On the formation of tilted flux ropes in the Earth's magnetotail observed with ARTEMIS

被引:26
作者
Kiehas, S. A. [1 ,2 ]
Angelopoulos, V. [1 ]
Runov, A. [1 ]
Moldwin, M. B. [3 ]
Moestl, C. [4 ,5 ]
机构
[1] Univ Calif Los Angeles, Dept Earth & Space Sci, Los Angeles, CA 90095 USA
[2] Austrian Acad Sci, Space Res Inst, A-8010 Graz, Austria
[3] Univ Michigan, Dept Atmospher Ocean & Space Sci, Ann Arbor, MI 48109 USA
[4] Univ Calif Berkeley, Space Sci Lab, Berkeley, CA 94720 USA
[5] Graz Univ, Inst Phys, Graz, Austria
基金
奥地利科学基金会;
关键词
TRAVELING COMPRESSION REGIONS; PLASMOID EJECTION; MAGNETIC-FIELD; DISTANT MAGNETOTAIL; KINETIC-PROPERTIES; GEOMAGNETIC TAIL; ISEE-3; EVOLUTION; IMP-8; SIGNATURES;
D O I
10.1029/2011JA017377
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
On 21 October 2010, ARTEMIS spacecraft P2, located at about -57 R-EGSM in the Earth's magnetotail, observed a series of flux ropes during the course of a moderate substorm. Subsequently, ARTEMIS spacecraft P1, located about 20 R-E farther downtail and farther into the lobe than P2, observed a series of TCRs, consistent with the flux ropes observed by P2. The dual-spacecraft configuration allows simultaneous examination of these phenomena, which are interpreted as an O-line, followed by a series of flux ropes/TCRs. An inter-spacecraft time of flight analysis, assuming tailward propagation of cross-tail aligned ropes, suggests propagation speeds of up to similar to 2000 km/s. A principal axis investigation, however, indicates that the flux ropes were tilted between 41 degrees and 45 degrees in the GSM x-y-plane with respect to the noon-midnight meridional plane. Taking this into account, the tailward propagation speed of the different flux ropes is determined to be between 900 and 1400 km/s. The same timing analysis also reveals that the flux rope velocity increased progressively from one flux rope to the next. A clear correlation between the magnetic field and plasma flow components inside the flux ropes was observed. As possible mechanisms leading to the formation of tilted flux ropes we suggest (a) a progressive spreading of the reconnection line along the east-west direction, leading to a boomerang-like shape and (b) a tilting of flux ropes during their formation by non-uniform reconnection with open field lines at the ends of the flux ropes. The progressive increase in the propagation velocity from the first to the last flux rope may be evidence of impulsive reconnection: initially deep inside the plasma sheet the reconnection rate is slow but as reconnection proceeds at the plasma sheet boundary and possibly lobes, the reconnection rate increases.
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页数:14
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