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dc.contributor.authorZahid, Zarqa
dc.contributor.authorParnell, C E
dc.contributor.authorQamar, Anisa
dc.date.accessioned2022-12-20T00:41:20Z
dc.date.available2022-12-20T00:41:20Z
dc.date.issued2021-12-20
dc.identifier277339536
dc.identifier3276fadc-f67e-4064-b5ed-4e2d53e36ce4
dc.identifier34972336
dc.identifier85122194302
dc.identifier000731945200002
dc.identifier.citationZahid , Z , Parnell , C E & Qamar , A 2021 , ' 3D non-driven magnetic reconnection at multiple separators ' , Chaos , vol. 31 , no. 12 , 123123 . https://doi.org/10.1063/5.0065957en
dc.identifier.issn1054-1500
dc.identifier.otherORCID: /0000-0002-5694-9069/work/105956272
dc.identifier.urihttps://hdl.handle.net/10023/26628
dc.descriptionFunding: We are thankful to the Higher Education Commission (HEC, Pakistan) for their financial support to one of the authors (Zarqa Zahid) under the IRSP program. We are also thankful to the School of Mathematics and Statistics, University of St. Andrews, North Haugh, St. Andrews, Scotland, UK, for accommodating one of the authors (Zarqa Zahid) in providing full support for the completion of this project.en
dc.description.abstractSeparators are important topological features of magnetic configuration for magnetic reconnection, commonly found in the solar plasma. They are located at the boundary shared among four distinctive flux domains; therefore, current layers easily build up around them. This paper aims to explore non-driven magnetic reconnection at multiple separators since little information is available about it. We have done two sets of experiments: non-resistive magnetohydrodynamic (MHD) relaxation and resistive MHD reconnection of a magnetic configuration consisting of two null points alongside their associated spines and three non-potential separators, which connect the same two null points. We used the LARE3D code for this purpose. The main current layers are formed along these separators where reconnection takes place. The reconnection occurs in two distinct phases: fast-strong and slow-weak. Most of the current dissipates at a fast rate, through Ohmic heating, during the fast-strong phase. The short-lived impulsive bursty reconnection events occur randomly in the slow-weak phase, while viscous heating exceeds Ohmic heating in this phase. The electric field component is parallel to field lines along the separators; likewise, the rate of reconnection along each of them evolved over time. However, work on separator reconnection has a strong potential to understand the underlying physics.
dc.format.extent14
dc.format.extent5232726
dc.language.isoeng
dc.relation.ispartofChaosen
dc.subjectQB Astronomyen
dc.subjectQC Physicsen
dc.subjectNDASen
dc.subjectMCCen
dc.subject.lccQBen
dc.subject.lccQCen
dc.title3D non-driven magnetic reconnection at multiple separatorsen
dc.typeJournal articleen
dc.contributor.institutionUniversity of St Andrews. Applied Mathematicsen
dc.identifier.doi10.1063/5.0065957
dc.description.statusPeer revieweden
dc.date.embargoedUntil2022-12-20


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