dc.creator | Elfimov, Artour | |
dc.date.accessioned | 2012-04-18T23:54:29Z | |
dc.date.accessioned | 2018-07-04T14:38:23Z | |
dc.date.available | 2012-04-18T23:54:29Z | |
dc.date.available | 2018-07-04T14:38:23Z | |
dc.date.created | 2012-04-18T23:54:29Z | |
dc.date.issued | 2008 | |
dc.identifier | PHYSICS OF PLASMAS, v.15, n.7, 2008 | |
dc.identifier | 1070-664X | |
dc.identifier | http://producao.usp.br/handle/BDPI/15976 | |
dc.identifier | 10.1063/1.2952837 | |
dc.identifier | http://dx.doi.org/10.1063/1.2952837 | |
dc.identifier.uri | http://repositorioslatinoamericanos.uchile.cl/handle/2250/1612798 | |
dc.description.abstract | Using 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.language | eng | |
dc.publisher | AMER INST PHYSICS | |
dc.relation | Physics of Plasmas | |
dc.rights | Copyright AMER INST PHYSICS | |
dc.rights | openAccess | |
dc.title | Kinetic effect on low frequency Alfven continuum in tokamaks | |
dc.type | Artículos de revistas | |