2022
DOI: 10.1016/j.amc.2022.127048
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Fast MATLAB evaluation of nonlinear energies using FEM in 2D and 3D: Nodal elements

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Cited by 6 publications
(11 citation statements)
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“…where for p = 1: s is the index of a node i ∈ {1, 2, 3, 4}, for p ≥ 2: s is the index of an edge j ∈ {1, 2, 3, 4}, for p ≥ 4: s = 4 + β, where β is the local index of a bubble function (7).…”
Section: Local Indexingmentioning
confidence: 99%
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“…where for p = 1: s is the index of a node i ∈ {1, 2, 3, 4}, for p ≥ 2: s is the index of an edge j ∈ {1, 2, 3, 4}, for p ≥ 4: s = 4 + β, where β is the local index of a bubble function (7).…”
Section: Local Indexingmentioning
confidence: 99%
“…The assemblies of FEM matrices are based on our vectorized codes [1,2]. The names of most of the mesh attributes and the domain rectangulation algorithms are taken from [7].…”
Section: Implementation Remarksmentioning
confidence: 99%
“…For (hyper)elastic materials, D τ disappears, α reduces to the displacement field (u), and E τ involves only gradient(s) of u (cf. [11]). Through different mathematical forms, the dissipation functional allows one to describe different types of path-dependent material responses.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, Moskovka and Valdman [11] developed and successfully verified the fully vectorized implementation of hyperelastic constitutive models into the finite element method (FEM) through mathematical optimization. Their approach relies on a concurrent (loop-free) evaluation of (both linear and gradient) energy contributions to the global energy functional and efficient evaluation of energy gradients (needed in optimization) by employing the concept of nodal patches.…”
Section: Introductionmentioning
confidence: 99%
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