Volume 22 Issue 3
Aug.  2002
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ZHANG Tianhui, XU Ronglan, LI Lei. THE CONVECTION ELECTRIC FIELD MODEL IN THE MAGNETOSPHERE[J]. Chinese Journal of Space Science, 2002, 22(3): 220-226. doi: 10.11728/cjss2002.03.20020304
Citation: ZHANG Tianhui, XU Ronglan, LI Lei. THE CONVECTION ELECTRIC FIELD MODEL IN THE MAGNETOSPHERE[J]. Chinese Journal of Space Science, 2002, 22(3): 220-226. doi: 10.11728/cjss2002.03.20020304

THE CONVECTION ELECTRIC FIELD MODEL IN THE MAGNETOSPHERE

doi: 10.11728/cjss2002.03.20020304 cstr: 32142.14.cjss2002.03.20020304
  • Received Date: 2001-01-18
  • Rev Recd Date: 2002-05-09
  • Taking the magnetic field lines as the equipotential lines, the convection field in the polar region at the ionospheric heights can be mapped into the magnetosphere where the electric field play a key role in various physical phenomena. To do this, a convection electric field in polar region and a magnetic model of magnetosphere are needed. In this paper, Volland's convection electric field model in the polar region and Tsyganenko's magnetic field model (T89) are used. It's not surprising that the electric field mapped from polar region is not a uniform dawn-dusk field. The results indicate that only in the distant magnetotail, the convection electric field can be considered as uniform dawn-dusk electric field. While, in the other region, there is not only the dawn-dusk electric field (Ey) but also the Ex and Ez. There exist three different regions in the magnetotail whose convection electric field has different characters. These characters are discussed. Generally, the dawn-dusk electric field become stronger and stronger when going from the distant magnetotail to the region near the earth. On the other hand, the electric field is stronger near the dawn and dusk magnetopause boundary than in the mid-plane.

     

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