Utilize este identificador para referenciar este registo: https://hdl.handle.net/1822/53347

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dc.contributor.authorAreias, P.por
dc.contributor.authorRabczuk, T.por
dc.contributor.authorSá, J. M. A. César depor
dc.contributor.authorAlves, J. L.por
dc.date.accessioned2018-03-23T14:00:46Z-
dc.date.available2018-03-23T14:00:46Z-
dc.date.issued2016-
dc.identifier.issn0141-0296por
dc.identifier.urihttps://hdl.handle.net/1822/53347-
dc.description.abstractA new semi-implicit stress integration algorithm for finite strain plasticity (compatible with hyperelas- ticity) is introduced. Its most distinctive feature is the use of different parameterizations of equilibrium and reference configurations. Rotation terms (nonlinear trigonometric functions) are integrated explicitly and correspond to a change in the reference configuration. In contrast, relative Green–Lagrange strains (which are quadratic in terms of displacements) represent the equilibrium configuration implicitly .In addition, the adequacy of several objective stress rates in the semi-implicit context is studied. We para- metrize both reference and equilibrium configurations, in contrast with the so-called objective stress integration algorithms which use coinciding configurations. A single constitutive framework provides quantities needed by common discretization schemes. This is computationally convenient and robust, as all elements only need to provide pre-established quantities irrespectively of the constitutive model. In this work, mixed strain/stress control is used, as well as our smoothing algorithm for the complemen- tarity condition. Exceptional time-step robustness is achieved in elasto-plastic problems: often fewer than one-tenth of the typical number of time increments can be used with a quantifiable effect in accuracy. The proposed algorithm is general: all hyperelastic models and all classical elasto-plastic models can be employed. Plane-stress, Shell and 3D examples are used to illustrate the new algorithm. Both isotropic and anisotropic behavior is presented in elasto-plastic and hyperelastic examplespor
dc.language.isoengpor
dc.publisherElsevier 1por
dc.rightsopenAccesspor
dc.subjectConstitutive integrationpor
dc.subjectNewton methodspor
dc.subjectElasto-plasticitypor
dc.subjectFinite strainspor
dc.titleSemi-implicit finite strain constitutive integration and mixed strain/stress control based on intermediate configurationspor
dc.typearticlepor
dc.peerreviewedyespor
dc.relation.publisherversionhttps://www.sciencedirect.com/science/article/pii/S0141029616303054por
oaire.citationStartPage344por
oaire.citationEndPage360por
oaire.citationVolume124por
dc.identifier.eissn0141-0296-
dc.identifier.doi10.1016/j.engstruct.2016.06.035por
dc.subject.fosEngenharia e Tecnologia::Engenharia Mecânicapor
dc.description.publicationversioninfo:eu-repo/semantics/publishedVersionpor
dc.subject.wosScience & Technologypor
sdum.journalEngineering Structurespor
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