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Rossler Funnel Attractor

What you are seeing: a cousin of the Lorenz attractor, written down by Otto Rossler in 1976 as the simplest 3D system that still produces chaos (only one nonlinear term, zxz \cdot x). The trajectory winds outward on a flat spiral, then a single fold throws it back to the centre. Push the control parameter cc past about 5.75.7 and the spiral grows a strong vertical lobe; the geometry earns its "funnel" name.

The equations are x˙=yz\dot x = -y - z, y˙=x+ay\dot y = x + a\,y, z˙=b+z(xc)\dot z = b + z\,(x - c). The classical parameters are a=b=0.2a = b = 0.2, c=5.7c = 5.7. Drop cc to about 44 and the attractor folds into a clean period-2 limit cycle; sweep it back up through 4.24.2, 5.05.0, 5.45.4 and watch a period-doubling cascade. λ1\lambda_1 in the corner is the running estimate of the largest Lyapunov exponent; it stays positive in the chaotic regime (about 0.070.07 at the default parameters) and collapses to zero in the periodic windows.

Figure 1. strange attractor in the (x, y) projection. Method: classical fourth-order Runge-Kutta from shared/js/engine/ode-rk.js, fixed dt = 0.02. Live max-Lyapunov estimator via tangent-vector renormalization.
a0.200
b0.200
c5.70
speed0.5

WHAT TO TRY

  • Raise the parameter c: the Rossler attractor period-doubles, its single funnel loop splitting into two, then four, then a chaotic band. Only one nonlinear term drives all of it.
  • Watch the trajectory spiral out in the plane then fold back through the funnel: the slow spiral plus the fast z-kick is the stretch-and-fold that makes the chaos.
  • Read the Lyapunov exponent lambda_1: positive means nearby trajectories diverge exponentially, the quantitative signature of the chaos you are watching trace out.