2007
DOI: 10.1007/s00707-006-0432-6
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On the stress function approach in three-dimensional elasticity

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Cited by 3 publications
(3 citation statements)
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“…The Lagrange multiplier term ensuring the symmetry of the stress tensor in functional (12) for cylindrical shells using (11) in terms of the expanded variables (31), (32), and (25) reads…”
Section: Dimensional Reductionmentioning
confidence: 99%
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“…The Lagrange multiplier term ensuring the symmetry of the stress tensor in functional (12) for cylindrical shells using (11) in terms of the expanded variables (31), (32), and (25) reads…”
Section: Dimensional Reductionmentioning
confidence: 99%
“…It should also be mentioned that the possible structure of the first-order stress functions giving zero complementary strain energy has to be found to obtain correct finite element solutions. This problem was investigated in two-dimensional elasticity in [17], and a possible structure of the zero-energy stress functions for the three-dimensional case was given in [11]. In addition, to avoid redundant approximation of the stress function components, the indeterminacy property of the stress function tensor should be taken into account.…”
mentioning
confidence: 99%
“…The stress function approach and the related complementary energy-based variational principles have been successfully applied in the finite element analysis of twodimensional elasticity problems, see, e.g., [2,[7][8][9]. For three-dimensional problems, however, no efficient finite element model exists, which is due mainly to the C 1continuity requirement for the second-order stress functions on the one hand, and to the structure of the zero-energy modes and the difficulties with their suppression for the case of first-order stress functions, on the other hand [10].…”
Section: Introductionmentioning
confidence: 99%