Vanishing Viscosity Limit For Incompressible Flow Inside A Rotating Circle

dc.creatorLopes Filho M.C.
dc.creatorMazzucato A.L.
dc.creatorNussenzveig Lopes H.J.
dc.date2008
dc.date2015-06-30T19:29:21Z
dc.date2015-11-26T14:44:48Z
dc.date2015-06-30T19:29:21Z
dc.date2015-11-26T14:44:48Z
dc.date.accessioned2018-03-28T21:53:49Z
dc.date.available2018-03-28T21:53:49Z
dc.identifier
dc.identifierPhysica D: Nonlinear Phenomena. , v. 237, n. 10-12, p. 1324 - 1333, 2008.
dc.identifier1672789
dc.identifier10.1016/j.physd.2008.03.009
dc.identifierhttp://www.scopus.com/inward/record.url?eid=2-s2.0-44649120782&partnerID=40&md5=2800febdb95e9beed60858cf724cb5df
dc.identifierhttp://www.repositorio.unicamp.br/handle/REPOSIP/106442
dc.identifierhttp://repositorio.unicamp.br/jspui/handle/REPOSIP/106442
dc.identifier2-s2.0-44649120782
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/1252267
dc.descriptionIn this article we consider circularly symmetric incompressible viscous flow in a disk. The boundary condition is no-slip with respect to a prescribed time-dependent rotation of the boundary about the center of the disk. We prove that, if the prescribed angular velocity of the boundary has finite total variation, then the Navier-Stokes solutions converge strongly in L2 to the corresponding stationary solution of the Euler equations when viscosity vanishes. Our approach is based on a semigroup treatment of the symmetry-reduced scalar equation. © 2008 Elsevier B.V. All rights reserved.
dc.description237
dc.description10-12
dc.description1324
dc.description1333
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dc.languageen
dc.publisher
dc.relationPhysica D: Nonlinear Phenomena
dc.rightsfechado
dc.sourceScopus
dc.titleVanishing Viscosity Limit For Incompressible Flow Inside A Rotating Circle
dc.typeArtículos de revistas


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