MHD study of coronal waves: A numerical approach

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dc.contributor.author Parhi, S.
dc.contributor.author Pandey, B.P.
dc.contributor.author Goossens, M.
dc.contributor.author Lakhina, G.S.
dc.contributor.author DeBruyne, P.
dc.date.accessioned 2015-09-28T06:29:39Z
dc.date.accessioned 2021-02-12T09:31:06Z
dc.date.available 2015-09-28T06:29:39Z
dc.date.available 2021-02-12T09:31:06Z
dc.date.issued 1997
dc.identifier.citation Astrophysics and Space Science, v.250, p.147-162, 1997 doi: 10.1023/A:1000444410913 en_US
dc.identifier.uri http://localhost:8080/xmlui/handle/123456789/488
dc.description.abstract The 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.iso en en_US
dc.subject Coronal waves en_US
dc.subject Solar corona en_US
dc.subject MHD waves en_US
dc.subject Current sheet en_US
dc.title MHD study of coronal waves: A numerical approach en_US
dc.type Article en_US
dc.identifier.accession 090997


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