This paper discusses the dynamics of the solar wind plasma based on solar wind origins. The MHD (Magnetohydrodynamics) and its formula derivation are reviewed, especially its features of discontinuous structure and rotation discontinuity, as shown by one dimensional space structure diagrams. By analyzing the satellite detection results, it is found that there are two magnetic field direction discontinuity surfaces: one is a tangential discontinuity (TD), and the other is a rotation discontinuity (RD). It is shown that for the TD, the magnetic-field component of the vertical discontinuity surface is zero and the electricity ions do not go through the surface. While the bilateral magnetic field directions of the RD are different, the size is the same and the electricity ions go through the discontinuity surface. It is observed that the rotation discontinuity surface in the solar wind is mainly related with the high-speed solar wind. The magnetic flux through the interface remains unchanged, the magnetic field in the tangential direction can change along any direction, therefore, the rotational discontinuity can be observed. By conparing the derivation results with the data verification diagrams, it is shown that the data diagram analysis supports the derivation of the formula and then proves the system of the rotation discontinuity of the solar wind origin area plasma.
[1] Spasojevi'c M, Frey H U, Thomsen M F, et al. The link between a de-tached subauroral proton arc and a plasmaspheric plume[J]. Geophys Res Lett, 2004, 31(4): 1521-1532.
[2] Schunk R W, Scherliess L, Sojka J S, et al. Global assimilation of iono-spheric measurements (GAIM)[J]. Radio Science, 2004, 39(1): 1033-1041.
[3] Schäfer S, Glassmeier K H, Eriksson P T I, et al. Spatial and temporal characteristics of poloidal waves in the terrestrial plasmasphere: a CLUS-TER case study[J]. Annales Geophysicae, 2007, 25(4): 1011-1024.
[4] Pierrard V, Cabrera J. Dynamical simulations of plasmapause deforma-tions[J]. Space Science Reviews, 2006, 122(1-4): 119-126.
[5] Chen S H, Moore T E. Magnetospheric convection and thermal ions in the dayside outer magnetosphere[J]. Journal of Geophysical Research, 2006, 111(1): 865-877.
[6] André N, Lemaire J F. Convective instabilities in the plasmasphere[J]. Journal of Atmospheric and Solar-terrestrial Physics, 2006, 68(2): 213-227.
[7] Parker E N. A quasi-linear model of plasma shock structure in a longitu-dinal magnetic field[J]. Journal of Nuclear Energy, 1961, 2(1): 146-158.
[8] Peng Q Y, Vienne A, Lainey V, et al. New evidence of precision premi-um for Galilean satellites from CCD imaging[J]. Planetary and Space Sci-ence, 2008, 56(2): 1807-1811.
[9] Zurbuchen T H, Richardson I G. In situ solar wind and magnetic field signatures of interplanetary coronal mass ejections[J]. Space Science Re-views, 2006, 123(3): 31-43.
[10] Fisk L A, Schwadron N A, Zurbuchen T H. On the slow solar wind[J]. Space Science Reviews, 1998, 86(1-4): 51.
[11] Cranmer S R, Ballegooijen A A V, Edgar R J. Self-consistent coronal heating and solar wind acceleration from anisotropic magnetohydrody-namic turbulence[J]. The Astrophysical Journal Supplement Series, 2007, 171(2): 520-551.
[12] Goossens M, Terradas J, Andries J, et al. On the nature of king MHD waves in magnetic flux tubes[J]. Astronomy and Astrophysics, 2009, 503(1): 213-223.
[13] Hartle R E, Sturrock P A. Two-fluid model of the solar wind[J]. The Astrophysical Journal, 1968, 151(2): 1155-1167.
[14] lonson J A. Resonant absorption of alfvenic surface waves and the heat-ing of solar coronal loops[J]. The Astrophysical Journal, 1978, 226(1): 650-673.
[15] Li B, Habbal S R, Li X, et al. Effect of the latitudinal distribution of temperature at the coronal base on the interplanetary magnetic field configuration and the solar wind flow[J]. Journal of Geophysical Re-search, 2005, 110(10): 12112-12142.