Three-dimensional finite element analysis of MHD duct flow by the penalty function formulation

dc.contributorUniversidade de São Paulo (USP)
dc.contributorENSIEG
dc.contributorUniversidade Estadual Paulista (Unesp)
dc.date.accessioned2014-05-20T15:30:39Z
dc.date.available2014-05-20T15:30:39Z
dc.date.created2014-05-20T15:30:39Z
dc.date.issued2001-09-01
dc.identifierIEEE Transactions on Magnetics. New York: IEEE-Inst Electrical Electronics Engineers Inc., v. 37, n. 5, p. 3384-3387, 2001.
dc.identifier0018-9464
dc.identifierhttp://hdl.handle.net/11449/39979
dc.identifier10.1109/20.952619
dc.identifierWOS:000171322000069
dc.description.abstractA numerical scheme based on the Finite Element Method (FEM) is presented to calculate the full solution of a three-dimensional steady magnetohydrodynamic (MHD) flow with moderately high Hartmann numbers and interaction parameters. An incompressible, viscous and electrically conducting liquid-metal is considered. Assuming a low magnetic Reynolds number, the solution method solves the coupled Navier-Stokes and Maxwell's equations through the use of a penalty function method. Results are presented for Hartmann numbers in the range 10(2)-10(3).
dc.languageeng
dc.publisherInstitute of Electrical and Electronics Engineers (IEEE)
dc.relationIEEE Transactions on Magnetics
dc.relation1.467
dc.relation0,488
dc.rightsAcesso restrito
dc.sourceWeb of Science
dc.subjectfinite element method
dc.subjectliquid metal flows
dc.subjectmagnetohydrodynamics
dc.subjectpenalty function method
dc.titleThree-dimensional finite element analysis of MHD duct flow by the penalty function formulation
dc.typeArtículos de revistas


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