The Rabinovich–Fabrikant equations are a set of three coupled ordinary differential equations exhibiting chaotic behaviour for certain values of the parameters. They are named after Mikhail Rabinovich and Anatoly Fabrikant, who described them in 1979.
System description The equations are:
x ˙ = y ( z − 1 + x 2 ) + γ x {\displaystyle {\dot {x}}=y(z-1+x^{2})+\gamma x\,}
y ˙ = x ( 3 z + 1 − x 2 ) + γ y {\displaystyle {\dot {y}}=x(3z+1-x^{2})+\gamma y\,}
z ˙ = − 2 z ( α + x y ) , {\displaystyle {\dot {z}}=-2z(\alpha +xy),\,}
where α, γ are constants that control the evolution of the system. For some values of α and γ, the system is chaotic, but for others it tends to a stable periodic orbit. Danca and Chen note that the Rabinovich–Fabrikant system is difficult to analyse (due to the presence of quadratic and cubic terms) and that different attractors can be obtained for the same parameters by using different step sizes in the integration, see on the right an example of a solution obtained by two different solvers for the same parameter values and initial conditions. Also, recently, a hidden attractor was discovered in the Rabinovich–Fabrikant system.
Equilibrium points
The Rabinovich–Fabrikant system has five hyperbolic equilibrium points, one at the origin and four dependent on the system parameters α and γ:
x ~ 0 = ( 0 , 0 , 0 ) {\displaystyle {\tilde {\mathbf {x} }}_{0}=(0,0,0)}
x ~ 1 , 2 = ( ± q − , ∓ α q − , 1 − ( 1 − γ α ) q − 2 ) {\displaystyle {\tilde {\mathbf {x} }}_{1,2}=\left(\pm q_{-},\mp {\frac {\alpha }{q_{-}}},1-\left(1-{\frac {\gamma }{\alpha }}\right)q_{-}^{2}\right)}
x ~ 3 , 4 = ( ± q + , ∓ α q + , 1 − ( 1 − γ α ) q + 2 ) {\displaystyle {\tilde {\mathbf {x} }}_{3,4}=\left(\pm q_{+},\mp {\frac {\alpha }{q_{+}}},1-\left(1-{\frac {\gamma }{\alpha }}\right)q_{+}^{2}\right)}
where
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