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IEEE TRANSACTIONS ON NEURAL NETWORKS AND LEARNING SYSTEMS, VOL. 25, NO. 12, DECEMBER 2014 2129 Adaptive Neural Control for a Class of Nonlinear Time-Varying Delay Systems With Unknown Hysteresis Zhi Liu, Guanyu Lai, Yun Zhang, Xin Chen, and Chun Lung Philip Chen, Fellow, IEEE Abstract— This paper investigates the fusion of unknown direction hysteresis model with adaptive neural control tech- niques in face of time-delayed continuous time nonlinear systems without strict-feedback form. Compared with previous works on the hysteresis phenomenon, the direction of the modified Bouc–Wen hysteresis model investigated in the literature is unknown. To reduce the computation burden in adaptation mechanism, an optimized adaptation method is successfully applied to the control design. Based on the Lyapunov–Krasovskii method, two neural-network-based adaptive control algorithms are constructed to guarantee that all the system states and adaptive parameters remain bounded, and the tracking error converges to an adjustable neighborhood of the origin. In final, some numerical examples are provided to validate the effective- ness of the proposed control methods. Index Terms— Adaptive neural control, Bouc–Wen hysteresis, nonlinear control, nonstrict-feedback system, unknown direction hysteresis. I. I NTRODUCTION O VER THE past few decades, approximation-based adap- tive backstepping control for nonlinear systems has received a great deal of attention, and some significant results are presented in [1]–[20]. Among them, [1]–[7] are for strict-feedback systems in single-input and single-output form and [8]–[11] research the multiple-input and multiple-output (MIMO) nonlinear systems, while the nonlinear systems with immeasurable states or time delays are investigated in [4], Manuscript received May 14, 2013; accepted February 5, 2014. Date of publication February 25, 2014; date of current version November 17, 2014. This work was supported in part by the National Natural Science Foundation of China under Project 60974047 and Project U1134004, in part by the Natural Science Foundation of Guangdong Province under Grant S2012010008967, in part by the Science Fund for Distinguished Young Scholars under Grant S20120011437, in part by the 2011 Zhujiang New Star, in part by the Ministry of education of New Century Excellent Talent under Grant NCET- 12-0637, in part by the 973 Program of China under Grant 2011CB013104, in part by the Doctoral Fund of Ministry of Education of China under Grant 20124420130001, and in part by the University of Macau Multiyear Research Grants. Z. Liu, G. Lai, and Y. Zhang are with the Faculty of Automation, Guangdong University of Technology, Guangzhou 510006, China (e-mail: [email protected]; [email protected]; [email protected]). X. Chen is with the College of Mechanical and Electrical Engineering, Guangdong University of Technology, Guangdong 510006, China (e-mail: [email protected]). C. L. P. Chen is with the Faculty of Science and Technology, University of Macau, Macau 99999, China (e-mail: [email protected]). Color versions of one or more of the figures in this paper are available online at http://ieeexplore.ieee.org. Digital Object Identifier 10.1109/TNNLS.2014.2305717 [5], and [13]–[20]. In these control schemes, fuzzy logic systems (FLSs) or neural networks (NNs) are employed to approximate the unknown nonlinear functions. Based on the backstepping or dynamic surface control (DSC) technique, adaptive fuzzy controller or adaptive neural controller are con- structed to guarantee a good tracking performance. However, all the aforementioned control schemes are only suitable to the nonlinear systems in strict-feedback form, which is in fact a special case of the nonstrict-feedback form proposed in [21] recently. Different from the conventional strict-feedback systems, the semistrict-feedback systems, or the affine pure-feedback systems, the unknown nonlinear functions in the nonstrict- feedback system contain whole state variable, i.e., they cannot be directly compensated by the approximators with current states. In addition, the virtual control signals require to be the functions of current states to guarantee their existence. To deal with these difficulties, Chen et al. [21] have proposed a variable separation technique. Based on the Lyapunov syn- thesis and the FLSs technique, an adaptive control scheme was constructed in [21] to guarantee the stability of nonstrict- feedback control system. Although much progress has been made in adaptive control field in [1]–[19] and [21], some challenging problems still remain. In practical application, the actuator of control system is often subjected to the nonsmooth characteristics, such as the hysteresis nonlinearity in [29], [30], [34]–[39], [41], [45], [57], and [74], the saturation nonlinearity in [22]–[28], [31], and [33], the dead-zone nonlinearity in [20], [43], and [44], and the backlash nonlinearity in [40]. Especially, the hysteresis phenomenon in the physical systems and devices severely limits the tracking performance and easily causes the instability [57]. Therefore, control of nonlinear systems preceded by the nonsmooth hysteresis characteristic has become one of the active topics. To address the control problem of nonsmooth hysteresis nonlinearity in the actuator, the authors in [30], [34]–[39], [41], [45], [57], and [74] have made outstanding contributions in the fusion of hysteresis models with available robust control techniques. These hysteresis models can be classified into four classes, which are the backlash-like hysteresis model in [30], [34], [45], and [74], the conventional Prandtl–Ishlinskii (P–I) hysteresis model in [35] and [36], the generalized P–I hysteresis model in [37] and [42], and the modified Bouc–Wen hysteresis model in [41], respectively. In [34], the backlash- like hysteresis model was first proposed to describe a class of 2162-237X © 2014 IEEE. Personal use is permitted, but republication/redistribution requires IEEE permission. See http://www.ieee.org/publications_standards/publications/rights/index.html for more information.

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Page 1: cdn.persiangig.comcdn.persiangig.com/dl/h7cWv/O4OU58tYBO/Adaptive...LIU et al.: ADAPTIVE NEURAL CONTROL FOR A CLASS OF NONLINEAR TIME-VARYING DELAY SYSTEMS 2139 [6] Y. S. Yang and

IEEE TRANSACTIONS ON NEURAL NETWORKS AND LEARNING SYSTEMS, VOL. 25, NO. 12, DECEMBER 2014 2129

Adaptive Neural Control for a Class of NonlinearTime-Varying Delay Systems With

Unknown HysteresisZhi Liu, Guanyu Lai, Yun Zhang, Xin Chen, and Chun Lung Philip Chen, Fellow, IEEE

Abstract— This paper investigates the fusion of unknowndirection hysteresis model with adaptive neural control tech-niques in face of time-delayed continuous time nonlinear systemswithout strict-feedback form. Compared with previous workson the hysteresis phenomenon, the direction of the modifiedBouc–Wen hysteresis model investigated in the literature isunknown. To reduce the computation burden in adaptationmechanism, an optimized adaptation method is successfullyapplied to the control design. Based on the Lyapunov–Krasovskiimethod, two neural-network-based adaptive control algorithmsare constructed to guarantee that all the system states andadaptive parameters remain bounded, and the tracking errorconverges to an adjustable neighborhood of the origin. In final,some numerical examples are provided to validate the effective-ness of the proposed control methods.

Index Terms— Adaptive neural control, Bouc–Wen hysteresis,nonlinear control, nonstrict-feedback system, unknown directionhysteresis.

I. INTRODUCTION

OVER THE past few decades, approximation-based adap-tive backstepping control for nonlinear systems has

received a great deal of attention, and some significant resultsare presented in [1]–[20]. Among them, [1]–[7] are forstrict-feedback systems in single-input and single-output formand [8]–[11] research the multiple-input and multiple-output(MIMO) nonlinear systems, while the nonlinear systems withimmeasurable states or time delays are investigated in [4],

Manuscript received May 14, 2013; accepted February 5, 2014. Date ofpublication February 25, 2014; date of current version November 17, 2014.This work was supported in part by the National Natural Science Foundationof China under Project 60974047 and Project U1134004, in part by the NaturalScience Foundation of Guangdong Province under Grant S2012010008967,in part by the Science Fund for Distinguished Young Scholars under GrantS20120011437, in part by the 2011 Zhujiang New Star, in part by theMinistry of education of New Century Excellent Talent under Grant NCET-12-0637, in part by the 973 Program of China under Grant 2011CB013104,in part by the Doctoral Fund of Ministry of Education of China under Grant20124420130001, and in part by the University of Macau Multiyear ResearchGrants.

Z. Liu, G. Lai, and Y. Zhang are with the Faculty of Automation,Guangdong University of Technology, Guangzhou 510006, China (e-mail:[email protected]; [email protected]; [email protected]).

X. Chen is with the College of Mechanical and Electrical Engineering,Guangdong University of Technology, Guangdong 510006, China (e-mail:[email protected]).

C. L. P. Chen is with the Faculty of Science and Technology, University ofMacau, Macau 99999, China (e-mail: [email protected]).

Color versions of one or more of the figures in this paper are availableonline at http://ieeexplore.ieee.org.

Digital Object Identifier 10.1109/TNNLS.2014.2305717

[5], and [13]–[20]. In these control schemes, fuzzy logicsystems (FLSs) or neural networks (NNs) are employed toapproximate the unknown nonlinear functions. Based on thebackstepping or dynamic surface control (DSC) technique,adaptive fuzzy controller or adaptive neural controller are con-structed to guarantee a good tracking performance. However,all the aforementioned control schemes are only suitable tothe nonlinear systems in strict-feedback form, which is in facta special case of the nonstrict-feedback form proposed in [21]recently.

Different from the conventional strict-feedback systems,the semistrict-feedback systems, or the affine pure-feedbacksystems, the unknown nonlinear functions in the nonstrict-feedback system contain whole state variable, i.e., they cannotbe directly compensated by the approximators with currentstates. In addition, the virtual control signals require to bethe functions of current states to guarantee their existence.To deal with these difficulties, Chen et al. [21] have proposeda variable separation technique. Based on the Lyapunov syn-thesis and the FLSs technique, an adaptive control schemewas constructed in [21] to guarantee the stability of nonstrict-feedback control system. Although much progress has beenmade in adaptive control field in [1]–[19] and [21], somechallenging problems still remain. In practical application, theactuator of control system is often subjected to the nonsmoothcharacteristics, such as the hysteresis nonlinearity in [29], [30],[34]–[39], [41], [45], [57], and [74], the saturation nonlinearityin [22]–[28], [31], and [33], the dead-zone nonlinearity in[20], [43], and [44], and the backlash nonlinearity in [40].Especially, the hysteresis phenomenon in the physical systemsand devices severely limits the tracking performance and easilycauses the instability [57]. Therefore, control of nonlinearsystems preceded by the nonsmooth hysteresis characteristichas become one of the active topics.

To address the control problem of nonsmooth hysteresisnonlinearity in the actuator, the authors in [30], [34]–[39],[41], [45], [57], and [74] have made outstanding contributionsin the fusion of hysteresis models with available robust controltechniques. These hysteresis models can be classified intofour classes, which are the backlash-like hysteresis model in[30], [34], [45], and [74], the conventional Prandtl–Ishlinskii(P–I) hysteresis model in [35] and [36], the generalized P–Ihysteresis model in [37] and [42], and the modified Bouc–Wenhysteresis model in [41], respectively. In [34], the backlash-like hysteresis model was first proposed to describe a class of

2162-237X © 2014 IEEE. Personal use is permitted, but republication/redistribution requires IEEE permission.See http://www.ieee.org/publications_standards/publications/rights/index.html for more information.

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2130 IEEE TRANSACTIONS ON NEURAL NETWORKS AND LEARNING SYSTEMS, VOL. 25, NO. 12, DECEMBER 2014

special hysteresis phenomenon in the actuator. By treating theeffect of backlash-like hysteresis as a bounded disturbance,the proposed model can be conveniently fused with availablerobust control techniques. Furthermore, Su et al. [35] havefused a more general conventional P–I hysteresis model withadaptive variable structure control approach. Based on theP–I model, an adaptive control algorithm was proposed in[35] to guarantee a good tracking performance. To enlargethe class of applicable systems, Ren et al. [36] considereda class of MIMO nonlinear systems with the conventionalP–I hysteresis input and time-varying delays. By using theNNs technique to approximate the unknown nonlinear func-tions, the restriction of the linearly parameterized unknownuncertainties can be removed. The effect of time-varyingdelays can be canceled by designing an appropriate Lyapunov–Krasovskii function. Therefore, an approximation-based adap-tive control scheme was developed in [36] to guarantee thesemiglobally uniformly ultimately bounded of control system.To accommodate more general classes of hysteresis shapes, ageneralized P–I hysteresis model was proposed in [42]. Forthe conventional P–I hysteresis model, the different hysteresisshapes are described by adjusting the density function only.For the generalized case, both the density function and theinput function can be utilized to formulate the different hys-teresis shapes, i.e., compared with the conventional case, thegeneralized P–I hysteresis model can capture the hysteresisphenomenon more accurately. Ren et al. [37] considered aclass of nonaffine pure-feedback nonlinear systems with thegeneralized P–I hysteresis input. To deal with the nonaffineproblem in the presence of nonsmooth characteristic of hys-teresis, the mean-value theorem was introduced. By using thebackstepping and NNs techniques, the control approach in [37]can guarantee the uniformly ultimately bounded of control sys-tem, and the tracking error converges to a small neighborhoodof the origin. To relax the restrictions about the density func-tion in P–I hysteresis model, a modified Bouc–Wen hysteresismodel was first proposed in [41]. By constructing a perfectinverse to compensate the effect of hysteresis nonlinearity, anadaptive control approach was provided in [41] to guaranteea good tracking performance. However, the directions of theaforementioned four classes of hysteresis models require tobe known. If the direction of hysteresis phenomenon in theactuator is unknown, the control approaches mentioned abovecannot be directly applied.

Motivated by the aforementioned researches, this paperfocuses on the problem of adaptive neural control for aclass of continuous time (CT) nonstrict-feedback systems withunknown direction modified Bouc–Wen hysteresis input andtime-varying delays. The main contributions in this literaturecan be summarized as follows.

1) The hysteresis models studied in [29], [30], [34]–[39],[41], [45], [57], and [74] are known direction hystere-sis, i.e., though the hysteresis parameter (it refers tothe coefficient or the function governing the hysteresisdirection) may be unknown, its sign must be known asprior knowledge. If the hysteresis direction is unknown,the aforementioned control schemes cannot be directlyapplied. In this paper, we investigate the fusion of

the unknown direction hysteresis with adaptive neuralcontrol approaches.

2) Compared with the unknown nonlinear functions ofcurrent states in conventional strict-feedback systems,the unknown functions in the nonstrict-feedback systemcontain whole state variables, i.e., more NN nodesshould be utilized to obtain a good approximated per-formance. If we still employ the conventional adaptationmechanism, it will lead to unacceptable large learningtime as the number of NN nodes increases. To solvethese difficulties in face of the control system withoutstrict-feedback form, an optimized method is included inthe adaptation mechanism in this literature. By employ-ing the optimized adaptation method, the number ofadaptive parameters does not increase as the NN nodesincrease, and the less knowledge about the centers andwidths of basis functions are needed for the controllerdesign.

3) Compared with the nonlinear systems in Brunovskyform or nonaffine pure-feedback form studied in[34]–[41], the control system investigated in this paperis the CT nonstrict-feedback form, which is in fact amore general case [21]. Therefore, the investigation inthis paper enlarges the class of applicable systems withhysteresis phenomenon.

II. PROBLEM FORMULATION AND SOME PRELIMINARIES

A. Nonlinear Control Problem

Consider the following nonstrict-feedback system withunknown hysteresis input and time-varying delays:

x = Ax + f (x) + h(x(τ (t))) + Bu + �(t, x)

u = H (v), y = CT x (1)

where

A =[

0 In−10 0

], B = [0, . . . , 0, 1]T ∈ Rn

C = [1, 0, . . . , 0]T ∈ Rn

f (x) = [. . . , fi (x), . . . , fn(x)]T , i = 1, . . . , n − 1

h(x(τ (t))) = [. . . , hi (x(t − τi (t))), . . . , hn(x(t − τn(t)))]T

�(t, x) = [. . . , ωi (t, x), . . . , ωn(t, x)]T (2)

where x = [x1, x2, . . . , xn]T ∈ Rn are the whole statevariables of control system. f (x) ∈ Rn , v ∈ R, and y(t) ∈ Rdenote the unknown smooth function of whole states, systeminput, and system output, respectively. �(t, x) ∈ Rn are theexternal disturbances and h(x(τ (t))) ∈ Rn are the unknownsmooth functions of time-varying time-delayed states. In−1 isan identity matrix. Here, the control signal is subjected to theunknown hysteresis nonlinearity H (v) : R → R given in thelater.

Remark 1: Different from the conventional strict-feedbacknonlinear systems, the unknown functions fi (x), hi (x), andωi (t, x) in the differentiation (1) are evidently the functions ofwhole state variables. Hence, these terms cannot be dealt withas done in most of the previous works, where they are approx-imated by the NNs of current states. To solve the difficulty,

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LIU et al.: ADAPTIVE NEURAL CONTROL FOR A CLASS OF NONLINEAR TIME-VARYING DELAY SYSTEMS 2131

Chen et al. [21] have proposed a variable separation technique.However, the fusion of unknown direction hysteresis withthese adaptive control techniques is still a challenging prob-lem, which directly motivates the investigation of this paper.

Remark 2: The hysteresis phenomenon has been inves-tigated in many previous works, such as the backlash-likehysteresis model in [30], [34], [45], and [74], the conven-tional P–I hysteresis model in [35] and [36], the generalizedP–I hysteresis model in [37] and [42], and the modifiedBouc–Wen hysteresis model in [41]. However, the directionsof these hysteresis models require to be known. If the practicalhysteresis direction is unknown, the aforementioned controlschemes cannot be directly applied. To the best of our knowl-edge, it is the first time, in the literature, that the fusionof unknown direction hysteresis with adaptive neural controltechniques is investigated.

The objective of this paper is to design a robust adaptiveneural controller for system (1) to guarantee two points.

1) All the system states and the adaptive parameters arebounded.

2) The tracking error z1(t) = y(t) − yr (t) converges toan adjustable neighborhood of the origin, where y(t) isthe output of control system and yr (t) is the referencesignal. Specifically, for any ε > 0, there exists a timevalue T (ε) > 0 such that z2

1(t) ≤ ε,∀t > T .

Assumption 1: For 1 ≤ i ≤ n, there exists an unknownpositive function �i (x) such that

|ωi (t, x)| ≤ �i (x). (3)

Remark 3: Similar external disturbances �i (t, x) wereconsidered in [69], where they should satisfy the restriction|wi (t, x)| ≤ �i (xi ), xi = [x1, . . . , xi ]T ∈ Ri . From thispoint of view, Assumption 1 is in fact a relaxed version of therestriction in [69]. Therefore, the external disturbances studiedin this paper are more general.

Assumption 2: For 1 ≤ i ≤ n, consider τi (t) is thetime-varying time delay. It requires to satisfy the followinginequalities:

0 < τi (t) ≤ τmax τi ≤ τmax < 1 (4)

where τmax and τmax are known constants.

B. Hysteresis Nonlinearity

A modified Bouc–Wen hysteresis nonlinearity can be for-mulated as follows [41]:

H (v) = μ1v + μ2ζ (5)

where μ1 and μ2 are the constants with the same signs, i.e.,sign(μ1) = sign(μ2). ζ can be specified as

ζ = v − β|v||ζ |n−1ζ − χv|ζ |n = v f (ζ, v), ζ(t0) = 0 (6)

where β > |χ |, n > 1. The shape and amplitude of thehysteresis can be described by the parameters β while thesmoothness from initial slope to asymptote’s slope can bedescribed by the parameter n. The auxiliary variable ζ is

TABLE I

SIMULATION PARAMETERS

Fig. 1. Trajectories of positive direction hysteresis and negative directionhysteresis.

bounded by the constant ζ , i.e., |ζ | ≤ ζ = n√

1/(β + χ). Thefunction f (ζ, v) can be formulated as follows:

f (ζ, v) = 1 − sign(v)β|ζ |n−1ζ − χ |ζ |n. (7)

Remark 4: It should be noted that the sign of μ1 governs thedirection of hysteresis. The issue can be clearly illustrated bythe following numerical example. The simulation parametersare given in Table I. By selecting the input signal v(t) ofhysteresis actuator as v(t) = sin(2t), the graphical result isshown in Fig. 1.

C. Neural Networks

In most of the robust adaptive neural control schemes, theradial basis function neural networks (RBFNNs) are utilizedto deal with unknown nonlinear terms as the approximationproperty. The RBFNNs have the form θT S(Z), where θ =[θ1, . . . , θN ]T ∈ RN is the weight vector with the integer N ,S(Z) = [S1(Z), . . . , SN (Z)]T ∈ RN is the vector of knownbasis function, and Z = [Z1, . . . , Zq ]T ∈ Rq is the inputvector of approximator, see in Fig. 2. Noting that the GaussianRBFNNs have the basis function Si (Z), which uses thestructure of Gaussian function and it can be formulated asfollows:

Si (Z) = exp−(Z − μi )

T (Z − μi )

η2i

, i = 1, 2, . . . , N (8)

where μi = [μi1, . . . , μiq ]T is the center of the receptive fieldand ηi is the width of the Gaussian function. It was proved thatRBFNNs can approximate any nonlinear continuous function

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2132 IEEE TRANSACTIONS ON NEURAL NETWORKS AND LEARNING SYSTEMS, VOL. 25, NO. 12, DECEMBER 2014

Fig. 2. Structure of RBFNN.

f j (Z)( j = 1, . . . , n) over a compact set Z ∈ � with anyaccuracy. Therefore, the following lemma holds.

Lemma 1: For any ε > 0, there exists an NN θT S(Z) suchthat

supZ∈�

| f j (Z) − θT S(Z)| ≤ ε (9)

where � is a compact set of Z . The universal approximationproperty can be well utilized to deal with the unknownnonlinear terms.

D. Nussbaum Function

A function N(ϑ) is the Nussbaum function if it satisfies

limk→±∞ sup

1

k

∫ k

0N(s)ds = ∞ (10)

limk→±∞ inf

1

k

∫ k

0N(s)ds = −∞. (11)

Thus, we know that many functions satisfy the aforemen-tioned conditions such as exp(ϑ2) cos ϑ , ϑ2 cos ϑ .

Lemma 2: Let V (·) and ϑ(·) be smooth functions defined on[t0, t f ) with V (t) ≥ 0,∀t ∈ [t0, t f ), N(·) is an even smoothNussbaum-type function. If the following inequality holds for∀t ∈ [t0, t f ):

V (t) ≤ h1 +∫ t

t0(ξ(t)N(ϑ) + 1)ϑe−h2(t−τ )dτ (12)

where h1 and h2 are positive scalars. ξ(t) is a boundedfunction, which takes values at the interval � : [l−, l+]and 0 /∈ �. A conclusion can be made that V (t), ϑ(t),∫ t

t0(ξ N(ϑ)+1)ϑdτ must be bounded on [t0, t f ). Furthermore,

t f can be extended to infinity, i.e., t f → ∞ if the solution ofthe resulting closed-loop system is bounded [20].

III. ADAPTIVE NEURAL CONTROL DESIGN

BASED ON LYAPUNOV SYNTHESIS

We use the backstepping and NN techniques to constructthe adaptive neural control schemes. The coordinate transfor-mations are defined as follows:

z1=y − yr (13)

zi=xi − αi−1 2 ≤ i ≤ n (14)

where yr is the reference signal and assuming its time deriv-atives up to nth order remain bounded and continuous.

Assumption 3: For 1 ≤ i ≤ n, there exists an unknownpositive function qi j such that

|hi (x(t))| ≤n∑

j=1

|z j (t)|qi j (x(t)) (15)

where x(t) = [x1(t), . . . , xn(t)]T are the whole state variablesof control system. z j is the coordinate transformation, i.e.,z1 = y − yr and z j = x j − α j−1(2 ≤ j ≤ n), where α j−1 isthe virtual controller given latter.

Remark 5: A similar assumption was made in [64]. How-ever, the time-delayed term hi (·) studied in [64] is a functionof current states, i.e., hi (·) = hi (xi ), where xi = [x1, . . . , xi ]T .In this paper, we extend the time-delayed term to hi (x),which contains the whole state variables. Therefore, the controlscheme proposed in this paper can be applied more extensively.

At each step of control design, we utilize the

Wi = Ni ||θi ||22 = NiθTi θi , i = 1, . . . , n

where θi = [θi,1, . . . , θi,Ni ]T and Ni are the weight vector andthe number of neurons in i th hidden layer, respectively. Theoperator ||·||2 represents the Euclidean norm of column vector.From the definition, we know that Wi is an unknown constant.The adaptive parameter Wi is utilized to estimate Wi and theestimated error is Wi = Wi − Wi . By directly estimating thenorm of weight vector θi , there are only n adaptive parametersneeded to adjust online. Compared with the control algorithmsproposed in [36] and [37], the computation in adaptationmechanism utilized in the literature can be reduced from∑n

i=1 Ni to n.In the following analysis, two control schemes are proposed

in the Section III-A and III-B, respectively. The control schemein Section III-A is for the nonlinear systems with knowndirection hysteresis, i.e., hysteresis parameter μ1 is unknownbut its sign requires to be known as prior knowledge. InSection III-B, we propose an adaptive neural control algorithmfor the nonlinear systems with unknown direction hysteresis.

A. Known Direction Hysteresis

To facilitate the control design, the following assumption isneeded.

Assumption 4: Consider the direction of unknown hysteresisis known, i.e., μ1 is an unknown parameter but its sign mustbe known. Without loss of generality, it is further assumedsign(μ1) > 0.

Theorem 1: Consider the nonstrict-feedback nonlinear sys-tem in (1), under the Assumptions 1–4, by selecting the virtualcontrollers α j , the auxiliary controller v and the actual controlsignal v as follows:

⎧⎪⎪⎨⎪⎪⎩

α j = −(k j + n2

4 j + 0.5)z j − 1

2a2jz j W j − z j−1

v = −(kn + n2

4n + 1)zn − 1

2a2n

znWn − zn−1

v = ev

(16)

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LIU et al.: ADAPTIVE NEURAL CONTROL FOR A CLASS OF NONLINEAR TIME-VARYING DELAY SYSTEMS 2133

where j = 1, . . . , n−1 and z0 = −yr . Define a parameter e ase = 1/μ1, and its estimated value is e = 1/μ1. The estimatederror is defined as e = e− e. The adaptive laws are selected as⎧⎨

⎩˙Wi = ri

2a2i

z2i − k0i Wi (i = 1, . . . , n)

˙e = −ηzn v − η0e.(17)

We can construct a robust adaptive neural control scheme toguarantee that all the system states and adaptive parameters arebounded. By increasing the designed parameters k1, . . . , kn ,k01, . . . , k0n, η, η0, r1, . . . , rn while reducing a1, . . . , an , thetracking error limitation can be adjusted arbitrarily small.

Proof: Backstepping technique is employed to demon-strate this theorem.

Step 1: Differentiating two sides of (13), we have

z1 = f1(x) + h1(x(t − τ1)) + x2 + ω1(t, x) − yr . (18)

The Lyapunov–Krasovskii function can be chosen asfollows:

V1=n∑

i=1

n∑j=1

1

1 − τmaxe−λ(t−τi )

∫ t

t−τi

eλsz2j (s)q

2i j (x(s))ds

+1

2z2

1 + 1

2r1W 2

1 . (19)

Differentiating V1 in (19) yields

V1 = z1( f1(x) + h1(x(t−τ1)) + x2 + ω1(t, x)− yr)

− 1

r1W1

˙W1 + 1

1−τmax

n∑i=1

n∑j=1

eλτi z2j (t)q

2i j (x(t))

− (1−τi)

1−τmax

n∑i=1

n∑j=1

z2j (t−τi )q

2i j (x(t−τi ))

−n∑

i=1

n∑j=1

·λ(1−τi)

1−τmaxe−λ(t−τi )

∫ t

t−τi

eλsz2j (s)q

2i j (x(s))ds.

(20)

Invoking Assumption 2, one has

−λ(1 − τi ) ≤ −λ(1 − τmax). (21)

By rearranging the terms

n∑i=1

n∑j=1

eλτi z2j (t)q

2i j (x(t)) =

n∑j=1

n∑i=1

eλτi z2j (t)q

2i j (x(t))

and combining with (20) and (21), we have

V1 ≤ z1( f1(x) + h1(x(t − τ1)) + z2 + α1 + ω1(t, x) − yr )

− 1

r1W1

˙W1 + 1

1 − τmax

n∑j=1

n∑i=1

eλτi z2j (t)q

2i j (x(t))

−n∑

i=1

n∑j=1

z2j (t − τi )q

2i j (x(t − τi )) − λ(1 − τmax)

×n∑

i=1

n∑j=1

e−λ(t−τi )

1 − τmax

∫ t

t−τi

eλsz2j (s)q

2i j (x(s))ds. (22)

Noting that

z1h1(x(t − τ1)) ≤ |z1|n∑

j=1

|z j (t − τ1)|q1 j (x(t − τ1))

≤ n2

4z2

1 + 1

n

n∑j=1

z2j (t − τ1)q

21 j (x(t − τ1)).

(23)

Similarly

z1ω1(t, x) ≤ 1

2|z1| + 1

2|z1|� 2

1 (x). (24)

We define the nonlinear term σ1 as follows:

σ1 =| f1(x)| + 1

2+ 1

2� 2

1 (x) +

n∑i=1

|z1|eλτmaxq2i1(x(t))

1 − τmax. (25)

With the conclusion of (9), we use the RBFNN θT1 S1 to

approximate the nonlinear term σ1 and the approximated erroris δ1 which satisfies |δ1| ≤ ε1. Combining with the conditionST

1 S1 ≤ N1, we have

|z1|σ1 =|z1|(θT

1 S1 + δ1)

≤ 1

2a21

z21||θ1||2ST

1 S1 + 1

2a2

1 + 1

2z2

1 + 1

2ε2

1

≤ 1

2a21

z21W1 + 1

2a2

1 + 1

2z2

1 + 1

2ε2

1. (26)

Substituting (23)–(26) into (22), we have

V1 ≤− k1z21 + z1z2 + 1

2a2

1 + 1

2ε2

1 + W1

r1

(r1

2a21

z21 − ˙W1

)

+ 1

1 − τmax

n∑j=2

n∑i=1

eλτi z2j (t)q

2i j (x(t)) − n − 1

n

×n∑

j=1

z2j (t − τ1)q

21 j (x(t − τ1)) − λ(1 − τmax)

×n∑

i=1

n∑j=1

e−λ(t−τi )

1 − τmax

∫ t

t−τi

eλsz2j (s)q

2i j (x(s))ds

−n∑

i=2

n∑j=1

z2j (t − τi )q

2i j (x(t − τi )). (27)

Step k(2 ≤ k ≤ n − 1): Differentiating two sides of (14)yields

zk= fk(x) + hk(x(t − τk)) + xk+1 + ωk(t, x) − αk−1. (28)

The Lyapunov–Krasovskii function is chosen as

Vk = Vk−1 + 1

2z2

k + 1

2rkW 2

k . (29)

Differentiating Vk in (29), we have

Vk = Vk−1 + zk( fk(x) + hk(x(t − τk)) + xk+1

+ ωk(t, x) − αk−1) − 1

rkWk

˙Wk

= Vk−1 + zk( fk(x) + hk(x(t − τk)) + zk+1 + αk

+ ωk(t, x) − αk−1) − 1

rkWk

˙Wk . (30)

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2134 IEEE TRANSACTIONS ON NEURAL NETWORKS AND LEARNING SYSTEMS, VOL. 25, NO. 12, DECEMBER 2014

Since

zkhk(x(t − τk)) ≤ |zk |n∑

j=1

|z j (t − τk)|qkj (x(t − τk))

≤ n2

4 · kz2

k + k

n

n∑j=1

z2j (t − τk)q

2kj (x(t − τk)).

(31)

Similarly

zkωk(t, x) ≤ 1

2|zk | + 1

2|zk |� 2

k (x). (32)

The time differentiation of the virtual control signalαk−1 is

αk−1 =k−1∑m=1

∂αk−1

∂xm( fm(x) + hm(x(t − τm)) + xm+1

+ ωm(t, x)) +k−1∑m=1

∂αk−1

Wm

˙Wm +k−1∑m=0

∂αk−1

∂y(m)r

y(m+1)r .

(33)

By analyzing some complex terms in the αk−1, we have

− zk

k−1∑m=1

∂αk−1

∂xmhm(x(t−τm))

≤ |zk |k−1∑m=1

∣∣∣∣∂αk−1

∂xm

∣∣∣∣n∑

j=1

|z j (t−τm)|qmj (x(t−τm))

≤k−1∑m=1

⎡⎣n2

4z2

k

(∂αk−1

∂xm

)2

+ 1

n

n∑j=1

z2j (t−τm)q2

mj (x(t−τm))

⎤⎦

≤k−1∑m=1

n2

4z2

k

(∂αk−1

∂xm

)2

+ 1

n

k−1∑l=1

n∑j=1

z2j (t−τl)q

2l j (x(t−τl)).

(34)

Noting that

−zk

k−1∑m=1

∂αk−1

∂xmωm(t, x)≤

k−1∑m=1

[|zk|2

(∂αk−1

∂xm

)2

+ |zk |2

� 2m(x)

].

(35)

We define σk as follows:

σk = | fk(x)| + 1

2+

k∑m=1

1

2� 2

m(x) +k−1∑m=1

∣∣∣∣∂αk−1

∂xm

∣∣∣∣ | fm(x)|

+k−1∑m=1

(n2

4|zk | + 1

2

) (∂αk−1

∂xm

)2

+k−1∑m=1

∣∣∣∣∂αk−1

∂xm

∣∣∣∣ |xm+1|

+k−1∑m=1

∂αk−1

Wm

˙Wm +k−1∑m=0

∂αk−1

∂y(m)r

y(m+1)r

+ 1

1 − τmax

n∑i=1

eλτmax |zk |q2ik(x(t)). (36)

We employ the RBFNN to approximate the nonlinear termσk , the approximated error is δk which satisfies |δk | ≤ εk .Combining with the condition ST

k Sk ≤ Nk , we have

|zk |σk = |zk |(θT

k Sk + δk) ≤ 1

2a2k

z2k Wk + 1

2a2

k + 1

2z2

k + 1

2ε2

k .

(37)

Substituting (31)–(37) into (30), we have

Vk ≤ −k∑

j=1

k j z2j + zkzk+1 + 1

2

k∑j=1

(a2

j + ε2j

)

+k∑

j=1

W j

r j

(r j

2a2j

z2j − ˙W j

)+

n∑j=k+1

n∑i=1

eλτi z2j (t)q

2i j (x(t))

1 − τmax

−n∑

i=k+1

n∑j=1

z2j (t − τi )q

2i j (x(t − τi )) − n − k

n

·k∑

l=1

n∑j=1

z2j (t − τl)q

2l j (x(t − τl)) − λ(1 − τmax)

·n∑

i=1

n∑j=1

e−λ(t−τi )

1 − τmax

∫ t

t−τi

eλsz2j (s)q

2i j (x(s))ds. (38)

Step n: The Lyapunov–Krasovskii function can be chosenas follows:

Vn = Vn−1 + 1

2z2

n + 1

2rnW 2

n + μ1

2ηe2. (39)

Differentiating two sides of (39), we have

Vn = Vn−1 + zn( fn(x) + hn(x(t − τn)) + H (v)

+ ωn(t, x) − αn−1) − 1

rnWn

˙Wn − μ1

ηe ˙e.

(40)

Since

znhn(x(t − τn)) ≤ n2

4 · nz2

n + n

n

n∑j=1

z2j (t − τk)q

2kj (x(t − τk)).

(41)

Noting that

znωn(t, x) ≤ 1

2|zn| + 1

2|zn |� 2

n (x). (42)

The time differentiation of the virtual controller αn−1 is

αn−1 =n−1∑m=1

∂αn−1

∂xm( fm(x) + hm(x(t − τm)) + xm+1

+ ωm(t, x)) +n−1∑m=1

∂αn−1

Wm

˙Wm +n−1∑m=0

∂αn−1

∂y(m)r

y(m+1)r .

(43)

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LIU et al.: ADAPTIVE NEURAL CONTROL FOR A CLASS OF NONLINEAR TIME-VARYING DELAY SYSTEMS 2135

Noting that

−zn

n−1∑m=1

∂αk−1

∂xmhm(x(t−τm))

≤n−1∑m=1

n2

4z2

k

(∂αk−1

∂xm

)2

+ 1

n

n−1∑l=1

n∑j=1

z2j (t−τl)q

2l j (x(t−τl)).

(44)

Subsequently, a compounded nonlinear term σn similar toσk in the equality (36) is also defined. By using the RBFNNto approximate the unknown nonlinear term σn , and theapproximated error is δn satisfying |δn| ≤ εn . Thus, we have

|zn |σn = |zn|(θT

n Sn + δn)

≤ 1

2a2n

z2n Wn + 1

2a2

n + 1

2z2

n + 1

2ε2

n. (45)

The hysteresis input H (v) in (40) can be dealt with asfollows:

zn H (v) = zn(μ1v + μ2ζ ). (46)

Consider μ1 is the unknown constant, we should utilize μ1to estimate μ1. By defining e = 1/μ1 and e = 1/μ1, thus, theestimated error is e = e − e. Combining with Assumption 4yields

zn H (v)= zn(μ1v + μ2ζ ) = znμ1ev + znμ2ζ

= znμ1

(1

μ1− 1

μ1

)v + znμ2ζ

= zn v − znμ1ev + znμ2ζ. (47)

Since

znμ2ζ ≤ 1

2z2

n + 1

2(μ2ζ )2 (48)

where ζ = n√

1/(β + χ).From (16), the auxiliary control signal v is designed as

v = −(

kn + n2

4 · n+ 0.5 + 0.5

)zn − 1

2a2n

zn Wn − zn−1.

(49)

Based on the analysis of (40)–(49), we have

Vn ≤ −n∑

j=1

k j z2j + 1

2

n∑j=1

(a2

j + ε2j

)+n∑

j=1

W j

r j

(r j

2a2j

z2j − ˙W j

)

− λ

n∑i=1

n∑j=1

e−λ(t−τi )

∫ t

t−τi

eλsz2j (s)q

2i j (x(s))ds

− μ1e

(zn v +

˙eη

)+ 1

2(μ2ζ )2. (50)

Noting that

n∑j=1

k0 j

r jW j W j ≤−

n∑j=1

k0 j

2r jW 2

j +n∑

j=1

k0 j

2r jW 2

j (51)

μ1η0

ηee ≤−μ1η0

2ηe2 + μ1η0

2ηe2. (52)

Substituting (51) and (52) into (50), we have

Vn ≤ −n∑

j=1

k j z2j −

n∑j=1

k0 j

2r jW 2

j +n∑

j=1

k0 j

2r jW 2

j + 1

2

n∑j=1

(a2

j +ε2j

)

− λ

n∑i=1

n∑j=1

e−λ(t−τi )

∫ t

t−τi

eλsz2j (s)q

2i j (x(s))ds

+ 1

2(μ2ζ )2 − μ1η0

2ηe2+ μ1η0

2ηe2. (53)

Let P = min{2k1, . . . , 2kn, k01, . . . , k0n, λ(1 − τmax), η0}and

Y =n∑

j=1

k0 j/2r j W 2j + 1/2

n∑j=1

(a2

j + ε2j

)

+ μ1η0/2ηe2 + 1/2(μ2ζ )2.

Consequently, the inequality (53) can be reexpressed as

Vn ≤ −PVn + Y. (54)

Thus, we have

Vn ≤(

Vn(0) − YP

)e−P t + Y

P . (55)

Noting that if t → ∞z2

1 = (y − yr )2 ≤ 2Y

P . (56)

By increasing the parameters k j , k0 j , η, and r j , η0 mean-while reducing the parameters a j , the tracking error limitation2Y/P can be adjusted arbitrarily small. Therefore, the controlscheme proposed in Theorem 1 can guarantee that all thesignals in the closed-loop system remain bounded, and theoutput of the system converges to an adjustable neighborhoodof the reference signal.

Remark 6: With the prerequisite of Assumption 4, a robustadaptive neural controller can be constructed for the nonstrict-feedback system in (1), and the conclusion is presented inTheorem 1. However, from Assumption 4, we know that thesign of μ1 must be known in advance as prior knowledge.To relax the restriction, a Nussbaum-type function is intro-duced to solve the problem of unknown control direction anda novel adaptive neural control scheme is proposed in thefollowing theorem.

B. Unknown Direction Hysteresis

In the section, we investigate the fusion of unknown direc-tion hysteresis with adaptive neural control approach. Thestable control algorithm is presented in the following theorem.

Theorem 2: Consider the nonstrict-feedback system in (1),under the Assumptions 1–3, if we choose the virtual con-trollers α j , the auxiliary controller v , the control law v, andthe adaptive laws as follows:⎧⎪⎪⎪⎪⎪⎪⎪⎪⎨⎪⎪⎪⎪⎪⎪⎪⎪⎩

α j = −(k j + n2

4 j + 0.5)z j − 12a2

jz j W j − z j−1

v = −(kn + n2

4n + 1)zn − 12a2

nznWn − zn−1

v = −N(ϑ)v

ϑ = −γ vzn˙Wi = ri

2a2i

z2i − k0i Wi (i = 1, . . . , n; j = 1, . . . , n − 1)

(57)

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2136 IEEE TRANSACTIONS ON NEURAL NETWORKS AND LEARNING SYSTEMS, VOL. 25, NO. 12, DECEMBER 2014

where z0 = −yr . We can construct a robust adaptive neuralcontrol scheme to guarantee that all system states and adaptiveparameters are bounded. By increasing the designed para-meters k1, . . . , kn , k01, . . . , k0n , γ, r1, . . . , rn while reducinga1, . . . , an , the tracking error limitation can be adjusted arbi-trarily small.

Remark 7: It should be highlighted that Assumption 4 is notnecessary to the control scheme in Theorem 2. Therefore, thecontrol algorithm in Theorem 2 can be applied to nonstrict-feedback system with the unknown direction hysteresis.

Proof: We employ the backstepping technique to demon-strate this theorem. The first n − 1 steps are similar tothe aforementioned procedures. At nth step, the Lyapunov–Krasovskii function is chosen as follows:

Vn = Vn−1 + 1

2z2

n + 1

2rnW 2

n . (58)

Differentiating two sides of (58), we have

Vn = Vn−1 + zn( fn(x) + hn(x(t − τn)) + H (v)

+ ωn(t, x) − αn−1) − 1

rnWn

˙Wn . (59)

Noting that

zn H (v) = zn(μ1v + μ2ζ ). (60)

Consider the sign of μ1 is unknown, we introduce aNussbaum-type function N(ϑ) as N(ϑ) = ϑ2 cos ϑ . Thecontrol signal v is constructed as v = −N(ϑ)v . Subsequently,we have

zn H (v) = −(μ1 N(ϑ) + 1)zn v + zn v + znμ2ζ (61)

where v is the auxiliary control signal needed to be furtherdesigned. The variable ϑ is obtained by the differentiationequation ϑ = −γ vzn . With these analysis, equality (61) canbe expressed as

zn H (v) = 1

γ(μ1 N(ϑ) + 1)ϑ + zn v + znμ2ζ. (62)

The auxiliary controller v and the adaptive parameters Wi

are designed in (57), respectively. By repeating the proceduresof (18)–(38), and combining with the analysis of (59)–(62), wehave

Vn ≤−n∑

j=1

k j z2j −

n∑j=1

k0 j

2r jW 2

j +n∑

j=1

k0 j

2r jW 2

j + 1

2

n∑j=1

(a2

j + ε2j

)

− λ

n∑i=1

n∑j=1

e−λ(t−τi )

∫ t

t−τi

eλsz2j (s)q

2i j (x(s))ds

+ 1

γ(μ1 N(ϑ) + 1)ϑ + 1

2(μ2ζ ).2 (63)

Two constants are defined as P = min{2k1, . . . , 2kn,k01, . . . , k0n, λ(1 − τmax)} and

Y =n∑

j=1

k0 j/2r j W 2j + 1/2

n∑j=1

(a2

j + ε2j

) + 1/2(μ2ζ )2.

Subsequently, inequality (63) can be written as the followingform:

Vn ≤ −PVn + Y + 1

γ(μ1 N(ϑ) + 1)ϑ. (64)

By direct integration of the differentiation inequality (64) atthe interval [0, t) yields

Vn ≤ Vn(0)e−P t + YP (1 − e−P t )

+e−P t

γ

∫ t

0(μ1 N(ϑ) + 1)ϑ · ePτ dτ. (65)

From Lemma 2, we can know that the terms Vn , ϑ , and∫ t0 (μ1 N(ϑ) + 1)ϑdτ are bounded at the interval [0, t). Fur-

thermore, the result can be extended to t → ∞. Consequently,let C0 be upper bound of � = ∫ t

0 (μ1 N(ϑ) + 1)ϑe−P(t−τ )dτ .Then, the following inequality holds:

Vn ≤(

Vn(0) − YP

)e−P t + Y

P + C0

γ. (66)

When t → ∞z2

1 = (y − yr )2 ≤ 2Y

P + 2C0

γ. (67)

By increasing the designed parameters k j , λ, γ , and k0 j

meanwhile reducing the parameters a j , the tracking errorlimitation can be adjusted arbitrarily small. Therefore, therestriction in Assumption 4 can be removed by the controlscheme presented in the Theorem 2. Furthermore, the controlalgorithm proposed in the Theorem 2 can guarantee that all thestate variables and adaptive parameters of the control systemare bounded.

IV. SIMULATION STUDY

In the section, three numerical examples are provided tovalidate the effectiveness of the proposed control schemes.Example 1 is a general nonlinear system model with thetime-varying delays and the unknown direction hysteresis.Examples 2 and 3 are practical physical models.

Example 1: Consider the following general third-ordernonstrict-feedback nonlinear system:⎡

⎣x1x2x3

⎤⎦=

⎡⎣0 1 0

0 0 10 0 0

⎤⎦ ·

⎡⎣x1

x2x3

⎤⎦ +

⎡⎣ f1(x)

f2(x)f3(x)

⎤⎦ +

⎡⎣h1(τ1(t))

h2(τ2(t))h3(τ3(t))

⎤⎦

+⎡⎣0.1 sin(t)x1x2

2 x3

0.3 cos(π t)x21 x2

20.1 sin(π t)x1x2

2

⎤⎦ +

⎡⎣0

0u

⎤⎦, u = H (v) (68)

where y = x1 is the output of control system. The unknownnonlinear functions are selected as f1(x) = x2

1 x2 + x3,f2(x) = x2

1 x2 + 2x3, and f3(x) = −7x1 − 10x22 − 5x2,

respectively. It should be noted that the external disturbancesw1 = 0.1 sin(t)x1x2

2 x3, w2 = 0.3 cos(π t)x21 x2

2 , and w3 =0.1 sin(π t)x1x2

2 contain whole state variables and time vari-able simultaneously. The time-delayed terms are selected ash1(τ1(t)) = x2(t − τ1(t))x3(t − τ1(t)), h2(τ2(t)) = 0.5x2

2(t −τ2(t))x3(t − τ2(t)), and h3(τ3(t)) = 0.01x2

1(t − τ3(t))x23

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LIU et al.: ADAPTIVE NEURAL CONTROL FOR A CLASS OF NONLINEAR TIME-VARYING DELAY SYSTEMS 2137

TABLE II

INITIAL VALUES AND DESIGNED PARAMETERS

Fig. 3. Trajectories of system output y and the corresponding tracking errorz1 = y − yr .

(t − τ3(t)), respectively. The time delays are selected asτ1(t) = 0.5 + 0.1 sin(t), τ2(t) = 0.5 + 0.3 sin(0.5t), andτ3(t) = 0.5 + 0.2 sin(π t), respectively.

The actual control signal is v, and the reference signal isyr = sin(t) + sin(2t) + cos(3t). The control objective of thissimulation is to construct a robust adaptive neural controlscheme to guarantee that all the system states and adaptiveparameters are bounded, and the tracking error can convergeto an adjustable neighborhood of the origin.

In the simulation, the hysteresis parameters are presentedin Table I, and the initial values of system states and adaptiveparameters are provided in Table II. In addition, the designedparameters are also given in Table II. Based on the theoremderived in this paper and the aforementioned designed para-meters, a robust adaptive neural control scheme is constructed.The simulation results are shown in Figs. 3 and 4, respectively.Fig. 3 shows the tracking performance of control system. Fig. 4shows that the trajectories of system states x2, x3 and thecorresponding actual control signal v.

Example 2: Consider the following inverted pendulum withhysteresis actuator shown in Fig. 5. By writing x1 = θand x2 = θ , the inverted pendulum can be modeled as thefollowing second-order differentiation equation [45]:

x1 = x2

x2 = f (x2) + g(x2)H (v) + d(t) (69)

Fig. 4. Trajectories of system states x2, x3 and actual control signal v .

Fig. 5. Inverted pendulum system with hysteresis actuator.

where

f (x2)= 9.8(mc + m) sin x1 − mlx22 cos x1 sin x1

l(

43 − m cos2 x1

mc+m

)(mc + m)

(70)

g(x2)= cos x1

l(

43 − m cos2 x1

mc+m

)(mc + m)

(71)

d(t) = 3 + 2 cos(2t). (72)

The physical parameters are selected as mc = 1 kg,m = 0.1 kg, and l = 0.5 m, respectively.

It should be noted that the simulation model has beenperformed in [45]. However, the works in [45] consideredthe known direction backlash-like hysteresis model. Comparedwith the simulation model in [45], we consider a more generalmodified Bouc–Wen hysteresis model in this paper. Further-more, the hysteresis direction does not require to be known.By constructing the stable control scheme as the Theorem 2,the simulation results are shown in Figs. 6 and 7, respectively.The comparative simulation results can further validate theeffectiveness of the proposed control scheme in this paper.

Example 3: Consider the following piezo-positioning mech-anism subjected to unknown direction hysteresis input:

M y(t) + Dy(t) + Fy(t) = u, u = H (v) (73)

where y, y, and y represent the position, the velocity, and theacceleration, respectively. v is the voltage signal applied tothe piezo-positioning mechanic system. M , D, and F denote

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2138 IEEE TRANSACTIONS ON NEURAL NETWORKS AND LEARNING SYSTEMS, VOL. 25, NO. 12, DECEMBER 2014

Fig. 6. Trajectories of the system output y and control signal v .

Fig. 7. Trajectories of adaptive parameters W1 and W2.

Fig. 8. Trajectories of the system output y and control signal v .

the mass, damping, and stiffness coefficients, respectively.These parameters are all unknown. In the simulation, the actualparameter values are chosen as M = 1 kg, D = 0.15 Ns/m,F = 1 M/m. The modified Bouc–Wen hysteresis parametersare μ1 = μ2 = 1, β = 1, χ = 0.5, and n = 2. The initialvalue of state is chosen as y(0) = 1.5. The reference signal isyr = 2 sin(0.5π t).

Remark 8: The piezo-position mechanic model in (73)has been investigated in [41] and [75]. However, the controlschemes in [41] and [75] require both the parameters andthe direction of modified Bouc–Wen hysteresis to be knownas prior knowledge. To relax these restrictions, an adaptivecontrol algorithm is proposed in Theorem 2 for the nonlinearsystems with the unknown direction hysteresis input.

In the simulation, the initial values of adaptive parame-ters are chosen as W1(0) = 0.1, W2(0) = 0.01, andϑ(0) = 0.1, respectively. The designed parameters are selectedas k1 = 15, k2 = 16, a1 = a2 = 10, r1 = 250, r2 =250, γ = 1, k01 = 0.003, and k02 = 0.002, respectively.Therefore, we can construct a neural-network-based adaptive

Fig. 9. Trajectories of adaptive parameters W1 and W2.

controller as Theorem 2. The simulation results are shownin Figs. 8 and 9, respectively. Fig. 8 shows that the track-ing trajectory and the corresponding actual control signal v.Fig. 9 shows the trajectories of adaptive parameters W1 andW2. Clearly, the simulation results can further validate theeffectiveness of the proposed control scheme in this paper.

V. CONCLUSION

In this paper, two NN-based adaptive control algorithmsare proposed for a class of CT nonstrict-feedback systemswith unknown modified Bouc–Wen hysteresis input and timevarying delays. Compared with the previous works on hys-teresis phenomenon, the direction of the modified Bouc–Wenhysteresis model studied in the literature can be unknown.Furthermore, an optimized method is proposed to reduce thecomputation burden in adaptation mechanism. Based on theLyapunov–Krasovskii method, two adaptive neural controlschemes are constructed to guarantee that all the system statesand adaptive parameters remain bounded, and the trackingerror is driven to an adjustable neighborhood of the origin.In addition, three simulation examples are provided to verifythe effectiveness of the proposed control schemes.

ACKNOWLEDGMENT

The authors would like to thank the Associate Editor and theanonymous reviewers for a number of constructive commentsthat have improved the presentation of this paper.

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Zhi Liu received the B.S. degree from the HuazhongUniversity of Science and Technology, Wuhan,China, the M.S. degree from Hunan University,Changsha, China, and the Ph.D. degree fromTsinghua University, Beijing, China, all in electricalengineering, in 1997, 2000, and 2004, respectively.

He is currently a Professor with the Department ofAutomation, Guangdong University of Technology,Guangzhou, China. His current research interestsinclude fuzzy logic systems, neural networks, robot-ics, and robust control.

Guanyu Lai received the B.S. degree in electricalengineering and automation, and the M.S. degree incontrol science and engineering from the GuangdongUniversity of Technology, Guangdong, China, in2012 and 2014, respectively, where he is currentlypursuing the Ph.D. degree from the Department ofAutomation.

His current research interests include neural net-works, adaptive fuzzy control, cooperative control,and unmanned aerial vehicle.

Yun Zhang received the B.S. and M.S. degreesin automatic engineering from Hunan University,Changsha, China, and the Ph.D. degree in automaticengineering from the South China University of Sci-ence and Technology, Guangzhou, China, in 1982,1986, and 1998, respectively.

He is currently a Professor with the Department ofAutomation, Guangdong University of Technology,Guangzhou. His current research interests includeintelligent control systems, network systems, andsignal processing.

Xin Chen received the B.S. degree from ChangshaRailway Institute, Changsha, China, the M.S. degreefrom the Harbin Institute of Technology, Harbin,China, and the Ph.D. degree from the Huazhong Uni-versity of Science and Technology, Wuhan, China,all in mechanical engineering, in 1982, 1988, and1995, respectively.

He is currently a Professor with the Department ofMechatronics Engineering, Guangdong University ofTechnology, Guangzhou, China. His current researchinterests include mechatronics and robotics.

Chun Lung Philip Chen (S’88–M’88–SM’94–F’07) received the M.S. degree from the Universityof Michigan, Ann Arbor, MI, USA, and the Ph.D.degree from Purdue University, West Lafayette, IN,USA, all in electrical engineering, in 1985 and 1988,respectively.

He is currently a Chair Professor with the Depart-ment of Computer and Information Science and theDean of the Faculty of Science and Technology,University of Macau, Macau, China. His currentresearch interests include computational intelligence,

systems, and cybernetics.