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dc.contributor.authorParhi, S.
dc.contributor.authorPandey, B.P.
dc.contributor.authorGoossens, M.
dc.contributor.authorLakhina, G.S.
dc.contributor.authorDeBruyne, P.
dc.date.accessioned2015-09-28T06:29:39Z
dc.date.accessioned2021-02-12T09:31:06Z-
dc.date.available2015-09-28T06:29:39Z
dc.date.available2021-02-12T09:31:06Z-
dc.date.issued1997
dc.identifier.citationAstrophysics and Space Science, v.250, p.147-162, 1997 doi: 10.1023/A:1000444410913en_US
dc.identifier.urihttp://localhost:8080/xmlui/handle/123456789/488-
dc.description.abstractThe solar corona, modelled by a low β, resistive plasma slab sustains MHD wave propagations due to footpoint motions in the photosphere. The density, magnetic profile and driver are considered to be neither very smooth nor very steep. The numerical simulation presents the evolution of MHD waves and the formation of current sheet. Steep gradients in slow wave at the slab edges which are signature of resonance layer where dissipation takes place are observed. Singularity is removed by the inclusion of finite resistivity. Dissipation takes place around the resonance layer where the perturbation develops large gradients. The width of the resonance layer is calculated. The thickness of the Alfvén resonance layer is more than that of the slow wave resonance layer. Attempt is made to distinguish between slow and Alfvén wave resonance layers. Fast waves develop into kink modes. As plasma evolves the current sheets which provide the heating at the edges gets distorted and fragment into two current sheets at each edge which in turn come closer when the twist is enhanced.en_US
dc.language.isoenen_US
dc.subjectCoronal wavesen_US
dc.subjectSolar coronaen_US
dc.subjectMHD wavesen_US
dc.subjectCurrent sheeten_US
dc.titleMHD study of coronal waves: A numerical approachen_US
dc.typeArticleen_US
dc.identifier.accession090997
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