• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The invention relates to a shaft (1) of a rotating mobile (10) clockwork, said shaft (1) being made in one or more parts (2) aligned, characterized in that said shaft (1) is magnetically inhomogeneous, so to limit the magnetic interaction on it when it is within a movement incorporated into a timepiece.
    公开号:CH707790B1
    申请号:CH00664/13
    申请日:2013-03-26
    公开日:2017-12-15
    发明作者:Zaugg Alain；Sarchi Davide；Karapatis Nakis
    申请人:Montres Breguet Sa；
    IPC主号:
    专利说明:

    Description
    FIELD OF THE INVENTION [0001] The invention relates to a clock-pivoting mobile shaft, said shaft being made in one or more aligned parts.
    The invention also relates to a rotating watchmaker with such a shaft.
    The invention also relates to a clockwork mechanism comprising such a shaft and / or such a mobile, including an escape mechanism.
    The invention also relates to a watch movement comprising such a shaft and / or such a mobile and / or such a mechanism.
    The invention also relates to a timepiece, including a watch, including such a shaft and / or such a mobile, and / or such a mechanism, and / or such a movement.
    The invention relates to the field of watch mechanisms, in particular the field of regulating members, in particular for mechanical watches.
    BACKGROUND OF THE INVENTION [0007] The regulating organ of a mechanical watch is constituted by a harmonic oscillator, the balance spring, the oscillation frequency of which depends mainly on the inertia of the balance and the rigidity elastic of the spiral.
    The oscillations of the spiral balance, otherwise damped, are maintained by the pulses provided by an exhaust generally composed of one or two pivoting mobile. In the case of the Swiss lever escapement, these pivoting mobiles are the anchor and the escape wheel. The march of the watch is determined by the frequency of the sprung balance and by the disturbance generated by the impulse of the escapement, which generally slows down the natural oscillation of the sprung balance and thus causes a delay in running.
    The march of the watch is disturbed by all the phenomena that can alter the natural frequency of the sprung balance and / or the time dependence of the impulse provided by the exhaust.
    In particular, following the transient exposure of a mechanical watch to a magnetic field, operating defects (related to the residual effect of the field) are generally observed. The origin of these defects is the permanent magnetization of the fixed ferromagnetic components of the movement or the cladding and the permanent or transient magnetization of the moving magnetic components forming part of the regulating organ (sprung balance) and / or the exhaust .
    After exposure to the field, the magnetized components (balance, spiral, exhaust) magnetically or magnetically permeable are subjected to a magnetostatic torque and / or magnetostatic forces. In principle, these interactions modify the apparent rigidity of the sprung balance, the dynamics of the escape mobiles and the friction. These modifications produce a fault that can range from a few tens to a few hundred seconds a day.
    The interaction of the watch movement with the external field, during the exhibition, can also lead to stopping the movement. In principle, the arrest in the field and the residual run-out are not correlated, because the arrest in field depends on the transient magnetization, sub-field, of the components (and therefore of the permeability and the saturation field). components), while the residual run fault depends on the residual magnetization (and therefore, mainly, the coercive field of the components) which can be low even in the presence of a significant magnetic permeability.
    After the introduction of the spirals made of very weakly paramagnetic materials (for example, silicon), the spiral is no longer responsible for the running defect of the watches. The magnetic disturbances still observable for magnetization fields below 1.5 Tesla are therefore due to the magnetization of the balance shaft and to the magnetization of the escapement wheels.
    The anchor body and the escape wheel can be made of very weakly paramagnetic materials, without their mechanical performance being affected. On the contrary, the shafts of the mobiles require very good mechanical performances (good tribology, low fatigue) to allow an optimal and constant pivoting in the time, and it is therefore preferable to manufacture them in hardened steel (typically carbon steel type 20AP or the like). However, such steels are materials sensitive to magnetic fields because they have a high saturation field combined with a high coercive field. The balance, anchor and escape wheel shafts are currently the most critical components in the face of the magnetic disturbances of the watch. SUMMARY OF THE INVENTION The invention proposes to limit the magnetic interaction on the shafts of a watch mechanism, in a movement incorporated into a timepiece, in particular a watch.
    For this purpose, the invention relates to a mobile rotating watchmaking shaft, said shaft being made in one or more aligned parts, characterized in that said shaft is magnetically inhomogeneous, according to claim 1.
    According to a particular characteristic, said shaft is magnetically inhomogeneous with a variation of the intrinsic magnetic properties of said shaft radially with respect to said pivot axis.
    According to a particular characteristic, said shaft is magnetically inhomogeneous with a variation of the intrinsic magnetic properties of said shaft radially with symmetry of revolution with respect to said pivot axis.
    The invention also relates to a rotating watchmaker with such a shaft.
    The invention also relates to a clockwork mechanism comprising such a shaft and / or such a mobile, including an escape mechanism.
    The invention also relates to a watch movement comprising such a shaft and / or such a mobile and / or such a mechanism.
    The invention also relates to a timepiece, including a watch, including such a shaft and / or such a mobile, and / or such a mechanism, and / or such a movement.
    BRIEF DESCRIPTION OF THE DRAWINGS [0023] Other features and advantages of the invention will appear on reading the detailed description which follows, with reference to the appended drawings, in which: FIG. 1 represents, in the form of a three-dimensional diagram, a first variant of the mobile shaft according to the invention, comprising a central zone of intrinsic magnetic properties different from those of the peripheral zone which surrounds this central zone centered on the axis of pivoting of the mobile; fig. 2 shows, schematically, in sectional view and with a gray coloration all the more intense as the remnant field is high, a homogeneous tree of the prior art after exposure to a magnetic field; fig. 3 represents, schematically and similar to FIG. 2, the shaft of FIG. 1, with a remnant field concentrated on its central and axial zone; fig. 4 illustrates, in the form of a graph, the comparison of the magnetic couples exerted on these two models of balance shafts of FIG. 2 and FIG. 3, the graph G2 corresponding to the homogeneous tree of FIG. 2 is shown in broken lines, and the graph G3 corresponding to the inhomogeneous tree according to the invention is shown in solid lines. On the abscissa is the angle in degrees, and in ordinate the torque exerted on the balance, in mN.mm; fig. 5 illustrates, in the form of a graph, the comparison of the magnetic couples exerted on these two models of balance shafts of FIG. 2 and FIG. 3, compared to the return torque of the hairspring and the torque applied to the balance by the anchor. The graph G2 corresponding to the homogeneous tree of FIG. 2 is shown in broken lines, and the graph G3 corresponding to the inhomogeneous tree according to the invention is shown in solid lines. The interrupted mixed line G4 represents the return torque exerted by the spiral. The maintenance torque, applied to the balance by the anchor, is represented in the form of a horizontal G5 dotted line. fig. 6 shows, similarly to FIG. 1, a second variant of a mobile shaft according to the invention, comprising a median part of intrinsic magnetic properties different from those of two end zones which surround this median part, on either side in the direction of the pivot axis of the mobile; fig. 7 represents, in a similar manner to FIG. 3, the distribution of the remanent field on the shaft of FIG. 6, with a remnant field focused on its two axial end zones; fig. 8 represents, in the form of a block diagram, a timepiece, comprising a movement comprising a mechanism comprising a mobile equipped with a shaft according to the invention.
    DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS [0024] The aim of the invention is to limit the magnetic interaction on the shafts 1 of the mobiles 10 of a watch mechanism 20, within a movement 30 incorporated in a timepiece 40. in particular a watch, and, in particular for the maintenance (exhaust) and control (sprung-balance) components which constitute a preferred application, on the shafts of the balance wheel, the anchor and the escape wheel.
    The invention is described here for this application only to maintenance (exhaust) and regulating (balance spring). The skilled person, watchmaker, will extrapolate it to other mechanisms.
    The invention can allow watches with spiral, anchor body and nonmagnetic escape wheel to withstand, without stopping, magnetic fields of the order of a Tesla, and without the performance mechanical (chronometric and mobile aging) are affected.
    The invention reduces the residual effect of watches with hairspring, anchor body and non-magnetic escape wheel less than one second per day.
    The geometry of the shaft of a pendulum is generally more complex than the geometry of the anchor rod, and that of the shaft of the escape wheel.
    Two alternative variants, non-limiting, exploiting the same principle are illustrated for the case of a balance shaft. Their generalization in the case of the anchor rod and the escape wheel, or other mobiles, will be obvious to the skilled person.
    By convention, is called in the present description "axis" a virtual geometric element such as a pivot axis, and "tree" a real mechanical element, made in one or more parts. For example, a pair of pivots 2A and 2B aligned and reported on either side of a median portion 6 of a mobile 10, to guide it in pivoting is also called "tree".
    In the remainder of the description, "magnetically permeable" materials are defined as materials having a relative permeability of between 10 and 10,000, such as steels, which have a relative permeability close to 100 for rocker shafts. for example, or close to 4000 for steels commonly used in electrical circuits, or other alloys whose relative permeability reaches values of 8000 to 10000.
    The term "magnetic" materials, for example in the case of polar masses, materials capable of being magnetized so as to have a residual field of between 0.1 and 1.5 Tesla, such as for example the "Neodymium Iran" Boron "with a magnetic energy density Em of 512 kJ / m3 and giving a residual field of 0.5 to 1.3 Tesla. A lower residual field level, towards the lower part of the range can be used when combining, in a magnetization couple, such a magnetic material with a magnetically permeable antagonist component of high permeability, closer to 10000, in the range of 100 to 10,000.
    "Ferromagnetic materials" will be referred to as materials whose characteristics are: saturation field Bs
    > 0 at temperature T = 23 ° C, coercive field Hc> 0 at temperature T = 23 ° C, maximum magnetic permeability pR> 2 at temperature T = 23 ° C, Curie temperature Te> 60 ° C.
    More particularly, it will be described as "weakly ferromagnetic" those whose characteristics are saturation field Bs <0.5 T at temperature T = 23 ° C, coercive field Hc <1 kA / m at temperature T = 23 ° C, maximum magnetic permeability pR <10 at temperature T = 23 ° C, Curie temperature Te> 60 ° C.
    More particularly, those whose characteristics are: saturation field Bs> 1 T at temperature T = 23 ° C., coercive field Hc> 3 kA / m at temperature T = 23 °, will be described as "strongly ferromagnetic". C, maximum magnetic permeability pR> 50 at temperature T = 23 ° C, Curie temperature Te> 60 ° C
    "Paramagnetic" materials will be called materials of relative magnetic permeability between 1.0001 and 100, for example for spacers interposed between a magnetic material and a magnetically permeable antagonistic component, or alternatively between two magnetic materials, for example a spacer between a component and a polar mass. For example, weakly paramagnetic materials are: aluminum, gold, brass or the like (magnetic permeability less than 2).
    Diamagnetic materials will be called materials of relative magnetic permeability less than 1 (negative magnetic susceptibility, less than or equal to 10 -5), such as graphite or graphene.
    Finally, we call "soft magnetic" materials, not to say non-magnetic, especially for shielding, materials having high permeability but high saturation, because we do not want them to be permanently magnetized: they must drive the field as best as possible, so as to reduce the field to their outside. Such components can then also protect a magnetic system from external fields. These materials are preferably chosen to have a relative magnetic permeability of between 50 and 200, and with a saturation field greater than 500 A / m.
    Materials qualified as "nonmagnetic" have relative magnetic permeability very slightly greater than 1, and less than 1.0001, as typically silicon, diamond, palladium and the like. These materials can generally be obtained by MEMS technologies or by the "LIGA" process.
    Thus, the shaft 1 of rotating mobile watch 10 is made of one or more parts 2A 2B, which are then aligned on a pivot axis D.
    According to the invention, this tree 1 is magnetically inhomogeneous.
    In particular, this shaft 1 is magnetically inhomogeneous, with a variation of the intrinsic magnetic properties of this shaft 1, either in the axial direction of the pivot axis D of the shaft 1, or radially with a symmetry of revolution relative to this pivot axis D, both in the axial direction of the pivot axis D and radially with a symmetry of revolution relative to this pivot axis D.
    The shaft 1 is magnetically inhomogeneous with a variation of the intrinsic magnetic properties radially with respect to the pivot axis D.
    In a preferred embodiment, this variation of the intrinsic magnetic properties of the shaft 1 is made radially with a symmetry of revolution with respect to the pivot axis D.
    By "inhomogeneous shaft in the radial direction" is meant here that the magnetic properties of the shaft vary in the radial direction, from the center of the shaft to the periphery (while the tree may be, or not , magnetically homogeneous in the axial direction).
    Only the material located in the heart of the tree, in an area hereinafter called central zone 3, that is to say in the vicinity of the pivot axis D, has a high saturation field (Bs > 1 T), a magnetic permeability Pr maximum greater than 50, and a coercive field Hc greater than 3 kA / m (all these properties are typical of 20AP steel used preferably for pivoting shafts because of good mechanical performance). Naturally, if other materials are used, these threshold values must be adapted by routine tests.
    While the material at the periphery of the shaft, in a zone hereinafter referred to as the peripheral zone 4, is either weakly paramagnetic or ferromagnetic with a small saturation field (Bs <0.5 T), a low maximum magnetic permeability pR <10, and a weak coercive field.
    A diagram of this solution is shown in FIG. 1, which is a three-dimensional diagram of the first variant. The balance shaft 1 is composed of a highly ferromagnetic (grayed) central zone 3 and a paramagnetic or weakly ferromagnetic peripheral zone (in white).
    In this case, the two regions (strongly ferromagnetic in central zone 3, and weakly paramagnetic in peripheral zone 4) are precisely separated by a steep interface zone 7: the interface between the two regions 3 and 4 can however have a finite width, in correspondence of a regular gradient of the magnetic properties, without the results being affected. The strongly ferromagnetic region in the central zone 3 in the heart of the shaft 1 is preferably contained in a cylinder with a radius less than 100 micrometers (and centered on the pivot axis D) to achieve the desired performance.
    In practice, the magnetic inhomogeneity described here can be obtained by combining two different materials (by brazing, soldering or depositing a material on the other), or else, in the case where an alloy is used (by carbon steel), by heat treatment or under electric or magnetic field of all or part of the finished component.
    FIG. 2 shows the prior art, in the form of a conventional arm shaft 1 homogeneous, AP steel. This figure illustrates the remanent field, after magnetization at 0.2 T. During this magnetization, this shaft is subjected to an external field of 0.2 T oriented in the direction orthogonal to the pivot axis, the shaft is magnetized in all its volume, its remnant field being between 0.3 T and 0.6 T, as shown in FIG. 2 which shows: - in dark gray areas with a remnant field of 0.6T; - in medium shading areas with a remnant field of the order of 0.2 to 0.4T; - and in very light gray or white areas with a remnant field less than 0.2T. The magnetization is greater in correspondence of the maximum radius of the tree.
    FIG. 3 shows the remanent field of a radially inhomogeneous balance shaft 1 according to the first variant of the invention. This tree 1 has the same geometry as that of FIG. 2, but only the heart, in central zone 3, is made of steel AP, while its periphery, in peripheral zone 4, is weakly paramagnetic. The shaft is subjected to an external field of 0.2 T oriented in the direction orthogonal to the pivot axis D. The remanent field is about 0.4 T and concentrated in the core in central zone 3.
    When the timepiece is subjected to the action of an external magnetic field, during the oscillation of the sprung balance, the magnetized shaft of the balance is subjected to a magnetic torque which tends to orient it in the direction of the external field. The moment of this pair may be high enough to stop the movement of this balance-spring.
    Due to the highly differentiated magnetization, the homogeneous tree of FIG. 2 is subjected to a magnetic torque, whose moment is more than 10 times that which is applied to the inhomogeneous shaft of FIG. 3. Indeed, the shaft 1 according to the invention comprises a field of remanent field on a very small radius, while in the prior art areas of high remanent field are precisely in the areas of larger radius.
    Stopping the movement takes place if the torque acting on the shaft is greater than the restoring torque exerted by the hairspring for angles lower than the lifting angle, and the maintenance torque applied by the anchor. to the pendulum. These two pairs, obtained for typical parameters, are compared with the magnetic torque acting on the homogeneous shaft and on the inhomogeneous shaft, in the graph of FIG. 5.
    FIG. 4 illustrates the comparison of the magnetic couples exerted on these two models of balance shafts: the graph G2 corresponding to the homogeneous tree of FIG. 2 is shown in broken line, and the graph G3 corresponding to the inhomogeneous shaft 1 according to the invention (first variant of Figure 3, or second variant of Figure 7 exposed below) is shown in solid lines. On the abscissa is the angle in degrees, and in ordinate the torque exerted on the balance, in mN.mm. In both cases, the torque varies sinusoidally with the rotation angle of the balance spring (here zero is fixed arbitrarily).
    The homogeneous tree of FIG. 2 is subjected to a magnetic torque significantly greater than the pair of the spiral and the maintenance torque. In this case, the sprung balance will be stopped for a field smaller than 0.2 T.
    The inhomogeneous shaft 1 according to the first variant of the invention is subjected to a torque less than the torque exerted by the hairspring in the lifting angle (<30 °) and the maintenance torque. In this case, the sprung balance will not be stopped under a field of 0.2 T.
    FIG. 5 illustrates the comparison of the magnetic couples on a balance shaft, homogeneous according to the prior art, and inhomogeneous according to the invention (first variant, or second variant exposed later), imposed by an external field of 0.2 T, compared the return moment of the hairspring and the torque applied to the balance by the anchor. In the same way as fig. 4, fig. 5 illustrates the comparison, on a low angular amplitude, of the magnetic couples exerted on these two models of balance shafts: the graph G2 corresponding to the homogeneous tree is shown in broken lines, and the graph G3 corresponding to the inhomogeneous tree is shown in solid line. The interrupted mixed line G4 represents the return torque exerted by the spiral. The maintenance torque, applied to the balance by the anchor, is represented in the form of a horizontal G5 dotted line.
    As a result of the magnetization of the watch, the shaft 1 of the balance 10 is immersed in the magnetic field created by the fixed ferromagnetic components of the movement 30, and / or the timepiece 40, of which he belongs. The shaft 1 is then subjected to a torque similar to that shown in FIG. 4, but of weaker moment. This disturbance torque is responsible for the residual running error. A movement equipped with an inhomogeneous shaft 1 according to the first variant of the invention is therefore affected by a walking defect which is between 3 and 10 times less than that which affects a movement equipped with a traditional homogeneous tree.
    The second variant of the invention relates to a shaft which is inhomogeneous in the axial direction parallel to the axis of pivoting of the shaft.
    The inhomogeneity of the magnetic properties is this time carried out in the axial direction. The ends 2 of the shaft 1, constituted by the pivots 2A and 2B, which must have optimum mechanical properties, are generally made of magnetic materials, while the middle part 6 of the shaft 1 is made of a weakly paramagnetic material.
    The length (in the axial direction) accumulated of the magnetic parts of the shaft 1 is advantageously less than one third of the total length of the shaft 1.
    The difference in length between the magnetic parts is advantageously maintained less than 10%.
    This second variant is shown schematically in FIG. 6, on which preferably only the pivots 2A and 2B are made of ferromagnetic material.
    The shaft 1 of FIG. 6 comprises, in the direction of the pivot axis D, a median portion 6 surrounded on both sides by two end zones 8. And only these end zones 8, preferably made of pivoted steel, have a high saturation field of Bs greater than 1 T, a maximum magnetic permeability pR greater than 50, and a coercive field Hc greater than 3 kA / m. While the material in the middle part 6 is either weakly paramagnetic or ferromagnetic with a low saturation field Bs less than 0.5 T, a low maximum magnetic permeability p R less than 10, and a low coercive field.
    As for the first variant, the remanent field is lower (and more localized) than in the case of a homogeneous tree according to FIG. 2, as shown in FIG. 7.
    This fig. 7 represents the remanent field, after magnetization at 0.2 T, of an inhomogeneous balance shaft 1 according to the second variant of the invention. The pivots are made of 20 AP steel. The middle part 6 is weakly paramagnetic.
    The torque acting on the shaft 1 in this case is equivalent to that obtained for the first variant (FIG 4 and FIG 5).
    In practice, as for the first variant, the desired magnetic inhomogeneity can be obtained by combining two different materials (by brazing, welding or depositing a material on the other) or, in the case where an alloy is used (for example, carbon steel), by heat treatment or under electric or magnetic field of all or part of the finished component.
    It is still possible to mix the first and the second variant, the shaft 1 is then magnetically inhomogeneous with a variation of its intrinsic magnetic properties both in the axial direction of the pivot axis D and radially. relative to this pivot axis D.
    In one or the other of these variants, the invention is easy to implement and inexpensive, since, in practice, a simple two-material embodiment makes it possible to obtain the desired result. For example, an embodiment according to the first variant with a balance rod constituting the peripheral zone 4 which is produced, according to the desired inertia, of aluminum, gold, brass or the like, while the central zone 3 is made in the form of a 20AP steel bar or similar: a low inertia beam is obtained with a light alloy serge, in particular of aluminum, easy to machine and to drill through, and a core of drawn or drawn steel, or cleavage, with a diameter less than 100 micrometers. Similarly, a rocker according to the second variant and with very low inertia has a part
    权利要求:
    Claims (14)
    [1]
    median 6 machined aluminum alloy and having at its axial ends two housing for driving pivots 2A and 2B pivoted steel. The invention also relates to a pivoting mobile watch 10 having a shaft 1 according to the invention. The invention also relates to a clockwork mechanism comprising such a shaft 1 and / or such a mobile 10, in particular an escape mechanism. The invention also relates to a clockwork movement comprising such a shaft 1 and / or such a mobile 10 and / or such a mechanism 20. [0075] The invention also relates to a timepiece 40, in particular a watch, including such a shaft 1 and / or such a mobile 10, and / or such a mechanism 20, and / or such a movement 30. [0076] The invention, in one or the other of its variants, presents important advantages: - increased subfield field arrest strength for watches with hairspring, anchor body and non-magnetic escape wheel; this means that a watch should be subjected to magnetic fields much higher than those which the user may encounter in his normal life, before risking a disturbance likely to lead to the cessation of movement; - reduced residual effect for watches with spiral, anchor body and non-magnetic escape wheel; - Mechanical performance identical to the watches of the current state of the art, since the tribological contact surfaces continue to be made in materials validated for these applications. claims
    1. Shaft (1) of a rotating swivel (10) of horology, said shaft (1) being made in one or more aligned parts (2), characterized in that said shaft (1) is magnetically inhomogeneous, with a variation of intrinsic magnetic properties of said shaft (1), either in the axial direction of the pivot axis (D) of said shaft (1), or radially with respect to said pivot axis (D), or both in the direction axial axis of pivoting (D) of said shaft (1) and radially with a symmetry of revolution relative to said pivot axis (D).
    [2]
    2. Shaft (1) according to claim 1, characterized in that said shaft (1) is magnetically inhomogeneous with a variation of intrinsic magnetic properties of said shaft (1) radially with respect to said pivot axis (D).
    [3]
    3. Shaft (1) according to claim 2, characterized in that said shaft (1) is magnetically inhomogeneous with a variation of the intrinsic magnetic properties of said shaft (1) radially with a symmetry of revolution with respect to said pivot axis ( D).
    [4]
    4. Shaft (1) according to claim 1, characterized in that said shaft (1) is magnetically inhomogeneous with a variation of the intrinsic magnetic properties of said shaft (1) in the axial direction of the pivot axis (D) of said shaft (1).
    [5]
    5. Shaft (1) according to claim 1, characterized in that said shaft (1) is magnetically inhomogeneous with a variation of the intrinsic magnetic properties of said shaft (1) both in the axial direction of the pivot axis (D). ) of said shaft (1) and radially with respect to said pivot axis (D).
    [6]
    6. Shaft (1) according to claim 2 or 3, characterized in that only the material located at the heart of said shaft (1), in a central zone (3) in the vicinity of the pivot axis (D) of said shaft ( 1) made of steel, has a high saturation field of value (Bs) greater than 1 T, a maximum magnetic permeability pR greater than 50, and a coercive field (Hc) greater than 3kA / m, while the material in a zone peripheral (4) of said shaft (1), is either weakly paramagnetic with a magnetic permeability less than 2 or ferromagnetic with a low saturation field (Bs) of less than 0.5 T, a low maximum magnetic permeability (pR) less than 10, and a weak coercive field, lower than 1kA / m.
    [7]
    7. Shaft (1) according to claim 6, characterized in that the highly ferromagnetic region of said central zone (3) in the heart of said shaft (1) is contained in a cylinder with a radius less than 100 micrometers and centered on said axis of pivoting (D) of said shaft (1).
    [8]
    8. Shaft (1) according to claim 4, characterized in that it comprises, in the direction of said pivot axis (D), a central portion (6) surrounded on either side by two end zones ( 8), and that only said end zones (8), made of steel, have a high saturation field of value (Bs) greater than 1 T, a maximum magnetic permeability pR greater than 50, and a coercive field (Hc ) greater than 3kA / m, while the material in said middle part (6) of said shaft (1) is either weakly paramagnetic with a magnetic permeability of less than 2 or ferromagnetic with a low saturation field (Bs) of value less than 0.5 T, a low maximum magnetic permeability (pR) less than 10, and a low coercive field, lower than 1kA / m.
    [9]
    9. Shaft (1) according to one of claims 1 to 8, characterized in that its magnetic inhomogeneity is obtained, or by combination of two different materials by brazing, welding or depositing a material on the other, or by using an alloy subjected to a heat treatment or the action of an electric or magnetic field on all or part of said shaft (1) or said mobile (10).
    [10]
    10. Swivel mobile (10) clockwork comprising a said shaft (1) according to one of claims 1 to 9.
    [11]
    11. Mechanism (20) clockwork comprising a shaft (1) according to one of claims 1 to 9 and / or a said mobile (10) according to claim 10, characterized in that it is an escape mechanism .
    [12]
    12. Watch movement (30) comprising a shaft (1) according to one of claims 1 to 9 and / or a said mobile (10) according to claim 10 and / or a said mechanism (20) according to claim 11 .
    [13]
    13. Timepiece (40) comprising a shaft (1) according to one of claims 1 to 9 and / or a said mobile (10) according to claim 10, and / or a said mechanism (20) according to claim 11, and / or a said movement (30) according to claim 12.
    [14]
    14. Watch comprising a shaft (1) according to one of claims 1 to 9 and / or a mobile (10) according to claim 10, and / or a mechanism (20) according to claim 11, and / or a movement ( 30) according to claim 12.
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    法律状态:
    优先权:
    申请号 | 申请日 | 专利标题
    EP13161124.6A|EP2784601B1|2013-03-26|2013-03-26|Arbor of a pivotable clock mobile|
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