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On the magnetic reconnection and its properties during a flare using a magnetohydrodynamics simulation

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dc.contributor.author Nayak, Sushree S
dc.contributor.author Hu, Qiang
dc.contributor.author He, Wen
dc.contributor.author Kumar, Sanjay
dc.contributor.author Bhattacharyya, R
dc.date.accessioned 2025-07-16T08:44:26Z
dc.date.available 2025-07-16T08:44:26Z
dc.date.issued 2025-06
dc.identifier.citation Solar Physics, Vol. 300, No. 6, 79 en_US
dc.identifier.issn 0038-0938
dc.identifier.uri http://hdl.handle.net/2248/8758
dc.description Restricted Access en_US
dc.description The original publication is available at springerlink.com
dc.description.abstract We study the magnetic reconnection during a flare by investigating flare ribbon dynamics using observations and data-constrained magnetohydrodynamics (MHD) simulation. In particular, we estimate the reconnection flux and the reconnection flux rates using flare ribbons of an M1.1 flare hosted by the active region 12184 utilizing the technique developed by Qiu et al. (2002). The reconnection flux and corresponding flux rates are found to be 1020 Mx and 1018 Mx s‑1 respectively. To understand the flare onset and the origin of flare ribbons, we perform an MHD simulation initiated by the non-force-free-field extrapolation. Importantly, the extrapolated configuration identifies a three-dimensional (3D) magnetic neutral point and a flux rope in the flaring region, which is crucial to the flaring activity. The reconnection initiates at the null point and, subsequently the flux rope rises and appears to reconnect there, which is favorable for the eruption of the filament. The surrounding field lines also seem to take part in the null point reconnection. In later stage, a current sheet is formed below the null point ensuing a secondary reconnection near an X-type topology, further contributing to the energy release process in the flare. We trace the footpoint evolution of the field lines lying over the flare ribbons and find a significant similarity between the observed flare ribbons and the evolution of footpoints computed from the MHD simulation. We estimated induced electric field during the flare and found it to be ≈ 0.52 V cm‑1, a slight less value, as per many past literatures. Additional findings are the enhancement of vertical current density near the flaring ribbons, a signature of successive reconnections near the null point. Overall, the present work contributes to the understanding of the ribbon formation in a flaring process and the involved magnetic reconnection. en_US
dc.language.iso en en_US
dc.publisher Springer Nature en_US
dc.relation.uri https://doi.org/10.1007/s11207-025-02492-2
dc.rights © The Author(s), under exclusive licence to Springer Nature B.V. 2025
dc.subject Magnetic reconnection en_US
dc.subject Magnetohydrodynamics en_US
dc.subject Magnetic fields en_US
dc.subject Corona en_US
dc.title On the magnetic reconnection and its properties during a flare using a magnetohydrodynamics simulation en_US
dc.type Article en_US


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