EP2102717A2 - Mechanischer oszillator für uhr - Google Patents

Mechanischer oszillator für uhr

Info

Publication number
EP2102717A2
EP2102717A2 EP07857010A EP07857010A EP2102717A2 EP 2102717 A2 EP2102717 A2 EP 2102717A2 EP 07857010 A EP07857010 A EP 07857010A EP 07857010 A EP07857010 A EP 07857010A EP 2102717 A2 EP2102717 A2 EP 2102717A2
Authority
EP
European Patent Office
Prior art keywords
mechanical oscillator
balance
oscillator according
board
weights
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
Application number
EP07857010A
Other languages
English (en)
French (fr)
Other versions
EP2102717B1 (de
Inventor
Franck Orny
Stephen Forsey
Johnny Girardin
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Complitime SA
Original Assignee
Complitime SA
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Priority claimed from CH02119/06A external-priority patent/CH701155B1/fr
Application filed by Complitime SA filed Critical Complitime SA
Priority to EP07857010.8A priority Critical patent/EP2102717B1/de
Publication of EP2102717A2 publication Critical patent/EP2102717A2/de
Application granted granted Critical
Publication of EP2102717B1 publication Critical patent/EP2102717B1/de
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G04HOROLOGY
    • G04BMECHANICALLY-DRIVEN CLOCKS OR WATCHES; MECHANICAL PARTS OF CLOCKS OR WATCHES IN GENERAL; TIME PIECES USING THE POSITION OF THE SUN, MOON OR STARS
    • G04B17/00Mechanisms for stabilising frequency
    • G04B17/04Oscillators acting by spring tension
    • G04B17/06Oscillators with hairsprings, e.g. balance
    • G04B17/066Manufacture of the spiral spring
    • GPHYSICS
    • G04HOROLOGY
    • G04BMECHANICALLY-DRIVEN CLOCKS OR WATCHES; MECHANICAL PARTS OF CLOCKS OR WATCHES IN GENERAL; TIME PIECES USING THE POSITION OF THE SUN, MOON OR STARS
    • G04B17/00Mechanisms for stabilising frequency
    • G04B17/04Oscillators acting by spring tension
    • G04B17/06Oscillators with hairsprings, e.g. balance
    • G04B17/063Balance construction
    • GPHYSICS
    • G04HOROLOGY
    • G04BMECHANICALLY-DRIVEN CLOCKS OR WATCHES; MECHANICAL PARTS OF CLOCKS OR WATCHES IN GENERAL; TIME PIECES USING THE POSITION OF THE SUN, MOON OR STARS
    • G04B18/00Mechanisms for setting frequency
    • G04B18/006Mechanisms for setting frequency by adjusting the devices fixed on the balance

Definitions

  • the present invention relates to a mechanical oscillator for a timepiece, and more particularly to a mechanical oscillator for a wristwatch which has a high degree of isochronism.
  • the materials used to produce the balance and the hairspring in the most frequently used mechanical oscillators are chosen so that the variation of the moment of inertia of the balance and the variation of the return torque of the respective hairspring compensate each other.
  • a cupro-beryllium alloy balance associated with a spiral made of specially designed alloys such as invar and élinvar, which is an alloy of iron-nickel having a coefficient very weak dilatation.
  • This type of balance spring is however always sensitive to magnetic fields.
  • the search for new alloys that can be used for producing the hairspring is still relevant, as evidenced, for example, by the development of silinvar TM 1 .
  • the self-compensating result of these alloys is mainly the result of two contrary influences, notably that of the temperature and that of the magnetostriction on the modulus of elasticity of the metal.
  • Minimizing the isochronism defect is crucial for optimizing the accuracy of mechanical watches. This consists in producing a spiral balance having a high degree of isochronism allowing it to generate oscillations equal and independent of their amplitude. Thus, a beam as light as possible is frequently used, with as much inertia as possible.
  • This sprung balance is provided with a balance composed of a non-magnetic ceramic for which the coefficient of expansion The spiral is positive and less than + l * 10 ⁇ 6 K "1.
  • the hairspring is made from a composite of continuous carbon fibers of twisted or parallel texture with respect to the axial directions of the fiber. a thermosetting polymer matrix, thermoplastic or ceramic. The coefficient of thermal expansion of this composite is negative and greater than -l * 10 ⁇ 6 K "1 . More particularly, the materials used for producing the balance and the hairspring are selected so that the values of their coefficients of thermal expansion are similar, very small and of opposite signs.
  • this sprung balance makes it possible to obtain a high precision and a more stable operation of the oscillator thanks to a self-compensating effect of the spiral.
  • the present invention aims to at least significantly reduce the self-compensating effect of the spiral.
  • the present invention proposes a spiral balance which is in wide temperature ranges insensitive to variations in temperature. temperature to avoid dilation and variation of the moment of inertia of the pendulum.
  • the object of the present invention is to propose a spiral balance having an improved stability of its frequency, both with regard to its sensitivity to variations in temperature and amplitude, as well as to magnetic fields.
  • this object is achieved by a mechanical oscillator according to the invention, characterized by the production of the balance and the spiral in the same material.
  • This embodiment of the balance and the hairspring from the same material avoids the compensating effect of the hairspring relative to the balance, which thus has an almost constant inertia. As a result, self-compensation between the balance and the balance spring becomes negligible.
  • Fig. 1 an enlarged view of the top of a mechanical oscillator according to the invention
  • Fig. 2 an enlarged view of the mechanical oscillator of FIG. 1 in section
  • Fig. 3 a diagram showing diurnal step variations of two different mechanical oscillators.
  • Figs. 1 and 2 illustrate, by way of example, a mechanical oscillator of the spiral-balance type comprising a balance 10 and a balance spring 12.
  • the balance 10 comprises a shaft 14, a board 16 mounted rigidly on the shaft 14 and flyweights 18, d a first type, and 19 of a second type, a ferrule 20 and a plate 22.
  • the spiral 12 is made of a material that may or may not be the same as that used to make the plate 16 of the balance 10.
  • the spiral 12 is made from the same material as the rocker 10. More specifically, the spiral 12 and the plate 16 of the balance 10 are made of the same material. This embodiment of the balance 10 and / or its plate 16, and the spring 12 from the same material avoids the compensating effect of the spiral 12 relative to the balance 10, which thus has an almost constant inertia. As a result, the self-compensation between the balance 10 and the balance spring 12 is almost negligible.
  • the material chosen to produce the rocker 10, and / or its board 16, and the spiral 12, is preferably non-magnetic and has the advantage of having a coefficient of thermal expansion of 20 to 2 * 10 ⁇ 10 ppm / ° C maximum.
  • the thermal expansion coefficient is preferably 5-10 "6 ppm / ° C, and still more preferably 2-10 6 ppm / ° C maximum.
  • the density of the material is preferably in a range of 2.0 to 5.0 g / cm 3 , preferably 2.5 to 4.5 g / cm 3 , and still more preferably 3 to 4.0 g / cm 3 .
  • this material is diamond or synthetic diamond and, more generally, a diamond-based material.
  • other materials may be used, as described in more detail below, such as, for example, quartz, silicon, carbon, titanium or ceramic.
  • the shaft 14 of the balance 10 has an axis of symmetry, designated as the axis AA, which is also its axis of pivoting.
  • the shaft 14 is conventionally made of hardened steel and comprises a plate 14a, cylindrical portions 14b, 14c and 14d disposed on either side of the plate 14a and intended to receive respectively the shell 20, the plate 16 and the plateau 22. Its ends form pivots 14e and 14f intended to be engaged in bearings constituted in the frame of the timepiece, not shown in the drawing.
  • the board 16 has a central hole 16a and eight radially oriented openings defining eight arms 16b.
  • the outer ends of the arms 16b are interconnected to form a serge 16c.
  • the latter is pierced, in the extension of the arms 16b, holes 16d oriented parallel to the axis AA and in which the weights 18 and 19 are fixed.
  • the base of the serge 16c may be made of a material other than the board 16. In this case, when the board 16 is for example made of diamond, a diamond coating may be applied to the serge 16c in order to obtain the same physical characteristics for serge 16c as for board 16.
  • the rocker 10 and / or the spiral 12 are coated with nanoparticles of a material which is preferably non-magnetic and has the advantage of having a coefficient of thermal expansion of 20 to 2 * 10 ⁇ 10 ppm / ° C maximum.
  • This coefficient of thermal expansion is preferably 5-10 "6 ppm / ° C, and still more preferably 2-10 " 6 ppm / ° C maximum.
  • the density of said material is preferably in a range of 2.0 to 5.0 g / cm 3 , preferably 2.5 to 4.5 g / cm 3 , and still more preferably 3 to 4.0 g / cm 3 .
  • the balance 10 and the balance spring 12 have a nano-diamond coating.
  • This coating is also advantageously applicable to a sprung balance known to those skilled in the art, such as, for example, a sprung balance comprising a balance made of cupro-beryllium alloy associated with a spiral made of alloys specially studied as per example the invar.
  • the board 16 is in abutment against the plate 14a and positioned by the cylindrical portion 14c. It is fixed to the shaft 14 by glue points 24 arranged in housings formed in the periphery of the hole 16a.
  • the shell 20 is driven onto the shaft 14 in its cylindrical portion 14d, bearing against the board 16. It carries, mounted by gluing, the spring 12.
  • the board 16 is formed of a plate of a low density material with a low coefficient of thermal expansion, such as for example diamond, corundum, quartz or silicon, and whose thickness is of the order of a few tenths of millimeters. More particularly, this thickness is preferably in a range of 0.05 mm to 0.3 mm, and is typically 0.2 mm.
  • the hairspring 12 is made of a material that may or may not be the same as that used to make the balance 10 and / or its board 16. Thus, the material used to make the hairspring 12 may also be used. be selected from the above exemplified materials, ie diamond, quartz, silicon or corundum. The elasticity and length of these materials vary very little with temperature.
  • the weights 18 are each formed of a cylindrical nail 18a having an axis of symmetry, designated in FIG. 1 as the BB axis, of heavy material whose density is greater than 15 g / cm 3 , for example gold or platinum, provided with a head 18b and a body 18c, and a ring 18d made of the same material.
  • the body 18c of each of the weights 18 is engaged in a hole 16d, the head 18b bearing against the board 16.
  • the ring 18d associated with it is fixed on the other side of the board 16, by driving, gluing or welding.
  • the weights 18 have a symmetrical structure with respect to the axis BB of each of the nails 18a. In this way, during changes in temperature, the nails expand or contract radially relative to the axis BB, without their center of gravity moves. Consequently, as a first approximation, this expansion does not modify the inertia of the pendulum.
  • the weights 19 have a center of gravity offset from the axis of the hole 16d in which they are engaged. In this way, by turning them, it is possible to modify the moment of inertia and thus correct the frequency of the oscillator. To allow this rotation, the weights 19 comprise a cylindrical portion 19a provided with axially oriented slots 19b, allowing a frictional attachment.
  • the material used to make the balance 10 and the spiral 12 of the mechanical oscillator according to the present invention is likely to be insensitive to temperature.
  • this material is likely to be consistent with the margins established by the Swiss chronological chronometric criteria listed in Table 1 illustrated below.
  • Nonlimiting examples of materials satisfying the criteria indicated in Table 1, which are thus usable in the context of the present invention, are diamond, titanium, ceramic and quartz, as already described in more detail above. These materials have the following physical properties:
  • Fig. 3 illustrates a diagram showing exemplary diurnal cycle variations of two different mechanical oscillators by way of example. These diurnal cycle variations are represented in seconds ([s]) on an axis 41, depending on the different temperatures at which the corresponding mechanical oscillators were tested. These temperatures are represented in degrees Celsius ([ 0 C]] on an axis 31.
  • a first curve 30 illustrates a diurnal step variation of a timepiece comprising a standard mechanical oscillator. As shown in FIG. 3, this day-time variation is between a 6-second advance, as indicated by point 32, and a delay of 4 seconds, as indicated by point 34, when the timepiece is tested in a range. of temperatures between +8 and +38 0 C.
  • a second curve 40 illustrates a diurnal step variation of this timepiece when it is made with a mechanical oscillator according to a preferred embodiment of the present invention.
  • the variation in daytime running is between a zero advance, as indicated in point 42, and a delay of approximately 1.3 seconds, as indicated in point 44, during the test of the workpiece. in the temperature range between +8 and +38 0 C.
  • this frequency stability relative to the temperature of the mechanical oscillator according to the invention is added to other advantages obtained by the choice of the material used.
  • the materials constituting the balance 10 and spiral 12 being non-magnetic, a magnetic field can not interact with them. Only in the configuration described above, which uses the shaft 14 made of hardened steel, a magnetic field can interact with the shaft 14, but the influence of this interaction is virtually zero.
  • the specific mass of the constituent material of the board 16 is small, while the material constituting the weights 18, 19 is high, the total mass of the balance 10 is low for a given moment of inertia. As a result, the isochronism defect can be further reduced.
  • Weights 18, 19 gold or platinum can realize the balance 10 with a moment of inertia / mass ratio particularly favorable. It is also possible to use less expensive materials, for example brass or invar. In the latter case, the expansion of the weights 18, 19 could be further reduced.
  • pendulums for timepieces must be balanced. This can be done by removing or adding material. This operation is particularly advantageous by working on the weights 18, which have a symmetrical structure with respect to their axis BB.
  • at least a portion of said flyweights 18 preferably has a cylindrical shape of axis BB in their portion engaged in the board 16.
  • the present invention also claims a method of balancing by removal or addition of material from / to the balance 10, characterized in that material is removed from at least one of said weights 18 so symmetrical with reference to the axis of the cylinder or in that the equilibration is achieved by adding the material to at least one of the weights 18 symmetrically with reference to the axis of its cylinder.
  • the material used to make the weights 18 preferably has a specific mass greater than 10. It may be in particular gold or platinum, while the balance 10 and the spiral 12 are made of diamond. In this way, the ratio between the moment of inertia and the specific mass is particularly favorable.

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Micromachines (AREA)
  • Electric Clocks (AREA)
EP07857010.8A 2006-12-21 2007-12-20 Mechanischer oszillator für uhr Active EP2102717B1 (de)

Priority Applications (1)

Application Number Priority Date Filing Date Title
EP07857010.8A EP2102717B1 (de) 2006-12-21 2007-12-20 Mechanischer oszillator für uhr

Applications Claiming Priority (4)

Application Number Priority Date Filing Date Title
EP06026620 2006-12-21
CH02119/06A CH701155B1 (fr) 2006-12-27 2006-12-27 Oscillateur pour pièce d'horlogerie.
EP07857010.8A EP2102717B1 (de) 2006-12-21 2007-12-20 Mechanischer oszillator für uhr
PCT/EP2007/011287 WO2008080570A2 (fr) 2006-12-21 2007-12-20 Oscillateur mecanique pour une piece d'horlogerie

Publications (2)

Publication Number Publication Date
EP2102717A2 true EP2102717A2 (de) 2009-09-23
EP2102717B1 EP2102717B1 (de) 2013-06-26

Family

ID=39589024

Family Applications (1)

Application Number Title Priority Date Filing Date
EP07857010.8A Active EP2102717B1 (de) 2006-12-21 2007-12-20 Mechanischer oszillator für uhr

Country Status (4)

Country Link
US (1) US8240910B2 (de)
EP (1) EP2102717B1 (de)
JP (1) JP2010513886A (de)
WO (1) WO2008080570A2 (de)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US11982977B2 (en) 2016-06-13 2024-05-14 Rolex Sa Method of manufacturing a timepiece shaft

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EP2104005A1 (de) * 2008-03-20 2009-09-23 Nivarox-FAR S.A. Composite-Unruh und Herstellungsverfahren dafür
EP2104008A1 (de) * 2008-03-20 2009-09-23 Nivarox-FAR S.A. Monoblock-Regulierungsorgan und sein Herstellungsverfahren
US10324419B2 (en) * 2009-02-06 2019-06-18 Domasko GmbH Mechanical oscillating system for a clock and functional element for a clock
EP2677369B1 (de) * 2010-06-11 2015-01-14 Montres Breguet SA Hochfrequenzunruh für Uhr
EP2410386B1 (de) 2010-07-19 2018-10-03 Nivarox-FAR S.A. Unruh mit Trägheitsregulierung mit Einsatzteil
US9164485B2 (en) 2010-08-06 2015-10-20 Damasko Gmbh Oscillating body, mechanical oscillating system for wristwatches with such an oscillating body and watch with such an oscillating system
DE202011110747U1 (de) * 2010-08-06 2016-01-14 Damasko Gmbh Schwingkörper, mechanisches Schwingsystem für Armbanduhren mit einem solchen Schwingkörper sowie Uhr mit einem derartigen Schwingsystem
EP2466396A1 (de) * 2010-12-15 2012-06-20 The Swatch Group Research and Development Ltd. Magnetische Abschirmung für Spiralunruh einer Uhr
CH704924B1 (de) * 2011-05-13 2015-05-29 Bucherer Ag Unruh für eine Uhr sowie Uhr.
US9310774B2 (en) * 2011-12-22 2016-04-12 The Swatch Group Research And Development Ltd Method of improving the pivoting of a wheel set
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EP2680090A1 (de) * 2012-06-28 2014-01-01 Nivarox-FAR S.A. Triebfeder für Uhr
EP2703909A1 (de) * 2012-09-04 2014-03-05 The Swatch Group Research and Development Ltd. Gepaarter Spiralunruh-Schwinger
EP2717103B1 (de) 2012-10-04 2017-01-11 The Swatch Group Research and Development Ltd. Leuchtende Spiralfeder
CH707811A2 (fr) * 2013-03-19 2014-09-30 Nivarox Sa Composant monobloc indémontable d'horlogerie.
EP2781967B1 (de) * 2013-03-19 2018-07-04 Nivarox-FAR S.A. Spiralfeder einer Uhr
EP2784602B1 (de) * 2013-03-26 2018-12-05 Montres Breguet SA Welle eines beweglichen Elements mit optimierter Geometrie in einem magnetischen Umfeld
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EP3502786A1 (de) * 2017-12-22 2019-06-26 The Swatch Group Research and Development Ltd Unruh für uhr, und herstellungsverfahren einer solchen unruh
EP3647883A1 (de) * 2018-11-05 2020-05-06 CSEM Centre Suisse D'electronique Et De Microtechnique SA Unruh einer uhr
EP3719588B1 (de) * 2019-04-03 2021-11-03 The Swatch Group Research and Development Ltd Automatisch regulierbarer oszillator einer uhr
CH716384A1 (fr) * 2019-07-02 2021-01-15 Soprod Sa Oscillateur pour mouvement horloger et pièce d'horlogerie comportant un tel oscillateur.
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Publication number Priority date Publication date Assignee Title
US11982977B2 (en) 2016-06-13 2024-05-14 Rolex Sa Method of manufacturing a timepiece shaft

Also Published As

Publication number Publication date
US20100054090A1 (en) 2010-03-04
EP2102717B1 (de) 2013-06-26
WO2008080570A3 (fr) 2009-02-26
JP2010513886A (ja) 2010-04-30
US8240910B2 (en) 2012-08-14
WO2008080570A2 (fr) 2008-07-10

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