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首页> 外文期刊>Journal of Geophysical Research, A. Space Physics: JGR >Isothermalmagnetosheath electrons due to nonlocal electron cross talk
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Isothermalmagnetosheath electrons due to nonlocal electron cross talk

机译:由于外地Isothermalmagnetosheath电子电子相声

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Heating of the various plasma species at the Earth’s collisionless bow shock is not fully understood. Although the total amount of heating is constrained by the one-fluid Rankine-Hugoniot relations in terms of local plasma conditions, the partition of energy between, e.g., electrons and ions, is influenced by particle kinetics which are not considered in the Rankine-Hugoniot approach. Additionally, in this paper we demonstrate the impact of nonlocal effects. Here we model the effects of shock-heated electrons which traverse the magnetosheath to arrive at another point on the bow shock surface. We construct the distribution of electrons immediately downstream of each point on the bow shock from two populations: local solar wind electrons entering the magnetosheath for the first time and previously shocked electrons which have traversed the magnetosheath. We determine the self-consistent cross-shock potential at each point such that the resulting electron distribution gives a downstream plasma which is neutral and has zero parallel current. This leads to very little variation in the downstream electron temperature everywhere around the curved bow shock, in spite of large differences in the total (Rankine-Hugoniot) downstream temperature. Consequently, the partition of heating between electrons and ions at the shock, i.e., the equation of state, contains nonlocal contributions. We show that heating properties at the point where the shock is exactly perpendicular controls electron heating throughout the rest of the shock surface.
机译:加热的各种等离子体物种地球的无碰撞的弓形激波并不充分理解。由单一流体受限兰金雨贡纽关系的当地的等离子体条件下,分区之间的能量,例如,电子和离子受粒子动力学的影响兰金雨贡纽不考虑吗的方法。证明非局部效应的影响。我们的模型shock-heated电子的影响遍历磁鞘到达另一个点的弓形激波曲面。构建电子的分布立即弓上的每个点的下游冲击两个群体:当地的太阳风电子的磁鞘第一次和先前震惊电子穿过磁鞘。在每一个自洽的cross-shock潜力点,由此产生的电子分配给一个下游的等离子体中性和平行电流为零。在下游很少变化无处不在的电子温度曲线弓形激波,尽管巨大的差异总(兰金雨贡纽)下游温度。因此,分区之间的加热电子和离子的冲击,即状态方程,包含外地的贡献。是完全的冲击垂直控制电子加热在其余的冲击表面。

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