EP2299336A2 - Flat hairspring for a clock balance wheel and balance wheel -hairspring assembly - Google Patents

Flat hairspring for a clock balance wheel and balance wheel -hairspring assembly Download PDF

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Publication number
EP2299336A2
EP2299336A2 EP10405172A EP10405172A EP2299336A2 EP 2299336 A2 EP2299336 A2 EP 2299336A2 EP 10405172 A EP10405172 A EP 10405172A EP 10405172 A EP10405172 A EP 10405172A EP 2299336 A2 EP2299336 A2 EP 2299336A2
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EP
European Patent Office
Prior art keywords
spiral
hairspring
blade
outer end
rigidity
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Granted
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EP10405172A
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German (de)
French (fr)
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EP2299336B1 (en
EP2299336A3 (en
Inventor
Jérôme Daout
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Rolex SA
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Rolex SA
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    • G—PHYSICS
    • G04—HOROLOGY
    • G04B—MECHANICALLY-DRIVEN CLOCKS OR WATCHES; MECHANICAL PARTS OF CLOCKS OR WATCHES IN GENERAL; TIME PIECES USING THE POSITION OF THE SUN, MOON OR STARS
    • G04B17/00—Mechanisms for stabilising frequency
    • G04B17/04—Oscillators acting by spring tension
    • G04B17/06—Oscillators with hairsprings, e.g. balance
    • G04B17/066—Manufacture of the spiral spring
    • G—PHYSICS
    • G04—HOROLOGY
    • G04B—MECHANICALLY-DRIVEN CLOCKS OR WATCHES; MECHANICAL PARTS OF CLOCKS OR WATCHES IN GENERAL; TIME PIECES USING THE POSITION OF THE SUN, MOON OR STARS
    • G04B17/00—Mechanisms for stabilising frequency
    • G04B17/20—Compensation of mechanisms for stabilising frequency

Definitions

  • the present invention relates to a flat spring balance spring comprising a wound blade, shaped to ensure a substantially concentric development of the hairspring and a virtually zero force exerted on the pivots and the embedding point, during the rotation less than 360 ° of its inner end relative to its outer end in both directions, from its rest position.
  • This invention also relates to a sprung balance assembly.
  • the non-concentric development of a hairspring associated with a watch pendulum during the oscillation of the balance-hairspring assembly causes a decentering of the center of gravity of the hairspring, which is translated, according to the positions occupied by the watch, by a delay or advance effect, that is to say by a decrease or an increase in the natural frequency of the balance spring system.
  • This decentering of the center of gravity of the spiral also causes a lateral pressure of the pivots of the balance on the bearings.
  • the Breguet hairspring involves the formation of a terminal curve in a plane parallel to that of the flat hairspring, which requires the formation of two inverted bends to form an inclined connecting segment between the hairspring and the parallel terminal curve.
  • a Breguet hairspring can be made of different ferromagnetic or paramagnetic alloys, especially for self-compensating hairsprings.
  • a fragile material such as monocrystalline silicon or polycrystalline silicon. Indeed, it is not possible to form the two inverted bends intended to allow the formation of the terminal Breguet curve because of the brittle nature of such a fragile material, and it is thus necessary to resort to a technique to form solidarity structures on several levels.
  • the CH 327 796 proposes to modify the cross-section of the spiral blade to give it superior rigidity, over an arc of up to 180 °, either in the center or the outside. This modification is carried out by folding, adding material (galvanic deposition, welding), or pickling (rolling, etching).
  • the US 3,550,928 recommends to stiffen the terminal curve of the spiral by a non-rectangular section obtained by plastic deformation of a part of the last turn.
  • the EP 1 473 604 relates to a planar hairspring having on its outer turn a stiffened portion arranged to make the deformations of the turns substantially concentric.
  • the BE 526689 proposes to vary the section of the spiral blade on one or more parts of its length, or to modify the profile or to add to one or more parts of the blade any body intended to modify the flexibility of these parts. No further details are given as to these variations or modifications.
  • the EP 1431844 refers to a spiral whose section varies from one to the other of its ends. However, little precision is provided as to the mode of variation of the spiral section. The only information is that given in Figure 11 and in the part of the description associated with it.
  • the definition given on page 4, lines 55-57 speaks of "variable parallelepipedal section", "in this case a rectangular section E towards the center evolving to a square section E 'on the outside”. This definition, which is the only information on the type of variation, suggests a monotonic variation. Indeed, the two sections EE 'between which the section evolves seem to imply a continuous and monotonous variation of the section.
  • All the aforementioned spirals aim to improve the isochronism of the balance-balance oscillator for the different positions of the watch.
  • the simulation study of these different spirals shows that it is difficult to reduce significantly below a maximum difference between the different positions of 4 s / d for typical operating amplitudes, ie amplitudes greater than 200 °, while keeping sufficient security to prevent the turns from touching during the contraction and expansion of the hairspring , or following a shock suffered by the wristwatch.
  • the average slope of the gait curves as a function of the amplitude of the balance-balance oscillator should be as small as possible, ideally slightly negative so as to compensate for the isochronism defects generated by a flight exhaust. Swiss anchor. It will also be more difficult to obtain good performance for small spirals, for example below 2.5mm distance between the axis of rotation and the outer end.
  • the object of the present invention is to provide a solution that makes it possible to be closer to these objectives than the spirals of the state of the art.
  • this invention firstly relates to a flat spring balance spring comprising a wound blade and shaped to ensure a substantially concentric development of the hairspring and a virtually zero force exerted on the pivots and the mounting point during rotation less than 360 ° from its inner end relative to its external end in both directions from its rest position, as defined by claim 1.
  • Another subject of the invention is a balance spring and spiral assembly. according to claim 12.
  • substantially concentric development and “almost zero force” are intended to encompass spirals capable of achieving at least performance equal to that of Breguet curve spirals, its aim being to achieve at least such performance, but with a flat hairspring.
  • the hairspring according to the invention is equally applicable to ductile material spirals to fragile materials such as silicon.
  • the performance of the balance-balance oscillator in particular the difference between the positions, can vary substantially with the torque developed by the spiral and with its bulk, that is to say the distance between the point of contact. internal attachment of the spiral to the ferrule and the external attachment point.
  • the number of turns also has a significant influence.
  • the spirals given by way of examples in the figures all have the same nominal torque (same inertia of the balanced balance spring to obtain an oscillation frequency of 4 Hz), and the same size.
  • the spirals are made of Si.
  • the distance to the axis of rotation is 0.6mm for the inner end and 2.1mm for the outer end.
  • the height of the turns is 150 ⁇ m.
  • the section can be modified, and more particularly the thickness of the blade as it is known that the rigidity of a blade varies with the thickness of the cube. It would also be possible to use a localized heat treatment or to act on the shape of the blade for example, without changing the section, for example by changing the orientation of the cross section of the spiral relative to a center of rotation provided for this spiral. This could be achieved by twisting or waving the spiral blade, or combining these stiffening modes with the section change.
  • the spiral object of the invention may be of a fragile material, in particular a crystalline material such as silicon. It is easy to realize such a spiral having a variable section by using the manufacturing process described in EP 0732635 B1 which uses the etching techniques with etching which are perfectly mastered in the field of electronics for the work of silicon wafers in particular.
  • This document precisely describes a manufacturing method that can be used in particular for spirals. Although this document does not mention the possibility of making a hairspring with non-constant section, it is obvious that the masking technique used lends itself perfectly to obtaining such a result. In addition, this method allows for the spiral integrally with its ferrule and its embedding means.
  • the processes mentioned are particularly suitable for producing spirals whose section of the blade is not constant to obtain a non-monotonically variable rigidity in order to maintain the center of gravity of the spiral substantially on a center of rotation provided for this hairspring.
  • Other methods could also be used, for example heat treatment or machining. laser, to subsequently modify the rigidity of the hairspring in a non-monotonic manner in order to obtain the desired result.
  • a treatment or machining could also be associated with a spiral comprising at least two segments of different sections.
  • thermocompensation of the spirals is carried out by known means.
  • a layer of material on the surface of the turns that compensates for the first thermal coefficient of the Young's modulus of the base material.
  • a suitable material for the layer is SiO 2 .
  • the spiral object of the invention illustrated by the figure 1 has an extra thickness that decreases from its inner end over 360 ° and a thickening that grows gradually over 360 ° (more than five turns in the case of the figure 1 ) before the outer end and up to this outer end.
  • This non monotonic thickness variation is illustrated by the diagram of the figure 2 . Between the outer end of the hairspring and its minimum thickness, the thickness decreases by a factor of 2.6. Between its inner end and its minimum thickness, the thickness decreases by 35%.
  • the pitch of the spiral object of the invention can also vary from non-monotonic way, as illustrated by the diagram of the figure 3 .
  • This diagram shows a decrease in pitch from the inner end of the hairspring, followed by a slight increase and then a local maximum, two turns of the outer end in this example.
  • This local maximum (a sudden increase followed by a sudden decrease) is intended to prevent the turns from touching during oscillations of the sprung balance assembly.
  • this variation of pitch does not require a substantial increase in the spacing of the end turn, which makes it possible to have a hairspring with a high number of turns, in this example more than 14 turns for a hairspring of 2.1 mm radius.
  • the maximum pitch of the hairspring is not located at its outer end, but is located on the outer third of the hairspring (between 1 and 3 turns of this end, and more precisely to 1.75 turns in this example) and that the value of the pitch has a local maximum on the outer third of the hairspring (between 1 and 3 turns of the outer end).
  • the second embodiment illustrated by the figure 5 comprises two end-stage curves with progressive rigidity, one internal and the other external, whose function is to achieve a smooth transition between the ends and the central turns.
  • the areas where the pitch is larger are useful so that the turns do not touch in operation, that is to say in contraction and expansion.
  • the intermediate part between these two zones can very well be satisfied by a small step approximately constant (variation of the pitch of about 4% in the example of the figure 7 ).
  • the middle part moves globally as a whole towards the contraction center, or outwardly expanding. She needs space on both sides.
  • the square located towards the center may be smaller than the one located outside, and is not necessarily necessary as shown in the diagram of the figure 3 .
  • the thickness diagram of the figure 6 is similar to that of the form of execution of Figures 1-4 , that is to say, extra thicknesses at both ends of the spiral thus constituting terminal curves extending over more than 360 °. Between the outer end of the hairspring and its minimum thickness, the thickness decreases by a factor of 4.4. Between its inner end and its minimum thickness, the thickness decreases by 48%.
  • the thickness of the inner and / or outer coil could stop growing, or even decrease slightly, on the last internal and / or external turn, without noticeably changing the properties of the oscillator.
  • the step diagram of the figure 7 has non-monotonic and progressive variations, with a local maximum located in the first third of the hairspring (at 2 turns of the inner end) in addition to that located in the outer third (about 3 turns from the outer end) .
  • the 250 ° amplitude difference of the balance-balance oscillator is 1.99 s / d and is comparable to the example of the figure 4 , with an average of the difference between 200 and 300 ° of amplitude lower than for the spiral of the figure 1 .
  • Two other forms of execution are still represented.
  • One is illustrated by the figure 9 with zones with turns spaced apart in the inner third and the outer third, with a continuous variation of the pitch, with no local maximum of the pitch neither inside nor outside.
  • the thickness variation curve has a similar appearance to that of the first embodiment illustrated by the figure 2 , with a decrease from the inner end to the inner third (first four rounds), a portion of constant thickness, then an increase on the outer third to the outer end (last two rounds).
  • the pitch it varies non-monotonically, gradually decreasing from the inner end to the middle of the length of the hairspring and then increasing progressively to the outer end of the hairspring, with no maximum local.
  • the chronometric performances are better than for the spirals with constant pitch and thickness, but slightly less good than for the first two embodiments (maximum gap between positions of 2.67 s / d at 250 °).
  • the other embodiment is illustrated by the figure 10 and has a much larger central area and no variation of pitch in the inner part of the hairspring.
  • the thickness variation curve looks similar to that of the first embodiment illustrated by the figure 2 , with a decrease from the inner end to the inner third (first four rounds), a portion of constant thickness, then an increase on the outer third to the outer end (last three rounds).
  • the spiral pitch illustrated by the figure 10 is constant on the inner first third of the length of the hairspring, then it undergoes a sudden increase followed by a decrease, ie a local maximum, at 3 and a half turns of the outer end. The pitch then increases again to the outer end.
  • the chronometric performances are comparable to those of the first two forms of execution (maximum difference between positions of 2.08 s / d at 250 °).

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Manufacturing & Machinery (AREA)
  • Springs (AREA)
  • Stringed Musical Instruments (AREA)
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Abstract

The hairspring has a wound strip shaped to ensure a concentric development of hairspring and a zero force on pivots and on a fixing point during rotation of less than 360 degrees of inner end relative to outer end in directions from a rest position, where the hairspring is formed from fragile and crystalline materials and silicon. Stiffness of the strip gradually decreases beyond 360 degrees from a point located between the lower end and a turn and from another point located between the outer end and a last turn, where the lowest stiffness is situated in a median part of the strip.

Description

La présente invention se rapporte à un spiral plat pour balancier d'horlogerie comportant une lame enroulée, conformée pour assurer un développement sensiblement concentrique du spiral et une force quasi nulle exercée sur les pivots et le point d'encastrement, lors de la rotation inférieure à 360° de son extrémité interne par rapport à son extrémité externe dans les deux sens, à partir de sa position de repos. Cette invention se rapporte également à un ensemble balancier-spiral.The present invention relates to a flat spring balance spring comprising a wound blade, shaped to ensure a substantially concentric development of the hairspring and a virtually zero force exerted on the pivots and the embedding point, during the rotation less than 360 ° of its inner end relative to its outer end in both directions, from its rest position. This invention also relates to a sprung balance assembly.

Le développement non concentrique d'un spiral associé à un balancier d'horlogerie lors de l'oscillation de l'ensemble balancier-spiral provoque un décentrage du centre de gravité du spiral, qui se traduit, suivant les positions occupées par la montre, par un effet de retard ou d'avance, c'est-à-dire par une diminution ou une augmentation de la fréquence propre du système balancier-spiral. Ce décentrage du centre de gravité du spiral provoque également une pression latérale des pivots du balancier sur les paliers.The non-concentric development of a hairspring associated with a watch pendulum during the oscillation of the balance-hairspring assembly causes a decentering of the center of gravity of the hairspring, which is translated, according to the positions occupied by the watch, by a delay or advance effect, that is to say by a decrease or an increase in the natural frequency of the balance spring system. This decentering of the center of gravity of the spiral also causes a lateral pressure of the pivots of the balance on the bearings.

Ces effets de déséquilibre du spiral et de pressions latérales des pivots détruisent les conditions nécessaires à l'isochronisme des oscillations du balancier. Depuis le milieu du XVIIIe siècle, les horlogers s'étaient rendu compte que le développement non concentrique du spiral a une mauvaise influence sur l'isochronisme et en particulier que la pression latérale provoquée par un spiral décentré sur les pivots du balancier occasionne des perturbations de la marche et une usure des pivots. Ces mêmes horlogers ont alors préconisé de former une ou deux courbes terminales tout d'abord sur des spiraux cylindriques puis sur un spiral de type Archimède contenu dans un plan, c'est le spiral Breguet du nom de son inventeur.These effects of imbalance of the balance and lateral pressures of the pivots destroy the conditions necessary for the isochronism of the pendulum oscillations. Since the mid-eighteenth century, watchmakers had realized that the non-concentric development of the spring has a bad influence on the isochronism and in particular the lateral pressure caused by an off-spring of the pivots of the balance causes disruptions walking and wear of the pivots. These same watchmakers then recommended forming one or two terminal curves first of all on cylindrical spirals then on a spiral of the type Archimedes contained in a plan is the spiral Breguet name of its inventor.

Ces courbes étaient faites de manière plus ou moins empiriques et corrigées en fonction des résultats de la marche de l'oscillateur, avant que certaines formes soient retenues en fonction de ces résultats. Ce n'est que plusieurs dizaines d'années plus tard que les conditions mathématiques de cette courbe terminale ont été étudiées par Ed. Phillips, apportant ainsi une confirmation théorique aux intuitions antérieures des horlogers, à savoir que si le centre de gravité du spiral est maintenu sensiblement sur l'axe de balancier pendant l'oscillation du système balancier-spiral, le spiral n'exerce pratiquement aucune force latérale sur les pivots du balancier et son développement reste concentrique.These curves were made in a more or less empirical way and corrected according to the results of the oscillator's progress, before certain forms were selected according to these results. It is only several decades later that the mathematical conditions of this terminal curve have been studied by Ed. Phillips, thus bringing a theoretical confirmation to the previous intuitions of watchmakers, namely that if the center of gravity of the hairspring is maintained substantially on the balance shaft during the oscillation of the balance spring system, the spiral exerts virtually no lateral force on the pivots of the balance and its development remains concentric.

Les conditions énoncées par Phillips sont les mêmes que celles définies par les horlogers qui les avaient eux-mêmes déduites de leurs observations des défauts induits par le spiral, par rapport aux règles de l'isochronisme d'un corps oscillant énoncées au XVIIe siècle par Huygens.The conditions set by Phillips are the same as those defined by the watchmakers who themselves had deduced from their observations of defects induced by the spiral, from the rules of the isochronous a tumbling body set in the seventeenth century by Huygens.

Le spiral Breguet implique la formation d'une courbe terminale dans un plan parallèle à celui du spiral plat, ce qui nécessite la formation de deux coudes inversés pour former un segment de liaison incliné entre le spiral et la courbe terminale parallèle.The Breguet hairspring involves the formation of a terminal curve in a plane parallel to that of the flat hairspring, which requires the formation of two inverted bends to form an inclined connecting segment between the hairspring and the parallel terminal curve.

Un spiral Breguet peut être réalisé en différents alliages ferromagnétiques ou paramagnétiques, notamment pour les spiraux auto-compensateurs. Par contre, il est beaucoup plus difficile à réaliser en un matériau fragile tel que le silicium mono-cristallin ou poly-cristallin. En effet, il n'est pas possible de former les deux coudes inversés destinés à permettre la formation de la courbe Breguet terminale en raison de la nature cassante d'un tel matériau fragile, et il est ainsi nécessaire de recourir à une technique permettant de former des structures solidaires sur plusieurs niveaux.A Breguet hairspring can be made of different ferromagnetic or paramagnetic alloys, especially for self-compensating hairsprings. On the other hand, it is much more difficult to produce a fragile material such as monocrystalline silicon or polycrystalline silicon. Indeed, it is not possible to form the two inverted bends intended to allow the formation of the terminal Breguet curve because of the brittle nature of such a fragile material, and it is thus necessary to resort to a technique to form solidarity structures on several levels.

On a déjà proposé d'obtenir un effet technique comparable à celui de la courbe Breguet sur un spiral plat, en variant l'épaisseur de la lame du spiral.It has already been proposed to obtain a technical effect comparable to that of the Breguet curve on a flat hairspring, by varying the thickness of the spiral blade.

Dans le US 209 642 , on a proposé d'augmenter l'épaisseur de la lame du spiral de façon graduelle ou discontinue, depuis le centre jusqu'à l'extérieur du spiral.In the US 209,642 it has been proposed to increase the thickness of the spiral blade in a gradual or discontinuous manner, from the center to the outside of the hairspring.

Le CH 327 796 propose de modifier la section droite de la lame du spiral pour lui conférer une rigidité supérieure, sur un arc de 180° au maximum, soit au centre, soit à l'extérieur. Cette modification est réalisée par pliage, par ajout de matière (déposition galvanique, soudage), ou par décapage (laminage, attaque chimique).The CH 327 796 proposes to modify the cross-section of the spiral blade to give it superior rigidity, over an arc of up to 180 °, either in the center or the outside. This modification is carried out by folding, adding material (galvanic deposition, welding), or pickling (rolling, etching).

Le US 3 550 928 préconise de rigidifier la courbe terminale du spiral par une section non rectangulaire obtenue par déformation plastique d'une partie de la dernière spire.The US 3,550,928 recommends to stiffen the terminal curve of the spiral by a non-rectangular section obtained by plastic deformation of a part of the last turn.

Le EP 1 473 604 se rapporte à un spiral plan comportant sur sa spire extérieure une portion rigidifiée agencée pour rendre les déformations des spires sensiblement concentriques.The EP 1 473 604 relates to a planar hairspring having on its outer turn a stiffened portion arranged to make the deformations of the turns substantially concentric.

Le BE 526689 propose de varier la section de la lame du spiral sur une ou plusieurs parties de sa longueur, ou de modifier le profil ou d'ajouter à une ou plusieurs parties de la lame un corps quelconque destiné à modifier la flexibilité de ces parties. Aucune autre précision n'est donnée quant à ces variations ou modifications.The BE 526689 proposes to vary the section of the spiral blade on one or more parts of its length, or to modify the profile or to add to one or more parts of the blade any body intended to modify the flexibility of these parts. No further details are given as to these variations or modifications.

On a proposé dans l'article d' Emile et Gaston Michel, Spiraux plats concentriques sans courbes, Bulletin Annuel de la Société Suisse de Chronométrie et du Laboratoire de Recherches Horlogères, Vol.IV, 1957-1963, pages 162-169, 01. 01.1963 , de former une partie de la lame en cornière. Cette « partie traitée en cornière ne fléchit pratiquement plus aux fortes amplitudes. Elle ne compte plus dans le réglage, c'est en quelque sorte un bout mort dans la spire » (fin page 164-début page 165). Il s'agit donc de neutraliser le spiral sur une partie de sa longueur.It has been proposed in the article Emile and Gaston Michel, concentric flat spirals without curves, Annual Bulletin of the Swiss Chronometry Society and the Horological Research Laboratory, Vol.IV, 1957-1963, pages 162-169, 01. 01.1963 to form a part of the angle blade. This "angle treated part hardly any longer strong amplitudes. It no longer counts in the setting, it is somehow a dead end in the turn "(end page 164-beginning page 165). It is therefore necessary to neutralize the hairspring over part of its length.

Le EP 1431844 se rapporte à un spiral dont la section varie de l'une à l'autre de ses extrémités. Toutefois, peu de précision est fournie quant au mode de variation de la section du spiral. La seule information est celle qui est donnée par la figure 11 et dans la partie de la description qui lui est associée. La définition donnée page 4, lignes 55-57 parle de « section parallélépipédique variable », « en l'occurrence une section E rectangulaire vers le centre évoluant jusqu'à une section E' carrée à l'extérieur ». Cette définition qui est la seule information quant au type de variation fait penser à une variation monotone. En effet, les deux sections E-E' entre lesquelles la section évolue semblent impliquer une variation continue et monotone de la section.The EP 1431844 refers to a spiral whose section varies from one to the other of its ends. However, little precision is provided as to the mode of variation of the spiral section. The only information is that given in Figure 11 and in the part of the description associated with it. The definition given on page 4, lines 55-57 speaks of "variable parallelepipedal section", "in this case a rectangular section E towards the center evolving to a square section E 'on the outside". This definition, which is the only information on the type of variation, suggests a monotonic variation. Indeed, the two sections EE 'between which the section evolves seem to imply a continuous and monotonous variation of the section.

La question de la variation du pas illustrée par la figure 10 du EP 1431844 est limitée à une variation du pas le long d'un axe radial F-F' qui donne au spiral une forme d'ellipse. Ce qui est montré par cette figure ressemble plus à une déformation de la spirale selon l'un des deux axes qu'à une variation du pas proprement dite, et ne permet pas d'obtenir un spiral fonctionnel, en particulier un spiral dont les spires ne se touchent pas en fonctionnement.The question of the variation of the step illustrated by figure 10 of EP 1431844 is limited to a variation of the pitch along a radial axis FF 'which gives the hairspring an elliptical shape. What is shown by this figure is more like a deformation of the spiral along one of the two axes than a variation of the pitch itself, and does not provide a functional spiral, especially a spiral whose turns do not touch each other during operation.

Enfin dans le EP 1 593 004 , la section de la lame du spiral diminue progressivement du centre du spiral vers l'extérieur.Finally in the EP 1 593 004 the section of the spiral blade gradually decreases from the center of the spiral outwards.

Tous les spiraux susmentionnés visent à améliorer l'isochronisme de l'oscillateur balancier-spiral pour les différentes positions de la montre. L'étude par simulation de ces différents spiraux montre cependant qu'il est difficile de descendre sensiblement au-dessous d'un écart maximal entre les différentes positions de 4 s/j pour des amplitudes typiques de fonctionnement, soit des amplitudes supérieures à 200°, tout en gardant des sécurités suffisantes pour éviter que les spires ne se touchent en fonctionnement lors de la contraction et de l'expansion du spiral, ou suite à un choc subi par la montre-bracelet. Par ailleurs, la pente moyenne des courbes de marche en fonction de l'amplitude de l'oscillateur balancier-spiral devrait être la plus faible possible, dans l'idéal légèrement négative de façon à compenser les défauts d'isochronisme engendrés par un échappement à ancre suisse. Il sera en outre d'autant plus difficile d'obtenir de bonnes performances pour des spiraux de petite taille, par exemple en dessous de 2.5mm de distance entre l'axe de rotation et l'extrémité externe.All the aforementioned spirals aim to improve the isochronism of the balance-balance oscillator for the different positions of the watch. The simulation study of these different spirals, however, shows that it is difficult to reduce significantly below a maximum difference between the different positions of 4 s / d for typical operating amplitudes, ie amplitudes greater than 200 °, while keeping sufficient security to prevent the turns from touching during the contraction and expansion of the hairspring , or following a shock suffered by the wristwatch. Moreover, the average slope of the gait curves as a function of the amplitude of the balance-balance oscillator should be as small as possible, ideally slightly negative so as to compensate for the isochronism defects generated by a flight exhaust. Swiss anchor. It will also be more difficult to obtain good performance for small spirals, for example below 2.5mm distance between the axis of rotation and the outer end.

Le but de la présente invention est d'apporter une solution qui permette de se rapprocher davantage de ces objectifs que les spiraux de l'état de la technique.The object of the present invention is to provide a solution that makes it possible to be closer to these objectives than the spirals of the state of the art.

A cet effet, cette invention a tout d'abord pour objet un spiral plat pour balancier d'horlogerie comportant une lame enroulée et conformée pour assurer un développement sensiblement concentrique du spiral et une force quasi nulle exercée sur les pivots et le point d'encastrement, lors de la rotation inférieure à 360° de son extrémité interne par rapport à son extrémité externe dans les deux sens à partir de sa position de repos, tel que défini par la revendication 1. Cette invention a également pour objet un ensemble balancier-spiral selon la revendication 12.For this purpose, this invention firstly relates to a flat spring balance spring comprising a wound blade and shaped to ensure a substantially concentric development of the hairspring and a virtually zero force exerted on the pivots and the mounting point during rotation less than 360 ° from its inner end relative to its external end in both directions from its rest position, as defined by claim 1. Another subject of the invention is a balance spring and spiral assembly. according to claim 12.

Les expressions "développement sensiblement concentrique" et "force quasi nulle" sont destinées à englober des spiraux susceptibles d'atteindre au moins des performances égales à celle des spiraux à courbes Breguet, son but étant d'atteindre au moins de telles performances, mais avec un spiral plat.The terms "substantially concentric development" and "almost zero force" are intended to encompass spirals capable of achieving at least performance equal to that of Breguet curve spirals, its aim being to achieve at least such performance, but with a flat hairspring.

Le spiral selon l'invention s'applique aussi bien à des spiraux en matériau ductile qu'à des matériaux fragiles tel que le silicium.The hairspring according to the invention is equally applicable to ductile material spirals to fragile materials such as silicon.

Les dessins annexés illustrent, schématiquement et à titre d'exemple, différentes formes d'exécution du spiral plat objet de la présente invention.

  • La figure 1 est une vue en plan d'un spiral plat au repos dont le centre de gravité est situé sur un centre de rotation prévu pour ce spiral;
  • la figure 2 est un diagramme de l'épaisseur E de la lame du spiral en fonction du nombre de tours N du spiral de la figure 1;
  • la figure 3 est un diagramme du pas P du spiral en fonction du nombre de tours N du spiral de la figure 1;
  • la figure 4 est un diagramme des courbes de marche théoriques d'un oscillateur balancier-spiral équipé du spiral de la figure 1, dans les différentes positions en fonction de l'amplitude de cet oscillateur (isochronisme libre);
  • la figure 5 est une vue en plan d'une deuxième forme d'exécution de spiral plat au repos dont le centre de gravité est situé sur un centre de rotation prévu pour ce spiral;
  • la figure 6 est un diagramme de l'épaisseur E de la lame du spiral en fonction du nombre de tours N du spiral de la figure 5;
  • la figure 7 est un diagramme du pas du spiral P en fonction du nombre de tours N du spiral de la figure 5;
  • la figure 8 est un diagramme des courbes de marche théoriques d'un oscillateur balancier équipé du spiral de la figure 5, dans les différentes positions en fonction de l'amplitude de cet oscillateur (isochronisme libre);
  • la figure 9 est une vue en plan d'une troisième forme d'exécution du spiral plat au repos dont le centre de gravité est situé sur un centre de rotation prévu pour ce spiral;
  • la figure 10 est une vue en plan d'une quatrième forme d'exécution du spiral plat au repos dont le centre de gravité est situé sur un centre de rotation prévu pour ce spiral.
The accompanying drawings illustrate, schematically and by way of example, various embodiments of the flat hairspring object of the present invention.
  • The figure 1 is a plan view of a flat hairspring at rest whose center of gravity is located on a center of rotation provided for this hairspring;
  • the figure 2 is a diagram of the thickness E of the spiral blade as a function of the number of turns N of the spiral of the figure 1 ;
  • the figure 3 is a diagram of the pitch of the spiral as a function of the number of turns N of the spiral of the figure 1 ;
  • the figure 4 is a diagram of the theoretical curves of a balance-balance oscillator equipped with the spiral of the figure 1 , in the different positions according to the amplitude of this oscillator (free isochronism);
  • the figure 5 is a plan view of a second embodiment of flat spiral rest whose center of gravity is located on a center of rotation provided for this spiral;
  • the figure 6 is a diagram of the thickness E of the spiral blade as a function of the number of turns N of the spiral of the figure 5 ;
  • the figure 7 is a diagram of the pitch of the spiral P as a function of the number of turns N of the spiral of the figure 5 ;
  • the figure 8 is a diagram of the theoretical curves of a pendulum oscillator equipped with the spiral of the figure 5 , in the different positions according to the amplitude of this oscillator (free isochronism);
  • the figure 9 is a plan view of a third embodiment of the flat hairspring at rest whose center of gravity is located on a center of rotation provided for this hairspring;
  • the figure 10 is a plan view of a fourth embodiment of the flat hairspring at rest whose center of gravity is located on a center of rotation provided for this hairspring.

Les performances de l'oscillateur balancier-spiral, en particulier l'écart de marche entre les positions, peuvent varier sensiblement avec le couple développé par le spiral et avec son encombrement, c'est-à-dire la distance entre le point d'attache interne du spiral à la virole et le point d'attache externe. Le nombre de tours a également une influence non-négligeable. Pour cette raison, les spiraux donnés à titre d'exemples dans les figures présentent tous le même couple nominal (même inertie du balancier apparié au spiral pour obtenir une fréquence d'oscillation de 4 Hz), et le même encombrement. Les spiraux sont réalisés en Si. La distance à l'axe de rotation est de 0.6mm pour l'extrémité interne et 2.1mm pour l'extrémité externe. La hauteur des spires est de 150µm.The performance of the balance-balance oscillator, in particular the difference between the positions, can vary substantially with the torque developed by the spiral and with its bulk, that is to say the distance between the point of contact. internal attachment of the spiral to the ferrule and the external attachment point. The number of turns also has a significant influence. For this reason, the spirals given by way of examples in the figures all have the same nominal torque (same inertia of the balanced balance spring to obtain an oscillation frequency of 4 Hz), and the same size. The spirals are made of Si. The distance to the axis of rotation is 0.6mm for the inner end and 2.1mm for the outer end. The height of the turns is 150 μm.

Pour augmenter ou diminuer sélectivement la rigidité de la lame du spiral, on peut en modifier la section, et plus particulièrement l'épaisseur de la lame vu qu'il est connu que la rigidité d'une lame varie avec l'épaisseur au cube. Il serait aussi possible d'avoir recours à un traitement thermique localisé ou encore d'agir sur la forme de la lame par exemple, sans en changer la section, par exemple en modifiant l'orientation de la section droite du spiral par rapport à un centre de rotation prévu pour ce spiral. Ceci pourrait être obtenu en la vrillant ou en formant des ondulations sur la lame du spiral, ou en combinant ces modes de rigidification avec le changement de section.To selectively increase or decrease the rigidity of the spiral blade, the section can be modified, and more particularly the thickness of the blade as it is known that the rigidity of a blade varies with the thickness of the cube. It would also be possible to use a localized heat treatment or to act on the shape of the blade for example, without changing the section, for example by changing the orientation of the cross section of the spiral relative to a center of rotation provided for this spiral. This could be achieved by twisting or waving the spiral blade, or combining these stiffening modes with the section change.

Le spiral objet de l'invention peut être en un matériau fragile, notamment un matériau cristallin tel que le silicium. On peut aisément réaliser un tel spiral présentant une section variable en ayant recours au procédé de fabrication décrit dans le EP 0732635 B1 qui utilise les techniques de masquage avec attaque chimique qui sont parfaitement maîtrisées dans le domaine de l'électronique pour le travail des plaquettes de silicium en particulier. Ce document décrit précisément un procédé de fabrication utilisable notamment pour des spiraux. Bien que ce document ne mentionne pas la possibilité de réaliser un spiral à section non constante, il est évident que la technique de masquage utilisée se prête parfaitement à l'obtention d'un tel résultat. De plus, ce procédé permet de réaliser le spiral d'un seul tenant avec sa virole et son moyen d'encastrement.The spiral object of the invention may be of a fragile material, in particular a crystalline material such as silicon. It is easy to realize such a spiral having a variable section by using the manufacturing process described in EP 0732635 B1 which uses the etching techniques with etching which are perfectly mastered in the field of electronics for the work of silicon wafers in particular. This document precisely describes a manufacturing method that can be used in particular for spirals. Although this document does not mention the possibility of making a hairspring with non-constant section, it is obvious that the masking technique used lends itself perfectly to obtaining such a result. In addition, this method allows for the spiral integrally with its ferrule and its embedding means.

D'autres techniques utilisant l'électrodéposition multi-couches associée à la technique de masquage pour fabriquer des pièces de micromécanique sont décrites dans deux articles publiés dans Elsevier Sensors and Actuators A 64 (1998) 33-39 , High-aspect-ratio, ultrathick, negative-tone near-UV photoresist and its applications for MEMS, et dans Elsevier Sensors et Actuators A 53 (1996) 364-368 , Low-cost technology for multilayer electroplated parts using laminated dry film resist. Ces techniques sont donc utilisables pour former des pièces métalliques de micromécanique présentant un rapport de forme élevé et sont donc tout à fait adaptées à la fabrication d'un spiral métallique de section variable pour produire un spiral à variation de rigidité non monotone. Grâce à ces techniques, il est donc également possible de réaliser un spiral métallique.Other techniques using multi-layer plating associated with the masking technique for making micromechanical parts are described in two articles published in Elsevier Sensors and Actuators A 64 (1998) 33-39 High-aspect-ratio, ultrathick, negative-tone near-UV photoresist and its applications for MEMS, and in Elsevier Sensors and Actuators A 53 (1996) 364-368 Low-cost technology for multilayer electroplated parts using laminated dry film resist. These techniques can therefore be used to form micromechanical metal parts having a high aspect ratio and are therefore entirely suitable for the manufacture of a metal spiral of variable section to produce a spiral with non-monotonic stiffness variation. Thanks to these techniques, it is also possible to make a metal hairspring.

Bien entendu, les procédés mentionnés sont particulièrement adaptés à la fabrication de spiraux dont la section de la lame n'est pas constante pour obtenir une rigidité variable de façon non monotone en vue de maintenir le centre de gravité du spiral sensiblement sur un centre de rotation prévu pour ce spiral. On pourrait aussi utiliser d'autres procédés, par exemple un traitement thermique ou un usinage par laser, pour modifier ultérieurement à sa fabrication proprement dite, la rigidité du spiral de façon non monotone en vue d'obtenir le résultat recherché. Un traitement ou usinage pourrait aussi être associé à un spiral comprenant au moins deux segments de sections différentes.Of course, the processes mentioned are particularly suitable for producing spirals whose section of the blade is not constant to obtain a non-monotonically variable rigidity in order to maintain the center of gravity of the spiral substantially on a center of rotation provided for this hairspring. Other methods could also be used, for example heat treatment or machining. laser, to subsequently modify the rigidity of the hairspring in a non-monotonic manner in order to obtain the desired result. A treatment or machining could also be associated with a spiral comprising at least two segments of different sections.

D'autres moyens de rigidifier sélectivement le spiral pour atteindre le but recherché peuvent être envisagés. C'est ainsi que l'on pourrait varier de manière non monotone la rigidité de ce spiral en formant une couche d'un matériau plus rigide. Cette couche pourrait notamment être réalisée par électrodéposition.Other means of selectively stiffening the hairspring to achieve the desired purpose can be envisaged. Thus one could vary non-monotonously the rigidity of this spiral forming a layer of a more rigid material. This layer could in particular be made by electrodeposition.

On pourrait encore changer la rigidité de ce spiral par dopage du silicium notamment par une technique d'implantation ionique ou par diffusion.We could still change the rigidity of this spiral by doping silicon in particular by an ion implantation technique or by diffusion.

La thermocompensation des spiraux est réalisée par des moyens connus. On peut par exemple utiliser une couche de matériau à la surface des spires qui compense le premier coefficient thermique du module d'Young du matériau de base. Dans le cas d'un spiral en Si, un matériau adéquat pour la couche est le SiO2.The thermocompensation of the spirals is carried out by known means. For example, it is possible to use a layer of material on the surface of the turns that compensates for the first thermal coefficient of the Young's modulus of the base material. In the case of a Si spiral, a suitable material for the layer is SiO 2 .

Le spiral objet de l'invention illustré par la figure 1 comporte une surépaisseur qui va en diminuant à partir de son extrémité interne sur plus de 360° et une surépaisseur qui croît progressivement sur plus de 360° (plus de cinq tours dans le cas de la figure 1) avant l'extrémité externe et jusqu'à cette extrémité externe. Cette variation d'épaisseur non monotone est illustrée par le diagramme de la figure 2. Entre l'extrémité externe du spiral et son épaisseur minimum, l'épaisseur diminue d'un facteur 2,6. Entre son extrémité interne et son épaisseur minimum, l'épaisseur diminue de 35%.The spiral object of the invention illustrated by the figure 1 has an extra thickness that decreases from its inner end over 360 ° and a thickening that grows gradually over 360 ° (more than five turns in the case of the figure 1 ) before the outer end and up to this outer end. This non monotonic thickness variation is illustrated by the diagram of the figure 2 . Between the outer end of the hairspring and its minimum thickness, the thickness decreases by a factor of 2.6. Between its inner end and its minimum thickness, the thickness decreases by 35%.

Parallèlement à cette variation d'épaisseur non monotone de la lame du spiral et donc de sa rigidité, avantageusement, le pas du spiral objet de l'invention peut aussi varier de façon non monotone, comme illustré par le diagramme de la figure 3. Ce diagramme montre une diminution du pas à partir de l'extrémité interne du spiral, suivie d'une légère augmentation puis d'un maximum local, à deux tours de l'extrémité externe dans cet exemple. Ce maximum local (une brusque augmentation suivie d'une brusque diminution) a pour but d'éviter que les spires ne se touchent lors des oscillations de l'ensemble balancier-spiral. On constatera que cette variation de pas ne nécessite pas d'augmenter sensiblement l'écartement de la spire terminale, ce qui permet d'avoir un spiral avec un nombre de tours élevé, dans cet exemple, plus de 14 tours pour un spiral de 2.1 mm de rayon. Or on sait que plus le nombre de tours est élevé, plus la pente moyenne de l'isochronisme est faible.In parallel with this variation of non-monotone thickness of the spiral blade and therefore its rigidity, advantageously, the pitch of the spiral object of the invention can also vary from non-monotonic way, as illustrated by the diagram of the figure 3 . This diagram shows a decrease in pitch from the inner end of the hairspring, followed by a slight increase and then a local maximum, two turns of the outer end in this example. This local maximum (a sudden increase followed by a sudden decrease) is intended to prevent the turns from touching during oscillations of the sprung balance assembly. It will be noted that this variation of pitch does not require a substantial increase in the spacing of the end turn, which makes it possible to have a hairspring with a high number of turns, in this example more than 14 turns for a hairspring of 2.1 mm radius. However, we know that the higher the number of revolutions, the lower the average isochronism slope.

On peut constater que dans cette forme d'exécution, le pas maximal du spiral n'est pas situé à son extrémité externe, mais se situe sur le tiers externe du spiral (entre 1 et 3 tours de cette extrémité, et plus précisément à 1.75 tours dans cet exemple) et que la valeur du pas présente un maximum local sur le tiers externe du spiral (entre 1 et 3 tours de l'extrémité externe).We can see that in this embodiment, the maximum pitch of the hairspring is not located at its outer end, but is located on the outer third of the hairspring (between 1 and 3 turns of this end, and more precisely to 1.75 turns in this example) and that the value of the pitch has a local maximum on the outer third of the hairspring (between 1 and 3 turns of the outer end).

Les simulations effectuées à l'aide de ce spiral ont montré que cette géométrie de spiral permet de diviser par 2 l'écart maximum entre les différentes positions dans lesquelles la pièce d'horlogerie est testée (CH et FH qui sont les positions horizontales, fond tourné vers le haut, respectivement cadran tourné vers le haut; 3H, 6H, 9H et 12H qui sont les positions verticales avec rotation de 90° entre les positions successives) par rapport à un spiral à pas et à épaisseur constants. L'écart à 250° d'amplitude de l'oscillateur balancier-spiral est de 1,87 s/j. Quant à la pente moyenne de l'isochronisme, le diagramme de la figure 4 montre qu'elle est très légèrement négative à cette amplitude et permet de compenser la pente très légèrement positive due à l'échappement ancre suisse standard.The simulations carried out using this spiral have shown that this spiral geometry makes it possible to divide by 2 the maximum difference between the different positions in which the timepiece is tested (CH and FH which are the horizontal positions, bottom turned upwards, respectively upwards facing dial; 3H, 6H, 9H and 12H which are the vertical positions with 90 ° rotation between the successive positions) with respect to a spiral with constant pitch and thickness. The difference at 250 ° amplitude of the balance-balance oscillator is 1.87 s / d. As for the average slope of isochronism, the diagram of the figure 4 shows that it is very slightly negative at this amplitude and compensates for the very slightly positive slope due to the standard Swiss anchor escapement.

La deuxième forme d'exécution illustrée par la figure 5 comporte deux courbes terminales à rigidité progressive, l'une interne, l'autre externe, qui ont pour fonction de réaliser une transition douce entre les extrémités et les spires centrales. Les zones où le pas est plus grand sont utiles afin que les spires ne se touchent pas en fonctionnement, c'est-à-dire en contraction et en expansion. La partie intermédiaire entre ces deux zones peut très bien se satisfaire d'un petit pas approximativement constant (variation du pas d'environ 4% dans l'exemple de la figure 7). En fait, ce qui se passe lors du développement du spiral est que la partie intermédiaire se déplace globalement dans son ensemble vers le centre en contraction, ou vers l'extérieur en expansion. Elle a donc besoin de place de part et d'autre. La place située vers le centre peut être plus petite que celle située à l'extérieur, et n'est donc pas forcément nécessaire comme le montre le diagramme de la figure 3.The second embodiment illustrated by the figure 5 comprises two end-stage curves with progressive rigidity, one internal and the other external, whose function is to achieve a smooth transition between the ends and the central turns. The areas where the pitch is larger are useful so that the turns do not touch in operation, that is to say in contraction and expansion. The intermediate part between these two zones can very well be satisfied by a small step approximately constant (variation of the pitch of about 4% in the example of the figure 7 ). In fact, what happens during the development of the hairspring is that the middle part moves globally as a whole towards the contraction center, or outwardly expanding. She needs space on both sides. The square located towards the center may be smaller than the one located outside, and is not necessarily necessary as shown in the diagram of the figure 3 .

En résumé, le diagramme d'épaisseur de la figure 6 est analogue à celui de la forme d'exécution des figures 1-4, c'est-à-dire des surépaisseurs aux deux extrémités du spiral constituant ainsi des courbes terminales s'étendant sur plus de 360°. Entre l'extrémité externe du spiral et son épaisseur minimum, l'épaisseur diminue d'un facteur 4,4. Entre son extrémité interne et son épaisseur minimum, l'épaisseur diminue de 48%.In summary, the thickness diagram of the figure 6 is similar to that of the form of execution of Figures 1-4 , that is to say, extra thicknesses at both ends of the spiral thus constituting terminal curves extending over more than 360 °. Between the outer end of the hairspring and its minimum thickness, the thickness decreases by a factor of 4.4. Between its inner end and its minimum thickness, the thickness decreases by 48%.

Selon une variante de la figure 6, l'épaisseur de la spire interne et/ou externe pourrait cesser de croître, voire décroître légèrement, sur le dernier tour nterne et/ou externe, sans changer notablement les propriétés de l'oscillateur.According to a variant of the figure 6 , the thickness of the inner and / or outer coil could stop growing, or even decrease slightly, on the last internal and / or external turn, without noticeably changing the properties of the oscillator.

Le diagramme du pas de la figure 7 comporte des variations non-monotones et progressives, avec un maximum local situé dans le premier tiers du spiral (à 2 tours de l'extrémité interne) en plus de celui situé dans le tiers externe (à environ 3 tours de l'extrémité externe).The step diagram of the figure 7 has non-monotonic and progressive variations, with a local maximum located in the first third of the hairspring (at 2 turns of the inner end) in addition to that located in the outer third (about 3 turns from the outer end) .

Comme le montre la figure 8, l'écart à 250° d'amplitude de l'oscillateur balancier-spiral est de 1,99 s/j et est comparable à l'exemple de la figure 4, avec une moyenne de l'écart entre 200 et 300° d'amplitude plus faible que pour le spiral de la figure 1.As shown in figure 8 , the 250 ° amplitude difference of the balance-balance oscillator is 1.99 s / d and is comparable to the example of the figure 4 , with an average of the difference between 200 and 300 ° of amplitude lower than for the spiral of the figure 1 .

Deux autres formes d'exécution sont encore représentées. L'une est illustrée par la figure 9 avec des zones à spires écartées dans le tiers intérieur et dans le tiers extérieur, avec une variation continue du pas, sans maximum local du pas ni à l'intérieur ni à l'extérieur. La courbe de variation d'épaisseur a une allure similaire à celle de la première forme d'exécution illustrée par la figure 2, avec une diminution depuis l'extrémité interne sur le tiers interne (quatre premiers tours), une partie d'épaisseur constante, puis une augmentation sur le tiers externe jusqu'à l'extrémité externe (deux derniers tours). Quant au pas, il varie de façon non-monotone, en diminuant de façon progressive de l'extrémité interne jusqu'au milieu de la longueur du spiral et en augmentant ensuite de façon progressive jusqu'à l'extrémité externe du spiral, sans maximum local. Les performances chronométriques sont meilleures que pour les spiraux à pas et à épaisseur constants, mais légèrement moins bonnes que pour les deux premières formes d'exécution (écart maximal entre positions de 2.67 s/j à 250°).Two other forms of execution are still represented. One is illustrated by the figure 9 with zones with turns spaced apart in the inner third and the outer third, with a continuous variation of the pitch, with no local maximum of the pitch neither inside nor outside. The thickness variation curve has a similar appearance to that of the first embodiment illustrated by the figure 2 , with a decrease from the inner end to the inner third (first four rounds), a portion of constant thickness, then an increase on the outer third to the outer end (last two rounds). As for the pitch, it varies non-monotonically, gradually decreasing from the inner end to the middle of the length of the hairspring and then increasing progressively to the outer end of the hairspring, with no maximum local. The chronometric performances are better than for the spirals with constant pitch and thickness, but slightly less good than for the first two embodiments (maximum gap between positions of 2.67 s / d at 250 °).

L'autre forme d'exécution est illustrée par la figure 10 et comporte une zone centrale beaucoup plus étendue et sans variation de pas dans la partie intérieure du spiral. La courbe de variation d'épaisseur a une allure similaire à celle de la première forme d'exécution illustrée par la figure 2, avec une diminution depuis l'extrémité interne sur le tiers interne (quatre premiers tours), une partie d'épaisseur constante, puis une augmentation sur le tiers externe jusqu'à l'extrémité externe (trois derniers tours). Le pas du spiral illustré par la figure 10 est constant sur le premier tiers interne de la longueur du spiral, ensuite il subit une brusque augmentation suivie d'une diminution, soit un maximum local, à 3 tours et demi de l'extrémité externe. Le pas augmente ensuite à nouveau jusqu'à l'extrémité externe. Les performances chronométriques sont comparables à celles des deux premières formes d'exécution (écart maximal entre positions de 2.08 s/j à 250°).The other embodiment is illustrated by the figure 10 and has a much larger central area and no variation of pitch in the inner part of the hairspring. The thickness variation curve looks similar to that of the first embodiment illustrated by the figure 2 , with a decrease from the inner end to the inner third (first four rounds), a portion of constant thickness, then an increase on the outer third to the outer end (last three rounds). The spiral pitch illustrated by the figure 10 is constant on the inner first third of the length of the hairspring, then it undergoes a sudden increase followed by a decrease, ie a local maximum, at 3 and a half turns of the outer end. The pitch then increases again to the outer end. The chronometric performances are comparable to those of the first two forms of execution (maximum difference between positions of 2.08 s / d at 250 °).

Les formes d'exécution qui précèdent sont données à titre d'exemples non limitatifs. De plus, les variations d'épaisseur et de pas devront être optimisées en fonction du cahier des charges du spiral, c'est-à-dire du couple développé et de l'encombrement (rayon à la virole et rayon au piton) afin d'obtenir des performances chronométriques optimales (écarts de marche entre positions et pente moyenne de l'isochronisme les plus faibles possibles) tout en évitant un contact entre les spires lors du fonctionnement.The foregoing embodiments are given by way of non-limiting examples. In addition, variations in thickness and pitch should be optimized according to the specification of the spiral, that is to say the developed torque and size (radius to the shell and radius to the peak) to to obtain optimal chronometric performances (differences between the positions and the average isochronism slope as low as possible) while avoiding contact between the turns during operation.

Claims (12)

Spiral plat pour balancier d'horlogerie comportant une lame enroulée, conformée pour assurer un développement sensiblement concentrique du spiral et une force quasi nulle exercée sur les pivots et le point d'encastrement, lors d'une rotation inférieure à 360° de son extrémité interne par rapport à son extrémité externe dans les deux sens à partir de sa position de repos, caractérisé en ce que la rigidité de sa lame décroit de manière progressive et sur plus de 360° à partir, d'une part d'un point situé entre son extrémité interne et sa deuxième spire, d'autre part d'un point situé entre son extrémité externe et son avant dernière spire, la rigidité la plus faible se situant dans la partie médiane de ladite lame.Flat spiral for clockwork comprising a wound blade, shaped to ensure a substantially concentric development of the hairspring and a virtually zero force exerted on the pivots and the embedding point, during a rotation less than 360 ° of its inner end relative to its outer end in both directions from its rest position, characterized in that the rigidity of its blade decreases progressively and over more than 360 ° from, on the one hand, a point situated between its inner end and second turn, on the other hand a point between its outer end and its penultimate turn, the lowest rigidity being in the middle portion of said blade. Spiral selon la revendication 1, dans lequel la rigidité de sa lame décroit de manière progressive et sur plus de 360°, à partir de chacune de ses deux extrémités.Spiral according to claim 1, wherein the rigidity of its blade decreases progressively and more than 360 °, from each of its two ends. Spiral selon l'une des revendications précédentes, dans lequel le pas du spiral varie de façon non monotone en diminuant entre son extrémité externe et le tiers externe compté en nombre de tours.Spiral according to one of the preceding claims, wherein the pitch of the spiral varies non-monotonously decreasing between its outer end and the outer third counted in revolutions. Spiral selon l'une des revendications précédentes, dans lequel le pas du spiral varie de façon non monotone en diminuant entre son extrémité interne et le tiers interne compté en nombre de tours.Spiral according to one of the preceding claims, wherein the pitch of the spiral varies non-monotonously decreasing between its inner end and the inner third counted in revolutions. Spiral selon l'une des revendications précédentes, dans lequel le pas du spiral subit une brusque augmentation suivie d'une brusque diminution, le tout s'étendant sur plus de 360° et se situant à au moins un tour d'au moins une de ses extrémités.Spiral according to one of the preceding claims, in which the pitch of the hairspring undergoes a sudden increase followed by a sudden decrease, all extending over more than 360 ° and being at least one turn of at least one of its ends. Spiral selon l'une des revendications précédentes, dans lequel les rigidités respectives différentes correspondent à des sections respectives différentes de la lame du spiral.Spiral according to one of the preceding claims, wherein the respective respective rigidities correspond to respective different sections of the spiral blade. Spiral selon l'une des revendications précédentes, dans lequel la rigidité diminue d'au moins un facteur 8 entre un point situé entre son extrémité externe et son avant dernière spire, et la valeur minimum.Spiral according to one of the preceding claims, wherein the rigidity decreases by at least a factor 8 between a point between its outer end and its penultimate turn, and the minimum value. Spiral selon l'une des revendications précédentes, dans lequel la rigidité diminue d'au moins 50% entre son extrémité interne et la valeur minimum.Spiral according to one of the preceding claims, wherein the rigidity decreases by at least 50% between its inner end and the minimum value. Spiral selon l'une des revendications précédentes, réalisé en un matériau fragile.Spiral according to one of the preceding claims, made of a fragile material. Spiral selon l'une des revendications précédentes, réalisé en un matériau cristallin.Spiral according to one of the preceding claims, made of a crystalline material. Spiral selon l'une des revendications précédentes, réalisé en silicium.Spiral according to one of the preceding claims, made of silicon. Ensemble balancier-spiral utilisant un spiral selon l'une des revendications précédentes.Spiral balance assembly using a hairspring according to one of the preceding claims.
EP10405172.7A 2009-09-21 2010-09-16 Flat hairspring for a clock balance wheel and balance wheel -hairspring assembly Active EP2299336B1 (en)

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CH00319/10A CH701846B8 (en) 2009-09-21 2010-03-09 Flat spiral for clockwork pendulum and balance-sprung assembly.

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WO2017163148A1 (en) 2016-03-23 2017-09-28 Patek Philippe Sa Geneve Balance wheel oscillator for timepiece
US11249440B2 (en) 2016-03-23 2022-02-15 Patek Philippe Sa Geneve Balance-hairspring oscillator for a timepiece
FR3088396A1 (en) 2018-11-08 2020-05-15 Abdou Dib CONSTANTLY TORQUE SPIRAL TORSION SPRING FOR ENERGY STORAGE
EP3913441A1 (en) 2020-05-22 2021-11-24 Patek Philippe SA Genève Oscillator for a timepiece
EP4293428A1 (en) 2022-06-14 2023-12-20 Patek Philippe SA Genève Hairspring for timepiece resonator
WO2023242746A1 (en) 2022-06-14 2023-12-21 Patek Philippe Sa Geneve Balance spring for a timepiece resonator
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EP4372479A1 (en) * 2022-11-18 2024-05-22 Richemont International S.A. Method for manufacturing timepiece hairsprings

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EP2299336B1 (en) 2019-04-24
JP5496034B2 (en) 2014-05-21
CH701846A1 (en) 2011-03-31
JP2011064687A (en) 2011-03-31
US20110069591A1 (en) 2011-03-24
CH701846B8 (en) 2015-06-15
CN102023558A (en) 2011-04-20
CN102023558B (en) 2014-08-20
CH701846B1 (en) 2014-07-15
EP2299336A3 (en) 2017-10-11
US8348497B2 (en) 2013-01-08

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