“…there exists a canonical transformation (£, rj) = S(x, y) taking H(x(t), y(t)) to H(£(t), tj(*)), with £ and 17 satisfying i)-iii) in place of x and y respectively and such that Z = tj(/) Although this last condition does not necessarily eliminate all solutions which are not modes, it provides a computationally useful condition automatically satisfied by the classical modes of linear systems. We shall not investigate existence of modes in the most general setting, although it would be of considerable interest to know whether the modes shown to exist by Rosenberg [14,17,19] and Cooke and Struble [6] also satisfy our condition (iv). We shall instead apply this definition to the study of isoenergetic stability of some special modes of vibration for a class of simple conservative nonlinear oscillators.…”