Issue |
A&A
Volume 673, May 2023
|
|
---|---|---|
Article Number | A150 | |
Number of page(s) | 10 | |
Section | Catalogs and data | |
DOI | https://doi.org/10.1051/0004-6361/202346087 | |
Published online | 24 May 2023 |
The F-CHROMA grid of 1D RADYN flare models
1
Institute of Theoretical Astrophysics, University of Oslo,
PO Box 1029
Blindern,
0315
Oslo,
Norway
e-mail: mats.carlsson@astro.uio.no
2
Rosseland Centre for Solar Physics, University of Oslo,
PO Box 1029
Blindern,
0315
Oslo,
Norway
3
SUPA School of Physics and Astronomy, University of Glasgow,
Glasgow
G12 8QQ,
UK
4
NASA/Goddard Space Flight Center,
Code 671,
Greenbelt,
MD 20771,
USA
5
Astronomical Institute of the Czech Academy of Sciences,
25165
Ondřejov,
Czech Republic
6
University of Wroclaw, Center of Scientific Excellence – Solar and Stellar Activity,
Kopernika 11,
51-622
Wroclaw,
Poland
7
National Solar Observatory, University of Colorado Boulder,
3665 Discovery Drive,
Boulder,
CO 80303,
USA
8
Department of Astrophysical and Planetary Sciences, University of Colorado,
Boulder,
2000 Colorado Ave,
CO 80305,
USA
9
Laboratory for Atmospheric and Space Physics, University of Colorado Boulder,
3665 Discovery Drive,
Boulder,
CO 80303,
USA
10
Astrophysics Research Centre, School of Mathematics and Physics, Queen’s University Belfast,
Belfast BT7 1NN,
Northern Ireland,
UK
11
Center for Radio Astronomy and Astrophysics Mackenzie, Engineering School, Mackenzie Presbyterian University,
São Paulo,
Brazil
Received:
6
February
2023
Accepted:
22
March
2023
Context. Solar flares are the result of the sudden release of magnetic energy in the corona. Much of this energy goes into accelerating charged particles to high velocity. These particles travel along the magnetic field and the energy is dissipated when the density gets high enough, primarily in the solar chromosphere. Modelling this region is difficult because the radiation energy balance is dominated by strong, optically thick spectral lines.
Aims. Our aim is to provide the community with realistic simulations of a flaring loop with an emphasis on the detailed treatment of the chromospheric energy balance. This will enable a detailed comparison of existing and upcoming observations with synthetic observables from the simulations, thereby elucidating the complex interactions in a flaring chromosphere.
Methods. We used the 1D radiation hydrodynamics code RADYN to perform simulations of the effect of a beam of electrons injected at the apex of a solar coronal loop. A grid of models was produced, varying the total energy input, the steepness, and low-energy cutoff of the beam energy spectrum.
Results. The full simulation results for a grid of models are made available online. Some general properties of the simulations are discussed.
Key words: hydrodynamics / Sun: atmosphere / Sun: chromosphere / Sun: flares
© The Authors 2023
Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
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