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 |
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dc.date.issued |
1995-05 |
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dc.identifier.citation |
Solar Physics, Vol. 158, No. 2, pp. 259 - 268 |
en |
dc.identifier.issn |
0038-0938 |
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dc.identifier.uri |
http://hdl.handle.net/2248/2566 |
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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 |
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dc.format.mimetype |
application/pdf |
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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 |