Published Date
7 February 2005, Vol.280(1):289–310, doi:10.1016/j.jsv.2003.12.031
Author
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http://www.sciencedirect.com/science/article/pii/S0022460X04000677
7 February 2005, Vol.280(1):289–310, doi:10.1016/j.jsv.2003.12.031
Author
Received 16 October 2002. Accepted 4 December 2003. Available online 9 April 2004.
Abstract
The variational equations derived in Part 1 of this work are extended to include the superposed angular velocity by means of the Coriolis effect. The resulting equations enable a semi-analytic treatment for the calculation of the dynamic characteristics of a vibratory angular-rate gyroscope composed of small piezoceramic bimorphs arranged in the shape of one half of a single tuning fork; use of mirror symmetries of that basic shape allows the construction of an H-shaped tuning fork gyroscope. The calculations are performed at the resonant frequency of the fundamental flexural mode. The dimensions of a typical half of a tuning fork shape structure considered in this work are approximately , which has fundamental natural frequencies ranging between 5 and , and can measure rotation-rates at least as high as . In order to have greater sensitivity it is necessary to have simultaneously large amplitudes of vibration in both the actuating and sensing modes. On account of this the two forced vibration problems are solved only at the matched first natural frequency of the fundamental flexural mode, which is obtained from the eigenanalysis that enables the selection of geometry for the frequencies to be matched.
Abstract
The variational equations derived in Part 1 of this work are extended to include the superposed angular velocity by means of the Coriolis effect. The resulting equations enable a semi-analytic treatment for the calculation of the dynamic characteristics of a vibratory angular-rate gyroscope composed of small piezoceramic bimorphs arranged in the shape of one half of a single tuning fork; use of mirror symmetries of that basic shape allows the construction of an H-shaped tuning fork gyroscope. The calculations are performed at the resonant frequency of the fundamental flexural mode. The dimensions of a typical half of a tuning fork shape structure considered in this work are approximately , which has fundamental natural frequencies ranging between 5 and , and can measure rotation-rates at least as high as . In order to have greater sensitivity it is necessary to have simultaneously large amplitudes of vibration in both the actuating and sensing modes. On account of this the two forced vibration problems are solved only at the matched first natural frequency of the fundamental flexural mode, which is obtained from the eigenanalysis that enables the selection of geometry for the frequencies to be matched.
- * Corresponding author. Currently: Assistant Professor, School of Mechanical Engineering, College of Engineering, Chung-Ang University, 221, Heukseok-Dong, Dongjak-Gu, Seoul 156-756, Korea. Tel.: +82-31-215-3319; fax: +82-31-215-3319
For further details log on website :
http://www.sciencedirect.com/science/article/pii/S0022460X04000677
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