首页> 外文期刊>Journal of Geophysical Research, A. Space Physics: JGR >Modeling magnetospheric current response to solar wind dynamic pressure enhancements during magnetic storms: 2. Application to different storm phases
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Modeling magnetospheric current response to solar wind dynamic pressure enhancements during magnetic storms: 2. Application to different storm phases

机译:模拟磁暴期间磁层电流对太阳风动态压力增强的响应:2.在不同风暴阶段的应用

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摘要

Two patterns of ground H perturbation as response to pressure enhancements during different phases of storms are found. One is polarity asymmetry under southward IMF B z , e.g., 25 September 1998, 29 May 2003, and 10 January 1997 events; the other is positive H perturbation everywhere under northward IMF B z , e.g., 7 November 2000 event. The polarity asymmetry can be further divided into two categories: dawn-dusk asymmetry with negative H perturbation at dusk extending through noon to late morning (25 September 1998 event) and positive H perturbation elsewhere, and day-night asymmetry with a smaller region of negative H perturbation extending less far toward dusk (29 May 2003 and 10 January 1997 events). The net field-aligned current (FAC) system from the R1, R2, and the partial ring current (PRC) closure FAC, the equatorial portion of the PRC, and Chapman-Ferraro (CF) current are responsible for the polarity asymmetry. The stronger effect of the R1 is primarily responsible for the negative H perturbation at noon and positive at midnight. The PRC strength at the onset of pressure enhancements determines how far the negative H perturbation at noon extends toward dusk and which pattern is most likely. A stronger (weaker) PRC extends negative H perturbation more (less) toward dusk and thus increases the likelihood of dawn-dusk (day-night) asymmetry. Positive H perturbation everywhere results from the dominant contribution of the CF and lack of significant preexisting PRC and R1 and R2.
机译:发现了两种形式的地面H摄动,作为风暴不同阶段对压力增强的响应。一种是在IMF B z向南的情况下的极性不对称,例如1998年9月25日,2003年5月29日和1997年1月10日的事件;另一个是在北向IMF B z下(例如2000年11月7日的事件)处的正H摄动。极性不对称性可进一步分为两类:黎明至黄昏的不对称性,在黄昏到整个中午到清晨(1998年9月25日的事件)的负H扰动和其他地方的正H扰动,以及昼夜不对称,负值较小H扰动向黄昏延伸的距离较小(2003年5月29日和1997年1月10日的事件)。来自R1,R2的净磁场对准电流(FAC)系统以及部分环电流(PRC)闭合FAC,中华人民共和国的赤道部分和查普曼-费拉罗(CF)电流是极性不对称的原因。 R1的较强作用主要是造成中午负H扰动和午夜正H扰动。压力增强开始时的PRC强度决定了中午负H扰动向黄昏延伸的程度以及最有可能的模式。较强的(较弱的)PRC将负H扰动更多(较少)扩展到黄昏,因此增加了黎明黄昏(昼夜)不对称的可能性。到处都是正H扰动,这是因为CF的主要贡献以及缺乏明显的预先存在的PRC和R1和R2。

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