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Bifurcations and chaos in electrostatic vibration energy harvesters
Date Issued
2012-05
Date Available
2012-04-03T11:31:07Z
Abstract
In this paper, we present an analysis of an electrostatic vibration harvester operating in the constant-charge mode. The goal of the study is to bound regions of control parameters where the system displays steady-state harmonic oscillations as
required for practical use. We show how the system can be presented as a nonlinear oscillator and analysed employing the
multiple scales method, Floquet theory and Lyapunov exponents. We determine the conditions for the onset of steady-state oscillations, the period doubling bifurcation and transition to chaos.
This allows us to bound regions of control parameters where the system displays desired regular oscillations and, therefore, to
identify maximal harvestable power for a particular architecture.
required for practical use. We show how the system can be presented as a nonlinear oscillator and analysed employing the
multiple scales method, Floquet theory and Lyapunov exponents. We determine the conditions for the onset of steady-state oscillations, the period doubling bifurcation and transition to chaos.
This allows us to bound regions of control parameters where the system displays desired regular oscillations and, therefore, to
identify maximal harvestable power for a particular architecture.
Sponsorship
Science Foundation Ireland
Type of Material
Conference Publication
Publisher
IEEE
Copyright (Published Version)
2012 IEEE
Subject – LCSH
Energy harvesting
Bifurcation theory
Chaotic behavior in systems
Oscillations
Language
English
Status of Item
Not peer reviewed
Journal
Circuits and Systems (ISCAS), 2012 IEEE International Symposium on [proceedings]
Conference Details
Paper presented at the IEEE International Symposium on Circuits and Systems 2012 (ISCAS 2012), Seoul, Korea, 20-23 May 2012
ISBN
978-1-4673-0218-0
This item is made available under a Creative Commons License
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ISCAS2012_eVEHs.pdf
Size
454.96 KB
Format
Adobe PDF
Checksum (MD5)
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