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THEMIS two‐point measurements of the cross‐tail current density: A thick bifurcated current sheet in the near‐Earth plasma sheet

机译:THEMIS交叉尾电流密度的两点测量:近地等离子体板中的厚分叉电流板

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摘要

The basic properties of the near‐Earth current sheet from 8 RE to 12 RE were determined based on Time History of Events and Macroscale Interactions during Substorms (THEMIS) observations from 2007 to 2013. Ampere's law was used to estimate the current density when the locations of two spacecraft were suitable for the calculation. A total of 3838 current density observations were obtained to study the vertical profile. For typical solar wind conditions, the current density near (off) the central plane of the current sheet ranged from 1 to 2 nA/m2 (1 to 8 nA/m2). All the high current densities appeared off the central plane of the current sheet, indicating the formation of a bifurcated current sheet structure when the current density increased above 2 nA/m2. The median profile also showed a bifurcated structure, in which the half thickness was about 3 RE. The distance between the peak of the current density and the central plane of the current sheet was 0.5 to 1 RE. High current densities above 4 nA/m2 were observed in some cases that occurred preferentially during substorms, but they also occurred in quiet times. In contrast to the commonly accepted picture, these high current densities can form without a high solar wind dynamic pressure. In addition, these high current densities can appear in two magnetic configurations: tail‐like and dipolar structures. At least two mechanisms, magnetic flux depletion and new current system formation during the expansion phase, other than plasma sheet compression are responsible for the formation of the bifurcated current sheets.
机译:根据2007年至2013年亚暴期间的事件和宏观尺度相互作用的时间历程(THEMIS)观测,确定了从8 RE到12 nearRE的近地电流表的基本特性。安培定律用于估计位置时的电流密度两个航天器中有一个适合进行计算。总共进行了3838次电流密度观测,以研究垂直剖面。对于典型的太阳风条件,靠近(离开)电流表中心平面的电流密度范围为1至2AnA / m 2 (1至8 nA / m 2 )。所有高电流密度都出现在电流板的中心平面以外,表明当电流密度增加到2 nA / m 2 时,形成了分叉的电流板结构。中线轮廓也显示出分叉的结构,其中一半厚度约为3 RE。电流密度的峰值与电流片的中心平面之间的距离为0.5至1 RE。在某些情况下,观察到高电流密度高于4 nA / m 2 ,这些电流优先发生在亚暴期间,但也发生在安静时期。与通常接受的图像相反,这些高电流密度可以在没有高太阳风动压的情况下形成。此外,这些高电流密度可能以两种磁性结构出现:尾状和偶极结构。至少两个机制,即等离子板压缩以外的膨胀阶段的磁通损耗和新的电流系统形成是造成分叉电流板形成的原因。

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