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Rössler map

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In 1979 Otto Rössler found the inspiration from a Taffy-Pulling machine to his Non-linear three-dimensional deterministic dynamical system. This system behaves much as the Lorenz attractor for specific values of the parameters and was found to follow the period-two doubling route to chaos like the Logistic map. The Rössler system having only one linearity appears like:

The Lorenz attractor is defined by a set of three coupled nonlinear differential equations:

{dx \over dt} = -y -z
{dy \over dt} = x + ay
{dz \over dt} = b+z(x-c)

Numerical integration shows that the system exhibits a strange attractor for a=b=0.2 and c=5.7.


References

  • Steven H. Strogatz, Nonlinear Dynamics and Chaos, Perseus publishing 1994.
  • O.E. Rössler, An Equation for Hyperchaos, Phys.let. Vol.71A no 2,3 1979.
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