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Author:

Zhou, Shengxi (Zhou, Shengxi.) | Cao, Junyi (Cao, Junyi.) | Erturk, Alper (Erturk, Alper.) | Lin, Jing (Lin, Jing.) | Zhang, Xining (Zhang, Xining.)

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Abstract:

To establish the dynamical model of piezoelectric energy harvester with magnetic coupling, the modeling approach for the harvester is proposed based on nonlinear polynomial description of nonlinear restoring force. The nonlinear restoring force of the cantilever beam being in different positions is measured directly by a small electronic dynamometer and the polynomial parameters of the force are estimated. Then the nonlinear restoring force is taken into account to establish the nonlinear model following Hamilton principle, Euler-Bernoulli beam theory and piezoelectric theory. Runge-Kutta method is introduced to simulate the nonlinear output characteristics of the harvester. The results show that the proposed model enables to simply solve the parameters, reduce calculation task and avoid the direct calculation of magnetic force. And the model can describe the important designing parameters in terms of the jump frequency, maximum voltage and effective bandwidth for the mechanism analysis of magnetic coupled piezoelectric energy harvester.

Keyword:

Broadband Euler Bernoulli beam theory Non-linear model Nonlinear restoring force Output characteristics Piezoelectric Piezoelectric energy harvesters Vibration energy harvesting

Author Community:

  • [ 1 ] [Zhou, Shengxi;Cao, Junyi;Lin, Jing;Zhang, Xining]State Key Laboratory for Manufacturing Systems Engineering, Xi'an Jiaotong University, Xi'an 710049, China
  • [ 2 ] [Erturk, Alper]G.W. Woodruff School of Mechanical Engineering, Georgia Institute of Technology, Atlanta 30332, United States

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Source :

Hsi-An Chiao Tung Ta Hsueh/Journal of Xi'an Jiaotong University

ISSN: 0253-987X

Year: 2014

Issue: 1

Volume: 48

Page: 106-111

Cited Count:

WoS CC Cited Count: 0

SCOPUS Cited Count: 15

ESI Highly Cited Papers on the List: 0 Unfold All

WanFang Cited Count: -1

Chinese Cited Count: -1

30 Days PV: 0

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