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An LMI approach to H∞ synchronization of second-order neutral master-slave systems

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Abstract— TheH synchronization problem of the master and

slave structure of a second-order neutral master-slave systems with time-varying delays is presented in this paper. Delay-dependent sufficient conditions for the design of a delayed output-feedback control are given by Lyapunov-Krasovskii method in terms of a linear matrix inequality (LMI). A controller, which guarantees H synchronization of the master

and slave structure using some free weighting matrices, is then developed. A numerical example has been given to show the effectiveness of the method.

I. INTRODUCTION

In the last few years, synchronization in chaotic dynamical systems has received a great deal of interest among scientists from various fields [1, 2]. The results of chaos synchronization are utilized in biology, secret communication and cryptography, nonlinear oscillation synchronization and some other nonlinear fields. The first idea of synchronizing two identical chaotic systems with different initial conditions was introduced by Pecora and Carroll [3], and the method was realized in electronic circuits. The methods for synchronization of the chaotic systems have been widely studied in recent years, and many different methods have been applied theoretically and experimentally to synchronize chaotic systems, such as feedback control [4-8], adaptive control [9, 10], backstepping [11] and sliding mode control [12].

One of the most attractive dynamical systems is the second-order systems which capture the dynamic behaviour of many natural phenomena, and have found applications in many fields, such as vibration and structural analysis, spacecraft control, electrical networks, robotics control and, hence, have attracted much attention (see, [13-16]). It has been proved that in special situations a second-order system may show chaotic dynamics, for instance, in [17], a second-order linear plant containing a relay with hysteresis type nonlinearity shows the chaotic nature of its dynamical behavior. Moreover, complex dynamical behavior of second-order linear plants controlled with conventional controllers is investigated in [18, 19]. On the other hand, in view of the time-delay phenomenon, which is frequently encountered in practical situations, this delay may induce complex behaviors for the systems concerned (see [20, 21]). Up to H.R. Karimi, M. Zapateiro and N. Luo are with the Institute of Informatics and Applications, University of Girona, Girona, Spain (e-mails: {hamidreza.karimi, mauricio.zapateiro, ningsu.luo}@udg.edu).

J.M. Rossell is with Dpt. Mat. Aplicada III, Universitat Politecnica de Catalunya, Spain (e-mail: [email protected]).

now, to the best of the authors’ knowledge, no results about the synchronization of second-order master-slave systems with time-varying delays using delayed output-feedback control are available in the literature, which remains to be important and challenging.

In this paper, we make an attempt to develop an efficient approach forHsynchronization problem of second-order neutral master-slave systems with time-varying state delays. The main merit of the proposed method lies in the fact that it provides a convex problem via introduction of additional decision variables such that the control gains can be found from the LMI formulations without reformulating the system equations into a standard form of a first-order neutral system. By using a Lyapunov-Krasovskii method and some free weighting matrices, new sufficient conditions are established in terms of a delay-dependent LMI for the existence of desired delayed output-feedback control such that the resulting closed-loop system is asymptotically stable and satisfies a prescribedH∞performance. A significant advantage of our result is that the desired control is designed directly instead of coupling the model to a first-order neutral system and then designing the control law in a higher dimensional space. Therefore, our result can be implemented in a numerically stable and efficient way for high-dimensional second-order systems. Furthermore, retaining the model in matrix second-order form has many advantages such as preserving physical insight of the original problem, preserving system matrix sparsity and structure, preserving uncertainty structure and entailing easier implementation. Finally, the simulation results are given to illustrate the usefulness of our results.

II. PROBLEM DESCRIPTION

Consider a model of second-order neutral master-slave systems in the form of

[

]

[

]

⎪ ⎪ ⎪ ⎪ ⎩ ⎪⎪ ⎪ ⎪ ⎨ ⎧ = − + = − ∈ = − ∈ = = − + + − + + − + + − + ), ( ) ( )), ( ( ) ( ) ( , 0 }, , { max ), ( ) ( , 0 }, , { max ), ( ) ( , 0 ))) ( ( ( )) ( ( )) ( ( ) ( )) ( ( ) ( )) ( ( ) ( 3 2 1 2 1 1 1 1 t x C t y t r t x C t x C t z r d t t t x r d t t t x t r t x g N t x f N t r t x B t x B t r t x A t x A t d t x M t x M m m m m m M M m M M m m m m m m m m m φ φ         (1)

An LMI Approach to

H

Synchronization of Second-Order

Neutral Master-Slave Systems

H.R. Karimi, M. Zapateiro, N. Luo, J.M. Rossell

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[

]

[

]

⎪ ⎪ ⎪ ⎪ ⎩ ⎪⎪ ⎪ ⎪ ⎨ ⎧ = − + = − ∈ = − ∈ = + = − + + − + + − + + − + ), ( ) ( )), ( ( ) ( ) ( , 0 }, , { max ), ( ) ( , 0 }, , { max ), ( ) ( ), ( ) ( ))) ( ( ( )) ( ( )) ( ( ) ( )) ( ( ) ( )) ( ( ) ( 3 2 1 2 2 1 1 1 1 t x C t y t r t x C t x C t z r d t t t x r d t t t x t w D t u B t r t x g N t x f N t r t x B t x B t r t x A t x A t d t x M t x M s s s s s M M s M M s s s s s s s s s ϕ ϕ         (2) where xm(t),xs(t) are the n×1 state vector of the master and slave systems, respectively; u(t) is the r×1 control input;

) (t

w is the q×1 external excitation (disturbance), )

( ), (t z t

zm s are the

s

×

1

controlled output and ym(t),ys(t) is

the l×1 measured output. The time-varying vector valued initial functions φ and (t) ϕ(t) are continuously differentiable functionals, and the time-varying delays d(t) and r(t) are functions satisfying, respectively,

⎪⎩ ⎪ ⎨ ⎧ ≤ ≤ < < ≤ ≤ < . ) ( , ) ( 0 , 1 ) ( , ) ( 0 D M D M r t r r t r d t d d t d   (3)

Assumption 1: The nonlinear functions f,g:nn are

continuous and satisfy f(0)= g(0)=0 and the Lipschitz condition, i.e., f(x0y0) f(x0)f(y0) ≤ f(x0−y0) and

) ( ) ( ) (x0 y0 g x0 g y0 g − ≤ − ≤ g(x0−y0) for all n y x0, 0∈ℜ and

g

g

f

f

,

,

,

are some known matrices.

Now, the synchronization error of the master and slave systems (1) and (2) is defined as e(t)=xs(t)−xm(t), then the error dynamics between (1) and (2), namely synchronization error system, can be expressed by

⎪ ⎪ ⎩ ⎪ ⎪ ⎨ ⎧ = − + = + = − + + − + + − + + − + ), ( ) ( )), ( ( ) ( ) ( ), ( ) ( ))) ( ( ( ˆ )) ( ( ˆ )) ( ( ) ( )) ( ( ) ( )) ( ( ) ( 3 2 1 2 2 1 1 1 1 t e C t y t r t e C t e C t z t w D t u B t r t e g N t e f N t r t e B t e B t r t e A t e A t d t e M t e M e e      (4) where ze(t)=zs(t)−zm(t),fˆ(e(t)):= f(xs(t))− f(xm(t)) and ))) ( ( ( : ))) ( ( ( ˆ et r t g x t r t g − = s − −g(xm(tr(t))).

The problem to be addressed in this paper is formulated as follows: given the second-order neutral master-slave systems (1) and (2) with any time-varying delays satisfying (3) and a prescribed level of disturbance attenuationγ>0, find a delayed output-feedback control

u

(t

)

of the form

)) ( ( ) ( : )) ( ( )) ( ( ) ( ) ( ) ( 1 2 3 4 t r t C K t C K t r t y K t r t y K t y K t y K t u r e e e e − + = − + − + + = ξ ξ   (5) where K:=[K1 K2], Kr:=[K3 K4], C:=diag{C3,C3}, )} ( ), ( { ) (t =col et et

ξ and the matrices 4

1

}

{Ki i= are the control

gains to be determined such that

1) the synchronization error system (4) is asymptotically stable for any time delays satisfying (3);

2) under zero initial conditions and for all non-zero ] , 0 [ ) (t ∈ L2 ∞

w , the H∞ performance measure, i.e.,

∞ ∞ = − 0 2 () () ) ( ) (t z t w t wt dt z J T e T e γ , satisfies J∞<0;

in this case, the systems (1) and (2) are said to be asymptotically stable with H∞ performance measures.

III. MAIN RESULTS

In this section, sufficient conditions for the solvability of the delayed output-feedback control design problem are proposed using the Lyapunov method and an LMI approach.

Lemma 1 ([22]): For any arbitrary positive definite matrix

H and a matrix W the following inequality holds:

− − − ⎥⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + + ∗ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ≤ − t t r t T T t t r t T ds s b s a I W H H I W H W H H s b s a ds s a s b ) ( 1 ) ( ( ) ) ( ) ( ) ( ) ( ) ( ) ( ) ( 2

where the symbol

denotes the elements below the main diagonal of a symmetric block matrix.

Lemma 2: ([23]) For a given Μp×nwith

n p

rank(Μ)= < , assume that Zn×nis a symmetric matrix,

then there exists a matrix Zˆp×p such that ΜZ=ZˆΜif

and only if T V Z Z diag V Z= . { 1, 2}. and T U Z U Z 1 1 ˆ ˆ ˆ= Μ Μ, whereZ p×p 1 , ) ( ) ( 2 p n p n

Z − × − and the singular value

decomposition of the matrix Μ is represented as

T

V U[Μˆ 0] =

Μ with the unitary matrices Up×p,Vn×n

and a diagonal matrix Μˆp×pwith positive diagonal

elements in decreasing order.

Theorem 1: For given scalars dM,rM >0,dD <1,rD and

0 >

γ , the second-order neutral master-slave systems (1) and (2) with any time-varying delays satisfying (3) is robustly stabilizable by (5) and satisfies the H performance measure, if there exist some matrices P2, P3, W,

2 1 } {Fi i= , positive-definite matrices P1, 2 1 } {Qi i= ,H and

positive-definite diagonal matrices 3 1

}

i i=, such that the following

inequality is feasible, 0 ] 0 ˆ [ 0 ) ˆ ( 33 23 22 13 12 1 1 11 < ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎣ ⎡ Π ∗ ∗ Π Π ∗ Π Π ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ + Π = Π I C I C T (6) with ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ + + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ = Π 0 ˆ ) ˆ ( ) ~ 0 ˆ 0 ( 2 1 1 2 1 2 12 I C I C F F I A H W A P T T T T , I C C I I g I g sym F sym Q r T T T D) { } {( ˆ) ˆ} ˆ ˆ 1 ( 1 2 3 2 2 22 =− − − − Λ + Π , , 0 ) ( ˆ , 0 ) ( ˆ 0 , 0 : 1 2 1 1 13 ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ + Λ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ + Λ + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎢ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ = Π T T IT f f T IT g g T N P M P ⎥ ⎥ ⎦ ⎤ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ 0 , 0 , 0 1 2 F D P N PT T ,

[

]

2 3 23: 0,0,0,Iˆ (g g) ,0,F T T Λ + = Π ,

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} , }, { }, { }, { , ) 1 ( { : 1 2 3 2 1 2

33 =diag− −dD QsymΛ −symΛ −symΛ − IrMP

Π γ , } ˆ ˆ 0 { } ˆ ˆ 0 { } ˆ ~ ~ ˆ { : 1 2 1 11 I g gI I sym I f f I I sym M A I I I P sym T T T T T T T Λ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − Λ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ = Π ] 0 [ 0 0 0 1 0 0 ~ 0 0 ~ } }, { { ) ( ) ( ]} 0 ~ [ 0 { 1 1 1 2 1 1 1 1 I A H A I r r I I P I I r Q F sym Q diag P I HW H I H W P r I A H W P sym T D M T M T T M T T ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − + ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ + + + + + + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + − where A1 BI A A1 I B2KC ~ ) ( ˆ : ˆ = + + , A B B K C r 2 1 2: [ 0] ˆ = , the

operatorsym{A} denotesA AT

+ and the matrices and I~ are defined, respectively, as Iˆ:=[I 0] and I~:=[0 I].

Proof: Firstly, we represent the synchronization error system

(4) in an equivalent descriptor model form as

⎪ ⎪ ⎪ ⎩ ⎪⎪ ⎪ ⎨ ⎧ − − + + − − + + − + = = ∫ − ), ( ))) ( ( ( ˆ )) ( ( ˆ ) ( )) ( ( ˆ ) ( ˆ )) ( ( ) ( 0 ), ( ) ( 2 1 ) ( 1 2 1 1 t w D t r t e g N t e f N ds s A t r t A t A t d t M t M t t e t t r t η ξ ξ η η η  (7) Define the Lyapunov-Krasovskii functional

= = 5 1 ) ( ) ( i i t V t V , (8) where , ) ( ) ( ] ) ( ) ( [ : ) ( ) ( ) ( 1 1 ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ = = t t P T t t t P t t V T T T η ξ η ξ ξ ξ

− = t t r t TQ s ds s t V ) ( 1 2() ξ( ) ξ( ) ,

− = t t d t TQ s ds s t V ) ( 2 3() η( ) η( ) ,

∫ ∫

− + = 0 ) ( 1 4() ( ) ( ) t r t t T P s dsd s t V θ θ ξ ξ  ,

− ⎥⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + − − = t t r t T T D ds s A H A s t r t s r t V ) ( 1 1 5 ( ) 0 0 ) ( )) ( ( 1 1 ) ( η η ,

with T =diag{I,0} and ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ = 2 3 1 0 P P P P , where P PT 1 1 0< = . Differentiating V1(t) along the system trajectory becomes

) ( )} ( 0 ))) ( ( ( ˆ 0 )) ( ( ˆ 0 )) ( ( ˆ 0 )) ( ( 0 ) ( ) ( ˆ ~ ~ ˆ { ] ) ( ) ( [ 2 0 ) ( ] ) ( ) ( [ 2 ) ( ) ( 2 ) ( 2 1 2 1 1 1 1 t t w D t r t e g N t e f N t r t A t d t M t t M A I I I P t t t P t t t P t t V T T T T T T T T T β ξ η η ξ η ξ ξ η ξ ξ ξ + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − − ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + − × ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + − ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ = ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ = =    (9) where

− ⎥⎦ ⎤ ⎢ ⎣ ⎡ − = t t r t T T T s ds A P t t t ) ( 1 ) ( 0 ] ) ( ) ( [ 2 ) ( ξ η η β . Using Lemma 1

for a(s)=col{0,A1}η(s) and b=Pcol{ξ(t),η(t)}we obtain

∫ − − ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + − − ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + + ≤ t t r t T T T T T T T T T T M ds s A H A s t r t t I A H W P t t t t P I HW H I H W P t t r t ) ( 1 1 1 1 ) ( 0 0 ) ( ))) ( ( ) ( ( ~ 0 ] ) ( ) ( [ 2 ) ( ) ( ) ( ) ( ] ) ( ) ( [ ) ( η η ξ ξ η ξ η ξ η ξ β (10)

Also, differentiating the second to forth Lyapunov terms in (8) give )), ( ( )) ( ( ) 1 ( ) ( ) ( ) ( 1 1 2 t t Q t r t r t Q t r t V T D T ≤ξ ξ ξ ξ  (11) )), ( ( )) ( ( ) 1 ( ) ( ) ( ) ( 2 2 3 t t Q t d t d t Q t d t V T D T ≤η η η η  (12)

− − ≤ t t r t T T M t P t s P s ds r t V ) ( 1 1 4() ξ() ξ() ξ( ) ξ( )  (13)

and the time derivative of the last term of V(t) in (8) is

− ⎥⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − ≤ t t r t T T T T D M s ds A H A s t A H A t r r t V ) ( 1 1 1 1 5 () 0 0 ) ( ) ( 0 0 ) ( 1 ) ( η η η η  (14)

Moreover, from the Leibniz-Newton formula, the following equation holds for any matrices 2

1 1} {F i= with appropriate dimensions: 0 ) ) ( )) ( ( ) ( )( )) ( ( ) ( ( 2 ) ( 2 1+ − − − −

= − t t r t T T t F t rt F t t rt s ds ξ ξ ξ ξ ξ  (15)

On the other hand, for any positive scalars 3 1 } {Λi i= we have: ))) ( ( ))) ( ( ( ˆ ( ))) ( ( ))) ( ( ( ˆ ( 2 0 )) ( )) ( ( ˆ ( )) ( )) ( ( ˆ ( 2 0 )) ( )) ( ( ˆ ( )) ( )) ( ( ˆ ( 2 0 3 2 1 t r t e g t r t e g t r t e g t r t e g t e g t e g t e g t e g t e f t e f t e f t e f T T T − − − Λ − − − − < − Λ − − < − Λ − − < (16) Using the obtained derivative terms (9)-(15) and adding the right-hand sides of equation (16) into, we obtain the following result for V(t),

) ( ) ( )) ( ( )) ( ( ) 1 ( ) ( ) ( ) ( ) ( )) ( ( ) ( ) ( 2 )) ( ( ) ) 1 ))(( ( ( ) ( ) ( ) ( ) ( 0 0 ) ( 1 ))) ( ( ) ( ( ~ 0 ] ) ( ) ( [ 2 ) ( ) ( ) ( ) ( ] ) ( ) ( [ )} ( 0 ))) ( ( ( ˆ 0 )) ( ( ˆ 0 )) ( ( ˆ 0 )) ( ( 0 ) ( ) ( ˆ ~ ~ ˆ { ] ) ( ) ( [ 2 ) ( ) ( 1 1 2 2 1 1 2 2 2 1 1 1 1 1 1 1 1 2 1 2 1 1 5 1 t F P F t r t d t Q t d t d t Q t t P t r t r t F F t t r t F F Q r t r t t F F Q t t A H A t r r t r t t I A H W P t t t t P I HW H I H W P t t r t w D t r t e g N t e f N t r t A t d t M t t M A I I I P t t t V t V T T M T D T T M T T T D T T T T T D M T T T T T T T T M T T T T T i i ϑ ϑ η η η η ξ ξ ξ ξ ξ ξ ξ ξ η η ξ ξ η ξ η ξ η ξ ξ η η ξ η ξ − − = + − − − − × + + − − + − + + − − − + + + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ × ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − + − − ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + + + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − − ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + − ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + − × ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ ≤ =

   

− − + + − − − − Λ − − − − − × Λ − − − Λ − − t t r t T T T T T T T T ds P s F t P P s F t t r t I g t r t e g t r t I g t r t e g t I g t e g t I g t e g t I f t e f t I f t e f ) ( 1 1 1 1 3 2 1 ) ) ( ) ( ( ) ) ( ) ( ( ))) ( ( ˆ ))) ( ( ( ˆ ( ))) ( ( ˆ ))) ( ( ( ˆ ( 2 )) ( ˆ )) ( ( ˆ ( )) ( ˆ )) ( ( ˆ ( 2 )) ( ˆ )) ( ( ˆ ( )) ( ˆ )) ( ( ˆ ( 2 ξ ϑ ξ ϑ ξ ξ ξ ξ ξ ξ   (17) where the vectors ϑ(t)andN are, respectively,

)} ( )), ( ( )), ( ( ), ( ), ( { : ) (t =col ξ t η t ξ trt η td t wt ϑ , (18) } 0 , 0 , , 0 , { : col F1 F2 F = . (19)

(4)

Under zero initial conditions, the H performance measure can be rewritten as ∫ ∞ ∞= − − − + 0 2 () () ()] )) ( ) ( ( )) ( ) ( [(z t z t z t z t wt wt V t dt J T m s T m s γ  (20) Substituting the terms of ξ(t)

[

IˆTI~ I~T

]

.col{ξ(t),η(t)}

=  , )), ( ( ˆ ) ( ˆ ) ( ) (t z t C1I t C2I t r t

zsm = ξ + ξ − and upper bound of

) (t

V in (17) results in (20) being less than the integrand )

( ) (t T ϑt

ϑ Π where the matrix

Π

, by Schur complement, is given in (6). Now, if

Π

<

0

, then J∞ <0. ■

Remark 1: It is easy to see that the inequality (6) imply 0

11<

Π . Hence by Proposition 4.2 in the reference [24], the matrix P is nonsingular. Then, according to the structure of the matrix P, the matrix X:= P−1 has the form

⎥ ⎦ ⎤ ⎢ ⎣ ⎡ = 2 3 1 0 X X X X , where = −1 i i P X (i=1,2) and X3=−X2P3X1.

Remark 2: According to structure of matrixC, i.e.,

} , { : diag C3 C3

C = , with rank(C3)=l<n, Lemma 2 proposes that an equivalent condition on equation CX1=Xˆ1C is

T V X X diag V X1= . { 11, 22} , T U C X C U X 1 11 1 ˆ ˆ ˆ =, whereX 2l2l 11∈ℜ × , ) ( 2 ) ( 2 22 l n l n X − × − and C=U[Cˆ 0]VT (the

singular value decomposition of the matrixC), with l

C

rank( )=2 , U2l×2l , V2n×2nand Cˆ2l×2l.

Theorem 2: Consider the second-order neutral master-slave

systems (1) and (2) with any time-varying delays satisfying (3). For given scalars dM,rM >0,dD <1,rD and γ >0, there

exits an output-feedback control in the form of (5) such that the resulting closed-loop system is robustly asymptotically stable and satisfies H performance measure in Definition 1, if there exist a scalar

α

, matrices 2

1 } ˆ {Fi i= , 2 1 } ~ {Xi i= ,X2,X3, positive-definite matrices X11,X22, 2 1 } ˆ {Qi i= , H and positive

definite diagonal matrices 3 1

}

i i= , satisfying the LMI

0 ˆ ˆ ˆ ˆ 0 ˆ ˆ 0 ˆ } ˆ { ˆ ) 1 ( ˆ ˆ ˆ ˆ ˆ 55 45 44 35 33 25 23 2 1 15 14 13 12 11 < ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎣ ⎡ Π ∗ ∗ ∗ ∗ Π Π ∗ ∗ ∗ Π Π ∗ ∗ Π Π − − − ∗ Π Π Π Π Π F sym Q rD (21) where ⎥ ⎥ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎢ ⎢ ⎣ ⎡ + ∗ ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ + + − + + + ⎟ ⎟ ⎠ ⎞ ⎜ ⎜ ⎝ ⎛ + + + + + + = Π T T T T T T T T T T T T T T M X X M M X X I B X C I A A I B X Q I X X I F F I I X X I I 2 2 3 2 2 1 1 1 1 3 3 1 1 1 1 11 ~ ~ ) ~ ) ) 1 ( ( ˆ ( ˆ ~ ~ ˆ ˆ ˆ ~ ~ ˆ : ˆ α

[

]

}} { }, { }, { , ˆ ) 1 ( { ˆ ~ ) ~ ˆ ( ˆ ˆ : ˆ , ) ( ˆ , 0 , 0 , 0 ˆ 0 , 0 ) ( ˆ , 0 ) ( ˆ 0 , 0 ˆ 3 2 1 2 33 2 2 1 1 1 1 2 12 1 23 3 2 1 1 1 1 13 Λ − Λ − Λ − − − = Π ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ − − − = Π + = Π ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ Λ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ + ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ + + Λ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ = Π sym sym sym Q d diag C X B X I A I B F F g g I X N g g I X f f I X N X M D T T T T T T T T T T T α } , , , , { ˆ ) 1 ( , 0 ) ˆ ( , ~ ~ ˆ ~ , 0 ˆ , 0 ˆ 1 1 2 44 1 2 3 1 1 14 H r I X r X r I diag H r I C I X I X I I X r F D M M M M T T T T M − − − − − = Π ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ + ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ + ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − = Π γ α ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎥ ⎦ ⎤ ⎢ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ = Π ˆ ˆ ,0 0 , ˆ ˆ 0 , 0 0 , ˆ 1 2 1 3 2 3 15 I g I g I f I f I I A X A X X X T T T T T T T T T T

[

]

[

]

} , , , , , , 1 , { ˆ ˆ ˆ , 0 , 0 , 0 , 0 ˆ 3 3 2 2 1 1 2 55 25 Λ − Λ − Λ − Λ − Λ − Λ − − − − = Π = Π H r r Q diag g I g I M D T T

The desired control gains in (5) are given by 1 1 2 1 1 1 ˆ ~ , ˆ ~ − = − =X X K X X K r from LMI (21), (22)

where the matrices X1 and Xˆ1 follow from Remark 2.

Proof: Let diag{X ,X1,X1, 1, 2, 3,I,X1,X1,I,H}

T Λ Λ Λ = ζ where Λ :=Λ−1 i i and 1 − = H H . By introducing T:=HWP as a new decision variable (with T XI), applying the Schur complement to the matrix inequality (6) in Theorem 1 and premultiplying ζ and postmultiplying T

ζ where Λ :=Λ−1

i i

and H = H−1and using the inequalities

I g g I I g g I I g g I sym I g g I I I g g I I I g g I I sym I f f I I I f f I I I f f I I sym T T T T T T T T T T T ˆ ˆ ˆ ˆ } ˆ ˆ { ˆ ˆ 0 ˆ ˆ 0 } ˆ ˆ 0 { ˆ ˆ 0 ˆ ˆ 0 } ˆ ˆ 0 { 3 3 3 2 2 2 1 1 1 Λ + Λ ≤ Λ − Λ + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ Λ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ≤ Λ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − Λ + ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ Λ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ ≤ Λ ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ − (23) and considering 1: ˆ1 ~ X K X = , Qˆ X1QiX1 T i= and Fˆ X1FiX1 T i = ,

we obtain the LMI (21). ■

IV. SIMULATION RESULTS

Consider the second-order neutral master-slave systems (1) and (2), where the system matrices are given by

⎥ ⎦ ⎤ ⎢ ⎣ ⎡ = 01 00.8 M , ⎦ ⎤ ⎢ ⎣ ⎡ = 00.5 00.4 1 M , ⎦ ⎤ ⎢ ⎣ ⎡ = 01.3 00..55 A , ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ = 00.075.25 00..125125 1 A , ⎦ ⎤ ⎢ ⎣ ⎡ = 00..24 00..31 B , ⎦ ⎤ ⎢ ⎣ ⎡ = 00.05.1 00..075025 1 B , ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ = 00..48 00..55 1 N , ⎦ ⎤ ⎢ ⎣ ⎡ = 00..21 00..125125 2 N , T C C ⎦ ⎤ ⎢ ⎣ ⎡ = = 2 11 1 , ⎥ ⎦ ⎤ ⎢ ⎣ ⎡ = 11 01.5 3 C , ⎦ ⎤ ⎢ ⎣ ⎡ = 00..11 D .

The delays r(t)=d(t)=(1et) (1+et)are time-varying and satisfy 0r(t)=d(t)1 and r(t)= td()0.5. For simulation purpose, a uniformly distributed random signal with minimum and maximum -1 and 1, respectively, as the

(5)

disturbance is imposed on the response system. With the above parameters, the neutral master-slave systems (1) and (2) exhibit chaotic behaviours such the xm1−xm2 and

2 1 m

m x

x − planes with ξ(0)= col{0.4,0.6,−0.3,−0.2}, } 1 . 0 , 1 . 0 , 7 . 0 , 8 . 0 { ) 0 ( = col

ζ , respectively, are shown in

Fig. 1. -5 -4 -3 -2 -1 0 1 1 2 3 4 5 6 7 8 (a) -2 -1.5 -1 -0.5 0 0.5 1 1.5 2 -5 -4 -3 -2 -1 0 1 2 3 4 (b)

Figure 1. The phase trajectories: a)xm1−xm2 plot and b) 2

1 m

m x

x − plot.

Figure 2. The synchronization errors: a) e1(t)(solid line) and b) e2(t) (dashed line).

It is required to design the control law (5) such that the closed-loop system is asymptotically stable and satisfies the

H performance measure. To this end, in light of Theorem 2, we solved LMI (21) with the disturbance attenuation

2 . 0 =

γ and obtained the following control gains by using Matlab LMI Control Toolbox

[

8.9681 -9.0207 37.1101 -30.0309

]

= K ,

[

-0.0250 0.1896 0.5152 -2.1808

]

= r K .

Figure 3. Time-response of the control law for system.

Figure 4. Comparison of the controlled outputs: a) closed-loop system (solid line) and b) open-closed-loop system (dashed line).

Now, by applying the delayed state feedback controller (5) with the parameters above, the synchronization error between the drive system and response system, i.e.

) ( ) ( ) (t x t x t

e = sm , is shown in Fig. 2. It is seen that the

synchronization errors e1(t)=xs1(t)−xm1(t) and ) ( ) ( ) ( 2 2 2 t x t x t

e = sm converge to zero. The curve of

output-feedback control is also shown in Fig. 3. To observe the H performance, the response of the controlled output, i.e., ) ( 1 t xm ) ( 2 t xm ) ( 1 t xm ) ( 2 t xm

(6)

) (t

ze , is depicted and compared with the output signal in the

open-loop system under the disturbance in Fig. 4. V. CONCLUSION

This paper presented the H∞ synchronization problem of the master and slave structure of a second-order neutral chaotic system with time-varying delays. Delay-dependent sufficient conditions for the design of a delayed output-feedback control were given by Lyapunov-Krasovskii method in terms of an LMI. A controller guaranteeing asymptotic stability, and H synchronization of the master and slave structure using some free weighting matrices was developed directly instead of coupling the model to a first-order neutral chaotic system.

ACKNOWLEDGMENT

This work has been partially funded by the European Union (European Regional Development Fund) and the Ministry of Science and Innovation (Spain) through the coordinated research project DPI2008-06699-C02. The author H.R. Karimi is grateful to the grant of Juan de la Cierva program of the Ministry of Science and Innovation (Spain) and the author Mauricio Zapateiro to the FI Grant of the Department for Innovation, University and Enterprise of the Government of Catalonia (Spain).

REFERENCES

[1] Chen G., ‘Control and Synchronization of Chaos, a Bibliography’ Department of Electrical Engineering, University of Houston, Texas, 1997.

[2] Chen G. and Dong X., ‘On feedback control of chaotic continuous-time systems,’ IEEE Trans. Circuits and Systems, 40, 591–601, 1993.

[3] Pecora L.M. and Carroll T.L., ‘Synchronization in chaotic systems,’ Physical Review Letters, 64, 821–824, 1990.

[4] Kapitaniak T., ‘Continuous control and synchronization in chaotic systems,’ Chaos Solitons and Fractals, 6,237– 244, 1995.

[5] Gao H., Lam J., and Chen G., ‘New criteria for synchronization stability of general complex dynamical networks with coupling delays’ Physics Letters A , 360(2), 263-273, 2006.

[6] Lu H., and van Leeuwen C., ’Synchronization of chaotic neural networks via output or state coupling’ Chaos, Solitons and Fractals, vol. 30, pp. 166-176, 2006. [7] Hou Y. Y., Liao T. L., and Yan J. J., ’H

synchronization of chaotic systems using output feedback control design’ Physics A, vol. 379, pp. 81-89, 2007.

[8] Wen G., Wang Q.G., Lin C., Han X. and Li G., ‘Synthesis for robust synchronization of chaotic systems under output feedback control with multiple random

delays’ Chaos, Solitons & Fractals, 29(5), 1142-1146, 2006.

[9] Liao T. L., and Tsai S. H., ’Adaptive synchronization of chaotic systems and its application to secure communication’ Chaos, Solitons and Fractals, 11(9),1387-1396, 2000.

[10] Feki M., ’An adaptive chaos synchronization scheme applied to secure communication’ Chaos, Solitons and Fractals, 18, 141-148, 2003.

[11] Park J.H., ‘Synchronization of Genesio chaotic system via backstepping approach’ Chaos Solitons and Fractals, 27, 1369–1375, 2006.

[12] Yan J.J., Yang Y.S., Chiang T.Y. and Chen C.Y., ‘Robust synchronization of unified chaotic systems via sliding mode control’ Chaos, Solitons & Fractals, 34(3), 947-954, 2007.

[13] Alvin, K.F., and Park, K.C., ‘Second-order structural identification procedure via state-space-based system identification’ AIAA Journal, 32(2), 397-406, 1994. [14] Friswell, M.I., ‘Extracting second-order systems from

state-space representations’ AIAA Journal, 37(1), 132-135, 1999.

[15] Balas M.J., ‘Trends in large space structure control theory: Fondest hopes, wildest dreams,’ IEEE Trans. Automatic Control, 27, 522–535, Mar. 1982.

[16] Duan G.R., ‘Parametric Eigenstructure Assignment in Second-Order Descriptor Linear Systems’ IEEE Trans. Automatic Control, 49(10), 1789-1795, 2004.

[17] Cook PA., ‘Simple feedback systems with chaotic behavior.’ Syst Contr Lett, 6, 223–7, 1985.

[18] Alvarez J and Veruzco F., ‘Bifurcation and chaos in a PD-controlled pendulum.’ J. Dynam. Syst. Measur. Contr., 120, 146–9, 1998.

[19] Alvarez J, and Curiel LE. ‘Bifurcations and chaos in a linear control system with saturated input.’ Int J Bifurcat Chaos, 7(8), 1811–1822, 1997.

[20] Krasovskii, N.N., ‘Stability of motion.’ Stanford, CA: Stanford University Press, 1963.

[21] Lam, J., Gao, H., and Wang, C., ‘H∞ model reduction of linear systems with distributed delay.’ IEE Proc. Control Theory Appl., 152(6), 662-674, 2005.

[22] Park, P., ‘A delay-dependent stability criterion for systems with uncertain time-invariant delays.’ IEEE Trans. Automatic Control, 44, 876-877, 1999.

[23] Ho D.W.C., and Lu G., ‘Robust stabilization for a class of discrete-time nonlinear via output feedback: the unified LMI approach’ Int. J. Control, 76(2), 105-115, 2003.

[24] Fridman, E., and Shaked, U., ‘A descriptor system approach to Hcontrol of linear time-delay systems.’ IEEE Trans. Automatic control, 47(2), 253-270, 2002.

References

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