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The Anishchenko–Astakhov Oscillator of Chaotic Self-Sustained Oscillations

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Deterministic Nonlinear Systems

Abstract

In general form, self-sustained oscillatory systems with one degree of freedom are described by the equation

$$\displaystyle{ \ddot{x} +\varPhi (x,\boldsymbol{\alpha })\dot{x} +\varPsi (x,\boldsymbol{\alpha }) = 0\;, }$$
(11.1)

where x is a variable oscillating periodically, \(\varPhi (x,\boldsymbol{\alpha })\) and \(\varPsi (x,\boldsymbol{\alpha })\) are nonlinear functions characterizing the action of forces providing periodic self-sustained oscillations, and \(\boldsymbol{\alpha }\) is a vector of parameters \((\alpha _{1},\alpha _{2},\ldots,\alpha _{n})\).

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Notes

  1. 1.

    Problems arise when using the above algorithm due to a discontinuity of the second derivative Φ(x) = I(x)x 2 in (11.26). If one approximates Φ(x) by the exponential function exp(x) − 1 and restricts to the first three terms of its Taylor expansion, then the calculation can be carried through and it can be shown that L 1(g) < 0 for any g > 0.

  2. 2.

    Such calculations requiring transitions to unstable cycles at points C and F are non-trivial, but possible with a suitable modification of calculation algorithms for the cycle multipliers. Usual integration leads to the loss of cycle and to the abrupt change of regimes here.

References

  1. Anishchenko, V.S.: Dynamical Chaos – Models and Experiments. World Scientific, Singapore (1995)

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  2. Anishchenko, V.S., Astakhov, V.V., Neiman, A.B., Vadivasova, T.E., Schimansky-Geier, L.: Nonlinear Dynamics of Chaotic and Stochastic Systems. Springer, Berlin (2002)

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Anishchenko, V.S., Vadivasova, T.E., Strelkova, G.I. (2014). The Anishchenko–Astakhov Oscillator of Chaotic Self-Sustained Oscillations. In: Deterministic Nonlinear Systems. Springer Series in Synergetics. Springer, Cham. https://doi.org/10.1007/978-3-319-06871-8_11

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