Zobrazit minimální záznam



dc.contributor.authorSchmidt , Jaroslav
dc.contributor.authorJanda , Tomáš
dc.contributor.authorZemanová , Alena
dc.contributor.authorZeman , Jan
dc.contributor.authorŠejnoha , Michal
dc.date.accessioned2021-03-10T15:43:33Z
dc.date.available2021-03-10T15:43:33Z
dc.date.issued2020
dc.identifier.citationActa Polytechnica. 2020, vol. 60, no. 6
dc.identifier.issn1210-2709 (print)
dc.identifier.issn1805-2363 (online)
dc.identifier.urihttp://hdl.handle.net/10467/93807
dc.description.abstractThis paper investigates a time-stepping procedure of the Newmark type for dynamic analyses of viscoelastic structures characterized by a generalized Maxwell model. We depart from a scheme developed for a three-parameter model by Hatada et al. [1], which we extend to a generic Maxwell chain and demonstrate that the resulting algorithm can be derived from a suitably discretized Hamilton variational principle. This variational structure manifests itself in an excellent stability and a low artificial damping of the integrator, as we confirm with a mass-spring-dashpot example. After a straightforward generalization to distributed systems, the integrator may find use in, e.g., fracture simulations of laminated glass units, once combined with variationally-based fracture models.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherČeské vysoké učení technické v Prazecs
dc.publisherCzech Technical University in Pragueen
dc.relation.ispartofseriesActa Polytechnica
dc.relation.urihttps://ojs.cvut.cz/ojs/index.php/ap/article/view/5981
dc.rightsCreative Commons Attribution 4.0 International Licenseen
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/
dc.titleNewmark algorithm for dynamic analysis with Maxwell chain model
dc.typearticleen
dc.date.updated2021-03-10T15:43:33Z
dc.identifier.doi10.14311/AP.2020.60.0502
dc.rights.accessopenAccess
dc.type.statusPeer-reviewed
dc.type.versionpublishedVersion


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Zobrazit minimální záznam

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