Method for acquiring vibration mode angle of hemispherical resonator gyroscope with electrode angle error
A technology of hemispherical resonant gyroscope and acquisition method, which is applied in the field of inertia, can solve the problems that hemispherical resonant gyroscopes cannot achieve accurate angle measurement and low accuracy, and achieve the effects of improving navigation accuracy, improving measurement accuracy, and improving angle measurement accuracy
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specific Embodiment approach 1
[0021] Specific implementation mode one: combine figure 1 Describe this embodiment. In this embodiment, a method for obtaining the mode angle of a hemispherical resonator gyro when there is an error in the electrode angle is as follows:
[0022] The invention proposes a method for acquiring the mode angle of a hemispherical resonator gyro when there is an error in the electrode angle. The method is based on an improved angle measurement equation and uses a nonlinear least square to identify. The method obtains the precise angle measurement formula by identifying the electrode angle error, thereby calculating the precise mode angle of the harmonic oscillator, and realizing the high-precision angle measurement of the gyroscope. The present invention can also realize the identification of the electrode angle error by expanding nonlinear identification algorithms such as Kalman filter.
[0023] Step 1, install and fix the hemispherical resonant gyro on the turntable so that the...
specific Embodiment approach 2
[0031] 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.
[0032] Other steps and parameters are the same as those in Embodiment 1.
specific Embodiment approach 3
[0033] 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:
[0034] 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:
[0035]
[0036] 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;
[0037] The signals Cx', Sx', Cy', Sy'...
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