Abstract
It is suggested that a thermal nonequilibrium or catastrophe may trigger
a solar flare, rather than a magnetic instability, and this possibility
is demonstrated by approximately solving the energy equation for a loop
under a balance between thermal conduction, optically thin radiation,
and a heating source. It is found that if one begins with a cool
equilibrium at a few times 10,000 K, and gradually increases the heating
or decreases the loop pressure, critical metastable conditions are
ultimately reached beyond which no equilibrium exists. During thermal
flaring in which the plasma heats up explosively, to a new
quasi-equilibrium at 10 million K, any magnetic disruption or particle
acceleration are secondary. The cool core of an active-region loop heats
up and the magnetic plasma tube maintains its position in the case of a
compact flare, while a two-ribbon flare has the material of an active
region filament heating and expanding along the filament.
| Original language | English |
|---|---|
| Pages (from-to) | 289-311 |
| Journal | Solar Physics |
| Volume | 73 |
| DOIs | |
| Publication status | Published - 1 Oct 1981 |
Keywords
- Magnetohydrodynamics
- Nonequilibrium Thermodynamics
- Plasma Heating
- Solar Flares
- Solar Physics
- Coronal Loops
- Optical Thickness
- Particle Acceleration
- Solar Prominences
- Thermodynamic Equilibrium