When perturbation theory is applied to a quantity for which a variatio
nal principle holds (eigenenergies of Hamiltonians, Hartree-Fock or de
nsity-functional-theory energy, etc.), different variational perturbat
ion theorems can be derived. A general demonstration of the existence
of variational principles for an even order of perturbation, when cons
traints are present, is provided here. Explicit formulas for these var
iational principles for even orders of perturbation, as well as for th
e ''2n + 1 theorem,'' to any order of perturbation, with or without co
nstraints, are also exhibited. This approach is applied to the case of
eigenenergies of quantum-mechanical Hamiltonians, studied previously
by other methods.