If a non linear system is in a state of periodic motion then we can find the period of the mtion using
(1)
where the last integral is expressed as a function of q using the Hamiltionian.
If the Hamiltonian has the form
then we can write
so that![]()
Substituting this into (1) gives
![]()
It must be noted here that the period is independent of the initial phase so the limits need only differ by![]()
Example: The Hamiltonian of a vertical pendulum is given by![]()
If
the pendulum has enough energy to describe a vertical circle and
![]()
![]()

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after using the half angle formulae and putting![]()