For parametrized Hamiltonian systems with an arbitrary, finite number
of degrees of freedom, it is shown that secularly stable families of e
quilibrium solutions represent approximate trajectories for small (not
necessarily Hamiltonian) perturbations of the original system. This b
asic result is further generalized to certain conservative, but not ne
cessarily Hamiltonian, systems of differential equations. It generaliz
es to the conservative case a theorem due, in the dissipative case, to
Tikhonov, to Gradshtein, and to Levin and Levinson. It justifies the
use of physically motivated approximation procedures without invoking
the method of averaging and without requiring nonresonance conditions
or the integrability of the unperturbed Hamiltonian.