HIDDEN ATTRACTORS IN DYNAMICAL SYSTEMS. FROM HIDDEN OSCILLATIONS IN HILBERT-KOLMOGOROV, AIZERMAN, AND KALMAN PROBLEMS TO HIDDEN CHAOTIC ATTRACTOR IN CHUA CIRCUITS

被引:645
作者
Leonov, G. A. [1 ]
Kuznetsov, N. V. [1 ,2 ]
机构
[1] St Petersburg State Univ, Math & Mech Fac, Dept Appl Cybernet, St Petersburg, Russia
[2] Univ Jyvaskyla, Dept Math Informat Technol, SF-40351 Jyvaskyla, Finland
来源
INTERNATIONAL JOURNAL OF BIFURCATION AND CHAOS | 2013年 / 23卷 / 01期
基金
芬兰科学院; 俄罗斯基础研究基金会;
关键词
Hidden oscillation; hidden attractor; large (normal amplitude) and small limit cycle; Lienard equation; quadratic system; Lyapunov focus values (Lyapunov quantities; Poincare-Lyapunov constants; Lyapunov coefficients); 16th Hilbert problem; Aizerman conjecture; Kalman conjecture; absolute stability; nonlinear control system; harmonic balance; describing function method; phase-locked loop (PLL); drilling system; induction motor; Chua circuits; QUADRATIC DIFFERENTIAL-SYSTEMS; SIZE LIMIT-CYCLES; LYAPUNOV QUANTITIES; ABSOLUTE STABILITY; WEAK FOCUS; ASYMPTOTIC STABILITY; 16TH PROBLEM; ORDER; COMPUTATION; BIFURCATIONS;
D O I
10.1142/S0218127413300024
中图分类号
O1 [数学];
学科分类号
0701 ; 070101 ;
摘要
From a computational point of view, in nonlinear dynamical systems, attractors can be regarded as self-excited and hidden attractors. Self-excited attractors can be localized numerically by a standard computational procedure, in which after a transient process a trajectory, starting from a point of unstable manifold in a neighborhood of equilibrium, reaches a state of oscillation, therefore one can easily identify it. In contrast, for a hidden attractor, a basin of attraction does not intersect with small neighborhoods of equilibria. While classical attractors are self-excited, attractors can therefore be obtained numerically by the standard computational procedure. For localization of hidden attractors it is necessary to develop special procedures, since there are no similar transient processes leading to such attractors. At first, the problem of investigating hidden oscillations arose in the second part of Hilbert's 16th problem (1900). The first nontrivial results were obtained in Bautin's works, which were devoted to constructing nested limit cycles in quadratic systems, that showed the necessity of studying hidden oscillations for solving this problem. Later, the problem of analyzing hidden oscillations arose from engineering problems in automatic control. In the 50-60s of the last century, the investigations of widely known Markus-Yamabe's, Aizerman's, and Kalman's conjectures on absolute stability have led to the finding of hidden oscillations in automatic control systems with a unique stable stationary point. In 1961, Gubar revealed a gap in Kapranov's work on phase locked-loops (PLL) and showed the possibility of the existence of hidden oscillations in PLL. At the end of the last century, the difficulties in analyzing hidden oscillations arose in simulations of drilling systems and aircraft's control systems (anti-windup) which caused crashes. Further investigations on hidden oscillations were greatly encouraged by the present authors' discovery, in 2010 (for the first time), of chaotic hidden attractor in Chua's circuit. This survey is dedicated to efficient analytical-numerical methods for the study of hidden oscillations. Here, an attempt is made to reflect the current trends in the synthesis of analytical and numerical methods.
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页数:69
相关论文
共 207 条
[1]  
AIZERMAN M., 1949, Uspehi Matem. Nauk (N.S.), V4, P187
[2]  
Aizerman M. A., 1964, Absolute Stability of Regulator Systems
[3]  
AIZERMAN MA, 1953, AVTOMAT TELEMEKH, V14, P597
[4]  
Albarakati WA., 2000, Elec. J. Differ. Equ, V2000, P1
[5]  
Allgower E. L., 1990, Numerical continuation methods, an introduction
[6]  
Alli-Oke R, 2012, IFAC P VOLUMES IFAC, V45, P27
[7]  
Andronov A., 1947, AVTOMATIKA TELEMEKHA, V8
[8]  
Andronov A.A., 1966, Theory of oscillators
[9]  
[Anonymous], 1952, Mat. sb
[10]  
[Anonymous], 1968, Modern Control Principles and Application