We investigate biased diffusion in a stochastic lattice gas with equal
numbers of oppositely <<charged>> particles, interacting only through
an excluded-volume constraint. Particle-particle exchanges are allowe
d, but occur on a much slower time scale than the dominant particle-ho
le exchanges. With increasing particle density, the system orders firs
t into a charge-segregated state, and disorders again near complete fi
lling, through first-order transitions which turn second order at high
er densities. A set of mean-field equations reflects the variations of
the density profiles in the different phases.