Solar wind interaction with the Earth's magnetosphere: the role of reconnection in the presence of a large scale sheared flow

The Earth's magnetosphere and solar wind environment is a laboratory of excellence for the study of the physics of collisionless magnetic reconnection. At low latitude magnetopause, magnetic reconnection develops as a secondary instability due to the stretching of magnetic field lines advec...

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Main Authors: F. Califano, M. Faganello, F. Pegoraro, F. Valentini
Format: Article
Language:English
Published: Copernicus Publications 2009-01-01
Series:Nonlinear Processes in Geophysics
Online Access:http://www.nonlin-processes-geophys.net/16/1/2009/npg-16-1-2009.pdf
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spelling doaj-d0fea34fd77d448f9f51de28c81b26282020-11-24T21:08:50ZengCopernicus PublicationsNonlinear Processes in Geophysics1023-58091607-79462009-01-01161110Solar wind interaction with the Earth's magnetosphere: the role of reconnection in the presence of a large scale sheared flowF. CalifanoM. FaganelloF. PegoraroF. ValentiniThe Earth's magnetosphere and solar wind environment is a laboratory of excellence for the study of the physics of collisionless magnetic reconnection. At low latitude magnetopause, magnetic reconnection develops as a secondary instability due to the stretching of magnetic field lines advected by large scale Kelvin-Helmholtz vortices. In particular, reconnection takes place in the sheared magnetic layer that forms between adjacent vortices during vortex pairing. The process generates magnetic islands with typical size of the order of the ion inertial length, much smaller than the MHD scale of the vortices and much larger than the electron inertial length. The process of reconnection and island formation sets up spontaneously, without any need for special boundary conditions or initial conditions, and independently of the initial in-plane magnetic field topology, whether homogeneous or sheared. http://www.nonlin-processes-geophys.net/16/1/2009/npg-16-1-2009.pdf
collection DOAJ
language English
format Article
sources DOAJ
author F. Califano
M. Faganello
F. Pegoraro
F. Valentini
spellingShingle F. Califano
M. Faganello
F. Pegoraro
F. Valentini
Solar wind interaction with the Earth's magnetosphere: the role of reconnection in the presence of a large scale sheared flow
Nonlinear Processes in Geophysics
author_facet F. Califano
M. Faganello
F. Pegoraro
F. Valentini
author_sort F. Califano
title Solar wind interaction with the Earth's magnetosphere: the role of reconnection in the presence of a large scale sheared flow
title_short Solar wind interaction with the Earth's magnetosphere: the role of reconnection in the presence of a large scale sheared flow
title_full Solar wind interaction with the Earth's magnetosphere: the role of reconnection in the presence of a large scale sheared flow
title_fullStr Solar wind interaction with the Earth's magnetosphere: the role of reconnection in the presence of a large scale sheared flow
title_full_unstemmed Solar wind interaction with the Earth's magnetosphere: the role of reconnection in the presence of a large scale sheared flow
title_sort solar wind interaction with the earth's magnetosphere: the role of reconnection in the presence of a large scale sheared flow
publisher Copernicus Publications
series Nonlinear Processes in Geophysics
issn 1023-5809
1607-7946
publishDate 2009-01-01
description The Earth's magnetosphere and solar wind environment is a laboratory of excellence for the study of the physics of collisionless magnetic reconnection. At low latitude magnetopause, magnetic reconnection develops as a secondary instability due to the stretching of magnetic field lines advected by large scale Kelvin-Helmholtz vortices. In particular, reconnection takes place in the sheared magnetic layer that forms between adjacent vortices during vortex pairing. The process generates magnetic islands with typical size of the order of the ion inertial length, much smaller than the MHD scale of the vortices and much larger than the electron inertial length. The process of reconnection and island formation sets up spontaneously, without any need for special boundary conditions or initial conditions, and independently of the initial in-plane magnetic field topology, whether homogeneous or sheared.
url http://www.nonlin-processes-geophys.net/16/1/2009/npg-16-1-2009.pdf
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