| Literature DB >> 32943800 |
Anthony R Yeates1, Tahar Amari2, Ioannis Contopoulos3, Xueshang Feng4, Duncan H Mackay5, Zoran Mikić6, Thomas Wiegelmann7, Joseph Hutton8, Christopher A Lowder9, Huw Morgan8, Gordon Petrie10, Laurel A Rachmeler11, Lisa A Upton12, Aurelien Canou2, Pierre Chopin2, Cooper Downs6, Miloslav Druckmüller13, Jon A Linker6, Daniel B Seaton14, Tibor Török6.
Abstract
Seven different models are applied to the same problem of simulating the Sun's coronal magnetic field during the solar eclipse on 2015 March 20. All of the models are non-potential, allowing for free magnetic energy, but the associated electric currents are developed in significantly different ways. This is not a direct comparison of the coronal modelling techniques, in that the different models also use different photospheric boundary conditions, reflecting the range of approaches currently used in the community. Despite the significant differences, the results show broad agreement in the overall magnetic topology. Among those models with significant volume currents in much of the corona, there is general agreement that the ratio of total to potential magnetic energy should be approximately 1.4. However, there are significant differences in the electric current distributions; while static extrapolations are best able to reproduce active regions, they are unable to recover sheared magnetic fields in filament channels using currently available vector magnetogram data. By contrast, time-evolving simulations can recover the filament channel fields at the expense of not matching the observed vector magnetic fields within active regions. We suggest that, at present, the best approach may be a hybrid model using static extrapolations but with additional energization informed by simplified evolution models. This is demonstrated by one of the models.Keywords: Magnetic fields; Sun: corona; Sun: surface magnetism
Year: 2018 PMID: 32943800 PMCID: PMC7493006 DOI: 10.1007/s11214-018-0534-1
Source DB: PubMed Journal: Space Sci Rev ISSN: 0038-6308 Impact factor: 8.017