Both methods require a previous determination of the unstable periodic orbits of the chaotic system before the controlling algorithm can be designed.Į.
Several techniques have been devised for chaos control, but most are developments of two basic approaches: the OGY (Ott, Grebogi and Yorke) method, and Pyragas continuous control. The perturbation must be tiny compared to the overall size of the attractor of the system to avoid significant modification of the system's natural dynamics. The result is to render an otherwise chaotic motion more stable and predictable, which is often an advantage. Ĭontrol of chaos is the stabilization, by means of small system perturbations, of one of these unstable periodic orbits. This results in a complicated and unpredictable wandering over longer periods of time. Chaotic dynamics, then, consists of a motion where the system state moves in the neighborhood of one of these orbits for a while, then falls close to a different unstable, periodic orbit where it remains for a limited time, and so forth. Any chaotic attractor contains an infinite number of unstable, periodic orbits.
In lab experiments that study chaos theory, approaches designed to control chaos are based on certain observed system behaviors. For other uses, see Chaos Control (disambiguation). This article is about chaos observed within non-linear systems.
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