Patent Application
20130070572
This application claims priority from European Patent Application No. 11181508.0 filed Sep. 15, 2011, the entire disclosure of which is incorporated herein by reference.
The invention relates to a timepiece with permanently coupled oscillators and a timepiece of this type comprising two oscillators intended to display at least one value less than or equal to a second with better resolution and/or better precision.
It is known to form timepieces with increased frequency in order to improve resolution. However, these timepieces may be very shock sensitive or high energy consumers, which prevents them from becoming common.
It is therefore clear that it is easier to manufacture a calibre by mounting a low frequency oscillator, typically 4 Hz, to display the time and another high frequency oscillator, typically 10 or 50 Hz, which is independent from the first, to display a measured time with improved resolution. However, after several seconds, it is observed that the seconds display of the two oscillators is no longer the same, which may make the quality of the timepiece appear dubious.
It is an object of the present invention to overcome all or part of the aforementioned drawbacks by proposing a timepiece capable of displaying the time with better resolution, while ensuring the usual robustness of a mechanical watch, reduced energy consumption and minimum drift between the oscillators.
The invention therefore relates to a timepiece comprising a first oscillator oscillating at a first frequency and connected by a first gear train to an energy source and a second oscillator oscillating at a second frequency and connected to a second gear train, characterized in that the second gear train is connected to the first gear train by an elastic coupling means in order to synchronise the rate of the two oscillators using the same energy source.
It is therefore clear that, in the event of shocks, rate variations will be minimal owing to the construction which allows the two oscillators to be synchronised. Consequently, the timepiece according to the invention is capable of displaying the time with better resolution and/or better precision while ensuring a high level of robustness, low power consumption and minimal drift between the gear trains.
In accordance with other advantageous features of the invention:
Other features and advantages will appear clearly from the following description, given by way of non-limiting illustration, with reference to the annexed drawings, in which:
As illustrated in
Advantageously according to the invention, the second gear train 25 is permanently connected to first gear train 5 by an elastic coupling means 41 in order to synchronise the rate of the two oscillators 15, 35, using the same energy source 9. As seen in the example of
Preferably according to the invention, elastic coupling means 41 is formed by a spring 43 connecting one wheel of first gear train 5 to another wheel of second gear train 25. As illustrated in
Preferably according to the invention, it is seen that a double wheel 42 is used. As shown more clearly in
Advantageously according to the invention, the time display, i.e. the hours, minutes and/or seconds, can be achieved either using the first or second gear train 5, 25.
Depending upon the desired application of the timepiece, the first f1 and second f2 frequencies may or may not be identical. Thus, in a first embodiment, the first and second frequencies f1, f2 are identical and preferably higher than 5 Hz for displaying the time with better resolution and/or better precision. In this embodiment, frequencies f1, f2 may, for example, be equal to 10 Hz or 50 Hz for displaying 1/20th or 1/100th of a second respectively.
Thus, depending upon the oscillator chosen as reference, it may be useful to mount the hour and minute display on the gear train of said oscillator selected as reference and the seconds display on the gear train of the second oscillator. Indeed, it has been observed that, when there is a shock, the seconds display may cause induced torque in the oscillator capable of changing the amplitude and rate of said oscillator.
In a second embodiment, the first frequency f1 is higher than the second frequency f2 so as to display the time with better resolution and/or better precision. In a similar manner to the first embodiment, the first frequency f1 is at least equal to 10 Hz and the second frequency f2 is preferably comprised between 1 and 5 Hz. Indeed, by way of example, it may be desired for a second to be incremented by a single step per second, i.e. second frequency f2 is equal to 1 Hz, “like” a quartz watch.
In a third embodiment, the first frequency f1 is lower than the second frequency f2 so as to display the time with better resolution and/or better precision. In this embodiment, which is the reverse of the second embodiment, the same advantages are obtained.
Simulations were developed hereinafter to describe the synchronisation between these two oscillators 15 and 35. The third embodiment has been arbitrarily selected for the explanation. Thus, oscillator 15, which is selected as the reference, is of the low frequency type and is called the first oscillator. Consequently, in the example below, the second oscillator will be high frequency oscillator 35, which will be synchronised with low frequency oscillator 15.
Preferably according to the invention, the second oscillator 35 is selected with a strong anisochronism according to amplitude, described by the anisochronism slope and the amplitude A20 at which the rate is zero. Moreover, since the first oscillator 15 is selected as the reference, it always has a substantially zero rate by slightly varying its amplitude.
The simulations show the change in the two oscillators 15, 35, i.e. their amplitude and state of phase difference with time, and thus mean that it can be checked whether or not it is possible to synchronise second oscillator 35 with first oscillator 15.
Preferably, second oscillator 35 is constructed so that its rate is zero when it oscillates at an amplitude A20, positive when it oscillates at an amplitude higher than A20 and negative when it oscillates at an amplitude lower than A20.
Further, elastic coupling means 41 is devised so that the torque transmitted to second gear train 25 remains constant if the two gear trains 5, 25 are rotating at the same speed, decreases if second gear train 25 is advancing more quickly than first gear train 5 (spring 43 is letting down) and increases if second gear train 25 is advancing more quickly than first gear train 5 (spring 43 is being wound).
If the above conditions are satisfactory, the timepiece will always move towards the stable situation where second oscillator 35 oscillates at amplitude A20 and in which spring 43 transmits to second gear train 25 the torque M2 necessary to keep second oscillator 35 at amplitude A20.
Consequently, if second oscillator 35 receives a torque lower than M2, its amplitude decreases, i.e. it has an amplitude of less than A20. As explained above, its rate becomes negative, i.e. second oscillator 35 falls behind first oscillator 5, selected as the reference.
It is thus clear that second gear train 25 will rotate more slowly than first gear train 5 while winding coupling spring 43, i.e. increasing the torque transmitted to second gear train 25. Consequently, since the torque is increasing, the amplitude of second oscillator 35 is automatically corrected. It is thus observed that the torque and amplitude of second oscillator 35 are structurally synchronised on the stable torque M2 and stable amplitude A20.
Similarly, if the torque received exceeds torque M2, then the amplitude of second oscillator 35 becomes greater than value A20, which means that the rate of second oscillator 35 will be positive. Second gear train 25 is then ahead of first gear train 5 while letting down spring 43. Consequently, the torque on second gear train 25 will decrease towards stable torque M2, and the amplitude of second oscillator 35 will again tend towards stable amplitude A20.
It is thus seen that regardless of the situation, whether it is when the watch is started, or after a shock, the system will always move towards stabilisation in the stable situation where the torque on second gear train 25 has a value M2 and the amplitude of second oscillator 35 has a value of A20.
Preferably according to the invention, it is assumed that the barrel torque 9 and the frequency f1, f2 of the two oscillators 15, 35 are given parameters. It is thus clear that the parameters still to be selected are:
Preferably according to the invention, the parameters are selected as follows:
Advantageously according to the invention, it is also preferred to “adjust” K and so that:
Empirically, it was demonstrated that it is preferable for the product K. to be kept identical in order to have the same stabilisation time in the continuing approximation. Thus, increasing K (and thus decreasing
by the same amount) decreases the fluctuations in amplitude and torque (thus preventing the torque being cancelled out). However, this also increases the maximum state drift prior to stabilisation, and the instantaneous rate, which may become extreme. A compromise must therefore be found between these two effects.
It was also observed that increasing the frequency of the oscillator which is synchronised (second oscillator 35 above) decreases the stabilisation time. Finally, during tests, it was demonstrated that decreasing the quality factor of the oscillator which is synchronised (the second oscillator above) also decreases the stabilisation time.
for each simulation.
Part A of each Figure corresponds to the fraction of amplitude of each oscillator relative to the reference amplitude if it received all of the torque from the energy source. It is to be noted that for the examples in the Figures, the amplitude A20 chosen for the second oscillator is approximately ⅓. Thus, after 2 and 1.5 seconds respectively, each oscillator is stabilised at its synchronised amplitude.
Part B of each Figure corresponds to the fraction of torque that each oscillator receives from the energy source. It is to be noted that for the examples in the Figures, the proportion of torque chosen for the second oscillator is around 10%. Thus, after 2 and 1.5 seconds respectively, each oscillator receives its proportion of torque in a stabilised manner.
Part C of each Figure corresponds to the rate of the second oscillator. It is to be noted therefore that after 5.5 and 2 seconds respectively, the second oscillator is stabilised around its zero rate.
Finally, part D of each Figure corresponds to the difference in state in seconds between each oscillator. It is therefore to be noted that after 5 and 2 seconds respectively, the difference is stabilised at its zero value.
Parts A-D of
Moreover, during tests, it was discovered that not only did the first oscillator selected as the reference preferably have better quality isochronism than the second oscillator so as to facilitate synchronisation of said second oscillator, but the second oscillator preferably has a lower quality factor than the first oscillator, preferably lower than 100, so as to obtain more rapid stabilisation, i.e. typically less than 2 seconds.
Of course, this invention is not limited to the illustrated example but is capable of various variants and alterations that will appear to those skilled in the art. In particular, the oscillator selected as the reference may equally well be either first oscillator 15 or second oscillator 35, since the conclusions relating respectively to the first oscillator and second oscillator will not change.
Thus, to invert the above example, the oscillator selected as the reference could be second oscillator 35, selected with a high frequency so as to form a precision timepiece. In this case, the time display will preferably be achieved using the first gear train 5 of the first oscillator chosen at low frequency to limit the propagation of torque induced by any shock to the second, high frequency oscillator 35.
Moreover, the oscillator which preferably has a frequency at least equal to 10 Hz, may be a Clifford oscillator (see for example CH Patent No. 386344 incorporated herein by reference) instead of the oscillator disclosed above. Further, the oscillator, which has a frequency comprised between 1 and 5 Hz, will preferably be of the sprung balance type and have a Swiss lever escapement.
Of course, elastic coupling means 41 is not limited to a double wheel 42 cooperating with a spring 43, as illustrated in
Advantageously according to the invention, it is clear that the timepiece may thus structurally include a display for a value of less than a second permanently or non-permanently secured (i.e. via a coupling) to gear train 5, 25 which has a high frequency oscillator. Thus the value could be as low, for example, as 1/20th of a second, if the oscillator beats at at least 10 Hz, or 1/100th of a second if the oscillator beats at at least 50 Hz. The timepiece may even comprise a disconnectable chronograph system, also secured to the first or second gear trains 5, 25.
Finally, it is possible to further optimise the behaviour of the system if the anisochronism of the second oscillator is non-linear. By way of example, the second oscillator may have a low anisochronsim around the amplitude of equilibrium and a strong anisochronism far from the amplitude of equilibrium, or vice versa.
| Number | Date | Country | Kind |
|---|---|---|---|
| 11181508.0 | Sep 2011 | EP | regional |
