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Brightening of onset arc precedes the dipolarization onset: THEMIS observations of two events on 1 March 2008

机译:起弧弧变亮先于双极化起弧:THEMIS观测到2008年3月1日发生的两个事件

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We present a new M-I coupling model of substorm duringsouthward IMF based on the THEMIS observations of two events on 1 March2008. The first event (E-1) was classified as a pseudo-breakup: brighteningof the onset arc preceded the first dipolarization onset by ∼71 ± 3 s,but the breakup arcs faded within ∼5 min without substantialpoleward expansion and the dipolarization stopped and reversed to thinning.The second event (E-2) was identified as a substorm: brightening of thesecond onset arc preceded the second dipolarization onset by ∼80 ± 3 s, leading to a full-scale expanding auroral bulge during the substormexpansion phase for ∼20 min. The Alfvén travel time from theionosphere to the dipolarization onset region is estimated at ∼69.3 sin E-1; at ∼80.3 s in E-2, which matched well with the observedtime delay of the dipolarization onset after the brightening of the onsetarc, respectively in E-1 and E-2. Brightening of the onset arc precedes thedipolarization onset suggest that the onset arc brightening is caused by theintense upward field-aligned currents originating from the divergence of theCowling electrojet in the ionosphere. The Cowling electrojet current loop(CECL) is formed to close the field-aligned currents at all times. Theclosure current in the Alfvén wavefront is anti-parallel to thecross-tail current. Dipolarization onset occurs when the Alfvénwavefront incident on the near-Earth plasma sheet to disrupt the cross-tailcurrent in the dipolarization region. Slow MHD waves dominate the disruptionof the cross-tail current in the dipolarization region.
机译:我们根据2008年3月1日对两个事件的THEMIS观测结果,提出了一个新的M-I耦合模式,用于南向IMF。第一个事件(E-1)被归类为伪破裂:起弧弧的增亮在第一次双极化起弧之前〜71± 3 s,但破裂弧在约5分钟内消失,没有明显的极点扩张,并且偶极极化停止并反转为变薄。第二个事件(E-2)被确认为是亚暴:第二个爆发弧的变亮先于第二个偶极极化发生了〜 80± 3 s,导致在次暴雨扩展阶段约20分钟内,全方位扩大了极光凸起。从电离层到双极化起始区域的Alfvén传播时间估计约为69.3 sin E-1; E-2和E-2分别在E-2的约80.3 s处与双极起效的延迟时间相吻合。起始电弧的增亮先于双极化起始,这表明起始电弧的增亮是由电离层中Cowling电喷发散所产生的向上向上的场对准电流引起的。整流罩电喷电流回路(CECL)形成为始终关闭磁场对准的电流。 Alfvén波前的闭合电流与交叉尾电流反向平行。当Alfvén波前入射到近地等离子体片上时,会破坏双极化区域中的交叉尾电流,从而发生双极化。慢的MHD波主导着双极化区域交叉尾电流的破坏。

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