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dc.contributor.authorFuentes-Fernandez, Jorge
dc.contributor.authorParnell, Clare E.
dc.date.accessioned2013-08-22T14:01:04Z
dc.date.available2013-08-22T14:01:04Z
dc.date.issued2012-06
dc.identifier.citationFuentes-Fernandez , J & Parnell , C E 2012 , ' Magnetohydrodynamics dynamical relaxation of coronal magnetic fields : III. 3D spiral nulls ' , Astronomy & Astrophysics , vol. 544 , A77 . https://doi.org/10.1051/0004-6361/201219190en
dc.identifier.issn0004-6361
dc.identifier.otherPURE: 66348475
dc.identifier.otherPURE UUID: 9a71ccf9-43db-41f7-ab70-bd6d75044611
dc.identifier.otherArXiv: http://arxiv.org/abs/1206.5527v1
dc.identifier.otherScopus: 84864739472
dc.identifier.otherORCID: /0000-0002-5694-9069/work/73700737
dc.identifier.urihttps://hdl.handle.net/10023/3978
dc.description.abstractContext: The majority of studies on stressed 3D magnetic null points consider magnetic reconnection driven by an external perturbation, but the formation of a genuine current sheet equilibrium remains poorly understood. This problem has been considered more extensively in two-dimensions, but lacks a generalization into 3D fields. Aims: 3D magnetic nulls are more complex than 2D nulls and the field can take a greater range of magnetic geometries local to the null. Here, we focus on one type and consider the dynamical non-resistive relaxation of 3D spiral nulls with initial spine-aligned current. We aim to provide a valid magnetohydrostatic equilibrium, and describe the electric current accumulations in various cases, involving a finite plasma pressure. Methods: A full MHD code is used, with the resistivity set to zero so that reconnection is not allowed, to run a series of experiments in which a perturbed spiral 3D null point is allowed to relax towards an equilibrium, via real, viscous damping forces. Changes to the initial plasma pressure and other magnetic parameters are investigated systematically. Results: For the axi-symmetric case, the evolution of the field and the plasma is such that it concentrates the current density in two cone-shaped regions along the spine, thus concentrating the twist of the magnetic field around the spine, leaving a radial configuration in the fan plane. The plasma pressure redistributes in order to maintain the current density accumulations. However, it is found that changes in the initial plasma pressure do not modify the final state significantly. In the cases where the initial magnetic field is not axi-symmetric, a infinite-time singularity of current perpendicular to the fan is found at the location of the null.
dc.format.extent9
dc.language.isoeng
dc.relation.ispartofAstronomy & Astrophysicsen
dc.rightsCopyright, ESO 2012.en
dc.subjectMagnetohydrodynamic (MHD)en
dc.subjectCoronaen
dc.subjectMagnetic topologyen
dc.subjectMagnetic reconnectionen
dc.subjectQC Physicsen
dc.subject.lccQCen
dc.titleMagnetohydrodynamics dynamical relaxation of coronal magnetic fields : III. 3D spiral nullsen
dc.typeJournal articleen
dc.description.versionPostprinten
dc.contributor.institutionUniversity of St Andrews. Applied Mathematicsen
dc.identifier.doihttps://doi.org/10.1051/0004-6361/201219190
dc.description.statusPeer revieweden


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