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Structure of the dissipation region during magnetic reconnection in collisionless plasma

Journal Article · · Journal of Geophysical Research; (United States)
DOI:https://doi.org/10.1029/91JA00893· OSTI ID:5222580
;  [1];  [2]
  1. Naval Research Lab., Washington, DC (USA)
  2. Univ. of Maryland, College Park (USA)
The results of an analytic and numerical investigation of the structure of the X line during steady state magnetic reconnection in collisionless plasma are presented. The structure of the X line essentially depends on a single dimensionless parameter F, which is a measure of the influx of plasma into the reconnection region. For small F the self-consistent plasma current driven at the X line is small, and the magnetic fields are nearly unchanged from the initial vacuum state. With increasing F the current driven at the X line becomes large, and the dissipation region collapses in the direction of the inflow and elongates along the outflow. For sufficiently large F the velocity of the plasma ejected from the X line exceeds the local Alfven velocity. In this regime a fast mode shock forms at the outflow end of the dissipation region which slows the high-velocity outflow plasma to the subsonic flow characteristics of the broader outflow region. Finally, at a critical plasma flux F{sub c} the dissipation region collapses to zero thickness; no steady solutions are found for F > F{sub c}. By matching the energy dissipated at the neutral line with the change in global magnetic energy, a self-consistent equation for F is derived which indicates that F always adjusts so that F {approx lt} F{sub c}. Predictions of reconnection rates and associated parameters for the geomagnetic tail are presented which are in reasonable agreement with observations.
OSTI ID:
5222580
Journal Information:
Journal of Geophysical Research; (United States), Journal Name: Journal of Geophysical Research; (United States) Journal Issue: A7 Vol. 96:A7; ISSN 0148-0227; ISSN JGREA
Country of Publication:
United States
Language:
English