Method for acquiring vibration mode angle of hemispherical resonator gyroscope in case of inconsistent forward amplification coefficients
A hemispherical resonant gyro and forward amplification technology, applied in the inertial field, can solve the problems that the hemispherical resonant gyroscope cannot accurately measure the angle of the carrier and reduce the accuracy of navigation, so as to improve the accuracy of navigation and realize high-precision angle measurement. high effect
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specific Embodiment approach 1
[0023] Specific implementation mode one: combine figure 1 This embodiment is described. In this embodiment, a hemispherical resonator gyroscope mode angle acquisition method when the forward amplification coefficients are inconsistent is as follows:
[0024] The purpose of the present invention is to provide a method for obtaining the mode angle of the hemispherical resonator gyroscope when the forward amplification coefficients are inconsistent, and to propose an improved angle measurement method for the problem of angle measurement errors when the forward amplification coefficients of the hemispherical resonant gyroscope detection circuit are not equal. Formula, based on this formula, an extended Kalman filter is established. While rotating the gyroscope, the vibration signals collected by the 0° and 45° electrodes are demodulated, low-pass filtered, etc., and the obtained signals E, R, and S are used as extended The input of the Kalman filter realizes the identification of ...
specific Embodiment approach 2
[0033] Embodiment 2: The difference between this embodiment and Embodiment 1 is that in the step 2, the excitation electrodes are arranged on the hemispherical resonant gyroscope at intervals. Such as Figure 4 shown.
[0034] Other steps and parameters are the same as those in Embodiment 1.
specific Embodiment approach 3
[0035] Specific embodiment three: the difference between this embodiment and specific embodiment one or two is that the reference signal v generated by the phase-locked loop is used in the step 4 rc , v rs Demodulate the detected vibration signals x and y respectively to obtain signals Cx, Sx, Cy and Sy, respectively perform low-pass filtering on the signals Cx, Sx, Cy and Sy to obtain signals Cx', Sx', Cy' and Sy ', and then combine the signals Cx', Sx', Cy', and Sy' twice to obtain E, R, and S signals; the specific process is:
[0036] The reference signal v generated by the phase-locked loop rc , v rs The detected vibration signals x and y are respectively demodulated to obtain signals Cx, Sx, Cy and Sy. The expressions are:
[0037]
[0038]The signals Cx, Sx, Cy, and Sy are low-pass filtered to filter out the double frequency in the signals Cx, Sx, Cy, and Sy respectively, and the signals Cx', Sx', Cy', and Sy' are obtained;
[0039] The signals Cx', Sx', Cy', Sy' ...
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