Filament interaction modeled by flux rope reconnection

Hα observations of solar active region NOAA 10501 on 2003 November 20 revealed a very uncommon dynamic process: during the development of a nearby flare, two adjacent elongated filaments approached each other, merged at their middle sections, and separated again, thereby forming stable configuration...

Descripción completa

Guardado en:
Detalles Bibliográficos
Autores principales: Török, T., Chandra, R., Pariat, E., Démoulin, P., Schmieder, B., Aulanier, G., Linton, M.G., Mandrini, C.H.
Formato: Artículo publishedVersion
Publicado: 2011
Materias:
Acceso en línea:http://hdl.handle.net/20.500.12110/paper_0004637X_v728_n1_p_Torok
https://repositoriouba.sisbi.uba.ar/gsdl/cgi-bin/library.cgi?a=d&c=artiaex&d=paper_0004637X_v728_n1_p_Torok_oai
Aporte de:
id I28-R145-paper_0004637X_v728_n1_p_Torok_oai
record_format dspace
spelling I28-R145-paper_0004637X_v728_n1_p_Torok_oai2024-08-16 Török, T. Chandra, R. Pariat, E. Démoulin, P. Schmieder, B. Aulanier, G. Linton, M.G. Mandrini, C.H. 2011 Hα observations of solar active region NOAA 10501 on 2003 November 20 revealed a very uncommon dynamic process: during the development of a nearby flare, two adjacent elongated filaments approached each other, merged at their middle sections, and separated again, thereby forming stable configurations with new footpoint connections. The observed dynamic pattern is indicative of "slingshot" reconnection between two magnetic flux ropes. We test this scenario by means of a three-dimensional zero β magnetohydrodynamic simulation, using a modified version of the coronal flux rope model by Titov and Démoulin as the initial condition for the magnetic field. To this end, a configuration is constructed that contains two flux ropes which are oriented side-by-side and are embedded in an ambient potential field. The choice of the magnetic orientation of the flux ropes and of the topology of the potential field is guided by the observations. Quasi-static boundary flows are then imposed to bring the middle sections of the flux ropes into contact. After sufficient driving, the ropes reconnect and two new flux ropes are formed, which now connect the former adjacent flux rope footpoints of opposite polarity. The corresponding evolution of filament material is modeled by calculating the positions of field line dips at all times. The dips follow the morphological evolution of the flux ropes, in qualitative agreement with the observed filaments. © 2011. The American Astronomical Society. All rights reserved. Printed in the U.S.A. Fil:Mandrini, C.H. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina. application/pdf http://hdl.handle.net/20.500.12110/paper_0004637X_v728_n1_p_Torok info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar Astrophys. J. 2011;728(1) Methods: numerical Sun: corona Sun: filaments, prominences Filament interaction modeled by flux rope reconnection info:eu-repo/semantics/article info:ar-repo/semantics/artículo info:eu-repo/semantics/publishedVersion https://repositoriouba.sisbi.uba.ar/gsdl/cgi-bin/library.cgi?a=d&c=artiaex&d=paper_0004637X_v728_n1_p_Torok_oai
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-145
collection Repositorio Digital de la Universidad de Buenos Aires (UBA)
topic Methods: numerical
Sun: corona
Sun: filaments, prominences
spellingShingle Methods: numerical
Sun: corona
Sun: filaments, prominences
Török, T.
Chandra, R.
Pariat, E.
Démoulin, P.
Schmieder, B.
Aulanier, G.
Linton, M.G.
Mandrini, C.H.
Filament interaction modeled by flux rope reconnection
topic_facet Methods: numerical
Sun: corona
Sun: filaments, prominences
description Hα observations of solar active region NOAA 10501 on 2003 November 20 revealed a very uncommon dynamic process: during the development of a nearby flare, two adjacent elongated filaments approached each other, merged at their middle sections, and separated again, thereby forming stable configurations with new footpoint connections. The observed dynamic pattern is indicative of "slingshot" reconnection between two magnetic flux ropes. We test this scenario by means of a three-dimensional zero β magnetohydrodynamic simulation, using a modified version of the coronal flux rope model by Titov and Démoulin as the initial condition for the magnetic field. To this end, a configuration is constructed that contains two flux ropes which are oriented side-by-side and are embedded in an ambient potential field. The choice of the magnetic orientation of the flux ropes and of the topology of the potential field is guided by the observations. Quasi-static boundary flows are then imposed to bring the middle sections of the flux ropes into contact. After sufficient driving, the ropes reconnect and two new flux ropes are formed, which now connect the former adjacent flux rope footpoints of opposite polarity. The corresponding evolution of filament material is modeled by calculating the positions of field line dips at all times. The dips follow the morphological evolution of the flux ropes, in qualitative agreement with the observed filaments. © 2011. The American Astronomical Society. All rights reserved. Printed in the U.S.A.
format Artículo
Artículo
publishedVersion
author Török, T.
Chandra, R.
Pariat, E.
Démoulin, P.
Schmieder, B.
Aulanier, G.
Linton, M.G.
Mandrini, C.H.
author_facet Török, T.
Chandra, R.
Pariat, E.
Démoulin, P.
Schmieder, B.
Aulanier, G.
Linton, M.G.
Mandrini, C.H.
author_sort Török, T.
title Filament interaction modeled by flux rope reconnection
title_short Filament interaction modeled by flux rope reconnection
title_full Filament interaction modeled by flux rope reconnection
title_fullStr Filament interaction modeled by flux rope reconnection
title_full_unstemmed Filament interaction modeled by flux rope reconnection
title_sort filament interaction modeled by flux rope reconnection
publishDate 2011
url http://hdl.handle.net/20.500.12110/paper_0004637X_v728_n1_p_Torok
https://repositoriouba.sisbi.uba.ar/gsdl/cgi-bin/library.cgi?a=d&c=artiaex&d=paper_0004637X_v728_n1_p_Torok_oai
work_keys_str_mv AT torokt filamentinteractionmodeledbyfluxropereconnection
AT chandrar filamentinteractionmodeledbyfluxropereconnection
AT pariate filamentinteractionmodeledbyfluxropereconnection
AT demoulinp filamentinteractionmodeledbyfluxropereconnection
AT schmiederb filamentinteractionmodeledbyfluxropereconnection
AT aulanierg filamentinteractionmodeledbyfluxropereconnection
AT lintonmg filamentinteractionmodeledbyfluxropereconnection
AT mandrinich filamentinteractionmodeledbyfluxropereconnection
_version_ 1809357049670139904