EP2998801A1 - Magnetic clock escapement and device for controlling the operation of a clock movement - Google Patents
Magnetic clock escapement and device for controlling the operation of a clock movement Download PDFInfo
- Publication number
- EP2998801A1 EP2998801A1 EP14185638.5A EP14185638A EP2998801A1 EP 2998801 A1 EP2998801 A1 EP 2998801A1 EP 14185638 A EP14185638 A EP 14185638A EP 2998801 A1 EP2998801 A1 EP 2998801A1
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- European Patent Office
- Prior art keywords
- magnetic
- magnet
- periodic
- pattern
- resonator
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- 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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- G—PHYSICS
- G04—HOROLOGY
- G04C—ELECTROMECHANICAL CLOCKS OR WATCHES
- G04C5/00—Electric or magnetic means for converting oscillatory to rotary motion in time-pieces, i.e. electric or magnetic escapements
- G04C5/005—Magnetic or electromagnetic means
-
- 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
- G04B15/00—Escapements
- G04B15/14—Component parts or constructional details, e.g. construction of the lever or the escape wheel
Definitions
- the present invention relates to the field of devices regulating the movement of a watch movement.
- the present invention relates to watchmaking escapements of the magnetic type, the usual functions of which are the maintenance of a resonance mode of a resonator, in particular an oscillation or a continuous rotation of an inertial part of this resonator, and the timing of a counter wheel.
- the magnetic escapement provides these two functions by means of an escape wheel comprising a magnetic structure, which is magnetically coupled to at least one magnet carried by a part of the resonator undergoing the resonance movement. .
- a resonator of the tuning fork type The magnet of the resonator is magnetically coupled to these two out-of-phase tracks so that it is alternately attracted by the magnetic zones of the first track and the second track.
- the escape wheel thus rotates with a speed of rotation such that it advances an angular period of the two tracks at each oscillation of the resonator.
- the escape wheel provides the energy necessary to maintain the oscillation of the resonator arm carrying the magnetic coupling magnet and this resonator controls or regulates the rotational speed of this escapement wheel, which is proportional at the resonance frequency.
- There is therefore a magnetic exhaust associated with a resonator which together form a device regulating the running of a counter wheel of a watch movement.
- the aforementioned magnetic type regulating devices are provided in the prior art for resonators having a single degree of freedom for each resonant-moving part.
- the resonator is arranged so that the magnet, carried by a member undergoing a resonance movement, oscillates in a substantially radial direction, that is to say substantially orthogonal to the two annular magnetic tracks.
- the embodiments mentioned in the prior art have the advantage of having a frequency reduction between the frequency of the oscillation of the resonator and the rotation frequency (in revolutions / s) of the escapement wheel carrying the magnetic structure. No rotated mobile turns or oscillates at a frequency of the order of magnitude of the resonant frequency.
- the reduction factor is given by the number of angular periods of the annular magnetic tracks.
- the aforementioned advantage resulting from a frequency reduction between the oscillation of the resonator and the rotation of the escape wheel, has a corollary which poses a problem for the magnetic coupling strength.
- to increase the frequency reduction it is necessary to increase the number of periods of the magnetic tracks.
- an increase in the number of periods results in a decrease in the area of the magnetic zones of the annular tracks. Since the magnet of the resonator extends over an angular distance less than half a period of the annular tracks, the dimensions of this magnet must also decrease as the frequency reduction increases.
- Synchronization comprises a proportional relationship determined between the resonance frequency and the rotation frequency of the escape wheel.
- watchmaking devices of the magnetic type comprising a resonator with two degrees of freedom, in particular a resonator whose inertial part has a translational trajectory substantially describing a circle, rotating continuously in the same direction, are not known. .
- a need to design magnetic type escapements for such resonators with two degrees of freedom, with a reduction in the magnetic coupling, however exists in the field of watchmaking. This need seems even crucial when the resonator operates with a relatively high resonance frequency, for example resonators whose resonant organ turns a frequency greater than ten revolutions per second (10 revolutions / s 10 Hz).
- the object of the present invention is to respond to the identified needs in the field of clock control devices, in particular for resonators with two degrees of freedom with a circular resonance movement, and to find a solution to the problem related to the weak magnetic interaction in the case of resonators with a single degree of freedom associated with a known magnetic exhaust having a large frequency reduction.
- the subject of the present invention is a magnetic escapement equipping a mechanical horological movement and comprising an escape wheel driven by a motor device and associated with a resonator of this mechanical clockwork movement, this escape wheel comprising a first structure magnetic device defining, in a non-zero radial range of this escape wheel, a first periodic pattern with a first angular period P1 such that 360 ° / P1 is equal to a first integer number N1, the magnetic escapement comprising at least one magnet mounted on the resonator and magnetically coupled to the escape wheel so that, when the mechanical watch movement is operating, the magnet has a periodic resonance movement at a resonance frequency and the escape wheel rotates with a frequency proportional to this resonance frequency.
- the magnetic escapement furthermore comprises a second magnetic structure parallel to the first magnetic structure and defining, in said radial range, a second periodic pattern having a second angular period P2 such that 360 ° / P2 is equal to a second integer number N2 different from the integer N1, the difference in absolute value
- ⁇ N / 2, N being the lower number of the numbers N1 and N2.
- the first and second magnetic structures are arranged such that, when the watch movement is operating, the first magnetic structure rotates relative to the second magnetic structure at a first relative angular frequency F1 rel .
- the first periodic pattern and the second periodic pattern are selected so that they generate in said radial range, in projection on a geometrical surface parallel to the first and second magnetic structures, a combined pattern alternately defining at least the number
- Angular frequency is understood to be the number of revolutions per second corresponding to the inverse of the period of time of the periodic movement.
- the magnet has a magnetization axis perpendicular to the geometric surface of said combined pattern.
- the combined pattern defines a periodic combined pattern alternately having the number
- , ie P3 360 ° /
- the magnetic escapement according to the invention comprises a second magnet mounted on the resonator and supported by said resonant portion or by another resonant portion of the resonator.
- This second magnet is arranged relative to the first magnet on the other side of the first and second magnetic structures, so that it is aligned with the first magnet in a direction substantially parallel to the axis of rotation and has a motion periodic resonance similar to that of the first magnet at the resonant frequency.
- the second magnet has a magnetization axis parallel to that of the first magnet and in the opposite direction. In a second variant, the second magnet has a magnetization axis parallel to that of the first magnet and in the same direction.
- the magnetic escapement comprises a third magnetic structure defining a periodic pattern substantially identical to the periodic pattern defined by the first or second magnetic structure and superimposed thereto, this third periodic structure being integral with rotation with this first or second magnetic structure, in the case where the latter undergoes rotation.
- the two magnetic structures having the same periodic pattern are located respectively on one side and the other side of the magnetic structure having a different periodic pattern.
- the second magnetic structure is fixed relative to the watch movement, the first relative angular frequency F1 rel defining the angular frequency of the escape wheel relative to this watch movement.
- the present invention also relates to a first device regulating the movement of a watch movement comprising a magnetic escapement according to the invention and a resonator, a resonant part supporting said magnet undergoes, during the operation of the watch movement, an oscillation according to a degree of freedom.
- the resonator is arranged so that the center of the magnet in its rest position is substantially located, for any angular position of the escape wheel, on a zero position circle which is centered on the axis of rotation of the magnet. escape wheel and which is crossed by the degree of freedom of the resonant portion of the resonator.
- the periodic combined pattern defined by the magnetic escapement is located on a first side of the zero position circle projected perpendicularly into the geometrical surface, the annular region of the first and second magnetic structures defined by said radial range being magnetically coupled to the magnet in a first half cycle of each period of said oscillation so that, for each period of this oscillation, the periodic combined pattern rotates by an angular distance equal to its angular period P3.
- the periodic combined pattern is a first periodic combined pattern and the radial range is a first radial range, the first and second magnetic structures respectively defining, in a second non-zero radial range of the wheel. escapement located on the other side of the zero position circle relative to the first radial range, a third periodic pattern and a fourth periodic pattern which generate a second periodic combined pattern alternately having the number
- the second periodic combined pattern is angularly offset by half an angular period P3 relative to the first periodic combined pattern, this second periodic combined pattern also rotating with the relative angular frequency F2 rel of the first periodic combined pattern, the annular region of the first and second magnetic structures, defined by the second radial range, being magnetically coupled to the magnet in a second alternation of each period of said oscillation.
- the first and second periodic combined patterns are substantially contiguous.
- the present invention also relates to a second device for regulating the movement of a clockwork movement comprising a magnetic escapement according to the invention and a resonator having a resonant part supporting said magnet, this resonator being arranged in such a way that this resonant part is subjected to a radial return force relative to the axis of rotation of the escape wheel when the center of the magnet moves away from this axis of rotation, and so that the center of this magnet substantially defines a circle, centered on said axis of rotation, at an angular frequency of resonance when it is distant from this axis of rotation and that this magnet is rotated with a substantially constant torque.
- the annular region of the first and second magnetic structures is magnetically coupled to the magnet so that the magnet is rotated by a magnetic interaction torque resulting from the combined rotating pattern when a driving torque, in a useful range of the motor torque, is provided to the escape wheel, the angular frequency of the combined pattern being slaved to the resonant angular frequency in this useful range of the torque, which is selected so that the magnetic interaction torque remains less than a maximum magnetic interaction torque and that the circle described by the center of the magnet has a radius in the radial range for any motor torque of this useful range.
- the resonator is arranged and the useful range of the selected motor torque so that the magnet is entirely superimposed on the combined pattern for any motor torque of this useful range.
- This first circular network thus has a first angular period P1 equal to 360 ° / N1.
- This second circular network thus has a second angular period P2 equal to 360 ° / N2.
- the lines 4 extend substantially over half of the first angular period P1 and the lines 10 extend substantially over half of the second angular period P2.
- Magnetic material comprises a material with high magnetic permeability, in particular a ferromagnetic material.
- between the numbers N1 and N2 is here equal to (
- 1).
- between the numbers N1 and N2 is less than or equal to N / 2, ie
- ⁇ N / 2, where N is the lower number of the numbers N1 and N2.
- is less than or equal to N / 3 or
- ⁇ N / 3.
- the first and second circular arrays are mounted in parallel at a relatively short distance from one another. They are arranged in such a way that, when the watch movement is operating, the first network has a rotation relative to the second network, around the axis of rotation 6 of the escape wheel, at a first angular frequency F1.
- the second magnetic structure is fixed relative to the watch movement so that the frequency F1 is that of the first circular network in the watch movement (defining a fixed reference).
- the first and second circular arrays generate in an annular surface (thus having a non-zero radial range), in projection in a geometric plane parallel to these circular arrays, a combined pattern 14 defining a first zone 15 with a high proportion of magnetic surface and a second zone 16 with a lower proportion of magnetic surface.
- the combined pattern 14 rotates with a second angular frequency F2 which is in absolute value N1 times greater than the first angular frequency F1 for the particular case of the given example where the number
- 1.
- the magnetic surface density in the combined pattern varies substantially linearly between 50% and 100%. Magnetic surface proportion is understood to mean the ratio of the areas defined by the magnetic material of the first and second circular arrays in a given area of the combined pattern to the total area of that area.
- the first magnetic structure forms an escape wheel.
- the number ⁇ N can be positive or negative. In the case where it is positive, the combined pattern rotates in the same direction as the escape wheel. In the case where the number ⁇ N is negative, the combined pattern rotates in the opposite direction to that of the escape wheel; which corresponds mathematically to a negative frequency.
- the magnetic escapement 12 further comprises at least one magnet fixed to the resonator and coupled to the first and second circular networks, as will be discussed later.
- the first circular network 3 is similar to that of the Figure 1 but it extends over a greater radial distance.
- the second magnetic structure 18 forms two concentric circular arrays 19 and 20 which extend into respective contiguous annular surfaces.
- These two networks have the same number N2 of magnetic lines 21 and 22, separated by lines defined by vacuum or a substantially amagnetic material, and therefore have the same period P2. They are angularly offset by half a period P2 / 2 and thus have a phase shift of 180 °.
- N2 N1 + 2.
- a first combined pattern 25 which extends in an outer annular surface and a second combined pattern 26 which extends into an inner annular surface is obtained in projection in a parallel geometrical plane.
- 2
- each combined pattern alternately has two areas with a high proportion of magnetic area and two areas with a smaller proportion of magnetic area.
- the two combined patterns 24 and 26 also have a phase shift of 180 °.
- the alternation of zones with a high proportion of magnetic surface and zones with a smaller proportion of magnetic surface defines a periodic combined pattern having an angular period P3 whose value is equal to 360 ° divided by the absolute value of the difference
- between the numbers N1 and N2, ie P3 360 ° /
- the realization of figure 2 is a special case with a single circular network on the escape wheel which extends in an annular surface corresponding to the two concentric annular surfaces of the two circular arrays of the second magnetic structure.
- the first magnetic structure also comprises two distinct circular arrays of the same period P1.
- these two circular arrays have an angular offset of P1 / 4 and the two circular arrays of the second magnetic structure have an angular offset of P2 / 4.
- the two circular arrays of the first magnetic structure have different periods P1 and P2 and also those of the second magnetic structure, by inverting the periods P1 and P2 between the two magnetic structures.
- the magnetic escapement 24 comprises at least one magnet 32 mounted on the resonator and magnetically coupled to the two superimposed magnetic structures so that, when the mechanical clockwork movement is operating, this magnet has a periodic resonance movement at a resonance frequency.
- the magnet in magnetic interaction with the two magnetic structures undergoes a movement which is associated with the resulting combined pattern, which can rotate much faster than the escape wheel.
- the magnet has a magnetization axis perpendicular to the geometric surface of the combined pattern.
- the magnet is located above a first zone of the combined pattern having a high proportion of magnetic surface.
- the two arrays are angularly offset so that together they form a relatively continuous magnetic path for the field lines 34A of the magnet; which has the effect of reducing the magnetic reluctance for the magnet.
- the magnet is located above a second area of the combined pattern having a smaller proportion of area magnetic.
- the two networks are substantially superimposed so that the magnetic path for the magnet in these networks is interrupted by the voids or formed of a non-magnetic material provided between the magnetic lines. It is understood that the field lines 34B of the magnet at the two networks must pass through the void spaces or non-magnetic regions.
- Magnetic reluctance is therefore increased relative to the situation of the Figure 3A .
- a variation of the magnetic potential energy E pot which is shown by the graph 36 to the Figure 3C .
- This variation of the potential magnetic energy E pot generates a force on the magnet to drive it in rotation and / or to maintain a resonance movement using two concentric annular magnetic tracks.
- FIG. 4 To the Figure 4 is represented a first embodiment of a regulator device 40 according to a first type.
- This regulating device comprises a magnetic escapement 24 as described in FIG. Figure 2 .
- the two superimposed magnetic structures 2 and 18 generate two periodic combined patterns 25 and 26, 180 ° out of phase, as indicated above.
- the resonator 42 is formed by a tuning fork with two branches 43 and 44. At the free ends of these two branches are respectively fixed two magnets 46 and 48 with axial magnetization. In their rest position, the centers of the two magnets are located on a circle 50, defining a circle of zero position. This circle 50 is chosen so that it is coincident with the circle separating the two contiguous combined patterns.
- the two combined patterns form two magnetic tracks with a periodic variation of the potential energy of the oscillator, formed of the tuning fork 42 and the magnetic escapement.
- Each magnet oscillates with a substantially radial degree of freedom. It is attracted alternately by the areas of low magnetic reluctance of the two magnetic tracks. Above each track, the magnets accumulate magnetic potential energy and brake the escape wheel. By crossing the zero position circle, they each receive a pulse serving to maintain the resonance since they experience a magnetic potential jump by virtue of the angular offset of the two periodic combined patterns 25 and 26.
- the magnets follow a trajectory 50 corresponding to an oscillation according to the degree of freedom of each magnet.
- a second embodiment of a regulator device 60 comprising a magnetic escapement 24A formed by a first magnetic structure 2 defining the first circular network 3, this structure 2 being mounted on a shaft and rotating around a axis of rotation 6.
- the magnetic escapement is furthermore formed by a second magnetic structure 18 defining two out-of-phase circular networks as explained above in relation to the Figures 2 and 4 .
- This second embodiment differs from the previous embodiment in that the resonant portion 68 of the resonator 70 comprises two magnets 32 and 62 respectively arranged on both sides of the two magnetic structures and forming the magnetic escapement 24A.
- Such a configuration solves a problem of the first embodiment in that, insofar as the two magnetic structures are substantially equidistant from the respective magnets facing them, the axial attraction forces on the two magnets by the Magnetic structures compensate each other for the most part. It is the same for the attraction forces exerted by the two magnets on the set of two magnetic structures.
- the two magnets are attached to the ends of a non-magnetic member having a U shape.
- the resonator is shown with a schematic spring.
- the resonant portion 68 may for example be attached to a free end of a tuning fork.
- the operation is similar to that of the first embodiment.
- Each magnet is magnetically coupled to the circular arrays in the manner previously described. They are aligned axially so as to both be perpendicular to the zero position circle.
- the structure 18 is fixed and supported by a disc 66 formed of a non-magnetic material. A lateral recess is provided in this disc to allow the resonant portion 68 to pass under the structure 18.
- the magnetic structures 2 and 18 each have an inner annular portion and an outer annular portion which connect the lines of the circular networks 3, 19 and 20.
- the two magnets have an axial magnetization of opposite direction.
- This configuration is advantageous because it makes it possible to amplify the magnetic interaction as can be seen in FIG. Figure 6 .
- the magnetic interaction is in first approximation approximately equal to twice that for the case of a single magnet.
- the two magnets repel each other in the empty spaces between the magnetic lines. This repulsive force increases the magnetic potential energy E pot.
- the curve 74 of E pot has a profile similar to that of curve 36 of the Figure 3C . However, a computer simulation has established that the amplitude of the periodic curve 74 is a priori an order of magnitude greater than the amplitude of the periodic curve 36.
- both magnets have an axial magnetization of the same direction.
- the lines of the circular networks are provided here thicker. It is observed on the graph of the magnetic potential energy that the curve 76 of E pot is the opposite of the curve 74. Indeed, since in this variant the magnetic flux between the two magnets is substantially axially channeled, a The area of high magnetic area proportion of a combined pattern has a greater magnetic reluctance for the two magnets than in the case where they face an area of least proportion of magnetic area.
- the amplitude of the periodic curve 76 is a priori in the configuration represented approximately half of that of the periodic curve 74.
- FIG. Figure 8 A third embodiment of a regulator device 80 of the first type is shown in FIG. Figure 8 .
- the common elements with the realization of the Figure 5 will not be described again in detail.
- the regulator device comprises a resonator 70 and a magnetic escapement 24B formed by a first magnetic structure 2A, defining a first circular network similar to the network 3 of the Figure 2 , and by a second magnetic structure 18A defining two concentric circular networks corresponding to the networks 19 and 20 of the figure 2 . Note that in this case, it is the two concentric circular arrays that form the escape wheel and which rotate around the axis 6, the structure 2A being fixedly mounted in the watch movement.
- This third embodiment differs essentially from the previous embodiment in that it comprises a third magnetic structure 82 defining a fourth circular network which extends, like the first network, in an annular surface comprising the second and third phase-shifted networks of the structure. 18A.
- This third structure is integral with the first structure 2A, the fourth circular network being identical to the first circular network and their magnetic lines are superimposed axially (no angular offset between the two networks).
- the first and fourth networks are respectively located on one side and the other of the magnetic structure 18A forming the second and third networks.
- the magnetic structure 18A comprises a central annular portion which is continuous. Between the second and third networks is provided an annular intermediate portion which is continuous, preferably of magnetic material. In addition, there is also provided a continuous annular peripheral portion.
- the three continuous annular parts allow to have a magnetic structure 18A in one piece with the magnetic lines of the two networks fixed at both ends. So that the continuous annular zones do not disturb the operation of the magnetic escapement, it is expected that the circular arrays extend over a radial length substantially greater than that of the oscillating magnets.
- This structure 18A is taken in a nonmagnetic hub 86 mounted on the shaft of the escape wheel.
- the two fixed structures 2A and 82 respectively comprise two continuous annular peripheral parts which are connected by a nonmagnetic spacer 84.
- the two superimposed magnetic structures are attracted to each other because of the magnetic flux of the magnets. Thanks to the superposition of the three magnetic structures, these Most of the attraction forces cancel out if the intermediate magnetic structure is located substantially in the middle of the other two.
- the two concentric out-of-phase networks are provided in the first and third magnetic structures while the second magnetic structure forms a single extended circular network.
- the first and third outer structures are mounted on the shaft of the escape wheel and are integral in rotation, while the second intermediate structure is fixedly mounted in the watch movement.
- This regulator device 90 is distinguished by the fact that the magnetic escapement 24C comprises two magnetic structures 2B and 82A, located on either side of an escape wheel, which are connected to the watch movement by two non-magnetic supports 94 and 96 central respectively fixed in two bridges 95 and 97, and in that the two intermediate circular networks 19 and 20 are doubled and arranged on both sides of a nonmagnetic disc 92 forming the escape wheel.
- the regulator device 100 comprises a magnetic escapement 12 as described with the aid of FIG. Figure 1 , with the only difference that the superimposed circular networks have more magnetic lines and thus a smaller angular period. However, as in Figure 1 , the difference of magnetic lines
- 1).
- An escape wheel (not shown entirely) carries one of the two magnetic structures forming the combined pattern 14 and rotates about the central axis 6 circular networks defined by these two magnetic structures.
- the regulator device further comprises a resonator 102 having a resonant portion comprises a magnet 104.
- This resonator has two degrees of freedom with a resonance mode in which the magnet 104 substantially follows a circular path with an angular frequency of resonance, without turning on itself.
- this resonator is arranged so that, when the center of the magnet moves away from the axis of rotation 6, its resonant portion is subjected to a radial restoring force relative to the axis of rotation 6, this restoring force is preferably angularly isotropic and radially linear so that the regulating device is isochronous.
- the resonator is arranged so that the center of the magnet 104 substantially follows a circular path, centered on the axis of rotation, with an angular frequency of resonance F res when it is distant from this axis of rotation and that this magnet is rotated with a substantially constant torque.
- the trajectory can also be elliptical in this system without harming isochronism. In the latter case, it will be ensured that the magnet remains at least partially superimposed on the combined pattern formed by the superimposed circular magnetic gratings.
- Such a resonator is shown schematically in the Figure 10 by a magnet 104 connected to two springs 106 and 108 which are orthogonal and which have substantially the same coefficient of elasticity, these two springs being respectively mounted on the supports 110 and 112 which slip without friction respectively in two orthogonal rails 114 and 116; which is schematized by trolleys on wheels which theoretically have no inertia.
- the vector sum of the radial forces of the springs generates a restoring force (centripetal force) allowing the inertial portion of the resonator to follow a substantially circular or elliptical trajectory.
- the annular region of the first and second magnetic structures defining the combined pattern 14 with a first area 15 having a high proportion of magnetic area and a second area 16 having a smaller proportion of magnetic area, is magnetically coupled to the magnet 104 so that this magnet is rotated by a magnetic interaction couple resulting from the combined pattern rotating at angular frequency ⁇ .
- the combined pattern rotates when a torque motor, a useful range of the engine torque is supplied to the escapement wheel, the angular frequency ⁇ of the combined pattern being slaved to the angular resonance frequency F res in this useful range of the torque , the latter being selected so that the aforementioned magnetic interaction torque remains below a maximum magnetic interaction torque and said circle described by said center of the magnet has a radius comprised in the radial range of the combined pattern 14 for any motor torque of this useful range.
- the magnetic interaction in this resonator has the effect of synchronizing the angular frequency ⁇ of the escape wheel with the resonance frequency F res of the resonator.
- the combined pattern 14 generates a variation of the potential energy E pot in the resonator, as a function of the relative angular position of the magnet and this combined pattern, between a minimum energy when the magnet is above the first zone 15 and a maximum energy when it is above the second zone 16.
- the angular gradient of this potential energy generates a tangential driving force on the magnet. To avoid a loss of synchronization, it will be ensured that the braking torque exerted by the magnet on the escape wheel remains less than the maximum magnetic interaction torque depending on the maximum value of the potential energy gradient E pot .
- the resonator is arranged and the useful range of the selected motor torque so that the magnet 104 is entirely superimposed on the combined pattern 14 for any motor torque of this useful range.
- the Figure 11 shows an alternative embodiment of the regulating device of the Figure 10 .
- the elements already described above will not be again.
- This variant is distinguished from the previous one by the fact that the magnetic escapement 24A is formed by two superimposed circular arrays with a difference in absolute value
- 2, similarly to the realization of one of the two combined patterns of the Figure 2 .
- the combined pattern 25A alternately has two areas 15A having a high proportion of magnetic area and two areas 16A having a smaller proportion of magnetic area. Since the difference in magnetic potential energy between the extreme values is substantially equal to that of the preceding variant, but this difference occurs over an angular range that is twice as small, the maximum magnetic magnetic interaction force is substantially twice stronger.
- the ratio between the angular frequency of the combined pattern 25A and the rotation frequency of the escapement wheel carrying one of the two circular magnetic gratings is equal to half of the ratio of the preceding variant.
- the useful range of the engine torque is increased but the multiplication ratio between the frequency of the escape wheel and the resonance frequency is decreased.
- the magnet 104 has an angular offset ⁇ less than 90 ° and in particular less than 45 °, this angular displacement varying as a function of the torque resulting from the magnetic interaction between the magnet 104 and the combined pattern 25A.
- the Figure 12 schematically represents a second embodiment of the second regulator device according to the invention.
- This regulator device 130 is a particular embodiment implementing the physical characteristics mentioned in the preceding description of the first embodiment.
- the resonator 132 is formed by a bar 134 elastically deformable in two degrees of freedom substantially defining a sphere portion, this bar being embedded in a base 136.
- This bar carries at its free end a magnet 104A.
- the magnetic exhaust 12A is similar to that described in Figures 2 and 10 .
- first magnetic structure 2A forming a first circular network 3A whose magnetic lines 4A extend in a first frustoconical surface
- second magnetic structure 8A forming a second circular network 9A whose magnetic lines 10A extend in a second frustoconical surface parallel to the first frustoconical surface.
- the first magnetic structure 2A is mounted on a shaft 138 which is guided in rotation by two ball bearings arranged in a bridge 142.
- the second magnetic structure is fixed and arranged on a non-magnetic support 146.
- the structure 2A comprises a continuous inner annular portion which connects the magnetic lines 4A and the structure 8A comprises a continuous outer annular portion which connects the magnetic lines 10A.
- a frustoconical portion 140 At one end of the shaft 138 is provided a frustoconical portion 140 forming a central circular stop for the magnet 104A, this stop being arranged so that at least the major part of this magnet remains superimposed on the combined pattern 14A when no torque engine is provided to the escape wheel formed here by the first magnetic structure 2A, the shaft 138 and a pinion 144.
- This pinion is associated with a counting gear of a mechanical watch movement through which it receives a motor torque provided by a motor device (not shown).
- the invention relates to a mechanical clockwork comprising a regulating device, a counter wheel clocked by this regulating device and a motor device driving the counter wheel and maintaining a resonance mode of the regulating device.
- This watch movement is characterized in that it comprises a magnetic escapement according to the invention or a regulating device according to the invention.
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Abstract
L'échappement magnétique horloger (12), respectivement le dispositif régulateur comportant un tel échappement comprennent un premier réseau circulaire (3) formé de N1 lignes magnétiques (4) et un deuxième réseau circulaire (9) formé de N2 lignes magnétiques (10), le nombre N2 étant différent du nombre N1. Les premier et deuxième réseaux sont superposés de manière à définir un motif combiné (14) présentant un effet Moiré magnétique. Le motif combiné est couplé magnétiquement à au moins un aimant d'un résonateur pour cadencer la marche d'un mouvement horloger mécanique. La première structure magnétique est portée par une roue d'échappement et peut tourner relativement à la deuxième structure magnétique fixe avec une fréquence angulaire F1. Le motif combiné tourne avec une fréquence angulaire F2 supérieure et égale à la fréquence angulaire F1 multipliée par le nombre N1 et divisée par le nombre ”N égal à ce nombre N1 moins le nombre N2, soit F2=F1 ·N1/”N.The horological magnetic escapement (12) and the regulating device comprising such an escapement comprise a first circular network (3) formed of N1 magnetic lines (4) and a second circular array (9) formed of N2 magnetic lines (10), the number N2 being different from the number N1. The first and second networks are superimposed to define a combined pattern (14) having a magnetic Moire effect. The combined pattern is magnetically coupled to at least one magnet of a resonator to pace the march of a mechanical watch movement. The first magnetic structure is carried by an escape wheel and is rotatable relative to the second fixed magnetic structure with an angular frequency F1. The combined pattern rotates with an angular frequency F2 greater than and equal to the angular frequency F1 multiplied by the number N1 and divided by the number "N equal to this number N1 minus the number N2, ie F2 = F1 · N1 /" N.
Description
La présente invention concerne le domaine des dispositifs régulateurs de la marche d'un mouvement horloger. En particulier, la présente invention concerne les échappements horlogers du type magnétique dont les fonctions usuelles sont l'entretien d'un mode de résonance d'un résonateur, notamment une oscillation ou une rotation continue d'une partie inertielle de ce résonateur, et le cadencement d'un rouage compteur. Dans le cadre de la présente invention, l'échappement magnétique assure ces deux fonctions au moyen d'une roue d'échappement comprenant une structure magnétique, laquelle est couplée magnétiquement à au moins un aimant porté par une partie du résonateur subissant le mouvement de résonance.The present invention relates to the field of devices regulating the movement of a watch movement. In particular, the present invention relates to watchmaking escapements of the magnetic type, the usual functions of which are the maintenance of a resonance mode of a resonator, in particular an oscillation or a continuous rotation of an inertial part of this resonator, and the timing of a counter wheel. In the context of the present invention, the magnetic escapement provides these two functions by means of an escape wheel comprising a magnetic structure, which is magnetically coupled to at least one magnet carried by a part of the resonator undergoing the resonance movement. .
Les dispositifs de régulation de la vitesse d'une roue, nommé aussi rotor, par un couplage magnétique, aussi nommé accouplement magnétique, sont connus depuis de nombreuses années. L'application horlogère est aussi connue. De nombreuses demandes de brevet relatives à ce domaine ont été déposées par la société Horstmann Clifford Magnetics pour des inventions de C. F. Clifford. On citera notamment les documents
On remarquera que les dispositifs régulateurs du type magnétique mentionnés précédemment sont prévus dans l'art antérieur pour des résonateurs ayant un seul degré de liberté pour chaque partie subissant un mouvement de résonance. En général, on agence le résonateur de manière que l'aimant, porté par un organe subissant un mouvement de résonance, oscille selon une direction sensiblement radiale, c'est à-dire sensiblement orthogonale aux deux pistes magnétiques annulaires. Dans ce cas, les réalisations mentionnées de l'art antérieur présentent l'avantage d'avoir une réduction de fréquence entre la fréquence de l'oscillation du résonateur et la fréquence de rotation (en tours /s) de la roue d'échappement portant la structure magnétique. Aucun mobile pivoté ne tourne ou n'oscille à une fréquence de l'ordre de grandeur de la fréquence de résonance. Le facteur de réduction est donné par le nombre de périodes angulaires des pistes magnétiques annulaires.It will be appreciated that the aforementioned magnetic type regulating devices are provided in the prior art for resonators having a single degree of freedom for each resonant-moving part. In general, the resonator is arranged so that the magnet, carried by a member undergoing a resonance movement, oscillates in a substantially radial direction, that is to say substantially orthogonal to the two annular magnetic tracks. In this case, the embodiments mentioned in the prior art have the advantage of having a frequency reduction between the frequency of the oscillation of the resonator and the rotation frequency (in revolutions / s) of the escapement wheel carrying the magnetic structure. No rotated mobile turns or oscillates at a frequency of the order of magnitude of the resonant frequency. The reduction factor is given by the number of angular periods of the annular magnetic tracks.
Dans le cas de ces résonateurs à un seul degré de liberté, l'avantage susmentionné, découlant d'une réduction de fréquence entre l'oscillation du résonateur et la rotation de la roue d'échappement, a un corolaire qui pose un problème pour la force du couplage magnétique. En effet, pour augmenter la réduction de fréquence il est nécessaire d'augmenter le nombre de périodes des pistes magnétiques. Pour un diamètre donné de la roue d'échappement, une augmentation du nombre de périodes a pour conséquence une diminution de surface des zones magnétiques des pistes annulaires. Comme l'aimant du résonateur s'étend sur une distance angulaire inférieure à une demi-période des pistes annulaires, les dimensions de cet aimant doivent aussi diminuer lorsque la réduction de fréquence augmente. On comprend donc que la force d'interaction magnétique entre le résonateur et la roue d'échappement diminue; ce qui limite le couple pouvant être appliqué à la roue d'échappement et augmente donc le risque de perte de la synchronisation entre ce résonateur et cette roue d'échappement. Par synchronisation, on comprend ici une relation proportionnelle déterminée entre la fréquence de résonance et la fréquence de rotation de la roue d'échappement.In the case of these resonators with a single degree of freedom, the aforementioned advantage, resulting from a frequency reduction between the oscillation of the resonator and the rotation of the escape wheel, has a corollary which poses a problem for the magnetic coupling strength. Indeed, to increase the frequency reduction it is necessary to increase the number of periods of the magnetic tracks. For a given diameter of the escape wheel, an increase in the number of periods results in a decrease in the area of the magnetic zones of the annular tracks. Since the magnet of the resonator extends over an angular distance less than half a period of the annular tracks, the dimensions of this magnet must also decrease as the frequency reduction increases. It is therefore understood that the magnetic interaction force between the resonator and the escape wheel decreases; which limits the torque that can be applied to the escape wheel and therefore increases the risk of loss of synchronization between the resonator and the escape wheel. Synchronization here comprises a proportional relationship determined between the resonance frequency and the rotation frequency of the escape wheel.
On remarquera finalement que des dispositifs régulateurs horlogers du type magnétique comprenant un résonateur à deux degrés de liberté, en particulier un résonateur dont la partie inertielle a une trajectoire en translation décrivant sensiblement un cercle, en tournant continument dans un même sens, ne sont pas connus. Un besoin de concevoir des échappements du type magnétique pour de tels résonateurs à deux degrés de liberté, avec une réduction au niveau du couplage magnétique, existe toutefois dans le domaine de l'horlogerie. Ce besoin paraît même crucial lorsque le résonateur fonctionne avec une relativement haute fréquence de résonance, par exemple des résonateurs dont l'organe résonant tourne à une fréquence supérieure à dix tours par seconde (10 tours /s = 10Hz). En effet, un couplage mécanique, qui consisterait à relier un tel organe résonant à un mobile, aurait pour conséquence d'entraîner en rotation ce mobile à la fréquence de résonance. Un mobile pivoté à une fréquence de rotation supérieure à cinq ou six tours par seconde pose un problème majeur de perte d'énergie par frottement et un problème d'usure au niveau des paliers.Finally, it will be noted that watchmaking devices of the magnetic type comprising a resonator with two degrees of freedom, in particular a resonator whose inertial part has a translational trajectory substantially describing a circle, rotating continuously in the same direction, are not known. . A need to design magnetic type escapements for such resonators with two degrees of freedom, with a reduction in the magnetic coupling, however exists in the field of watchmaking. This need seems even crucial when the resonator operates with a relatively high resonance frequency, for example resonators whose resonant organ turns a frequency greater than ten revolutions per second (10 revolutions / s = 10 Hz). Indeed, a mechanical coupling, which would connect such a resonant member to a mobile, would result in rotating this mobile to the resonance frequency. A mobile rotated at a rotation frequency greater than five or six revolutions per second poses a major problem of energy loss by friction and a wear problem at the bearings.
La présente invention a pour but de répondre aux besoins identifiés dans le domaine des dispositifs régulateurs horlogers, en particulier pour les résonateurs à deux degrés de liberté avec un mouvement de résonance circulaire, et de trouver une solution au problème lié à la faible interaction magnétique dans le cas des résonateurs à un seul degré de liberté associé à un échappement magnétique connu présentant une grande réduction de fréquence.The object of the present invention is to respond to the identified needs in the field of clock control devices, in particular for resonators with two degrees of freedom with a circular resonance movement, and to find a solution to the problem related to the weak magnetic interaction in the case of resonators with a single degree of freedom associated with a known magnetic exhaust having a large frequency reduction.
A cet effet, la présente invention a pour objet un échappement magnétique équipant un mouvement horloger mécanique et comprenant une roue d'échappement entraînée par un dispositif moteur et associée à un résonateur de ce mouvement horloger mécanique, cette roue d'échappement comprenant une première structure magnétique définissant, dans une plage radiale non nulle de cette roue d'échappement, un premier motif périodique avec une première période angulaire P1 telle que 360°/ P1 est égal à un premier nombre entier N1, l'échappement magnétique comprenant au moins un aimant monté sur le résonateur et couplé magnétiquement à la roue d'échappement de manière que, lorsque le mouvement horloger mécanique fonctionne, cet aimant présente un mouvement de résonance périodique à une fréquence de résonance et que la roue d'échappement tourne avec une fréquence proportionnelle à cette fréquence de résonance. L'échappement magnétique comprend en outre une deuxième structure magnétique parallèle à la première structure magnétique et définissant, dans ladite plage radiale, un deuxième motif périodique ayant une deuxième période angulaire P2 telle que 360°/P2 est égal à un deuxième nombre entier N2 différent du nombre entier N1, la différence en valeur absolue |ΔN| entre les nombres N1 et N2 étant un nombre inférieur ou égal à N/2, soit |ΔN|<= N/2, N étant le nombre inférieur des nombres N1 et N2. Les première et deuxième structures magnétiques sont agencées de manière que, lorsque le mouvement horloger fonctionne, la première structure magnétique a une rotation relativement à la deuxième structure magnétique à une première fréquence angulaire relative F1rel . Le premier motif périodique et le deuxième motif périodique sont sélectionnés de manière qu'ils génèrent dans ladite plage radiale, en projection sur une surface géométrique parallèle aux première et deuxième structures magnétiques, un motif combiné définissant en alternance au moins le nombre |ΔN| de première(s) zone(s) avec une première proportion de surface magnétique et au moins ce nombre |ΔN| de deuxième(s) zone(s) avec une deuxième proportion de surface magnétique qui est inférieure à la première proportion, et que le motif combiné tourne relativement à la deuxième structure magnétique avec une deuxième fréquence angulaire relative F2rel égale à la première fréquence angulaire relative F1re! multipliée par le nombre N1 et divisée par la différence ΔN entre les nombres N1 et N2, soit F2rel = F1rel·N1 / ΔN où ΔN = N1-N2.For this purpose, the subject of the present invention is a magnetic escapement equipping a mechanical horological movement and comprising an escape wheel driven by a motor device and associated with a resonator of this mechanical clockwork movement, this escape wheel comprising a first structure magnetic device defining, in a non-zero radial range of this escape wheel, a first periodic pattern with a first angular period P1 such that 360 ° / P1 is equal to a first integer number N1, the magnetic escapement comprising at least one magnet mounted on the resonator and magnetically coupled to the escape wheel so that, when the mechanical watch movement is operating, the magnet has a periodic resonance movement at a resonance frequency and the escape wheel rotates with a frequency proportional to this resonance frequency. The magnetic escapement furthermore comprises a second magnetic structure parallel to the first magnetic structure and defining, in said radial range, a second periodic pattern having a second angular period P2 such that 360 ° / P2 is equal to a second integer number N2 different from the integer N1, the difference in absolute value | ΔN | between the numbers N1 and N2 being a number less than or equal to N / 2, ie | ΔN | <= N / 2, N being the lower number of the numbers N1 and N2. The first and second magnetic structures are arranged such that, when the watch movement is operating, the first magnetic structure rotates relative to the second magnetic structure at a first relative angular frequency F1 rel . The first periodic pattern and the second periodic pattern are selected so that they generate in said radial range, in projection on a geometrical surface parallel to the first and second magnetic structures, a combined pattern alternately defining at least the number | ΔN | of first zone (s) with a first proportion of magnetic surface and at least this number | ΔN | second zone (s) with a second proportion of magnetic area that is smaller than the first proportion, and that the combined pattern rotates relative to the second magnetic structure with a second relative angular frequency F2 rel equal to the first angular frequency relative F1 re! multiplied by the number N1 and divided by the difference ΔN between the numbers N1 and N2, ie F2 rel = F1 rel · N1 / ΔN where ΔN = N1-N2.
On comprend par fréquence angulaire le nombre de tours par seconde, correspondant à l'inverse de la période temporelle du mouvement périodique.Angular frequency is understood to be the number of revolutions per second corresponding to the inverse of the period of time of the periodic movement.
Dans une variante préférée, l'aimant présente un axe d'aimantation perpendiculaire à la surface géométrique dudit motif combiné.In a preferred variant, the magnet has a magnetization axis perpendicular to the geometric surface of said combined pattern.
Dans un mode de réalisation préféré, le motif combiné définit un motif combiné périodique présentant en alternance le nombre |ΔN| de première(s) zones et ce nombre |ΔN| de deuxième(s) zones, une quelconque première zone et une deuxième zone adjacente définissant une période angulaire P3 de ce motif combiné périodique dont la valeur est égale à 360° divisé par le nombre |ΔN|, soit P3 = 360 ° /|ΔN|.In a preferred embodiment, the combined pattern defines a periodic combined pattern alternately having the number | ΔN | of first zone (s) and this number | ΔN | second zone (s), one any first zone and a second adjacent zone defining an angular period P3 of this periodic combined pattern whose value is equal to 360 ° divided by the number | ΔN |, ie P3 = 360 ° / | ΔN |.
Dans un mode de réalisation perfectionné, l'échappement magnétique selon l'invention comprend un deuxième aimant monté sur le résonateur et supporté par ladite partie résonnante ou par une autre partie résonnante du résonateur. Ce deuxième aimant est agencé relativement au premier aimant de l'autre côté des première et deuxième structures magnétiques, de manière qu'il est aligné avec le premier aimant selon une direction sensiblement parallèle à l'axe de rotation et qu'il présente un mouvement de résonance périodique semblable à celui du premier aimant à la fréquence de résonance.In an improved embodiment, the magnetic escapement according to the invention comprises a second magnet mounted on the resonator and supported by said resonant portion or by another resonant portion of the resonator. This second magnet is arranged relative to the first magnet on the other side of the first and second magnetic structures, so that it is aligned with the first magnet in a direction substantially parallel to the axis of rotation and has a motion periodic resonance similar to that of the first magnet at the resonant frequency.
Dans une première variante, le deuxième aimant à un axe d'aimantation parallèle à celui du premier aimant et de sens opposé. Dans une deuxième variante, le deuxième aimant à un axe d'aimantation parallèle à celui du premier aimant et de même sens.In a first variant, the second magnet has a magnetization axis parallel to that of the first magnet and in the opposite direction. In a second variant, the second magnet has a magnetization axis parallel to that of the first magnet and in the same direction.
Dans une variante avantageuse du mode de réalisation perfectionné, l'échappement magnétique comprend une troisième structure magnétique définissant un motif périodique sensiblement identique au motif périodique défini par la première ou deuxième structure magnétique et superposé à celui-ci, cette troisième structure périodique étant solidaire en rotation avec cette première ou deuxième structure magnétique, dans le cas où cette dernière subit une rotation. Les deux structures magnétiques ayant un même motif périodique sont situées respectivement d'un côté et de l'autre de la structure magnétique présentant un motif périodique différent.In an advantageous variant of the improved embodiment, the magnetic escapement comprises a third magnetic structure defining a periodic pattern substantially identical to the periodic pattern defined by the first or second magnetic structure and superimposed thereto, this third periodic structure being integral with rotation with this first or second magnetic structure, in the case where the latter undergoes rotation. The two magnetic structures having the same periodic pattern are located respectively on one side and the other side of the magnetic structure having a different periodic pattern.
Dans une variante avantageuse, la deuxième structure magnétique est fixe relativement au mouvement horloger, la première fréquence angulaire relative F1rel définissant la fréquence angulaire de la roue d'échappement relativement à ce mouvement horloger.In an advantageous variant, the second magnetic structure is fixed relative to the watch movement, the first relative angular frequency F1 rel defining the angular frequency of the escape wheel relative to this watch movement.
La présente invention concerne également un premier dispositif régulateur de la marche d'un mouvement horloger comprenant un échappement magnétique selon l'invention et un résonateur dont une partie résonnante supportant ledit aimant subit, lors du fonctionnement du mouvement horloger, une oscillation selon un degré de liberté. Le résonateur est agencé de manière que le centre de l'aimant dans sa position de repos est sensiblement situé, pour toute position angulaire de la roue d'échappement, sur un cercle de position zéro qui est centré sur l'axe de rotation de la roue d'échappement et qui est traversé par le degré de liberté de la partie résonante du résonateur. Le motif combiné périodique défini par l'échappement magnétique est situé d'un premier côté du cercle de position zéro projeté perpendiculairement dans la surface géométrique, la région annulaire des première et deuxième structures magnétiques, définie par ladite plage radiale, étant couplée magnétiquement à l'aimant dans une première alternance de chaque période de ladite oscillation de manière que, pour chaque période de cette oscillation, le motif combiné périodique tourne d'une distance angulaire égale à sa période angulaire P3.The present invention also relates to a first device regulating the movement of a watch movement comprising a magnetic escapement according to the invention and a resonator, a resonant part supporting said magnet undergoes, during the operation of the watch movement, an oscillation according to a degree of freedom. The resonator is arranged so that the center of the magnet in its rest position is substantially located, for any angular position of the escape wheel, on a zero position circle which is centered on the axis of rotation of the magnet. escape wheel and which is crossed by the degree of freedom of the resonant portion of the resonator. The periodic combined pattern defined by the magnetic escapement is located on a first side of the zero position circle projected perpendicularly into the geometrical surface, the annular region of the first and second magnetic structures defined by said radial range being magnetically coupled to the magnet in a first half cycle of each period of said oscillation so that, for each period of this oscillation, the periodic combined pattern rotates by an angular distance equal to its angular period P3.
Dans un mode de réalisation préféré du premier dispositif régulateur, le motif combiné périodique est un premier motif combiné périodique et la plage radiale est une première plage radiale, les première et deuxième structures magnétiques définissant respectivement, dans une deuxième plage radiale non nulle de la roue d'échappement située de l'autre côté du cercle de position zéro relativement à la première plage radiale, un troisième motif périodique et un quatrième motif périodique qui génèrent un deuxième motif combiné périodique présentant en alternance le nombre |ΔN| de troisième(s) zone(s), avec une troisième proportion de surface magnétique supérieure à ladite deuxième proportion, et ce nombre |ΔN| de quatrième(s) zone(s) avec une quatrième proportion de surface magnétique qui est inférieure aux première et troisième proportions, ce deuxième motif combiné périodique ayant ladite période angulaire P3 . Le deuxième motif combiné périodique est décalé angulairement de la moitié d'une période angulaire P3 relativement au premier motif combiné périodique, ce deuxième motif combiné périodique tournant également avec la fréquence angulaire relative F2rel du premier motif combiné périodique, la région annulaire des première et deuxième structures magnétiques, définie par la deuxième plage radiale, étant couplée magnétiquement à l'aimant dans une deuxième alternance de chaque période de ladite oscillation.In a preferred embodiment of the first regulating device, the periodic combined pattern is a first periodic combined pattern and the radial range is a first radial range, the first and second magnetic structures respectively defining, in a second non-zero radial range of the wheel. escapement located on the other side of the zero position circle relative to the first radial range, a third periodic pattern and a fourth periodic pattern which generate a second periodic combined pattern alternately having the number | ΔN | third zone (s), with a third proportion of magnetic area greater than said second proportion, and this number | ΔN | fourth zone (s) with a fourth proportion of magnetic area that is smaller than the first and third proportions, this second periodic combined pattern having said angular period P3. The second periodic combined pattern is angularly offset by half an angular period P3 relative to the first periodic combined pattern, this second periodic combined pattern also rotating with the relative angular frequency F2 rel of the first periodic combined pattern, the annular region of the first and second magnetic structures, defined by the second radial range, being magnetically coupled to the magnet in a second alternation of each period of said oscillation.
Dans une variante particulière, les premier et deuxième motifs combinés périodiques sont sensiblement contigus.In a particular variant, the first and second periodic combined patterns are substantially contiguous.
La présente invention concerne également un deuxième dispositif régulateur de la marche d'un mouvement horloger comprenant un échappement magnétique selon l'invention et un résonateur ayant une partie résonnante supportant ledit aimant, ce résonateur étant agencé de manière que cette partie résonante est soumise à une force de rappel radiale relativement à l'axe de rotation de la roue d'échappement lorsque le centre de l'aimant s'éloigne de cet axe de rotation, et de manière que le centre de cet aimant décrive sensiblement un cercle, centré sur ledit axe de rotation, à une fréquence angulaire de résonance lorsqu'il est éloigné de cet axe de rotation et que cet aimant est entraîné en rotation avec un couple sensiblement constant. La région annulaire des première et deuxième structures magnétiques, définie par ladite plage radiale, est couplée magnétiquement à l'aimant de manière que cet aimant est entraîné en rotation par un couple d'interaction magnétique résultant du motif combiné tournant lorsqu'un couple moteur, dans une plage utile du couple moteur, est fourni à la roue d'échappement, la fréquence angulaire du motif combiné étant asservie à la fréquence angulaire de résonance dans cette plage utile du couple, laquelle est sélectionnée de manière que le couple d'interaction magnétique reste inférieur à un couple d'interaction magnétique maximal et que le cercle décrit par le centre de l'aimant a un rayon compris dans la plage radiale pour tout couple moteur de cette plage utile.The present invention also relates to a second device for regulating the movement of a clockwork movement comprising a magnetic escapement according to the invention and a resonator having a resonant part supporting said magnet, this resonator being arranged in such a way that this resonant part is subjected to a radial return force relative to the axis of rotation of the escape wheel when the center of the magnet moves away from this axis of rotation, and so that the center of this magnet substantially defines a circle, centered on said axis of rotation, at an angular frequency of resonance when it is distant from this axis of rotation and that this magnet is rotated with a substantially constant torque. The annular region of the first and second magnetic structures, defined by said radial range, is magnetically coupled to the magnet so that the magnet is rotated by a magnetic interaction torque resulting from the combined rotating pattern when a driving torque, in a useful range of the motor torque, is provided to the escape wheel, the angular frequency of the combined pattern being slaved to the resonant angular frequency in this useful range of the torque, which is selected so that the magnetic interaction torque remains less than a maximum magnetic interaction torque and that the circle described by the center of the magnet has a radius in the radial range for any motor torque of this useful range.
Dans une variante préférée, le résonateur est agencé et la plage utile du couple moteur sélectionnée de manière que l'aimant soit entièrement superposé au motif combiné pour tout couple moteur de cette plage utile.In a preferred variant, the resonator is arranged and the useful range of the selected motor torque so that the magnet is entirely superimposed on the combined pattern for any motor torque of this useful range.
D'autres caractéristiques particulières de l'invention seront exposées ci-après dans la description détaillée de l'invention.Other particular features of the invention will be described below in the detailed description of the invention.
L'invention sera décrite ci-après à l'aide de dessins annexés, donnés à titre d'exemples nullement limitatifs, dans lesquels :
- La
Figure 1 représente schématiquement en plan deux structures magnétiques intervenant dans un premier mode de réalisation d'un échappement magnétique selon l'invention et leur superposition pour former ce premier mode de réalisation; - La
Figure 2 représente schématiquement en plan deux structures magnétiques intervenant dans un deuxième mode de réalisation d'un échappement magnétique selon l'invention et leur superposition pour former ce deuxième mode de réalisation; - La
Figures 3A et 3B montrent, en coupe partielle, un échappement magnétique selon l'invention respectivement dans une première position d'un aimant de cet échappement magnétique et dans une deuxième position de cet aimant; - La
Figure 3C montre un graphe schématique de la variation d'énergie potentielle magnétique de l'échappement magnétique représenté auxFigures 3A et 3B ; - La
Figure 4 représente schématiquement un premier mode de réalisation d'un premier dispositif régulateur selon l'invention; - La
Figure 5 représente schématiquement, en coupe, un deuxième mode de réalisation du premier dispositif régulateur selon l'invention; - La
Figure 6 montre deux coupes partielles et un graphe, respectivement similaires à ceux desFigures 3A, 3B et 3C , relatives à un troisième mode de réalisation d'un échappement magnétique selon l'invention; - La
Figure 7 montre deux coupes partielles et un graphe, respectivement similaires à ceux desFigures 3A, 3B et 3C , relatives à un quatrième mode de réalisation d'un échappement magnétique selon l'invention; - La
Figure 8 représente schématiquement, en coupe, un troisième mode de réalisation du premier dispositif régulateur selon l'invention; - La
Figure 9 représente schématiquement une variante de réalisation du dispositif régulateur de laFigure 8 ; - La
Figure 10 représente schématiquement, en plan, un premier mode de réalisation d'un deuxième dispositif régulateur selon l'invention; - La
Figure 11 représente schématiquement une variante de réalisation du dispositif régulateur de laFigure 10 ; et - La
Figure 12 représente schématiquement, en coupe, un deuxième mode de réalisation du deuxième dispositif régulateur selon l'invention.
- The
Figure 1 schematically shows in plan two magnetic structures involved in a first embodiment of a magnetic escapement according to the invention and their superposition to form this first embodiment; - The
Figure 2 schematically shows in plan two magnetic structures involved in a second embodiment of a magnetic escapement according to the invention and their superposition to form this second embodiment; - The
Figures 3A and 3B show, in partial section, a magnetic escapement according to the invention respectively in a first position of a magnet of this magnetic escapement and in a second position of this magnet; - The
Figure 3C shows a schematic graph of the variation of magnetic potential energy of the magnetic escapement represented inFigures 3A and 3B ; - The
Figure 4 schematically represents a first embodiment of a first regulator device according to the invention; - The
Figure 5 schematically shows, in section, a second embodiment of the first regulator device according to the invention; - The
Figure 6 shows two partial sections and a graph, respectively similar to those ofFigures 3A, 3B and 3C , relating to a third embodiment of a magnetic escapement according to the invention; - The
Figure 7 shows two partial sections and a graph, respectively similar to those ofFigures 3A, 3B and 3C , relating to a fourth embodiment of a magnetic escapement according to the invention; - The
Figure 8 schematically represents, in section, a third embodiment of the first regulator device according to the invention; - The
Figure 9 schematically represents a variant embodiment of the regulating device of theFigure 8 ; - The
Figure 10 schematically represents, in plan, a first embodiment of a second regulator device according to the invention; - The
Figure 11 schematically represents a variant embodiment of the regulating device of theFigure 10 ; and - The
Figure 12 schematically represents, in section, a second embodiment of the second regulator device according to the invention.
A la
La différence en valeur absolue |ΔN| entre les nombres N1 et N2 est ici égale un (|AN| = 1). De manière générale, il est prévu que la différence en valeur absolue |ΔN| entre les nombres N1 et N2 est inférieure ou égale à N/2, soit |ΔN| <= N/2, N étant le nombre inférieur des nombres N1 et N2. Dans une variante préférée, il est prévu que le nombre |ΔN| soit inférieur ou égal à N/3, soit |ΔN| <= N/3.The difference in absolute value | ΔN | between the numbers N1 and N2 is here equal to (| AN | = 1). In general, it is expected that the difference in absolute value | ΔN | between the numbers N1 and N2 is less than or equal to N / 2, ie | ΔN | <= N / 2, where N is the lower number of the numbers N1 and N2. In a preferred variant, the number | ΔN | is less than or equal to N / 3 or | ΔN | <= N / 3.
Les premier et deuxième réseaux circulaires sont montés de manière parallèle à relativement faible distance l'un de l'autre. Ils sont agencés de manière que, lorsque le mouvement horloger fonctionne, le premier réseau a une rotation relativement au deuxième réseau, autour de l'axe de rotation 6 de la roue d'échappement, à une première fréquence angulaire F1. Dans l'exemple donné, la deuxième structure magnétique est fixe relativement au mouvement horloger de sorte que la fréquence F1 est celle du premier réseau circulaire dans le mouvement horloger (définissant un référentiel fixe). Les premier et deuxième réseaux circulaires génèrent dans une surface annulaire (ayant donc une plage radiale non nulle), en projection dans un plan géométrique parallèle à ces réseaux circulaires, un motif combiné 14 définissant une première zone 15 avec une forte proportion de surface magnétique et une deuxième zone 16 avec une moindre proportion de surface magnétique. Ce qui est remarquable, c'est que le motif combiné 14 tourne avec une deuxième fréquence angulaire F2 qui est en valeur absolue N1 fois supérieure à la première fréquence angulaire F1 pour le cas particulier de l'exemple donné où le nombre |ΔN| = 1. Ainsi, avec un premier réseau circulaire 3 ayant vingt lignes, comme représenté à la
Par analogie à l'effet Moiré optique, la génération du motif combiné avec des zones ayant différentes proportions de surface magnétique est considérée ici comme un effet Moiré magnétique. De manière générale, en prévoyant une différence de lignes |ΔN| entre les deux réseaux, |ΔN| étant la différence en valeur absolue entre le nombre N1 et le nombre N2, on obtient en alternance un nombre |ΔN| de première(s) zone(s) avec une première proportion de surface magnétique et un nombre |ΔN| de deuxième(s) zone(s) avec une deuxième proportion de surface magnétique qui est inférieure à la première proportion. Le motif combiné tourne avec une deuxième fréquence angulaire F2 égale à la première fréquence angulaire F1 multipliée par le nombre N1 et divisée par la différence ΔN = N1-N2, soit F2 = F1·N1 /ΔN. Dans le cadre de la présente invention, la première structure magnétique forme une roue d'échappement. On notera que le nombre ΔN peut être positif ou négatif. Dans le cas où il est positif, le motif combiné tourne dans le même sens que la roue d'échappement. Dans le cas où le nombre ΔN est négatif, le motif combiné tourne dans le sens inverse à celui de la roue d'échappement ; ce qui correspond mathématiquement à une fréquence négative. L'échappement magnétique 12 comprend encore au moins un aimant fixé au résonateur et couplé aux premier et deuxième réseaux circulaires, comme ceci sera exposé par la suite.By analogy with the Moire optical effect, the generation of the pattern combined with areas having different proportions of magnetic surface is considered here as a magnetic Moire effect. In general, by providing a difference of lines | ΔN | between the two networks, | ΔN | being the difference in absolute value between the number N1 and the number N2, we obtain alternately a number | ΔN | of first zone (s) with a first proportion of magnetic surface and a number | ΔN | second zone (s) with a second proportion of magnetic area that is smaller than the first proportion. The combined pattern rotates with a second angular frequency F2 equal to the first angular frequency F1 multiplied by the number N1 and divided by the difference ΔN = N1-N2, ie F2 = F1 · N1 / ΔN. In the context of the present invention, the first magnetic structure forms an escape wheel. It will be noted that the number ΔN can be positive or negative. In the case where it is positive, the combined pattern rotates in the same direction as the escape wheel. In the case where the number ΔN is negative, the combined pattern rotates in the opposite direction to that of the escape wheel; which corresponds mathematically to a negative frequency. The
A la
Etant donné le déphasage entre des réseaux circulaires 19 et 20, les deux motifs combinés 24 et 26 ont également un déphasage de 180°. De manière générale, l'alternance de zones avec une forte proportion de surface magnétique et de zones avec une moindre proportion de surface magnétique définit un motif combiné périodique ayant une période angulaire P3 dont la valeur est égale à 360° divisé par la valeur absolue de la différence |ΔN| entre les nombres N1 et N2, soit P3 = 360° / |ΔN|. Dans l'exemple de la
Comme montré aux
A la
Concernant le rapport de réduction entre la fréquence d'oscillation Fosc du diapason et la fréquence de rotation F1 de la roue d'échappement portant la première structure magnétique (dans le cas où la deuxième structure magnétique ne tourne pas), on a d'une part la fréquence de rotation F2 des motifs combinés 25 et 26 qui est égale F1·N1 / ΔN (ΔN étant la différence entre N1 et N2). D'autre part, la fréquence d'oscillation Fosc est égale à F2·AN. On obtient une relation Fosc = F2·ΔN = F1·N1 quel que soit ΔN. Ainsi, le rapport de réduction est indépendant du nombre ΔN. On peut tirer avantage de ce fait en sélectionnant ΔN petit, notamment |ΔN| = 2 ou 4. L'invention est remarquable car on peut avoir des motifs combinés périodiques avec une relativement grande période pour un grand rapport de réduction, et permettre ainsi d'utiliser des aimants de grandes dimensions ayant une relativement grande zone d'interaction magnétique avec les structures magnétiques définissant les motifs combinés, sans nécessiter une diminution du rapport de réduction. Pour que les aimants du diapason oscillent de manière symétrique par rapport à l'axe de rotation 6, le nombre ΔN est un nombre pair. A la
A la
Les deux aimants sont fixés aux extrémités d'un organe amagnétique ayant une forme en U. Le résonateur est représenté avec un ressort schématique. La partie résonnante 68 peut par exemple être fixée à une extrémité libre d'un diapason. Le fonctionnement est similaire à celui du premier mode de réalisation. Chaque aimant est couplé magnétiquement aux réseaux circulaires de la manière exposée précédemment. Ils sont alignés axialement de manière à être tous deux à la perpendiculaire du cercle de position zéro. La structure 18 est fixe et supportée par un disque 66 formé d'un matériau amagnétique. Un évidement latéral est prévu dans ce disque pour permettre à la partie résonnante 68 de passer sous la structure 18. On remarquera que dans la variante montrée, les structures magnétiques 2 et 18 présentent chacune une partie annulaire intérieure et une partie annulaire extérieure qui relient les lignes des réseaux circulaires 3, 19 et 20.The two magnets are attached to the ends of a non-magnetic member having a U shape. The resonator is shown with a schematic spring. The
Dans la variante représentée, les deux aimants ont une aimantation axiale de sens opposé. Cette configuration est avantageuse car elle permet d'amplifier l'interaction magnétique comme on peut le voir à la
Dans une variante représentée à la
Un troisième mode de réalisation d'un dispositif régulateur 80 du premier type est représenté à la
La structure magnétique 18A comprend une partie annulaire centrale qui est continue. Entre les deuxième et troisième réseaux est prévue une partie intermédiaire annulaire qui est continue, de préférence en matériau magnétique. De plus, on a également prévu une partie périphérique annulaire continue. Les trois parties annulaires continues permettent d'avoir une structure magnétique 18A en une seule pièce avec les lignes magnétiques des deux réseaux fixées aux deux extrémités. Pour que les zones annulaires continues ne perturbent pas le fonctionnement de l'échappement magnétique, on prévoit que les réseaux circulaires s'étendent sur une longueur radiale sensiblement supérieure à celle des aimants oscillant. Cette structure 18A est prise dans un moyeu amagnétique 86 monté sur l'arbre de la roue d'échappement. Les deux structures fixes 2A et 82 comprennent respectivement deux parties périphériques annulaires continues qui sont reliées par une entretoise amagnétique 84. Ce mode de réalisation résout un problème restant dans le deuxième mode de réalisation. En effet, les deux structures magnétiques superposées sont attirées l'une vers l'autre à cause du flux magnétique des aimants. Grâce à la superposition des trois structures magnétiques, ces forces d'attraction s'annulent en majeure partie si la structure magnétique intermédiaire est située sensiblement au milieu des deux autres. On remarquera que diverses variantes sont envisageables. Dans une première variante, les deux réseaux déphasés concentriques sont prévus dans les première et troisième structures magnétiques alors que la deuxième structure magnétique forme un seul réseau circulaire étendu. Dans une autre variante, il est prévu que les première et troisième structures extérieures sont montées sur l'arbre de la roue d'échappement et sont solidaires en rotation, alors que la deuxième structure intermédiaire est montée fixement dans le mouvement horloger.The
On décrira rapidement une variante de réalisation à l'aide de la
Un premier mode de réalisation d'un deuxième dispositif régulateur de la marche d'un mouvement horloger sera décrit à l'aide de la
Ensuite, la région annulaire des première et deuxième structures magnétiques, définissant le motif combiné 14 avec une première zone 15 ayant une forte proportion de surface magnétique et une deuxième zone 16 ayant une moindre proportion de surface magnétique, est couplée magnétiquement à l'aimant 104 de manière que cet aimant est entraîné en rotation par un couple d'interaction magnétique résultant du motif combiné tournant à la fréquence angulaire ω. Le motif combiné tourne lorsqu'un couple moteur, dans une plage utile du couple moteur, est fourni à la roue d'échappement, la fréquence angulaire du motif combiné ω étant asservie à la fréquence angulaire de résonance Fres dans cette plage utile du couple, cette dernière étant sélectionnée de manière que le couple d'interaction magnétique susmentionné reste inférieur à un couple d'interaction magnétique maximal et que ledit cercle décrit par ledit centre du l'aimant a un rayon compris dans la plage radiale du motif combiné 14 pour tout couple moteur de cette plage utile. L'interaction magnétique dans ce résonateur a pour effet de synchroniser la fréquence angulaire ω de la roue d'échappement à la fréquence de résonance Fres du résonateur. Le motif combiné 14 engendre une variation de l'énergie potentielle Epot dans le résonateur, en fonction de la position angulaire relative de l'aimant et de ce motif combiné, entre une énergie minimale lorsque l'aimant est au-dessus de première zone 15 et une énergie maximale lorsqu'il est au-dessus de la deuxième zone 16. Le gradient angulaire de cette énergie potentielle engendre une force d'entraînement tangentielle sur l'aimant. Pour éviter une perte de la synchronisation, on veillera à ce que le couple de freinage exercé par l'aimant sur la roue d'échappement reste inférieur au couple maximal d'interaction magnétique dépendant de la valeur maximale du gradient de l'énergie potentielle Epot.Then, the annular region of the first and second magnetic structures, defining the combined
Dans une variante préférée, le résonateur est agencé et la plage utile du couple moteur sélectionnée de manière que l'aimant 104 soit entièrement superposé au motif combiné 14 pour tout couple moteur de cette plage utile.In a preferred variant, the resonator is arranged and the useful range of the selected motor torque so that the
La
La
Finalement, de manière générale, l'invention concerne un mouvement horloger mécanique comprenant un dispositif régulateur, un rouage compteur cadencé par ce dispositif régulateur et un dispositif moteur entraînant le rouage compteur et entretenant un mode de résonance du dispositif régulateur. Ce mouvement horloger est caractérisé par le fait qu'il comprend un échappement magnétique selon l'invention ou un dispositif régulateur selon l'invention.Finally, in general, the invention relates to a mechanical clockwork comprising a regulating device, a counter wheel clocked by this regulating device and a motor device driving the counter wheel and maintaining a resonance mode of the regulating device. This watch movement is characterized in that it comprises a magnetic escapement according to the invention or a regulating device according to the invention.
Claims (22)
Priority Applications (24)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP14185638.5A EP2998801A1 (en) | 2014-09-19 | 2014-09-19 | Magnetic clock escapement and device for controlling the operation of a clock movement |
EP14186297.9A EP2911015B1 (en) | 2013-12-23 | 2014-09-25 | Natural escapement |
CH01450/14A CH709061A2 (en) | 2013-12-23 | 2014-09-25 | Mechanism of natural exhaust. |
EP14186652.5A EP2891929B1 (en) | 2013-12-23 | 2014-09-26 | Magnetic or electrostatic resonator |
PCT/EP2014/076930 WO2015096973A2 (en) | 2013-12-23 | 2014-12-08 | Escapement mechanism having a contactless timepiece cylinder |
US15/106,433 US9746829B2 (en) | 2013-12-23 | 2014-12-08 | Contactless cylinder escapement mechanism for timepieces |
RU2016130266A RU2666451C2 (en) | 2013-12-23 | 2014-12-08 | No-touch cylindrical trigger mechanism for watches |
JP2016542197A JP6236164B2 (en) | 2013-12-23 | 2014-12-08 | Non-contact cylinder escapement mechanism for timepiece |
CN201480070342.9A CN105849650B (en) | 2013-12-23 | 2014-12-08 | Contactless cylinder escapement for clock and watch |
CN201480070592.2A CN105849653B (en) | 2013-12-23 | 2014-12-09 | magnetic and/or electrostatic resonator |
JP2016533632A JP6130603B2 (en) | 2013-12-23 | 2014-12-09 | Natural escapement |
RU2016130276A RU2660530C2 (en) | 2013-12-23 | 2014-12-09 | Natural trigger mechanism |
PCT/EP2014/077039 WO2015096979A2 (en) | 2013-12-23 | 2014-12-09 | Natural escapement |
PCT/EP2014/076991 WO2015096976A2 (en) | 2013-12-23 | 2014-12-09 | Magnetic or electrostatic resonator |
RU2016130281A RU2624713C1 (en) | 2013-12-23 | 2014-12-09 | Magnetic or electrostatic resonator |
US15/028,599 US9927773B2 (en) | 2013-12-23 | 2014-12-09 | Natural escapement |
JP2016541686A JP6166847B2 (en) | 2013-12-23 | 2014-12-09 | Magnetic and / or electrostatic resonator |
US15/102,389 US9651920B2 (en) | 2013-12-23 | 2014-12-09 | Magnetic and/or electrostatic resonator |
CN201480070616.4A CN105849652B (en) | 2013-12-23 | 2014-12-09 | Natural style escapement |
EP15766420.2A EP3191899B1 (en) | 2014-09-09 | 2015-09-04 | Magnetic clock escapement and device for controlling the operation of a clock movement |
PCT/EP2015/070237 WO2016037938A1 (en) | 2014-09-09 | 2015-09-04 | Magnetic timepiece escapement and regulator device for the operation of a timepiece movement |
US15/308,902 US9891591B2 (en) | 2014-09-09 | 2015-09-04 | Magnetic clock escapement and device for regulating the operation of a clock movement |
JP2016563129A JP6220465B2 (en) | 2014-09-09 | 2015-09-04 | Devices that regulate the operation of the watch magnetic escape and watch movement |
CN201580023592.1A CN106462109B (en) | 2014-09-09 | 2015-09-04 | The device of magnetic timepiece escapement and the operation for adjusting timekeeper machine core |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP14185638.5A EP2998801A1 (en) | 2014-09-19 | 2014-09-19 | Magnetic clock escapement and device for controlling the operation of a clock movement |
Publications (1)
Publication Number | Publication Date |
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EP2998801A1 true EP2998801A1 (en) | 2016-03-23 |
Family
ID=51564596
Family Applications (2)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP14185638.5A Withdrawn EP2998801A1 (en) | 2013-12-23 | 2014-09-19 | Magnetic clock escapement and device for controlling the operation of a clock movement |
EP15766420.2A Active EP3191899B1 (en) | 2014-09-09 | 2015-09-04 | Magnetic clock escapement and device for controlling the operation of a clock movement |
Family Applications After (1)
Application Number | Title | Priority Date | Filing Date |
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EP15766420.2A Active EP3191899B1 (en) | 2014-09-09 | 2015-09-04 | Magnetic clock escapement and device for controlling the operation of a clock movement |
Country Status (5)
Country | Link |
---|---|
US (1) | US9891591B2 (en) |
EP (2) | EP2998801A1 (en) |
JP (1) | JP6220465B2 (en) |
CN (1) | CN106462109B (en) |
WO (1) | WO2016037938A1 (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP3361325A1 (en) * | 2017-02-14 | 2018-08-15 | Ecole Polytechnique Fédérale de Lausanne (EPFL) EPFL-TTO | Two degree of freedom mechanical oscillator |
EP3373080A1 (en) * | 2017-03-06 | 2018-09-12 | Montres Breguet S.A. | Clock movement provided with a device for positioning a mobile member in a plurality of discrete positions |
Families Citing this family (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP3182225B1 (en) * | 2015-12-18 | 2018-08-08 | Montres Breguet S.A. | Timepiece sequencer mecanism with recess wheel having a reduced mechanical friction |
EP3316046B1 (en) * | 2016-10-25 | 2019-07-31 | The Swatch Group Research and Development Ltd | Optimised clock movement |
EP3602207B1 (en) * | 2017-03-28 | 2020-12-30 | The Swatch Group Research and Development Ltd | Timepiece comprising a mechanical movement of which the operation is improved by a correction device |
EP3602206B1 (en) * | 2017-03-28 | 2020-12-30 | The Swatch Group Research and Development Ltd | Mechanical timepiece comprising a movement of which the operation is improved by a correction device |
CH714345A2 (en) * | 2017-11-16 | 2019-05-31 | Eta Sa Mft Horlogere Suisse | Device for selecting a combination of patterns |
EP3579058B1 (en) * | 2018-06-07 | 2021-09-15 | Montres Breguet S.A. | Timepiece comprising a tourbillon |
EP3767397B1 (en) * | 2019-07-19 | 2022-04-20 | The Swatch Group Research and Development Ltd | Clock movement comprising a rotary element provided with a magnetic structure having a periodic configuration |
EP3839647B1 (en) * | 2019-12-19 | 2023-10-11 | The Swatch Group Research and Development Ltd | Winding assembly with moire effect for automatic movement of a timepiece |
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FR2132162A1 (en) * | 1971-03-30 | 1972-11-17 | Horstmann Magnetics Ltd | |
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DE602005023633D1 (en) * | 2004-10-26 | 2010-10-28 | Tag Heuer Sa | WATCH CLOCK REGULATOR AND MECHANICAL MOVEMENT WITH SUCH A REGULATOR |
EP2463732B1 (en) * | 2010-12-10 | 2016-03-30 | Montres Breguet SA | Chiming mechanism of a watch or a music box |
EP2466401B1 (en) * | 2010-12-15 | 2013-08-14 | Asgalium Unitec SA | Magnetic resonator for mechanical timepiece |
AT510941B1 (en) * | 2011-09-05 | 2012-07-15 | Seh Ltd | MAGNETIC DEVICE |
EP2887157B1 (en) * | 2013-12-23 | 2018-02-07 | The Swatch Group Research and Development Ltd. | Optimised escapement |
WO2015097172A2 (en) * | 2013-12-23 | 2015-07-02 | The Swatch Group Research And Development Ltd | Device intended to control the angular speed of a train in a timepiece movement and including a magnetic escapement |
JP6087895B2 (en) * | 2013-12-23 | 2017-03-01 | ザ・スウォッチ・グループ・リサーチ・アンド・ディベロップメント・リミテッド | Angular velocity adjustment device for wheelset in watch movement including magnetic escapement mechanism |
-
2014
- 2014-09-19 EP EP14185638.5A patent/EP2998801A1/en not_active Withdrawn
-
2015
- 2015-09-04 EP EP15766420.2A patent/EP3191899B1/en active Active
- 2015-09-04 JP JP2016563129A patent/JP6220465B2/en active Active
- 2015-09-04 CN CN201580023592.1A patent/CN106462109B/en active Active
- 2015-09-04 WO PCT/EP2015/070237 patent/WO2016037938A1/en active Application Filing
- 2015-09-04 US US15/308,902 patent/US9891591B2/en active Active
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FR1113932A (en) | 1953-11-07 | 1956-04-05 | Horstmann Magnetics Ltd | Mechanism comprising magnetically coupled oscillating and rotating systems |
US2946183A (en) | 1955-06-14 | 1960-07-26 | Horstmann Magnetics Ltd | Self-starting magnetic escapement mechanisms |
FR2132162A1 (en) * | 1971-03-30 | 1972-11-17 | Horstmann Magnetics Ltd | |
JPS5263453U (en) | 1975-11-04 | 1977-05-11 |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP3361325A1 (en) * | 2017-02-14 | 2018-08-15 | Ecole Polytechnique Fédérale de Lausanne (EPFL) EPFL-TTO | Two degree of freedom mechanical oscillator |
EP3373080A1 (en) * | 2017-03-06 | 2018-09-12 | Montres Breguet S.A. | Clock movement provided with a device for positioning a mobile member in a plurality of discrete positions |
US10488823B2 (en) | 2017-03-06 | 2019-11-26 | Montres Breguet S.A. | Timepiece movement provided with a device for positioning a movable element in a plurality of discrete positions |
Also Published As
Publication number | Publication date |
---|---|
JP2017518484A (en) | 2017-07-06 |
EP3191899A1 (en) | 2017-07-19 |
EP3191899B1 (en) | 2018-12-12 |
CN106462109B (en) | 2019-04-19 |
JP6220465B2 (en) | 2017-10-25 |
CN106462109A (en) | 2017-02-22 |
US9891591B2 (en) | 2018-02-13 |
US20170068222A1 (en) | 2017-03-09 |
WO2016037938A1 (en) | 2016-03-17 |
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