Here the autonomous planar system is , . Its equilibrium points are
The Jacobian matrix is
For even , the eigenvalues are , so these points are unstable saddle equilibria. Writing , their local unstable and stable directions are and respectively. For odd , the eigenvalues are .
To classify the latter points nonlinearly, differentiate the first integral
At this energy has a strict local minimum. Its nearby level sets are closed curves, proving that the odd- points are stable center equilibria, with no attraction to the center. The phase portrait consists of closed oscillatory orbits for , heteroclinic orbits at joining consecutive saddle equilibria, and open rotating orbits for . The separating curves have
Above the horizontal axis , so flow is rightward; below it flow is leftward. The closed orbits are clockwise, and these same signs orient every separating and rotating orbit.

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