An analytic solution to the problem of strongly magnetized plasma flow
past a smooth, conducting sphere is considered. The magnetic field is
taken to be uniform at very large distances and the sphere is assumed
to be unmagnetized. In addition, the flow speed is assumed to be subs
onic and super-Alfvenic. It is shown that a steady state solution is p
ossible only if the frozen-in condition can be relaxed near the surfac
e of the sphere. By inclusion of a small resistivity, the presence of
two, nested boundary layers near the surface is demonstrated. The magn
etic field is shown to drape about the sphere with a scale size of the
order of the square root of the resistivity. (C) 1997 American Instit
ute of Physics.