Electric-field-induced interfacial instabilities of a soft elastic membrane confined between viscous layers

Title
Electric-field-induced interfacial instabilities of a soft elastic membrane confined between viscous layers
Author(s)
주상우모하르데이Dipankar Bandyopadhyay[Dipankar Bandyopadhyay]아슈샬마스즈첸
Keywords
THIN LIQUID-FILMS; NONLINEAR STABILITY ANALYSIS; POLYMER-FILMS; PATTERN-FORMATION; CURVATURE ELASTICITY; LIQUID/LIQUID INTERFACES; CONTACT INSTABILITY; ELASTOMERIC LAYERS; DYNAMICS; BILAYERS
Issue Date
201210
Publisher
AMER PHYSICAL SOC
Citation
PHYSICAL REVIEW E, v.86, no.4
Abstract
We explore the electric-field-induced interfacial instabilities of a trilayer composed of a thin elastic film confined between two viscous layers. A linear stability analysis (LSA) is performed to uncover the growth rate and length scale of the different unstable modes. Application of a normal external electric field on such a configuration can deform the two coupled elastic-viscous interfaces either by an in-phase bending or an antiphase squeezing mode. The bending mode has a long-wave nature, and is present even at a vanishingly small destabilizing field. In contrast, the squeezing mode has finite wave-number characteristics and originates only beyond a threshold strength of the electric field. This is in contrast to the instabilities of the viscous films with multiple interfaces where both modes are found to possess long-wave characteristics. The elastic film is unstable by bending mode when the stabilizing forces due to the in-plane curvature and the elastic stiffness are strong and the destabilizing electric field is relatively weak. In comparison, as the electric field increases, a subdominant squeezing mode can also appear beyond a threshold destabilizing field. A dominant squeezing mode is observed when the destabilizing field is significantly strong and the elastic films are relatively softer with lower elastic modulus. In the absence of liquid layers, a free elastic film is also found to be unstable by long-wave bending and finite wave-number squeezing modes. The LSA asymptotically recovers the results obtained by the previous formulations where the membrane bending elasticity is approximately incorporated as a correction term in the normal stress boundary condition. Interestingly, the presence of a very weak stabilizing influence due to a smaller interfacial tension at the elastic-viscous interfaces opens up the possibility of fabricating submicron patterns exploiting the instabilities of a trilayer.
URI
http://hdl.handle.net/YU.REPOSITORY/27120http://dx.doi.org/10.1103/PhysRevE.86.041602
ISSN
1539-3755
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공과대학 > 기계공학부 > Articles
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