Adhesion of biological systems is often made possible through thin elastic layers, such as human skin. To address the question of when a layer is sufficiently thin to become adhesive, we extended Green's function molecular dynamics (GFMD) to account for the finite thickness of an elastic body that is supported by a fluid foundation. We observed that thin layers can much better accommodate rough counterfaces than thick structures. As a result, the contact area is enlarged, in particular, when the width of the layer omega approaches or even falls below the short-wavelength cutoff lambda(s) of the surface spectra. In the latter case, the proportionality coefficient between area and load scales is ( w/lambda(s))(3), which is consistent with Persson's contact mechanics theory.

A Green’s Function Molecular Dynamics Approach to the Mechanical Contact between Thin Elastic Sheets and Randomly Rough Surfaces

Putignano, Carmine;
2016-01-01

Abstract

Adhesion of biological systems is often made possible through thin elastic layers, such as human skin. To address the question of when a layer is sufficiently thin to become adhesive, we extended Green's function molecular dynamics (GFMD) to account for the finite thickness of an elastic body that is supported by a fluid foundation. We observed that thin layers can much better accommodate rough counterfaces than thick structures. As a result, the contact area is enlarged, in particular, when the width of the layer omega approaches or even falls below the short-wavelength cutoff lambda(s) of the surface spectra. In the latter case, the proportionality coefficient between area and load scales is ( w/lambda(s))(3), which is consistent with Persson's contact mechanics theory.
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11589/125406
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