A universal version of the Hamilton-Jacobi equation on R x TM arises from t
he Liouville-Arnol'd theorem for a completely integrable system on a finite
-dimensional manifold M. We give necessary and sufficient conditions for su
ch complete integrability to imply a canonical separability of both this un
iversal Hamilton-Jacobi equation and its traditional counterpart. The geode
sic case is particularly interesting. We show that these conditions also ap
ply for systems of second-order ordinary differential equations (contact Bo
ws) which are not Euler-Lagrange. The Kerr metric, the Toda lattice and a c
ompletely integrable contact flow are given as examples.