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Wavelet Adaptive Backstepping Control

for a Class of Nonlinear Systems

Chun-Fei Hsu, Member, IEEE, Chih-Min Lin, Senior Member, IEEE, and Tsu-Tian Lee, Fellow, IEEE

Abstract—This paper proposes a wavelet adaptive backstepping

control (WABC) system for a class of second-order nonlinear sys-tems. The WABC comprises a neural backstepping controller and a robust controller. The neural backstepping controller containing a wavelet neural network (WNN) identifier is the principal con-troller, and the robust controller is designed to achieveL2tracking performance with desired attenuation level. Since the WNN uses wavelet functions, its learning capability is superior to the con-ventional neural network for system identification. Moreover, the adaptation laws of the control system are derived in the sense of Lyapunov function and Barbalat’s lemma, thus the system can be guaranteed to be asymptotically stable. The proposed WABC is applied to two nonlinear systems, a chaotic system and a wing-rock motion system to illustrate its effectiveness. Simulation results verify that the proposed WABC can achieve favorable tracking per-formance by incorporating of WNN identification, adaptive back-stepping control, andL2robust control techniques.

Index Terms—Adaptive control, backstepping control, chaotic

system, robust control, wavelet neural network (WNN), wing-rock system.

I. INTRODUCTION

R

ECENTLY, the neural network-based control technique has represented an alternative method to solve control problems [1]–[6]. The most useful property of neural networks is their ability to approximate arbitrary linear or nonlinear mapping through learning. Based on their approximation ability, the neural networks have been used for approximation of control system dynamics or controllers. The basic issues in neural network feedback control are to provide online learning algorithms that do not require preliminary offline tuning. Some of these online learning algorithms are based on the backpropagation learning algorithm [2], and some are based on the Lyapunov stability theorem [1], [3]–[6]. Recently, some researchers have developed the structure of neural network based on the wavelet functions to construct the wavelet neural network (WNN) [7]–[10]. Unlike the sigmoidal functions used in conventional neural networks, wavelet functions are spatially localized, so that the learning capability of WNN is

Manuscript received June 28, 2004; revised February 14, 2005. This work was supported in part by the National Science Council of Republic of China under Grant NSC 92-2213-E-009-009.

C.-F. Hsu is with the Department of Electrical and Control Engineering, Na-tional Chiao-Tung University, Hsinchu 300, Taiwan, R.O.C. (e-mail: fei@cn. nctu.edu.tw).

C.-M. Lin is with the Department of Electrical Engineering, Yuan-Ze Univer-sity, Chung-Li 320, Taiwan, R.O.C. (e-mail: cml@saturn.yzu.edu.tw).

T.-T. Lee is with the Department of Electrical Engineering, National Taipei University of Technology, Taipei 106, Taiwan, R.O.C. (e-mail: ttlee@ntut.edu. tw).

Digital Object Identifier 10.1109/TNN.2006.878122

more efficient than the conventional sigmoidal function neural network for system identification. The training algorithms for WNN typically converge in a smaller number of iterations than for the conventional neural networks [7]. There has been considerable interest in exploring the applications of WNN to deal with nonlinearity and uncertainties of real-time servo control system [11]–[14]. These WNN controllers combine the capability of artificial neural networks for learning ability and the capability of wavelet decomposition for identification ability. Thus, the WNN-based control systems can achieve better control performance than NN-based control systems.

In the past decade, backstepping design procedures have been intensively introduced [15]–[18]. The backstepping control is a systematic and recursive design methodology for nonlinear sys-tems to offer a choice to accommodate the unmodeled nonlinear effects and parameter uncertainties. The essence of backstep-ping design is to select recursively some appropriate functions of state variables as pseudocontrol inputs for lower dimension subsystems of the overall system. Each backstepping stage re-sults in a new pseudocontrol design, expressed in terms of the pseudocontrol designs from preceding design stages. When the procedure is terminated, a feedback design for the true control input results, which achieves the original design objective by virtue of a final Lyapunov function, which is formed by sum-ming up the Lyapunov functions associated with each individual design stage [15].

Robust control techniques have been used as the system is subject to bounded external disturbances whose upper bound is unknown. Combing the robust control with adaptive fuzzy con-trol, some robust adaptive fuzzy control approaches have been proposed to attenuate the effects of approximation error to a pre-scribed level [19]–[21].

This paper proposes a wavelet adaptive backstepping control (WABC) system for a class of second-order nonlinear systems; this control system combines the advantages of WNN identi-fication, adaptive backstepping control, and robust control techniques. The proposed WABC is comprised of a neural back-stepping controller and a robust controller. The neural backstep-ping controller containing a WNN identifier is designed in the sense of the backstepping control technique, and the WNN iden-tifier is utilized to online estimate the system dynamic function. The robust controller is designed to achieve tracking per-formance by attenuating the effect of the approximation error caused by the WNN identifier. The adaptive laws of the WABC system are derived in the sense of Lyapunov function and Bar-balat’s lemma; thus the system can be guaranteed to be asymp-totically stable. Finally, a chaotic system and a wing-rock mo-tion system are provided as the simulamo-tion examples to verify

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that the proposed WABC scheme can achieve favorable tracking performance with regard to parameter variations and unknown dynamic function.

II. DESIGN OFIDEALBACKSTEPPINGCONTROLLER

Consider a class of second-order nonlinear systems

(1) where is the state trajectory of the system, which is assumed to be available for measurement, is a unknown real con-tinuous function, and is the input of the system. The control objective is to find a control law so that the state trajectory can track a trajectory command closely. Assuming that the pa-rameters of the system (1) are known, the design of ideal back-stepping controller is described step-by-step as follows.

Step 1) Define the tracking error

(2) and the derivative of tracking error is defined as

(3) The can be viewed as a virtual control in the equa-tion. Define the following stabilizing function

(4) where is a positive constant.

Step 2) Define

(5) then the derivative of is expressed as

(6) Step 3) If the system dynamic function is known, the ideal

backstepping controller can be obtained as

(7) where is a positive constant. Substitution of (7) into (1) yields

(8) Step 4) Define a Lyapunov function as

(9) Differentiating (9) with respect to time and using (3), (6), and (8), it is obtained that

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Fig. 1. Network structure of a WNN.

Since , that is , it implies that and are bounded. Now define the following term:

(11) then

(12) Because is bounded and is nonin-creasing and bounded, the following result can be obtained:

(13) Also is bounded, so by Barbalat’s Lemma [22], it can be shown that . This implies that and converge to zero as . Therefore, the ideal backstepping controller in (7) will asymptoti-cally stabilize the system.

III. DESIGN OF WAVELET ADAPTIVE

BACKSTEPPINGCONTROLLER

Since the system dynamic function may be unknown or perturbed in practical application, the ideal backstepping con-troller (7) cannot be precisely obtained. To solve this problem, a WNN identifier is utilized to approximate the system dynamic function. The descriptions of the WNN identifier and the design steps of the control system are described as follows.

A. WNN Identifier

The network structure of the WNN identifier is shown in Fig. 1, which can be considered as “1”-layer feedforward neural network with input preprocessing element. The WNN output with wavelet basis functions can perform the mapping ac-cording to [7]

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where is the input vector,

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functions, and are the dilation and translation parameters, respectively, is the output layer weight, and is the number of units (also called nodes and neurons) in the translation layer. Each wavelet network’s neuron in the translation layer can be represented by

(15)

where the “Mexican hat” mother wavelet function is defined as . For ease of notation, (14) can be expressed in a compact vector form as

(16)

where ,

, , and

. By the universal approximation theorem, there exists an ideal WNN identifier such that [7]

(17) where denotes the approximation error and is assumed to be bounded by , in which is a positive constant; and , , and are the optimal parameter vectors of , , and , respectively. In fact, the optimal parameter vectors that are needed to best approximate a given nonlinear function are difficult to determine. Thus, an estimate function is defined as

(18) where , , and are the estimation of , , and , respec-tively. For notational convenience, denote

and . Define the estimated error as

(19) where and . In the following, some tuning laws will be derived to online tune the parameters of the WNN identifier to achieve favorable estimation of the system dynamic function. To achieve this goal, the Taylor expansion linearization technique is employed to transform the nonlinear function into a partially linear form [5], i.e.,

..

. ... ... (20)

or

(21)

where ; ; is a vector of higher

order terms; ;

; and and are defined as

(22) (23)

Substitution of (21) into (19) yields

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where the uncertain term .

B. WABC System

The proposed WABC system is shown in Fig. 2, which is comprised of a neural backstepping controller and a robust controller . The tracking error is defined in (2), a stabi-lizing function in (4), and in (5). The control law of the WABC is developed as follows:

(25) The neural backstepping controller is chosen as

(26) where the WNN identifier is designed to online estimate the system dynamic function . Substitution of (25) and (26) into (1) yields

(27) By substituting (24) into (27), we obtain

(28) Then, Theorem 1 shows the properties of the proposed WABC control system.

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Fig. 2. WABC for nonlinear systems.

Theorem 1: Consider a nonlinear system represented by (1).

The control system is designed as (25) where the neural back-stepping controller is designed as (26), in which the adaptation laws of the WNN identifier are designed as

(29) (30) (31) where , , and are the learning rates with positive con-stants, and the robust controller is designed as

(32) where is a prescribed attenuation constant. Then, the overall control scheme guarantees the following properties:

1)

(33)

where .

2) If is squared integrable, that is , then .

Proof: Define a Lyapunov function as

(34)

Differentiating (34) with respect to time and using (2) and (28)–(32)

(35) Integrating (35) from to , yields

(36) Since , (36) implies the following:

(37) Using (34), (37) is equivalent to (33). Since is finite, if the approximation error , that is , using the Barbalat’s lemma [22], it implies that .

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Remark 1: The inequality (33) reveals that the integrated

squared error of is less than or equal to the sum of some initial squared errors, some parameter initial squared value and the in-tegrated squared error of . Since the initial squared errors and parameter initial squared value are finite, if is squared inte-grable then we can conclude that will approach to zero.

Remark 2: If the system starts with initial conditions

, , , , and , then the

performance in (33) can be rewritten as

(38) where the -gain from to the must be equal to or less than a level [19]–[21].

IV. SIMULATIONRESULTS

In this section, the proposed WABC technique is applied to control two nonlinear systems: a chaotic system (Example 1) and a wing-rock motion system (Example 2). It should be em-phasized that development of the WABC does not require the knowledge of the system dynamic function.

1) Example 1 (Chaotic System): Chaotic systems have been

known to exhibit complex dynamical behavior. Several control techniques have been proposed for the chaotic systems [23], ; however, some of them cannot achieve favorable control per-formance and some of them require system dynamic function. Consider a second-order chaotic system such as well known Duffing’s equation describing a special nonlinear circuit or a pendulum moving in a viscous medium under control [23]

(39) where , , , and are real constants; is the time variable;

is the frequency; is the

system dynamic function; and is the control effort. Depending on the choice of these constants, it is known that the solutions of system (39) may exhibit periodic, almost periodic, and chaotic behavior. For observing the chaotic unpredictable behavior, the open-loop system behavior with was simulated with

, , , and . The phase plane plots from an initial condition point (1,1) are shown in Fig. 3(a)–(c) for , , and , respectively. It is shown that the uncontrolled chaotic system has different trajectories for different values.

The system dynamic function would be online estimated by the WNN identifier. A WNN identifier with five hidden nodes is utilized to approach the system dynamic function of the chaotic system. In addition, the control parameters are selected as

, , and for .

These parameters are chosen through some trials to achieve fa-vorable transient control performance. The trajectory command is set as . The simulation results of the WABC for , , and are shown in Figs. 4–6, re-spectively. For the attenuation level , the tracking re-sponses of state are shown in Figs. 4(a)–6(a); the tracking responses of state are shown in Figs. 4(b)–6(b); and the as-sociated control efforts are shown in Figs. 4(c)–6(c), respec-tively. Moreover, to achieve smaller attenuation level, the case

Fig. 3. Phase plane of uncontrolled chaotic system.

for is reconsidered. In this case, the tracking responses of state are shown in Figs. 4(d)–6(d); the tracking responses of state are shown in Figs. 4(e)–6(e); and the associated control efforts are shown Figs. 4(f)–6(f), respectively. A performance index is defined as . The performance index is shown in Figs. 4(g)–6(g), respectively. It is shown that the proposed WABC can achieve favorable tracking performance; moreover, the better tracking performance can be achieved as specified attenuation level is chosen smaller.

2) Example 2 (Wing-Rock Motion System): Some combat

air-crafts often operate at subsonic speeds and high angles of attack. These aircrafts may become unstable due to oscillation, mainly a rolling motion known as wing-rock motion [24], [25]. A dy-namic system of the wing-rock motion system can be written in a state variable form as

(40) where is the roll angle and the parameters ,

are nonlinear functions of the angle of attack. The aerodynamic

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Fig. 4. Simulation results of chaotic system forq = 0:62.

, , , and

. The open-loop system time response with

Fig. 5. Simulation results of chaotic system forq = 1:95.

was simulated for two initial conditions: a small initial condition ( , s ) and a large initial condition ( ,

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Fig. 6. Simulation results of chaotic system forq = 7:00.

s ). The phase-plane plot is shown in Fig. 7. For the small initial condition, a limit cycle oscillation is obtained, and

Fig. 7. Phase-plane portrait of uncontrolled wing-rock motion system.

for the large initial condition, the roll angle is divergent. Thus, it is shown that the uncontrolled nonlinear wing-rock motion system will be unstable for some initial conditions.

The system dynamic function would be online estimated by the WNN identifier. A WNN identifier with five hidden nodes is utilized to approach the system dynamic function of the wing-rock motion system. In addition, the control parameters are

se-lected as , , and

for . These parameters are chosen through some trials to achieve favorable transient control performance. The simulation results of the WABC for small and large initial con-ditions are shown in Figs. 8 and 9, respectively. For the attenua-tion level , the tracking responses of state are shown in Figs. 8(a) and 9(a); and the associated control efforts are shown Figs. 8(b) and 9(b), respectively. Moreover, to achieve smaller attenuation level, the case for is reconsidered. In this case, the tracking responses of state are shown in Figs. 8(c) and 9(c); and the associated control efforts are shown Figs. 8(d) and 9(d), respectively. A performance index is defined as . The performance index is shown in Figs. 8(e) and 9(e), respectively. It is shown that the proposed WABC can achieve favorable tracking performance. Similar to the chaotic system (Example 1), the better tracking performance can be achieved as specified attenuation level is chosen smaller.

V. CONCLUSION

For some systems, since the dynamic characteristics of the control system are nonlinear and the precise models are diffi-cult to obtain, the model-based control approaches are diffidiffi-cult to be implemented. To overcome this drawback, a novel WABC system has been proposed. The developed WABC system is comprised of a neural backstepping controller and a robust con-troller. In the neural backstepping controller, a WNN identifier is utilized to online estimate the system dynamic function. The adaptive laws of the WABC system are synthesized using the Lyapunov function and Barbalat’s lemma so that the asymptotic stability of the control system can be guaranteed. The contri-butions of the proposed design method are the use of WNN to

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Fig. 8. Simulation results of wing-rock motion system for small initial condition.

achieve favorable identification performance, the use of adap-tive backstepping control to achieve favorable control perfor-mance, and the use of robust control to achieve tracking performance with desired attenuation level. Finally, a chaotic system and a wing-rock motion system are simulated to illus-trate the effectiveness of the proposed design method. Simula-tion results verified that the proposed WABC system can achieve favorable tracking performance of these nonlinear systems.

Fig. 9. Simulation results of wing-rock motion system for large initial condition.

ACKNOWLEDGMENT

The authors would like to thank the Associate Editor and re-viewers for their valuable comments.

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Chun-Fei Hsu (M’05) received the B.S., M.S., and

Ph.D. degrees in electrical engineering from Yuan-Ze University, Taiwan, Chung Li, R.O.C., in 1997, 1999, and 2002, respectively.

After graduation, he joined the Department of Electrical and Control Engineering, National Chiao-Tung University (NCTU), Hsinchu, Taiwan, R.O.C.. During 2002–2006, he was a postdoctoral student with Professor Tsu-Tian Lee in the area of a virtual-reality dynamic simulator and an intelligent transportation system. His research interests include servomotor drives, adaptive control, flight control, and intelligent control using fuzzy system and neural network technologies.

Chih-Min Lin (S’86–M’87–SM’99) received the B.S. and M.S. degrees in control engineering and the Ph.D. degree in electronics engineering from National Chiao Tung University (NCTU), Hsinchu, Taiwan, R.O.C., in 1981, 1983, and 1986, respectively.

During 1986–1992, he was with the Chung Shan Institute of Science and Technology, Lungt’an, Taoyuan County, Taiwan, R.O.C., as a Deputy Di-rector of System Engineering of a missile system. He also served concurrently as an Associate Professor at NCTU and Chung Yuan University, Chung Li, Taiwan, R.O.C. He joined the faculty of the Department of Electrical Engineering, Yuan-Ze University, Chung Li, Taiwan, R.O.C., in 1993, and is currently a Professor of Electrical Engineering. He also served as the Committee Member of Chinese Automatic Control Society and the Deputy Chairman of IEEE Control Systems Society, Taipei Section. During 1997–1998, he was the Honor Research Fellow in the University of Auckland, Auckland, New Zealand. His research interests include guidance and flight control, intelligent control, and systems engineering.

Tsu-Tian Lee (M’87–SM’89–F’97) was born in

Taipei, Taiwan, R.O.C., in 1949. He received the B.S. degree in control engineering from the National Chiao-Tung University (NCTU), Hsinchu, Taiwan, R.O.C., in 1970, and the M.S. and Ph.D. degrees in electrical engineering from the University of Oklahoma, Norman, in 1972 and 1975, respectively. In 1975, he was appointed Associate Professor and in 1978 Professor and Chairman of the Department of Control Engineering at NCTU. In 1981, he became a Professor and Director of the Institute of Control Engineering, NCTU. In 1986, he was a Visiting Professor and in 1987 a Full Professor of electrical engineering at the University of Kentucky, Lexington. In 1990, he was a Professor and Chairman of the Department of Electrical En-gineering, National Taiwan University of Science and Technology (NTUST), Taipei, Taiwan, R.O.C. In 1998, he became the Professor and Dean of the Of-fice of Research and Development, NTUST. Since 2000, he has been with the Department of Electrical and Control Engineering, NCTU, where he is now a Chair Professor. Since 2004, he has been with the National Taipei University of Technology (NTUT), Taipei, Taiwan, R.O.C., where he is now the President.

Prof. Lee received the Distinguished Research Award from the National Sci-ence Council, R.O.C., in 1991–1998, the Academic Achievement Award in En-gineering and Applied Science from the Ministry of Education, R.O.C., in 1997, the National Endow Chair from the Ministry of Education, R.O.C., in 2003, and the TECO Science and Technology Award from TECO Technology Foundation, in 2003. He was elected to the grade of IEE Fellow in 2000, respectively. He became a Fellow of New York Academy of Sciences (NYAS) in 2002. He has served as Member of Technical Program Committee and Member of Advisory Committee for many IEEE sponsored international conferences. He is now the Vice President of Membership, a member of the Board of Governors, and the Newsletter Editor for the IEEE Systems, Man, and Cybernetics Society.

數據

Fig. 1. Network structure of a WNN.
Fig. 2. WABC for nonlinear systems.
Fig. 3. Phase plane of uncontrolled chaotic system.
Fig. 5. Simulation results of chaotic system for q = 1:95.
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