Electron-electron interactions appear to play qualitatively vital role
s in the behavior of expanded liquid metals; these systems display phe
nomena that simply do not occur in a single-electron picture. Motivate
d by a desire to understand such liquids, and to model electron intera
ction effects in liquids more generally, we show in this paper how one
can formulate and solve a Hartree-Fock theory within a liquid by usin
g liquid theory methods. The work generalizes the previous efforts of
Logan and co-workers by removing the restrictions to model band shapes
and Hubbard Hamiltonians. The Pariser-Parr-Pople Hamiltonian used her
e has the added feature of an interatomic Coulombic interaction and th
erefore allows us to assess the role of interaction-induced fluctuatio
ns in the local field at each atom. The model also requires a calculat
ion of a quantity with the significance of a bond order, a concept of
some possible utility in a wide variety of electronic-structure-in-liq
uids problems.