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不同磁暴條件下GEO衛(wèi)星表面充電電位分布(英文)

Distribution of spacecraft surface charging potential in plasma sheet at geosynchronous orbit during geomagnetic storms

  • 摘要: 文章利用1989-2004年間“Los Alamos”7 顆地球同步軌道衛(wèi)星的數(shù)據(jù)對不同磁暴條件下處于地球同步軌道高度等離子體片區(qū)域的衛(wèi)星表面充電電位和熱電子(0.03~45 keV)溫度隨地方時的分布及隨磁暴發(fā)生時間的變化規(guī)律進(jìn)行統(tǒng)計(jì)分析。根據(jù)對磁層頂電流修正后的Dst指數(shù)(Dst*)將磁暴分成弱磁暴、強(qiáng)磁暴以及超大磁暴。在隨地方時的分布上,弱磁暴時衛(wèi)星最可能在午夜后側(cè)負(fù)向強(qiáng)充電(>800 V);隨著磁暴強(qiáng)度的增加,在超大磁暴情況下該區(qū)域會沿東西方向擴(kuò)展到夜晚21時到凌晨4時的區(qū)域。在隨磁暴發(fā)生時間的分布上,弱磁暴下衛(wèi)星表面充電到高負(fù)電位主要發(fā)生在Dst*最低點(diǎn)前3 h和后2 h的時刻,強(qiáng)磁暴下主要發(fā)生在Dst*最低點(diǎn)時刻,而超大磁暴下主要發(fā)生在恢復(fù)相,持續(xù)時間達(dá)十幾個小時。表面電位的分布規(guī)律和熱電子溫度的分布規(guī)律表現(xiàn)一致:衛(wèi)星表面負(fù)電位超過100 V的區(qū)域主要集中在熱電子溫度大于2 keV的區(qū)域,而表面負(fù)電位最可能超過800 V的區(qū)域主要集中在熱電子溫度大于2.5 keV的區(qū)域。通過統(tǒng)計(jì)分析看出,對于那些極可能發(fā)生高負(fù)電位充電(>8 kV)情況下的衛(wèi)星表面電位分布與磁暴的強(qiáng)弱并無明顯的相關(guān)性,但發(fā)現(xiàn)在弱磁暴情況下明顯集中在正午前側(cè)區(qū)域。

     

    Abstract: The 16 years’ accumulation of magnetospheric plasma analyzer data from seven Los Alamos geosynchronous satellites is used for a statistical study on the hot electron temperature (0.03~45 keV) and the spacecraft (S/C) surface sunlit charging potential in the plasma sheet region at the geosynchronous orbit and their dependence on the local time (LT) and the epoch time (ET) with respect to storms of three categories: moderate, intense and super storms, based on different geomagnetic activity levels as measured by Dst index corrected by the solar wind dynamic pressure. As a function of LT and three categories of storms, the measured S/C surface charging potential is shown with distinct spatial and temporal distributions well consistent with hot electron temperature behaviors. The area of the most probable charging and of a high negative level expands following a systematic trend with increasing storm size, and the post-midnight region for moderate storms will expand to the LT=21~04 region for super storms. The most probable charging with a high negative level dominates at about 3 hours before and 2 hours after the moderate storm peak, just at the intense storm peak and in the recovery phase of the super storms. However, there is no systematic relations between a large negative charging (>8 kV) and the magnitude of storms as evidenced in this study; it can occur in all geomagnetic activity levels and perhaps more likely in the pre-noon sector during the moderate storm peak time.

     

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