We study the equilibrium states of a nonlinearly elastic conducting ro
d in a magnetic field, a problem we have considered in several previou
s papers. We are now able to prove a global bifurcation theorem for th
is problem. To do this, two difficulties must be overcome. The first i
s the presence of the rotation group SO(2) as a symmetry group for the
problem. The second is that, for some values of certain parameters, t
he linearized problem is a nonstandard eigenvalue problem. The former
difficulty is overcome by applying an idea due to Healey, who observed
the existence of an additional symmetry in a related problem first po
sed by the present author. The latter problem is handled by using some
nonstandard tools from functional analysis.