A numerical hydrodynamic model of a heated coronal loop

The fluid equations describing a fully ionized single-temperature (i.e., electron and proton temperatures assumed identical) hydrogen plasma in a coronal loop subject to a transient heating pulse (2 x 10 super(9) ergs cm super(-) super(2) sec super(-) super(1) ) centered about the loop apex have bee...

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Bibliographic Details
Published inSolar physics Vol. 103; no. 1; pp. 47 - 66
Main Author MacNeice, Peter
Format Journal Article
LanguageEnglish
Published Boston, MA Reidel 01.01.1986
Dordrecht
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ISSN0038-0938
1573-093X
DOI10.1007/BF00154858

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Summary:The fluid equations describing a fully ionized single-temperature (i.e., electron and proton temperatures assumed identical) hydrogen plasma in a coronal loop subject to a transient heating pulse (2 x 10 super(9) ergs cm super(-) super(2) sec super(-) super(1) ) centered about the loop apex have been solved numerically. An adaptive regridding scheme was used to ensure adequate spatial resolution throughout the transition region, and appropriate consideration was given to the numerical time constants. Because of the fine gridding made possible by this scheme, these results represent the first reliable simulation of the impact of a downward-propagating conduction front on the transition region, and the early stages of the development of the downward-moving compression and upward ablation. Intensities in the OV (1371-A) transition region line were calculated from the model results. Estimates have been made of the importance of the downward-streaming collisionless high-energy tail of the distribution in the transition region resulting from the very steep temperature gradients. It is shown that the mass and energy densities are not substantially altered by the non-Maxwellian tail, except insofar as they are coupled to higher moments of the distribution function, such as the heat flux through the fluid equations.
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ISSN:0038-0938
1573-093X
DOI:10.1007/BF00154858