EP3054356B1 - Isochroner Resonator für Uhr - Google Patents

Isochroner Resonator für Uhr Download PDF

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Publication number
EP3054356B1
EP3054356B1 EP15153656.2A EP15153656A EP3054356B1 EP 3054356 B1 EP3054356 B1 EP 3054356B1 EP 15153656 A EP15153656 A EP 15153656A EP 3054356 B1 EP3054356 B1 EP 3054356B1
Authority
EP
European Patent Office
Prior art keywords
crosspiece
oscillator mechanism
isochronous
mass
primary resonators
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.)
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Application number
EP15153656.2A
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English (en)
French (fr)
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EP3054356A1 (de
Inventor
Pascal Winkler
Jean-Luc Helfer
Gianni Di Domenico
Thierry Conus
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.)
ETA SA Manufacture Horlogere Suisse
Original Assignee
ETA SA Manufacture Horlogere Suisse
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.)
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Publication date
Priority to EP17152205.5A priority Critical patent/EP3206091B1/de
Application filed by ETA SA Manufacture Horlogere Suisse filed Critical ETA SA Manufacture Horlogere Suisse
Priority to CH00139/15A priority patent/CH710691A2/fr
Priority to EP15153656.2A priority patent/EP3054356B1/de
Priority to CN201680001224.1A priority patent/CN106662839B/zh
Priority to US15/309,094 priority patent/US9983549B2/en
Priority to PCT/EP2016/051486 priority patent/WO2016124436A1/fr
Priority to JP2017507084A priority patent/JP6326549B2/ja
Priority to EP16701499.2A priority patent/EP3254158B1/de
Publication of EP3054356A1 publication Critical patent/EP3054356A1/de
Application granted granted Critical
Publication of EP3054356B1 publication Critical patent/EP3054356B1/de
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    • 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
    • G04B43/00Protecting clockworks by shields or other means against external influences, e.g. magnetic fields
    • G04B43/002Component shock protection arrangements
    • GPHYSICS
    • G04HOROLOGY
    • G04CELECTROMECHANICAL CLOCKS OR WATCHES
    • G04C3/00Electromechanical clocks or watches independent of other time-pieces and in which the movement is maintained by electric means
    • G04C3/08Electromechanical clocks or watches independent of other time-pieces and in which the movement is maintained by electric means wherein movement is regulated by a mechanical oscillator other than a pendulum or balance, e.g. by a tuning fork, e.g. electrostatically
    • 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
    • G04B17/045Oscillators acting by spring tension with oscillating blade springs
    • 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
    • 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
    • G04B17/10Oscillators with torsion strips or springs acting in the same manner as torsion strips, e.g. weight oscillating in a horizontal plane
    • 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
    • G04B17/20Compensation of mechanisms for stabilising frequency
    • G04B17/28Compensation of mechanisms for stabilising frequency for the effect of imbalance of the weights, e.g. tourbillon
    • 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
    • G04B5/00Automatic winding up
    • G04B5/02Automatic winding up by self-winding caused by the movement of the watch
    • G04B5/04Automatic winding up by self-winding caused by the movement of the watch by oscillating weights the movement of which is limited

Definitions

  • the invention relates to an isochronous clock oscillator mechanism of the tuning fork type, comprising a fixed support and a carrying beam of a plurality of primary resonators each comprising at least one mass carried by an elastic flexible blade constituting an elastic return means and which is arranged to work in bending and which is embedded in said cross.
  • the invention also relates to a watch movement comprising at least one such isochronous oscillator mechanism.
  • the invention also relates to a watch comprising at least one such movement.
  • the invention relates to the field of clock oscillator mechanisms and regulators, in particular for mechanical movements.
  • the isochronism of the movement must be optimal in all positions in space, which implies the design of movements able to compensate for the effects of gravitation on their constituents.
  • oscillators comprising a plurality of primary resonators having flexible branches, arranged relative to each other so as to average their errors.
  • a first type of oscillator with coupled primary resonators is known as a tuning fork whose each branch is formed by a primary resonator; however, such a system is very sensitive to variations in position in space.
  • the patent CH 451021 in the name of Ebauches SA and describes a symmetrical oscillator in U whose two flexible branches vibrate in tuning fork mode, each being connected to a rigid arm forming a counterweight, and each resonator
  • the primary component thus formed is arranged so that the instantaneous center of rotation coincides with the center of gravity, so that the frequency of the oscillator does not vary substantially during changes in position of the center of gravity.
  • the transition to a U-shaped architecture with extended branches is better than the U-shape of the prior art.
  • the patent CH 466 993 also in the name of Ebauches SA is a variant of the above, comprising a counting device transforming the oscillating movements of one of the two resonators into rotating movements of a counting wheel, this counting device being attached to one of these arms rigid, so that the counting device is insensitive to accelerations and in particular to shocks.
  • the patent GB 1293159 in the name of SEIKO also describes a U-shaped oscillator with extended branches and minimizes the position error for all of the vertical positions empirically, by moving the center of rotation of each primary resonator from its theoretically ideal position .
  • the invention proposes to jointly solve the problem of isochronism and that of obtaining the best possible quality factor. It is, in a way, to combine the respective advantages of known mechanisms using as resonator, or a balance-spiral assembly relatively insensitive to differences in position in space in its developments and most advanced montages but whose quality factor is strongly limited by the pivoting and the different losses, or a tuning fork with parallel blades which, free of pivoting, has a quality factor better than a sprung balance but is very sensitive to the position in space.
  • the invention relates to an isochronous pendulum clock oscillator mechanism according to claim 1.
  • the invention also relates to a watch movement comprising at least one such isochronous oscillator mechanism.
  • the invention also relates to a watch comprising at least one such movement.
  • the invention proposes to realize a resonator mechanism with the least possible loss, and which is the least sensitive chronometrically to its orientation in the gravitational field.
  • the invention seeks to reduce losses, in particular due to friction of pivots, and displacements of the recess.
  • the inventive step is to remove the traditional pivots, while minimizing the movements of the center of mass and the reactions of the support.
  • a mechanical resonator necessarily comprises at least one elastic element and an inertial element.
  • the search for a high quality factor encourages the use of a tuning fork structure.
  • the inventive step consists in producing a tuning fork isochronous resonator, with a plurality of primary resonators arranged in a symmetry geometry with respect to an axis, and together constituting a tuning fork.
  • the invention is more particularly described below, in a nonlimiting manner, in the preferred form of a tuning fork with two primary resonators symmetrical with respect to a plane of symmetry, which constitutes a particular advantageous case because of its simplicity.
  • the invention is applicable to any number of resonators: three, four, or more, provided that the symmetry of their relative arrangement and their relative temporal phase shift make it possible to compensate for the effects of the reaction torques on the embedding.
  • the invention relates to an equilibrium tuning clock-type isochronous oscillator mechanism 1 comprising a fixed support 2 and a crossbar 4 carrying a plurality of primary resonators 10.
  • the primary resonators 10 constitute the equivalent of the arms that comprises a conventional fork fork, and crosses 4 the equivalent of the common part of the tuning fork which these arms.
  • Each primary resonator 10 each comprises at least one mass 5 carried by an elastic flexible blade 6 arranged to work in bending and embedded in the crossbar 4.
  • these primary resonators 10 have at least one identical resonance mode, they are arranged to vibrate in a phase shift between them of the value 2 ⁇ / n, where n is their number, and are arranged according to a symmetry in the space such that the resultant forces and torques applied by the primary resonators 10 on the crossbar 4 is zero.
  • the Figures 1 to 17 illustrate examples with two primary resonators
  • the figure 19 illustrates an example with four primary resonators.
  • this crosspiece 4 is fixed to the fixed support 2 by a main elastic connection 3, whose rigidity is greater than the rigidity of each elastic flexible blade 6. This characteristic provides a coupling between the primary resonators 10.
  • the rigidity of the main elastic connection 3 is greater than the total of the rigidities of all the flexible flexible strips 6 that comprise the primary resonators 10.
  • the damping of the main elastic connection 3 is greater than the damping of each elastic flexible blade 6, and, more particularly, the damping of the main elastic connection 3 is greater than the total of the damping of all the blades.
  • the primary resonators 10 are arranged in space so that the resultant of their operating errors due to gravitation is zero.
  • the primary resonators 10 are rotatable, which makes the isochronous oscillator mechanism 1 according to the invention insensitive to gravitation.
  • each primary resonator 10 forms a rotary resonator, whose center of mass is on the place whose translations are minimal during rotation. This is to minimize movements of the center of mass in the gravity field or under the effect of shocks, and thus improve the chronometry of the system.
  • This main elastic connection 3 is preferably constituted by an elastic blade, it does not move substantially when the isochronous oscillator mechanism 1 oscillates in tuning fork mode. Indeed, the branches of the tuning fork constituted by the primary resonators 10 exchange energy movement through the cross 4, but the movements of the cross 4 are minimal.
  • the direction in which the centers of mass CM of the primary resonators 10 are moved is called the longitudinal direction X.
  • a transverse direction Y is substantially perpendicular to this longitudinal direction X.
  • a direction Z completes the direct trihedron.
  • crossbar 4 is straight and extends in the longitudinal direction X.
  • all or part of the isochronous oscillator mechanism 1 is arranged symmetrically with respect to a plane of symmetry PS which extends parallel to the transverse direction Y.
  • the main elastic connection 3 extends between the cross member 4 and the fixed support 2. Preferably, but not necessarily, this main elastic connection 3 extends along the main direction Y, as can be seen in the examples of the figures.
  • the primary direction which connects the point of embedding on the crosspiece 4 of an elastic flexible blade 6 to the center of mass CM of the corresponding primary resonator 10, when the latter is at rest is parallel to the longitudinal direction X.
  • the figure 1 illustrates a simplified embodiment of an isochronous clock oscillator mechanism 1 according to the invention, of tuning fork type, comprising a fixed support 2 which carries, by a main elastic connection 3, made in the form of a flexible blade, a crossbar 4 carrier of two primary planar resonators 10A, 10B, symmetrical with respect to a plane of symmetry PS, and each having a mass, respectively 5A, 5B, carried by an elastic flexible blade, respectively 6A, 6B, arranged to work in bending and recessed in the crossbar 4, symmetrically with respect to the plane of symmetry PS.
  • the primary directions of the different primary resonators 10 which constitute this isochronous oscillator mechanism 1 are parallel to the longitudinal direction X, or merged.
  • the resilient flexible blades 6 are arranged so that the displacement of each center of mass CM of the given primary resonator 10 is minimal in the transverse direction Y where compensation is not provided, and so the displacements of the different mass centers CM of the given primary resonators 10 are compensated with respect to one another in the longitudinal direction X: if, as in the case of the figures, the isochronous oscillator mechanism 1 comprises two primary resonators 10A and 10B arranged back to back on either side of the crosspiece 4, their respective centers of mass CMA and CMB move essentially in the longitudinal direction X, but with displacements of the same value but in opposite directions.
  • the advantage of an arrangement according to the invention is to have elastic blades working in almost pure bending, which makes it possible to obtain an isochronous resonator.
  • the torque is proportional to the angle a whose corresponding mass pivots.
  • the frequency is therefore independent of the amplitude of the oscillation.
  • the distance between the embedding of the resilient flexible blade 6 in the crossbar 4 and the center of mass CM is equal to the distance between the center of mass CM and the embedding of the elastic flexible blade 6 in the associated mass 5, as visible on the figure 1 .
  • the center of mass CM thus remains on the X axis, or in the immediate vicinity of the X axis, that is to say at a distance of a few micrometers.
  • each primary resonator 10 is arranged to oscillate in a plane.
  • each primary resonator 10 is monolithic.
  • the cross member 4 and the flexible flexible blades 6 of the primary resonators 10 form a monolithic assembly.
  • the fixed support 2, the main elastic connection 3, the crosspiece 4, and the flexible flexible blades 6 of the primary resonators 10, form a monolithic assembly.
  • the fixed support 2, the main elastic connection 3, the crosspiece 4, and the flexible flexible blades 6 of the primary resonators 10, form a monolithic assembly.
  • Such an embodiment makes it possible to obtain elastic blades 6 called “high leaf”, which have a height very large relative to their thickness, in particular at least five times higher than thick, and more particularly at least ten times higher than thick.
  • Such blades in high sheet make it possible to ensure the guiding function, and to overcome traditional pivots, which allows a significant increase in the quality factor.
  • the architecture in the form of a tuning fork, according to the invention makes it possible to compensate for all the reactions to the recesses, which still considerably increases the quality factor.
  • the masses 5, 51, 52, primary resonators 10 are essentially subjected to a pivoting movement.
  • the corresponding resilient flexible blade 6 provides the pivotal guiding function.
  • the invention is illustrated here in variants where, each time, a single elastic flexible blade 6 maintains the respective mass 5 with respect to the crossbar 4. It is possible to imagine other variants where these blades 6 would be doubled or multiplied to ensure even better guidance.
  • the advantage of the single blade is to work in pure bending, which eliminates shear stresses, or transverse forces, which are unfavorable for isochronism, which explains the preference for a single flexible blade 6, which ensures therefore a better chronometry of a watch incorporating an oscillator 1 according to the invention.
  • each primary resonator 10 is arranged to oscillate in a plane
  • all the primary resonators 10 are arranged to oscillate in planes parallel to each other, or in the same plane.
  • all these primary resonators 10 are arranged to oscillate in the same plane, for example on the embodiments illustrated in FIGS. Figures 1 to 12 .
  • these primary resonators 10 each extend in a separate plane.
  • FIGS. 1 to 12 illustrate an isochronous oscillator mechanism 1, all primary resonators 10 are identical, even in number, and arranged in symmetry with respect to a plane of symmetry PS extending parallel to a transverse direction Y which is that of the main elastic link 3 and perpendicularly to a longitudinal direction X in which the centers of mass CM of the primary resonators 10 are movable.
  • the primary resonators 10 then oscillate in phase opposition, which guarantees the compensation of the movements of the centers of mass CM in the longitudinal direction X.
  • the main elastic connection 3 is straight.
  • the resilient flexible blades 6 are straight in the longitudinal direction X.
  • the centers of mass CM of the primary resonators 10 are considered in their alignment at rest. This arrangement guarantees the insensitivity to the positions of the isochronous oscillator mechanism 1 according to the invention, unlike a tuning fork of the conventional type with parallel branches which is much too sensitive to the positions in space if it is incorporated in a watch, and which can only be suitable for a piece of clock.
  • the residual defect after compensation of the displacements of the centers of mass in X is of very small value, of the same order of magnitude as the defect due to displacements of the centers of mass in Y, which is limited to 3 or 4 micrometers, for a blade of 1 mm long, the cumulative defect thus remains less than 6 seconds per day.
  • the symmetry thus compensates for any error in residual market.
  • the resilient flexible blades 6 that comprise the primary resonators 10 are straight and aligned in pairs.
  • the elastic flexible blades 6 are spiral wound around the centers of mass CM primary resonators 10 considered.
  • FIG. 13 and 14 An illustrated variant on Figures 13 and 14 represents a torsion tuning fork which comprises arms 51 and 52, each provided with a mass at its distal end, and oscillating in parallel planes P1 and P2 and symmetrically with respect to an axis A parallel to these two planes P1 and P2.
  • tuning fork illustrated by the figure 15 comprises two resonators, each comprising a spiral spring recessed at a first end on a common cross-member and having a mass at a second distal end, these two resonators extending in two parallel planes and being, in projection on one of these planes, symmetrical with respect to a plane of symmetry PS which is perpendicular to these two planes.
  • the resulting torque is zero at the embedding at the crossbar 4.
  • the mechanisms must be usable in a watch, and incorporate security, including shockproof.
  • the preferred mode of tuning fork in H is represented on the Figures 1 to 7 .
  • This crosspiece 4 carries a pair of marked masses 51 and 52, mounted symmetrically on either side of the fixed support 2 and the first elastic connection 3.
  • each of them comprises an arm connected in its middle to the corresponding flexible blade 6, this arm extending substantially parallel in the transverse direction Y, and being either a solid arm as on the figure 3 , either an arm with inertial flyweights at its opposite ends, or substantially punctual as on the figure 1 , in the form of annular sectors, as visible on the figures 2 , and 4 to 7 .
  • Each of these masses 51, 52 is mounted oscillating about a virtual pivoting axis of position determined relative to the crossbar 4, and recalled by an elastic flexible blade 6, respectively marked 61, 62, which constitutes means of resilient return and which is secured to one end 41, 42 of the cross member 4, the two ends 41 and 42 being opposite and on either side of the crossbar 4.
  • These flexible blades 61, 62 extend from preferably linearly in the extension and on both sides of the crossbar 4.
  • Each virtual pivoting axis is, in the rest position of the isochronous oscillator mechanism 1, coinciding with the center of mass CM1, CM2, of the respective mass 51, 52.
  • These resilient flexible blades 61, 62 are arranged to limit the displacement of the centers of mass CM1, CM2, to a transverse stroke relative to the crossbar 4, as small as possible in the transverse direction Y, and to a longitudinal stroke according to the longitudinal direction X greater than this transverse stroke.
  • the longitudinal arrangement of the resilient flexible blades 61, 62 makes it possible to compensate for the direction of greater displacement of the centers of mass CM1 and CM2, which move symmetrically relative to the plane symmetry PS.
  • the isochronous oscillator mechanism 1 advantageously comprises rotational stops, and / or translational limit stops in the X and Y directions, and / or translation Z limit stops. These stroke limiting means can be integrated, part of a one-piece construction, and / or be reported.
  • the masses 51, 52 advantageously comprise abutment means 7, labeled 71, 72, which are arranged to cooperate with complementary abutment means 73, 74, which the crosspiece 4 comprises, and to limit the displacement of the elastic flexible blades. 61, 62, with respect to the crossbar 4, in the event of shocks or similar accelerations.
  • a mass 5 is not directly carried by the flexible blade 6, the latter comprises, on the other side relative to the main body of the crosspiece 4, an end plate 45, which is arranged to receive, directly or indirectly, this mass 6.
  • the execution of figures 4 and 5 of the invention as the variant of the second type of figures 11 and 12 adjacent to the invention, comprises end pieces 53, 54, arranged to be attached to such an end plate 45 and to receive a mass 51 or 52.
  • the variant of the preferred embodiment of figures 6 and 7 comprises a socket 55 arranged to perform the same function.
  • the ends of the crosspiece 4 each comprise two abutment bearing surfaces 42, which are each arranged to stop an oblique surface 74 that comprises the end plate 45, so as to limit the angle of deformation ⁇ (defined in FIG. figure 1 ) that can take the flexible blade 6 relative to its installation in the crossbar 4, and thus constituting stops in rotation.
  • the corresponding end of the crosspiece 4 further comprises a housing 79, in this case a bore, arranged to act as a limit stop around the periphery 48 of the substantially circular end plate 45, to limit X and Y translations. at these different stops, which limit translations in X and Y, it limits the possible influence of shocks, protects the flexible blade 6, and preserves this flexible blade 6 against excessive deformation. And of course the possible movement of the CM centers of mass is limited.
  • Z stops are provided mainly when using end caps 53, 54, sockets 55, or the like; for example the figure 5 illustrates tips 53, 54, which either have bores aligned with pins 56 carried by a plate, or comprise aligned bearings with bores of a plate, the bearings thus formed being non-contact in normal operating conditions, and being arranged to take the forces, especially Z, in case of impact.
  • the detail of the figure 6 shows, with regard to the variant with the receipt of a bush 55, a similar arrangement with respect to the stops.
  • the end plate 45 further comprises a lug with stop surfaces 76 arranged to cooperate abutting abutment with complementary surfaces 78 of the cross member 4, to limit the translations.
  • the bushing 55 has a skirt 57 driven on the end plate 45, but the periphery 59 of this bushing 55 remains at a distance from the bore 79 of the cross member 4, and thus ensures with it the safety in translation in X and in Y .
  • Z-shaped shoulders may also be provided on certain surfaces to form Z-limiting abutment surfaces.
  • the complementary surfaces of the stops In the absence of unexpected accelerations such as shocks, the complementary surfaces of the stops must not be in contact with each other, so as to avoid any unnecessary friction detrimental to the quality factor.
  • Some stroke limiting means may be used to perform damping functions of unwanted vibration modes.
  • FIG. 1 The illustrations of the preferred embodiment of the invention, and the second type of neighbor of the invention, thus show the fixed support 2 and the crossbar 4 which are separated only by a narrow groove 30, here called “honey groove” , around the main elastic link 3, which is designed to allow tuning fork coupling.
  • the groove 30 limits the angular movement of the crossbar 4, which is insignificant in normal operation, but can occur in case of impact.
  • this groove is filled with a viscous or pasty product, which allows the dissipation of energy in the event of excessive travel.
  • cooperating Z surfaces with a solid friction, or viscous, or pasty, and preferably increasing with the speed and / or with the amplitude, for example with conical surfaces corner, as shown on the sketches of the Figures 17 and 18 .
  • the resilient flexible blades 61, 62 which extend substantially in the longitudinal direction X, are short blades, that is to say of a length less than the smallest value between four times their height or thirty times their thickness. It is this short blade characteristic that makes it possible to limit the movements of the center of mass CM concerned.
  • each primary resonator 10 does not move substantially in the transverse direction Y: it performs a crawling movement, on either side of an average axis parallel to the longitudinal direction X, around from a point on this mean axis.
  • the resilient flexible blades 61 and 62 are preferably aligned, these blades being preferably straight.
  • the second type of goat horn tuning fork which is a neighbor of the invention, is represented on the Figures 8 to 12 .
  • this crosspiece 4 carries a pair of masses 5 marked 51 and 52, mounted symmetrically on both sides of the fixed support 2 and the first elastic connection 3.
  • Each of these masses 51, 52 is mounted oscillatingly and recalled by an elastic flexible blade 6 respectively marked 61, 62, which is a spiral 8, respectively 81, 82, or an assembly of spirals.
  • a first hairspring 81 and a second hairspring 82 are each bonded at its inner turn to an end plate 45 for receiving a mass 51, 52, and attached to the respective end 41, 42 of the sleeper 4. by its external turn.
  • the masses 51 and 52 each pivot about a virtual pivot axis of position determined relative to the crossbar 4.
  • Each virtual pivoting axis is, in the rest position of the isochronous oscillator mechanism 1, coinciding with the center of mass CM1, CM2, of the respective mass 51, 52.
  • the masses 51, 52 extend substantially in the transverse direction Y.
  • each of them comprises an arm connected in the middle to the corresponding flexible blade 6, this arm s' extending substantially parallel in the transverse direction Y, and being either a solid arm as on the figure 3 , either an arm with inertial flyweights at its opposite ends, or substantially punctual as on the figure 8 , in the form of annular sectors, as visible on the Figures 9 to 12 adjacent to the invention.
  • each spiral 81, 82 is section or variable curvature along its development.
  • the version illustrated by the figures is a variation of variable thickness, optimized to limit the movements of the center of mass CM.
  • the pendulum mass 5 is preferably suspended by a coil thicker than the rest of the spiral.
  • the development of the hairspring is greater than one turn, and in particular greater than 1.5 turns, which is easier to minimize the displacement of the center of mass.
  • a regular decrease in thickness over 270 °, followed by a thickness increase can make it possible to limit the displacement of the center of mass CM to 3 micrometers in Y and 4 micrometers in X.
  • the polar elemental stiffness advantageously passes through an extremum, for example a mini between two maxi, or vice versa.
  • a satisfactory simulation consists, again, in giving the hairspring an upper stiffness in its portion 89 which is beyond the center of mass towards the outside, than in its portion 88 which lies between the two centers of mass CM1 and CM2.
  • variable thickness corresponds to an elaboration MEMS easier.
  • the modes of oscillation in translation and the displacements in the event of shocks are preferably mechanically limited by axes, or by end pieces 53, 54, or sockets 55.
  • the first hairspring 81 and the second hairspring 82 are attached to the ends 41, 42, in alignment with their respective virtual pivoting axis, in the rest position of the isochronous oscillator mechanism 1.
  • the figure 16 illustrates another embodiment close to the invention, where this diagram of the second type of figure is extrapolated by suspending each mass, not to a single spiral, but pairs of spirals 81, 810, respectively 82, 820, attached to the cross 4, on either side of the centers of mass in the Y direction.
  • This very robust embodiment is however closer to a system with crossed flexible blades than the principle of the present invention.
  • the figure 19 illustrates a variant where the crossbar 4 constitutes a frame surrounding the primary resonators 10, in an example of application to four resonators 10A, 10B, 10C, 10D. It will be understood that this inverse architecture of the preceding examples can also be used for the implementation of the invention, in all its variants exposed above, and which are therefore not detailed further here.
  • the figure 20 illustrates, in this variant of crossbar 4 formed by a frame, the pendulum of the H tuning fork.
  • the crossbar 4 carries a pair 51, 52, masses 5, mounted symmetrically inside the crossbar 4 which forms a frame suspended by the first elastic connection 3 to the fixed structure 2, the masses 51, 52 extending substantially in the transverse direction Y.
  • Each of the masses 51, 52 is oscillatingly mounted around a virtual pivot axis of position determined relative to the crossbar 4, and recalled by an elastic flexible blade 6, respectively 61, 62, which is secured to one side of the frame forming the crossbar 4, the flexible blades 61, 62, extending linearly to the inside the frame.
  • FIG 21 illustrates, in this variant of crossbar 4 formed by a frame, adjacent to the invention, the pendulum fork horns goat.
  • the crossbar 4 carries a pair 51, 52, masses 5, mounted symmetrically inside the crossbar 4 which forms a frame suspended by the first elastic connection 3 to the fixed structure 2, and substantially in a transverse direction Y perpendicular to the longitudinal direction X in which the centers of mass CM of the primary resonators 10 are movable.
  • Each of the masses 51, 52 is oscillatingly mounted about a virtual pivot axis of position determined with respect to the crossbar 4, and recalled by a spiral 8, respectively 81, 82, which is integral with one side of the frame forming the crossbar 4, these spirals 81, 82, extending inside the frame.
  • the masses 5, 5A, 5B, 51, 52, form rockers.
  • the masses 51, 52 comprise, for balancing adjustment, inertia and adjustment of oscillation frequency, flyweights 91, 92, and / or housing 93 for receive such flyweights, preferably in the areas farthest from the ends 41, 42 of the crossbar 4.
  • flyweights advantageously comprise an eccentric insert, for example platinum, to facilitate adjustment by pivoting the insert.
  • particular areas of these masses may be assigned to laser ablation, or, conversely, to plasma, ink jet or the like, to provide these settings.
  • the invention also relates to a clockwork movement 100, in particular a mechanical movement, comprising such an isochronous oscillator mechanism 1.
  • the invention also relates to a watch 200 comprising such a mechanical movement 100.
  • the oscillator according to the invention constitutes a tuning fork consisting of two resonators, preferably rotating, with flexion blades, mounted on a cross member connected, preferably viscoelastically, to the plate.
  • each primary resonator 10 is designed to minimize the displacement of the center of mass CM in the transverse direction Y of the symmetry plane PS of the tuning fork.
  • the symmetry plane PS of the tuning fork is chosen so that the operating errors due to the positions in the longitudinal direction X perpendicular to the transverse direction Y, cancel out between the two branches of the tuning fork constituted by the primary resonators 10, both sides of the crossbar 4.
  • tuning fork type limits the effect of reactions to embedding.
  • the invention minimizes the displacement of the center of mass CM of each primary resonator 10.
  • the invention makes it possible to obtain a perfectly isochronous oscillator, very compact, requiring no adjustment other than the inertia of the masses, and very easy assembly.

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Piezo-Electric Or Mechanical Vibrators, Or Delay Or Filter Circuits (AREA)

Claims (21)

  1. Isochroner Uhren-Oszillatormechanismus (1) des Stimmgabeltyps, umfassend einen festen Träger (2) und einen Querträger (4), der eine Mehrzahl von primären Resonatoren (10) trägt, wovon jeder mindestens eine Masse (5) aufweist, die von einem elastischen biegsamen Plättchen (6) getragen wird, das ein elastisches Rückstellmittel bildet und das dafür ausgelegt ist, durch Biegung zu arbeiten, und das in den Querträger (4) eingelassen ist, wobei die primären Resonatoren (10) mindestens eine gleiche Resonanzbetriebsart besitzen und dafür ausgelegt sind, mit einer gegenseitigen Phasenverschiebung von 2π/n zu schwingen, wobei n die Anzahl der primären Resonatoren (10) ist, und in einer Symmetrie im Raum angeordnet sind, derart, dass die Resultierende der Kräfte und der Drehmomente, die durch die primären Resonatoren (10) auf den Querträger (4) ausgeübt werden, null ist, und wobei der Querträger (4) an dem festen Träger (2) durch eine elastische Hauptverbindung (3) befestigt ist, deren Starrheit größer als die Starrheit jedes der elastischen biegsamen Plättchen (6) ist, und wobei die primären Resonatoren (10) im Raum in einer Weise angeordnet sind, dass die Resultierende ihrer Gangabweichung aufgrund der Schwerkraft null ist, wobei die elastischen biegsamen Plättchen (6), die er aufweist, geradlinige Plättchen (61, 62) sind, die sich im Wesentlichen in einer Längsrichtung erstrecken, in der die Massenschwerpunkte der primären Resonatoren bewegbar sind, und dadurch gekennzeichnet, dass die elastischen biegsamen Plättchen (6) kurze Plättchen (61, 62) mit einer Länge sind, die kleiner als der kleinste Wert aus ihrer vierfachen Höhe und ihrer dreißigfachen Dicke ist.
  2. Isochroner Oszillatormechanismus (1) nach Anspruch 1, dadurch gekennzeichnet, dass die primären Resonatoren (10) drehbar sind.
  3. Isochroner Oszillatormechanismus (1) nach Anspruch 1 oder 2, dadurch gekennzeichnet, dass die Starrheit der elastischen Hauptverbindung (3) größer als die Starrheit sämtlicher elastischer biegsamer Plättchen (6) zusammengenommen ist.
  4. Isochroner Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 3, dadurch gekennzeichnet, dass jeder primäre Resonator (10) dafür ausgelegt ist, in einer Ebene zu oszillieren.
  5. Isochroner Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 4, dadurch gekennzeichnet, dass alle primären Resonatoren (10) dafür ausgelegt sind, in zueinander parallelen oder deckungsgleichen Ebenen zu oszillieren.
  6. Isochroner Oszillatormechanismus (1) nach Anspruch 5, dadurch gekennzeichnet, dass alle primären Resonatoren (10) dafür ausgelegt sind, in derselben Ebene zu oszillieren.
  7. Isochroner Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 6, dadurch gekennzeichnet, dass alle primären Resonatoren (10) eben sind.
  8. Isochroner Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 7, dadurch gekennzeichnet, dass alle primären Resonatoren (10) gleich sind, in gerader Anzahl vorhanden sind und symmetrisch in Bezug auf eine Symmetrieebene (PS) angeordnet sind, die sich parallel zu einer Querrichtung (Y) erstreckt, die zu der Längsrichtung (X) senkrecht ist.
  9. Isochroner Oszillatormechanismus (1) nach Anspruch 8, dadurch gekennzeichnet, dass sich die elastische Hauptverbindung (3) in der Querrichtung (Y) erstreckt.
  10. Isochroner Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 9, dadurch gekennzeichnet, dass die primären Resonatoren (10) in gerader Anzahl vorhanden sind und dass die elastischen biegsamen Plättchen (61, 62), die sie aufweisen, geradlinig und paarweise aufeinander ausgerichtet sind.
  11. Isochroner Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 10, dadurch gekennzeichnet, dass die gegenüberliegenden Enden (41, 42) des Querträgers (4) jeweils Drehanschlagmittel (78) aufweisen, die die Winkelbahn des jeweiligen kurzen Plättchens (61, 62) begrenzen.
  12. Isochroner Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 11, dadurch gekennzeichnet, dass die gegenüberliegenden Enden (41, 42) des Querträgers (4) jeweils Translationsanschlagmittel (78) aufweisen, die die Verlagerung in der Längsrichtung (X) und in der Querrichtung (Y) der Massenschwerpunkte (CM) der jeweiligen Massen (5) begrenzen.
  13. Isochroner Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 12, dadurch gekennzeichnet, dass die gegenüberliegenden Enden (41, 42) des Querträgers (4) jeweils Translationsanschlagmittel (78) aufweisen, die die Verlagerung in einer Richtung (Z) senkrecht zu der Längsrichtung (X) und zu der Querrichtung (Y) der Massenschwerpunkte (CM) der jeweiligen Massen (5) begrenzen.
  14. Isochroner Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 13, dadurch gekennzeichnet, dass der Querträger (4) ein Paar (51, 52) der Massen (5) trägt, die symmetrisch auf beiden Seiten des festen Trägers (2) und der ersten elastischen Verbindung (3) montiert sind, wobei sich die Massen (51, 52) im Wesentlichen in einer Querrichtung (Y) senkrecht zu der Längsrichtung (X), in der die Massenschwerpunkte (CM) der primären Resonatoren (10) bewegbar sind, erstrecken und die Seitenschenkel eines H bilden, dessen Querlinie (4) den horizontalen Schenkel bildet, wobei jede der Massen (51, 52) oszillierend um eine virtuelle Drehachse mit gegebener Position in Bezug auf den Querträger (4) montiert ist und durch ein elastisches biegsames Plättchen (6) zurückgestellt wird, das mit einem Ende (41, 42) des Querträgers (4) fest verbunden ist, wobei sich die biegsamen Plättchen (6) geradlinig in der Verlängerung und auf beiden Seiten des Querträgers (4) erstrecken.
  15. Isochroner Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 13, dadurch gekennzeichnet, dass der Querträger (4) ein Paar (51, 52) der Massen (5) trägt, die symmetrisch in dem Querträger (4) montiert sind, der einen durch die erste elastische Verbindung (3) an der festen Struktur (2) aufgehängten Rahmen bildet, wobei sich die Massen (51, 52) im Wesentlichen in einer Querrichtung (Y) senkrecht zu einer Längsrichtung (X) erstrecken, in der die Massenschwerpunkte (CM) der primären Resonatoren (10) bewegbar sind, wobei jede der Massen (51, 52) oszillierend um eine virtuelle Drehachse mit gegebener Position in Bezug auf den Querträger (4) montiert ist und durch ein elastisches biegsames Plättchen (6) zurückgestellt wird, das mit einer Seite des den Querträger (4) bildenden Rahmens fest verbunden ist, wobei sich die biegsamen Plättchen (6) geradlinig in dem Rahmen erstrecken.
  16. Isochroner Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 15, dadurch gekennzeichnet, dass der feste Träger (2) und der Querträger (4) durch einen schmalen Schlitz (30) um die elastische Hauptverbindung (3) getrennt sind, die die Kopplung im Stimmgabelmodus sicherstellt, wobei der Schlitz (30) dafür ausgelegt ist, die Winkelbewegung des Querträgers (4) zu begrenzen, und mit einem viskosen oder pastösen Produkt gefüllt ist, das dafür ausgelegt ist, die Abführung von Energie im Fall eines zu großen Ausschlags sicherzustellen.
  17. Isochroner Oszillatormechanismus (17) nach einem der Ansprüche 1 bis 16, dadurch gekennzeichnet, dass die Massen (51, 52) Unruhen sind.
  18. Isochroner Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 17, dadurch gekennzeichnet, dass der Querträger (4) geradlinig ist und sich in der Längsrichtung (X) erstreckt.
  19. Isochroner Oszillatormechanismus (1) nach Anspruch 14, dadurch gekennzeichnet, dass die Massen (51, 52) Stäbe sind, die Endgewichtchen an den von den gegenüberliegenden Enden (41, 42) des Querträgers (4) am weitesten entfernten Punkten aufweisen, wobei sich der Querträger (4) in einer Längsrichtung (X) erstreckt, in der die Massenschwerpunkte (CM) der primären Resonatoren (10) bewegbar sind, wobei sich die Massen (51, 52) im Wesentlichen in einer Querrichtung (Y) senkrecht zu der Längsrichtung (X) erstrecken.
  20. Uhrwerk (100), umfassend mindestens einen isochronen Oszillatormechanismus (1) nach einem der Ansprüche 1 bis 19.
  21. Uhr (200), umfassend mindestens ein Werk (100) nach Anspruch 20.
EP15153656.2A 2015-02-03 2015-02-03 Isochroner Resonator für Uhr Active EP3054356B1 (de)

Priority Applications (8)

Application Number Priority Date Filing Date Title
CH00139/15A CH710691A2 (fr) 2015-02-03 2015-02-03 Résonateur isochrone d'horlogerie.
EP15153656.2A EP3054356B1 (de) 2015-02-03 2015-02-03 Isochroner Resonator für Uhr
EP17152205.5A EP3206091B1 (de) 2015-02-03 2015-02-03 Isochroner resonator für eine uhr
US15/309,094 US9983549B2 (en) 2015-02-03 2016-01-26 Isochronous timepiece resonator
CN201680001224.1A CN106662839B (zh) 2015-02-03 2016-01-26 等时钟表谐振器
PCT/EP2016/051486 WO2016124436A1 (fr) 2015-02-03 2016-01-26 Resonateur isochrone d'horlogerie
JP2017507084A JP6326549B2 (ja) 2015-02-03 2016-01-26 等時性を有する計時器用共振器
EP16701499.2A EP3254158B1 (de) 2015-02-03 2016-01-26 Isochroner resonator für uhr

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EP15153656.2A EP3054356B1 (de) 2015-02-03 2015-02-03 Isochroner Resonator für Uhr

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CH713055A2 (fr) 2016-10-18 2018-04-30 Eta Sa Mft Horlogere Suisse Mouvement d'horlogerie comportant un mécanisme résonateur et un mécanisme d'échappement coopérant en transmission continue.
CH713166B1 (fr) 2016-11-16 2021-10-29 Swatch Group Res & Dev Ltd Protection des lames d'un résonateur de montre mécanique en cas de choc.
EP3336613B1 (de) 2016-12-16 2020-03-11 Association Suisse pour la Recherche Horlogère Resonator für uhr, der zwei pendellager umfasst, die so angeordnet sind, dass sie auf derselben ebene schwingen können
CH714019A2 (fr) * 2017-07-26 2019-01-31 Eta Sa Mft Horlogere Suisse Mouvement mécanique d'horlogerie avec résonateur rotatif.
EP3971655A1 (de) * 2020-09-18 2022-03-23 ETA SA Manufacture Horlogère Suisse Stossdämpfungsschutz mit anschlag eines resonatormechanismus mit flexibler drehführung
EP4009115A1 (de) * 2020-12-02 2022-06-08 Omega SA Spiralfeder für resonatormechanismus eines uhrwerks, der mit mitteln zum ausgleichen der starrheit ausgestattet ist

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CH46203A (de) 1908-08-10 1910-02-16 Wladimir Popow Einrichtung zum selbsttätigen Wägen von Schüttgütern
CH435122A (fr) * 1965-03-10 1966-12-15 Longines Montres Comp D Diapason pour pièce d'horlogerie
CH451021A (fr) 1965-05-28 1968-05-15 Ebauches Sa Oscillateur symétrique à flexion pour pièce d'horlogerie
CH485145A (fr) * 1966-03-29 1970-01-31 Ebauches Sa Dispositif transformant les mouvements oscillants d'un résonateur acoustique en mouvements rotatifs d'une roue de comptage
GB1293159A (en) 1969-12-10 1972-10-18 Suwa Seikosha Kk A vibrator for an electric timepiece
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FR1605076A (de) * 1966-09-26 1973-01-12

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CH710691A2 (fr) 2016-08-15

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