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Magnetohydrostatic equilibrium in solar coronal arcades

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dc.contributor.author Chandra, S
dc.contributor.author Prasad, L
dc.date.accessioned 2007-05-17T05:11:29Z
dc.date.available 2007-05-17T05:11:29Z
dc.date.issued 1994
dc.identifier.citation BASI, Vol. 22, No. 2, pp. 149-157 en
dc.identifier.uri http://hdl.handle.net/2248/1591
dc.description.abstract We 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 behavior en
dc.format.extent 527834 bytes
dc.format.mimetype application/pdf
dc.language.iso en en
dc.publisher Astronomical Society of India en
dc.subject Solar physics en
dc.subject Solar flares en
dc.title Magnetohydrostatic equilibrium in solar coronal arcades en
dc.type Article en


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