AGU Fall Meeting, San Francisco, 6-10 December 1998
Abstract:
2.5 dimensional magnetohydrodynamic simulations of the evolution
of interplanetary magnetic clouds in a sheared solar wind flow
have been carried out. The CME is injected into a wind comprising
a high speed region near the poles and a low speed region toward
the equator, such as was observed by the Ulysses satellite at
solar minimum. Despite the tendency of such a magnetic cloud to
be torn apart, the magnetic tension force associated with the
cloud field ensures that the parts of the CME in the high and low
speed wind remain magnetically connected. However, the magnetic
field lines near the center of the cloud do undergo magnetic
reconnection, resulting in the creation of secondary flux ropes
embedded inside the cloud. However, in the absence of strong plasma
flows into the reconnection site, the reconnection rate is quite slow.
CMEs with straight field lines show no such coherence and break into
two parts, similar to the case with no magnetic field as presented
by Gosling and Riley.