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Please use this identifier to cite or link to this item: http://acervodigital.unesp.br/handle/11449/74062
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dc.contributor.authorMonzani, R. C.-
dc.contributor.authorPrado, A. J.-
dc.contributor.authorKurokawa, S.-
dc.contributor.authorBovolato, L. F.-
dc.contributor.authorPissolato Filho, J.-
dc.date.accessioned2014-05-27T11:27:25Z-
dc.date.accessioned2016-10-25T18:40:39Z-
dc.date.available2014-05-27T11:27:25Z-
dc.date.available2016-10-25T18:40:39Z-
dc.date.issued2012-12-11-
dc.identifierhttp://dx.doi.org/10.1109/PESGM.2012.6345161-
dc.identifier.citationIEEE Power and Energy Society General Meeting.-
dc.identifier.issn1944-9925-
dc.identifier.issn1944-9933-
dc.identifier.urihttp://hdl.handle.net/11449/74062-
dc.identifier.urihttp://acervodigital.unesp.br/handle/11449/74062-
dc.description.abstractThis paper presents a method for analyzing electromagnetic transients using real transformation matrices in three-phase systems considering the presence of ground wires. So, for the Z and Y matrices that represent the transmission line, the characteristics of ground wires are not implied in the values related to the phases. A first approach uses a real transformation matrix for the entire frequency range considered in this case. This transformation matrix is an approximation to the exact transformation matrix. For those elements related to the phases of the considered system, the transformation matrix is composed of the elements of Clarke's matrix. In part related to the ground wires, the elements of the transformation matrix must establish a relationship with the elements of the phases considering the establishment of a single homopolar reference in the mode domain. In the case of three-phase lines with the presence of two ground wires, it is unable to get the full diagonalization of the matrices Z and Y in the mode domain. This leads to the second proposal for the composition of real transformation matrix: obtain such transformation matrix from the multiplication of two real and constant matrices. In this case, the inclusion of a second matrix had the objective to minimize errors from the first proposal for the composition of the transformation matrix mentioned. © 2012 IEEE.en
dc.language.isoeng-
dc.sourceScopus-
dc.subjecteigenvalue-
dc.subjecteigenvector-
dc.subjectelectromagnetic transients-
dc.subjectground wires-
dc.subjecthomopolar mode-
dc.subjectline transmission-
dc.subjectClarke's matrix-
dc.subjectConstant matrix-
dc.subjectDiagonalizations-
dc.subjectEigen-value-
dc.subjectEigenvalue analysis-
dc.subjectElectro-magnetic transient-
dc.subjectFrequency ranges-
dc.subjectGround wire-
dc.subjectMode domain-
dc.subjectReal transformation-
dc.subjectThree phase system-
dc.subjectThree-phase lines-
dc.subjectTransformation matrices-
dc.subjectEigenvalues and eigenfunctions-
dc.subjectElectric lines-
dc.subjectTransients-
dc.subjectTransmission line theory-
dc.subjectWire-
dc.subjectLinear transformations-
dc.titleEigenvalue analyses for non-transposed three-phase transmission line considering non-implicit ground wiresen
dc.typeoutro-
dc.contributor.institutionUniversidade Estadual Paulista (UNESP)-
dc.contributor.institutionUniversidade Estadual de Campinas (UNICAMP)-
dc.description.affiliationElectrical Engineering Department DEE UNESP Paulista State University, Av. Brasil, 56, Ilha Solteira-
dc.description.affiliationElectrical Engineering Department DSCE Campinas State University-
dc.description.affiliationUnespElectrical Engineering Department DEE UNESP Paulista State University, Av. Brasil, 56, Ilha Solteira-
dc.identifier.doi10.1109/PESGM.2012.6345161-
dc.identifier.wosWOS:000312493704009-
dc.rights.accessRightsAcesso restrito-
dc.relation.ispartofIEEE Power and Energy Society General Meeting-
dc.identifier.scopus2-s2.0-84870597413-
Appears in Collections:Artigos, TCCs, Teses e Dissertações da Unesp

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