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Spreading of electron scale magnetic reconnection with a wave number dependent speed due to the propagation of dispersive waves

机译:由于分散波的传播,带有波数依赖性速度的电子秤磁性重新连接

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摘要

In this work, we study electron scale spreading of localized magnetic reconnection in the presence of a guide magnetic field, however, without the influence of ions and cross-scale coupling. These fundamental physics studies will help to understand the coupling of the electron scale spreading with the ion scales in real systems. An electron-magnetohydrodynamic (EMHD) model is employed to model the physics at electron scales. Three dimensional EMHD simulations and linear eigen mode analysis are performed for different guide field strengths. The simulations show a wave-like bi-directional spreading of magnetic reconnection at electron scales. The electron scale spreading, however, unlike the ion scale spreading by Alfven waves, is caused by the uni- and bidirectional propagation of the dispersive flow induced and whistler wave modes, respectively. The dispersive nature of the two wave modes makes the spreading-speed dependent on the wave numbers of the unstable tearing mode, which depend on the thickness of the electron current sheet and the strength of the guide field. A model of the speed of spreading is developed, in which the spreading-speeds parallel and anti-parallel to the guide field are given by linear combinations of the group speeds of the two wave modes. The model prediction of the spreading speeds agrees well with the speeds obtained from the simulation results. For small guide fields, the spreading is asymmetric being faster in the direction of the electron flow. On increasing the guide field, the spreading becomes increasingly symmetric, with the speeds of the order of electron Alfven speed in the guide magnetic field, due to the dominance of the whistler group speed in determining the speed of the spreading. As a consequence of the asymmetric spreading, the chain of alternate X-and O-points, formed due the growth of oblique tearing modes, extends farther in the direction of electron flow as compared to that in the direction of the guide magnetic field. Published by AIP Publishing.
机译:在这项工作中,我们研究了在导磁场的存在下局部磁性重新连接的电子尺度扩散,但是没有离子和交叉凝固耦合的影响。这些基本物理学研究将有助于了解电子秤与真实系统中的离子秤的耦合。使用电子磁力学(EMHD)模型来模拟电子秤的物理学。三维EMHD模拟和线性eIGEN模式分析用于不同的导场强度。模拟显示电子尺度磁重新连接的波形双向扩展。然而,与Alfven波的离子量表不同,电子秤扩散是由分散流动引起的和吹口波模式的单向和双向传播引起的。两波动模式的分散性质使得展开速度取决于不稳定的撕裂模式的波浪数,这取决于电子电流板的厚度和导轨的强度。开发了一种速度速度的模型,其中通过两波动模式的组速度的基准速度的线性组合给出平行和反平行于引导场的扩散速度。扩频速度的模型预测与从模拟结果获得的速度很好地吻合。对于小导磁场,展开在电子流方向上不对称。在增加引导栏上,扩展变得越来越对称,引导磁场中的电子ALFven速度顺序的速度,由于吹口机组速度在确定扩散的速度时。由于非对称扩展的结果,与倾斜撕裂模式的生长形成的交替X-o和O点的链,与导磁场的方向相比,在电子流方向上延伸。通过AIP发布发布。

著录项

  • 来源
    《Physics of plasmas》 |2017年第8期|共8页
  • 作者

    Jain Neeraj; Buechner Joerg;

  • 作者单位

    Max Planck Princeton Ctr Plasma Phys Max Planck Inst Solar Syst Res Justus von Liebig Weg 3 D-37077 Gottingen Germany;

    Max Planck Princeton Ctr Plasma Phys Max Planck Inst Solar Syst Res Justus von Liebig Weg 3 D-37077 Gottingen Germany;

  • 收录信息
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 等离子体物理学;
  • 关键词

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