Hemispherical resonator gyroscope X/Y path driving gain asymmetry and electrode non-orthogonal error identification method
A hemispherical resonant gyro, gain asymmetry technology, applied in gyroscope/steering sensing equipment, gyro effect for speed measurement, speed/acceleration/shock measurement, etc., can solve hemispherical resonant gyroscope X/Y channel drive gain asymmetry, Error, standing wave azimuth drift control loop and other problems, to solve the standing wave azimuth drift and control loop error, improve the effect of performance
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specific Embodiment approach 1
[0036] Embodiment 1: A hemispherical resonant gyro X / Y channel drive gain asymmetry and electrode non-orthogonal error identification method of this embodiment, the specific process of the method is:
[0037] Step 1. Calculate the precession velocity ω according to the azimuth angle θ of the standing wave and the vibration amplitude A r ; The specific process is:
[0038]
[0039] Among them, F x , F y are the electrostatic forces applied to the x and y-axis electrodes, respectively, when k x ≠k y And the declination angle of the y-axis electrode and the orthogonal direction of the x-axis is when, F x , F y The expression is:
[0040]
[0041] where k x , k y are the gain coefficients of the x and y-axis drive circuits, respectively, G is the kinematic model of the harmonic oscillator, ω 0 is the given precession speed;
[0042] Step 2. Define H=k 0 Gω 0 , k 0 is the ideal x, y axis drive circuit gain coefficient;
[0043] And given the initial value k(0)...
specific Embodiment approach 2
[0058] Embodiment 2. The difference between this embodiment and Embodiment 1 is that the Jacobian matrix J r The expression for (i) is:
[0059]
[0060] Other steps and parameters are the same as in the first embodiment.
specific Embodiment approach 3
[0061] Embodiment 3. The difference between this embodiment and Embodiment 1 or 2 is that: according to the Jacobian matrix J r (i) Calculate the increment of the drive gain asymmetry coefficient k and the non-orthogonal declination angle of the electrodes at time i The increment of and the increment of H, which are:
[0062]
[0063] Among them, Δk(i) is the increment of the drive gain asymmetry coefficient k at time i, is the electrode non-orthogonal declination angle The increment at time i, ΔH(i) is the increment of H at time i, the superscript T represents the transpose of the matrix, and the superscript -1 represents the inverse of the matrix.
[0064] Other steps and parameters are the same as in the first or second embodiment.
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