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26) 2 MASH Digital Delta–Sigma Modulator with Multi-Moduli 19 In practice, the input DC X is set as 0 < X < M1 . 27) 1 where 1 is the greatest common divisor of M1 and X . If M1 and X are co-prime numbers, 1 equals to 1. 34) 20 T. Xu and M. e1 / is a decimal fraction. e1 / is always an integer. e1 /. , 2 D 1 . 38) 1 When X and M1 are also co-prime numbers, sequence length for y2 is obtained as: 1 equals to 1. ei 1 /. e0 / D X and 0 D M0 D 1. If fM1 , M2 , . . , Mi g are co-prime numbers, Mi and M1 M2 ; : : : ; Mi 1 have to be co-prime numbers as well.

4) is the harmonic oscillation equation. 4), equivalently an additional rigidity caused by electrostatic force between parallel plates of sensing capacitor. 6) When there is acceleration which direction shown as in Fig. 2, the displacement of proof mass caused by inertial force is x. The electrostatic force between parallel plates of sensing capacitor will change and result in displacement variation y1 of the electrode on the vibrating beam. Thus, the gap distance of sensing parallelplate capacitor change x C y1 .

A navigation grade micro-machined silicon accelerometer. Position Location and Navigation Symposium, IEEE 94, 51–58 (1994) 5. : Bulk silicon resonant accelerometer. Chin. J. Semiconduct. 26(2), 281–286 (2005) 6. : Resonant microbeam accelerometers. The 8th International Conference on Solid-State Sensors and Actuators, and Eurosensors IX. Stockholm, Sweden, pp. 659–662, 25–29 June 1995 4 Design of Silicon Resonant Micro Accelerometer Based on Electrostatic Rigidity 45 7. : A novel resonant accelerometer: electrostatic stiffness type.

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Breakdown - History of Recover Vehicles in British Army - Brian Baxter 1990


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