2001
DOI: 10.1016/s0045-7825(01)00257-2
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A new solution procedure for application of energy-conserving algorithms to general constitutive models in nonlinear elastodynamics

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Cited by 53 publications
(46 citation statements)
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“…The original construction of S pt for general models of hyperelasticity can be found in [40], and is elaborated upon in [30]. However, a more convenient form is from references [21], [22] and is given as…”
Section: The Lagrangian Mesh Dynamicsmentioning
confidence: 99%
See 1 more Smart Citation
“…The original construction of S pt for general models of hyperelasticity can be found in [40], and is elaborated upon in [30]. However, a more convenient form is from references [21], [22] and is given as…”
Section: The Lagrangian Mesh Dynamicsmentioning
confidence: 99%
“…Unfortunately, a consistent linearization of equations (29) - (31), with the stress defined as in (54), produces an unsymmetric tangent matrix [21], [30], [40].…”
Section: It Is Not Necessary To Use a Midpoint-based Energy Conservinmentioning
confidence: 99%
“…Such observation has motivated the development of energy conserving schemes. Following the pioneering work by Simo and Tarnow [40], many studies extended this conserving algorithm to general hyperelastic materials [24,33,35,16] and arbitrary geometric nonlinearities [38,39]. Other work focused on applying these algorithms to specific finite element formulations (beam and shell elements) [41,42,15,48] and multi-body systems [7,10,28].…”
Section: Introductionmentioning
confidence: 99%
“…It consists in a mid-point scheme with an adequate evaluation of the internal forces, and was derived for a Saint Venant-Kirchhoff hyperelastic material. Laursen [2] generalized this approach to other hyperelastic models. His method involves resolving iteratively a new equation for each material point in order to compute the adequate Piola-Kirchhoff stress tensor.…”
Section: Introductionmentioning
confidence: 99%