Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/2566
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dc.contributor.authorSingh, J-
dc.contributor.authorGupta, S. S-
dc.date.accessioned2008-07-01T11:08:14Z-
dc.date.available2008-07-01T11:08:14Z-
dc.date.issued1995-05-
dc.identifier.citationSolar Physics, Vol. 158, No. 2, pp. 259 - 268en
dc.identifier.issn0038-0938-
dc.identifier.urihttp://hdl.handle.net/2248/2566-
dc.description.abstractWe 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.extent791851 bytes-
dc.format.mimetypeapplication/pdf-
dc.language.isoenen
dc.publisherSpringeren
dc.relation.urihttp://adsabs.harvard.edu/abs/1995SoPh..158..259Sen
dc.relation.urihttp://www.springerlink.com/content/w0r8062724v00755/en
dc.subjectDynamic Stabilityen
dc.subjectSolar Physicsen
dc.subjectSolar Prominencesen
dc.subjectSunen
dc.subjectThermal Stabilityen
dc.subjectChromosphereen
dc.subjectH Alpha Lineen
dc.subjectHeatingen
dc.subjectSolar X-Raysen
dc.titleOn the eruption of prominences and disappearance of quiescent filamentsen
dc.typeArticleen
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