14th WCCM-ECCOMAS Congress 2021
DOI: 10.23967/wccm-eccomas.2020.201
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Mixed Finite Element Formulations for Polyconvex Anisotropic Material Formulations

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Cited by 3 publications
(10 citation statements)
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“…The finite element discretization follows from the mixed principle of virtual power (see Reference [5,2]). Here, we need the complete internal energy, which consists of the assumed temperature field Θ, the entropy density field η as the corresponding Lagrange multiplier, the superimposed stress tensor S S S to derive an energy-momentum scheme, an independent mixed field C C C and the corresponding Lagrange multiplier S S S. The internal energy functional reads…”
Section: Finite Element Formulationmentioning
confidence: 99%
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“…The finite element discretization follows from the mixed principle of virtual power (see Reference [5,2]). Here, we need the complete internal energy, which consists of the assumed temperature field Θ, the entropy density field η as the corresponding Lagrange multiplier, the superimposed stress tensor S S S to derive an energy-momentum scheme, an independent mixed field C C C and the corresponding Lagrange multiplier S S S. The internal energy functional reads…”
Section: Finite Element Formulationmentioning
confidence: 99%
“…Furthermore, this leads to a less complex weak form. The superimposed fields (see Reference [2] and [5]), which have both variants in common, are given by…”
Section: Finite Element Formulationmentioning
confidence: 99%
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“…The finite element discretization follows from the mixed principle of virtual power (see Reference [4,5]). Here, we need the complete internal energy, which consists of the assumed temperature fieldΘ, the entropy density field η as the corresponding Lagrange multiplier, the superimposed stress tensorS S S to derive an energy-momentum scheme, an independent mixed fieldC C C and the corresponding Lagrangian multiplier S S S. The internal energy functional reads…”
Section: Finite Element Formulationmentioning
confidence: 99%
“…For both formulations we introduce an superimposed fieldH H H to obtain an energy-momentum scheme, as well. The superimposed fields (see Reference [5] and [4]) are given bỹ…”
Section: Finite Element Formulationmentioning
confidence: 99%