2004
DOI: 10.1007/s10659-005-0929-6
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Asymptotic Considerations Shedding Light on Incompressible Shell Models

Abstract: The incompressible singularity found in 3D elasticity when Poisson's ratio approaches 1/2 is not present in classical shell models, nor in the limit models obtained from 3D elasticity when performing an asymptotic analysis with respect to the thickness parameter. However, some specific shell models -such as the 3D-shell model -do retain the incompressible singularity. These observations raise the issue of how adequately shell models can represent incompressible conditions, which this paper aims at investigatin… Show more

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Cited by 6 publications
(3 citation statements)
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“…The incompressibility constraint is used to eliminate the transverse normal strain, and based on which, a numerical shell theory with five parameters for a generalized orthotropic incompressible hyperelastic material was developed. In [6], Chapelle et al examined whether the plane stress assumption or the asymptotic limits of thickness can commute with the incompressibility constraint, justifying the usages of classical shell models and a modified 3D shell model in the incompressible conditions. In Kiendl et al [7], a shell theory for compressible and incompressible isotropic hyperelastic materials was developed based on the Kirchhoff-Love kinematics which includes the assumptions of zero transverse normal stress and straight and normal cross sections, and then an isogeometric discretization was introduced for numerical computation.…”
Section: Introductionmentioning
confidence: 99%
“…The incompressibility constraint is used to eliminate the transverse normal strain, and based on which, a numerical shell theory with five parameters for a generalized orthotropic incompressible hyperelastic material was developed. In [6], Chapelle et al examined whether the plane stress assumption or the asymptotic limits of thickness can commute with the incompressibility constraint, justifying the usages of classical shell models and a modified 3D shell model in the incompressible conditions. In Kiendl et al [7], a shell theory for compressible and incompressible isotropic hyperelastic materials was developed based on the Kirchhoff-Love kinematics which includes the assumptions of zero transverse normal stress and straight and normal cross sections, and then an isogeometric discretization was introduced for numerical computation.…”
Section: Introductionmentioning
confidence: 99%
“…Itskov [31] proposed an orthotropic hyperelastic constitutive model, which is coupled with incompressible shell kinematics to deal with large strains and finite rotations of shell structures. Chapelle et al [32] analyzed whether the stress assumption or the asymptotic limits of thinness can be commuted with the incompressibility condition, which justified the usages of classical shell models and a modified 3D shell models under incompressibility condition. By using the normalΓ -convergence method, Li and Chermisi [33] rigorously derived the von Kármán shell theory for incompressible materials.…”
Section: Introductionmentioning
confidence: 99%
“…While sometimes effective, these elements display severe illconditioning when the shell becomes thin and when the shell is an (almost) incompressible medium [17,18]. To improve the element behavior and computational effectiveness, instead of displacement degrees of freedom, enhanced strains have been used, see for example Refs.…”
Section: Introductionmentioning
confidence: 99%