Fringe instability in constrained soft elastic layers

Soft elastic layers with top and bottom surfaces adhered to rigid bodies are abundant in biological organisms and engineering applications. As the rigid bodies are pulled apart, the stressed layer can exhibit various modes of mechanical instabilities. In cases where the layer's thickness is muc...

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Bibliographic Details
Main Authors: Lin, Shaoting (Contributor), Cohen, Tal (Contributor), Zhang, Teng (Contributor), Yuk, Hyunwoo (Contributor), Abeyaratne, Rohan (Contributor), Zhao, Xuanhe (Contributor)
Other Authors: Massachusetts Institute of Technology. Department of Civil and Environmental Engineering (Contributor), Massachusetts Institute of Technology. Department of Mechanical Engineering (Contributor)
Format: Article
Language:English
Published: Royal Society of Chemistry, 2017-03-09T16:26:59Z.
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Online Access:Get fulltext
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042 |a dc 
100 1 0 |a Lin, Shaoting  |e author 
100 1 0 |a Massachusetts Institute of Technology. Department of Civil and Environmental Engineering  |e contributor 
100 1 0 |a Massachusetts Institute of Technology. Department of Mechanical Engineering  |e contributor 
100 1 0 |a Lin, Shaoting  |e contributor 
100 1 0 |a Cohen, Tal  |e contributor 
100 1 0 |a Zhang, Teng  |e contributor 
100 1 0 |a Yuk, Hyunwoo  |e contributor 
100 1 0 |a Abeyaratne, Rohan  |e contributor 
100 1 0 |a Zhao, Xuanhe  |e contributor 
700 1 0 |a Cohen, Tal  |e author 
700 1 0 |a Zhang, Teng  |e author 
700 1 0 |a Yuk, Hyunwoo  |e author 
700 1 0 |a Abeyaratne, Rohan  |e author 
700 1 0 |a Zhao, Xuanhe  |e author 
245 0 0 |a Fringe instability in constrained soft elastic layers 
260 |b Royal Society of Chemistry,   |c 2017-03-09T16:26:59Z. 
856 |z Get fulltext  |u http://hdl.handle.net/1721.1/107250 
520 |a Soft elastic layers with top and bottom surfaces adhered to rigid bodies are abundant in biological organisms and engineering applications. As the rigid bodies are pulled apart, the stressed layer can exhibit various modes of mechanical instabilities. In cases where the layer's thickness is much smaller than its length and width, the dominant modes that have been studied are the cavitation, interfacial and fingering instabilities. Here we report a new mode of instability which emerges if the thickness of the constrained elastic layer is comparable to or smaller than its width. In this case, the middle portion along the layer's thickness elongates nearly uniformly while the constrained fringe portions of the layer deform nonuniformly. When the applied stretch reaches a critical value, the exposed free surfaces of the fringe portions begin to undulate periodically without debonding from the rigid bodies, giving the fringe instability. We use experiments, theory and numerical simulations to quantitatively explain the fringe instability and derive scaling laws for its critical stress, critical strain and wavelength. We show that in a force controlled setting the elastic fingering instability is associated with a snap-through buckling that does not exist for the fringe instability. The discovery of the fringe instability will not only advance the understanding of mechanical instabilities in soft materials but also have implications for biological and engineered adhesives and joints. 
520 |a United States. Office of Naval Research (Grant N00014-14-1-0528) 
520 |a Massachusetts Institute of Technology. Institute for Soldier Nanotechnologies 
520 |a National Science Foundation (U.S.) (Grant CMMI- 1253495) 
520 |a Samsung Scholarship Foundation 
520 |a National Institutes of Health (U.S.) (Grant UH3TR000505) 
520 |a MIT-Technion Fellowship 
546 |a en_US 
655 7 |a Article 
773 |t Soft Matter