Processing math: 100%
van der Pol Oscillator on the phase plane
The 2nd order ODE for van der Pol oscillator
¨x+(x2−1)˙x+x=0 is written as a system
of first order ODEs
˙x=y+x−x33,˙y=−x.
Notice the unusual choice of the variable y=˙x−x+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.