The nature of quiescent solar prominences
β Scribed by Max Kuperus; Einar Tandberg-Hanssen
- Publisher
- Springer
- Year
- 1967
- Tongue
- English
- Weight
- 550 KB
- Volume
- 2
- Category
- Article
- ISSN
- 0038-0938
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β¦ Synopsis
Quiescent prominences occur as long-lasting cool sheets of matter in the surrounding hot corona at the base of coronal streamers. Seen on the disk they appear as dark filaments dividing regions of opposite magnetic polarity.
In this paper a theoretical model is presented, which describes the general appearance of quiescent prominences.
It is shown that the neutral sheet between two regions of oppositely directed magnetic fields is thermally unstable. This gives rise to compression and cooling of coronal material to prominence material in a characteristic time of the order of one day for a field strength of 0.5 gauss in the lower corona.
It is assumed that due to the finite electrical resistivity of the plasma, filamentary structures are formed by the 'tearing-mode' resistive plasma instability. These structures are thermally insulated from the hot surroundings by the newly formed closed azimuthal magnetic field configuration.
It has been shown that for fine structures with a diameter of 300 km the growth rate of the 'tearingmode' instability is of the same order as the cooling time. The occurrence of fine structures within the prominence is of vital importance for their origin.
π SIMILAR VOLUMES
In some quiescent prominences, areas are found where the Ha emission profiles are centrally reversed. By combining good spatial, spectral, and temporal resolution, the detailed behavior of these reversal regions has been investigated. Many of the regions show a growth and subsequent decay in the aff
For stable equilibrium, prominences must be supported with magnetic lines of force leaning
A class of 2-D models of solar quiescent prominences, with normal polarity, is presented. These represent an extension to the Kippenhahn-Schlt~ter model for which the prominence configuration matches smoothly onto an external non-potential coronal solution of a constant ~ field. Using typical promin