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      Peeling of Finite-Length Plates From an Elastomeric Foundation: A 1D Cylindrical Bending Solution

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      Journal of Applied Mechanics
      ASME International

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          Abstract

          Quasi-static peeling of a finite-length, flexible, horizontal, one-dimensional (1D) plate (strip, thin film) from a horizontal, thin, elastomeric layer (foundation) is considered. The displaced end of the plate is subjected to an upward deflection or to a rotation. The top of the interlayer is perfectly bonded to the plate, and its lower surface is bonded to a rigid, flat substrate. A transversality (debonding) condition is derived for peeling, based on the common fracture mechanics approach. Whereas debonding from a Winkler foundation can be expressed in terms of the displacement (or equivalently the foundation stress2) at the bond termination, the sixth-order formulation required for elastomeric foundations involves a more complex debonding criterion. Transversality relationships are used to describe this limit state (here the onset of debonding) in terms of co-state variables, herein the deflection and slope at the peel front. In the analysis, bending is assumed to be paramount, linear Kirchhoff–Love (classical) plate theory is used to model the deformation, and therefore displacements are assumed to be small. The foundation is linearly elastic and incompressible. The effects of the work of adhesion, the length of the plate, and the initial nonbonded length of the plate are investigated. The results are compared to those for a Winkler foundation. By replacing the shear modulus of the interlayer by viscosity, and displacements by their time derivatives, the results are expected to apply to viscous liquid interlayers as well.

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          Most cited references38

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          Internal Rupture of Bonded Rubber Cylinders in Tension

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            Contact, Adhesion and Rupture of Elastic Solids

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              Meniscus instability in a thin elastic film

              A new kind of meniscus instability leading to the formation of stationary fingers with a well-defined spacing has been observed in experiments with elastomeric films confined between a plane rigid glass and a thin curved glass plate. The wavelength of the instability increases linearly with the thickness of the confined film, but it is remarkably insensitive to the compliance and the energetics of the system. However, lateral amplitude (length) of the fingers depends on the compliance of the system and on the radius of curvature of the glass plate. A simple linear stability analysis is used to explain the underlying physics and the key observed features of the instability.
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                Author and article information

                Journal
                Journal of Applied Mechanics
                ASME International
                0021-8936
                1528-9036
                September 01 2023
                September 01 2023
                May 23 2023
                : 90
                : 9
                Article
                10.1115/1.4062493
                8e714933-5805-4387-9d63-51cd399a2654
                © 2023

                https://www.asme.org/publications-submissions/publishing-information/legal-policies

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