Reconnection current sheet structure in a turbulent medium

In the presence of turbulence, magnetic field lines lose their dynamical identity and particles entrained on field lines diffuse through space at a rate determined by the amplitude of the turbulence. In previous work (Lazarian and Vishniac, 1999; Kowal et al., 2009; Eyink et al., 2011) we showed tha...

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Main Authors: E. T. Vishniac, S. Pillsworth, G. Eyink, G. Kowal, A. Lazarian, S. Murray
Format: Article
Language:English
Published: Copernicus Publications 2012-11-01
Series:Nonlinear Processes in Geophysics
Online Access:http://www.nonlin-processes-geophys.net/19/605/2012/npg-19-605-2012.pdf
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spelling doaj-4df88de486964549a7bd74c1786cccb72020-11-24T23:42:40ZengCopernicus PublicationsNonlinear Processes in Geophysics1023-58091607-79462012-11-0119660561010.5194/npg-19-605-2012Reconnection current sheet structure in a turbulent mediumE. T. VishniacS. PillsworthG. EyinkG. KowalA. LazarianS. MurrayIn the presence of turbulence, magnetic field lines lose their dynamical identity and particles entrained on field lines diffuse through space at a rate determined by the amplitude of the turbulence. In previous work (Lazarian and Vishniac, 1999; Kowal et al., 2009; Eyink et al., 2011) we showed that this leads to reconnection speeds which are independent of resistivity. In particular, in Kowal et al. (2009) we showed that numerical simulations were consistent with the predictions of this model. Here we examine the structure of the current sheet in simulations of turbulent reconnection. Laminar flows consistent with the Sweet-Parker reconnection model produce very thin and well ordered currents sheets. On the other hand, the simulations of Kowal et al. (2009) show a strongly disordered state even for relatively low levels of turbulence. Comparing data cubes with and without reconnection, we find that large scale field reversals are the cumulative effect of many individual eddies, each of which has magnetic properties which are not very different from turbulent eddies in a homogeneous background. This implies that the properties of stationary and homogeneous MHD turbulence are a reasonable guide to understanding turbulence during large scale magnetic reconnection events. In addition, dissipation and high energy particle acceleration during reconnection events take place over a macroscopic volume, rather than being confined to a narrow zone whose properties depend on microscopic transport coefficients.http://www.nonlin-processes-geophys.net/19/605/2012/npg-19-605-2012.pdf
collection DOAJ
language English
format Article
sources DOAJ
author E. T. Vishniac
S. Pillsworth
G. Eyink
G. Kowal
A. Lazarian
S. Murray
spellingShingle E. T. Vishniac
S. Pillsworth
G. Eyink
G. Kowal
A. Lazarian
S. Murray
Reconnection current sheet structure in a turbulent medium
Nonlinear Processes in Geophysics
author_facet E. T. Vishniac
S. Pillsworth
G. Eyink
G. Kowal
A. Lazarian
S. Murray
author_sort E. T. Vishniac
title Reconnection current sheet structure in a turbulent medium
title_short Reconnection current sheet structure in a turbulent medium
title_full Reconnection current sheet structure in a turbulent medium
title_fullStr Reconnection current sheet structure in a turbulent medium
title_full_unstemmed Reconnection current sheet structure in a turbulent medium
title_sort reconnection current sheet structure in a turbulent medium
publisher Copernicus Publications
series Nonlinear Processes in Geophysics
issn 1023-5809
1607-7946
publishDate 2012-11-01
description In the presence of turbulence, magnetic field lines lose their dynamical identity and particles entrained on field lines diffuse through space at a rate determined by the amplitude of the turbulence. In previous work (Lazarian and Vishniac, 1999; Kowal et al., 2009; Eyink et al., 2011) we showed that this leads to reconnection speeds which are independent of resistivity. In particular, in Kowal et al. (2009) we showed that numerical simulations were consistent with the predictions of this model. Here we examine the structure of the current sheet in simulations of turbulent reconnection. Laminar flows consistent with the Sweet-Parker reconnection model produce very thin and well ordered currents sheets. On the other hand, the simulations of Kowal et al. (2009) show a strongly disordered state even for relatively low levels of turbulence. Comparing data cubes with and without reconnection, we find that large scale field reversals are the cumulative effect of many individual eddies, each of which has magnetic properties which are not very different from turbulent eddies in a homogeneous background. This implies that the properties of stationary and homogeneous MHD turbulence are a reasonable guide to understanding turbulence during large scale magnetic reconnection events. In addition, dissipation and high energy particle acceleration during reconnection events take place over a macroscopic volume, rather than being confined to a narrow zone whose properties depend on microscopic transport coefficients.
url http://www.nonlin-processes-geophys.net/19/605/2012/npg-19-605-2012.pdf
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