Physics
Scientific paper
Feb 2009
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2009jgra..11402204l&link_type=abstract
Journal of Geophysical Research, Volume 114, Issue A2, CiteID A02204
Physics
10
Space Weather: Magnetic Storms (2788), Magnetospheric Physics: Ring Current, Magnetospheric Physics: Magnetic Reconnection (7526, 7835)
Scientific paper
For low values of the solar wind electric field, the response of the polar cap potential is essentially linear, but at high values of VB s, the polar cap potential saturates and does not increase further with increasing VB s. On the other hand, the ring current injection rate does increase linearly with VB s and shows no evidence of saturating. If enhanced convection is the origin of the ring current, this poses a paradox. How can the polar cap potential, and thus convection, saturate when the ring current does not? We examine a possible explanation based on the reexamination of the Burton equation by Vasyliunas (2006). We show that this explanation is not a viable solution to the paradox since it would require a changing polar cap flux, and we demonstrate that the polar cap flux saturates (at around 1 GWb) as the polar cap potential saturates. Instead, we argue that during storms a quasi-steady reconnection region forms in the tail near the Earth. This reconnection region moves closer to the Earth for higher values of solar wind B s, although the polar cap potential, the dayside merging and nightside reconnection rates, and the amount of open flux do not change much as a function of B s once the polar cap potential has become saturated. As the neutral line moves closer, the volume per unit magnetic flux in the closed field line region is less. Flux tubes leaving the reconnection region in general have lower PV γ as B s increases, and lower PV γ flux tubes can penetrate deeper into the inner magnetosphere, leading to a corresponding greater injection of particles into the inner magnetosphere. Thus a reconnection region that is closer to Earth is more effective in creating a strong ring current. This leads to a continued dependence of the ring current injection rate on VB s, although the polar cap potential has saturated.
Brogl S.
Bruntz Robert
Lopez Robert E.
Lyon John G.
Merkin V. G.
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