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首页> 外文期刊>Journal of Geophysical Research, A. Space Physics: JGR >Diagnostics of Closed Magnetic Flux Depletion in the Near-Earth Magnetotail During the Substorm Growth Phase
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Diagnostics of Closed Magnetic Flux Depletion in the Near-Earth Magnetotail During the Substorm Growth Phase

机译:诊断近地磁磁铁中近乎磁磁磁靶机的诊断

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Based on magnetohydrodynamics simulations, it was recently suggested that magnetotail reconfiguration during the substorm growth phase results from combined action of two large-scale processes: (1) open magnetic flux accumulation (OMFA) in the tail lobes and (2) closed magnetic flux depletion (CMFD) in the near-Earth tail, caused by flux evacuation to the dayside magnetopause. Simultaneous action of uniform along the tail OMFA and strongly nonuniform CMFD leads to different rates of magnetic flux growth in different tail cross sections. According to Global magnetohydrodynamics simulations CMFD is about 35% of OMFA, the corresponding differences of magnetic flux increase in two-tail cross sections at -7R_E and -20R_E being as large as 0.1–0.2 GWb. To study this effect on real data, we applied the recent method of magnetotail flux estimation (Shukhtina et al., 2016) to simultaneous Cluster and Geotail observations in the tail lobes. By finding such rare observations in the inner and middle magnetotail (at -10 R_E and - 21R_E) we confirm a larger magnetic flux increase in the midtail, with the ratio between OMFA and CMFD comparable to that obtained in magnetohydrodynamics, although with a large scatter. These results confirm the scenario of two decoupled magnetotail regions with different convection regimes during the growth phase. Convection is depressed in the midtail plasma sheet, showing the pressure crisis in action inherent to tail-like 2-D magnetic configuration. At the same time convection is substantially enhanced in the inner magnetosphere, where the pressure crisis is solved due to azimuthal flux transport around the Earth, essentially a 3-D effect.
机译:基于磁性动力学模拟,最近建议在磁靶期间重新配置两种大规模过程的组合作用:(1)在尾叶中的开放磁通量(OMFA)和(2)闭合磁通量消耗(CMFD)在近地尾巴中,由助焊剂疏散引起的磁通磁性常规引起。沿着尾部OMFA和强不均匀CMFD的同时作用导致不同尾部横截面中的磁通量生长的不同速率。根据全局磁力流体动力学模拟,CMFD约为OMFA的35%,在-7R_E和-20R_E处的双尾横截面中磁通量增加的相应差异为0.1-0.2 GWB。为研究实际数据的这种影响,我们将最近的磁幂磁通估计方法(Shukhtina等,2016)应用于尾叶中的同时簇和地理箱观测。通过在内磁靶(在<> -10 r_e和-21r_e)中找到如此罕见的观察,我们确认了中间锆中的较大磁通量增加,OMFA和CMFD之间的比率与磁性流体动力学中获得的比率相当,尽管一个大的散射。这些结果证实了在生长阶段期间具有不同对流制度的两个分离磁船区域的场景。在MidTail等离子片中抑制了对流,显示了尾状2-D磁性配置固有的动作中的压力危机。在同一时,内磁层中基本上增强了对流,其中压力危机由于地球周围的方位传递,基本上是3D效应。

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