2014
DOI: 10.1017/s0956792514000291
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Elastic-plated gravity currents

Abstract: We consider a nonlinear diffusion equation describing the planar spreading of a viscous fluid injected between an elastic sheet and an underlying rigid plane. The dynamics depends sensitively on the physical conditions at the contact line where the sheet is lifted off the plane by the fluid. We explore two possibilities for these conditions (or “regularisations”): a pre-wetted film and a constant-pressure fluid lag (a gas-filled gap between the fluid edge and the contact line). For both flat and inclined plane… Show more

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Cited by 68 publications
(132 citation statements)
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References 30 publications
(71 reference statements)
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“…When deflections are smaller than the thickness of the pocket, the pocket is bent and analytical solutions developed in previous works were sought (Koialovich, 1902;Boobnoff, 1902;Amon and Widera, 1969;Chandrashekhara, 2001;Meleshko, 1997;Hewitt et al, 2015), while when the deformations are greater than the thickness, the pocket is stretched and numerical solutions were extended using Finite Element Analysis.…”
Section: Discussionmentioning
confidence: 99%
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“…When deflections are smaller than the thickness of the pocket, the pocket is bent and analytical solutions developed in previous works were sought (Koialovich, 1902;Boobnoff, 1902;Amon and Widera, 1969;Chandrashekhara, 2001;Meleshko, 1997;Hewitt et al, 2015), while when the deformations are greater than the thickness, the pocket is stretched and numerical solutions were extended using Finite Element Analysis.…”
Section: Discussionmentioning
confidence: 99%
“…In the case of a ring, when α tends to 1, Hewitt et al (2015) obtained an asymptotical approximation of γ b equal to (1 − σ 2 )/32. In the stretching regime, the maximum deflection reduces as well when the size of the hole (α) increases for both shapes.…”
Section: Maximum Displacementsmentioning
confidence: 99%
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“…The solution for γ (υ) is discussed below, but first, we translate the result back to the notation of the ruck problem. We have determined 11) and so the energy constraint (2.11) is…”
Section: (B) a Thermodynamic Adhesion Modelmentioning
confidence: 99%