In Paper I (Emslie, 1985) we derived 'scaling laws' which relate peak loop temperature to injected non-thermal electron flux in electron-heated models of the flare corona. In this paper, we compare these predicted relationships with recent coordinated observations in hard X-rays and soft X-rays. Sa
The structure of high-temperature solar flare plasma in non-thermal flare models
โ Scribed by A. Gordon Emslie
- Publisher
- Springer
- Year
- 1985
- Tongue
- English
- Weight
- 492 KB
- Volume
- 98
- Category
- Article
- ISSN
- 0038-0938
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โฆ Synopsis
We solve the energy equation for the high-temperature (coronal) component of flare plasma for two models of energy input: (i) direct collisional heating by a beam of suprathermal electrons, and (ii) ohmic heating by the beam-neutralizing reverse current. We discuss the regimes where each case is applicable, and solve for the differential emission measure distribution of the coronal plasma in each case. 'Scaling laws' between loop temperatures and injected electron fluxes are derived for both models; these are testable observationally through coordinated soft X-ray and hard X-ray observations, thus providing a method of discriminating between the two cases. We also readdress the question of the energetic importance of a return current which is below the instability threshold for generation of ion-acoustic plasma turbulence. We find that unless the ambient coronal density is very low ( ~ 10 9 cm -3), collisional heating will always dominate there, in agreement with the findings of previous authors. However, in the chromosphere/corona transition region, the relatively low temperature and correspondingly high plasma resistivity imply that reverse current ohmic heating can predominate the flare energetics, by up to an order of magnitude. * Presidential Young Investigator.
๐ SIMILAR VOLUMES
Quasi-steady high-temperature current sheets are an energy source during the 'main' or 'hot' phase of solar flares. Such sheets are shown to be stabilized with respect to the tearing instability by a small transverse component of magnetic field existing in the sheets. \* Send offprint requests to B.