of 10° of the wheel's circumference, would be for the diameter of wheel = 1 : 1 ■ :j.l41fi . 10 _3.1416 360 ~ 36 = 0.08727. The diameter of the lucking circle is found in the fol- lowing way: Given the diameter of wheel = 1. The radius a f? =0.5 coLUJix foi;k. The diameter of the inner pallet circle is, by the con- structiim of the escapement ( Diagram 2) equal to the dia- meter of locking circle less the breadth of pallet arm : 0.5774 — 0.0873 = 0.4901. COLUMNS FIVE, SIX AND SEVEN. The calculation of the lifting circles corresponding to the lifting angles 7", 8i° and 101° is the following. *The value of this tangent and of all trigonometric functions will be found in any good handbook of mathematica or navigation. 61 Of tlic triangle a h c the known jiarls are: a=^-- — = 0.3323 (nidiiis of outer circle) , 0.4901 „.,,- ,. ,. . . , 0= — - = (1.^-1.) ( radius ol inner circle) 0=7", or 8A" or 10]^. 5) < 0= 7' ^ ^^ I "^ " —90" _: := MO^ — 2 2 ■ 3° 30' = 86° 30' ^-«-(^H5^— «-5 0.3323 — 0.245 = 0J«23T():245'^"^'"'«- 30' 0.087:! cotano;. 3" 30' 0.5773 log. 873= 2.!)410* + log. c.tang. 3° 30' =11.2135 14,1545 — log. 5773 = 3.7fi]4 •In all tbesB caloulatious the oapitol letters siguify angles and the lower case letters, lines. log. tang. (A-^) = < A 10.3931 68° <^ +^ = 86° 30' 2 Hence follows: A — 86° 30' + OS" -= 15^° 30' £ = 86^ 30' — 68" = 18° 30' C(already known) = 7° — ' 180°—' (,The .sum of the three angles in each triangle.) This calculation was made for the purpose of finding the value of the angled. This angle serves now to de- tiriiiiiie the lino ;/ d in the rectangular triangle g df, of which is known : The hypotheuuse ;/ f ^0.3323. and<7?" =18° 30' yd- __^= 91) 2 2 4" l.V = S.-)° 4o log. 873 = 2.9410 + log. cotang. 4-" 1 -V = 1 1.129 14.0700 — log. 5773 = 3.76 14 log. tang./^Lzj?) = 10.3080 A—B = fi3° .")()' 2 B = 85" 45' — 63° 50' = 21° 55' g(l = f/f sm B = 0..S32:: . sin 21" 5.5' = 0.3323 . 0.3733 = 0.124047. Diameter of lifting circle - 2 . 0.124 = 0.248 7) < ^ < hg I — < I g 1= i 20° — 1° 30' (locking angle) = 118° 30'. The sides gh and g i being e(|ual, tli.> angles opjjosite to them must be equal too : ]80°— 118° 30' < g h I = < gili=^ ^ 61" 30' = 30" 45' A perpendicular line drawn from the point g to the line ///divides the triangle y /i / in two equal rectangular tri- angles. This perpendicular line does not coincide com- pletely with the line of centres (/ a, but as the divergence of the.se two lines is but ii°, it may be neglected altogether 68 in the drawing. We suppose then the point h to be the point of intersection, and the two rectangular triangles axe: ghk and gik. COLUMN NINE. The breadth of pallet arm has already been intlieated as being equal to the opening of an angle of 10° at the wheel's centre, measured at the circumference of the wheel. This breadth is = 0.0873 for the diameter of the wheel = 1. COLUMN TEN. The distance of centres can be found by the rectangular tri- angle a c g, of which we know: *" ac= 0.5 < cag = ZO° (by construction.) ac ay ^= cos. cag 0.5 cos. 30" 0.5 0:866 =0.5774. TABLE TI. COLUMNS one .and two. The real and nie.isiued diameters of wheel are unaltered. In tliese two triannles we kmnv: g h =z gi =0.3:!23. ' = (1.3192 . sin 20° = 11.3192.0.342 = 0.109166 72 Diameter of lifting circle = 2 . ffd=r.2 . 0.10916(5 = ((.2188. Diameter of lilting circle = 2 . gd = 2 . 0.157174 = 0.31-14 .1- 2 tang. Total angle of movement = 10" Locking angle = 1 2 ? Lifting angle of wheel = 2i° Lifting angle of pallet = 6° : 90" — 3" = 87'^ b --S^90°_£ i^-l _ . cotang. I = 0.1056 . cotang. 3° = 0.105(J . 1.9081 = 2.0149a till^ = 63° 35' 2 £ = 87° — 63" 35' = 23° 25' 5, £« = a. sin 5 =0.3192 .sin 23" 25' = 0.3192 . 0.3974 = 0.12685 Diameter of lifting circle = 2 . jr rf = 2 . 0.12685 = 0.2537 A+B Total angle of movement =^ 12b Locking angle =l-i° Lifting angle of wheel = 25" Lifting angle of pallet = 8° C ■ 40 = 86' 90° _ _= 902,- 2 2 U—B\ a—h , C tang.(_^)=— cotang.^ = 0.1056 . cotang . 4" = 0.1056 . 14.301 = 1.5102 :^~^_ 56° 30' 2 - B = 86" — 56° 30' ^ 29" 30' gd = a. sin B = 0.3192 . sin 29" 30' = 0.3192 . 0,4924. = 0.157174. Lifting-Circles, Table IV.— Pallet with Equidistant Lockings. For greater simplification of the matter, we shall calculate the lifting circles of the first arm for all the three angles at first, because the greater part of the coefficients are the same for all. lifting circles of the first pallet arm. Angle of movement = 8" Lifting angle of pallet = 5° a ■= 0,2887 (radius of locking-circle) h ^ 0,2279 (radius of inner circle) C=5° A ^ B C — 2^ _ 90° _ 2 = 90" — 2° 30' = 87° 30' tang / A — ^ \ ^^ a — b C \ 2 / a + b' cotang. 2 0,2887 — 0,2276 ■ ((,2887 + 0,2276' cotang. 2° 30' 73 "-"tin . 90 on' = 0,1183.22,904 =2.7095 ^i— ^ = 09"^ 45' B -.= 86" _ 59^ 25' = 26° 35' gd=a. sin 5 = 0,2887 . 0,4475 :^- 0,12919 Diameter of lifting-circle ^= 1 g d = 2 . 0,12919 = 0,2584 . B — S7° 30' — 69" 45' = 17° 45' r/ (/ = a . sin £ . = 0,2887 . 0,3040 = 0,088025 Diameter of lifting- circle = 2 g d =2 . 0,088025 = 0,176 A+ B 90° Angle of movement = 10° Lifting-angle of pallet = 6° ^= 90" _ 3" = 87? tang . \ 2 /= 0,1183 . cotang. 3" = 0,1183 . 19,081 . = 2,2573. ^^ P^ 66'' 5' 2 5 = 872 — 66? 5' = 20° 55' . g d= a .sm B . = 0,2887 . 0,357 .■ = 0,10307 . Diameter of lifting-circle ^ 2 . g d ^ 2 . 0,1030 < = 0,2061 Angle of movement = 12°, Lifting-angle of the pallet = 8° :£±^= 90°— ~- 90" t.u^A-B^^^ 4° = 86"'- 1183 . cotang. 4° )1 = = 59° 25' = 0,1183.14,301 = 1,6918 . 9 LIFTING CIRCLKS OF SECOND PALLET ARM. Angle of movement = 8° a =^ 0,34978 (radius of outer circle) b = 0,2887 (radius of locking circle) C=5" 4_+j?.= 90° — 4^ = 2° 30' = 87° 30' tang / .4 -^i; \ u,: V --i I 0,: 0,34978 — 0,2887 , O ' ' cotang. — 34978 + 0,2887 ^ 2 0,06108 , .,o ..„' cotang. 2" 30 A—B 0,63848 = 0,09568 . 22.904 = 2,19145 . = 65° 30' B = 87° 30' — 65° 30' = 22° gd = a.iim B = 0,34978 . 0,3746 . = 0,131028 74 Diameter of lifting circle = 2 . g d = 2 .0,131028 = 0,2621 .' CIRCULAR PALLET — HEIGHT OV KKtJMENT. Angle of movement =10° Lifting angle of the pallet = =0.2887 (radius of locking-circle) ^=4° .30' a =h . tang. A =0.2887. tang. 4i° =0.2887 . 0.0787 . =0.0227 . Outer diameter =. 1+2 « = H-2 . 0,0227 =1+0,0454 = 1,0454 fOLUJIN •'!. Measured diameter = 1.0454 . 0.09 = 1 .0.349 . COLUMN FOUR. The diameter of outer circle of pallet = the diameter of the locking-circle = 0.5774 . -f the breadth of pallet-arm = 0.0436 . 0.G210 COLUMN FIVE. The diameter of inner pallet-circle = the r.idius of the locking-circle ^ 0.5774 — the breadth of pallet-arm = 0.0436 , 0..5338 COLUMN SIX. The lifting-circle has been calculated merely for the angle of movement of 10°, in order to simplify the table. 79 a = 0.8105 (radius of outer circle) b = 0.2669 (radius of inner circle.) C= 4° A + £ 2 =90° — £= 90'= 2 — 2° = = 88° tang. (^ 7^. a—b a + b cotang. C 2 0.3105 - 0.3105 - 0.2669 + 0.2669 . cotang 0.0436 ~ 0.5774' cotang. 2° =0,0755. 28,636. = = 2.162 A — ^_ = 65° 10' no B = 88° — 65° 10' = 22° 50' gd = a . sin B. = 0.3105.9.3881. = 0.1215. Diameter of lifting-circle = 2 . gd. =■2.0.1215=0.243. COLUMN SEVEN. The height of segment is to be found in the same way as it has been done in the corresponding cases referring to Tables I and IV. gh = gi = 0.3105 (radius of outer circle.) < ghi =-118° 30' (by construction.) 180"— 118° 30' 61° 30' < ghi = < gih = In the rectangular triangle ghk we know : gh = 0.31 05. < ghi = 30° 45' gk = gh . sin . 30° 45' = 0.3105. 0.5113. =0.1588. The sum of the radius of the outer pallet circle=0.3105 + the line gk ' =0.1588. is the height of segment=^0.4693. COLUMN EIGHT. Breadth of pallet arm = 5° of the primitive circle oi uheel, 3.141G.5 0.1416 = 30° 45' 360 -= 0.0430. 80 Diagram XIII. \rr \H1 DiAGEAM XIV Diagram XV ^ t/\ • i ■ > ' 1 X ■1 .' \ \ '_ . i Vv\i Diagram XVI. COLUMN NINE. The breadth of the wheel teeth before making the in- clined planes, measured at the primitive circle of the wheel, is 3.1416.5.5° 3.1416.1.1 3.4.5576 360 72 72 . = 0.048 . COLUMN TEN. The tangent circle for the inclined planes on the wheel teeth. \\ \ \i a = 0.0227. b = 0.048. 0.048 = 2.1146. tang. B. = - * a 0.0227 jB = 64° 40' In the rectangular triangle dc/f there is: dg = 0.5227 . (radius of outer wheel circle) < B=-. (M" 40' (jf = d(j.m\ . B. = 0.5227. sin 64° 40' = 0.5227. 0.9038 = 0.4724. Diameter of tangent circle = 2. (/f = 2.0.4724 == 0.9448. COLUMN ELEVEN. The distance of centres is equal to that of Tables I and IV. Explanation of Table VI. Thi& table refers to the pin anchor, and though this construction is very rarely employed, and, I may say, very little known, I think it likely that some who have read the particulars of it in the fifth chapter might be desirous to try it for such purpose as it may be suitable. Therefore, and for greater completeness, a table of proportions of the pin anchor might be useful. Still, I have executed it in a simplified way, only referring to the angle of movement of 10°, this being about the average of the angles in use. With the aid of this table an anchor of this kind will not be an object of difficult execution, as it requires no jewels, nor anything beyond the reach of every watch- maker's workshop. COLUMNS one, two AND THREE. The primitive diameter is, as well as in all the preced- ing calculations, supposed to be^ 1. The outer diameter must be calculated according to the 81 TABLE VI. Pallet with I Equidistant Lockings . Ratche' r Wheel. 1 2 3 4 5 6 7 8 9 10 11 Diameter of wheel circle. 1 Thickness Breadth of Tangent. Distance Distance Diameter Height Distance of the pics. teetli moa- Burttl at the circle for the between the pins. measured across the of pin-circle of triangle. of 1 centres. ( Outer. primitive inclined outt.r sides (locking- Primitive. I.UO Beat Measured circle. planes. of the pins. circle.) 1.0658 1.055 0.0218 0.0698 0.9369 0.5171 0.5389 0.5774 0.1393 0.5774 5.0 5.33 .5.28 0.11 0.35 4.68 2.59 2.70 2.89 0.70 2.S9 5.2 5.54 5.49 0.11 0.36 4.87 2.69 2.80 3.00 0.72 3.00 5.4 5.76 5.70 0.12 0.38 5.06 2.79 2.91 3.12 0.75 3.12 5.6 5.97 5.91 0.12 0.39 5.25 2.90 3.02 3.23 0.78 3.23 5.8 6.18 6.12 0.13 0.40 5.43 3.00 3.13 3.35 0.81 3.35 6.0 6..39 6.33 0.13 0.42 5.62 3.10 3.23 3.46 0.84 3.46 6.2 6.61 6.54 0.14 0.43 5.81 3.21 3.34 3.58 0.86 3.58 6.4 6.82 6.75 0.14 0.45 6.00 3.31 .3.45 3.70 0.89 3.70 6.6 7.03 6.96 0.14 0.46 6.18 3.41 3.56 3.81 0.92 3.81 6.8 7.25 7.17 0.15 0.47 6.37 3..52 3.67 3.93 0.95 3.93 7.0 7.46 7.39 0.15 0.49 6.56 3.62 .3.77 4.04 0.98 4.04 7.2 T ii7 7.60 0.16 0.50 6.75 3.72 3.88 • 4.16 1.00 4.16 7.4 7.8!) 7.81 0.16 0.52 6.93 3.83 3.99 4.27 1.03 4.27 7.6 8.10 8.02 0.17 0.53 7.12 3.93 4.10 4.39 1.06 4.39 7.8 8.31 8.23 0.17 0.54 7.31 4.03 4.20 4.50 1.09 4.50 8.0 «..53 8.44 0.17 0.56 7.50 4.14 4.31 4.62 1.11 4,62 8.2 8.74 8.65 0.18 0.57 7.68 4.24 4.42 4.73 1.14 4.73 8.4 8.95 8.S6 0.18 0.59 7.87 4.34 4.53 4.85 1.17 4.85 8.6 9.17 9.07 0.19 0.60 8.06 4.45 4.64 4.97 1.20 4.97 8.8 9.38 9.28 0.19 0.61 8.24 4.55 - 4.74 5.08 1.23 5.08 9.0 9.59 9.50 0.20 0.(!3 8.43 4.65 4.85 5,20 1.25 5.20 9.2 9.S1 9.71 0.20 0.(>4 8.62 4.76 4.96 5.31 1.28 5.31 9.4 10.(1.; !).'.)2 0.20 0.66 8.81 4.86 5.07 5.43 1.31 5.43 ' 9.6 10.2:; 10.13 0.21 0.67 8.99 4.96 5.17 5.54 1.34 5.54 9.8 10.44 10.34 0.21 0.68 9.18 5.07 5.28 5.66 1.37 5.00 10.0 10.658 10.55 0.218 0.698 9.369 5.171 5..389 5.774 1.393 5.774 82 lifting angle peif(jriiiL'd by tlic wheel teeth, which is for an angle of 10°=6J°. /) = 0.2887 (radius of locking circle) ; A - IJ° 30' «= b. tang. A. = 0.2887. tang. 6° 30' = 0.2887.0.1139 = 0.03288 . Outer diam. =1+-" = 1+2.0.03288 = 1+0.0658. = 1.0658. Measured diameter = 1.0658.0.99 = 1.055142. COLUMN HIX. The tangent circle for the inclined planes of the wheel teeth. For such a considerable angle (8°) as is given here for the breadth of wheel tooth, the triangle a b c cannot be KUjii)osed to be a rectangular one. The angle at tlie wheel centre for the tooth being 8°, the two radii enclosing it form with the line b an isosceles triangle, of which the value >. \ i COLUMN FOUR. The thickness of the anchor pins is the primitive circle of the wheel : 3.1416.2.5 3.1416 2i°, measured at 360 144. -= 0.02182. COLUMN FIVE. The breadth of teeth, measured at the primitive circle, is = 8° of this circle : 3.1416.8 3.1416 360 45 0.0698. 83 of any of the two other angles is ^ 180°— 8° 172° =86' 2 2 Accordingly, the angle Cin the small triangle of tooth a h r being the supplement to this former, is = 180° — 86° = 94°. Thus we know of the triangle a h <■ : (I = 0.03288 (difference ot outer and primitive radius of wheel.) fc = 0.0698 (breadth of tooth.) C=94° R — ^ • «ia C* _ 0.0698 . 0.9976 tang. i> — ^^_^ ^^^ ^ 0.03288 + 0.0698 . 0.0698 0.00963 0.06068 0.03775 ' : 1.844556. 0.03288 + 0.00487 ' 5 = 61° 30' In the rectangular triangle dfi f, we know : dg = 0.53288 (radius of outer wheel circle) i=61°30' r/f =d(/.s\D.B= 0.53288 . 0.8791 = 0.46845 Diameter of tangent circle 2 . f/f = 2.0.46845 = 0.9369. COLUMN SEVEN. The distance of the jjiu.s — that is, the distance from one centre of pin to the other, is found in the following way : The triangle «7c/ is by the construction an isosceles tri- angle, the sides g c and gf, and consequently the angles op- posite to them, being equal. \ i / \ i / V The angle c y (< = 120° (by construction) < c5r/= < <-gd-{- < dgf. In the rectangular triangle d gf there is : gd = 0,2887 (radius of locking circle) df= the sum of: half the thickness of the pin = 10.0109 + the difference of outer and prim, radius = 0.03288. 004379. tang, dgf- d,f _ 0.04379 0.2887 0.1.517 < d^/=8°40' ghf'= < gfh 2 52° ,50' 26° 25' hf- gf.sm hgf _ 0.2887 . sin . 127° 10' sin g hf sin . 26° 25' 0.2887 . 0.7969 0.230065 0.4449 0.4449 = 0.5171 COLUMN EIGHT. The distance, measured from the outside of one pin to that of the other, may be useful when it is required to make an escape wheel to a ready made pin anchor. In this case the sizes of columns eight, nine and ten must serve to ascertain the diameter of wheel, proportionate to the an- chor. 84 This distance is the sum of: the line /(/, just calculated = (1.5171. 4- the thickness of one pin = 0.0318. COLtTtfN NINE. The diameter of the circle from the pallet centre, in which the centres of the pin are embraced, is equal to the diameter of locking circle in Tables II and IV,=:<).5774. COLfMN TEN. The height of triangle is the distance from the centre of the anchor to the line, touching the two pins on the side turned towards the centre of the wheel. The line g k, in the diagram belonging to column seven, is = 7/ . sin. f/fl- = 0.2887 . sin. 26° 2.V = 0.2887 . 0.4440 = Diam. of impulse. Distance Diana. Dist Diam. Dist. Diam. Dist. Diam. Dist. Diam. Dist. Diam. Dist. Diam. Dist. s centres. impulse. centi'Bs. o' impulse. of centres. of impulse. of centres. of impulse. of centi-es. of impulse. of centrss. of impulse. of centres. of impulse. of centres. 0.64 1.3124 0.533.. 1.2581 0.666.. 1.3215 0.5714 , 1.9727 0.5 1.234 0.666.. 2.00 1.3097 0,5714 1.2G67 0.5 1.2294 3.0 1.92 3.94 1.60 3.77 2.00 3.96 1.71 3.82 1.5 3.70 3.93 1.71 3.80 1.5 3.09 0.2 2.05 4.20 1.71 4.03 2.13 4.23 1.83 4.07 1.6 3.95 2.13 4.19 1.83 4.05 1.6 3.93 8.4 2.18 4.46 1.81 4.2S 2.26 4.49 1.94 4.33 1.7 4.20 2.26 4.45 1.94 4.31 1.7 4.18 8.(i 2.30 4.72 1.92 4.53 2.40 4.76 2.06 4.58 1.8 4.44 2.40 4.71 2.06 4.56 1.8 4.43 8.8 2.43 4.99 2.03 4.78 2.53 5.02 2.17 4.84 1.9 4.69 2..53 4.98 2.17 4.81 1.9 4.67 4.0 2..-)G 5.25 2.13 5.03 2.66 5.29 2.29 5.09 2.0 4.94 2.66 5.24 2 29 5.07 2.0 4.92 4.2 2.69 5.51 2.24 5.28 2.80 5.55 2.40 5.35 2.1 5.18 2.80 5.50 2.40 5.32 2.1 5.16 4.4 5.77 2.35 5.54 2.93 5.82 2.51 5.60 2.2 5.43 2.93 5.76 2.51 5.57 2 2 5.41 4.6 2.94 6.04 2.45 5.79 3.06 6.08 2.63 5.85 2.3 5.68 3.06 6.02 2,63 5.83 2.3 5.66 4.8 3.07 6.30 2.56 6.04 3.20 6.34 2.74 6.11 2.4 5.92 3.20 6.29 2.74 6.08 2.4 5.90 5.0 3.20 6.56 2.67 6.29 3.33 6.61 2.86 6.36 2.5 6.17 3.33 6.55 2.86 6.33 2.5 6.15 b:A 3.33 6.82 2.77 6.54 3.46 6.87 2.97 6.62 2.6 6.42 3.46 6.81 2.97 6.59 2.6 6.39 K-'* 3,46 7.09 2.88 6.79 3.60 7.14 3.09 6.87 2.7 6.66 3.60 7.07 3.09 6.84 2.7 6.64 b.G 3.58 7.35 2.99 7.05 3.73 7.40 3.20 7.13 2.8 6.91 3.73 7.33 3,20 7.09 2.8 6.88 b.S 3.71 7.61 3.09 7.30 3.86 7.66 3.31 7.38 2.9 7.16 3.86 7.60 3.31 7.35 2.9 7,13 fi.O 3.84 7.87 3.20 7.55 4.00 7.93 3.43 7.64 3.0 7.40 4.00 7.86 3.43 7.60 3.0 7. .38 0.2 3.97 8.14 3.31 7.80 4.13 8.19 3.54 7.89 3.1 7.65 4.13 8.12 3.54 7.85 3.1 7.62 0.4 4.10 8.40 3.41 8.05 4.26 8.46 3.66 8.15 3.2 7.90 4.26 8.38 3.66 S.ll 3.2 7.87 0.0 4.22 8.66 3.52 8.30 4.40 8.72 3.77 8.40 3.3 8.14 4.40 8.64 3.77 8.36 3.3 8.11 0.8 4.35 8.92 3.63 8.50 4.53 8.99 3.89 8.65 3.4 8.39 4.53 8.91 3.89 8.01 3.4 8.36 7.0 4.48 9.19 3.73 8.81 4.66 9.25 4.00 8.91 3.5 8.64 4.GG 9.17 4.00 8.87 3.5 8.61 'i.2 4.61 9.45 3.84 9.00 4.80 9.51 4.11 9.16 3.6 8.88 4.80 9.43 4.11 9.12 3.6 8.85 'lA 4.74 9.71 3.95 9.31 4.93 9.78 4.23 9.42 3.7 9.13 4.93 9.69 4,23 9 37 3.7 9 10 V.O 4.86 9.97 4.05 9.56 5.06 10.04 4.34 9.67 3.8 9.38 5.06 9.95 4,34 9.63 3.8 9.34 V.8 4.99 10.24 4.16 9.81 5.20 10.31 4.46 9.93 3.9 9.G3 5.20 10.22 4.46 9.88 3.9 9.59 8.0 5.12 10.499, 4.2G6 10.0648 5.3334- 10.572 4.5712 10.1816 4.00 9.872 5.333+ 10.4776 4.5712 10.1336 4.00 9.835 Or, supposing a to be = 1, sin (A+B) sin A . Example : A = 15° £ = 5° _ sin (15+5'^ __ sin 20 ° sin 15° sin 15° " 0.342 0.1322. 0.2588 The table gives, for greater convenience in practical application, the diameters of the impulse circles instead of the radii, though these latter are, properly speaking, the acting lengths. By this arrangement the practical work- man need only make a disc of the exact size of the diame- ter contained in the table for the special given case, and mark the point for the impulse pin by the edge of this disc. Calculations to Tabljs VII. The (acting) length of lever supposed to be = 1. Column Two. — Angle of pallet = 8°. Angle of roller 8 = 25°. Radius of impulse =-.= 0.32. pulse= 2.032 = 0.64. Column Four.— Angle of pallet 8°. g 30°. Radius of impulse = — = 0.266. ^ 30 pulse = 2.0266... = 0.533... Column Six. — Angle of pallet = 10° 30-. Radius of impulse = — 30 0.3.33. impulse = 2.0.333... = O.dCC, Column Eight. Angle uf jjallet = roller = 35°. Radius of impulse = .^- 3o eter of impulse = 2.02.S')7 = 0.5714. Diameter of im- Augle of roller Diameter of im- Angle of roller Diameter (jf 10°. Angle of = 0.2857. Diam- CoLUMN Ten. — Angle of pallet —10". Angle of roller =n 40°. Radius of impulse = = 0.2.5. Diameter of impulse — 2.025 = 0.500. Column Twelve. — Angle of pallet 12°. Angle of 12 roller 36°. Radius of impulse ==.,. = 0.333 Diame- .3(j ter of impulse = 2.0333. . . = 0.666. . . Column Fourteen. — Angle of pallet 12°. Angle of roller 42°. Radius of impulse= -^^=0.2857. Diameter of impulse = 2.02H57 =^ 0.5714. Column Sixteen. — Angle of pallet = 12°. Angle of 12 roller = 48°. Radius of impulse =r _ ^= 0.25. Diam- eter of impulse = 2.0.25 = 0.5. Distances of Centres. _, , a .sin (A+B) Formula : c = ^ ' a ^ 1. sin A . B = 12A° 4° A = B = 1.5° 4" A = 15° 5° ^ = 17^ 5° COLUMN THREE. sin . 16i° 0.2840 sin 12i° 0.2164 1.3124. COLUMN FIVE. sin 19° = 0.3256 sin. 15° 0.2588 COLUMN SEVEN. sin 20° ^ 0.3420 '' sin 15° 0.2588 = 1.2581. = 1.3215. COLUMN NINE. sin^22!° _ 0.3827 " sin 17.;° 0.3007 1.27l"i 87 COLUMN ELEVEN. A = 20° B= 5° sin 25° 0.4226 ^ ^34 ' sin. 20° 0.3420 COLOMN THIBTEEN ^ = 18° 5= 0° = sin 24S _ 0.4067 _ ^ 3„,^ siu.l8° 0.3090 COLUMN PIPTEEN. ^ = 21° . _ Sin 27° _ 0.4540 _ , ^^^, 5= 6° sin 21° 0.3584 COLUMN SEVENTEEN. ^ = 24° £=6° ^ _ sin . 30° _ 0.5000 _ ^ .^.,^^^ sin. 24^ 0.4067 The following general rules are deductions from the contents of this chapter, and, resuming the constructive necessities tor the two actions of the escapement, may be found useful for the replacement of parts in ready-made watches as well as for constructing new escapements. 1. If the diameter of a ratchet wheel, or the primitive diameter of a club or pin anchor wheel is given, the dis- tance of centres is determined, and vice versa. (Always supposing a wheel of fifteen teeth and a pallet 'scaping over thi'ee teeth). 2. To a given wheel, ratchet or club-toothed, a circular pallet may be made as well as one with equidistant lock- ings, and the centre distance will be the same in both cases. 3. To a given wheel, the pallet may be made with a large or small angle of lifting; the centre distance will not be altered by this difference. 4. A given pallet will admit but one diameter (primitive diameter) of wheel ; auy larger or smaller wheel is incor- rect. (See Chapter XVI.) 5. To a given pallet the wheel cannot be made at dis- cretion with club or ratchet teeth ; for, if the pallet be made for a club wheel, the ratchet wheel would have too much drop, and if it be made for a ratchet wheel, the club wheel Tould have no drop at all. 6. If the wheel of a pin anchor escapement is given, the lifting of the anchor is determined. 7. If the centre distance of fork and roller and the act- ing lengths of the two levers of fork and roller are given, both the angles of movement of the fork and roller are de- termined. 8. If the centre distance, the acting length of the fork, and its angle of movement are given, the acting length of the roller and its angle of movement are determined. 9. If the centre distance, the acting length of fork, and the angle of movement of the roller are given, the acting length of roller and the angle of movement of the lever are determined. 10. If the center distance and both the angles are given, the acting lengths of fork and roller are determined. 11 . If the centre distance, the acting length of the roller, and one of the two angles are given, the acting length of the fork and the other angle are determined. 12. If the acting length of the fork and both the angles are given, the acting length of the roller and the centre distance are determined. 13. If the acting length of the roller and both the angles are given, the acting length of the fork and the center dis- tance are determined. 14. If the acting lengths of the fork and roller are given, the respective proportions of the two angles are determined, and vice versa. 15. If the acting lengths of the fork and roller and one of the two angles are given, the other angle and the centre distance are determined. 88 CHAPTEII XIII. PROCEDURE OF MAKING A GOOD AND CORRECT LEVER ES- CAPEMENT. After what has been said in the two last chapters on the proper respective proportions of the acting parts of the lever escapement, it remains but to explain how these pro- portions may be accurately observed in the process of con- struction. I deem it unnecessary to explain here the me- chanical processes of tiling, cutting, polishing, etc., for these are things which can never be learned from books. I treat the subject wholly from a mathematical point of view, firmly convinced that this treatise will be found useful for prac- tical escapement makers, not by teaching them how to file and polish, which they already know as well as any body could teach them, but by explaining to them how to avail themselves of the teachings of science, which exists as well for the watchmaker m for the engineer, and should guide the work of the one at; veil as that of the other. For the reader w lo has thoroughly mastered the con- tents of the two last chapters itic process of making a cor- rect lever escapemou' , or any part of it, will require little explanatiallets of any size whatever. For making a pallet with equidistant lockings, five steel discs are required, whose sizes must be sought for in Table II. We suppose the measured diameter of the wheel to be 7.72 m., and the angle to be performed, 12°. The corre- sponding sizes would be : Outer circle = 5.86 m. Locking circle = 4,50 m. Inner circle = 3.14 m. Fii-st lifting circle = 1.09 m. Second lifting circle = 2.91 m. Height of segment = 4.23 m. Five discs must be made ot the size indicated by the above mentioned first five numbers, and the largest of them, that of the outer circle, must be flattened away as much as to measure in the right angle to its flattened part, 4.23 m. Then take a slip of steel, prepared as already explaiued, trace the outlines of the pallet according to the three discs, file the open side of the pallet away until touching the line indicated by the segment, file the locking face of the first pallet arm to an angle of 112° and the outer side of the other pallet arm to an angle of 120°, file out the space be- tween the arms and make their inner faces parallel to the outer ones, giving the arms the breadth indicated by the table to be 0.68 m. Fix the fourth disc on the pallet and trace a tangent to it from the entrance corner of the first arm, fix then the fifth disc and draw a tangent to it from the delivery corner of the second arm. File the driving planes on both the pallet arras to agree with these tangents and then the acting [jarts of the pallet are of the righi size and shape. In case it is required to make a wheel to a given pallet and centre distance, which occurs often when repairing lever watches, the distance of centres must be measured and the proper size sought in Table I, column 10, if the pallet is a circular one, and in Table II, column 11, if the lockings should be equidistant. Suppose the centre distance to be 90 5.2 m., we find in the first coliimu of botli tables tliat a disc for a wlieel must be turned of a diameter of 9.0 iii. This .size must lie taken in the first cohimu, because there is a full round disc in question liere — tliat is, the wheel be- fore its teeth are cut. If in any case the given sizes and circumstances should not be found to agree perfectly with the numbers contained in the tables — for instance, if a circular pallet with a move- meot of 8'^ is to be made to fit to a wheel of the measured diameter of 6.83 m., the next two diameters in the table must serve to determine the right sizes by a simple system of interpolation The required size (6.83 ra.) is just between the next numbers (in column 2) of which it is the middle- rate, and therefore iu all the columns wauted the middle of the numbers contained in these two horizontal ranges must be taken : Outer circle Inner circle Lifting circle 4.52 + 4.65 0.17 2 = — — = 4.58 m. 3.34 + 3.43 _ 6.77 = 3.3S m. 1.44+1.48 2.92 Height of segment = - 3.41 +3.51 _6.92 = 1.46 m. = 3.46 1 If the diameter of wheel had been 6.78 m., the difference of this size to the next one iu the table, 6.73, would be (1.05 m., or one-fourth of the difference between the two next sizes in the table, 6.73 and 6.93. Therefore in all the columns the number in the horizontal range of 6.73 must be taken and augmented by one-fourth of the difference between this and the next number in the same column : Outer circle = 4.52 + Hi-' = 4.52 + 0.033 = 4.55 4 Inner Liftina: circle 3..34 +2:!I^ = 3.31 + 0.02 = 3.36 4 ^ = 1.44 4 0.04 1.44 + 0.01 = 1.45 Height of segment =3.41 +—'!=- .3.41 + 0.03 = 3.44 4 The use of Table VII for finding the proportionate lever length and radius of impulse for certain given or intended angles of lifting, is very easy. Supposing the acting length of a lever given to be 4.2 m., having a total movement of 8'^, and the lifting angle of the roller intended to be SO'', we must look for the diameter of impulse in the fourth col- umn, where the corresponding size is 2.24 m. Make a disc of steel of that size, fi.x it on the table roller so that it is concentric with it, and trace the circle in which the acting edges of the ruby pin are embraced, close to the edge of this disc. If it is required to make a lever and roller to a given centre distance, as 4.45 m., the pallet making an angle of 10° and the lifting angle on the roller intended to be 40°, find in column 11 the number 4.45, and in the same hori- zontal range the corresponding diameter of impulse will be found iu column 10, = 180 m., and the acting length of lever in column 1, = 3.60 m. If a roller has been lost and is to be replaced so as to give with a lever length of 4.8 m. and a pallet movement of 12°, a lifting angle of 42^ on the roller, look in column 1 for the lever length of 4.S tn., and proceed in the horizon- tal range of that nund)er to column 14, where the diameter of impulse will be found to be 2 74 m. If in the same case a certain centre distance . must be kept, as in most cases of replacing a roller, there is no lib- erty allowed as to the angle of lifting on the roller. If, for instance, the centre distance is given = 5.9 m., the angle of 91 lifting on tiic roller must be 18'^, and the inipulso radius 2.4 m. When in such case this latter would be made 2.74 ni., it would require an alteration of ihe lever length or centre distance, which cannot be granted in a ready-made watch, and without those alterations it would not perform the in- tended angle, and would require a wider banking, because it would force the pallet to travel a much greater angle than it requires for escaping. It might be asked, what is the use of making steel discs for every size, and is it not better to measure directly and trace the circles with a compass or depthing tool? Tliis must be answered in the negative, for no compass or depth- ing tool can be adjusted so nicely as to distinguish hun- dredths of a millimeter, but a disc can be directly measured with the micrometer, and consequently be made with all the accuracy required. CHAPTER XIV. ON THE MATERIAL EMPL(1YED IN MAKING LEVER ES- CAPEMENTS. This is a very important question in the construction of the lever escapement, and every escapement maker should make it the subject of his most earnest study, the more especially as we encounter very diverging opinions among the various manufacturers. The English lever escapements have almost uniformly a brass escape wheel and the pallet and lever of tempered steel. The Swiss show a greater variety ; still, most of their escapement wheels are of tempered steel, and almost all their pallets and a considerable proportion of their levers are of the same material. Sometimes we see levers of brass or German silver, and wheels of brass and gilt; but it seems that in most cases the choice is decided by taste and fancy, without any regard to the practical service of the parts. Supposing the question, which of these materials is the best suited to the acting parts, we will try to elucidate the mat- ter by discussing the reasons for and against each of them. To begin with steel, it cannot be denied that it is in many essential points a very good material for the parts of escapements. It is tolerably hard and elastic, and suscep- tible of a beautiful polish. Besides, its specific weight is the lowest of all materials that are applicable. Still, there are very bad qualities in steel, which are greatly to its disad- vantage. The first is its liability to oxidize or rust. 92 When we consider huw caieftiUy llie escapenieul maker strives tu reduce the friction of tlie acting parts by giving them the highest polish, it is a discouraging reflection that these beautifully polished surfaces may, by being carelessly touched by a moist hand when the watch is under repair, or even by atmospheric influences, or by the action of gas or vapor of acids, be deprived not only of their nice look- ing appearance, but also of that smoothness of surface which has been produced with so much care. Many ex- cellent specimens of workmanship are destroyed by this natural defect of the steel. Another great danger resulting from the employment of steel is its susceptibility of magnetism, especially in watches with compensated balances, which necessarily are made of steel. It has the most detrimental influence on the rate of the watch if, by causes which are not yet fully un- derstood, and which very often cannot be avoided even by the greatest precaution, any part of the escapement has be- come magnetized. The lever, being the longest part of it, is most of all exposed to magnetic polarity, and the influ- ence is the more pernicious because it is acting on its end. It will there produce quite unaccountable deviations of rate, even in watches in which all the requirements for a good performance are united. A third and very great drawback in steel as a material, is the necessity of hardening it for such purposes. If not hardened, the steel would hardly offer any essential advan- tage over other good materials, and the process of harden- ing involves unavoidable danger to the soundness of the parts. Nobody can guarantee that a hardened ])iece of the best steel may not have some trifling defect which will ren- der it worthless when ready and finished. True, the skill and care of the workman may reduce the liability of such occurrence, but even then it is bad enough to be aware that there may hi' liidden some tendency to break in any ])art of the escapement. Besides, the necessity of polishing the steel parts all over after having hardened theui causes much trouble, es- pecially when the wlieel is also made of steel, and necessar- ily augments the manufacturing expense. These natural defects would compel the absolute disuse of steel in watchwork if there w-ere another metal known to replace it. So long as this is not the case, we are obliged to make our pinions, arbors, pivots, screws, etc., of steel, but there is no necessity for making the wheel, pallet and lever of our escapements of this material. Therefore we must try to ascertain whether there is any other metal as appro- priate, or more so. Another metal very frequently employed, especially for wheels, is brass. Its qualities render it a very proper ma- terial, because when carefully hammered it has considera- ble density and elasticity. Its specific weight, though about one-seventh more than that of steel, is no objection to its employment, and it is free from the above mentioned nat- ural defects of steel. Therefore we have strong reasons to prefer it to the latter for the material of wheel, pallet and lever. Still, it might be objected that it is impossible to give to the brass, however it might be prepared, the degree of hardness and elasticity which is shown by tempered steel. An escape wheel of brass, as has already been mentioned, should always be polished on its surfaces, and not gilt, for reasons which have been explained in Chapter VIII. German silver is, in its physical qualities, very much like brass, but experience has shown that the iriction in the German silver fork is greater than in forks of brass and steel. Four or five years ago a new alloy was invented at Vienna, and called sterro-metal. It was said to be of very 93 greal malleability, tenacity and elasticity It occurred to me that it might be very useful for this and similar pur- poses. I procured a quantity of it, in several different thicknesses, and found its exterior very much like brass, of a rather reddish color. I was told that it was composed of copper, zinc, tin and iron, and its tensile strength was stated by a commission in the imperial arsenal at Vienna to be 4, .500 kilogr. on the square-centimeter, and consequently approaching that of east steel, which is commonly accepted at between 4,900 to 8,300, while that of brass is about half as much. This encouraged me to try the qualities of the sterro-metal for watchmaking purposes I took five slips of itf each 2.5 m. thick and 18 m. broad, which I worked out in several ways. I took the first between a pair of good flattening rollers and rolled it by degrees down to the thick- ness of 1.1 m., at which point I was obliged to stop because the metal showed many fissures on its edge. The second specimen was heated red hot and cooled in water. This diminished the hardness a little, but not so much as is the case with brass by heating. Then we worked it out between the rollers to the thickness of 1.1 m., after which I found it quite sound. After once more heating and cooling, we re- duced it to O.G m. The specimen, though stretched out to more than three times its length, jiroved to be entirely with- out defects. I cut a part off, heated and cooled it, and rolled it down to 0.2 m. This was a reduction in thickness to 8 ])er cent, of its original size, and the soundness of the metal was perfect. The hardness and elasticity were very satisfactory, and it could only be broken by bending it at a very sharp angle. I took then the third specimen, heated and cooled it, and rolled it down to 0.75 m.. when it was cracked all over. The fourth specimen I rolled four times with red heat, and then forged the fifth specimen four ^mes, lieating it red each time. These two last slips were very good, and of excellent elasticity. These experiments were sufficient to convince me of the advantages to be ob- tained by the employment of the sterro-metal for lever es- capements. I have had many escapements made of it, and never experienced any disadvantage from its use. The high degree of tenacity and ductility shown by it is more than the best English or Bavarian brass could be expected to possess. The specific weight is 8.9, about equal to that of brass, and its expansive ratio is a trifle higher than that of brass I also tried the sterro-metai lor train wtieels, but found it would not answer, because in cutting the teeth it spoils the cutters very soon. The polished surfaces of the sterro- metal do not look so good as those of good, hard brass. When well hammered, gold is a very good material for lever escapements. It may be said to nearly equal in hardness and ductility the sterro metal, but it breaks more easily. It is not necessary for this purpose to employ gold of 18 carat; the alloy of 12 carat will do quite as well, and is capable of a beautiful polish. Still, its specific weight is an objection against its use. Gold of 12 carat is about 14.0. This is too heavy for parts of an escapement, and increases the inertia considerably, a circumstance not to be underrated in the lever escapement, which has so many intermissions in Its action. Besides, the price of the gold would be an objection to its general employment. Cousidering its very low specific gravity, aiuminium at one time seemed to me a desirable metal for escapements; but it very soon proved quite unfit, because it was found impossible to give it the hardness and elasticity indispensa- ble for this work. One of the alloys of this metal, however, has claimed the attention of mechanicians by its unrivaled strength, and great hardness, and resistance to wear by friction: It is the alloy of copper and aluminium, known 94 under the name of aluminium-bronze. Tiie honor of its in- vention is a matter of dispute between France and England, the former claiming it for St. Clauc Deville and Debray, while the English attribute it to Dr. Percy As the most earnest eflbrts were at this time universally dii-ected to the complete e.Karaination of aluminium and its alloys, it is not unlikely that both invented it independently of one another. The only aluminium-bronze 1 have tested in my experi- ments was that of 10 per cent, aluminium to 90 per cent, of copper. The alloys in which a smaller quantity of aluminium is contained wore described in the reports as not promising satisfactory results; besides, the desire for a material of the least specific gravity would naturally lead to the choice of an alloy with the largest proportion of alum inium. But such alloys have been proven brittle, and de- void of the necessary elasticity. The aluminium bronze of 10 per cent, has been found by the experiments of Mr. An- derson, at the Royal Gun Factory, Woolwich, Mes.sis. Simms, London, and Mr. Morin, Nanterre, to have a ten- sile strength of 5328 kilogr. on the ['] C" as the mean rate of several trials, thus approaching to tlie average strength of cast steel. Its resistance to compression and its mallea- bility are very satisfactory, though not of much importance for escapement makincr. But a very important point, the transverse strength, or resistance to being bent, was found on a comparative trial with brass and gun metal to be: Brass, - - 2.22 Gun metal, - - 0.15 Aluminium bronze, 0.05 That is to say, three bars of the above mentioned met- ais, of the same dimensions, were fastened at one end so as to be in a horizontal position, and a certain weight applied to the free end of each bar made that of brass bend 2.22 degrees of the instrument, etc. This experiment proves that the aluminium bronze opposes three times greater re- sistance to flexion than gun metal, and that its resistance is 4-1 times as great as that of brass. The exj)ansive ratio is considerably less than that of brass. Its resistance to oxydation by atmospheric inlluences is not determined, but is certainly greater than that of brass, though inferior to gold of 18 k. Resistance to friction is a quality in which, to judge from the reports, the aluminium bronze is unsur- passed. This combination of desirable qualities induced me to try the aluminium bronze 'vith special reference to its em- ployment for horological purposes. I took some slips of 10° aluminium bronze plate of 2.4 ni thickness, and tried at first how much they could be treated between the rollers without heating. I soon found ihat this material would not bear .i i';ductioi2 of more thru one-fourth to one-third of its thiclmes:: \.'ithout 'getting many fissures. When heated to red hea'b and cooled in w'atci', however, after having been rolled down about ono-fourth its thickness, it will bear a further operation of tlie same kind and extent. Thus, by alternate heatiu;^' and rolling I brought it to a thickness of 0.2 m. The specimen did not show the slightest fissures on its edges, but proved to be of remarkable hardness and elasticity. It occurred to me that it might be useful to make a comparative trial of the resistance to breaking by flexion. I took specimens -f sterro-metal, gold and alum- inium bronze, each reduced in the most careful w;iy t(j the thickness of 0.2 m. I found that the specimen of gold when merely bent with the fingers to a right angle, broke short ofi'. The specimen of sterro-metal did not break by this flexion, but in most cases it broke when it was bent into the straight line, or very little beyond it, to the other side. The specimen of aluminium bronze withstood being bent three or four times at right angles altei'nately to the 95 one and to the other side before it broke, and even then it did not break at once, but only on a part of its breadth, ■while otlier parts resisted further flexion. This tenacity is very astonishing, and can hardly be equalled by any other material. Other experiments in treating the aluminium bronze in a hot state- gave very satisfactory results. It opposes a greater resistance to files and cutters than brass or gold do, but the cut of it is very smooth and regular. cannot be denied that a metal possessing so many valuable qualities is an excellent material for lever escape- ments. I have made all my escapements of aluminium bronze since that time, and am very well satisfied with it. The polish is beautiful, and it looks very much like gold. I found this alloy also very useful for other purposes where hardened steel was formerly employed, as for click springs, wheels for keyless winding mechanisms, etc., etc. I am perfectly aware that I place my opinion in oppo- sition to that of a great majority of horologists, or at least to the usual course adhered to, when I assert that the alum- inium bronze is preferable to all materials hitherto in use for wheels, pallets and levers ; but with such facts as are contained in the following tables 1 think it is easy to sup- port my conclusions. PHYSICAI, QUALITIES OF METALS. The following are the physical qualities of materials mentioned in this chapter, and of some others of possible adaptation to the same purposes, as they could be found in physical treatises, but for the purpose of estimating the rel- ative value of these diflerent alloys as materials for lever escapements, these notations are very unsatisfactory: Gold of 18 k. - Gold of 12 k.- - Gold of 9 k.- - Silver - - . . German Silver - Sterro-metal - - Copper - - - Steel - - . . Steel hardened - Brass .... Aluminium - - Aluminium l)r(iiizi Tensile strength. 5000 5000 6400 8000—9000 10000—12000 2500 6400 Specific gravity. about 16.8 about 14.2 about 12.8 10.6 . 8.7 8.4 8.9 7.9 7.9 8.7 2.8 7.7 Expansive ratio. 0.001466 0.001520 0.001910 0.001700 0.001718 0.001079 0.001240 0.001868 0.001600 Finding no more definite iniormation in books, I un- dertook myself a series of experiments with a view to sup- plying this deficiency. The qualities necessary in materials for making delicate pieces of mechanism are : transverse strength, resistance against permanent flection, hardness, or resistance against compression, and resistance against breaking by being bent. The first step in conducting these experiments was to procure bars of all the materials to be tried, of a certain length, and exactly the same profile. To meet the last requirement the employment of round wire seemed the most convenient, because a carefully drawn wire presents in all its length the same thickness, and consequently for finding its profile it was only required to verify the diameter. I took care to prepare of all the materials wires of exactly the same diameter, and drawn as hard as could be without injury to their soundness. Their diameter was 2.50 m. For trying the transverse strength, I fixed one end of the wire solidly, and fastened an index upon it at exactly 200 m. from the fixed end. I chose three weights, which were hung on the wire close to the index, and noted the flexion produced hy each of them in millimeters. The first of 96 Diagram XVII. © L \ 4. 6. o 19. 18. 14. 15. 17. 1 ( ) le. K(o: / ; ! o DiAGKAM XVIII. Diagram XIX ^^^ these weights was 27 grammes, the second 98.5 gr. and the third 140 gr. They were the same for all the experiments. The flexibility of the different materials was found to be: 1st weight. 2d weight. 3d weight. Cast steel (Sheffield) - 2.1 7.4 11.2 Cast steel hardened, light blue 2.3 8.2 12.4 Cast steel hardened and blue 2.3 8.2 12.4 Cast steel hardened and yellow 2.3 8.2 12.4 Cast steel hardened 2.4 8.4 12.7 Cast steel hardened and red - 2.4 8.6 12.S Copper . - - - 3.7 12.4 18.6 German silver 4.0 13.2 19.3 Toinliac . . - 4.0 13.8 20.7 Aluminium bronze 4.4 15.2 22.7 Brass from Berlin - 4.4 15.G 23.4 Gold of 18 k. 4.7 16.3 24.0 Gold of 9 k. - 4.7 16.4 24.3 Gold of 12 k. 4.8 16.5 24.4 Brass from Augsburg 5.2 18.0 27.0 Sterro metal . .' . 5.3 18.2 27.1 Silver, standard 5.3 18.7 28.1 It will be easily understood that the transverse strength of the specimens must be in the inverse ratio of the num- bers contained in this table. But it is not exactly the flexi- bility or rigidity which must be valued for our purpose ; a much greater importance must be attached to the elasticity, or resistance to permanent flexions. At first sight it might appear that a conclusion may be allowed from the trans- verse strength upon this latter quality, but experiment proved this supposition incorrect. U.sing rods of the same dimensions as before, I bent each specimen, reading by the aid of a graduated arc and the index on the wire, the extent of flexion ; and after leaving the wire free to return to its former position, I verified whether any per- nanent flexion had taken place. This bending was in- creased by five millimetres each time, and continued until the permanent flexion amounted to 1 m. or mori'. The re- sults of these experiments are given in the following table : ] 5 20 25! 30 35 40 45 50 55| 60 Cast steel, hard Cast steel, hard, yellow Cast steel, hard and red Cast steel, hard and blue — Cast steel, hard,light blue Aluminium lironze Sterro metal Gold of 18 k. - Gold of 9 k. Brass ii(jm Berlin German silver Brass from Augsburg Gold of 12 k. Silver Tombac Cast steel, soft - Copper -,0.1 - 0.1 0.1,0.2,0.8 1.0:1.2 0.1 .1 0.2 0.1 0.2 2,0 1,0 -0 1;0 •7 brok'u 0.1 0.3 0.1 0.3 0.2 0.4 0.2 0.3 0.2 0.1|0.2;0.4 0.2 0.4 0.2 0.1 0.5 ;o.5,o.6 tO.50.7 : 0.4 0.6 ;0.3|0.7 i;0.9,1.0 65 Cast steel, hard Cast steel, hard and yellow Cast steel, hard and red Cast steel, hard and blue Cast steel, hard, light blue Aluminium bronze Sterro metal - Gold of 18 k. Gold of 9 k. - Brass from Berlin German silver Brass from Augsburg Gold of 12 k. - Silver Tombac Cast steel, soft - ,j Copper 0.1 70 75 80 85| 90 100 105 110 0.1 0.1 0.2 0.1: 0.5 0.2 0.4 0.5 0.8 0.9 1.0 1.7 0.2 0.1 0.5 0.2 0.6 ,0.6 0.9 broken. 0.2 0.3 0.2 0.3 0.6 0.7 0.3 0.5 0.7 0.9 1.0 0.3 0.4 0.8 0.9 0.4 0.4 0.5 0.8 0.5 0.7 97 Cast steel, hard - Cast steel, hard and yellow Cast steel, hard and red Cast steel, hard and blue Cast steel, hard and light l)luc Aluminium bronze Sterro metal - - - Gold of 18 k. Gold of 9 k. - Brass from Berlin German silver - - - Brass from Augsburg Gold of 12 k. - Silver Tombac - - - - Cast steel, soft Copper - - - - 115-120 broken. O.S 0.9 125 130 135 140 145 0.1 ; 0.1 0.2 A comparison between this and the preceding table shows clearly that there is no great connection between tranverse strength and elasticity. For instance, copper is the least elastic of all the materials in the preceding table, but shows sufficient transverse strength to hold first place among the other materials, except steel. Sterro metal shows great flexibility with a remarkable degree of elas- ticity. The superiority of aluminium bronze in this respect is also confirmed by my experiments, though I failed to find it so pronounced as Mr. Anderson states it to be. Perhaps lie has not tried the metals in tlie form of round wire, and, which I think most likely, he may have tried them as they were cast, without being hammered or rolled. For watch making purposes, of course, we have to deal with the ma- terials in their greatest density and hardness. Resistance to compression, or hardness, is another jioint which I thought desirable to try. Different methods have been employed for this purpose ; the manner of testing the hardness of materials in mineralogy, by scraping the one with the other, is the oldest; but for metals this would hardly answer, and would never admit of any exact grad- uation. Another way was taken by Hugueny. He tried to force a pointed punch into the different specimens by a blow of equal violence, and by the greater or smaller im- pression made he estimated the hardness of the specimens. This method, though giving much more positive results, did not satisfy me, because the degree of hardness was only to be estimated by vision. I tried to find a way to ascertain by direct measurement the compression resulting from a blow, and to this end employed a little stamping press to produce blows of exactly equal force. In the cylinder of this press I inserted a flat punch of one square centimeter, and the wire specimens served at the same time for these ex- periments. Thus, by measuring the compression of the part on which the blow had fallen, I obtained the numbers of hardness contained in the follow'iug table, and I may re- mark here that they are the mean rates of three different experiments. It might be said against this method thf t the employment of wire is not correct, because the impres- sions cannot be in a reirular arithmetic progression with the force of the blow, as might be expected when employing specimens of a rectangular profile. I know that well enough; still, the diameter of the wires and the blow being always exactly the same, I think the results obtained may not be very far from correct. Finally, I made the resistance to breaking the object of iiome experiments. I used the same specimens, fastened them in a vise at one end, and bent them to a right angle. After that I bent those which stood against this flexion, straight again to the other side in right angle, and con- tinued so until they broke. By addition of all these angles of flexion which they had resisted, I obtained the numbers contained in the second column of the table, wh'ch are also the mean rates of three or more experiments, while the third column shows the remarks made upon the manner in which the fracture took place. Compression Resistance Bemarks about iu to breaking the manner in MiUimeters. (in angles). which it broke. Cast steel, hard Burst 5-10° Very quick. Ca?t steel, hard, yell'-w Imperceiitiljlf 10° V^ery quick. t^ast steel, hard and r d 0.1)20 111. 22° Very quick. Cast steel, hard and blue 0.027 m. 25° Very quick. Cast steel, hard, light blue O.OSl m. Very quick. Aluminium bronze O.MtiT 111. 207° (^uick. Cast steel, soft 0.3;t8 111. 45-1 ;io°* Very quick. Gold of 12 k. - 0.4-10 111. 100° Quick. German silver O.-ISS 111. 17.5° Middling. Gold of 18 k. - 0.,")08 111. 110° Quick. Gold of 9 k. - 0.520 ni. 95° Quick. Sterro metal 0.540 111. 150° Very quick. Brass, Berlin - 0.500 111. 3oa° Slow. Brass, Augsburg - 0.570 III. 103° Quick. Tombac 0.043 111. 210° Slow. Silver 0.005 III. 30S° Very slow , Copper O.SIiG III. 170° 81ow. I am aware these resear:;hes were of a rather rudimen- tary character and might be imjjroved upon iu many re- spects, and for this reason I would have refrained from pub- lishing them but for the en I ire absence of such tables iu general, and especially for honjlogical purposes. Iu fact, I would feel very much gratified should the incompleteness of the results obtained by me occasion some scientific or practical mau to complete or correct them. One of the most important points, however, could not *One and the same foot of steel wire, broken at different jilaces, qa\n the numbers: 4r,°, 80°, QU", ll.j', liiJ''. .-ill Ihu other material-; showni a much yreater re.jularity of structure. be tested, which is the resistance to wearing by friction, and I fear it would be very difficult to get comparative num- bers of any value for this purpose. It would require a great amount of time, many experiments, and some appar- atus. Perhaps another may be more fortunate thau I in finding a simple way of testing this important quality of materials. 99 CHAPTER XV. OF THE POINTS TO WHICH THE EXAMINER SHOULD DIRECT HIS ATTENTION. It is au inseparable consequeiice of the compound action of the lever escapement that for good performance it is not sufficient oufy to have its separate actions correct, each in itself, but a j^ei'fect harmony between these sepa- rate actions is also necessary. Therefore the careftil exam- ining of a detaclied lever escapement is by no means an easy task, for there are many points to be tested on which good performance and time-keeping depend entirely ed that two courses may be taken. The one is the way of calcula- ting the proportions, as indicated in Chapter XII ; but as there are not many practical men able or willing to under- take those calculating operations, the graphic system, con- sisting in drawing the objects to be constructed on a large scale, and in strict accordance with the proportions dictated by mechanical rules, may be considered as an admissible expedient. This- method of proceeding, however, requires the subsequent reduction of the sizes in the drawing to the working size, which is made by such simple calculations as are familiar to a man of but little education or attainments. Therefore, even the employment of the graphic method does not exclude calculation. Any system of measurement inll be unfit for calculation, unless its division is strictly decimal. 2. The unit of a standard for watcMvork should be of a dimension corresponding to the dimensions of watchwork. The inch, for example, even if divided decimally, is not an appropriate unit for our purpose, because it is much too large. Watchwork is not a kind of work to be measured by inches. The diflerence between the largest and smallest sizes of movements does not amount to an inch. Now, when such extreme differences can only be expressed by fractions of the unit, we must conclude that this unit is too large. This deficiency of the inch system has been much felt in the trade, and this impression manifests itself by a sizing of the movements and other objects, which has no connection with the inch, and is expressed in merely conventional num- bers. When speaking of a movement of 14-size, nobody can form by this number the slightest conception of the diameter meant by it, and it may be considered rather doubtiol whether watchmakers . agree perfectly between tbeip;ri'7cs as to the ^z^^ct dimensions represented by those 104 sizes. The Swiss manufacturers have taken a more positive steji by indicating the sizes of their movements by French lines, which are nearly equal to the intervals of the English sizes. Every man, whether he be a watchmaker or not, is enabled to verify the diameter of a watch movement which is said to be one of 19 lignes. After it has been proven by the above example that the inch is too large a unit to measure movements with, it must be much more improper for the very small interior parts of the watch. The inch is sufficiently small for mill work and steam engines, but it will never answer as a unit for watch- work sizes. 3. The system chosen should offer the prospect of as uni- versal adoption as possible. It will require no proof that in our time, .when dis- tances are reduced by steam and electricity and bars to international communication are removed by treaties, when the loj'al and liberal interchange of ideas and exjieriences between cultivated nations become stronger every day, that amidst these anxious exertions of the civilized world to pro- mote association it would ill become a body of scientific Englishmen to create a standard in the use of which they would only have the Russians to keep them company, and even those probably but for a short time. This'would in- deed bo electing a kind of a Chinese wall around English watch and cLck manufacture. 4. The system to he introdvced must not only be perfect in theory, but it should be accompanied by the means of turn- ing it into profit for any purpose in practical work. These means are the measuring instruments. 5. The measuring instruments must be of such a nature us not to depend upon the sight, which will not answer when grsat accuracy is required, The object to be measured must be seized between two parts of the instrument, and the index must register the size. It would, for example, be impossible to verify the outer diameter of a pinion to the one-hundredth of an inch with an instrument recommended not long ago in the Horolog- ical Journal, under the head : "The Inch Decimally Di- vided." It is a small rule, on the edges of which a length of two inches is divided into 50 and 100 parts. Besides, a dif- ference of one-hundredth of an English inch is a very essen- tial amount for watchwurk. Let us, then, examine from these points of view whether the metrical system, which is the basis of all the tables and calculations in this treatise, would be suitable for the purpose. 1. Its applicability for calculation cannot be doubted, because its division is purely decimal, and, by being so, su- perior to any other system. It would be a very tiresome task to prepare or to use tables of proportions founded upon a system of measurement not decimally divided. 2. Its proportions to the dimensions of watchwork re- quires no demonstration. The millimeter is about one twenty-fifth of the English inch and about two-fifths of the French line, thus admitting of operation with integer num- bers, while with a larger unit the same sizes must be ex- pressed by fractions. 3. Regarding the prospect of its spreading over the civ- ilized world, the metric system stands decidedly the best chance, and the arguments which have been adduced in be- half of the English inch from this point of view are, on close investigation, of very little value. It has been said by Mr. Rankine that as the English inch is used in Great Britain, Russia and the United States, it is consequently used by one-fourth the population of our planet, which could not be said of any other standard measure. I think there never was a more unlair statement than that. Mr. Rankin^ cal- 105 culates the population of Great Britam at 174,000,000, of course including India, Australia, etc. At least three-fourths of this number of British subjects are quite ignorant of the fact that there is such a thing as the English inch existing in the world. The population of the Russian empire, too, stated to be 64,000,000, must contain all the different tribes of Eastern Europe and Asia, the Bashkirs, Tartars, Cal- mucks, Kirgheese, etc., who according to all probability measure merely by the spanning of their fingers or by the lengtk of their own feet, instead of by the Englisli foot and inch. Very likely the estimate of population in the United States at 32,000,000 is also swollen to that amount by in- cluding the backwoodsman and the red skin, as well as the negroes. A reduction of the alleged total number of 270,- 000,000 to one-fourth of that amount will certainly not be unfair when the question is to be decided how many people are measuring by English inches. When we compare this reduced number with the population of France, consisting of about 40,000,000 of civilized people, to whom the measur- ing standard is a fomiliar thing, augmented by the Spanish and Italian nations, who very soon, we hope, will be joined by the German nation in its totality, not to speak of Bel- gium and other small states, it may be assumed that the ad- herents of the English standard are considerably outnum- bered. 4. The requirement of the new system being accompan- ied by the necessary instruments for practically using it may be answered in favor of the metrical system by the fol- lowing description of the measuring instruments as they have been used in the watch manufactories of Glashutte for more than twenty years by a considerable number of work- men and employers. 5. It will be seen by the subsequent description of the measuring instruments that they are so constructed thr.t the measuring is not intrusted to the touch or sight, but that on the contrary it is effected by mechanical means, and the result brought to view by an index. The metric measuring system has been introduced in Glashutte since the commencement of watch manufactur- ing, in 1845, by the founder, Mr, A. Lange, who even at this eaily period adopted this system in consideration of its general superiority and special applicability to watch work. The construction of the round micrometer is due to Mr. Lange. DiSCRIPTION OF THE MEASURING INSTRUMENTS USED AND MANUFACTURED IN GLASHUTTE. 1. The meter measure is a kind of sliding rule with rec- tangular arms, between which the objects to be measured are inserted. The edge of the rule is divided by millime- ters, and with the aid of a vernier the tenths of millimeters can be read. This instrument is very convenient for use as a rule and angle, and to verify the parallelism of two planes by apply- ing the measuring arms. The diameters of wheels, barrels, jjlates, glasses, etc., may be measured with it in the readiest and most accurate manner to one-tenth of the millimeter. (See Diagram XIX, Figs. 1, 2 and 3.) For the jsurpose of drawing or tracing calculated lengths upon metal it is very convenient to have two points on it, and the accurate adjustment is facilitated by an adjusting- screw. (Figs. 4, 5 and 6, same Diagram.) 2. The tenth measure is illustrated by Figs. 7, 8 and 9, and its construction being very simple, it will not require explanation. It will be found very useful for measuring the bottoms of barrels or sinks, for measuring objects on the lathe, for testing the thickness of wire and plate, etc. The 106 index shows the measured size in tenths of a millimeter. A total opening of 10 m. is provided, and therefore the arc is divided into 100 parts. 3. The micrometer is illustrated by Diagram XIX, Figs. 10, 11, 12 and l.S. It shows a pair of small steel tongs, b b, cue-half of which is fixed solidly upon the plate, while the other half is fastened to the end of lever a, mov- able cu two pivots around the point h. For multiplying the movement of this lever, in order to make it more per- ceptible to the eye, the lever a carries a rack c, fixed on it concentric to the point h. This rack gears into a pinion (/, on the arbor of which is mounted the small rack e; this lat- ter drives the center pinion, which carries the hand on its projecting pivot. These two elements give a total multipli- cation of 180. The dial is divided into 200 parts, so that half a revolution of the hand indicates the size of 1 milli- meter. But there would be no reliability on the registra- tions of the hand on the dial if the shake wiiich the centre pinion must necessarily have for tree action were not re- moved, because the hand would shake more than one de- gree, and thus destroy all accuracy of measuring. There- fore, the second small rack /, pitching also into the center pinion, has a pendulum spring mounted upon it, with a tendency to move the center pinion back. An angular lever, g, projecting »t the outside of the case, serves to open the tongs. The object to be measured must be inserted between the opened tongs, and when' the lever g is let loose the tongs will hold it, if it is not too heavy, by the tension of the pen- dulum spring constantly acting in a direction so as to shut the tongs The hand on the dial shows the distance at which the two parts of the tongs are kept apart by the object be- tween them, or, which is the same, the thickness of this ob- ject. The total opening of the instrument is 6 to 8 m. The hundredths of a millimeter indicated by this micrometer are commonly called degress by our workmen, and this de- gree is the unit for pivots and other small objects. A measurement by hundredths of millimeters is a very jQinute one, for the thinnest measurable object, the human hair, for instance, measures 4 to (! degrees. The thinnest paper shows a thickness of 3 degrees. This instrument, as well as the tenth measure, has a mathematical defect, because it measures the arc described by the tongs, and not the chord of this arc, which latter is the true thickness of the measured objects. This error in- creases with the angle of opening. Of course it will be of much more consequence in the tenth measure, but in this instrument the error is compensated as much as possible by dividing a straight line into 100 parts, and transferring this division to the arc of the instrument. For the micrometer this elimination of the error is impossil)le, but happily it is not of so great consequence, because its angle of opening, a c supposed to be = m., amounts only to (^°. The error arising out of the dillerence between the arc and chord of an angle of not more than 0°, is very trifling, and may be ignored altogether, even where great accuracy is required. The micrometer is commonly made with a base of wood, to have it at convenient height from the surface of the table. The nicety of measuring with the micrometer may be tested by an experiment : Take a piece of brass wire about 1 ui. thick, put one of its ends between the tongs of the micrometer, support the other end, put a lamp under the wire at about 1 to 1 J inches distant from the tongs, and heat the wire to a low red heat. The expansion of the wire will be indicated by an evident movement of the hand, and the subsequent contraction through the cooling of the wire will cause the reverse of this movement. These three instruments, the meter measure, the tenth •iieasure and the micrometer, are quite sufficient for all prac- 107 tical wants of watch and clock making. Their application for the graphic method of working is the following: Sap- pose that a circular pallet is to be made to a ratchet wheel, the real diameter of which is = 8 m. The diameter of the wheel, as drawn in Diagram 2, is 200 ni., or 25 times the size of the wheel to which the pallet is to be made. Therefore all the sizes of the pallet in the drawing must be measured with the meter measure and divided by 25 or multiplied by 0.04, to give the working sizes. The inner circle of pallet, for example, has on the drawing a diameter of 98 ni. The disc of this circle (Chap- no ter XIII; must therefore be made i? =: ".92 m. or 392 degrees of the micrometer, etc. This is also the size indi- cated by Table I for the diameter of inner pallet circle when the real diameter of the wheel is = 8 ni. It is frequently the case that micrometers are ordered for special purposes, such as for iron works, to verify the thickness of wires, for pianoforte makers fur the same pur- pose, for paper mills to guage the quantity of material re- quired for a certain sheet of paper, for spinning establish- ments to ascertain the thickness of the yarns, etc. I have often found that micrometers employed for these technical purposes do not always meet with the careful treatment wa'i,chmakers are accustomed to accord their tools, and some- times I receive the instruments back for repair in very bad condition. This prompted me to devise a measuring instru- ment which would stand rough treatment without getting out of order, yet possessing the same accuracy as the mi- crometer. It occurred to me that the multiplication effected in the micrometer by two depths might be attained with one depth only by employing longer levers. Diagram XX, Figs. 1, 2 and 3, show the simplified micrometer. One of the two arms, a a, is fastened to the plate and carries the foot c, serving as the center of motion, and on its other ex- tremity the fixed half of the tongs. The other arm, b b, turns round its axis in r. The foot is hollowed out to re- ceive the arbor, and the lower pivot moves in a hole near the lower end of the foot, while the upper pivot is fitted into a cock screwed upon the upper surfiice of the fixed arm, a a. This arrangement allows a greater length of the axis, and consequently a greater soundness of movement. The mov- able arm h h carries on the extremity of its long lever a rack, d, concentric to the point c, and pitching into a pin- ion,/, of fifteen leaves in the center, the projecting pivot of which carries the hand. The shake of the pinion and hand is eliminated by a secondary rack, identical to the other, and fixed upon it with two screws, leaving it a small shake in the direction in which the rack is moving. A small spring is constantly pressing against the secondary rack, so that its teeth always stand a trifle beside those of the fixed rack, thus exerting an elastic pressure on the pinion leaves, and removing the shake without prejudice to the freedom of movement. The extremity of the short lever of the mov- able arm 6 h carries the other half of the tongs, correspond- ing to that on the arm a a. A long flat spring, g, with a tendency to shut the tongs, completes the arrangement. This simplified micrometer has given very satisfactory results. The dial and its division is entirely the same. Its parts are strong enough, and so very simjjle that it does not require the care of a watchmaker to keej) it in acting order. The greater simplicity of construction admits also its sell- ing at a cheaper price than the round micrometer. There may be some objection to a micrometer of this kind, in that the unavoidable error formerly alluded to arising from the diflTerence between arc and chord is much more marked, because the shortness of the lever arms car- rying the tongs requires a larger angle of opening. In 108 fact, this angle Is =; 15° for an opeuing of 6 m. Never- theless, this instrument will be found to answer very well, as many comparative experiments have convinced me that in point of accurate measuring they are in no way inferior to the round micrometer. I attribute this favorable result to the omission of one depth, for pinions and wheels, if even made with the greatest care, will always bear some trifling uuequalities which, by a multiplication of more than 100, become considerable quantities. After having tested this principle I received orders for instruments for special purposes, one from a manufacturer of gold and silver lace, fur measuring the finest threads, and the other fur a scientific amateur, both requiring a direct measurement of 1-500 m. I did not think it advis- able to entrust a measurement of such subtlety to the enor- mous multiplication by two depths, but constructed the in- strument in the same way as the preceding. The arms are luuger and the dial is larger, and divided into 500 degrees. 'One revolution of the hand is =r 1 m. (Diagram XX, Figs. 4, 5 and tl.) Since that time I have manufactured many such instruments for special purposes, and, as far as I know, they give satisfaction. This measuring system may prove very useful for the English watch and clock manufacture if universally intro- duced. Finally, I thought it would be convenient to the read- ers of this treatise to have joined to it tables of reduction, in order to compare easily the sizes in millimeters with those expressed in English inches and French lines. 109 Table X. Milli- Milli- meter EDgliah inch. French line. meter Engliah inch. French line. (I.Ol 0.0003937 0.004433 18 0.70866 7.9794 0.02 0.0007874 0.008866 19 0.74803 8.4227 0.03 0.0011811 0.013299 0.04 0.05 0.0015748 0.0019685 0.017732 0.022165 20 21 0.78740 0.82677 8.8660 9.3093 0.06 0.0023622 0.026598 22 0.86614 9.7526 0.07 0.0026559 0.031031 23 0.90551 10.1959 O.OS 0.0031496 0.035464 24 0.94488 10.6392 o.oa 0.0035433 0.039897 25 0.98425 11.0825 26 1.02362 11.5258 0.1 0.003937 0.04433 27 1.06299 11.9691 0.2 0.007874 0.08866 28 1.10236 12.4124 0.3 0.011811 0.13299 29 1.14173 12.8557 0.4 0.015748 0.17732 0.5 0.019685 0.22165 O.G 0.023622 0.26598 30 1.18110 13.2990 0.7 0.026559 0.31031 31 1.22047 13.7423 0.8 0.9 0.031496 0.035433 0.35464 0.39897 32 33 1.25984 1.29921 14.1856 14.6289 34 1.33858 15.0722 1 2 0.03937 0.07874 0.4433 0.8866 35 36 1.37795 1.41732 15.5155 15.9588 3 0.11811 1.3299 37 1.45669 16.4021 4 0.15748 1.7732 38 1.49606 16.8454 5 0.19685 2.2165 39 1.53543 17.2887 C 0.23022 2.6598 7 0.26559 3.1031 40 1.57480 17.7320 8 0.31496 3.5464 41 1.61417 18.1753 9 0.35433 3.9897 42 1.65354 18.6186 43 1.69291 19.0619 10 0.39370 4.4330 44 1.73228 19.5052 n 0.43307 4.8763 45 1.77165 19.9485 12 0.47244 5.3196 46 1.81102 20.3918 13 0.51181 5.7629 47 1.85039 20.8351 14 0.55118 6.2062 48 1.88976 21.2784 15 0.59055 6.6495 49 1.92913 21.7217 16 0.62992 7.0928 17 0.66929 7.5361 50 1.96850 22.1650 Table XI. English Inch. MiUtmeter. Fienob line. English Inch. Millimeter. French line. 0.001 0.025399 0.011260 0.1 2.5399 1.12595 0.002 0.050798 0.022519 0.2 5.0798 2.25190 0.003 0.076197 0.033779 0.3 7.6197 3.37785 0.004 0.101596 0.045038 0.4 10.1596 4.50380 0.005 0.126995 0.056298 0.5 12.6995 5.62975 0.006 0.152394 0.067557 0.6 15.2394 6.75570 0.007 0.177793 0.078817 0.7 17.7793 7.88165 0.008 0.203192 0.090076 0.8 20.3192 9.00760 0,009 0.228591 0.101336 0.9 22.8591 10.13355 0.01 0.25399 0.112595 1.0 25.3990 11.25945 0.02 0.50798 0.225190 1.1 27.9389 12.38545 0.03 0.76197 0.337785 1.2 30.4788 13.51140 0.04 1.01596 0.450380 1.3 33.0187 14.63735 0.05 1.26995 0.562975 1.4 35.5586 15.70330 0.06 1.52394 0.675570 1.5 38.0985 16.88925 0.07 1.77793 0.788165 1.6 40.6384 18.01510 0.08 2.03192 0.900760 1.7 43.1783 19.14105 0.09 2.28591 1.013355 1.8 45.7182 20.26700 1.9 48.2581 21.29295 2.0 50.7980 22.51890 Table XIL French French line. English inch. Millimeter. line. English fnoh. Millimeter. 0.01 0.000888 0.0225583 0.1 0.008881 0.225583 0.02 0.001776 0.0451166 0.2 0.017763 0.451166 0.03 0.002664 0.0676749 0.3 0.026644 0,676749 0.04 0.003552 0.0902332 0.4 0.035526 0.902332 0.05 0.004440 0.1127915 0.5 0.044407 1.127915 0.06 0.005328 0.1353498 0.6 0.053288 1.353498 0.07 0.006217 0.1579081 0.7 0.062169 1.579081 0.08 0.007105 0.1804664 0.8 0.071051 1.804664 0.09 0.007993 0.2030247 0.9 0.079933 2.030247 1.0 0.088814 2.25583 11.0 0.97696 24.81413 2.0 0.177628 4.51166 12.0 1.06577 27.06996 3.0 0.266442 6.76749 13.0 1.15458 29.32579 4.0 0.355256 9.02332 14.0 1.24340 31.58162 5.0 0.444070 11.27915 15.0 1.33221 33.83745 6.0 0.532884 13.53498 16.0 1.42103 36.09328 7.0 0.621698 15.79081 17.0 1.50984 38.34911 8.0 0.710512 18.04664 18.0 1.59865 40.60494 y.o 0.799326 20.3024" 19.0 1.68747 42.86077 10.0 0.88814 22.55830 1 20.0 1.77628 45.11660 110 Ask PATENT SNAP BEZEL Dust Proof Cases MADE IN FILLED^AND SOLID GOLD. ALSO A FULL ASSORTMENT OF REGULAR LINE OF FILLED CASES. 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