HEAT—EXPANSION AND CONTRACTION.
From an article by J. Gordon Ogden, Ph.D., in “Popular Mechanics,” September, 1910, we quote:
“Expansion is one of the most remarkable of the phenomena to be reckoned with in the natural world. Practically every bit of matter from the Great Brooklyn Bridge to the tiny hairspring in one’s watch is under its imperial domination. It is a tremendous force, and the world of mechanics has to treat it with the deference and respect due to its gigantic power. Unlike gravity, and other forces of nature, it is whimsical and takes sudden fits and starts, now acting one way, now another. It affects different bodies in different ways, and seems to be at variance with the time-honored forces whose action can be predicted under all circumstances. At least that is what it apparently does. In our meagre knowledge of the great underlying laws that control the universe it is possibly unwise to speak so unkindly of expansion, as though it were a spoiled child in need of correction; its behavior, however, is so contrary to what one might expect that one is at a loss to say anything else.
“The walls of a building are sometimes rectified by the enormous force exerted by the contraction of iron rods. Bars of iron are placed so as to join the two walls where the bulging is most pronounced. These bars terminate in screws furnished with nuts. The whole of their length is heated and the nuts tightened. On cooling the bars will contract with practically irresistible force, causing the walls to straighten up. This operation is repeated until the rectification is completed. Boiler plates are fastened with red-hot rivets. The contraction of the rivets incident upon their cooling draws the plates tightly together, forming a steam-proof joint.”
“Tyndall, in his work on heat, gives an excellent illustration of the force of expansion and contraction. ‘The choir of Bristol Cathedral was covered with sheet lead, the length of the covering being 60 feet and its depth 19 feet 5 inches. It had been laid in the year 1851, and two years afterward it had moved bodily down for a distance of 18 inches. The descent had been continually going on from the time the lead had been laid down, and an attempt to stop it by driving nails into the rafters had failed, for the force with which the lead had descended was sufficient to draw out the nails. The roof was not a steep one, and the lead could have rested on it forever without sliding down by gravity. What, then, was the cause of the descent? The lead was exposed to the varying temperatures of day and night. During the day the heat imparted to it caused it to expand. Had it lain upon a horizontal surface, it would have expanded all around; but as it lay upon an inclined surface it expanded more freely downward than upward. When, on the contrary, the lead contracted at night its upper edge was drawn more easily downward than its lower edge upward. Its motion was, therefore, exactly like that of a common earthworm; it pushed its lower edge forward during the day and drew its upper edge after it during the night, and thus by degrees it crawled through a space of 18 inches in two years.’
“Mention has been made in a preceding article of the effect of unequal expansion upon two different metals that have been bolted together. It is by this principle that the action of the ordinary thermostat, so familiar now as a controller and regulator of the temperature of high buildings, is explained—a rod made up of two different metals whose rates of expansion are different. When the temperature of the room in which the thermostat is placed becomes too high the rod curls toward the metal point S and touches it, completing an electrical contact which causes a motor to shut off the draft. When the temperature of the room falls below a certain point the rod curls in the opposite direction toward the metal point T. This causes a motor to open the draft and thus furnish a more abundant supply of hot air.
“Everybody in these days of cheap and reliable timepieces carries a watch. And yet there are very few who appreciate the methods and devices by means of which the troublesome expansion and contraction of metals are corrected, in order that a watch may keep correct time. The balance wheel of a watch corresponds to the pendulum of a clock, and any variation in its dimensions will cause it to move faster or slower, as the case may be. The hairspring is really a long strip of metal which becomes weakened in its effect when expanded by an increase in temperature and has its power augmented when contraction takes place.
“To correct both of these conditions the rim of the balance wheel is made up of two different metals, the outer part brass, the inner part iron. When the hairspring becomes weaker by expansion the brass of the balance wheel also expands; but as it expands more than the iron to which it is bonded, it curls in toward the center of the wheel, making practically a wheel of smaller diameter, and causing the same effect as is produced when a clock pendulum is shortened. Exactly the opposite conditions obtain when the timepiece is exposed to extreme cold and the balance wheel has its diameter increased, thus causing a slowing up to counteract the increased strain produced by the contraction of the hairspring. The same principle is applied in the construction of first-class clocks. Any uncorrected variation in the length of a pendulum is fatal to the timekeeping quality of a clock. A gridiron pendulum made up of alternate rods of steel and brass serves to correct the result of the expansive force.
“The central steel rod passes through holes in the lower horizontal framework and supports the bob at the lower end. The steel rods are so arranged that they will expand downward, while the brass rods expand upward and the total length of each metal used is exactly sufficient to counteract each other’s expansion, and the centre of the bob will remain at a constant distance from the point of suspension.”
Scientific men and engineers are more or less familiar with the phenomena of expansion. But no inventor produced a system capable of utilizing this force to run a clock until Bangerter succeeded in mastering the problem.
Bangerter’s clock is unquestionably a triumph of human ingenuity. It is a mechanical masterpiece. Herewith follows the complete specification:
SPECIFICATION
TO ALL WHOM IT MAY CONCERN:
Be it known that I, FRIEDRICH BANGERTER, of the City of New York (Borough of Richmond), County of Richmond and State of New York, have invented certain new and useful improvements in
APPARATUS FOR THE EDUCTION, STORAGE
AND APPLICATION OF ENERGY FROM
EXPANSIBLE MATERIALS,
of which the following is a full, clear and exact specification, such as will enable others skilled in the art to which it appertains to make and use the same.
This invention relates to apparatus whereby energy may be educed from expansible materials, due to the expansion and contraction thereof on changes of temperature, and the said energy either applied direct or stored and applied for the purpose of operating machines and devices of various kinds.
I show and describe herein two forms of apparatus for obtaining such expansion and contraction and the required energy therefrom, and I also show two forms in which the energy so obtained is accumulated and stored. In connection therewith, I show the application of my invention to the running of clocks, but it will be understood that the invention is not limited in its application to that particular class of machine, and that it may be applied to any use of which it is susceptible.
It is well known that all metals are capable of some degree of expansion and contraction, and some metals have this property in greater degree than others. The amount of expansion for each degree rise in temperature is quite regular, and is called the co-efficient of expansion. It is also well known that zinc has this property in greater degree than any other of the solid metals, its co-efficient of linear expansion being appreciably higher. For this reason, as well as because of its relatively low cost, I preferably make use of zinc in the construction of the expansible parts of my apparatus.
One of the objects of my invention, therefore, is to provide an expansion device of novel construction and arrangement, which will generate energy and maintain motion during changes in temperature, to such an appreciable and useful amount, as to constitute it in fact a temperature motor.
A further object of my invention is to provide means for accumulating or storing the energy thus generated.
A further object is to provide means for applying the energy thus generated and stored.
Other objects, such as compactness, durability and comparatively low cost of the apparatus, will appear in the following description, in which reference is had to the accompanying drawings.
In the drawings:—
[Fig. 1] is a front elevation, showing the application of my invention to a clock provided, in this case, with a mainspring as usual;
[Fig. 2] is a rear elevation of the same with a part removed;
[Fig. 3] is an enlarged perspective detail showing how the strips forming part of the expansion member or coil are connected up;
[Fig. 4] is a sectional view, on lines 5—5 of [Fig. 1];
[Fig. 5] is an enlarged detail elevation, with parts removed;
[Fig. 6] is an enlarged detail cross section of the central portion of the apparatus, with part broken away;
[Fig. 7] is a rear elevation of the same with parts broken away;
[Fig. 8] is an enlarged detail of the upper portion of the apparatus shown in [Fig. 4], with parts removed;
[Fig. 9] is a perspective detail, partly broken away;
[Fig. 10] is an enlarged detail of a portion of the ratchet mechanism shown in the lower portion of [Figs. 6] and [7];
[Fig. 11] is an enlarged section of a flexible coupling shown in [Fig. 7];
[Fig. 12] is an elevation of a modification of the expansion coil;
[Fig. 12ª] is a perspective view showing how two of such modified expansion coils may be connected;
[Fig. 13] is a front elevation showing my invention applied to another form of force storage mechanism;
[Fig. 14] is a plan view of same, on lines 14—14 of [Fig. 13];
[Fig. 15] is a rear elevation on lines 15—15 of [Fig. 14];
[Fig. 16] is a vertical section on lines 16—16 of [Fig. 14];
[Fig. 17] is an enlarged detail of part of the apparatus shown in the upper portion of [Fig. 16];
[Fig. 18] is an enlarged detail of the ball-discharging means shown in the lower portion of [Fig. 16];
[Fig. 19] is an enlarged detail of the loading device shown in the opposite part of the lower portion of [Fig. 16]; and
[Fig. 20] is a plan view on lines 20—20 of [Fig. 13].
Referring to the construction illustrated in [Fig. 1] to 11, inclusive, B represents the outer frame of the apparatus.
Mounted within the outer frame B is an inner frame comprising the uprights C, C¹, which are rigidly secured by cross-bars D¹, D².
The outer frame B, as well as the inner frame uprights C, C¹ are preferably formed of wood or other material capable of a low degree of expansion.
Within the upper and lower ends of the inner frame are anti-friction knife-bars E, E¹, the upper one of which, E, has each end within a vertically disposed slot E² in the uprights C, C¹, within which said knife-bar may be moved vertically, as hereinafter described.
Each end of the lower knife-bar E¹ lies immovable within a recess in a plate E³ mounted on each of the uprights C, C¹.
These knife-bars, which are preferably formed of hardened steel, have oppositely disposed relatively sharp edges E5, which act as bearings for a series of horizontally disposed anti-friction levers, F, F¹, which I will term balance-levers, since they are intended to balance evenly and freely on the thin edges of the knife-bars with little friction somewhat in the nature of a scale-balance. These levers are pivotally connected to a series of metallic expansion strips G, G¹, G², G³, etc., the construction and arrangement and manner of connecting up the same being more clearly shown in [Fig. 3].
It will be observed that the arrangement of the levers F and expansion strips G, G¹, etc., is such as to form, in effect, a spiral, the short strip G being connected to one end of one of the balance-levers F, and the strip G being connected at its lower end to the opposite end of said lever, the upper end of said strip G¹ being connected to one end of the first one of the levers F¹. To the opposite end of said lever F¹ the upper end of strip G² is connected, the lower end of said strip being connected to the left-hand end of the second one of the levers F, and so on to the final short strip Gx. The levers F, F¹ must be formed of a metal capable of withstanding great strain without bending, and for this purpose I prefer to use the metal known as macadamite.
For convenience of designation, I will refer to each of these groups of balance-levers F, F¹, and expansion strips G, G¹, etc., as expansion coils, and while I have herein shown but two sets of such expansion coils, it is to be understood that there may be any number of such sets desired, and any desired number of strips and levers composing such coils, depending upon the character of the work to be performed.
Furthermore, I desire it to be understood that when I use the terms “strips"—as characterizing the members connecting the balance-levers—either in the specification or claims, I do not limit myself to the form of connecting member or “strips” shown, but mean to include in the use of the term “strips” any other form such as wires, rods or bars of either square, round, hexagonal or other cross sectional shape.
The ends of the short strips G, Gx are connected by wires H, H¹ with the opposite ends of what I will term a coil lever I, which, as more clearly shown in [Fig. 5], is keyed to a shaft J, which latter has its end journaled upon the cross-bars J¹, J² secured to the uprights C, C¹ of the inner frame of the apparatus, and this shaft I will name a coil shaft.
Keyed to the coil shaft J is a lever K, which it may be proper to designate as a stress lever, since from it is suspended a weight K¹, the function of which is to place a certain amount of stress upon the series of expansion strips and balance-levers composing the expansion coil, keeping the metal of the strips slightly stretched and preventing any loss of motion at the different points of connection, and thereby furthering a very important object, which is to make of each series of expansion strips
and balance-levers a single spiral unit, throughout which the expansion and contraction of the strips are transmitted.
Also keyed to the shaft J is a power transmisson lever L, and any rotary motion imparted to said shaft is necessarily imparted to the lever L in the form of reciprocating motion.
Referring now to the power storage device, one or a number of which may be used in connection with my expansion coils.
Disposed approximately midway of the uprights C, C¹ and within casing M, secured at its ends to said uprights, is rotatably mounted a power transmission shaft M¹, keyed to which is a spur wheel M². Also mounted on the shaft M¹ is a spur wheel M³, meshing with which at its upper and lower sides are two spur wheels M4, M5, loosely mounted upon short supporting shafts M6, M7, journaled in uprights M8, M8 secured to the casing M. To each of the spur wheels M4, M5 is secured the outer end of a coil spring M9, M10, respectively, the inner ends of said springs being secured to the respective shafts M6, M7, the arrangement being such that when the springs are placed under tension by the rotation of the shafts M6, M7, the force of the springs rotates the spur wheels M4, M5, thereby rotating the spur wheel M³, shaft M¹ and the spur wheel M².
Also mounted upon each of the respective short shafts M6, M7, and keyed thereto, is a ratchet wheel M11, M12, and adjacent thereto and loosely mounted upon each of said shafts M6, M7 is a pawl carrier plate M13, M14, each carrying a pawl indicated at M15, M16, which is adapted to engage the teeth of the ratchet wheels M11, M12, being held in engagement therewith by springs, one of which is shown at M17, secured to said pawl carrier M13. Suitably mounted upon the casing M, and adapted to engage the teeth of the ratchet wheels M11, M12, is a detent M19, to prevent reverse movement of said ratchet wheels.
The pawl carrier plate M13 is provided with a pin M21, and secured thereby loosely to said carrier is one end of a connecting rod M21ª, the other end of said connecting rod being connected to one end of a longitudinally flexible coupling M22, the other end of said coupling being secured by means of the connecting rod M23 to the power transmission lever L. The function of the flexible coupling M22 will be hereinafter referred to.
The pawl carrier M13 also carries, at its lower end, a pin N, and loosely mounted thereon is one end of a connecting rod N¹, the other end of said rod being connected to a pin N² secured to the pawl carrier M14, whereby, when motion is imparted to pawl carrier M13 and, through the pawl M15 to the ratchet wheel M11, motion is imparted to the pawl carrier M14, and through its pawl M16 to the ratchet wheel M12. From the pin N² is suspended a weight N³ to return the pawl carriers to their lowermost positions when they complete their upward travel.
The flexible coupling M22 comprises a tubular casing N4, which is provided at one end with an opening N5, through which projects a rod N6 having a head N7, which is adapted to bear against a spiral spring N8 mounted within said casing, the other end of said rod N6 being connected to the rod M23.
The operation of the apparatus, as thus far described, will be more readily apparent from an inspection of [Fig. 5].
Assuming that the expansion coil there shown has been subject to a normal temperature of say 75 degrees Fahrenheit, and at that temperature the lever L is in the position shown in full lines on a decrease in temperature of say 10 degrees, the contraction of the coil, which will operate upon its entire length, will exert a pressure at the ends thereof in the direction of the arrows, the result of which will be to rotate the shaft J and raise the lever L against the force of the weighted lever K (carrying the latter therewith) to the position shown in dotted lines, thereby actuating the ratchet wheels M11, M12, and winding up the springs M9, M10, of the power-storage device, the force there stored being afterwards taken off, as required, through the medium of the power transmission shaft M¹ and spur wheel M² and any suitable gearing or power transmission means.
The function of the flexible coupling indicated at M22 will now be quite clear. It will be seen that the coil spring N8 will be sufficiently strong not to give under the pull of the lever L except when the springs M9, M10 are wound full. When that condition exists, the coil spring N8 will give, under the force of the lever L, and
no further power will be applied to the springs M9, M10. When, however, those springs have become unwound to a sufficient extent the spring N8 of the coupling M22 will be stronger than the springs of the power-storage device and will transmit, from the expansion coil, the force necessary to wind said springs as often as they become unwound; in other cases the force will be expended in simply compressing the coil spring N8 without effect upon the springs of the power-storage device.
Referring now to what I will term the force-increasing devices, which are more clearly shown in Figs. [1], [2], [4], [8] and [9].
Near each end of the upper knife-bar E, and contacting therewith at its under surface, is a support O, in the form of a flat-headed bolt (Fig. 8), the shank of said bolt passing through one end of lever O¹, which is fulcrumed at O² upon the upper surface of a cross-bar O³ securely fastened to the rear portion of the uprights C, C¹. To the front of said uprights is rigidly secured a second cross-bar O4, and at the lower portion of said uprights and rigidly secured thereto is a third cross-bar O5, against the under surface of which rests a lever O6 (Fig. 9) having its fulcrum point at O7.
As shown in [Fig. 2], there are three sets of the levers O¹, at the upper end of the expansion coils at the rear side thereof below the knife-bars E, one lever at each end of said bar and one in the middle thereof. As these levers act directly upon the under surface of the knife-bars E to raise the same I will call them knife-bar lifting-levers. There are also the same number of levers O6 at the lower end of the expansion coils below the cross-bar O5 projecting through to the forward side of the apparatus, as shown in [Fig. 1].
Rigidly secured to the cross-bar O4 is one end of a relatively heavy metallic expansion strip O8,—preferably formed of zinc—the lower end being secured to one end of the lever O6; to the opposite end of the lever O6 is secured the lower end of a similar but longer zinc strip O9, the upper end of the strip O9 being secured to the rear end of the lever O¹. As shown in [Figs. 1] and [2], there are two of these strips O8 at the front and two of the strips O9 at the rear of the apparatus.
In addition to the heavy strips O8, O9, there is provided at the front of the apparatus a heavy wide expansion sheet or strip O10, which, at its upper end, is rigidly secured to the cross-bar O4, and at its lower end to the front end of the middle one of the levers O6. A similar heavy wide expansion sheet or strip O11 is secured, at its lower end, to the rear end of the middle lever O6, and, at its upper end, to the middle one of the levers O¹.
These heavy strips O8, O9 and sheets O10, O11 are preferably formed of zinc, and are not only capable of great expansion and contraction, but will be capable by their contraction of lifting the entire weight of the knife-bars E, with the carried balance-levers and expansion strips of expansion coils, the operation thereof being as follows:
The front strips O8 and rear strips O9 and the front sheets O10 and the rear sheets O11 are connected to the levers O6, so as to form, in effect, single expansion strips and sheets of relatively great length. They are fastened, however, at their front upper ends to the cross-bars O4, so that the expansion cannot extend beyond that point and takes place in a direction towards the opposite end, and, of course, the contraction takes place in the opposite direction. Assuming now that at a temperature of say 75 degrees Fahr. these heavy strips and sheets lie in the position shown in [Figs. 4] and [9] (the heavy strips O8, O9 being shown in [Fig. 9], and the heavy wide sheets O10, O11 in [Fig. 4]), on a decrease in temperature of say five degrees Fahr., the heavy strips O8, O9 and sheets O11, O12 will contract in the direction of the arrows, depressing the rear ends of the levers O¹, O6, and thereby through the levers O¹ lifting the knife-bars E, and the balance-levers suspended thereon, with the result that the force normally exerted at the ends of each expansion coil is increased to the extent of the lifting power of the contraction of the metal strips and sheets.
I have found by experiment as well as observation that the average daily change of temperature in residence and office buildings is about five degrees. Sometimes the changes will be much greater, and sometimes less. On even a low average of temperature change, my apparatus will be able to generate force in larger amounts than required, and the surplus will be stored in a power-storage device such as above described, or by means hereinafter referred to, which surplus will
be drawn upon when it should happen that the average temperature is approximately uniform.
For clearness of illustration, I have shown, as above stated, but two sets of expansion coils, but there is no limit to the number that may be used. Assuming that we have an apparatus with four expansion coils, each knife-bar holding 50 balance levers, giving a total of 200 levers, with expansion strips of the same number, in 5-foot lengths, we would have a total of 1,000 linear feet of zinc strips, which entire length of strips will, on the slightest change of temperature, get longer or shorter. The expansion and contracting of this 1,000 feet of zinc strips for every temperature change of 5 degrees Fahr. will be 1 inch. Now, assuming that the knife-bars are pulled upward by heavy strips O8, O9, and sheets O10, O11 of five feet length (making ten feet for the front and rear strips and sheets), on a decrease in temperature of 5 degrees Fahr. the upward movement of those bars will be 10-1000 of one inch; this contraction (10-1000) will now be multiplied as many times as there are levers and strips in the expansion coils, viz., 200 times, which would be 2 inches, and this, together with 1 inch from the contraction of the expansion coils alone, will give a total movement of 3 inches. If the strips are of a capacity to pull or lift 100 pounds, we obtain a lift of 100 pounds 3 inches. As thirty-three per cent approximately must be deducted for loss by stress (it being necessary to place the coils under strain, as shown in the drawings and described above), the final result will be a power to lift 100 pounds 2 inches, or 10 pounds 20 inches, and this force will be sufficient to run a large sized time clock with powerful striking force.
As illustrated in [Figs. 4], [5], [6] and [7], the power applied by the springs M9, M10 to the power transmission shaft M¹ is taken, through the spur wheel M² by means of any suitable gearing, to run a clock or any other machine adapted to the purpose. As there illustrated, I show the spur wheel M² meshing with a pinion P, through which is driven the spur wheel P¹, which latter meshes with a pinion P², through which is driven a sprocket wheel P³ carried by the bracket P4, which latter, as well as the shafts carrying said spur wheels and pinions, are supported by an upright P5 mounted upon the casing M. The sprocket wheel P³ carries a sprocket chain P6, which, through any suitable gearing, is adapted to wind the main spring of a clock indicated at Q, carried by suitable supports on the cross-bar Q¹ secured to the uprights C, C¹. As this clock may be of any well known form, it will not be necessary to describe the same in detail, except to state that as soon as the main spring of the clock becomes weaker than the springs of the power-storage device illustrated in [Fig. 7], the latter will wind the clock main spring, and as in this manner it is wound frequently, it is always kept at a uniform high tension, which is desirable and results in good time-keeping.
In [Fig. 12] I show a modification of my invention, wherein, instead of having the balance-levers F, F¹ arranged side by side, they are superposed one above the other, in this case a plurality of knife-bars E, E¹ also being superposed one above the other, the expansion strips G, G¹, etc. (in this case shown as formed of wires or rods), and balance-levers being arranged in the same plane, somewhat in the nature of a coiled spring, the coil shaft being indicated at J and the coil lever at I, to which are connected the end expansion strips G, Gx, and the weight K¹ for placing the coil under tension. By this arrangement of balance-levers and expansion strips, in the same plane, much economy of space is effected, and when desired, a great number of such coils may be suspended upon the series of knife-bars.
In [Fig. 12ª] I show two such coils connected in series, the terminal expansion strip Gx of the front coil being connected to one end of the lever I, and the opposite terminal G of that coil being connected to the shortest one of the rear set of levers F1ª, the terminal Gy of the rear set being connected to the other end of the lever I. Thus two or more such coils may be connected, and the force of expansion and contraction of the combined coils transmitted to the lever I. When a number of such combined coils are suspended from the knife-bars E, E¹, the levers connecting their respective terminals may be themselves connected by a system of compound levers such, for example, as shown in [Fig. 13], to be hereinafter referred to.
Referring now to [Figs. 13] to [20] inclusive. These figures illustrate another form of the invention whereby not only the power-storage device of the preceding
figures may be dispensed with, but also the main spring of the clock there shown, both of these elements being supplanted by apparatus effecting the raising and lowering of weights (in this instance shown in the form of balls), the force of expansion and contraction of the coils being utilized to operate a rotary member which elevates a series of weights and discharges the same into a storage receiver, the clock (or other machine) being operated through the energy so stored and given up by the falling of said weights.
As illustrated in said figures, this feature of the invention consists of a frame, indicated in whole at 10, located about midway the length of the expansion coils shown in [Fig. 1], and it may be supported by securing it to the uprights C, C¹, or in any other suitable manner.
Said frame comprises two horizontally disposed longitudinal framing members, 10ª, 10b, which are connected at each end by cross-bars (not shown).
Mounted on the supports 10ª, 10b, are four uprights, 12ª, 12b, 13ª, 13b. The uprights 12ª 12b are connected at their upper ends by a longitudinal framing member 14ª, and the uprights 13ª 13b are connected by longitudinal framing member 14b, said framing members 14ª 14b being also in turn connected at their ends by transverse bars (not shown), said members constituting an open frame for the working parts of the apparatus.
Mounted respectively upon the longitudinal framing members 10ª 10b, approximately midway thereof, are two standards, 16ª 16b, which are rigidly secured together by a cross-bar 17, said standards and cross-bar constituting a rigid support for the gearing now to be described.
Rotatably mounted upon the standards 16ª, 16b is a driving shaft 18, one end of which is journaled in the standard 16ª, and the other end in a bearing-bolt 19 passing through the standard 16b, which, being threaded, is capable of fine adjustment.
Mounted upon and keyed to the shaft 18 is a wheel 19, the spokes 20 of which support a rim 21, within which are set a series of pockets 22, the inner surfaces of which are so shaped as to permit their receiving successively, at the bottom of the wheel, a series of balls 23 and holding the same during a travel of 180 degrees, or one-half revolution of the wheel, when they are discharged as hereinafter described. This wheel I will term an energy-storing wheel, since it acts through the force taken from the expansion coils to raise the balls, the lowering of which is to drive the wheel now to be described.
Loosely mounted on the shaft 18 is a wheel 24, smaller in diameter than the wheel 19, the spokes 25 of which, secured to the hub 26, support a rim 27, within which are set a series of pockets 28, which are adapted to receive successively, at the top of the wheel, the balls 23, and discharge the same when they have been lowered through 180 degrees or, in other words, at the bottom of the wheel. The inner wall of the pockets 28 is formed, for the most part, with a pronounced rounded groove (indicated at 28ª), as shown above the ball in [Fig. 18], which groove lies under the ball when the pocket is in its uppermost position, as shown in [Fig. 17], said groove becoming less pronounced at one edge towards the opposite portion of the pocket, at which point it has an approximately level surface at one side, as shown in [Fig. 18], and indicated at 28b; the subject of this arrangement being that the ball may be readily discharged in this position, and securely held within the pocket when the ball and pocket are in other positions. The wheel 24—which I will designate as the power-transmission wheel—is supported upon ball bearings indicated at 28c, 28d, which are held in position by collars 28e, 28f, both keyed to shaft 18.
Mounted upon a collar 29, which is keyed to the driving shaft 18, is a ratchet wheel 30, engaging the teeth of which are two pawls 31, 32, secured to one arm of a double-arm pawl-carrier 33, the other arm of which is connected by a rod 34 to a lever 35, one end of which lever is pivotally connected to a standard 36, secured to the frame, and the other end of which is provided with a weight 36ª.
Near the inner end of the lever 35 connection is made by means of the connecting rods 37 and 38, link 39 and rods 40, 41, with two levers indicated at L, L, which are adapted to take power from the expansion coils heretofore described, through the coil shafts J, J, to which shafts are also connected the coil levers I, I, the ends of the latter being connected to the strips G, Gx of the expansion coil by the wires H, H¹, as already set forth and clearly illustrated in [Figs. 2], [3], 5, 6 and 7.
As illustrated in [Fig. 13], upon contraction of the
| Fig. 8. | Fig. 10. |
| Fig. 9. | Fig. 11. |
expansion coils, the wires H, H¹ will be pulled in the direction indicated by the arrows, the ends of the long arms of the levers L, L—through the movement of the shafts J, J—will rise, thereby, through the rods 40, 41, link 39 and rods 38, 37, raising the lever 35, and through the rod 34 actuating the pawl carrier 33, and through the pawls 31, 32, imparting rotary motion to the ratchet wheel 30, and, through it, to the shaft 18 and the power-storing wheel 19, said pawl carrier being returned to its normal position by the weight 36ª. Motion of said wheel and shaft in the reverse direction is prevented by means of a ratchet wheel 42, keyed to the collar 29, engaging the teeth of which wheel is a detent 43, carried by a plate 44, secured to the supports 45, affixed to the standard 16ª.
The hub member 26 of the power transmission wheel 24 is provided with a sprocket wheel 46, which is adapted to engage and drive a sprocket chain 47, and thereby drive the great wheel of a clock mechanism or gearing of any other machine adapted to the purpose.
Having shown the mechanism for driving the energy-storing wheel 19, which, as already stated, is keyed to the shaft 18, I will now describe the mechanism for driving the power transmission wheel 24, which runs loose on the shaft 18.
It will be seen from an inspection of [Fig. 16] that the wheel 19 is of greater diameter than the wheel 24.
Suitably mounted between said wheels, on cross-bars 48, 49, I provide a series of ball-storage runways designated in whole at 50 (see [Fig. 14]), and, as shown in [Fig. 16], these runways are laterally inclined downwardly from the wheel 19 to the wheel 24.
Similar ball runways designated in whole at 51 are provided at the lower portion of said wheels and between the same (Fig. 20), being mounted upon cross-bars 52, 53, but the last named runways are laterally inclined in the reverse direction to that of the runways 50.
The ball-storage runways 50 comprise inclined floor members 54, 54ª, 54b, each having longitudinally a slight downward inclination in the direction of the arrows. These runways also comprise longitudinally extending walls 55, 56, 57, 58, one end of the wall 55 being curved to meet one end of the wall 57, leaving a passageway 59 between it and one end of the wall 56. One end of the wall 58 is similarly curved to meet one end of the wall 56, leaving a passageway 60 between it and one end of the wall 57. Thus are provided parallel runways 61, 62 and 63, with passageways from one to the other, whereby a ball deposited in runway 61 will move continuously from that end of the series of runways to the other end. The runway 61 is provided with an end wall 61ª, and adjacent thereto the longitudinal wall 55 is provided with an opening 61b to permit the passage therethrough successively of balls from the energy-storing wheel 19 to the runway 61.
Projecting through the standard 16b is a threaded bolt 63ª, the end of the shank of which is beveled, as clearly shown in [Figs. 14] and [16], the function of which is to eject from the uppermost pocket 22 of the wheel 19, as the same revolves, the balls 23, and thrust them successively into the runway 61.
At the lower end of the runway 63 is provided a laterally movable receptacle 64, which has a receiving capacity of one ball only. Said receptacle comprises a base 65 and perpendicular stop 66. The base 65 is connected to the floor member 54b of the runway 63 by a horizontally disposed hinge 67, and to it is also affixed a plate 68, carrying a downwardly extending lever arm 69, which is formed at its lower extremity with an outwardly curving portion 70, which is adapted to engage with the spokes 25 of the wheel 24 and be thereby pressed inwardly, the result of which is to depress the outer end of the base 65 of the ball receptacle 64, inclining the same in such position that the ball therein will fall into the adjacent pocket of the wheel 24, the ball being prevented from falling therefrom on the opposite side by the stop 71 secured to the standard 16ª. The center of gravity of the lever arm 69 is such that when the curved lower portion is in its normal forwardly extended position the rear side of the base 65 of the receptacle 64 will be depressed and the forward side elevated, so that the forward side will normally project above the floor level of the runway 63 and serve as a stop to prevent more than one ball occupying any of the space within said receptacle at one time.
The ball-storage runways 51 comprise inclined floor members 72, 72ª, 72b, each having a slight downward inclination longitudinally in the direction of the arrows. They also comprise longitudinally extending walls 73,
74, 75 and 76, one end of the wall 73 being curved to meet one end of the wall 75, leaving a passageway 77 between it and one end of the wall 74. One end of the wall 76 is similarly curved to meet one end of the wall 74, leaving a passageway 78 between it and the other end of the wall 75. There are thus formed parallel runways 79, 80 and 81, with passageways from one to the other, whereby a ball deposited at the other end of the runway 79 will move continuously from that end of the series of runways to the other end. The runway 79 is provided with an end wall 82, and adjacent thereto the longitudinal wall 76 is provided with an opening 76ª to permit the passage therethrough, at intervals, of balls from the power-transmission wheel 24 to the runway 79. Adjacent the wall 82 is perpendicularly disposed pin 82ª whereby the balls, as they pass through the opening in the wall 76 are deflected to pass through the runway 79 in the direction of the arrow.
At the lower end of the runway 81 is provided a laterally movable receptacle 83, which has a receiving capacity for one ball only. Said receptacle comprises a base 84 and end stop 85. Said receptacle is horizontally hinged at 86 to the floor member 72 of the runway 81, and is provided with an outward extension 87, which is adapted to be engaged by a shoulder 88 on the ball pockets 22, and thereby depress the outer edge of the base of the receptacle in such a way as to eject the ball therefrom, and place the same in the pocket of the wheel 19.
It will be seen that the hinge 86 (Fig. 19) is off center and when the base 84 of the receptacle 83 is depressed at the rear the upper end of a pin 89, projecting upwardly from the base 84 contacts with the upper portion of the wall 74, thereby preventing the rear portion of the base being depressed too low. When a ball is in said receptacle, the forward end will be elevated so that a portion of the side edge of the base will be projected above the floor member of the runway 81, serving as a stop to prevent more than one ball occupying any of the space within said receptacle. When one ball moves into a pocket 22, another ball quickly moves into the receptacle, taking its position at the rear thereof. This operation takes place when the base 84 is level with the floor member of the runway 81, the outer end of the base rising as soon as the pocket and its ball have passed by the projection 87.
It will be seen that the energy-storing wheel 19, which takes its motive power through the shaft 18 from the expansion coils, acts to raise the balls or weights from the lower ball runways 51 to the ball storage runways 50. The wheel 19 may act at more or less irregular intervals, while the power transmission wheel 24 acts—and must act—continuously and regularly. This wheel takes and transmits power from the lowering of the balls, which are delivered to it when the pockets are in the position of the one shown uppermost in [Fig. 15], and are discharged from the pockets when in the position of the one shown lowermost in said figure, in which position of the wheel the approximately flat surface of the pocket (Fig. 18) is lowermost, or under the ball, permitting ready discharge of same. From the delivery side of the power transmission wheel 24 the balls are discharged into the runway 79, being deflected into proper direction by the pin 83ª, thence passing through the passageway 78 through the runway 80 in the direction of the arrow, thence through the opening 77 into the runway 81, thence into receptacle 83, and when the shoulder 88 of the energy-storing wheel 19 reaches a point opposite said receptacle the base of the latter is depressed, which results in passing a ball into the wheel pocket; as the wheel turns and the next pocket arrives in position another ball is taken on, and so on, as long as there are any balls in the lower runway. When a ball on the wheel 19 reaches the uppermost position, as shown in Fig. 16, it contacts with the ejector 63ª and is thereby passed into the runway 61 and thence to the lower end of that series of runways, and in the same way the balls following will take position in the upper series of runways.
It will be understood that when my invention is applied to the operation of a clock the power taken from the power transmission wheel 24 will be given up gradually, being controlled by the pendulum or balance wheel governed escapement in the usual way.
In the application of my invention as last above described the apparatus will be designed and built to furnish energy sufficient not only to run the clock, but provide a surplus for storage. On some days the variation in temperature may be but two or three degrees, and on
other days it may be as high as twenty degrees. If the clock requires for its operation the lowering of three balls each day the apparatus will be so arranged that with an average daily temperature variation of, say, six degrees, four balls will be raised, of which three will operate the power transmission wheel and one will be held in storage. With a variation of twelve degrees, eight balls will be raised, of which five balls will be left in storage. If the ball storage runways each have a holding capacity for one hundred balls, and the variation in temperature is greater than required, the balls will soon be lifted from the lower to the upper runways. Assuming that on certain days there will be no variation in temperature, and as a result the energy-storing wheel should not revolve, the running of the clock will not be interrupted, for the power transmission wheel will continue revolving, taking its power from the balls in storage.
I wish it understood that I do not confine myself to the precise details of construction and arrangement of parts as herein set forth and described or to the materials specified, as modification and variation may be made without departing from the spirit of the invention as defined by the appended claims.
BANGERTER’S NON-ELECTRIC REGULATOR
TIME CLOCK
ANNIVERSARY SELF-WINDING
The Bangerter Anniversary Self-Winding Regulator deserves this title because its construction embodies all the principles essential to a Regulator to be the very best time-keeper. “Graham dead-beat escapement” and a pendulum provided with means for keeping its gravity always the same length, overcoming the variation which change in temperature invariably brings about.
Another great improvement is the daily Self-Winding System, winding a weight which is the only means of maintaining an even pull to the delicate works of the clock. Wound by a force which requires attention one minute a year only.
This invention relates to clocks, and particularly that class wherein a pendulum escapement is employed and wherein the clock-train is weight driven.
It is well known to those skilled in the art that the most accurate and reliable clocks are those which are driven by a weight. Most of such clocks are provided with a plurality of weights, one being used to supply the energy necessary to strike the time, and the other the energy for operating the clock-train, and in clocks of such construction they have to be wound frequently, usually either daily or weekly.
Many attempts have been made to produce clocks which will run for a relatively long time without requiring the attention of an attendant to wind the same. In such clocks (other than electrical clocks) powerful springs have been employed, one of such springs being used for time-striking and the other for actuating the clock-train. Clocks of this class designed to run for an extended length of time, such, for example, as period of, say, a year or more, have been indifferent time-keepers, due to the fact that the power of the springs becomes materially lessened during the latter part of the cycle of operations. Therefore, spring-operated clocks, calculated to be run for any great length of time, have been more or less unsatisfactory, and have not gone into very extensive use.
The object of my invention is to provide a clock which will not require the attention of an attendant but once in a long period of time, and which will also be an accurate time-keeper.
A further object is to provide a clock operated by a uniformly pulling weight, the pull of which is not varied by the lifting of said weight.
A further object is to provide a power-storage device and power transmission mechanism and automatic devices connected thereto, whereby the power of said power-storage mechanism is utilized to wind up the clock—that is to say, to lift the clock-train operating weight at certain definitely recurring intervals of time.
A further object of my invention is to provide, in connection with such power-storage mechanism, time-striking means operated by said power-storage device, which being independent of the clock-train operating means does not interfere therewith.
A further object of my invention is to provide a single power-storage mechanism which will afford the power to strike the time and effect the winding of the clock, doing away with two sets of mechanism (one for each purpose), as heretofore used.
A further object of my invention is to provide such a power-storage device that with one winding of the same the clock may be kept running, and also striking the time, for a year or more in duration.
A further object of my invention is to provide means in connection with said power-storage device whereby the winding of the clock-train does not interfere with continuous running and perfect time-keeping of the clock, and does not require any supplemental propelling mechanism for the clock-train during the winding operation.
BANGERTER’S FIRE DETECTOR AND FIRE ALARM.
This is the most marvelous little machine that science has ever devised to watch your house day and night. It is the truest of all Watch Dogs and will in case of fire make such a loud and noisy alarm that you will wake up from the deepest of sleeps. It calls when the fire is at its infancy, in time to save you and your beloved ones. It is a most simple little apparatus requiring no electricity, no wiring or connections, no care of any kind; just as reliable after it has been hanging in your room for twenty years as it was when newly installed.
BANGERTER’S FIRE ALARM AND SPRINKLER.
More than a hundred million dollars is the yearly loss by fire in the United States; 50 per cent. of this loss is by water. How important therefore is Bangerter’s “Watch Dog Fire Alarm and Sprinkler,” regulated to ring, first a loud call when a fire is in its infancy. A watchman or anyone hearing the call can rush to the place and extinguish the fire. The sprinkler will only work when the alarm call is not attended to. Our Fire Alarm and Sprinkler system can be connected to piping from the water main, or to the tank on the roof of a building, but can also be installed in any place if there should be no water piping or tank. In this case a water tank of from twenty to one hundred gallons of water has to be installed. This tank can be set in any out of the way place. Compressed air keeps this water under high pressure, and in case of fire the valves are automatically opened and the sprinkler will act with efficacious result.
BRIEF BIOGRAPHY
OF
FRIEDRICH BANGERTER
Friedrich Bangerter can justly lay claim to being one of this country’s leading inventors.
He has some fifty inventions to his credit.
He has been honored with Silver and Gold Medals and Diplomas.
His displays at great World’s Expositions have occasioned the utmost favorable comment.
His splendid record speaks for itself and shows the profound student, the practical machinist and brainy inventor of worldwide experience with a long list of successes to his credit.
Born in Lyss, Switzerland, in 1868, at the age of 16 he entered the machine shop of his town’s watch factory as an apprentice. There he was favored with the opportunity to become familiar with all sorts of tools and machines used in making watches.
By the age of 22 he so progressed that “all by himself” he constructed all the necessary machines to make watches and added so many important improvements, embracing such automatic devices and machines in which hands, moving from place to place, picking up pieces of work, then setting them in the right positions (operating with such perfection and precision) that he was called a wizard. One of these automatic machines would pick up blanks from a wire, set them in the machine from one to twenty-four at a time and cut the teeth of watch gearing perfectly.
Another of Bangerter’s machines would take small, smooth, round steel rods and automatically make perfectly finished pinions with pivots, shoulders and smallest holes.
An automatic trumpet of his invention would play a complete tune and was so simple in operation that a one-year-old child, by simply blowing in it, could play it.
United States Patent 543668 for a Hair Clipper, issued to F. Bangerter, San Francisco, is specified as follows:—
543668. Hair Clipper. Fred Bangerter, San Francisco, Cal., assignor, by mesne assignments, to Charles H. Greene, same place. Filed July 21, 1894. Renewed July 2, 1895. Serial No. 554,715. (No model.)
Claim 1. In a Hair Clipper, the combination of the stationary and movable plates, a pair of pivoted handles, one of said handles being hinged or connected with one of said plates so that the device may be turned to different angles, an opposing plate having its rear portion recessed and provided with rearwardly and upwardly extending curved arms, and the other handle having arms adapted to enter the recess of said plate and engage the curved arms thereof in whatever position the device is turned.
In 1892 he exhibited an automatic figure in a big department store in San Francisco which drew a complete portrait of Christopher Columbus.
United States Patent 512089 was issued to Mr. Bangerter for an “Automatic Delineating Machine,” a toy doll which would correctly write the complete alphabet. Later he so improved this figure that it could spell and talk while writing.
At the Paris Exposition in 1900 he exhibited a most remarkable machine which made collar buttons. Three rods of metal were used at the same time—one to make the head of the button, one the bottom or base, and the other the stud. The three parts of the collar button were perfectly made and finished.
The head was drilled and tapped, the stud was threaded and screwed into the head while spun into the base or bottom. The manufactured collar buttons fell into a box at the rate of 300 an hour—thus effecting a great economy of metal.
In 1905, at the Belgium Exposition, he displayed an intensely interesting novelty—an “Automatic Jeweler"—which, with arm and hand, operated an ordinary machine which turned out perfectly made collar buttons of which thousands were sold within the Exposition Grounds.
A most marvelous contrivance was his four-spindle
automatic watch chain machine composed of over three thousand parts.
This machine made from wire of four different metals, namely, gold, silver, nickel and German silver, being fed into the machine at the same time would automatically make four watch chains of four different patterns completely and properly finished. The chain itself, an invention of Mr. Bangerter, was called the Bangerter Chain. Patent sold in France.