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首页> 外文期刊>Journal of Geophysical Research, A. Space Physics: JGR >A statistical study of plasma sheet electrons carrying auroral upward field-aligned currents measured by Time History of Events and Macroscale Interactions during Substorms (THEMIS)
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A statistical study of plasma sheet electrons carrying auroral upward field-aligned currents measured by Time History of Events and Macroscale Interactions during Substorms (THEMIS)

机译:对通过亚暴期间事件的时间历史和宏观相互作用进行测量的,带有极光向上场对准电流的等离子薄片电子的统计研究

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We have statistically investigated the electron density ne,M and temperature T_(e,M) in the near-Earth plasma sheet in terms of the magnetosphere-ionosphere coupling process, as measured by the electrostatic analyzer (ESA) on board the Time History of Events and Macroscale Interactions during Substorms (THEMIS-D) satellite from November 2007 to January 2010. To find out when and where an aurora can occur, either with or without electron acceleration, the thermal current j_∥~(th) and the conductivity K along the magnetic field line were also estimated from observations of the magnetospheric electrons with pitch angle information inside 12 RE. The thermal current, j_∥~(th)(∝ n_(e,M) T_(e,M)~(1/2) ), represents the upper limit of the field-aligned current that can be carried by magnetospheric electrons without a field-aligned potential difference. The conductivity, K(∝ n_(e,M) T_(e,M)~(1/2)), relates the upward field-aligned current, j_∥, to the field-aligned potential difference, V_∥, assuming adiabatic electron transport. The thermal current is estimated by two methods: (1) from the relation by using n_(e,M) and T_(e,M) and (2) from the total downward electron number flux. We find that in the dawnside inner magnetosphere, the thermal currents estimated by both methods are sufficient to carry typical region 2 upward field-aligned current. On the other hand, in the duskside outer magnetosphere, a field-aligned potential difference is necessary on the region 1 current since the estimated thermal current is smaller than the typical region 1 current. By using the relationship, j_∥ = KV_∥, where K is the conductivity estimated from Knight’s relation and j-∥ is the typical auroral current, we conclude that a field-aligned potential difference of V_∥ = 2–5 kV is necessary on the duskside region 1 upward field-aligned current.
机译:我们已经根据磁层-电离层耦合过程,通过静电分析仪(ESA)的时间历程,对近地等离子体片中的电子密度ne,M和温度T_(e,M)进行了统计研究。 2007年11月至2010年1月在亚暴期间(THEMIS-D)卫星发生的事件和宏观相互作用。为了弄清何时和何地发生极光(无论是否具有电子加速),热电流j_∥〜(th)和电导率K还通过对磁层电子的观测以及在12 RE内的俯仰角信息来估计沿磁场线的磁场。热电流j_∥〜(th)(∝ n_(e,M)T_(e,M)〜(1/2))代表了磁层电子可以在不存在磁场的情况下携带的场取向电流的上限场对准电位差。假设绝热,电导率K(,n_(e,M)T_(e,M)〜(1/2))将向上的场对准电流j_∥与场对准的电位差V_∥相关电子传输。通过两种方法估算热电流:(1)根据关系使用n_(e,M)和T_(e,M),以及(2)根据总向下电子数通量。我们发现在黎明边的内部磁层中,通过两种方法估算的热电流足以承载典型的区域2向上的磁场对准电流。另一方面,在黄昏侧外磁层中,由于估计的热电流小于典型的区域1电流,因此在区域1电流上需要场取向的电势差。通过使用关系式j_∥=KV_∥,其中K是根据奈特关系估计的电导率,而j-∥是典型的极光电流,我们得出结论,在V_∥= 2–5 kV的情况下,需要在场上对准电势差黄昏侧区域1向上的场对准电流。

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