Table 1.
Lyapunov spectra for different initial conditions (columns) and different values of the tie breaking parameter ɛ
| ɛ | λ | k = 1 | 2 | 3 | 4 | 5 |
|---|---|---|---|---|---|---|
| 0 | λ1 | +1.0 | +1.4 | +0.4 | +0.4 | +0.4 |
| λ2 | +0.2 | +0.3 | +0.3 | +0.3 | +0.3 | |
| λ3 | −0.5 | −0.4 | −0.3 | −0.3 | −0.3 | |
| λ4 | −0.7 | −1.2 | −0.4 | −0.4 | −0.4 | |
| 0.25 | λ1 | +49.0 | +35.3 | +16.6 | +0.4 | +0.4 |
| λ2 | +0.3 | +0.3 | +0.4 | +0.2 | +0.3 | |
| λ3 | −0.3 | −0.1 | −0.4 | −0.2 | −0.3 | |
| λ4 | −49.0 | −35.5 | −16.5 | −0.4 | −0.4 | |
| 0.50 | λ1 | +61.6 | +35.0 | +28.1 | +12.1 | +0.2 |
| λ2 | +0.6 | +0.3 | +0.1 | +0.0 | +0.2 | |
| λ3 | −0.6 | −0.4 | −0.2 | −0.1 | −0.2 | |
| λ4 | −61.5 | −35.8 | −28.0 | −12.2 | −0.3 |
k = 1, 2, 3, 4, 5 correspond to the initial conditions (x1, x2, x3, y1, y2, y3) = (0.5, 0.01k, 0.5 − 0.01k, 0.5, 0.25, 0.25) with k = 1, 2, … , 5. The Lyapunov exponents are multiplied by 103. Note that λ2 ≃ 0.0, λ3 ≃ 0.0, and λ4 ≃ −λ1 as expected. The Lyapunov exponents indicating chaos are shown in boldface.