dc.creatorElfimov, Artour
dc.date.accessioned2012-04-18T23:54:29Z
dc.date.accessioned2018-07-04T14:38:23Z
dc.date.available2012-04-18T23:54:29Z
dc.date.available2018-07-04T14:38:23Z
dc.date.created2012-04-18T23:54:29Z
dc.date.issued2008
dc.identifierPHYSICS OF PLASMAS, v.15, n.7, 2008
dc.identifier1070-664X
dc.identifierhttp://producao.usp.br/handle/BDPI/15976
dc.identifier10.1063/1.2952837
dc.identifierhttp://dx.doi.org/10.1063/1.2952837
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/1612798
dc.description.abstractUsing a quasi-toroidal set of coordinates in plasmas with coaxial circular magnetic surfaces, the Vlasov equation is solved, and dielectric tensor is found for large aspect ratio tokamaks in a low frequency band. Taking into account the q-profile and drift effects, Alfven wave continuum deformation by geodesic effects is analyzed. It is shown that the Alfven continuum has a minimum defined by the ion thermal velocity at the rational magnetic surfaces q(s)=-M/N, where M and N are the poloidal and toroidal mode numbers, respectively, and the parallel wave number is zero. Low frequency global Alfven waves are found below the continuum minimum. In hot ion plasmas, the geodesic term changes sign, provoking some deformation of Alfven velocity by a factor (1+q(2))(-1/2), and the continuum minimum disappears. (C) 2008 American Institute of Physics.
dc.languageeng
dc.publisherAMER INST PHYSICS
dc.relationPhysics of Plasmas
dc.rightsCopyright AMER INST PHYSICS
dc.rightsopenAccess
dc.titleKinetic effect on low frequency Alfven continuum in tokamaks
dc.typeArtículos de revistas


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