Starting from many-body perturbation theory we have constructed a new varia
tional expression for the total energy of many-electron systems. This expre
ssion is a functional of two independent variables, the one-electron Green
function and the screened Coulomb interaction. The new functional as well a
s a much older variational expression by Luttinger and Ward (LW) are tested
on the interacting electron gas. Both functionals yield extraordinary accu
rate total energies although the new functional requires a much cruder inpu
t and is therefore easier to apply to more realistic systems.