Conditional Symmetry of a Memristive System with Amplitude and Frequency Modulation Control

Zang, Hongyan; Huang, Lili; Lei, Tengfei; Wang, Yanling

doi:https://doi.org/10.1155/2021/4924323

Mathematical Problems in Engineering

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Research Article | Open Access

Volume 2021 | Article ID 4924323 | https://doi.org/10.1155/2021/4924323

Conditional Symmetry of a Memristive System with Amplitude and Frequency Modulation Control

Hongyan Zang,¹Lili Huang,¹Tengfei Lei,¹and Yanling Wang¹

Academic Editor: Zenghui Wang

Received15 Apr 2021

Accepted05 Jul 2021

Published17 Jul 2021

Abstract

In this study, we studied the effects of offset boosting on the memristive chaotic system. A system with symmetry and conditional symmetry was constructed, by adding the absolute value function to an offset boosting system. It is proved that the symmetric system or a conditionally symmetric system can be constructed with similar or the same dynamic characteristics by using certain correction and offset boosting in an asymmetric system. In addition to multiple stability, the memristive system can also realize the amplitude and frequency control by introducing a parameter. The simulation circuit verifies the amplitude modulation characteristics of the system.

1. Introduction

As the fourth basic circuit element, the memristor has attracted an extensive attention in the nonlinear field. In 1971, Chua proposed a memristor to represent the relationship between charge and flux from the view of symmetry when analyzing the relation among the voltage, current, charge, and flux. In 2008, HP laboratory released a TiO₂ charged memristor [1], declaring that a memristor was found. A large number of research studies on memristor models and typical chaotic systems have been published, making the memristor widely studied in secure communication [2, 3], cryptography [4, 5], image encryption [6, 7], associative memory [8, 9], voice encryption [10], and recognition and sequencing application [11]. Wang et al. [12] reported a special bursting behavior previously unobserved in third-order autonomous memristive circuits. Wang et al. [13] developed a simple scheme implementing a multisegment piecewise-linear Chua’s diode and an inductor-free multiscroll Chua’s circuit. In addition, the application of the memristor in artificial synapses has also been started, which is expected to be used for memristor calculation or system design. Many characteristics have also been widely studied, such as hidden attractors [14–17], coexisting attractors [18], multistability [19–21], symmetry [22, 23], amplitude control [24, 25], and offset boosting [26–29]. In [30], a simple parametric control scheme for generation of the multiscroll chaotic attractor from the jerk system has been presented. In [31], a modified Chua’s circuit with a 5-segment piecewise-linear Chua’s diode is presented, in which hidden attractors and coexisting attractors are identified.

Many scientists have shown that some signals do not require additional peripherals to provide pretuning, such as amplitude controllable, frequency controllable [32], and conditional symmetric attractors [23, 33, 34] in an asymmetric system, extremely multistability attractors [35–37], and so on.

In [38], Li and Sprott researched on amplitude of a chaos dynamical system. The chaos dynamical system can be controlled by the coefficient of one or more terms without changing the dynamics. In [39], cosine function was introduced to keep the polarity balance and conditional symmetric coexisting chaotic attractors. It was found that the initial condition can be used to change the starting oscillation as well as the amplitude and frequency [40]. The output polarity of the signal can be adjusted by adding a DC voltage source [41]. As is known to all, asymmetric systems give coexisting attractors from different directions. Offset boosting can be used to construct conditional symmetry to achieve polar balance.

In this study, an offset boosting chaotic system was constructed with the following properties: being of conditional symmetry, amplitude modulation, and frequency modulation. In Section 2, the model of the memristive chaotic system is introduced and its dynamical properties are investigated. In Section 4, amplitude modulation and frequency modulation are described. In Section 5, bifurcation and coexisting attractors are analyzed. In Section 6, circuit implementation is discussed. Section 7 gives conclusion and discussion.

2. System Model Description

2.1. Mathematical Model

A new chaotic system is obtained based on the chaotic system variable boosting VB24 [42]. The chaotic system (VB24) has only one linear term, one constant term, and four quadratic terms. We added an absolute value function to VB24. Its new system mathematical model is expressed aswhere x, y, and z are the three dynamical variables, and a and c are all positive parameters. b is a nonzero constant term. In system (1), an absolute value memristor is introduced to construct a four-dimensional memristor chaotic system (2).

The variable constraint relation of memristor is as follows:

The parameters of the system (3) are a = 1.5, b = 0.7, c = 0.5, and initial condition (IC) is (1 0 0 0). The Lyapunov exponents are LE1 = 0.117031, LE2 = 0.000306, LE = −0.401139, and LE4 = −1.190722, when time step is 1 s and time length is 500 s. Numerical simulation software MATLAB is used to numerical simulation, and the phase trajectories of each plane are shown in Figure 1. The attractor of system (1) is asymmetric attractor; it has no symmetry about any coordinate axis and does not have reflection symmetry, rotation symmetry, and inversion symmetry.

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2.2. Dynamical Analysis

With conventional dynamical analysis tools, such as bifurcation diagram and Lyapunov exponent spectrum, the dynamical behavior of the chaotic system are explored under the varying parameters a, b, and c.

Under the conditions of the fixed parameters b = 0.7, c = 0.5, and the fixed initial value, Lyapunov exponent and the corresponding bifurcation diagram of the state variable are shown in Figure 2, when the parameter a increases gradually from 0 to 5. Both the unstable and stable regions obtained by the Lyapunov exponent spectrum are consistent with those obtained by the bifurcation diagram in Figure 2. In the interval a ∈ [0, 2.9], the system is mainly in a chaotic state and there is a small window of the periodic orbit. The attractor gradually transitions from double to a single scroll attractor. For example, when a = 0.3, the system is double scroll, a = 1.5, the system is single scroll, and a = 0.9, the negative scroll become weaker. When a ∈ [2.95, 3.8] ∪ [4.2, 4.3] ∪ [4.8, 5], the system is a limit cycle. For example, when a = 3.5, the system is periodic of cycle 1, a = 4.5, the system is periodic of cycle 2, and a = 4.4, the attractor become sink. For diﬀerent values of a, several typical phase diagrams of the plane with respect to parameter a are shown in Figure 3.

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When c varies from 0 to 3 and other parameters are unchanged under the initial condition (1, 0, 0, 0), the bifurcation diagram of the state variable and the corresponding Lyapunov exponent spectrum are shown in Figure 4, respectively. As shown in Figure 4(a), the system is chaotic when c ∈ [0, 1.1] ∪ [2.85, 3], and the largest Lyapunov exponent is positive. When c ∈ [1.4, 1.5] ∪ [1.7, 1.8] ∪ [2, 2.8], system (2) is periodic. When c ∈ [1.2, 1.35] ∪ [1.8, 2], the system drops into an interval of chaotic and periodic states alternate with each other. For diﬀerent values of c, several typical phase diagrams of the plane with respect to parameter a are shown in Figure 5.

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3. Symmetry and Conditional Symmetry

3.1. Symmetry

By using to replace in x-dimension, a new four-dimensional memristive chaotic system is designed, and its state equation is

After the transformation of () ⟶ (), system (4) has a three-dimensional inversion symmetry property relative to . The two attractor phase orbital diagrams with inversion symmetry are shown in Figure 6.

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3.2. Conditional Symmetry

Here, the absolute value functions and are introduced to replace the variables x and y. The new system can be described as

The new absolute value function meet and meet . The increase of two absolute value functions not only does not change the dynamic characteristics of the original system but also brings additional conditional symmetry properties. Figure 7 shows two chaotic attractor phase diagrams with conditional symmetry under the transformation of , , , and , when a = 1.5, b = 0.7, c = 0.5, d = 35, and e = 50. The original asymmetric system now has symmetry, but it is different from other systems where two attractors are in two systems. System (5) only needs to change the initial state of the system to achieve the coexistence symmetry.

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4. Amplitude Modulation and Frequency Modulation

The system (5) is scaled by , , , , , and , and the scale transformation is carried out. The phase diagrams of system (6) at different scales of k = 1, 3, 5, and 8 with initial values IC = (1, 1, 1, 3), a = 1.5, b = 0.7, and c = 0.5 are shown in Figure 8. The signals x and z are the bipolar signals, so their amplitude changes in both positive and negative directions, but their average value is zero. The output signal y is a unipolar signal, and its amplitude changes positively, and the mean value increases with the change of parameter k. The output signal is a bipolar signal, but it is not regulated. Its mean value is zero, and its amplitude is almost unchanged. The waveform shows the change in the amplitude of signals caused by the correction of parameter k and the effect on the oscillation frequency of the system. The waveforms and average values of x(t), y(t), z(t), and with parameter k are shown in Figure 9.

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5. Bifurcation Analysis

When the parameters a = 1.5, b = 0.7, d = 15, e = 10, and c ∈ [0, 3], system (5) has other coexisting attractors, as shown in Figure 10, where the red trajectory corresponds to the initial condition (1 1 0 3) and the blue trajectory corresponds to the initial condition (−1 1 0 −3). It can be seen that the system is periodic when c = 2.5 and chaos when c = 1.5. The negative and positive bifurcations show the same Lyapunov exponent except in the region c = (2.42, 2.55). The system is chaotic when c [0.23, 2.42], and the largest Lyapunov exponent spectrum is positive at the initial values (1, 1, 0, 3). The coexistence period window of different structures appears in a small range near c = 2.5. The system drops into a periodic window, while c (2.42, 2.55) at the initial values (−1, 1, 0, −3). The bifurcation diagram of the state variable x and the corresponding Lyapunov exponent are shown in Figure 10.

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6. Circuit Implementation

In order to verify the chaotic behavior of the system, according to equation (6), the circuit equation is designed as equation (7) and the designed analog circuit diagram is shown in Figure 11. The circuit is composed of four channels, realize the integration, addition, and subtraction of state variables x, y, z, and . The operational amplifier 741 performs the addition and integration, and the analog multiplier AD633 performs the nonlinear product operation.where , respectively, indicate the voltage of x, y, z, and . Let t = , where is the dimensionless time. The amplitude modulation method in system (6) is used for the scale transformation of the circuit. The parameters are taken as follows: = 1 nF, = = = = = = = = R = 100 kΩ, = R/a, = R/a, = R/(k²b), = R/k, = R/c, = R/k, = 2R, = R/k, = = = = = 10 kΩ.

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The corresponding phase trajectories of system (6) when k is equal to 1/3, 1, and 2, predicted by Multisim simulation are shown in Figure 12. By comparing Figures 12 and 8, it can be seen that the phase diagram of Multisim and MATLAB is basically the same. The difference between the amplitude of the corresponding circuit simulation and the MATLAB numerical simulation is mainly due to the saturation distortion caused by the voltage range of the simulator, which can be solved by scaling the whole system. In this study, in order to verify the appearance of amplitude modulation, amplitude control is realized only by changing the parameter k. The results and discussion may be presented separately or in one combined section and may optionally be divided into headed subsections.

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7. Conclusions

In this study, an offset boosting chaotic system was constructed. The dynamical behavior of the system is demonstrated by phase trajectories, Lyapunov exponents, and bifurcation diagrams. The following conclusions are obtained. (1) Absolute value function is introduced in the chaotic system with variable boosting. A chaotic system of conditional symmetry is constructed and analyzed. It is proved that a symmetric system or a conditionally symmetric system can be constructed by using offset boosting. (2) The dynamic characteristics of the new system generated by scale change are the same as that of the original system, but a nonbifurcation parameter can be formed to adjust the amplitude and frequency of system (3). The simulation circuit verifies the amplitude modulation characteristics of the system.

Data Availability

The data used to support the findings of this study are available from the corresponding author upon request.

Conflicts of Interest

The authors declare that there are no conflicts of interest.

Acknowledgments

This work was supported by Shandong Province Key Research and Development Plan (2019GGX104092) and the Natural Science Foundation of Shandong Province (ZR2020KA007).

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Copyright © 2021 Hongyan Zang et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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