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    • 专利摘要:
    The invention relates to a vibrating inertial sensor, micro machined in a flat thin plate, for measuring an angular position (gyroscope) or an angular velocity (gyroscope). The sensor comprises two vibrating masses (M1, M2) suspended by springs with identical stiffness in X and Y and coupled together by identical stiffness springs in X and Y, and at least excitation transducers (Ex1, Ex2, Ey1, Ey2) and detection (Dx1, Dx2, Dy1, Dy2) arranged on at least one of the masses. The moving assembly constituted by a vibrating mass and the integral transducer parts of this mass has a generally symmetrical structure with respect to an axis of symmetry OX and with respect to an axis of symmetry OY.
    公开号:FR3022996A1
    申请号:FR1401451
    申请日:2014-06-27
    公开日:2016-01-01
    发明作者:Bernard Chaumet；Fabien Filhol；Claude Rougeot；Bertrand Leverrier
    申请人:Thales SA；
    IPC主号:
    专利说明:

    [0001] The invention relates to a vibrating inertial sensor, micro-machined in a flat thin plate, for measuring an angular position (gyroscope) or an angular velocity (gyroscope). The manufacture of these micro-machined sensors, also called MEMS sensors (Micro-Electro-Mechanical-Systems), uses collective micro-machining techniques, etching, doping deposits, etc., similar to those used for the manufacture of electronic integrated circuits, allowing low production costs. Such MEMS inertial sensors made on a silicon or quartz plate by micromachining are already known. The structure is flat in the plane of the silicon or quartz substrate in which it is etched. These sensors consist of a plurality of vibrating movable masses connected to each other and to their support by elastic elements so as to constitute an excitation resonator, or primary resonator, and a detection resonator, or secondary resonator, the two resonators being coupled between them by Coriolis acceleration. These sensors have means of excitation, detection, and often balancing. In these sensors, the masses are generally excited in vibration in the plane XY of the plate, perpendicular to a Z axis, said "sensitive axis" of the gyrometer. When the gyro rotates about its sensitive axis, the composition of the forced vibration with the angular rotation vector generates, by the Coriolis effect, forces that put the moving masses in natural vibration perpendicular to the excitation vibration and to the axis. sensitive; the amplitude of this natural vibration is proportional to the speed of rotation. The natural vibration is detected by a detection transducer whose electrical signals are operated by an electronic circuit to derive a value of the angular velocity around the sensitive axis.
    [0002] Different MEMS vibrating inertial sensor structures are known that define the shapes and layouts of the various elements of the structure. These various elements will typically be the vibrating elements, the suspension mechanisms of these elements, the coupling mechanisms; the electrostatic excitation and detection transducers allowing the actual measurement and the electrostatic transducers allowing different balancing or compensations making it possible to improve the accuracy of the measurement. These structures are developed to satisfy different constraints, measurement accuracy, low energy losses, while remaining in the field of MEMS manufacturing technologies.
    [0003] The performance of such sensors can be degraded by the energy losses of the resonators to the outside. To limit these energy losses, the excitation resonator of most gyrometers is first-order balanced by the use of two vibrating masses in phase opposition, such as a tuning fork. The useful mode of vibration in opposition of phase is separated from the parasitic mode in phase thanks to a central coupling elastic element which introduces a stiffness between the two masses. An example of such a sensor is described in patent FR2846740. However, in such sensors energy losses remain because the secondary resonator is not balanced by construction. As a result, this mode transmits a torque on the support of the tuning fork, which makes this mode sensitive to the conditions of fixation on the support and the external disturbances transmitted by the support. Tuning gyro structures comprising elastic coupling means between the tuning fork legs are well known and described in the patent literature. In these structures, therefore, the vibration of the masses in opposition of phase is exploited by separating the useful mode of vibration from the parasitic modes. To improve the measurement accuracy, these structures provide different means of adjustment or compensation, whether by construction and / or by the use of electrically controlled compensation or adjustment elements. Double tuning fork structures using four masses have also been proposed to compensate by construction for the balancing faults of the secondary resonator of the simple tuning fork structure. Patents FR2859527 and FR2859528 give examples thereof.
    [0004] In these different structures, residual balancing imperfections of the resonators remain, as well as parasitic couplings between the excitation mode and the detection mode, which may be due to the imbalances of the various elastic suspension and coupling means used. The present invention proposes a sensor architecture with axisymmetric rigid moving masses, which can be produced by collective micro-machining in a thin flat plate of silicon (or quartz) and operating in tuning fork mode. The architecture is balanced by construction and well insulated from its outside environment. It can be completed by means of compensation and electrostatic balancing for the compensation of defects in the construction of the structure. It allows in particular an excitation of the vibration in any direction of the plane perpendicular to the sensitive axis Z. This architecture comprises two concentric moving masses, which are suspended and coupled together by springs, and which vibrate in tuning fork mode, without a preferred axis in the XY plane of the plate: the useful vibration mode corresponds to a linear vibration of the two masses in phase opposition both along an X axis and along a Y axis orthogonal to the X axis. resonant system with two suspended masses, coupled together by elastic elements, which has few parasitic vibration modes and which allows a good separation between these modes and the useful mode of vibration; a parasitic vibration mode corresponds for example to a linear vibration of the two masses in phase, at a frequency all the more separated from the frequency of the useful mode that the stiffness of the coupling between the two masses is higher.
    [0005] The invention thus relates to a micro-machined inertial angular sensor comprising at least two vibrating masses machined in a generally flat support plate, movable with respect to the plate and movable relative to each other, suspended at points of rotation. fixed anchoring of the plate by suspension springs and coupled together by coupling springs to vibrate in opposition of phase.
    [0006] According to the invention, the sensor comprises: at least one excitation transducer of a vibration movement of one of the masses in a direction X in the plane of the plate, an excitation transducer of this mass in one direction Y perpendicular to the X direction and in the plane of the plate, a transducer for detecting a vibration of one of the masses in the X direction and a transducer for detecting a vibration of one of the masses in the Y direction; the two mobile vibrating masses are arranged around each other, in an internal mass and an external mass, and their centers of gravity are merged at rest; the coupling springs are each connected on one side to the internal mass and the other to the external mass, - the stiffness of the suspension springs of the internal mass and the stiffness of the suspension springs of the external mass are proportional to the values of the respective masses, - the moving assembly constituted by a vibrating mass and the integral transducer parts of this mass has a generally symmetrical structure with respect to an axis of symmetry OX parallel to the X direction and passing through the center of gravity of the mass, and also generally symmetrical with respect to an axis of symmetry OY parallel to the direction Y and passing through the center of gravity of the mass. Preferably, the stiffnesses of the coupling springs are identical in the X direction and in the Y direction, the stiffness of the suspension springs of the internal mass to the plate are identical in the X direction and in the Y direction and the stiffness of the The suspension springs of the mass external to the plate are identical in the X direction and in the Y direction. Particular cases will be described below where the generally symmetrical structure is not 100% symmetrical, these cases being mainly related to In fact, certain electrostatic transducers auxiliary to the structure may be interdigitated interdigitation interdigitation combs while the main electrostatic excitation and detection transducers are preferably asymmetrical interdigitated combs at rest. The minor differences of symmetry that may result from them and which nevertheless come within the framework of the general symmetry of the mobile sets of the invention will be explained below. The internal and external vibrating masses are preferably equal and the stiffness of the suspension springs of these masses are then identical. The transducers associated with a moving mass preferably each comprise a pair of interdigitated combs comprising a movable comb formed of a row of teeth integral with the moving mass and a fixed comb formed of a row of teeth integral with a fixed electrode. of the sensor. The interdigitation of the teeth at rest is asymmetrical for the excitation transducers and the detection transducers. Preferably, at least one of the vibrating masses is coupled to a first electrostatic frequency adjustment transducer, in interdigitated interdigitated interdigitation combs, capable of applying an X-direction adjustable electrostatic stiffness, and a second a frequency adjustment transducer similar to the first capable of applying an electrostatic stiffness adjustable in the Y direction to the mass. Preferably, the geographical arrangement, with respect to the axis of symmetry OX, of the excitation and detection transducers , but possibly also frequency adjustment or quadrature bias compensation transducers, working in the X direction is identical to the geographical arrangement with respect to the OY axis of the transducers performing the same functions but working in the Y direction Also preferably, at least one of the vibrating masses is coupled to at least one electrostatic quadrature bias compensation transducer, for modifying the symmetry of the mass suspension stiffness in the X direction and in the Y direction. This transducer is preferably an interdigital interdigitated comb transducer. There is preferably at least one positive quadrature bias compensation transducer and at least one negative quadrature bias compensation transducer.
    [0007] Each of the transducers associated with a vibrating mass may be formed of two pairs of interdigitated combs arranged symmetrically with respect to the direction of action or detection X or Y of the transducer, with one of the following configurations: the transducer is divided into two transducers arranged on either side of the vibrating mass, that is to say that the two mobile combs are arranged symmetrically on either side of the vibrating mass and the two fixed combs are arranged on both sides of the vibrating mass other of the vibrating mass, also symmetric except in the case of compensation transducers of a quadrature bias; - Or the teeth of the moving combs are located symmetrically on either side of a fixed electrode within an opening of the vibrating mass, the latter surrounding the pair of combs and the fixed electrode.
    [0008] Preferably, each of the two mobile vibrating masses comprises excitation transducers, detection transducers, and possibly also frequency adjustment transducers and quadrature bias compensation transducers. It is then arranged that the general configuration of the set of moving masses, and mobile combs associated with these masses is generally symmetrical with respect to the axis of symmetry OX and also with respect to the axis of symmetry OY, preferably according to a symmetry of order 4, that is to say an invariance of the configuration when the assembly is rotated by 90 ° around the axis OZ, and this with the possible exception of minor dissymmetries directly or indirectly due to the fact that the frequency adjustment transducers are symmetrical at rest, unlike the other transducers. It can advantageously be provided that the number of comb teeth of each type of transducer (excitation, or detection, or frequency adjustment, or quadrature bias compensation) is identical on the two masses, for each direction X and Y so to optimize the similarity of the physical effects exerted on the two masses. In general, the mechanical characteristics and in particular the distribution of the masses of the moving assemblies (masses themselves and moving combs or moving parts of the transducers which are integral with the masses) and the stiffness of the suspension arms and the stiffnesses of the arms of coupling are such that these mobile assemblies have, by construction, no preferred vibration axis in the XY plane. The overall symmetry of the moving assemblies makes it possible to reduce the sensitivity of the sensor to disturbances that would induce static displacements of the moving masses, for example static accelerations or stresses.
    [0009] In a judicious configuration of the transducers (interdigitated combs), for each mobile mass, provision is made for: the direction of action or detection of each electrostatic transducer is oriented parallel to the axis of symmetry OX or parallel to the axis of symmetry OY; the configuration of the teeth of the interdigitated combs of each transducer (at least for the excitation and detection combs) is symmetrical with respect to an axis parallel to the axis of action or detection of the transducer, that is to say say, parallel to the axis of symmetry X or to the axis of symmetry Y as the case may be; for each vibrating mass, the general arrangement of the transducers with respect to the axis of symmetry OX is the same as the arrangement of the transducers with respect to the axis of symmetry OY. If there are quadrature bias compensation transducers, the similarity of arrangement of the transducers around the X and Y axes is obtained either by arranging a pair of transducers with comb electrodes with X acting in positive and negative and a other pair with comb electrodes arranged in Y acting in positive and negative, or producing two transducers (for positive quadrature bias and negative quadrature bias respectively) with double combs having teeth oriented in both directions X and Y, or finally by providing a positive quadrature bias compensation transducer disposed along one of the axes, X for example, and a negative quadrature bias compensation transducer disposed along the other axis, Y in this case.
    [0010] If we are now interested in the similarity of arrangement of the transducers on the two inner and outer masses, it is preferably provided that each of the two masses has at least one electrostatic excitation transducer for the X direction and another for the Y direction, an electrostatic detection transducer for the X direction and another for the Y direction, an electrostatic frequency adjustment transducer for the X direction and another for the Y direction, and also preferably at least one compensation transducer bias in quadrature acting on the positive bias and a quadrature bias compensation transducer acting on the negative bias. The excitation and detection transducers with asymmetric interdigitation are preferably arranged on the internal vibrating mass and on the external mass with a direction of inverse dissymmetry, both in the X direction and in the Y direction.
    [0011] The transducers are of course associated with electronic circuits that allow their operation according to known principles. Other features and advantages of the invention will become apparent on reading the detailed description which follows and which is given with reference to the appended drawings in which: FIG. 1 represents the general principle of constitution of the mechanical resonator according to the invention; the transducers are not represented; - Figure 2 shows forms of suspension springs or coupling the masses; - Figure 3 shows an alternative arrangement of the two vibrating masses; - Figure 4 and Figure 5 show other variants; FIG. 6 represents the known block diagram of an interdigitated interdigitated comb transducer; FIG. 7 represents the block diagram of a symmetrical interdigitation comb frequency adjustment transducer; - Figure 8 shows a symmetrical arrangement of a dual transducer composed of two transducers opposite to the periphery of a vibrating mass; FIG. 9 shows a symmetrical arrangement of a transducer in an opening of a vibrating mass; FIG. 10 represents a possible arrangement of the transducers at the periphery of a vibrating mass; - Figure 11 shows another configuration where the transducers are placed in openings of the vibrating mass; Figure 12 shows an arrangement in which quadrature bias compensation transducers are provided in an opening of the vibrating mass; Fig. 13 shows an arrangement in which the bias compensation transducers are located at the periphery of the mass; FIG. 14 and FIG. 15 represent other possible constitutions of the bias compensation transducers; FIG. 16 represents a complete configuration of the vibrating masses with their transducers, only the internal mass being associated with transducers; FIGS. 17, 18, 19, 20 represent different possible configurations of mobile assemblies with their transducers, in which the two vibrating masses comprise transducers of each type; and Fig. 21 shows aspects of constitutions and arrangements of positive and negative quadrature bias compensation transducers. Briefly, the principles of fabrication of an MEMS inertial sensor are summarily recalled: a thin silicon plate is machined to make a gyrometer whose sensitive axis Z is perpendicular to the XY plane of the plate and whose excitation movements and detection are located in the plane of the plate. Silicon is chosen as the preferred material, on the one hand for its mechanical properties and on the other hand for its high conductivity when it is sufficiently doped by an appropriate impurity (boron in general for P-type silicon). Conductive silicon makes it possible to carry out the electrical functions of the sensor, in particular the electromechanical transduction functions which are generally performed by interdigital capacitive comb electrodes supplied with current or electrical voltage; the teeth of these combs, directly machined in the conductive silicon, serve as a reinforcement of capacitors useful for the excitation functions and the detection functions. The thickness of the silicon wafer is, for example, a few hundred micrometers, the plate comprises, on the one hand, fixed anchoring zones formed in this thickness and, on the other hand, the vibrating structure proper, free with respect to the zones anchoring and formed on a smaller thickness, for example on a thickness of a few tens of micrometers, isolated from the rest of the thickness of the plate by an empty gap. Over this thickness of a few tens of micrometers, the silicon wafer is cut by micromachining according to the desired patterns of vibrating masses, coupling structures between masses, suspension springs and interdigitated combs. To simplify the explanations, the general principle of the vibratory inertial sensor according to the invention will now be described by focusing first on the configuration of the vibrating masses, the suspension structures of these masses relative to the fixed anchoring points, and elastic coupling structures between these masses. The configuration of the different electrostatic excitation transducers acting on these masses and electrostatic detection transducers that detect their natural vibration will be explained. Then, the arrangement of the electrostatic transducers of frequency adjustment or bias compensation will be described. Finally, we will describe various possibilities of complete arrangement of the transducers on the vibrating masses.
    [0012] Configuration of the vibrating masses The principle of the mechanical resonator according to the invention is schematically illustrated in plan view in FIG. 1. It comprises two moving masses, M1 and M2, planar, concentric, vibrating in tuning fork mode, that is to say say in opposition of phase, in their own plan. This XY plane is the plane of the figure. OX and OY are two orthogonal axes in the plane of the plate and an axis OZ perpendicular to the plane. The axes OX and OY constitute two axes of symmetry of the mass M1 as well as the mass M2. We will call direction X a direction parallel to the axis OX and direction Y a direction parallel to the axis OY. The two masses are arranged one around the other in an internal mass M1 and an external mass M2 and have their centers of gravity 10 merged at rest. The center of gravity brought back into the plane of the drawing is indicated by O in the figure. The directions X and Y are the preferred directions of excitation of the vibration of the masses but a combined excitation is possible. Likewise, the X and Y directions are preferred directions of motion detection and they can be combined. This excitation and this detection are carried out in known manner by electrostatic transducers interdigitated combs, at least one of each type for each of the directions X and Y. In a well known manner, these interdigitated combs comprise a movable comb secured to the mobile mass 20 associated and a fixed comb secured to the sensor substrate. The teeth of the combs are perpendicular to the X direction or the Y direction and in this the excitation or detection according to X or Y is preferred. Each of the masses has a plane geometrical shape which generally has a fourth order symmetry with respect to the OZ axis, ie the overall shape remains largely unchanged when the mass is rotated by 90 °. . We will return to particular cases where a minimal dissymmetry of form can subsist. Each of the moving masses is suspended by suspension springs RS at fixed anchoring points A. The stiffness of the suspension springs of the internal mass are identical in the direction X and the direction Y, equal to a value denoted K1. The stiffnesses of the suspension springs of the external mass are identical in the direction X and the direction Y is equal to a value denoted K2. And the stiffnesses of the suspension springs are proportional to the respective mass values ml and 35 m 2 of the internal masses M1 and external M2, which is written: K1 / m1 = K2 / m2.
    [0013] The masses ml and m2, however, are preferably equal and therefore the stiffness K1 and K2 too. In the following, we note Ks the stiffness of the suspension springs. The two masses are interconnected by RC coupling springs, of stiffness Kc equal in direction X and direction Y. Each of these springs is fixed on one side to the internal mass, on the other to the external mass . The structure of the moving assembly consisting of the inner and outer masses, the orthotropic coupling and suspension springs (identical in the X and Y directions), as well as the excitation and detection transducers in each of the X and Y directions is a structure which is symmetrical with respect to the axis of symmetry OX and also symmetrical with respect to the axis of symmetry OY. The identity (or isotropy) of stiffness of the suspension springs in the X and Y directions is obtained by providing that these springs each comprise at least two orthogonal arms of the same length forming an L having an end secured to an anchor point. and an end fixed to the moving mass. Similarly, for the coupling springs, the ends of the L being integral with each of the movable masses.
    [0014] In FIG. 1, the springs RS and RC are represented as each comprising two L-shaped structures starting from the same points, that is to say that each spring is constituted by the four branches of a square whose sides are parallel. to the axes of symmetry OX and OY and whose two opposite corners are attached to a mass on one side and an anchor point or the other mass on the other side. There are four RS suspension springs arranged at the four corners of each moving mass, and four RC coupling springs between masses, also at the four corners. The lengths of the sides of the Ls or squares are greater for the coupling springs than for the suspension springs, the stiffness Kc being a priori lower than the stiffness Ks. FIG. 2 represents other possible forms of suspension springs. with identical stiffnesses in the X direction and in the Y direction. The desired stiffness is adjusted by the choice of the geometric dimensions of the springs: length, width, thickness and number of the arms. Folded arms can offer a longer useful length and therefore a lower stiffness. similar shapes are possible for the coupling springs. In FIG. 1, the internal mass is represented by a simple square and the external mass by a frame which surrounds this square. If the masses must be identical, the stiffness of the suspension springs then being identical for the two masses, the surfaces occupied by the square and the frame in the plan view must be identical. In this example of Figure 1, the anchoring points of the inner mass are located between the inner mass and the outer mass and the coupling springs surround these anchor points. The suspension springs are advantageously placed at the corners of the squares to be as far apart as possible, so as to limit the rotational movements in rotation. It would also be possible to place them anywhere else, since their function is not impaired and the symmetry of order 4 remains respected. FIG. 3 represents a variant in which: the anchoring points A of the internal mass are merged with the anchoring points 20 of the external mass; the suspension springs of the two masses are located on either side of these anchor points; the RC coupling springs surround the anchor points and the RS suspension springs; the inner mass is formed in the form of a cross to best occupy the space available inside the external mass while leaving a place 25 in the corners to springs and anchor points. Note that the two reaction forces from the deformation of the suspension springs cancel each anchor point. FIG. 4 shows another variant in which the four orthotropic suspension springs RS of the internal mass are arranged in the center of the latter, in an opening provided for this purpose, and connected to the same anchoring point A. even consider having in this opening four different anchor points and an orthotropic suspension spring associated with each of them. FIG. 5 represents another example intended to improve the mechanical robustness of the structure or to better separate the useful vibration mode (vibration of the masses in opposition of phase) from the parasitic modes with rotational movements or movements outside the plane . In this example, there is a greater number of suspension springs (eight per moving mass). The symmetry of order 4 remains however respected, that is to say that the general design of the moving assembly comprising the masses and the suspension and coupling springs remains invariant during a rotation of 90 ° around the OZ axis.
    [0015] When the overall structure is thus made generally symmetrical, with orthotropic suspensions (that is to say identical in the X and Y directions), the movements of the two coupled masses will be parallel (but in opposition to phase) and suitable vibration transducers acting in the X and Y directions can be used to maintain a forced vibration in any direction of the XY plane without a preferred axis, including a continuously variable direction, that is to say a movement of precession; the vibration is isotropic in the XY plane. A possible parasitic vibration mode, in phase and not in phase opposition, may exist, but its frequency is further removed from the frequency of the useful vibration mode as the stiffness of the coupling springs is greater. The frequency of the useful mode is proportional to the square root of (Ks + 2Kc) while the frequency of the parasitic mode is proportional to the square root of Ks, where Ks and Kc are the respective stiffness of the suspension and coupling springs. To excite the useful mode of vibration in any given direction of the plane, the excitation signal is decomposed into two components of respective adjusted amplitudes applied respectively to the excitation transducers acting in the direction X and to the excitation transducers acting in direction Y. When the gyro rotates about its sensitive axis Z, the Coriolis effect generates forces that put the moving masses in natural vibration perpendicular to the excitation vibration and the sensitive axis; the amplitude of this natural vibration is proportional to the speed of rotation. The electronics associated with the sensor calculates the amplitude of the vibration in the direction orthogonal to the direction of excitation whatever it is (known by hypothesis) by combining the information collected by the detection transducers acting along the X directions and Y. The sensor can operate in gyrometer mode: the natural vibration direction is kept fixed with respect to the sensor housing by modifying the excitation and the output information is then an image of the necessary energy that must be applied to the excitation transducers to maintain fixed natural vibration direction despite the movements of the housing. The sensor can also operate in gyroscope mode: the direction of the natural vibration is left free and is detected to give the angular orientation of the sensor. Constitution of the Transducers The constitutions of the transducers 15 associated with the inner and outer mobile masses will now be described. There are at least two excitation transducers associated with at least one of the two mobile masses (and preferably two transducers for each mobile mass), acting on this mass respectively in the direction X and in the direction Y. They will be called Ex and Ey. There are at least two detection transducers associated with at least one of the two mobile masses (and preferably two transducers for each mobile mass), detecting the movements of this mass in the X and Y directions and denoted Dx and Dy. There is also on at least one movable mass (and preferably on each of the two masses) at least one frequency adjustment transducer for each axis X and Y, denoted TX and Ty. They are capable of applying an electrostatic stiffness (variable with the electrical voltage) to the moving mass, a stiffness which for example compensates for mechanical stiffness inequalities of suspension springs possibly detected on the axes X and Y. Excitation and excitation transducers For good efficiency, the transducers are preferably made by interdigitated comb-gap electrodes.
    [0016] Each transducer comprises a pair of combs: there is a fixed comb PF whose teeth are integral with a fixed electrode EF of the machined plate and a mobile comb PM whose teeth, interdigitated with the teeth of the fixed comb, are integral with the moving mass associated with the transducer considered. The excitation consists in applying an alternating voltage between the moving comb and the fixed comb at the desired vibration frequency (mechanical resonance frequency of the suspended mobile mass). The generated motion is perpendicular to the teeth of the comb.
    [0017] The detection consists in applying a bias voltage between the fixed comb and the moving comb and in observing the load variations which result from the variations of capacity between the fixed comb and the movable comb due to variations in spacing between the teeth of the fixed comb. and mobile comb. The measured movement is the movement perpendicular to the teeth of the comb. For the detection and excitation transducers, the interdigitation of the combs is dissymmetrical at rest, the teeth of the mobile comb PM are offset with respect to the middle of the gap between two teeth of the fixed comb PF, as schematically represented in FIG. 6 for Ey or Dy transducers. Frequency Adjustment Transducer A frequency adjustment transducer is useful for the following reason: Due to the symmetry of the architecture according to the invention, by design, the different mass-spring systems of the system have very own frequencies relatives. However, manufacturing defects actually lead to a structure that is not perfectly symmetrical and orthotropic. This causes a degeneration of the useful mode in two orthogonal modes oriented along two orthogonal axes called principal axes of dynamic stiffness. The modal characteristics (mass and stiffness) of these two modes are then slightly different and the dynamic stiffness of the vibrating system varies according to the angular position of the vibration. The behavior of the system is no longer perfectly isotropic. It is therefore sought to compensate for these anisotropic defects of dynamic stiffness in the following manner: a compensation operation is carried out which consists first of all in orienting the vibration along the main axes of stiffness, then in measuring the frequency difference of resonance of the two modes, then equalize the resonance frequencies of each mode by means of an adjustable electrostatic stiffness. This electrostatic stiffness is delivered by frequency adjustment transducers ("frequency trimming") acting in the X and Y directions. When the compensation operation is performed, the orthogonal modes, which may be called excitation and detection mode, are identical, orthogonal and equal eigenfrequencies. The frequency adjustment transducers also make it possible to compensate for asymmetries of dynamic stiffness between the two branches of the tuning fork: the two branches of the resonator may exhibit differences in mass and stiffness due to the geometrical defects of embodiment. In the presence of these defects, the tuning fork movement is no longer perfectly balanced and makes the resonator slightly sensitive to its external environment. If electrostatic stiffness adjustment transducers are available on each of the two branches of the tuning fork in both X and Y directions, then it is possible to compensate for these dynamic stiffness asymmetries of the system. Fault compensation can be performed at the factory or in use provided that suitable electronic means are available, ie a possibility of zero interlocking of the differences between the frequencies. It is thus possible to compensate for the effects of temporal changes in the physical properties of the resonant system caused by aging or by thermomechanical effects. For the frequency adjustment transducers, consisting of a pair of interdigitated combs, the interdigitation of the combs is symmetrical at rest, i.e., the teeth of the moving comb PM are in the middle of the gap between two teeth of the fixed comb PF, as schematically shown in Figure 7 for a transducer Ty. Quadrature Bias Compensation Transducers To compensate for the dynamic stiffness anisotropy defects of the set of two vibrating masses, additional electrostatic transducers, referred to as quadrature bias compensation transducers, may be used. They allow to apply stiffness forces, tending to align exactly (in case of slight misalignment) the principal axes of dynamic stiffness of the moving assembly on the X and Y directions of the axes of symmetry of the assembly.
    [0018] They are used in the following manner, in combination with the frequency adjustment transducers: firstly, a precise alignment of the stiffness axes on the X and Y directions is measured, the frequency difference between the vibration frequencies is measured. of the two orthogonal modes, then equalizes the resonant frequencies of each mass by acting on the frequency adjustment transducers. When these compensation operations are performed, the orthogonal modes, which may be called excitation mode and detection mode, are identical, orthogonal and equal eigenfrequencies. Quadrature bias compensation transducers Q + and Q- are also interdigital comb transducers. FIG. 21 shows an example of transducers Q + and Q- having their comb electrodes arranged in direction Y. The interdigitation of the combs is asymmetrical at rest, the fingers of a half-comb not being exactly in the middle of the interval between two fingers of the other half-comb; we have at rest asymmetrical gaps e and Xe, where X is a real positive number. The stiffness terms created by one of the combs of such a transducer Q + are the following: stiffness in the X direction: kxq = 0 - stiffness in the Y direction: kyq n. £. V2 (1 + 7-1 .3) n. 2v e3 2 h) - coupling stiffness kxyq between the X axis and the Y axis: kxyq = e. 2 - - / 12 where the index q means that the term stiffness is caused by the compensation comb quadrature bias, N being the number of teeth per half-comb, h the thickness of the comb which is also that of the silicon wafer, I the overlap length, V the DC voltage between each comb and E the permittivity of the vacuum. In the example of FIG. 21, since the quadrature bias to be compensated may have any sign, there is provided another Q- comb, symmetrical of the Q + comb with respect to the axis of symmetry OX, to create a term of negative kxyq stiffness. It can be seen that the comb electrodes integral with the vibrating mass are symmetrical with respect to the axis of symmetry OY and with respect to the axis of symmetry OX, whereas the combs 10 integral with the fixed electrodes are symmetrical only with respect to OX. Depending on the sign of the quadrature bias to be compensated, either the positive quadrature bias offset transducers Q + receive an adjustable DC voltage VQ +, or the negative quadrature bias bias transducers Q- receive an adjustable DC voltage V0_. The electrostatic forces created by these voltages act to introduce a coupling stiffness kxyq between the movement of the mass along the X axis and the movement of the mass along the Y axis, the expression of which for all the comb electrodes shown in Figure 21 is: n. E. h (1, 2 e kxyq = -3 1 - VQ + 20 The values of the voltages VQ + and VQ- are adjusted to obtain a coupling stiffness kxyq which modifies the distribution of stiffness acting on the resonator so as to align exactly the principal axes of dynamic stiffness of the moving assembly on the axes of symmetry OX and OY of the assembly For a displacement Sy in the direction Y, the coupling stiffness force exerted in the direction X is Fxq = kxyq. This force changes sign with Sy and will therefore be of opposite sign for the internal vibrating mass and the external vibrating mass when these two masses are in motion according to the mode of useful vibration in opposition of phase. the quadrature bias compensation transducers will preferably be arranged on the internal vibrating mass and on the outer mass with interdigitation dissymmetries of combs of the same direction, both in the X direction and in the Y direction.
    [0019] On the other hand, in principle, the coupling stiffness is common to the two axes X and Y. It is therefore sufficient to have a pair of transducers Q + and Q- having a series of teeth aligned along one of the directions X or Y to compensate for positive quadrature bias and negative quadrature bias, respectively. Nevertheless, a positive action transducer and a negative action transducer arranged in such a way as to optimize the similarity between the distribution of the forces and the moving masses with respect to the axis of symmetry X are preferably provided in each X and Y direction. and with respect to the axis of symmetry Y, so as to improve the isotropy of the vibration in the XY plane. Configuration of the transducers with respect to the vibrating masses According to the invention, a configuration of the transducers is provided which is compatible with a resonator architecture without preferred axis, that is to say which does not disturb the isotropy of the vibration in all the XY plane directions. The configuration introduces the minimum of couplings and dissymmetries of mass, stiffness, or applied force, whatever the direction of the vibration, in order to disturb as little as possible the isotropy and the equilibrium of the resonant system. Firstly, for each electrostatic transducer, the axis of action or detection is oriented either in the direction X or in the direction Y and the teeth of the combs are configured to act or detect in one of these two directions that is, they are placed perpendicular to that direction. For this, one of the following two comb electrode configurations is used, for which the comb electrodes of an electrostatic transducer are symmetrically configured around their axis of action or detection. Each transducer is split into two pairs of interdigitated combs symmetrical with respect to the axis of action or X or Y detection, each pair comprising a fixed comb and a mobile comb. According to a first configuration, represented in FIG. 8, the two pairs are arranged symmetrically on either side of the vibrating mass, outside of it. The mobile combs PM are located outside the mass on two opposite sides thereof, and the fixed combs PF are located on either side of the moving combs, each secured to a respective fixed electrode EF.
    [0020] According to a second configuration, shown in FIG. 9, the two pairs of combs of the transducer are juxtaposed symmetrically inside an opening W formed in the moving mass. The two pairs, as well as a common fixed electrode EF, are thus surrounded by the moving mass. The first pair is located on one side of the fixed electrode, the second is located on the other side, symmetrical with respect to a straight line in the X or Y direction. This second configuration has the advantage of reducing the number fixed electrodes to be connected to the electronic circuit. With these symmetrical electrode configurations, a mass movement directed in the direction orthogonal to the direction of excitation or detection will not change the surface of the combs opposite, by differential effect. It will therefore be first order without parasitic effect on the response of the transducers. Thus, the transducers are insensitive to orthogonal movements to their direction of action or detection, which also makes them insensitive in this direction to static de-positionings induced for example by static accelerations or external stresses exerted on the sensor.
    [0021] The excitation transducers Ex, Ey apply static and dynamic electrostatic forces to the vibrating mass with which they are associated, respectively in the X and Y directions. On the other hand, the detection transducers Dx, Dy and the transducers frequency adjustment Tx, Ty (and also the bias compensation transducers Q + and Q- which will be discussed later) can be biased by a DC voltage and therefore are able to apply static forces on the vibrating mass to which they are associated. For each type of transducer and each X and Y direction, the combs are preferably made to be arranged symmetrically with respect to the axis of symmetry OX or OY of the suspended mass with which it is associated. By "symmetrically arranged combs" is meant that the arrangement of the movable comb teeth is symmetrical with respect to OX or OY. Due to the asymmetrical interdigitation of the combs of the excitation and detection transducers (and also the bias compensation transducers Q), this may lead to placing the fixed combs slightly asymmetrically, which is not a problem. In practice, this characteristic leads either to center a single transducer on an OX or OY axis of symmetry of the moving masses, or to split the transducer into two half-transducers arranged symmetrically with respect to this axis of symmetry OX or OY. The resultant of the forces applied by the transducers passes through the center of inertia O of the suspended mass, which makes it possible not to excite the parasitic modes with rotational movements; and the geometry of the moving combs thus produced makes it possible to limit as much as possible the imbalances of the mass around the axes of symmetry X and Y. Geographical organization with respect to the axes of symmetry Preferably, according to the invention, for each mobile mass, the The geographical arrangement with respect to the axis of symmetry OX of the transducers of the different types operating in the X direction (excitation or detection, but preferably also frequency adjustment and quadrature bias compensation) is the same as the arrangement around the X axis. OY axis of symmetry of the transducers working in the Y direction; and reciprocally the arrangement with respect to the axis of symmetry OX of the transducers working in the Y direction is the same as the arrangement with respect to the axis OY of the transducers working in the direction X. FIG. 10 shows such a configuration for the inner moving mass M1. There are: two transducers Ex of excitation of a movement in the direction X, arranged symmetrically with respect to the axis of general symmetry OX of the mass, two transducers Ey of excitation of a movement according to the direction Y, arranged symmetrically with respect to the general axis of symmetry OY of the mass, two transducers Dx for detecting a movement in the X direction, arranged symmetrically with respect to the general axis of symmetry OX of the mass, two transducers Dy for detecting a movement in the Y direction, arranged symmetrically with respect to the general axis of symmetry Y of the mass; two transducers Tx of frequency adjustment (with symmetrical interdigitation) arranged symmetrically with respect to the axis OX, acting in the X direction, and also centered on the axis OY, - two frequency adjusting transducers (symmetrical interdigitation) acting in the Y direction, arranged symmetrically relative to the axis OY and also centered on the axis OX. Only the transducers Tx and Ty have a symmetrical interdigitation at rest. The others are all asymmetrical interdigitation at rest. These transducers are all arranged outside the mobile mass. The configuration could be the same for the external mobile mass M2 not shown in FIG. 10. FIG. 11 represents another general configuration of the internal mobile mass M1. In this configuration, all the transducers 25 are placed in openings of the mass and not at the periphery thereof. They can be placed in this case all on the axis of symmetry OX or OY respectively. This example also makes it possible to show a peculiarity of possible minor exception to the general mechanical symmetry of the moving mass with respect to the axis OX and the axis OY: in fact, there is only one transducer. excitation acting in the direction X and an excitation transducer acting in the direction Y. The transducer Ex in the direction X is placed symmetrically on the axis OX. But he is not on the OY axis. The Ey transducer acting in the Y direction is placed symmetrically on the OY axis, but it can not be on the OX axis as well. Consequently, instead of constituting the mechanical symmetry of the moving assembly by using two transducers Ex placed symmetrically with respect to the axis OY, the transducer Tx is placed in the symmetrical position of the transducer Ex; in the same way, the transducer Ty is placed in the symmetrical position of the transducer Ey. If these transducers have exactly the same number of movable comb teeth and the same tooth dimensions and tooth intervals, then the symmetry of the moving assembly is 100% respected. But if there are differences, the overall symmetry remains respected but not quite 100%. It is possible, for example, for the transducer Tx to have a number of movable comb teeth different from that of the transducer Ex. These teeth are symmetric and not asymmetrical interdigitation; they may therefore be closer together and may be more numerous for this reason. If this results in an additional mass on the right side (the transducer Tx is on the right side), it may create an unbalance on the right side and we can compensate for this unbalance by making a small additional opening h in the moving mass near the transducer Tx without providing such an opening near the transducer Ex. This is shown in Figure 11. The same is true for the symmetry between the transducer Ty and the transducer Ey. Devices having this type of minor symmetry difference are within the scope of the present invention. It will be noted that it is possible to envisage configurations of transducers, some of which are placed in openings of the mass and others are placed at the periphery of the mass, the latter then being arranged symmetrically with respect to the axis of symmetry OX or OY which is parallel to their direction of action X or Y. In all cases, it is preferably provided that the arrangement of the transducers distributed around the axis of symmetry OX is similar to the arrangement of the transducers distributed around the axis OY. Thus, for example in FIG. 10, there are around the axis OX two transducers Ty centered on the axis OX, on either side of the mass, a transducer Dy and a transducer Ey on either side. a transducer Ty, and the same thing on either side of the other transducer Ty, and three transducers Ex, Tx, Dx disposed on each side of the mass symmetrically with respect to the axis OX; conversely, one finds around the axis OY with exactly the same distribution: two transducers Tx centered on the axis OY, on either side of the mass, a transducer Dx and an transducer Ex on both sides of the a transducer Tx, and the same thing on either side of the other transducer Tx, and three transducers Ey, Ty, Dy disposed on each side of the mass symmetrically with respect to the axis OY. For FIG. 11, it is the same thing: with respect to the axis OX, one finds successively on the axis OX a transducer Dx, an transducer Ex, a transducer Tx, a transducer Dx; conversely, one finds on the axis OY successively and with exactly the same arrangement a transducer Dy, a transducer Ey, a transducer Ty, a transducer Dy. Quadrature bias compensation transducers To compensate for the quadrature bias, which results from the fact that the excitation and detection directions are not aligned with the principal axes of dynamic stiffness, excitation and detection directions could be selected. oriented along the main axes of dynamic stiffness (which may be slightly misaligned relative to the axes of symmetry OX and OY before compensation), acting simultaneously on the transducers of the X and Y axes. But such a solution complicates the control electronics of the gyrometer because the reference in which the electronic control of the vibration modes defined by the X and Y axes of sensitivity or action of the transducers is made does not coincide with that of the modes of vibration defined by the principal axes of dynamic stiffness. A preferable solution is to rotate the mark defined by the main axes of dynamic stiffness so as to align with the X and Y axis mark in which the electronic control is done. The architecture according to the invention is compatible with such a solution. For this purpose, at least one pair of electrostatic transducers is added to interdigitated interdigitated interdigitating combs Q + and Q- capable of applying adjustable electrostatic coupling stiffnesses between the movements along X and along Y of the mass with which they are associated respectively. to compensate for positive quadrature bias and to compensate for negative quadrature bias. The design of the electrodes of the transducers Q + and Q- is therefore made in such a way as to respect the characteristics of geometric symmetry of the moving masses with respect to the axis OX and with respect to the axis OY. The quadrature bias compensation method by electrostatic stiffness can be realized during a step of adjusting the gyrometer at the end of manufacture, so as to correct the bias in intrinsic quadrature. It is also possible to apply this method continuously, by setting up in the electronic circuit a zero control of the quadrature bias, which makes it possible to compensate for the effects of temporal changes in the physical properties of the resonant system caused by aging or by thermomechanical effects. The quadrature bias compensation operation will preferably be performed for each of the gyrometer masses independently, i.e., each of the vibrating masses will have at least one pair of Q + and Q- transducers. The interdigitation of the combs of the transducer Q + is such that the application of a control voltage introduces a coupling stiffness kxyq between the movement of the mass along the axis X and the movement of the mass along the axis Y, then that for the same voltage, the interdigitation of the combs of the transducer Q- applies a coupling stiffness of opposite sign. In principle, the coupling stiffness is common to the two X and Y axes, it is therefore sufficient to have a pair of Q + and Q- transducers acting in one of the X or Y directions in order to be able to compensate for the bias in quadrature by For example, as illustrated in FIG. 12. In FIG. 12, the two compensation transducers Q + and Q-have comb electrodes arranged in the direction Y. They act in the direction Y for a displacement in the direction X and vice versa. in the direction X for a displacement in the direction Y. They are here placed in an opening of the mass. Nevertheless, in this case the moving electrodes of the transducers Q + and Q- can introduce a difference in the distribution of the mass around the axis of symmetry X, with respect to the distribution of the mass around the axis of symmetry Y, which reduces the isotropy of the vibration in the XY plane.
    [0022] To optimize the symmetry of the architecture and thus its equilibrium by construction, according to the invention, the similarity of the arrangement of the Q + and Q- electrodes between the two axes of symmetry is optimized by one of the following configurations: As indicated on FIG. 13 shows two symmetrical pairs of transducers Q + and Q- (with however an inversion of the asymmetry of the interdigitations of combs) arranged in the direction X and two other pairs of transducers Q + and Q- arranged in the direction Y (where other types of electrodes are not shown). The Q + transducer combs arranged in the X and Y directions simultaneously compensate for positive quadrature bias, while the X- and Y-direction Q- transducer combs simultaneously compensate for negative quadrature bias.
    [0023] Alternatively, it is possible, as in the example of FIG. 14, to arrange the electrodes Q + along an axis of symmetry of the vibrating mass (one on each side of the vibrating mass) and the electrodes Q- according to the other axis of symmetry of the vibrating mass, the Q + transducers then being arranged in a direction perpendicular to the Q- transducers.
    [0024] It is also possible to adopt a similar configuration, but inside the mass and not at the periphery, as for example illustrated in FIG.
    [0025] FIG. 16 represents an example of a complete configuration in which only the internal mobile mass comprises transducers, the external mobile mass M2 having none. In this example, all the transducers are placed in openings of the moving mass. The excitation transducers Ex, Ey and detection Dx, Dy are constituted as in Figure 9 (double fixed comb associated with the same fixed electrode); the frequency adjustment transducers are constituted as in FIG. 11 (possibly with a compensating opening); the bias compensation transducers are of the type shown in FIG. 15, and there are four of them in this example, arranged symmetrically (a symmetric Q + transducer of a Q- transducer) with respect to the axis OX and also relative to to the OY axis to ensure overall mechanical symmetry of the assembly; the frequency adjustment transducers are placed as in FIG. 11, that is to say that they form the counterpart of Ex and Ey excitation transducers and that they are possibly associated with a small compensation aperture of unbalance in the case where their moving combs are not exactly the same as the moving excitation combs. Finally, the suspension and coupling springs are arranged in this example as in FIG. 3. FIG. 17 shows another example of a complete configuration in which the two mobile masses are provided with transducers and in particular each has at least one transducer. an excitation transducer, a detection transducer, a frequency adjustment transducer. The number 1 is assigned to the transducers of the internal mass M1, the number 2 is assigned to the transducers of the external mass M2. In this example, the two masses also each have at least one bias compensation transducer. For the internal mass, the same arrangement as in FIG. 16 has been chosen here. The transducers of the two masses are placed here in openings of each of the masses. The fact of placing transducers on each of the masses has the following advantages: it is possible to compensate the dissymmetry of dynamic stiffness between the two branches of the tuning fork; Moreover, the excitation and detection transducers that are less sensitive to the static changes common to the two masses (for example a de-positioning according to their direction of action under the effect of an acceleration) are rendered more differential by differential effect; the excitation by the excitation transducers and the detection by the detection transducers is more efficient since the cumulative surface area of the comb teeth facing these transducers is roughly doubled if the combs are identical on the two masses. Preferably, the number of moving comb teeth of each type of transducer (E, or D, or T or Q) is identical on the two masses so as to optimize by construction the equilibrium between the two moving assemblies (masses with mobile combs that are attached to it).
    [0026] However, the number of transducers of each type may be different between the two masses; for example we see in Figure 17 that there are two detection transducers Dx1 on the first mass, placed on the axis OX and arranged symmetrically on either side of the axis OY, while each of the two transducers detecting Dx2 of the second mass is split into two separate transducers arranged two by two symmetrically with respect to the axis OX and symmetrically with respect to the axis OY; each Dx2 transducer has two times less moving comb teeth than a Dx1 transducer.
    [0027] It will be noted that the excitation and detection transducers with asymmetrical interdigitation of the first mass preferably have a direction of dissymmetry inverted with respect to the direction of dissymmetry of those of the first mass (see for example the detail view of Ey1 and Ey2 in FIG. 17), to take better account of the fact that the useful vibration mode is in phase opposition on the two masses. When there is a static dislocation of the masses (induced for example by static accelerations or stresses outside the sensor), the air gap of these comb teeth is reduced for one mass while it increases for the other. , but the overall efficiency of the excitation transducers and detection remains the same. This results in insensitivity to the first order with respect to these static de-positions common to both masses. Note also in Figure 17 that it can be provided if necessary openings Oa adjustment in one of the masses, here the outer mass, to balance the value of the two masses.
    [0028] FIG. 18 represents a configuration in which the transducers associated with the external mass are placed at the periphery thereof. They could also be placed on the inner edge of the mass or shared between the inner edge and the outer edge, or shared between the edges and openings of the mass. Furthermore, in the example of FIG. 18, it can be noted that the excitation transducers Ex1 or Ey1 of the internal mass have been split and thus also the adjustment transducers Tx1 or Ty1 which are opposite each other. transducers Ex1 or Ey1 by symmetry, and that separate apertures h have been provided for the compensation of the excess mass of the frequency adjusting transducers Tx1 and Ty1. These features could be adopted in any global sensor configuration.
    [0029] FIG. 19 shows a further possibility of grouping the fixed electrodes of the excitation transducers of the two mobile masses, these electrodes thus having a fixed comb having comb teeth turned towards the internal mass and another fixed comb. having teeth turned towards the outer mass, the two masses having movable comb teeth interdigitated respectively with these two fixed combs. Here again it is provided that the gap asymmetry at rest between the fixed teeth and the movable teeth is reversed between the internal mass and the external mass as shown by the detail of the Ex or Ey transducer of FIG. 19 so that the excitation produced by an alternating voltage applied to the fixed electrode of the Ex or Ey transducer causes an excitation movement in phase opposition on the two masses. The same arrangement is exactly adopted for the detection transducers, with also an opposite interdigitation dissymmetry on the two masses, as shown by the detail of the transducer Dx or Dy of FIG. 19. It will also be noted that in FIG. 19, contrary to FIG. 18, it is not a transducer Tx which is the counterpart of an Ex transducer, but it is indeed another Ex transducer.
    [0030] FIG. 20 again shows an example in which the symmetry of arrangement of the masses and the transducers is further improved with respect to the axis OX and the axis OY, in that all the transducers acting in the direction of an axis of symmetry have an identical half disposed symmetrically with respect to the other axis of symmetry. Thus, there are four detection transducers Dx on each mass symmetrical two by two with respect to OX and with respect to OY; similarly (with the same symmetry) four transducers Dy on each mass symmetrical two by two with respect to OX and with respect to OY; two excitation transducers Ex on each mass placed on the axis OX with symmetry with respect to this axis and two excitation transducers Ey on each mass with a similar symmetrical disposition but with respect to the axis OY; two frequency adjustment transducers Tx on each mass, placed on the axis OY with a symmetry with respect to this axis; two frequency adjustment transducers Ty of each mass with the same symmetrical disposition but with respect to the axis OX. The quadrature bias compensation transducers are eight in number on each mass: a Q + transducer is symmetrical with respect to the OX axis of another Q + transducer but with a reversal of the asymmetry of the interdigitations of the combs; a Q + transducer is symmetrical with respect to the axis OY of another transducer Q +, with also a reversal of the asymmetry of the interdigitations of the comb. In addition, a Q-transducer arranged in the direction X (or respectively Y) is symmetrical with respect to the axis OY (or respectively OX) of a transducer Q + disposed in the same direction X (or respectively Y). We recall here, and we see in this figure, or in other figures, for example Figure 14, that in the case of transducers that are of the asymmetrical type at rest, ie the transducers Ex and Ey, Dx and Dy or Q + and Q-, the symmetry of the interdigitated comb pairs arranged symmetrically with respect to one of the axes OX or OY is strictly true only for the mobile electrode part. Thus a structure according to the invention is "generally symmetrical" along the axes OX and OY, as has been described throughout the description, which covers possible minor dissymmetries, such as those just described. in the previous paragraph, and also openings in one or two of the masses to compensate for mass unbalance around the axes of symmetry X and Y, so that the center of gravity coincides with the center of symmetry of the structure .
    权利要求:
    Claims (13)
    [0001]
    REVENDICATIONS1. Micro-machined inertial angular sensor comprising - two vibrating masses (M1, M2), machined in a generally flat support plate, movable with respect to the plate and movable relative to each other, suspended at points fixed anchoring (A) of the plate by suspension springs (RS) and coupled together by coupling springs (RC) for vibrating in phase opposition, characterized in that the sensor comprises: - at least one transducer (Ex ) of excitation of a vibration movement of one of the masses in a direction X in the plane of the plate, a transducer (Ey) for excitation of this mass in a direction Y perpendicular to the direction X and in the plane of the plate, a transducer (Dx) for detecting a vibration of one of the masses in the X direction and a transducer (Dy) for detecting a vibration of one of the masses in the Y direction, and in that the two mobile vibrating masses are arranged one around the other, in an internal mass (M1) and an external mass (M2), and their centers of gravity (0) are merged at rest, - the coupling springs (RC) are each connected on one side to the internal mass and the other than the external mass, - the stiffness of the suspension springs of the internal mass and the stiffness of the suspension springs of the external mass are proportional to the values of the respective masses, - the moving assembly consisting of a vibrating mass and the parts of integral transducers of this mass has a generally symmetrical structure with respect to an axis of symmetry OX parallel to the X direction and passing through the center of gravity of the mass, and also generally symmetrical with respect to an axis of symmetry OY parallel to the direction Y and passing through the center of gravity of the mass.
    [0002]
    2. Sensor according to claim 1, characterized in that the stiffness of the coupling springs are identical in the X direction and in the Y direction, and the stiffness of the suspension springs of the internal mass are identical in the direction X and in the direction Y, and the stiffnesses of the suspension springs of the external mass are identical in the direction X and in the direction Y.
    [0003]
    3. Sensor according to claim 2, characterized in that the internal mass is equal to the external mass, and the stiffness of the suspension springs of the inner mass is equal to the stiffness of the suspension springs of the external mass.
    [0004]
    An angular sensor according to any one of claims 1 to 3, wherein the excitation (Ex, Ey) and detection transducers (Dx, Dy) each comprise a pair of interdigitated combs comprising a mobile comb formed of a row of teeth integral with the vibrating mass and a fixed comb formed of a row of teeth integral with a fixed electrode, the interdigitation of the teeth at rest being asymmetrical, characterized in that it further comprises at least a first transducer electrostatic frequency adjustment device (Tx), in interdigitated interdigitated interdigitated combs at rest, capable of applying an adjustable electrostatic stiffness to the vibrating mass in the X direction, and a second frequency adjustment transducer (Ty) similar to the first and capable of applying to the vibrating mass an adjustable electrostatic stiffness in the Y direction.
    [0005]
    5. Sensor according to claim 4, characterized in that the geographical arrangement with respect to the axis of symmetry OX excitation and detection transducers, frequency adjustment transducers, and other potential transducers such as quadrature bias compensation transducers, working in the X direction is identical to the arrangement with respect to the axis of symmetry OY of the transducers performing the same functions but working in the Y direction.
    [0006]
    6. A sensor according to claim 5, characterized in that excitation (Ex1, Ey1), detection (Dx1, Dy1), and optionally frequency adjustment (Tx1, Ty1) or other transducers are associated with the internal vibratory mass (M1) and other excitation transducers (Ex2, Ey2), detection transducers (Dx2, Ey2), and optionally frequency adjustment transducers (Tx2, Ty2) or others are associated with the external vibrating mass ( M2).
    [0007]
    7. Sensor according to claim 6, characterized in that the number of comb teeth of each type of transducer is identical on the inner mass and on the external mass.
    [0008]
    8. A sensor according to claim 5 or claim 6, characterized in that two excitation or detection transducers acting on the inner mass and on the outer mass in the same direction X or Y have interdigitation dissymmetries of opposite direction. .
    [0009]
    9. Sensor according to any one of claims 5 to 8, characterized in that the general configuration of the set of moving masses, and mobile combs associated with these masses is generally symmetrical with respect to the axis of symmetry OX and also with respect to the axis of symmetry OY, preferably in a symmetry of order 4, ie an invariance of the configuration when the assembly is rotated by 90 ° around the axis OZ , and this with the possible exception of minor dissymmetries due directly or indirectly to the fact that the frequency adjustment transducers are symmetrical at rest interdigitation unlike other transducers.
    [0010]
    10. Sensor according to any one of claims 6 to 9, characterized in that each excitation transducer or detection has a common electrode secured to two fixed tooth combs, the internal vibrating mass and the external vibrating mass each having a respective moving comb cooperating with one of the two fixed combs.
    [0011]
    11. A sensor according to any one of claims 4 to 10, characterized in that a transducer associated with a vibrating mass for excitation or detection in a direction X or Y comprises two pairs of interdigital combs arranged symmetrically with respect to the direction of excitation or X or Y detection, with one of the following configurations: the transducer is divided into two distinct transducers placed symmetrically on either side of the vibrating mass and having their movable combs placed symmetrically on the one hand; and other of the vibrating mass, and the fixed combs being arranged symmetrically on either side of the mass, - or the teeth of the mobile combs are located symmetrically on either side of an electrode fixed to the The interior of an opening of the vibrating mass, the latter surrounding the pair of combs and the fixed electrode.
    [0012]
    12. Sensor according to any one of the preceding claims, characterized in that at least one of the vibrating masses is coupled to at least one electrostatic compensation transducer of a quadrature bias (Q +, Q-), making it possible to modify the distribution of the stiffness acting on the vibrating mass so as to align the principal axes of dynamic stiffness on the axes of symmetry OX and OY. 20
    [0013]
    13. A sensor according to claim 12, characterized in that the electrostatic quadrature bias compensation transducer or transducers are arranged according to one of the following provisions: a pair of transducers acting in positive bias compensation and in negative bias compensation in the X direction and another pair acting in positive bias compensation and negative bias compensation in the Y direction, - a pair of positive and negative transducers respectively, these transducers having double combs having teeth oriented according to the X direction. the two directions X and Y, a positive bias compensation transducer acting in one of the X and Y directions, and a negative bias compensation transducer acting in the other direction orthogonal to the first direction.
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    同族专利:
    公开号 | 公开日
    US9574879B2|2017-02-21|
    US20150377621A1|2015-12-31|
    FR3022996B1|2017-12-01|
    EP2960625B1|2018-11-14|
    EP2960625A1|2015-12-30|
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    CN108225295B|2017-12-11|2021-01-05|东南大学|Three-axis micro gyroscope based on tuning fork driving effect|
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    JPWO2020203011A1|2019-03-29|2020-10-08|
    FR3112850A1|2020-07-24|2022-01-28|Thales|METHOD FOR CALIBRATION OF A VIBRATING INERTIAL SENSOR|
    法律状态:
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    2016-01-01| PLSC| Publication of the preliminary search report|Effective date: 20160101 |
    2016-05-26| PLFP| Fee payment|Year of fee payment: 3 |
    2017-05-30| PLFP| Fee payment|Year of fee payment: 4 |
    2018-05-29| PLFP| Fee payment|Year of fee payment: 5 |
    2019-06-03| PLFP| Fee payment|Year of fee payment: 6 |
    2021-03-12| ST| Notification of lapse|Effective date: 20210205 |
    优先权:
    申请号 | 申请日 | 专利标题
    FR1401451A|FR3022996B1|2014-06-27|2014-06-27|ANGULAR INERTIAL MEMS SENSOR OPERATING IN DIAPASON MODE|FR1401451A| FR3022996B1|2014-06-27|2014-06-27|ANGULAR INERTIAL MEMS SENSOR OPERATING IN DIAPASON MODE|
    EP15173393.8A| EP2960625B1|2014-06-27|2015-06-23|Mems angular inertial sensor in tuning fork mode|
    US14/750,862| US9574879B2|2014-06-27|2015-06-25|MEMS angular inertial sensor operating in tuning fork mode|
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