The effect of coupling between the extensional bulk mode and the flexural mode of a cantilever beam resonator has been experimentally studied by exciting the two modes simultaneously. The modal frequency shift of linear extensional bulk mode shows a quadratic relationship with the square of flexural mode's amplitude displacement, and a frequency shift up to 1492 Hz is observed when the flexural mode is driven by a AC signal Vac of 3 V and a DC bias of 30 V. The flexural mode shows a Duffing-like behavior with a softening nonlinearity and its frequency shift is influenced not only by its own nonlinear amplitude-frequency effect but also the extensional mode's amplitude as predicted. The nonlinear coupling coefficient is found to be about two orders of magnitude larger than the softening nonlinearity.
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28 November 2016
Research Article|
November 30 2016
Nonlinear coupling of flexural mode and extensional bulk mode in micromechanical resonators
Tianyi Zhang;
Tianyi Zhang
a)
1State Key Laboratory for Manufacturing Systems Engineering,
Xi'an Jiaotong University
, Xi'an 710049, China
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Juan Ren;
Juan Ren
a)
2School of Construction Machinery,
Chang'an University
, Xi'an 710064, China
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Xueyong Wei
;
Xueyong Wei
b)
1State Key Laboratory for Manufacturing Systems Engineering,
Xi'an Jiaotong University
, Xi'an 710049, China
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Zhuangde Jiang;
Zhuangde Jiang
1State Key Laboratory for Manufacturing Systems Engineering,
Xi'an Jiaotong University
, Xi'an 710049, China
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Ronghua Huan
Ronghua Huan
c)
3Department of Mechanics,
Zhejiang University
, Hangzhou 310027, China
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a)
T. Zhang and J. Ren contributed equally to this work.
b)
Electronic mail: [email protected]
c)
Electronic mail: [email protected]
Appl. Phys. Lett. 109, 224102 (2016)
Article history
Received:
July 28 2016
Accepted:
November 15 2016
Citation
Tianyi Zhang, Juan Ren, Xueyong Wei, Zhuangde Jiang, Ronghua Huan; Nonlinear coupling of flexural mode and extensional bulk mode in micromechanical resonators. Appl. Phys. Lett. 28 November 2016; 109 (22): 224102. https://doi.org/10.1063/1.4970556
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