.49> (w) = (x w (t); xw (t)) Hence every orbit fl(t) of this flow can be uniquely written as fl(t) = (x(t); x(t)), where x(t) is a solution of (E-L). 2 RICARDO MA ~ N ' E It is well known that solutions of (E-L), and trough them, orbits of the flow f t : TM ! TM , are characterized by local variational properties. Here we shall revisit an old subject: orbits of the flow f t , selected in the
... [Show full abstract] intrincate phase portrait of f t , by requiring of them to satisfy global variational properties instead of the local ones that every orbit satisfies. Research on these special orbits goes back to M