AnishchenkoAstakhov¶
Systems / ODEs / Oscillatory systems
A radiophysical self-oscillator with inertial nonlinearity — the canonical model of spiral (saddle-focus) chaos reached by the Feigenbaum period-doubling route.
Definition¶
\[
\begin{aligned}
\dot{y_{0}} &= \mu y_{0} - y_{0} y_{2} + y_{1} \\
\dot{y_{1}} &= - y_{0} \\
\dot{y_{2}} &= \frac{\eta y_{0}^{2} \left(\operatorname{sign}{\left(y_{0} \right)} + 1\right)}{2} - \eta y_{2}
\end{aligned}
\]
Parameters¶
| Symbol | Default | Role |
|---|---|---|
eta |
0.5 |
inertial-relaxation rate of the nonlinear element |
mu |
1.2 |
excitation parameter (negative damping of the circuit) |
Properties¶
Lyapunov spectrum
$+0.03327,\; -0.007017,\; -0.4509$
computed at build
computed at build
Kaplan–Yorke dimension
$D_{KY} = 2.058$
Divergence ∇·f
$\nabla\!\cdot f = - \eta + \mu - y_{2}$
state-dependent
state-dependent
Equilibria
1 equilibria
0 stable · 1 unstable
0 stable · 1 unstable
Define it in TSDynamics¶
import tsdynamics as ts
sys = ts.systems.AnishchenkoAstakhov()
traj = sys.integrate(final_time=100.0, dt=0.01)
exps = sys.lyapunov_spectrum()
ts.kaplan_yorke_dimension(exps)
Reference¶
Anishchenko et al. (2007), Nonlinear Dynamics of Chaotic and Stochastic Systems