Author | dc.contributor.author | Gomberoff, L. | |
Author | dc.contributor.author | Hernández, M. | |
Admission date | dc.date.accessioned | 2019-01-29T12:39:46Z | |
Available date | dc.date.available | 2019-01-29T12:39:46Z | |
Publication date | dc.date.issued | 1984 | |
Cita de ítem | dc.identifier.citation | Physics of Fluids, Volumen 27, Issue 2, 1984, Pages 392-398 | |
Identifier | dc.identifier.issn | 10706631 | |
Identifier | dc.identifier.other | 10.1063/1.864632 | |
Identifier | dc.identifier.uri | https://repositorio.uchile.cl/handle/2250/159637 | |
Abstract | dc.description.abstract | Nonideal effects such as viscosity and thermal conductivity on the stability of a cylindrical current‐carrying plasma in a shearless magnetic field are studied. It is shown that for magnetic fields satisfying Bθ/Bz ≫1, nonideal effects drastically change the shape of the unstable spectrum of the ideal case. In particular, there is a physical mode at k∥ =m−nq=0 which, for a given value of the product of the coefficient of perpendicular viscosity and thermal conductivity, triggers large‐scale steady convection in the plasma. This state is shown to be the analog in a plasma of the well‐known stationary convection in ordinary hydrodynamics. | |
Lenguage | dc.language.iso | en | |
Source | dc.source | Physics of Fluids | |
Keywords | dc.subject | Condensed Matter Physics | |
Título | dc.title | Large-scale stationary convection in a cylindrical current-carrying plasma | |
Document type | dc.type | Artículo de revista | |
dcterms.accessRights | dcterms.accessRights | Acceso a solo metadatos | |
Cataloguer | uchile.catalogador | jmm | |
Indexation | uchile.index | Artículo de publicación SCOPUS | |
uchile.cosecha | uchile.cosecha | SI | |