On accelerated magnetosheath flows under northward IMF

被引:17
|
作者
Erkaev, N. V. [1 ,2 ]
Farrugia, C. J. [3 ,4 ]
Harris, B. [3 ]
Biernat, H. K. [5 ,6 ]
机构
[1] Russian Acad Sci, Inst Computat Modeling, Krasnoyarsk 660036, Russia
[2] Siberian Fed Univ, Krasnoyarsk, Russia
[3] Univ New Hampshire, Ctr Space Sci, Durham, NH 03824 USA
[4] Univ New Hampshire, Dept Phys, Durham, NH 03824 USA
[5] Austrian Acad Sci, Space Res Inst, A-8042 Graz, Austria
[6] Graz Univ, Inst Theoret Phys, A-8010 Graz, Austria
关键词
SOLAR-WIND FLOW; AMPTE/IRM OBSERVATIONS; PLANETARY OBSTACLES; MAGNETIC-FIELD; 24; OCTOBER; MHD MODEL; BOW SHOCK; MAGNETOPAUSE; EQUATIONS; REGION;
D O I
10.1029/2010GL045998
中图分类号
P [天文学、地球科学];
学科分类号
07 ;
摘要
We study the acceleration of magnetosheath plasma using a semi-analytical magnetic string approach for a range of solar wind Alfven Mach numbers, M-A, between 2 and 20. We work with an IMF vector perpendicular to the solar wind velocity, V-sw, and pointing north. We do not invoke magnetic reconnection. Our results indicate that magnetosheath speeds can exceed the solar wind speed, and the ratio V/V-sw increases with decreasing M-A. Analyzing the dependence of this ratio on M-A, we find that for M-A = 2, maximum V/V-sw approximate to 1.6, and for M-A = 10-20, maximum V/V-sw varies from 1.21 to 1.13. Maximum speeds occur a few Earth radii (R-E) tailward of the dawn-dusk terminator. The thickness of the accelerated flow layer varies as M-A(-2). Taking the magnetopause subsolar distance as 10 R-E, we find typical values for the thickness of similar to 4 R-E for M-A = 3 and 0.35 R-E for M-A = 10. The physical mechanism is that of draping of the magnetic field lines around the magnetosphere, and the associated magnetic tension and total pressure gradient forces acting on the flow. For lower M-A the plasma depletion is stronger, and thus the acceleration produced by the pressure gradient is larger. An additional acceleration is produced by the magnetic tension, which is stronger for smaller M-A. At the dayside the pressure gradient and magnetic tension forces both act in the same direction. But tailward of the terminator the magnetic tension starts to act in the opposite direction to the pressure gradient. When the resulting force vanishes, the highest speed is attained. Citation: Erkaev, N. V., C. J. Farrugia, B. Harris, and H. K. Biernat (2011), On accelerated magnetosheath flows under northward IMF, Geophys. Res. Lett., 38, L01104, doi: 10.1029/2010GL045998.
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页数:5
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