#### Abstract

A modified fractional-order Chua chaotic circuit is proposed in this paper, and the chaotic attractor is obtained for . Based on the Mittag-Leffler function in two parameters and Gronwall’s Lemma, two control schemes are proposed to stabilize the modified fractional-order Chua chaotic system via the Caputo derivative of a single input. The numerical simulation shows the validity and feasibility of the control scheme.

#### 1. Introduction

Chaotic phenomena have been observed in many physical systems, such as Chua’s circuit and its fractional-order model [1, 2], the brushless DC motor [3], the microelectromechanical system [4], and the fractional-order gyroscopes [5]. Sometimes, chaos is undesirable in the field of mechanical engineering and power transmission, for example, in motor system, in sensor system, and in power transmission system, because the chaotic behavior can destroy the stable operation of system. In fact, chaos control is usually a prerequisite for many practical applications in chaos engineering, such as permanent magnet synchronous motor [6], complex networks control [7], authenticated encryption [6], and chaos communications [8]. So, chaos control is of great practical significance and has received great interest due to its potential application in many fields in the recent years. Up to now, many control schemes have been proposed, like OGY scheme [9], OPF scheme [10], backstepping scheme [11], and so on [12–14].

On the other hand, the stability of linear fractional-order system can be easily proved by the method proposed by Matignon [15]. However, this method can not be used to deal with the nonlinear fractional-order system. Based on Matignon’s method [15], the local stability result for the nonlinear fractional-order system is proposed by Ahmed et al. [16]. In Ahmed’s method [16], to evaluate the local stability of the equilibrium points in nonlinear fractional-order system, the nonlinear system is converted to a linear system by linear approximation near the equilibrium point. Now, many researchers always used the Ahmed method to control the nonlinear fractional-order chaotic systems [17–19]. But, it is known that the nonlinear problems of fractional-order systems can not be straightforward changed to the linear problems. So, this local stability [16] maybe needs to be further studied.

Motivated by what is mentioned above, based on the Mittag-Leffler function in two parameters and Gronwall’s Lemma, a modified fractional-order Chua’s chaotic circuit can be stable via a fractional-order scalar controller, which can be determined by the Caputo fractional derivative of a single input. Ahmed’s method [16] is not used in our paper. The numerical simulations are given and show the feasibility of the control scheme.

This paper is organized as follows. In Section 2, a modified fractional-order Chua’s chaotic circuit is reported, and the chaotic attractor is given. In Section 3, two control schemes are proposed to stabilize this fractional-order Chua’s chaotic circuit, and the numerical simulations are given. Conclusion is given in Section 4.

#### 2. A Modified Fractional-Order Chua’s Chaotic Circuit

Chua’s circuit [20] was the physical chaotic system discovered by Chua et al. in 1986. Since then, Chua’s circuit has been chosen as a classical paradigm in the research of chaos. Now, some modified Chua’s circuits including their fractional-order model have been reported by many researchers. In 2010, Muthuswamy and Chua [21] reported a simplest and autonomous modified Chua’s chaotic circuit which includes only three elements in series. Based on [21], a modified Chua’s circuit with fractional order is given in this paper, and its mathematical model is shown as follows:where is the fractional order and is the Caputo fractional derivative for state variable . Here , is the smallest integer larger than , , and is the th derivative in the usual sense.

By numerical calculation [22], we can obtain that the largest Lyapunov exponent (LLE) of fractional-order Chua’s circuit (1) is larger than zero for . Conversely, for , the LLE is smaller than zero. The LLE of fractional-order Chua’s circuit (1) with respect to the fractional-order is shown in Figure 1. For example, the LLE is 0.1329 for , and its chaotic attractor is shown as in Figure 2. The LLE is 0.1356 for .

According to what is mentioned above, the fractional-order Chua’s circuit (1) is chaotic for .

#### 3. Stabilization of the Fractional-Order Chua’s Chaotic Circuit (1)

In this section, how to stabilize the fractional-order Chua’s chaotic circuit (1) will be discussed. First we report some preliminary results.

Lemma 1 (see [23] Gronwall’s Lemma). *Let , , and be real-valued piecewise continuous functions, and let be nonnegative in a real time interval . For all in , ifthen*

Lemma 2 (see [24] Wen et al., 2008). *Consider a real matrix , and let be its eigenvalues. If holds, thenwhere be a constant, is the norm for , and is the Mittag-Leffler function in two parameters .*

Now, we are in the position to state the main result of this paper.

Theorem 3. *Let the controlled system bewhere fractional-order , let be a fractional-order scalar controller determined by the Caputo derivative of the state variable , and let be suitable feedback coefficient. If , then is a stable solution of the nonlinear fractional-order system (5).*

*Proof. *System (5) can be rewritten aswhereLetting be a constant, it is easy to obtain the following:According to system (6), it is easy to obtain thathenceAccording to (9)–(11), there exist a constant and such thatfor and .

According to the controlled system (6), one can obtain the eigenvalues of matrix as follows:Because , one hasAccording to (13)–(15), we haveNext, we study solution in the fractional-order system (6). Now, one can take Laplace transform on system (6) and haswhere is the initial condition. So one has Meanwhile, one can take Laplace inverse transform for (19) and obtainGive arbitrarily small, and consider solution in system (6) with initial condition . Using formulas (4), (8), (12), and (17), (20) givesUsing Lemma 1, inequality (21) can be changed asDue to in time interval and in time interval , soBy (23), inequality (22) can be changed as follows:Since is arbitrarily small, when time is long enough, based on inequality (24), one can obtain that is a stable solution of the controlled system (5), which allows concluding the proof.

For example, let the initial conditions be ; the simulation result is shown as in Figure 3 with .

Theorem 4. *Let the controlled system bewhere fractional-order , let be a fractional-order scalar controller determined by the Caputo derivative of the state variable , and let be suitable feedback coefficient. If , then is a stable solution of system (25).*

*Proof. *System (25) can be rewritten aswhereNow, we can complete the proof in a similar way with Theorem 3.

For example, let the initial conditions be ; the simulation results are shown as in Figure 4 with .

#### 4. Conclusions

Based on an autonomous 3D Chua’s chaotic circuit, a modified fractional-order Chua’s circuit system is proposed. By numerical calculation, we obtain that the largest Lyapunov exponent of the modified fractional-order Chua’s circuit system is larger than zero for . This result indicates that the modified fractional-order Chua’s circuit system exhibits chaotic behavior if . For example, the largest Lyapunov exponent of the modified fractional-order Chua’s circuit system is 0.1329 for . The chaotic attractor for is given. By using Laplace transform, Gronwall’s Lemma, and Mittag-Leffler function in two parameters, we proposed two control strategies to stabilize the modified fractional-order Chua’s chaotic circuit. In our control scheme, a scalar controller determined by a single input and its Caputo derivative is used. The numerical simulations show the proposed control strategies are valid.

#### Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.