Consider the following idealized motions
(i) The motion of a bob attached to a spring on a horizontal frictionless table,
(ii) the motion of a pendulum with an arbitrary amplitude without air resistance,
(iii) the motion of the earth around the Sun,
(iv) the motion of a ball dropped from a height that hits the ground elastically so that there is no loss of energy into heat and every time it bounces back to the same height.
The only commonality between these motions is that all of them are conservative systems and all of them are periodic. Though the mathematical forms of the potentials very different, all are conservative systems without dissipation. From these examples, my strong hunch is that a necessary condition for periodicity must be that the system must be conservative. Apart from that, all these motions are examples of motion that are either effectively one-dimensional motion or two-dimensional planar motion.
Is being conservative the only necessary condition for a motion to be periodic?
Is being conservative also the sufficient condition for a motion to be periodic?
Conditions for periodic motions in classical mechanics is a pre-existing answer. The accepted answer is packed with jargons (integrable motion, regular motion, quasi-periodic motion etc) and is unintelligible for me.