EP1654597A1 - Thermally-compensated balance wheel - Google Patents
Thermally-compensated balance wheelInfo
- Publication number
- EP1654597A1 EP1654597A1 EP04735863A EP04735863A EP1654597A1 EP 1654597 A1 EP1654597 A1 EP 1654597A1 EP 04735863 A EP04735863 A EP 04735863A EP 04735863 A EP04735863 A EP 04735863A EP 1654597 A1 EP1654597 A1 EP 1654597A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- balance wheel
- circumference
- disc
- balance
- pendulum
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G04—HOROLOGY
- G04B—MECHANICALLY-DRIVEN CLOCKS OR WATCHES; MECHANICAL PARTS OF CLOCKS OR WATCHES IN GENERAL; TIME PIECES USING THE POSITION OF THE SUN, MOON OR STARS
- G04B17/00—Mechanisms for stabilising frequency
- G04B17/04—Oscillators acting by spring tension
- G04B17/06—Oscillators with hairsprings, e.g. balance
- G04B17/063—Balance construction
-
- G—PHYSICS
- G04—HOROLOGY
- G04B—MECHANICALLY-DRIVEN CLOCKS OR WATCHES; MECHANICAL PARTS OF CLOCKS OR WATCHES IN GENERAL; TIME PIECES USING THE POSITION OF THE SUN, MOON OR STARS
- G04B17/00—Mechanisms for stabilising frequency
- G04B17/20—Compensation of mechanisms for stabilising frequency
- G04B17/22—Compensation of mechanisms for stabilising frequency for the effect of variations of temperature
- G04B17/222—Compensation of mechanisms for stabilising frequency for the effect of variations of temperature with balances
-
- G—PHYSICS
- G04—HOROLOGY
- G04B—MECHANICALLY-DRIVEN CLOCKS OR WATCHES; MECHANICAL PARTS OF CLOCKS OR WATCHES IN GENERAL; TIME PIECES USING THE POSITION OF THE SUN, MOON OR STARS
- G04B18/00—Mechanisms for setting frequency
- G04B18/006—Mechanisms for setting frequency by adjusting the devices fixed on the balance
Definitions
- the present invention relates to a pendulum of a watch movement made from a material having in particular a low coefficient of thermal expansion, such as diamond.
- the dimensional variations of a balance due to temperature variations, are one of the major problems of these objects; in fact, these dimensional variations, associated with those of the spiral spring associated with it, are a cause of variation of the oscillation frequency of the balance / hairspring system, respectively a cause of the lack of precision of a clockwork movement in function of the temperature.
- Means for compensating or correcting these variations have been proposed, for example the bimetallic balance wheel used in particular in marine chronometers.
- the disadvantage of such a rocker is its unfavorable aerodynamic shape causing poor penetration into the air during its oscillation movement and the difficulty of maintaining the center of gravity of the balance on its pivot axis. It can not be installed in a watch movement that must work in any position.
- a watch movement balance must have a mass as low as possible for as much inertia as possible, while having excellent mechanical strength.
- a material having a low coefficient of thermal expansion, a low density and a high mechanical strength these parameters being compared here to those materials usually used for the construction of rockers, as per for example, copper alloys or nickel.
- Several classes of materials fulfill these conditions: for example the non-metallic materials of the carbon group comprising, for example, diamond or else metal oxides including for example corundum such as sapphire or ruby, the list of materials mentioned here being absolutely not exhaustive.
- An object of the invention is therefore to provide a balance whose characteristics are significantly improved relative to those existing balances, in particular its behavior, respectively its insensitivity to temperature variations and its moment of inertia / mass ratio.
- a watch movement provided with such a balance, as well as a timepiece equipped with such a movement.
- FIG. 1 is a plan view of a balance wheel according to the invention
- FIG. 2 is a sectional view of a detail of FIG. 1.
- the balance 1 consists of a disc 10 obtained for example by chemical etching using a plasma (Deep reactive ion etching), or by any other method, a diamond plate of generally constant thickness.
- a rocker pivot 11 is fixed in known manner to the center of the disk 10.
- a plurality of fastening means 12, eight in the example shown, are arranged on a circumference 120 close to the outer perimeter of the disk 10.
- Ferrules or weights 2 are fixed on the disc 10 by the known fastening means 12.
- the rocker 1 is assembled in a known manner to a spiral spring, not shown in the figure so as not to overload, the latter being disposed under the plane of the disc 10 as shown in FIG.
- FIG. 1 shows some examples of execution of the flyweights 2, it being understood that generally a given balance has only weights 2 of a certain type.
- the weights 2 are essentially of shape or asymmetrically fixed relative to the circumference 120 on the disk 10.
- the disk 10 comprises eight weights in the form of elongate elements, as represented for example by the weight 20, and assuming that the balance 1 thus formed is subjected to an increase in temperature, the disc 10 made of very low coefficient of thermal expansion, for example diamond, will see its diameter increase only very slightly.
- the weights 20, that is to say made of a material with a thermal expansion coefficient that is much larger than that of the material constituting the disc 10, will have their dimensions increase by a ratio higher than that of the record 10.
- the oscillation frequency of the balance 1 depends in part on its moment of inertia, the latter parameter being equal to: mr 2 With: I: moment of inertia m. mass of the pendulum r: radius of gyration of the pendulum
- the radius of gyration is the radius of the circumference over which the whole mass m of a pendulum having the same moment of inertia as that considered would be concentrated.
- the oscillation frequency of the balance 1 also depends on the torque c supplied by the balance spring to said balance, this torque also varies with the temperature.
- I / c constant as a function of temperature.
- the mass m does not vary with the temperature, the shape, the dimensions and the positioning of the weights 20 will be determined so that for any temperature, the variation of the radius of gyration caused by the variation in diameter of the disk 10 is compensated by a corresponding variation of the radius of gyration caused by the dimensional variations of the weights.
- the disc 10 expands very slightly, thereby increasing its own radius of gyration. Due to the increased diameter of the disk 10, the attachment points 12 of the weights 20 also move on a circumference 120 of larger diameter.
- the weights 20 also increase their length, by a factor greater than the increase in diameter of the disc 10 since the coefficient of thermal expansion of the weights 20 is significantly higher than that of the material of the disc 10, and given the asymmetrical arrangement of weights on their attachment point, the portion of the mass of the weight placed on the side of the center of the disk 10 being generally larger than the portion of the mass of the weight placed in the direction of the outer perimeter of the disk, the center of gravity of the each weight moves towards the center of the disc 10, respectively the radius of gyration due solely to the flyweights decreases, partially compensating, completely or overcompensating the variation of the radius of gyration due to the disc.
- the phenomenon is exactly reversed in the event of a drop in temperature.
- FIG. 1 also shows other possible forms of flyweights 2, it being understood that they are only shown by way of example and in no way limit the possible forms making it possible to obtain the desired effect described hereinafter. above.
- the flyweight 21 is essentially triangular in shape with rounded corners, since its mass is distributed asymmetrically around its center of gravity, the adjustment of the degree of thermal compensation can be done by rotating the flyweight around its attachment point.
- the flyweight 22 is common at two attachment points.
- the weight 23 is in the form of an elongate bar, it can adjust its degree of compensation by varying the angle ⁇ that makes the axis of the weight to the radius of the disc. Another means of adjusting the degree of thermal compensation is shown on the weight 24 which has, for example an oblong hole 240 for adjusting the radial position of the weight.
- the weights of each pair of two radially opposed weights are adjusted symmetrically, so as not to create unbalance.
- at least one pair of orientable ferrules 25, generally known in the art, can be added to the device.
- the flyweights may be cut and formed in such a way as to reduce their friction in the air, as represented by way of example in FIG. 2.
- FIG. 1 shows a rocker disc provided with eight attachment points 12 of flyweights. It is understood that the balance wheel may comprise any number of attachment points, different from eight.
- Disk 10 is described above and shown as consisting of a solid disk. This embodiment is particularly advantageous in view of the friction in the air caused by the oscillation movements of the balance around its pivot, a balance in the form of a solid disc having a better aerodynamic behavior than a compound beam a center and a serge connected by arms.
- This form of execution in the form of a solid disc is achievable thanks to the low density of the material, the production of a solid disc not excessively peeling the mass of the disc 10.
- the disc 10 may not be absolutely flat and of constant thickness, it may also for example have a serge in the form of a flange on the outer perimeter of the disc.
- a rocker as described above, according to one or the other of its variants as well as made with one or the other of the materials adapted for this purpose, can be used advantageously with a made spiral it is also made of a material with a low coefficient of thermal expansion, such as diamond, as well as with a metal balance spring.
- the heat coefficient of the balance is then chosen so as to compensate for the thermal expansion of the spiral, low in the case of a diamond spiral and strong in the case of a metal balance spring.
Abstract
Description
Claims
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CH0300547 | 2003-08-13 | ||
CH21322003 | 2003-12-12 | ||
PCT/CH2004/000339 WO2005017631A1 (en) | 2003-08-13 | 2004-06-03 | Thermally-compensated balance wheel |
Publications (2)
Publication Number | Publication Date |
---|---|
EP1654597A1 true EP1654597A1 (en) | 2006-05-10 |
EP1654597B1 EP1654597B1 (en) | 2009-11-11 |
Family
ID=34195248
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP04735863A Active EP1654597B1 (en) | 2003-08-13 | 2004-06-03 | Thermally-compensated balance wheel |
Country Status (4)
Country | Link |
---|---|
EP (1) | EP1654597B1 (en) |
AT (1) | ATE448509T1 (en) |
DE (1) | DE602004024076D1 (en) |
WO (1) | WO2005017631A1 (en) |
Families Citing this family (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2842313B1 (en) | 2002-07-12 | 2004-10-22 | Gideon Levingston | MECHANICAL OSCILLATOR (BALANCING SYSTEM AND SPIRAL SPRING) IN MATERIALS FOR REACHING A HIGHER LEVEL OF PRECISION, APPLIED TO A WATCHMAKING MOVEMENT OR OTHER PRECISION INSTRUMENT |
GB0324439D0 (en) | 2003-10-20 | 2003-11-19 | Levingston Gideon R | Minimal thermal variation and temperature compensating non-magnetic balance wheels and methods of production of these and their associated balance springs |
WO2006123095A2 (en) | 2005-05-14 | 2006-11-23 | Gideon Levingston | Balance spring, regulated balance wheel assembly and methods of manufacture thereof |
US8100579B2 (en) | 2006-09-08 | 2012-01-24 | Gideon Levingston | Thermally compensating balance wheel |
EP2102717B1 (en) * | 2006-12-21 | 2013-06-26 | CompliTime S.A. | Mechanical oscillator for timepiece |
CH701155B1 (en) * | 2006-12-27 | 2010-12-15 | Complitime Sa | Balance spiral type mechanical oscillator for e.g. wrist watch, has balance and spiral, which are made of non-magnetic material such as diamond, where material possesses very low thermal expansion coefficient |
CH708926A3 (en) | 2013-12-05 | 2015-07-31 | Tgm Développement Sa C O Etude Tissot | Diamond mechanical part and method of manufacturing a mechanical diamond part for watch movement. |
CH708925A1 (en) | 2013-12-05 | 2015-06-15 | Tgm Développement Sa C O Etude Tissot | diamond mechanical room to watch movement. |
CH718969A2 (en) * | 2021-09-09 | 2023-03-15 | Rolex Sa | Inertial element for watch movement, resistant to magnetic fields. |
CN115091394B (en) * | 2022-08-22 | 2022-11-08 | 天津海鸥表业集团有限公司 | Positioning tool for balance wheel without clamping degree |
Family Cites Families (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CH88405A (en) * | 1920-03-15 | 1921-03-01 | Ravey Edouard | Watch balance. |
CH242883A (en) * | 1944-09-21 | 1946-06-15 | Marti Fritz | Regulator balance for watch movements. |
US5242711A (en) * | 1991-08-16 | 1993-09-07 | Rockwell International Corp. | Nucleation control of diamond films by microlithographic patterning |
FR2731715B1 (en) * | 1995-03-17 | 1997-05-16 | Suisse Electronique Microtech | MICRO-MECHANICAL PART AND METHOD FOR PRODUCING THE SAME |
ATE412205T1 (en) * | 2002-09-25 | 2008-11-15 | Fore Eagle Co Ltd | MECHANICAL PARTS |
-
2004
- 2004-06-03 EP EP04735863A patent/EP1654597B1/en active Active
- 2004-06-03 DE DE602004024076T patent/DE602004024076D1/en active Active
- 2004-06-03 WO PCT/CH2004/000339 patent/WO2005017631A1/en active Application Filing
- 2004-06-03 AT AT04735863T patent/ATE448509T1/en not_active IP Right Cessation
Non-Patent Citations (1)
Title |
---|
See references of WO2005017631A1 * |
Also Published As
Publication number | Publication date |
---|---|
DE602004024076D1 (en) | 2009-12-24 |
EP1654597B1 (en) | 2009-11-11 |
WO2005017631A1 (en) | 2005-02-24 |
ATE448509T1 (en) | 2009-11-15 |
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