2011
DOI: 10.1063/1.3568885
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Compression-induced failure of electroactive polymeric thin films

Abstract: The insurgence of compression induces wrinkling in actuation devices based on EAPs thin films leading to a sudden decrease of performances up to failure. Based on the classical tension field theory for thin elastic membranes (e.g.[11]), we provide a general framework for the analysis of the insurgence of in-plane compression in membranes of electroactive polymers (EAPs). Our main result is the deduction of a (voltage-dependent) domain in the stretch space which represents tensile configurations. Under the assu… Show more

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Cited by 33 publications
(25 citation statements)
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References 18 publications
(38 reference statements)
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“…The large actuation achieved due to the snap-through behaviour is desirable for many applications but is difficult to achieve in practice. Snapthrough is often prevented by electric breakdown [29] or by instabilities such as inhomogeneities [1], compression failure [5], band localisation [10], wrinkles [17,20,21,28,24,3], membrane wrinkling [12], etc.…”
Section: Introductionmentioning
confidence: 99%
“…The large actuation achieved due to the snap-through behaviour is desirable for many applications but is difficult to achieve in practice. Snapthrough is often prevented by electric breakdown [29] or by instabilities such as inhomogeneities [1], compression failure [5], band localisation [10], wrinkles [17,20,21,28,24,3], membrane wrinkling [12], etc.…”
Section: Introductionmentioning
confidence: 99%
“…Theoretical analysis of electromechanical instability has been considered by many authors, exemplified in [27][28][29][30][31][32][33][34][35][36][37][38][39][40][41][42]. Based on the theory of small deformations superimposed on large deformations for a general electroelastic material following the development of Dorfmann & Ogden [43], an analysis of the stability of an electroelastic plate was performed by the same authors in [44].…”
Section: (A) Planar Geometriesmentioning
confidence: 99%
“…The counterpart of (7.35) for the energy function Ω * , with variables λ 1 , λ 2 and K 4 is denoted Ω * (λ 1 , λ 2 , K 4 ) and obtained by specializing (7.7) as 37) whereω * (λ 1 , λ 2 ) =ω(λ 1 , λ 2 ) and λ…”
Section: (B) Isotropic Electroelasticitymentioning
confidence: 99%
“…3,4,22,23,30 The working principle of electromechanical harvesters is based on the idea that a part of the mechanical work done to deform a thin EAP membrane, sandwiched between compliant electrodes, can be used to pump electric charges from lower voltage to higher voltage: this is achieved by making use of filler-reinforced materials with enhanced elastic stiffness and dielectric permittivity. 22,23,25 Despite the positive features described above, the performances of electromechanical harvesters are affected by several limitations, spanning from the dielectric breakdown threshold of the EAP material, 2 to the occurrence of wrinkling and pull-in instabilities, [10][11][12]26,28 to the localization of deformations, 13,29,34 to the dissipation in the loading frame of the membrane, 22 and finally to dissipation processes taking place at the level of the polymeric material. This last aspect plays an important role in harvesting applications and the present analysis is devoted to its modelling.…”
mentioning
confidence: 99%