Comparison of the Hall Magnetohydrodynamics and Magnetohydrodynamics Evolution of a flaring solar active region

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dc.contributor.author Bora, Kamlesh
dc.contributor.author Bhattacharyya, Ramitendranath
dc.contributor.author Prasad, Avijeet
dc.contributor.author Joshi, Bhuwan
dc.contributor.author Hu, Qiang
dc.coverage.spatial United Kingdom
dc.date.accessioned 2022-02-16T08:48:06Z
dc.date.available 2022-02-16T08:48:06Z
dc.date.issued 2022-02
dc.identifier.citation Bora, Kamlesh; Bhattacharyya, Ramitendranath; Prasad, Avijeet; Joshi, Bhuwan and Hu, Qiang, "Comparison of the Hall Magnetohydrodynamics and Magnetohydrodynamics Evolution of a flaring solar active region", The Astrophysical Journal, DOI: 10.3847/1538-4357/ac3bce, vol. 925, no. 2, Feb. 2022. en_US
dc.identifier.issn 0004-637X
dc.identifier.issn 1538-4357
dc.identifier.uri https://doi.org/10.3847/1538-4357/ac3bce
dc.identifier.uri https://repository.iitgn.ac.in/handle/123456789/7522
dc.description.abstract This work analyzes the Hall magnetohydrodynamics (HMHD) and magnetohydrodynamics (MHD) numerical simulations of a flaring solar active region as a test bed while idealizing the coronal Alfvén speed to be less by two orders of magnitude. HMHD supports faster magnetic reconnection and shows richer complexity in magnetic field line evolution compared to the MHD. The magnetic reconnections triggering the flare are explored by numerical simulations augmented with relevant multiwavelength observations. The initial coronal magnetic field is constructed by non-force-free extrapolation of photospheric vector magnetic field. Magnetic structure involved in the flare is identified to be a flux rope, with its overlying magnetic field lines constituting the quasi-separatrix layers (QSLs) along with a three-dimensional null point and a null line. Compared to the MHD simulation, the HMHD simulation shows a higher and faster ascent of the rope together with the overlying field lines, which further reconnect at the QSL located higher up in the corona. The footpoints of the field lines match better with the observations for the HMHD case, with the central part of the flare ribbon located at the chromosphere. Additionally, field lines are found to rotate in a circular pattern in the HMHD, whereas no such rotation is seen in the MHD results. Interestingly, plasma is also observed to be rotating in a cospatial chromospheric region, which makes the HMHD simulation more credible. Based on the aforementioned agreements, HMHD simulation is found to agree better with observations and thus opens up a novel avenue to explore.
dc.description.statementofresponsibility by Kamlesh Bora, Ramitendranath Bhattacharyya, Avijeet Prasad, Bhuwan Joshi and Qiang Hu
dc.format.extent vol. 925, no. 2
dc.language.iso en_US en_US
dc.publisher IOP Publishing en_US
dc.subject Hall magnetohydrodynamics en_US
dc.subject Magnetohydrodynamics en_US
dc.subject Flaring solar active region en_US
dc.subject Quasi-separatrix layers en_US
dc.subject HMHD simulation en_US
dc.title Comparison of the Hall Magnetohydrodynamics and Magnetohydrodynamics Evolution of a flaring solar active region en_US
dc.type Article en_US
dc.relation.journal The Astrophysical Journal


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