1985
DOI: 10.1016/0165-232x(85)90048-5
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Visco-elastic buckling analysis of floating ice sheets

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Cited by 12 publications
(4 citation statements)
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“…The general situation of the slow buckling of a thin floating ice sheet can be treated as that of a visco-elastic medium under axial stress supported by an elastic medium (Sjölind 1985, Sanderson 1988). We lack the necessary material parameters to analyse this situation (in particular the elastic bending stiffness of a thick sheet of snow ice, and information on the creep behaviour of warm and cold snow ice at low strain rates (Weeks 2010, Timco & Weeks 2010)).…”
Section: Discussionmentioning
confidence: 99%
“…The general situation of the slow buckling of a thin floating ice sheet can be treated as that of a visco-elastic medium under axial stress supported by an elastic medium (Sjölind 1985, Sanderson 1988). We lack the necessary material parameters to analyse this situation (in particular the elastic bending stiffness of a thick sheet of snow ice, and information on the creep behaviour of warm and cold snow ice at low strain rates (Weeks 2010, Timco & Weeks 2010)).…”
Section: Discussionmentioning
confidence: 99%
“…At the other extreme, in the limit E → ∞ the Maxwell model reduces to a purely viscous fluid. The creep buckling of a viscous plate has been analyzed by Sjolind (1985) and Staroszczyk and Hedzielski (2004) and it is important to understand our results in the context of these earlier studies. The analog of elastic buckling for a viscous plate can be analyzed exactly as above starting with Equation 7 but taking as the rheological model…”
Section: Discussionmentioning
confidence: 99%
“…Post‐buckling amplification and failure is not explicitly modeled but assumed to occur in short order. In the creep buckling studies of Sjolind (1985) and Staroszczyk and Hedzielski (2004) small but finite initial disturbances grow to large amplitude after a few hours assuming the initial linear governing equation remains valid. Neither approach completely solves the problem; to do so requires a nonlinear, large amplitude theory.…”
Section: Discussionmentioning
confidence: 99%
“…In the limit case of a thin sheet lying on a liquid surface, it has be shown that the sinusoidal wrinkles appearing close to the buckling threshold (i.e for low confined configurations) spontaneously transform into a localized fold for highly confined configurations 16 . This phenomenon covers a wide range of length scales, spanning from lipid monolayers 17 up to ice pack in the ocean 18 , and may lead to the delamination of the film from the liquid 19 . Audoly 20 has derived an amplitude equation for the envelope of the pattern, explaining the localization of the buckling and relating it to the one on a nonlinear elastic foundation.…”
Section: Introductionmentioning
confidence: 99%