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van der Pol Oscillator on the phase plane

The 2nd order ODE for van der Pol oscillator ¨x+(x21)˙x+x=0 is written as a system of first order ODEs ˙x=y+xx33,˙y=x.
Notice the unusual choice of the variable y=˙xx+x3/3, which is more convenient to show the existence of the periodic solution (call limit cycle) than the conventional one y=˙x. You can click your mouse on the plane to see how the points converge to the periodic solution.


12-1-212-1-2xy