A mean-field version of a simplified model for liquid metals, which co
nsists of a lattice gas of atoms and a collection of spinless fermions
that are free to hop among occupied atomic sites, is solved exactly.
Phase diagrams and phase transition properties are studied for two spe
cial cases. It is found that when the fermion hopping energy is small,
the presence of the fermions in the system does not change the qualit
ative feature of the phase diagrams as compared with the pure lattice-
gas system. When the hopping energy becomes large, the system can have
up to three phases and two critical points. For the case where the fe
rmion density is proportional to the lattice-gas atomic density with t
he proportionality constant not equal to 1, there are two distinct cri
tical points. For the case where the fermion density is a constant or
where the fermion density is equal to the lattice-gas atomic density t
he system has a tri-critical point. The system exhibits different phas
e transition properties under different thermodynamical conditions.