An interesting situation occurs when the linearized dynamics of the shape o
f a formally stable Hamiltonian relative equilibrium at nongeneric momentum
1 : 1 resonates with a frequency of the relative equilibrium's generator.
In this case some of the shape variables couple to the group variables to f
irst order in the momentum perturbation, and the first order perturbation t
heory implies that the relative equilibrium slowly changes orientation in t
he same way that a charged particle with magnetic moment moves on a sphere
under the influence of a radial magnetic monopole. In the course of showing
this a normal form is constructed for linearizations of relative equilibri
a and for Hamiltonians near group orbits of relative equilibria.