This paper studies the dynamical fluid plus rigid-body system
consisting of a two-dimensional rigid cylinder of general
cross-sectional shape interacting with N point vortices. We derive
the equations of motion for this system and show that, in
particular, if the vortex strengths sum to zero and the rigid-body
has a circular shape, the equations are Hamiltonian with respect to
a Poisson bracket structure that is the sum of the rigid body
LiePoisson bracket on
, the dual of the Lie
algebra of the Euclidean group on the plane, and the canonical
Poisson bracket for the dynamics of
N point vortices in an
unbounded plane. We then use this Hamiltonian structure to study the
linear and nonlinear stability of the moving Föppl equilibrium
solutions using the energy-Casimir method.