Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/1591
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dc.contributor.authorChandra, S-
dc.contributor.authorPrasad, L-
dc.date.accessioned2007-05-17T05:11:29Z-
dc.date.available2007-05-17T05:11:29Z-
dc.date.issued1994-
dc.identifier.citationBASI, Vol. 22, No. 2, pp. 149-157en
dc.identifier.urihttp://hdl.handle.net/2248/1591-
dc.description.abstractWe present a solution of magnetohydrostatic equations after including the effect of gravity. For low values of the parameters beta, there exist two solutions for the common boundary condition at the base of the corona. These two solutions correspond to two different magnetic configurations with different energies. The high-energy configuration may become unstable due to physical conditions and relax to the low-energy configuration, releasing an amount of the energy that may be observed in the form of a solar activity, such as two-ribbon flares. When the value of beta exceeds the critical limit, the magnetohydrostatic equations have no solution. If the system is forced to exceed beyond the critical limit, the magnetic field may show a violent behavioren
dc.format.extent527834 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoenen
dc.publisherAstronomical Society of Indiaen
dc.subjectSolar physicsen
dc.subjectSolar flaresen
dc.titleMagnetohydrostatic equilibrium in solar coronal arcadesen
dc.typeArticleen
Appears in Collections:BASI Publications

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