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Two-dimensional MHD model of the reconnection diffusion region
1Institute of Computational Modelling, Russian Academy of Sciences, Krasnoyarsk, 660036, Russia
2Institute of Physics, University of St. Petersburg, St. Petergof, 198504, Russia
3Space Research Institute, Austrian Academy of Sciences, Schmiedlstrasse 6, Graz, A-8042, Austria
Abstract. Magnetic reconnection is an important process providing a fast conversion of magnetic energy into thermal and kinetic plasma energy. In this concern, a key problem is that of the resistive diffusion region where the reconnection process is initiated. In this paper, the diffusion region is associated with a nonuniform conductivity localized to a small region. The nonsteady resistive incompressible MHD equations are solved numerically for the case of symmetric reconnection of antiparallel magnetic fields. A Petschek type steady-state solution is obtained as a result of time relaxation of the reconnection layer structure from an arbitrary initial stage. The structure of the diffusion region is studied for various ratios of maximum and minimum values of the plasma resistivity. The effective length of the diffusion region and the reconnection rate are determined as functions of the length scale and the maximum of the resistivity. For sufficiently small length scale of the resistivity, the reconnection rate is shown to be consistent with Petschek's formula. By increasing the resistivity length scale and decreasing the resistivity maximum, the reconnection layer tends to be wider, and correspondingly, the reconnection rate tends to be more consistent with that of the Parker-Sweet regime.
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Citation: Erkaev, N. V., Semenov, V. S., and Biernat, H. K.: Two-dimensional MHD model of the reconnection diffusion region, Nonlin. Processes Geophys., 9, 131-138, 2002. Bibtex EndNote Reference Manager
