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Conference Paper: Natural modes of complex stiffness systems

TitleNatural modes of complex stiffness systems
Authors
Issue Date1991
Citation
Computational Mechanics, 1991, p. 581-586 How to Cite?
AbstractFor a vibrating dissipative system with hysteresis loop, complex (dynamic) stiffness is widely used. Although there are eigenvalue solvers available to solve the symmetric complex eigenvalue problems being produced, the physical interpretation of the eigensolutions which are no longer in complex conjugate pairs is generally impossible. An approximate method is introduced so that the natural modes are real while the natural frequencies are still complex. For certain forms of complex stiffness, the method is exact. In general, the imaginary part of the complex stiffness is transformed according to the requirement that the energy dissipated in each mode is the same under the transformation. The advantage of the present method is in its ability to produce real modal vectors and not necessary in its computational efficiency. The model vectors produced are orthogonal so that a realistic modal analysis is possible.
Persistent Identifierhttp://hdl.handle.net/10722/152087

 

DC FieldValueLanguage
dc.contributor.authorLeung, AYTen_US
dc.contributor.authorMiao, JLen_US
dc.contributor.authorCheung, YKen_US
dc.date.accessioned2012-06-26T06:35:07Z-
dc.date.available2012-06-26T06:35:07Z-
dc.date.issued1991en_US
dc.identifier.citationComputational Mechanics, 1991, p. 581-586en_US
dc.identifier.urihttp://hdl.handle.net/10722/152087-
dc.description.abstractFor a vibrating dissipative system with hysteresis loop, complex (dynamic) stiffness is widely used. Although there are eigenvalue solvers available to solve the symmetric complex eigenvalue problems being produced, the physical interpretation of the eigensolutions which are no longer in complex conjugate pairs is generally impossible. An approximate method is introduced so that the natural modes are real while the natural frequencies are still complex. For certain forms of complex stiffness, the method is exact. In general, the imaginary part of the complex stiffness is transformed according to the requirement that the energy dissipated in each mode is the same under the transformation. The advantage of the present method is in its ability to produce real modal vectors and not necessary in its computational efficiency. The model vectors produced are orthogonal so that a realistic modal analysis is possible.en_US
dc.languageengen_US
dc.relation.ispartofComputational Mechanicsen_US
dc.titleNatural modes of complex stiffness systemsen_US
dc.typeConference_Paperen_US
dc.identifier.emailCheung, YK:hreccyk@hkucc.hku.hken_US
dc.identifier.authorityCheung, YK=rp00104en_US
dc.description.naturelink_to_subscribed_fulltexten_US
dc.identifier.scopuseid_2-s2.0-0026300328en_US
dc.identifier.spage581en_US
dc.identifier.epage586en_US
dc.identifier.scopusauthoridLeung, AYT=7403012564en_US
dc.identifier.scopusauthoridMiao, JL=7102180214en_US
dc.identifier.scopusauthoridCheung, YK=7202111065en_US

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