Preliminary empirical model of inner boundary of ion plasma sheet

被引:6
|
作者
Cao, J. B. [1 ,2 ]
Zhang, D. [2 ,3 ]
Reme, H. [4 ,5 ]
Dandouras, I. [4 ,5 ]
Sauvaud, J. A. [4 ,5 ]
Fu, H. S. [1 ,2 ]
Wei, X. H. [2 ]
机构
[1] Beihang Univ, Space Sci Inst, Beijing 100191, Peoples R China
[2] Key Lab Space Weather NSSC, Beijing 100190, Peoples R China
[3] Chinese Acad Sci, Grad Univ, Beijing 100039, Peoples R China
[4] Univ Toulouse, UPS OMP, IRAP, Toulouse, France
[5] CNRS, IRAP, BP 44346, F-31028 Toulouse 4, France
关键词
Plasma sheet; Inner boundary; Magnetospheric convection; Kp index; Alfven layer; Empirical model; RING CURRENT DEVELOPMENT; GEOSYNCHRONOUS ORBIT; ELECTRIC-FIELDS; MAGNETOSPHERE; STORM; SPACECRAFT; CONVECTION; COLD; KP;
D O I
10.1016/j.asr.2015.06.017
中图分类号
V [航空、航天];
学科分类号
08 ; 0825 ;
摘要
The penetration of the plasma sheet into the inner magnetosphere is important to both ring current formation and spacecraft charging at geosynchronous orbit. This paper, using hot ion data recorded by HIA of TC-1/DSP, establishes an empirical model of the inner boundary of ion plasma sheet (IBIPS) on the near equatorial plane. All IBIPS are located inside geocentric radial distance of 9 RE. We divided local times (LT) into eight local time bins and found that during quiet times (Kp <= 2(-)), the IBIPS is closest to the Earth on the pre-midnight side (LT = 1930-2130) and farthest on the dawn side (LT = 0430-0730), which differs from previous spiral models. The geocentric radius of IBIPS in each local time bin can be described by a linear fitting function: R-ps = A + B-kp . Kp. The changing rate B-kp of the radius of IBIPS relative to Kp index on the midnight side (LT = 2230-0130) and post-night side (LT = 0130-0430) are the two largest (0.66 and 0.67), indicating that the IBIPS on the night side (LT = 2230-0430) moves fastest when Kp changes. Since the IBIPSs in different local times bins have different changing rates, both the size and shape of IBIPS change when Kp varies. The correlation coefficients between the radius of IBIPS and the instantaneous Kp increase with the increase of AT (the time difference between IBIPS crossing time and preceding Kp interval), which suggests that with the increase of Delta T, the radius of IBIPS is more and more controlled by instantaneous Kp, and the influence of preceding Kp becomes weaker. The response time of IBIPS to Kp is between 80 and 95 min. When Delta T > 95 min, the correlation coefficient basically keeps unchanged and only has a weak increase, suggesting that the IBIPS is mainly determined by the convection electric field represented by instantaneous Kp. (C) 2015 COSPAR. Published by Elsevier Ltd. All rights reserved.
引用
收藏
页码:1194 / 1199
页数:6
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