Surface Instability in Soft Materials Rui Huang University of Texas at Austin
Outline Elastomer (rubber) block Elastomer bilayer (thin film) or graded stiffness Polymer gels Electromechanical instability of dielectric elastomer A simple buckling problem
Elastomer block Wrinkling or creasing? Biot’s linear perturbation analysis for wrinkling Nonlinear stability analysis for creasing (Hohlfeld and Mahadevan, 2011; Hong et al., 2009) From wrinkles to creases (Cao and Hutchinson, PRSA 2012) Effect of surface energy (Chen et al., 2012)
From instantaneous to setback creases Diab, Zhang, Zhao, Gao and Kim (2013)
Elastic bilayers: from wrinkling to folding Cao and Hutchinson, JAM 2012
Effect of pre-stretched substrates Cao and Hutchinson, JAM 2012
Experiments Sun et al., 2012 Pocivavsek et al., 2008
More bifurcations Brau et al., 2010
Gels: Swell-Induced Instability Trujillo et al, Tanaka et al, 1987 Wrinkles or creases? Critical condition Characteristic size Effect of kinetics Abundant experimental observations, but lacking fundamental understanding.
Bilayer gels: two types of instability A B Wu, Bouklas and Huang, IJSS 50, (2013). Type A: soft-on-hard bilayer, critical condition at the short wave limit, forming surface creases; Type B: hard-on-soft bilayer, critical condition at a finite wavelength, forming surface wrinkles first (and then creases).
Gradient and kinetics Guvendiren et al, 2009 & 2010.
Other geometries Wu et al, Dervaux et al, DuPont et al, 2010.
Dielectric elastomer membranes: Electromechanical instability Plante and Dubowsky, IJSS Huang and Suo, 2012.
A simple buckling problem? simply supported, but allow vertical displacement x y At x = 0, buckling amplitude is zero (no buckling) At x → infinity, unconstrained buckling (long wavelength mode) In between, short-wavelength mode appears near the end, and transition of buckling mode occurs. Postbuckling behavior: how would the buckling mode change with position (x) and the compressive strain?
From graphene to curtain: Wrinklons? Vandeparre et al., 2011.