A Universal Concept in Nonlinear Sciences
By Arkady Pikovsky
By Michael Rosenblum
By Jürgen Kurths
Cambridge Nonlinear Science Series (No. 12)
Publisher: Cambridge University Press
Print Publication Year: 2001
Online Publication Date:July 2010
Chapter DOI: http://dx.doi.org/10.1017/CBO9780511755743.006
Subjects: Nonlinear Science and Fluid Dynamics
In this chapter we describe synchronization effects in chaotic systems. We start with a brief description of chaotic oscillations in dissipative dynamical systems, emphasizing the properties that are important for the onset of synchronization. Next, we describe different types of synchronization: phase, complete, generalized, etc. In studies of these phenomena computers are widely used, therefore in our illustrations we often use the results of computer simulations, but also show some real experimental data. Whenever possible, we try to underline a similarity to synchronization of periodic oscillations.
One of the most important achievements of nonlinear dynamics within the last few decades was the discovery of complex, chaotic motion in rather simple oscillators. Now this phenomenon is well-studied and is a subject of undergraduate and high-school courses; nevertheless some introductory presentation is pertinent. The term “chaotic” means that the long-term behavior of a dynamical system cannot be predicted even if there were no natural fluctuations of the system's parameters or influence of a noisy environment. Irregularity and unpredictability result from the internal deterministic dynamics of the system, however contradictory this may sound. If we describe the oscillation of dissipative, self-sustained chaotic systems in the phase space, then we find that it does not correspond to such simple geometrical objects like a limit cycle any more, but rather to complex structures that are called strange attractors (in contrast to limit cycles that are simple attractors).