Gas Damping Coefficient Research for the Mems Comb Linear Vibration Gyroscope

Silicon-MEMS gyroscope is an important part of MEMS ( Micro Electrical Mechanical System). There are some disturb ignored in traditional gyroscope that must be evaluated newly because of its smaller size (reach the level of micron). In these disturb, the air pressure largely influences the performance of the MEMS gyroscope. Different air pressure causes different gas damping coefficient for the MEMS comb linear vibration gyroscope and different gas damping coefficient influences the quality factor of the gyroscope directive. The quality factor influences the dynamic working bandwidth of the MEMS comb linear vibration gyroscope, so it is influences the output characteristic of the MEMS comb linear vibration gyroscope. The paper shows the relationship between the air pressure and the output amplified and phase of the detecting axis through analyzing the air pressure influence on the MEMS comb linear vibration gyroscope. It discusses the influence on the distributive frequency and quality factor of the MEMS comb linear vibration gyroscope for different air pressure. 1. BASIC STRUCTURE OF THE MEMS COMB LINEAR VIBRATION GYROSCOPE Fig. 1 is the sketch of the MEMS comb linear vibration gyroscope. It mainly consists of two side drivers, one mass, damper including springs that jointed the moving mass and static spring, and datum seat. There are some fixed combs in drivers and some moving combs in masses. The two side drivers are fixed on datum seat. The moving mass is jointed with datum seat by flexible springs. The mass are only moved linearly in the direction of x-axis and y-axis due to the action of flexible supports and springs. Fig. 1 Sketch of the MEMS comb linear vibration gyroscope It has periodical electrostatic force between the fixed combs and the moving combs in the direction of x-axis when the moving combs on detecting mass is jointed the ground and a alternating current with direct current excursion is added on the fixed combs on two side drivers. So the detecting mass is vibrated in line periodically between the two side drivers. Here, if the body is tuned round y-axis, the detecting mass is vibrated in line in the direction plumbed the datum seat (i.e. the direction of zaxis). Because it has sensitivity electrode under the detecting mass, the sensitivity capacitance is changed due to the linear vibration of the detecting mass in the direction of zaxis. The changing quantity of the capacitance is in proportion to the input angle rate (i.e. the angle rate of the body is tuned round y-axis). Then we can get the input angle rate when we detect the changing quantity of the sensitivity capacitance. 2. MOVING MODULE OF THE MEMS COMB LINEAR VIBRATION GYROSCOPE We assume that the angle rate of the body tuned round yaxis is IGy ω . The linear vibrated speed of the moving mass in the direction of x-axis is ) (t v . Then the Coriolis force acceleration generated in the direction of z-axis is ) ( 2 t v a IGy z ω = (2.1) The corresponding rate is ) ( ) ( 2 ) ( 2 t x dt t v v y IG IGy z ω ω ∫ = = (2.2) Then the movement equation of the moving mass in the direction of z-axis is ©EDA Publishing/DTIP 2007 ISBN: 978-2-35500-000-3 ha l-0 02 57 69 7, v er si on 1 20 F eb 2 00 8 Author manuscript, published in "DTIP 2007, Stresa, lago Maggiore : Italy (2007)"