Malyshkin Leonid M
Department of Astronomy and Astrophysics, University of Chicago, 5640 South Ellis Avenue, Chicago, Illinois 60637, USA.
Phys Rev Lett. 2008 Nov 28;101(22):225001. doi: 10.1103/PhysRevLett.101.225001. Epub 2008 Nov 24.
The rate of quasistationary, two-dimensional magnetic reconnection is calculated in the framework of incompressible Hall magnetohydrodynamics, which includes the Hall and electron pressure terms in Ohm's law. The Hall-magnetohydrodynamics equations are solved in a local region across the reconnection electron layer, including only the upstream region and the layer center. In the case when the ion inertial length di is larger than the Sweet-Parker reconnection layer thickness, the dimensionless reconnection rate is found to be independent of the electrical resistivity and equal to di/L, where L is the scale length of the external magnetic field in the upstream region outside the electron layer and the ion layer thickness is found to be di.
在不可压缩的霍尔磁流体动力学框架内计算准静态二维磁重联速率,该框架在欧姆定律中包含霍尔项和电子压力项。在重联电子层的局部区域求解霍尔磁流体动力学方程,该区域仅包括上游区域和层中心。当离子惯性长度di大于斯威特 - 帕克重联层厚度时,发现无量纲重联速率与电阻率无关,且等于di/L,其中L是电子层和离子层之外上游区域外部磁场的尺度长度,离子层厚度为di。