We study the weakly interacting Bose gas in both two and three dimensi
ons using a variational approach. In particular we construct the therm
odynamic potential of the gas to within ladder approximation and find
by minimization an accurate mean-field description of the dilute Bose
gas. Using spin-polarized atomic hydrogen as a specific example. we ob
tain an improved description of the Bose-Einstein condensed phase in t
hree dimensions, and a signature of a phase transition in two dimensio
ns. The latter cannot be found by a straightforward application of per
turbation theory around the ideal Bose gas.