We investigate the motion of a classical Wigner lattice in a two-dimensiona
l confined electron gas in the presence of a perpendicular magnetic field,
a (weak) driving electric field, and weak damping. In order to study the sy
stem at its lowest-energy states, initial configurations are produced by a
special quenching procedure. We observe the formation of a steady state in
which the entire electron-lattice cycles with a common uniform velocity. Ce
rtain runs show an intermediate instability leading to lattice rearrangemen
ts. A Hall resistance can be defined for this system and we find that it de
pends linearly, on the magnetic field with an anomalous coefficient reflect
ing the many-body contributions peculiar to two dimensions.