2014
DOI: 10.1016/j.ijnonlinmec.2014.10.018
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On the natural shape of a plastically deformed thin sheet

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Cited by 6 publications
(3 citation statements)
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“…Nevertheless, the multiplicative decomposition can be used for isotropic materials where both elastic and plastic rotations do not play any role in the final boundary-value-problem [15]. The need for a multiplicative decomposition can also be circumnavigated if we assume an additive decomposition of the total strain into elastic and plastic counterparts.…”
Section: Internal Stress and Natural Shapesmentioning
confidence: 99%
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“…Nevertheless, the multiplicative decomposition can be used for isotropic materials where both elastic and plastic rotations do not play any role in the final boundary-value-problem [15]. The need for a multiplicative decomposition can also be circumnavigated if we assume an additive decomposition of the total strain into elastic and plastic counterparts.…”
Section: Internal Stress and Natural Shapesmentioning
confidence: 99%
“…The concepts of material uniformity, material symmetry, and inhomogeneity in elastic Cosserat surfaces, following the pioneering works of Noll [52] and Wang [72], are also firmly established [23][24][25][26]73,74], although these works have neither attempted to describe the inhomogeneity distribution in terms of the curvature and non-metricity (the notion of torsion does appear in some of these works), nor have they discussed the relevant issue of strain incompatibility. A theory of materially uniform, inhomogeneous (dislocated) thin elastic films, derived from a 3-dimensional uniform, inhomogeneous (dislocated) elastic body, has been recently proposed by Steigmann [68], and applied to determining the natural shapes of plastically deformed thin sheets [15]. Finally, we mention, only in passing, the extensive work on mechanics of topologically defective ('geometrically frustrated') liquid crystalline surfaces [7,8,10,58], which, in contrast to the local theories mentioned above, have taken a distinguished local-global (geometrical-topological) standpoint in describing the nature of defects.…”
Section: Introductionmentioning
confidence: 99%
“…Note that even in the case when W 0 does not explicitly depend on X and is an isotropic function with respect to the second argument (which corresponds to a homogeneous and isotropic material), W depends on X via K and remains an isotropic function only for particular values of K. Thus, a locally homogeneous and isotropic material turns out to be inhomogeneous and anisotropic as part of a self-stressed body. This fact is characterized by the concepts of material uniformity and inhomogeneity [47][48][49][50].…”
mentioning
confidence: 99%