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The emergence of weakly twisted magnetic fields in the Sun
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dc.contributor.author | Archontis, Vasilis | |
dc.contributor.author | Hood, Alan William | |
dc.contributor.author | Tsinganos, K | |
dc.date.accessioned | 2014-08-14T11:01:03Z | |
dc.date.available | 2014-08-14T11:01:03Z | |
dc.date.issued | 2013-11-01 | |
dc.identifier.citation | Archontis , V , Hood , A W & Tsinganos , K 2013 , ' The emergence of weakly twisted magnetic fields in the Sun ' , Astronomical Journal , vol. 778 , no. 1 , 42 . https://doi.org/10.1088/0004-637X/778/1/42 | en |
dc.identifier.issn | 0004-6256 | |
dc.identifier.other | PURE: 101364093 | |
dc.identifier.other | PURE UUID: d5f2b873-dd83-433a-845a-fe21b74d1958 | |
dc.identifier.other | Scopus: 84887583749 | |
dc.identifier.other | ORCID: /0000-0003-2620-2068/work/58055191 | |
dc.identifier.other | ORCID: /0000-0002-6926-8676/work/73700863 | |
dc.identifier.uri | https://hdl.handle.net/10023/5151 | |
dc.description | The simulations were performed on the STFC and SRIF funded UKMHD cluster, at the University of St Andrews. K.T. and V.A. acknowledge EU support (IEF-272549 grant). | en |
dc.description.abstract | We have studied the emergence of a weakly twisted magnetic flux tube from the upper convection zone into the solar atmosphere. It is found that the rising magnetized plasma does not undergo the classical, single Ω-shaped loop emergence, but it becomes unstable in two places, forming two magnetic lobes that are anchored in small-scale bipolar structures at the photosphere, between the two main flux concentrations. The two magnetic lobes rise and expand into the corona, forming an overall undulating magnetic flux system. The dynamical interaction of the lobes results in the triggering of high-speed and hot jets and the formation of successive cool and hot loops that coexist in the emerging flux region. Although the initial emerging field is weakly twisted, a highly twisted magnetic flux rope is formed at the low atmosphere, due to shearing and reconnection. The new flux rope (hereafter post-emergence flux rope) does not erupt. It remains confined by the overlying field. Although there is no ejective eruption of the post-emergence rope, it is found that a considerable amount of axial and azimuthal flux is transferred into the solar atmosphere during the emergence of the magnetic field. | |
dc.format.extent | 15 | |
dc.language.iso | eng | |
dc.relation.ispartof | Astronomical Journal | en |
dc.rights | © 2013. The American Astronomical Society. All rights reserved. | en |
dc.subject | Sun: activity | en |
dc.subject | Sun: magnetic fields | en |
dc.subject | QB Astronomy | en |
dc.subject.lcc | QB | en |
dc.title | The emergence of weakly twisted magnetic fields in the Sun | en |
dc.type | Journal article | en |
dc.contributor.sponsor | Science & Technology Facilities Council | en |
dc.description.version | Publisher PDF | en |
dc.contributor.institution | University of St Andrews. Applied Mathematics | en |
dc.identifier.doi | https://doi.org/10.1088/0004-637X/778/1/42 | |
dc.description.status | Peer reviewed | en |
dc.identifier.grantnumber | ST/K000950/1 | en |
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