A unified model of solar prominence formation
arXiv:2104.13546 · doi:10.3847/2041-8213/abfbe0
Abstract
Several mechanisms have been proposed to account for the formation of solar prominences or filaments, among which direct injection and evaporation-condensation models are the two most popular ones. In the direct injection model, cold plasma is ejected from the chromosphere into the corona along magnetic field lines; In the evaporation-condensation model, the cold chromospheric plasma is heated to over a million degrees and is evaporated into the corona, where the accumulated plasma finally reaches thermal instability or non-equilibrium so as to condensate to cold prominences. In this paper, we try to unify the two mechanisms: The essence of filament formation is the localized heating in the chromosphere. If the heating happens in the lower chromosphere, the enhanced gas pressure pushes the cold plasma in the upper chromosphere to move up to the corona, such a process is manifested as the direct injection model. If the heating happens in the upper chromosphere, the local plasma is heated to million degrees, and is evaporated into the corona. Later, the plasma condensates to form a prominence. Such a process is manifested as the evaporation-condensation model. With radiative hydrodynamic simulations we confirmed that the two widely accepted formation mechanisms of solar prominences can really be unified in such a single framework. A particular case is also found where both injection and evaporation-condensation processes occur together.
10 pages, 4 figures, accepted for publication in ApJ Letters
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- Dynamic formation of multi-threaded prominences in arcade configurations
- Formation of a solar filament by magnetic reconnection and coronal condensation
- Winking filaments due to cyclic evaporation-condensation
- Modeling of Condensations in Coronal Loops Produced by Impulsive Heating
- Self-consistent numerical simulations for the formation and dynamics of solar prominences
- Formation and Characteristics of Filament Threads in Double-Dipped Magnetic Flux Tubes