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xhx020211(½ð±Ò+1): 2010-04-15 09:40
UT  ISI:000269425200033
Estimating the ultimate bound and positively invariant set for a new chaotic system and its application in chaos synchronization
CHAOS SOLITONS & FRACTALS
2Â¥2010-04-15 09:34:10
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stimating the ultimate bound and positively invariant set for a new chaotic system and its application in chaos synchronization
×÷Õß: Shu YL (Shu, Yonglu)1, Xu HX (Xu, Hongxing)1, Zhao YH (Zhao, Yunhong)1  
À´Ô´³ö°æÎï: CHAOS SOLITONS & FRACTALS    ¾í: 42    ÆÚ: 5    Ò³: 2852-2857    ³ö°æÄê: DEC 15 2009   
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ÕªÒª: In this paper, we investigate the ultimate bound and positively invariant set for a new chaotic system via the generalized Lyapunov function theory. For this system, we derive a three-dimensional ellipsoidal ultimate bound and positively invariant set. In addition, the two-dimensional bound with respect to x - z and y - z are established. Finally, the result is applied to the study of completely chaos synchronization, an exact threshold is given with the system parameters. Numerical simulations are presented to show the effectiveness of the proposed chaos synchronization scheme. (C) 2009 Elsevier Ltd. All rights reserved.
ÎÄÏ×ÀàÐÍ: Article  
ÓïÑÔ: English  
KeyWords Plus: LORENZ-SYSTEM; CHEN SYSTEM; ATTRACTOR; TRAJECTORIES; EQUATION; CIRCUIT; FAMILY  
ͨѶ×÷ÕßµØÖ·: Xu, HX (ͨѶ×÷Õß), Chongqing Univ, Coll Math & Phys, Chongqing 400044, Peoples R China  
µØÖ·:
1. Chongqing Univ, Coll Math & Phys, Chongqing 400044, Peoples R China  
µç×ÓÓʼþµØÖ·: xhx020211@sina.com  
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National Nature Youth Foundation of China  10601071  

[ÏÔʾ»ù½ð×ÊÖúÐÅÏ¢]   

Project supported by the Foundation item the National Nature Youth Foundation of China (No. 10601071).

³ö°æÉÌ: PERGAMON-ELSEVIER SCIENCE LTD, THE BOULEVARD, LANGFORD LANE, KIDLINGTON, OXFORD OX5 1GB, ENGLAND  
ѧ¿ÆÀà±ð: Mathematics, Interdisciplinary Applications; Physics, Multidisciplinary; Physics, Mathematical  
IDS ºÅ: 489MW  
ISSN: 0960-0779  
DOI: 10.1016/j.chaos.2009.04.003
3Â¥2010-04-15 09:39:29
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UT  ISI:000269425200033
Estimating the ultimate bound and positively invariant set for a new chaotic system and its application in chaos synchronization
CHAOS SOLITONS & FRACTALS
4Â¥2010-04-15 09:52:58
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Estimating the ultimate bound and positively invariant set for a new chaotic system and its application in chaos synchronization
Yonglu Shua, Hongxing Xu, a,  and Yunhong Zhaoa

aCollege of Mathematics and Physics, Chongqing University, Chongqing 400044, China

Accepted 1 April 2009.  Available online 1 May 2009.

Abstract
In this paper, we investigate the ultimate bound and positively invariant set for a new chaotic system via the generalized Lyapunov function theory. For this system, we derive a three-dimensional ellipsoidal ultimate bound and positively invariant set. In addition, the two-dimensional bound with respect to x-z and y-z are established. Finally, the result is applied to the study of completely chaos synchronization, an exact threshold is given with the system parameters. Numerical simulations are presented to show the effectiveness of the proposed chaos synchronization scheme.

Article Outline
1. Introduction
2. The ultimate bound and positive invariant set of this new chaotic system
3. Estimate of the two-dimensional bound with respect to y-z and x-z
4. The application in chaos synchronization
5. Simulation studies
6. Conclusions
References

1. Introduction
Since Lorenz discovered the well-known Lorenz chaotic system [1], many other chaotic systems have been found, including the well-known Rössler system [2], Chua¡¯s circuit [3], which have been served as models for the study of chaos. In late 1990s, a new chaotic system was found, which is dual to the Lorenz system, and it is called the Chen system [4]. Due to its close relation to the Lorenz system, it has been widely studied [5], [6] and [7]. In the new century, many new simple chaotic systems were found: L¨¹ system [8], unified system [9], and Lorenz-like system [10] to just name a few examples.

The ultimate bound of a system is important for the study of the qualitative behavior of a chaotic system [11] and [12]. If we can show that a system under consideration has a globally attractive set, then we know that the system cannot have equilibrium points, periodic solutions, quasi-periodic solutions, or other chaotic attractors outside the globally attractive set. This greatly simplifies the analysis of the dynamical properties of the system. The ultimate bound also plays an important role in designing scheme for chaos control and chaos synchronization.

The ultimate bound property of the Lorenz system has been investigated by many researchers. From1985 to 1987, Leonov gave the original results of globally ultimate bound of the Lorenz system [13], [14] and [15]. Then, Swinnerton-Dyer showed that Lyapunov function can be used to study the bounds for trajectories of the Lorenz equations [16]. This idea was further developed by Liao X et al. to get new globally attractive set and positively invariant set of the Lorenz system by constructing a family of generalized Lyapunov functions, and this result was applied to study of chaos control and chaos synchronization [17]. By using the same method, Li et al. filled the gap of estimating the ultimate bound of the Lorenz system for 0
However, the ultimate bounds of many other chaotic system remain to be solved. Sun [22] got an ultimate bound of a generalized Lorenz system. Li et al. [18] and [19] got an ultimate bound for the unified chaotic system for 0¦Á<1/29. Qin and Chen investigated the ultimate bound of Chen system in [23], but the parameter values considered does not cover the most interesting case of the Chen¡¯s chaotic attractor [4]. Yu and Liao showed that there exists exponential attractive set for a general chaotic system which does not belong to the known Lorenz system, or the Chen system, or the Lorenz family [24]. The estimation of the ultimate bound for the smooth Chua¡¯s system was given in [25]. And recently an ultimate bound and positively invariant set for the hyperchaotic Lorenz¨CHaken system was obtained in [26].

Recently, Chu and Li [27] introduced the following new system:



(1)where (a,b,c)R3 is a vector parameter. System (1) displays a typical chaotic attractor when a=5,b=16,c=1 (see Fig. 1). Some basic dynamical properties are studied in [27]. But many properties of this new system remain to be further uncovered. In this paper, we first investigate the ultimate bound and positively invariant set for this new chaotic system using the generalized Lyapunov function theory, and then we study the synchronization of this system. By employing a linear feedback controller with a single variable, an exact threshold is given with the system parameters based on the ultimate bound of what we get. As the scheme is simple, it is easy to implement in practical applications.
5Â¥2010-04-15 12:38:11
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