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On the eruption of prominences and disappearance of quiescent filaments

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dc.contributor.author Singh, J
dc.contributor.author Gupta, S. S
dc.date.accessioned 2008-07-01T11:08:14Z
dc.date.available 2008-07-01T11:08:14Z
dc.date.issued 1995-05
dc.identifier.citation Solar Physics, Vol. 158, No. 2, pp. 259 - 268 en
dc.identifier.issn 0038-0938
dc.identifier.uri http://hdl.handle.net/2248/2566
dc.description.abstract We suggest the following heuristic model for the evolution of a quiescent filament. The middle part of the filament rises due to heating, while its ends remain anchored in the chromosphere; and a kink appears in the H alpha filament due to projection and line-of-sight effects. Further, the top segment of the filament rises rapidly above the solar surface 1-2 days before the disappearance of a filament or eruption of a prominence. The top of the filament attains a high temperature due to further heating, thereby becoming invisible in H alpha, giving the impression that the filament has slit into two parts. It is expected that this gap between the H alpha filament can be seen in the observations in high-temperature lines and soft X-rays. en
dc.format.extent 791851 bytes
dc.format.mimetype application/pdf
dc.language.iso en en
dc.publisher Springer en
dc.relation.uri http://adsabs.harvard.edu/abs/1995SoPh..158..259S en
dc.relation.uri http://www.springerlink.com/content/w0r8062724v00755/ en
dc.subject Dynamic Stability en
dc.subject Solar Physics en
dc.subject Solar Prominences en
dc.subject Sun en
dc.subject Thermal Stability en
dc.subject Chromosphere en
dc.subject H Alpha Line en
dc.subject Heating en
dc.subject Solar X-Rays en
dc.title On the eruption of prominences and disappearance of quiescent filaments en
dc.type Article en


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