Top PDF A new chaotic attractor with two quadratic nonlinearities, its synchronization and circuit implementation

A new chaotic attractor with two quadratic nonlinearities, its synchronization and circuit implementation

A new chaotic attractor with two quadratic nonlinearities, its synchronization and circuit implementation

Abstract. A 3-D new chaotic attractor with two quadratic nonlinearities is proposed in this paper. The dynamical properties of the new chaotic system are described in terms of phase portraits, equilibrium points, Lyapunov exponents, Kaplan-Yorke dimension, dissipativity, etc. We show that the new chaotic system has three unstable equilibrium points. The new chaotic attractor is dissipative in nature. As an engineering application, adaptive synchronization of identical new chaotic attractors is designed via nonlinear control and Lyapunov stability theory. Furthermore, an electronic circuit realization of the new chaotic attractor is presented in detail to confirm the feasibility of the theoretical chaotic attractor model.
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A new two-scroll chaotic system with two nonlinearities: dynamical analysis and circuit simulation

A new two-scroll chaotic system with two nonlinearities: dynamical analysis and circuit simulation

For practical implementation of chaotic systems, it is important to design suitable electronic circuit design of chaotic systems [31-35]. Sambas et al. [31] discussed the circuit design of a six-term novel chaotic system with hidden attractor. Sambas et al. [32] derived a circuit design for a new 4-D chaotic system with hidden attractor. Sambas et al. [33] discussed the numerical simulation and circuit implementation for a Sprott chaotic system with one hyperbolic sinusoidal nonlinearity. Vaidyanathan et al. [34] presented a new 4-D chaotic hyperjerk system, and discussed its synchronization, circuit design and applications in RNG, image encryption and chaos-based steganography. Vaidyanathan et al. [35] reported a new chaotic attractor with two quadratic nonlinearities and discussed its synchronization via adaptive control and circuit implementation.
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Investigation of Chaos Behavior in a New Two-Scroll Chaotic System with Four Unstable Equilibrium Points, its Synchronization via Four Control Methods and Circuit Simulation

Investigation of Chaos Behavior in a New Two-Scroll Chaotic System with Four Unstable Equilibrium Points, its Synchronization via Four Control Methods and Circuit Simulation

Abstract—This paper reports the finding of a new 2-scroll chaotic system with four quadratic nonlinear terms. We also discover interesting properties of the new chaotic system such as equilibrium points, bifurcation and Lyapunov exponents. For a comparative study, we apply four different control methods for the global synchronization of the new chaotic system with itself and present a comparative analysis of the results obtained with the four control methods, viz. (A) Adaptive Control, (B) Backstepping Control, (C) Passive Control and (D) Integral Sliding Mode Control. Our results show that integral sliding mode control gives the best results for achieving synchronization of the new chaotic system with itself. An electronic circuit simulation of the new 2-scroll chaotic system is shown using MultiSIM to check the feasibility of the model.
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A novel double-convection chaotic attractor, its adaptive control and circuit simulation

A novel double-convection chaotic attractor, its adaptive control and circuit simulation

Abstract. A 3-D novel double-convection chaotic system with three nonlinearities is proposed in this research work. The dynamical properties of the new chaotic system are described in terms of phase portraits, Lyapunov exponents, Kaplan-Yorke dimension, dissipativity, stability analysis of equilibria, etc. Adaptive control and synchronization of the new chaotic system with unknown parameters are achieved via nonlinear controllers and the results are established using Lyapunov stability theory. Furthermore, an electronic circuit realization of the new 3-D novel chaotic system is presented in detail. Finally, the circuit experimental results of the 3-D novel chaotic attractor show agreement with the numerical simulations.
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A new two-scroll chaotic attractor with three quadratic nonlinearities, its adaptive control and circuit design

A new two-scroll chaotic attractor with three quadratic nonlinearities, its adaptive control and circuit design

In the last few decades, chaotic and hyperchaotic systems have been applied in several areas of science and engineering [1-2]. Some important applications of chaotic systems can be listed out such as chemical reactors [3-5], oscillators [6-8], neural networks [9-10], memristors [11-12], ecology [13-14], robotics [15-16], Tokamak reactors [17-18], finance [19-20], etc.

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PVT-Robust CMOS Programmable Chaotic Oscillator: Synchronization of Two 7-Scroll Attractors

PVT-Robust CMOS Programmable Chaotic Oscillator: Synchronization of Two 7-Scroll Attractors

Chaos synchronization is an important problem in nonlinear science. During the last three decades, synchronization has received a great interest among various scientists [1–7]. The synchronization can be seen as the property shared by some objects to express a uniform rate of coexistence. For example, two harmonic oscillators can be synchronized if their periods are equal. However, for the case of chaotic oscillators, the concepts of frequency and phase are not well defined and, therefore, two chaotic oscillators can be synchronized if eventually, after a transitional time (a long or short time span), the oscillations coincide exactly at all times despite both oscillators started at different initial conditions. The idea of synchronizing two identical chaotic systems from different initial conditions was introduced in the seminal work in [1]. After that, several synchronization schemes were introduced in [50,58–66]. Besides, the practical applications of chaotic synchronization has some limitations to accomplish identical synchronization. For example, parameter mismatch will probably destroy the manifold of a synchronization. To deal with this issue, generalized synchronization approaches were introduced [3,67]. In this manner, we perform the synchronization of two chaotic oscillators following the approach given in [3]. Therefore, the chaos generator model from Equation (3) in Generalized Hamiltonian form, is given by
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On the impulsive synchronization control for a class of chaotic systems

On the impulsive synchronization control for a class of chaotic systems

The remainder of this paper is organized as follows. The model description and preliminaries are proposed in Section 2. Based on impulsive control theory and Lyapunov method, we shall try to propose a new and practical impulsive strategy to realize the synchronization for a class of chaotic systems in Section 3. Finally, some typical examples will be included to show the correctness of the theoretical results in Section 4, and the paper will be concluded in Section 5.

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Application of a Chaotic Synchronization System to Secure Communication

Application of a Chaotic Synchronization System to Secure Communication

to secure communications. The transmission link is established via the Internet and National Instruments LabView, with the information encrypted and decrypted in the transmitter and the receiver, respectively, by computers. The audio signal is transmitted as follows. First, the initial conditions of the system and the sampling amount are determined. An identical number of keys are then generated, with which the audio signal is mixed accordingly. Figures 5 to 7 display the audio processing system, as well as summarize the experimental results. The image counterpart is described as follows. The encryption process is divided into two phases. The first one is the image itself, with both the symmetric key cryptosystem (SKC) and the master/slave system as the key, through which the image signal is encoded despite the same set of initial values. The initial values subsequently vary with the master/slave system status. The second one is the encryption of the master/slave system signal, with a Lorenz system as the key, as a means of removing the interception likelihood during data transmission. Figure 8 illustrates the image encryption/decryption system, where the Lorenz system is of invariant initial conditions; meanwhile, the master chaotic system randomly generates the initial conditions. Figures 9 to 11 summarize the experimental results. An entity photo of a Sprott master/slave system and a sliding mode controller are shown in Fig. 12.
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Category of Attractor and Its Application

Category of Attractor and Its Application

In this paper, we provide a new approach to study the geometry of attractor. By applying category, we investigate the relationship between attractor and its attraction basin. In a complete metric space, we prove that the categories of attractor and its attraction basin are always equal. Then we apply this result to both autonomous and non-autonomous systems, and obtain a number of cor- responding results.

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Isochronal function projective synchronization between chaotic and time delayed chaotic systems

Isochronal function projective synchronization between chaotic and time delayed chaotic systems

Isochronal function projective synchronization between chaotic and time-delayed chaotic systems with unknown parameters is investigated in this article. Based on Lyapunov stability theory, adaptive controllers and parameter updating laws are designed to achieve the isochronal function projective synchronization between chaotic and time-delayed chaotic systems. The scheme is applied to realize the synchronization between time-delayed Lorenz systems and time-delayed hyper- chaotic Chen systems, respectively. Numerical simulations are also presented to show the effectiveness of the proposed method.
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ESTIMATES OF REACHABLE SETS OF CONTROL SYSTEMS WITH BILINEAR–QUADRATIC NONLINEARITIES

ESTIMATES OF REACHABLE SETS OF CONTROL SYSTEMS WITH BILINEAR–QUADRATIC NONLINEARITIES

Abstract: The problem of estimating reachable sets of nonlinear impulsive control systems with quadratic nonlinearity and with uncertainty in initial states and in the matrix of system is studied. The problem is studied under uncertainty conditions with set-membership description of uncertain variables, which are taken to be unknown but bounded with given bounds. We study the case when the system nonlinearity is generated by the combination of two types of functions in related differential equations, one of which is bilinear and the other one is quadratic. The problem may be reformulated as the problem of describing the motion of set-valued states in the state space under nonlinear dynamics with state velocities having bilinear-quadratic kind. Basing on the techniques of approximation of the generalized trajectory tubes by the solutions of control systems without measure terms and using the techniques of ellipsoidal calculus we present here a state estimation algorithms for the studied nonlinear impulsive control problem bilinear-quadratic type.
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Adaptive observers for robust synchronization of chaotic systems

Adaptive observers for robust synchronization of chaotic systems

recurrently investigated in synchronization of chaotic systems are: 1) under which conditions systems synchronize (values of physical parameters, initial conditions, etc.) and consequently, 2) under which conditions one is able to design chaotic sys- tems that synchronize with others? To answer the first question Lyapunov stability theory may be used—cf. [17]–[19], for the second, distinct control approaches have been put to test—cf. [6], [7], [12]–[14]. Some papers rely on analytic study –[8], [20], [21] and others on numerical methods and validation in simulation—cf. [16], [22], [23]. Beyond stability theory, work on synchronization analysis includes the study of synchroniza- tion in networks of oscillators—cf. [24]–[29], relying on tools from e.g., graph theory. Fundamental work on pinning-control- lability just appeared in [24]. In [26] conditions are established in terms of the average coupling path lengths among network nodes; see also [25]. The recent paper [28] establishes synchro-
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A novel fractional order hyperchaotic system with a quadratic exponential nonlinear term and its synchronization

A novel fractional order hyperchaotic system with a quadratic exponential nonlinear term and its synchronization

Chaos synchronization has attracted a great deal of attention since Pecora and Carroll [] established a chaos synchronization scheme for two identical chaotic systems with dif- ferent initial conditions. Various effective methods such as robust control [], the sliding method control [], linear and nonlinear feedback control [], function projective [–], adaptive control [], active control [], backstepping control [], generalized backstep- ping method control [] and anti-synchronization [] have been presented to synchro- nize various chaotic systems.
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Hybrid Synchronization of a Chen Hyper Chaotic System with Two Simple Linear Feedback Controllers

Hybrid Synchronization of a Chen Hyper Chaotic System with Two Simple Linear Feedback Controllers

In order to observe the hybrid synchronization behav- ior of Chen hyper-chaotic system, assume that we have two Chen hyper-chaotic systems where the drive system with four state variables denoted by the subscript 1 and the response system with identical equations denoted by the subscript 2. Obviously, the initial condition on the drive system is different from that of response system. For the system (6), the drive and response systems are defined below, respectively:

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The Response of Two-Degree of Freedom Self-Sustained Systems with Quadratic Nonlinearities to a Parametric Excitation (RESEARCH NOTE)

The Response of Two-Degree of Freedom Self-Sustained Systems with Quadratic Nonlinearities to a Parametric Excitation (RESEARCH NOTE)

oscillations in two-degree-of-freedom systems with qu adratic nonlinearities is investigated. The fundamental parametric resonance of the first mode and 3:1 internal resonance is considered, followed b y 1:2 in ternal and par ametr ic reso nance s of the second m ode. Th e meth od of mu ltiple time scales is app lied t o derive fo u r fir st-or der no n-lin ear or dinar y different ial equations that describe the modulation of the amplitudes and phases of both modes caused by resonance. These equ ations are u sed to determine steady state amplitu des. To determine stability of the steady state solu tions, small distu rbances in the amplitu des and phases are su pe rposed on the stea dy state solu tions and the resu lt ing equ atio ns are linearized. The eigenvalues of the corresponding system of first-order differential equ ations determine the stability of the steady state solutions. The instability modes are discussed and the amplitude and frequency response curves are presented by varying parameters of the system.
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Coexistence of generalized synchronization and inverse generalized synchronization between chaotic and hyperchaotic systems

Coexistence of generalized synchronization and inverse generalized synchronization between chaotic and hyperchaotic systems

The study of nonlinear behaviour, such as stability, control and synchronization of dynam- ical systems, has become an interdisciplinary research. As a result, several research works have been published on this subject by researchers of different disciplines [5, 6, 9, 34]. Due to the importance and interdisciplinary nature of nonlinear dynamical systems, its applications have been discovered in field studies like mathematics, physics, chemistry,

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Two New Types of Chaotic Maps and Minimal Systems

Two New Types of Chaotic Maps and Minimal Systems

Definition 2.4 [10] Let (X,τ) be a topological space and α an operator associated with τ. A subset A of X is said to be α-open if for each x є X there exists an open set U containing x such that α(U) ⊂ A. according to this definition every α-open is open and not conversely. Let us denote the collection of all α-open, semi-open sets in the topological space ( X , τ ) by τ α , SO(τ), respectively. We then have τ ⊆ τ α ⊆ SO ( τ ) . A subset B of X is said to be α- closed [7] if its complement is α-open.

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ADAPTIVE SYNCHRONIZATION OF UNCERTAIN LI AND T CHAOTIC SYSTEMS

ADAPTIVE SYNCHRONIZATION OF UNCERTAIN LI AND T CHAOTIC SYSTEMS

This paper has been organized as follows. In Section 2, we derive results for the adaptive synchronization of identical uncertain Li systems (2009). In Section 3, we derive results for the adaptive synchronization of identical uncertain T systems (2008). In Section 4, we derive results for the adaptive synchronization of non- identical Li and uncertain T systems. In Section 5, we summarize the main results obtained in this paper.

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Fuzzy synchronization of the 3D chaotic systems using belbic

Fuzzy synchronization of the 3D chaotic systems using belbic

Control of complex irregular dynamics has evolved as one of the central issues in applied nonlinear science during the last decade. Nowadays the notion of chaos control involving stabilization of unstable periodic or stationary states in nonlinear dynamic systems has been extended to a much wider class of problems. Since the discovery of chaos synchronization introduced in (Carroll, 1990), there have been tremendous interests in studying the synchronization of chaotic systems. Recently, much research on the fuzzy model- based designs to stability and synchronization for chaotic systems have been carried out based on Takagi–Sugeno (T–S) fuzzy models (Park et al., 2002; Lian et al., 2001). In (Yan- Wu Wang et al., 2003), a fuzzy model-based designs for Chen’s chaotic stability and synchronization have been proposed. Based on the fuzzy hyper chaotic models, simpler fuzzy controllers have been designed for synchronizing hyper chaotic systems in (Hongbin Zhang, 2005). In this work, utilizing BELBIC model introduced in (Ali Reza Mehrabian et al., 2006; Saeed Jafarzadeh et al., 2008), we will design an intelligent controller for synchronization of two new 3D
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Control and Synchronization of a Fractional-order Chaotic Financial System

Control and Synchronization of a Fractional-order Chaotic Financial System

Abstract. In this paper, we study the synchronization control problem of a class of fractional-order chaotic financial systems with uncertain parameters. Based on the theory of fractional order stability and adaptive control method, a simple fractional-order synchronous controller of two fractional-order chaotic financial systems is designed, and a simple theoretical analysis is given to prove that the error system is stable. Then two fractional-order hybrid synchronization methods are proposed. Finally numerical simulation demonstrates the validity of methods.
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