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A mechanical oscillator system comprising a balance wheel and a spiral or helicoidal balance spring for use in horological mechanisms or other precision instruments. The balance spring is made of a non-magnetic composite, polymer, carbon or ceramic material, preferably a composite material of carbon

A mechanical oscillator system comprising a balance wheel and a spiral or helicoidal balance spring for use in horological mechanisms or other precision instruments. The balance spring is made of a non-magnetic composite, polymer, carbon or ceramic material, preferably a composite material of carbon fibres in a polymer, carbon or ceramic matrix, and the balance wheel is made from a non-magnetic ceramic. The values of the thermal expansion coefficients for the balance spring and balance wheel are similar, very small and stable over a wide temperature range. The expansion coefficients in the axial sense of the spring and of the balance wheel are of opposite sign and they compensate one another. The density of these materials is smaller than that of the currently used metals. Through this combination of materials it is possible to obtain significant advantages and a higher level of accuracy and stability compared with metal oscillator systems.

대표청구항 ▼

The invention claimed is: 1. A mechanical oscillator system for a horological mechanism or other precision instrument, the system comprising a non-magnetic ceramic balance and a non-magnetic balance spring formed of a composite material or a polymer, carbon or ceramic material, wherein the balance

The invention claimed is: 1. A mechanical oscillator system for a horological mechanism or other precision instrument, the system comprising a non-magnetic ceramic balance and a non-magnetic balance spring formed of a composite material or a polymer, carbon or ceramic material, wherein the balance and balance spring are adapted such that the coefficient of thermal expansion of the balance (α1), the coefficient of thermal expansion of the balance spring (α2) and the thermoelastic coefficient of the balance spring (∂E/E) cooperate to compensate for thermal variation in the system. 2. A system according to claim 1, wherein the material of the balance spring is a composite material having a matrix phase comprising polymer, carbon or ceramic. 3. A system according to claim 1, wherein the balance spring material comprises continuous fibres extending along the length of the balance spring from one end of said spring to the other end of said spring. 4. A system according to claim 3, wherein said continuous fibres are carbon fibres. 5. A system according to claim 3, wherein the fibres are produced from one of the precursors ‘PITCH’ or polyacrilonitrile ‘PAN’. 6. A system according to claim 1, wherein the material of the balance spring is a composite material having a coefficient of thermal expansion in the direction along the length of the balance spring which is negative and exhibits linear thermal variation up to 7000° Kelvin. 7. A system according to claim 1, wherein the damping of the modulus of elasticity of the balance spring is of the order of 0.001 Pa. 8. A system according to claim 1, wherein the balance spring material comprises ceramic fibres. 9. A system according to claim 8, wherein said ceramic fibres have a coefficient of thermal expansion whose magnitude is less than 6×10−6 K−1. 10. A system according to claim 3, wherein said fibres are substantially parallel to each other. 11. A system according to claim 3, wherein said fibres are twisted together. 12. A system according to claim 1, wherein the balance spring is a flexion spring configured to work in flexion to oscillate the balance. 13. A system according to claim 1, wherein the density of the balance spring material is less then 3 g/cm3. 14. A system according to claim 1, wherein the balance is formed by high precision injection moulding. 15. A system according to claim 1, wherein the material of the balance spring has a negative thermoelastic coefficient. 16. A system according to claim 1, wherein the balance spring is of flat spiral or helicoidal form, and the coefficient of thermal expansion of the balance spring in a direction along its length and the coefficient of thermal expansion of the balance are of opposite signs and of similar orders of magnitude. 17. A system according to claim 16, wherein the coefficient of thermal expansion of the balance is positive and the coefficient of thermal expansion of the material of the balance spring in the direction along the length of the balance spring is negative. 18. A system according to claim 17, wherein the thermal coefficient of expansion of the balance is less than 1×10−6 K−1 and the coefficient of thermal expansion of the material of the balance spring in the direction along the length of the balance spring is greater than −1×10−6 K−1. 19. A system according to claim 1, wherein the respective magnitudes and thermal variations of the coefficient of thermal expansion of the material of the balance (α1), the coefficient of thermal expansion of the material of the balance spring (α2) and the thermoelastic coefficient of the material of the balance spring (∂E/E) are selected such that, for thermal variation within a predetermined temperature range, the variation (U) in timekeeping changes for the system is minimized, where U=α1−3/2α2−1/2∂E/E. 20. A non-magnetic balance spring for oscillating a balance in an oscillator mechanism for a horological instrument, the balance spring formed from a composite material or a polymer, carbon or ceramic material, wherein the balance spring material has a coefficient of thermal expansion (α2) and a thermoelastic coefficient (∂E/E) arranged to cooperate with a coefficient of thermal expansion of the balance (α1), by decreasing in length and increasing in thickness with increase in temperature to compensate for thermal variation in the system.