Lesson 7 of 15
Van der Pol Oscillator
Van der Pol Oscillator
The Van der Pol oscillator is a nonlinear oscillator with self-sustaining oscillations. It was originally developed to model vacuum tube circuits but appears throughout biology, physics, and engineering.
The Equations
dx/dt = y
dy/dt = μ·(1 - x²)·y - x
The parameter μ controls the nonlinearity:
- μ = 0: Simple harmonic oscillator (no damping/driving)
- μ > 0: System has a limit cycle — all trajectories spiral toward a stable periodic orbit
- Large μ: Relaxation oscillations with sharp transitions
Limit Cycles
Unlike fixed-point attractors, the Van der Pol oscillator has a limit cycle attractor. Regardless of initial conditions, trajectories converge to the same closed orbit in phase space. This is a hallmark of many biological oscillators (heartbeat, circadian rhythms).
Euler Integration
We use simple Euler integration with timestep dt:
x_{n+1} = x_n + dt·(dx/dt)
y_{n+1} = y_n + dt·(dy/dt)
Your Task
Implement:
vdp_deriv(x, y, mu)— compute derivatives (dx/dt, dy/dt)vdp_euler(x0, y0, mu, dt, steps)— integrate using Euler methodvdp_amplitude(x0, y0, mu, dt, steps, n_keep)— find max amplitude after transients
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