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dc.contributor.authorTokad, Y.en_US
dc.date.accessioned2016-02-08T10:55:11Z
dc.date.available2016-02-08T10:55:11Z
dc.date.issued1992en_US
dc.identifier.issn0925-4668
dc.identifier.urihttp://hdl.handle.net/11693/26115
dc.description.abstractIn the formulation of equations of motion of three-dimensional mechanical systems, the techniques utilized and developed to analyze the electrical networks based on linear graph theory can conveniently be used. The success of this approach, however, relies on the availability of a complete and adequate mathematical model of the rigid body valid in the three-dimensional motion. This article is devoted to the derivation of such a mathematical model for the rigid body as a (k + 1)-port component. In this derivation, the dynamic properties of the rigid body are automatically included as a consequence of the analytical procedures used in the article. In this model, a general form of the terminal equations is given. In many applications, however, its special form, also given in this article, is used. © 1992 Kluwer Academic Publishers.en_US
dc.language.isoEnglishen_US
dc.source.titleDynamics and Controlen_US
dc.relation.isversionofhttp://dx.doi.org/10.1007/BF02169806en_US
dc.subjectEquations of Motionen_US
dc.subjectMathematical Techniques - Graph Theoryen_US
dc.subjectRigid Body Motionen_US
dc.subjectDynamicsen_US
dc.titleA network model for rigid-body motionen_US
dc.typeArticleen_US
dc.departmentDepartment of Mathematicsen_US
dc.citation.spage59en_US
dc.citation.epage82en_US
dc.citation.volumeNumber2en_US
dc.citation.issueNumber1en_US
dc.identifier.doi10.1007/BF02169806en_US
dc.publisherKluwer Academic Publishersen_US


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