Research Article  Open Access
Ying Li, Xiaozhu Xia, Yicheng Zeng, Qinghui Hong, "Composite One to SixScroll Hidden Attractors in a MemristorBased Chaotic System and Their Circuit Implementation", Complexity, vol. 2020, Article ID 3259468, 13 pages, 2020. https://doi.org/10.1155/2020/3259468
Composite One to SixScroll Hidden Attractors in a MemristorBased Chaotic System and Their Circuit Implementation
Abstract
Chaotic systems with hidden multiscroll attractors have received much attention in recent years. However, most parts of hidden multiscroll attractors previously reported were repeated by the same type of attractor, and the composite of different types of attractors appeared rarely. In this paper, a memristorbased chaotic system, which can generate composite attractors with one up to six scrolls, is proposed. These composite attractors have different forms, similar to the Chua’s double scroll and jerk double scroll. Through theoretical analysis, we find that the new system has no fixed point; that is to say, all of the composite multiscroll attractors are hidden attractors. Additionally, some complicated dynamic behaviors including various hidden coexisting attractors, extreme multistability, and transient transition are explored. Moreover, hardware circuit using discrete components is implemented, and its experimental results supported the numerical simulations results.
1. Introduction
Recently, much effort has been devoted to the analysis of various chaotic systems owing to its potential applications [1–4]. To our knowledge, chaotic attractors are categorized as either selfexcited attractors [5–7] or hidden attractors [8–11]. It should be particularly pointed out that hidden attractors have neither homoclinic nor heteroclinic orbits; thus, the Shil’nikov theorem [12] cannot be utilized to verify the existence of chaos, so that hidden chaotic systems attract great attention of scholars, and increasing number of researchers begin to study the rich dynamic behaviors of them.
As is known to all, multiscroll chaotic systems have aroused extensive interests for their much complicated dynamical properties than singlescroll ones. So, it is a more desirable task to explore the hidden multiscroll chaotic system, and there have been emerging related literatures on this topic. In 2016, Jafari et al. presented a novel noequilibrium chaotic system with multiscroll hidden chaotic sea by introducing a sine function into a 3D chaotic system [13]. In the same year, Hu et al. constructed two simple 3D chaotic systems without equilibrium based on an improved Sprott A system by adding a nonlinear function, from which hidden multiscroll attractors can be obtained [14]. Later, a new class of PWL dynamical system without equilibrium whose hidden chaotic attractors can display grid multiscroll has been introduced [15]. Deng and Wang proposed a multiscroll hidden chaotic system that has only two stable nodefoci equilibrium points [16]. Hong et al. investigated a novel method for designing multidirection multibutterfly chaotic attractors (MDMBCA) without reconstructing nonlinear functions [17]. Furthermore, some memristive chaotic systems, which can generate hidden multiscroll or multiwing chaotic attractors, are reported [18, 19]. However, all of the hidden multiscroll attractors discussed above are of the same type attractor repeated in unidirectional or multidirection ones. Are there hidden multiscroll attractors, which are composed of different attractors? We are surprised that the answer is positive.
If an attractor is compounded from two or more different singlescroll attractors, which is called composite attractor, its dynamic characteristics are more complicated. The composite attractor has been already discovered in some selfexcited chaotic systems. For example, Cang et al. proposed a Lorenzlike system with composite structure by controlling system parameters [20]. Zhang et al. reported an autonomoussystembased approach for creating composite chaotic attractors from a class of generalized Lorenz systems via switching control [21]. And then, Xiong et al. constructed a chaotic system, which can generate composite fourscroll attractor by adding a symbolic function into a 3D jerk system [22]. However, although the complexity of dynamic behavior of these chaotic systems, which can produce composite attractors, has increased, the operation methods and state equations have also been correspondingly complicated, and the circuit experiment is difficult to realize. Besides, these composite multiscroll chaotic attractors mentioned above are limited to selfexcited attractors, and the hidden composite multiscroll attractors have not been reported up to now. It is obvious that designing a simple chaotic system, which can generate hidden composite multiscroll attractors, is a meaningful task.
Based on these considerations, we introduce a quadratic fluxcontrolled memristor into the 3D jerk chaotic system to construct a memristorbased hidden composite multiscroll chaotic system, which can produce composite one to sixscroll hidden attractors through changing only one system parameter. It is pointed out that the composite sixscroll hidden attractor is composed of a Chua’s doublescroll attractor and two jerk doublescroll attractors. Compared with [22], this new memristorbased hyperchaotic system has more complex dynamic behaviors including hyperchaotic composite multiscroll hidden attractors and extreme multistability phenomenon. These composite multiscroll attractors break the previous pattern of the same singlescroll attractor that appeared repeatedly and has not been reported in previous literature.
The rest of this paper is organized as follows. In Section 2, the mathematical model of the proposed memristive hyperchaotic system and its typical attractor are presented. In Section 3, complex hidden dynamic behaviors of this new system including controllable multiscroll hidden chaotic or hyperchaotic attractors, coexistence of hidden attractors, extreme multistability, and transient transition behavior are described. In Section 4, the corresponding circuit implementation and experiment results are presented. The conclusion is presented in the last section.
2. Memristive Hyperchaotic System and Its Typical Attractors
In 2016, Kengne et al. performed a simple 3D autonomous jerk system with cubic nonlinearity [23], which is described aswhere x, y, z are state variables, and a, b are positive tunable parameters. In order to construct a memristorbased hyperchaotic system, a quadratic fluxcontrolled memristor model [24] described in equation (2) is added into system (1):where u, and i denote the internal state of the memristor, the input of the memristor, and the output of the memristor model, respectively. The m, n are two real parameters of the memristor model. So, we constructed a 4D memristorbased chaotic system, which can generate composite multiscroll hidden attractors, and it is described asin which x, y, z are state variables, a, b, c, k are real parameters, W (u) = (m + nu) is the memductance function, and p is positive control parameter. From a dissipative perspective, the divergence of the new system (3) can easily be obtained as follows:at any given point (x, y, z, u) of the state space. Consequently, the general condition of dissipativity related to the existence of attractive sets in our model is satisfied. The equilibrium points of system (3) can be obtained by solving the following equations: . It is obvious that the equations have no real solutions when parameter p is positive. That is to say, system (3) has no equilibrium, and it belongs to hidden chaotic system.
When fixing the control parameters a = 3.5, b = 0.8, m = 0.1, n = 0.3, , k = 0.2, c = 0.01 and selecting the initial conditions as (0.1, 0.1, 0.1, 0.1), a composite sixscroll hidden chaotic attractor and its Poincaré map on y = 0 section as well as power spectrum are displayed in Figures 1(a)–1(c). As is depicted in Figure 1(a), the sixscroll attractor is composed of a Chua’s doublescroll attractor and two jerk doublescroll attractors, and the two small jerk doublescroll attractors are inside the large Chua’s doublescroll attractor, respectively. It is surprising that the composite sixscroll hidden chaotic attractors have never appeared before as far as we know.
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3. Dynamic Analysis and Numerical Investigations
In this section, multifarious complicated dynamic behaviors including controllable multiscroll hidden attractors, coexisting of hidden chaotic or hyperchaotic attractors, extreme multistability, and transient transition behaviors of proposed system (3) are investigated in detail by means of Lyapunov exponent spectra, bifurcation diagrams, phase portraits, and time series. Note that all numerical simulations are carried out on MATLAB software, and the first 20000 points are discarded in the phase portraits.
3.1. Controllable Multiscroll Hidden Chaotic or Hyperchaotic Attractors
One interesting phenomenon is that the newly proposed system (3) can generate composite one to sixscroll hidden attractors by changing only one system parameter. Fixing the control parameters b = 0.8, m = 0.1, n = 0.3, k = 0.2, c = 0.01, and changing the parameter a in the interval of [1.3, 5] with the initial conditions (0.1, 0.1, 0.1, 0.1), the corresponding bifurcation diagram is drawn in Figure 2(a). Additionally, using the famous Wolf method [25], the corresponding Lyapunov exponent spectrum proves the complexity of system (3) as depicted in Figure 2(b).
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In reference to Figure 2(b), system (3) undergoes chaotic and hyperchaotic routes as follows: chaotic (1.3 ≤ a < 1.5) ⟶ hyperchaotic (1.5 ≤ a < 2.65) ⟶ chaotic (2.56 ≤ a < 3.06) ⟶ hyperchaotic (3.06 ≤ a < 3.42) ⟶ chaotic (3.42 ≤ a < 5). What surprised us is that system (3) generates composite one to sixscrolls hidden attractors when selecting appropriate parameters, and these attractors may exhibit either a symmetric or asymmetric structure. It is rare to see such attractors in an asymmetric system. Some typical hidden chaotic or hyperchaotic attractors with different values of parameter a are shown in Figures 3(a)–3(l). Note that Figures 3(a) and 3(b) display a pair of asymmetric singlescroll hidden chaotic attractors at a = 1.38 and 2.92. Figures 3(c) and 3(d) show a pair of symmetric doublescroll hidden hyperchaotic attractors at a = 2.3 and 2.55, and the corresponding Lyapunov exponents are (0.213, 0.179, 0, −1.381) and (0.255, 0.209, 0, −1.444), respectively. Figures 3(e) and 3(f) exhibit two different doublescroll hidden chaotic attractors at a = 2.946 and 5. And a pair of asymmetric composite 3scroll hidden chaotic and hyperchaotic attractors are drawn in Figures 3(g) and 3(h) with a = 2.974 and 3.117. Furthermore, a pair of symmetric composite 4scroll hidden chaotic and hyperchaotic attractors, a composite 5scroll hidden chaotic attractor, and a composite 6scroll hidden hyperchaotic attractor are presented in Figures 3(i) and 3(l) with a = 3.03, 3.076, 3.055, and 3.125, respectively. To explain more intuitively and clearly, the different types of attractors with different values of parameter a are listed in Table 1. Consequently, the unusual controllable multiscroll hidden chaotic or hyperchaotic attractors of system (3) are innovative.
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3.2. Coexistence of Hidden Attractors
Nowadays, attractor coexisting is one of the common nonlinear dynamic phenomena, which is a chaotic system performing more than one concurrent attractor for a given set of system parameters under the different initial conditions [26–32]. In this section, the coexistence of hidden attractors with some specific parameters setting and initial conditions in system (3) is discussed. By selecting the control parameters as b = 0.8, m = 0.1, n = 0.3, k = 0.2, c = 0.01, , the coexisting bifurcation diagram of the state variable x with respect to the parameter a is described in Figure 4(a). Figure 4(b) displays the Lyapunov exponent spectrum under the initial conditions (−0.1, −0.1, −0.1, −0.1), which is in accordance with the Lyapunov exponent spectrum under the initial conditions (0.1, 0.1, 0.1, 0.1) in Figure 2(b). Various composite multiscroll chaotic or hyperchaotic hidden coexisting attractors are shown in Figure 5; they are including symmetric attractors and asymmetric attractors coexisting, odd number of attractors, and even number of attractors coexisting. The more detailed information is displayed in Table 2. All in all, it is informative and rare that so many composite multiscroll attractors coexist, which injects new blood into the field of chaos coexisting.
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3.3. Extreme Multistability Relying on Memristor Initial Condition
In this subsection, we further studied the extreme multistability phenomenon [33–38] in system (3). To reveal extreme multistability phenomenon relying on memristor initial condition, the typical parameters a = 3.05, b = 0.8, c = 0.01, m = 0.1, n = 0.3, k = 0.2, and initial conditions x (0) = 0.1, y (0) = 0.1, z (0) = 0.1 are fixed. When the memristor initial condition u (0) is increased gradually from −4.8 to 10, the bifurcation diagram of the state variable x and the Lyapunov exponent spectrum are plotted in Figures 6(a) and 6(b), respectively. As can be seen from Figure 6, the system has extremely rich dynamic characteristics.
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To explain the coexistence of infinite number of attractors in system (2) more intuitively, several special values of u are selected as shown in Table 3 and the phase diagrams of the infinite coexisting attractors as shown in Figure 7.

Specially, when setting a = 20, b = 0.8, m = 0.1, n = 0.3, k = 0.2, c = 0.01, and initial conditions x (0) = 0.1, y (0) = 0.1, z (0) = 0.1, and change the memristor initial condition u (0) in the region of [0, 8], the bifurcation diagram is plotted in Figure 8. In light of Figure 8, it is clear that the system goes through reverse period doubling bifurcation route from chaos to periodic. In order to illustrate this phenomenon of extreme multistability, there are seven types of hidden attractors, which are presented in Figure 9. In fact, more different types of hidden attractors can be obtained under the different initial conditions. In general, Figures 7–9 intuitively reveal the coexisting infinitely many hidden hyperchaotic attractors, which indicates that system (3) possesses hidden extreme multistability indeed.
3.4. Transient Transition Behavior
In system exhibiting transient transition, the orbit is from one state (chaotic, periodic) to another state (chaotic, periodic) for a finite time interval before settling into a final state. Transient chaos with boundary crisis is often encountered in nonlinear dynamic systems [22, 39–43]. For the sake of verifying transient transition behavior in system (3), the system parameters are considered as a = 3.115, b = 0.8, m = 0.1, n = 0.3, k = 0.2, c = 0.01, , while the initial conditions are selected as (0.1, 0.1, 0.1, 0.1) and the time is t = 1000 s, and a phase diagram of six scrolls and the corresponding timedomain waveform with state variables x and z are shown in Figures 10(a)–10(c). Figure 11 displays three different phase diagrams with different simulation time and the Lyapunov exponent spectrum with increased time. From the Lyapunov exponent spectrum in Figure 11(d), it is clearly seen that there are two Lyapunov exponents greater than zero at t = 80 s; that is to say, system (3) transitions from chaotic to hyperchaotic in the time of t = 80 s.
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4. Circuit Implementation and Experiment Results
Circuit implementation provides an alternative approach to explore the novel noequilibrium memristive hyperchaotic system (3), and it is the key to the chaos application. In this part, a suitable electrical circuit is designed and a hardware circuit is implemented to verify the theoretical results obtained previously. The circuit diagram of the proposed system (3) is provided in Figure 12, and the circuits in the dashed box are constructed for the symbolic function circuit and memristor equivalent circuit.
The operational amplifiers of Figure 12 are LF353, whose supply voltages are ±15 V. And multipliers A_{1}, A_{2}, A_{3} are AD633 with output coefficient of 0.1. Based on system (3), select the system parameters as a = 3.5, b = 0.8, m = 0.1, n = 0.3, k = 0.2, c = 0.01, and let γ = γ_{0} t, where γ_{0} = 10000 is the timescale transformation factor and system (3) can be rewritten bywhere W(u) = (m + nu). Considering Kirchhoff’s law, the circuit equation of system (3) can be written asHere, , , and are the voltages on capacitors C_{1}, C_{2}, C_{3} and C_{u}, respectively, and the capacitors C_{1} = C_{2} = C_{3} = C_{u} = 10 nF, = −1 V. Comparing equation (5) with equation (6) and keeping the corresponding coefficients equal, one gets R_{1} = R_{2} = R_{4} = R_{8} = 10 kΩ, R_{3} = 2.86 kΩ, R_{5} = R_{10} = 10 MΩ, R_{6} = 5 kΩ, R_{7} = 12.5 kΩ, R_{9} = 100 Ω, R_{m} = 500 kΩ, R_{n} = 16.7 kΩ. Then, according to the circuit diagram in Figure 12, some offtheshelf discrete components are used on the breadboard to build the hardware circuit as shown in Figure 13 and the parameters in the circuit are set as above. We can see a composite sixscroll chaotic attractor as shown in Figure 14(a) by using digital oscilloscope, which is well consistent with the phase diagram simulated with MATLAB in Figure 1(a). Lastly, keeping the values of R_{1}, R_{2}, R_{4}, R_{5}, R_{6}, R_{7}, R_{8}, R_{9}, R_{m} and R_{n} unchanged, and adjusting the values of R_{3} to appropriate resistance, other composite multiscroll attractors can be obtained from this hardware circuit as shown in Figures 14(b)–14(f), which also agree with the results of MATLAB simulation aforementioned. All of what is discussed above demonstrates the effectiveness and feasibility of system (3).
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5. Conclusion
In this paper, a memristorbased chaotic system with abundant dynamic behaviors is reported. Compared with other memristorbased chaotic systems, the new system can display composite one to sixscroll hidden attractors by changing only one system parameter. And the composite multiscroll attractors are composed of different types of attractors. For example, a composite sixscroll attractor is composed of a Chua’s doublescroll attractor and two jerk doublescroll attractors. The coexistence of symmetric and asymmetric attractors with different numbers of scrolls also reflects the particularity of the system. Furthermore, extreme multistability phenomenon and chaotic transient transition are investigated in the system. Finally, the feasibility of the proposed chaotic system is verified by hardware circuit, and the results match very well with the numerical simulations. Due to the fact that such a new chaotic system constructed in this paper has complex dynamic properties, it could be utilized advantageously in chaosbased engineering applications including image encryption, random bit generation, and chaosbased secure communication, and for future investigation.
Data Availability
The MATLAB simulation program data used to support the findings of this study are included within the supplementary information file. The simulation data of the study are reflected in the manuscript.
Conflicts of Interest
The authors declare that they have no conflicts of interest.
Acknowledgments
The work was supported by the National Natural Science Foundations of China under Grant no. 62071411 and the Fundamental Research Funds for the Central Universities under Grant no. 531118010418.
Supplementary Materials
The following is the supplementary description for the given supplementary material. Appendix A: MATLAB simulation code for phase portrait. Appendix B: MATLAB simulation code for bifurcation diagram. Appendix C: MATLAB simulation code for Lyapunov exponent spectrum. (Supplementary Materials)
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