A novel narrow-band force rebalance control method for the sense mode of MEMS vibratory gyroscopes
Graphical abstract
Force rebalance control schematic for the sense.
Introduction
MEMS vibratory gyroscopes are widely used in various fields such as automotive industry, consumer electronics and navigation systems owing to their merits of low power, low cost and so on, which makes it significant to further advance the performances [1], [2]. Closed loop control for the sense mode can adjust the bandwidth, improve the nonlinearity, extend the measure range and so on, so that it is widely applied in the high-performance gyroscopes. Band-pass and low-pass sigma-delta modulator loops are widely used to realize the force feedback control [3], [4], [5], [6], [7], [8], but the robustness and stability are still problems since the signal–noise-ratio and stability may decrease due to the nonlinearity of the quantizer as the input amplitude increases [9], [10]. Adaptive controller and the adaptive laws based on a Lyapunov approach can be applied to closed loop control of the two modes [11], [12], [13]. However, bandwidth and non-smooth time-varying signals following performance are difficult issues to be solved. Automatic gain control (AGC) method can be utilized to set the vibration amplitude of the sense mode to a certain value according to Refs. [14], [15], but the input force cannot be balanced completely.
On the other hand, there are some closed loop control methods based on demodulation and modulation [16], [17], [18], [19], [20], [21], that is to say, two similar closed loops can be applied to balance the Coriolis force and quadrature force, respectively, due to demodulation and modulation. These methods are proved effective, but still a little complex because the signals’ phases should be control precisely in the demodulation and modulation components. Therefore, in this work, a simple and novel closed loop control method for the sense mode will be proposed after making a comparison and combination of the control methods above. There is no demodulation and modulation components in the control loop and the Coriolis force and quadrature force are balanced together in the same loop. Detailed theoretical analysis and experimental tests will be conducted in the following sections.
Section snippets
Theoretical analysis
The simplified schematic of a Z-axis doubly decoupled MEMS tuning fork gyroscope is shown in Fig. 1, and the design aims to make a gyroscope achieve a sub 10 deg/h bias instability, as well as a bandwidth larger than 90 Hz. The two groups of combs, namely slide-film drive combs and slide-film drive-sensing combs, are used for closed loop control of the drive mode. Similarly, another two groups of combs, namely squeeze-film sense combs and slide-film force feedback combs, are applied to closed
Simulation analysis
For the sake of comparison, the MEMS gyroscope applied to this research is identical to that used in literature [21], the key parameters of the gyroscope are depicted in Table 1. Qd represents the quality factor of the drive mode. Thus, the frequency responses of D(s), T(s), S(s) and Tr(s) can be simulated by Matlab with theoretical Eqs. (1), (2), (3), (4), (5), (6), (7), (8), (9), (10) in f domain and fr domain, respectively, as shown in Fig. 5, Fig. 6, Fig. 7. The expected control goals are
Experimental tests
After tuning with simulation by Matlab, the relevant parameters of the control loop can be confirmed finally, and the theoretical control schematic can be converted to a practical circuit, as shown in Fig. 8. The circuit mainly comprises a vacuum sealed gyroscope, a closed loop for the drive mode and a closed loop for the sense mode. Fig. 9 illustrates the typical differential force-generating circuit and the circuit of HPF and BPF, which are simple to be realized.
The test circuit is mounted on
Conclusion
This work presents a novel closed loop control method for the sense mode of a MEMS gyroscope. There is no demodulation and modulation components in the control loop, and the Coriolis force and quadrature force are rebalanced simultaneously in only one control loop. Moreover, a band pass filter is adopted as a controller to accomplish the feedback control, which simplifies the closed loop system much. Detailed theoretical analyses are performed to acquire the frequency response models of the
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