By L. Marton, C. Marton (Eds.)
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Additional info for Advances in Electronics and Electron Physics, Vol. 54
Here we see the switchoff of B, as one crosses the shock passing downstream (from 40" toward 90"). Computer shock profiles (Figs. 6 and FIG. 24. Superposition of DIPD Kerr-cell-photographs, field line maps, and contours of constant current density. Note relation of luminosity changes and current contours to the Wb/m. 0 psec, negative print separatrix. Field lines are labeled by value of A in enhances contrast. ] 44 m o;;Fi P. J. BAUM AND A . O 100 80 60 I I 0 80 100 40 60 8 80 100 . 25. Magnetic field components near the DIPD separatrix (top).
The shock OA is now curved rather than straight and shows the surprising property that the field strength increases as one approaches the neutral point 0 from above. Extension of the Y eh-Axford type analysis to three dimensions has been carried out by Rosenau (1977, 1979), who finds shocks unnecessary. Extension of theory to collisionless plasma was done by Coroniti and Eviatar (1977). Kaw (1976) finds a link between Petschek’s mechanism and tearing theory. The models of the previous subsection assumed time stationarity, whereas 18 P.
There is assumed to be no field component perpendicular to these components as would be established by finite external sources parallel to the current layer. The current sheet tears into periodically spaced filaments treatable by Fourier analysis. , to a quadrupole field. The electric field arising during sheet rupture appears to be effective in accelerating particles. The theory of sheet rupture is more difficult than simple tearing so that analytic results are presently incomplete. , the potential field of Fig.
Advances in Electronics and Electron Physics, Vol. 54 by L. Marton, C. Marton (Eds.)