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dc.contributor.authorÇiftçi, Ünver
dc.date.accessioned2022-05-11T14:31:12Z
dc.date.available2022-05-11T14:31:12Z
dc.date.issued2013
dc.identifier.issn1941-4889
dc.identifier.issn1941-4897
dc.identifier.urihttps://doi.org/10.3934/jgm.2013.5.167
dc.identifier.urihttps://hdl.handle.net/20.500.11776/7363
dc.description.abstractAlthough conservative Hamiltonian systems with constraints can be formulated in terms of Dirac structures, a more general framework is necessary to cover also dissipative systems such as gradient and metriplectic systems with constraints. We define Leibniz-Dirac structures which lead to a natural generalization of Dirac and Riemannian structures, for instance. From modeling point of view, Leibniz-Dirac structures make it easy to formulate implicit dissipative Hamiltonian systems. We give their exact characterization in terms of bundle maps from the tangent bundle to the cotangent bundle and vice verse. Physical systems which can be formulated in terms of Leibniz-Dirac structures are discussed.en_US
dc.language.isoengen_US
dc.publisherAmer Inst Mathematical Sciences-Aimsen_US
dc.identifier.doi10.3934/jgm.2013.5.167
dc.rightsinfo:eu-repo/semantics/openAccessen_US
dc.subjectDirac manifoldsen_US
dc.subjectdissipative Hamiltonian systemsen_US
dc.subjectgradient systemsen_US
dc.subjectHamiltonian-Systemsen_US
dc.subjectAlgebroidsen_US
dc.subjectEquationsen_US
dc.titleLeibniz - Dirac Structures and Nonconservative Systems with Constraintsen_US
dc.typearticleen_US
dc.relation.ispartofJournal of Geometric Mechanicsen_US
dc.departmentFakülteler, Fen Edebiyat Fakültesi, Matematik Bölümüen_US
dc.identifier.volume5en_US
dc.identifier.issue2en_US
dc.identifier.startpage167en_US
dc.identifier.endpage183en_US
dc.institutionauthorÇiftçi, Ünver
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US
dc.identifier.wosWOS:000322004700002en_US


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