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Ma and Li Journal of Inequalities and Applications (2018) 2018:293 https://doi.org/10.1186/s13660-018-1886-5
R E S E A R C H Open Access
Stability criteria on delay-dependentrobust stability for uncertain neutralstochastic nonlinear systems with time-delayTengyu Ma1,2 and Longsuo Li1*
*Correspondence:[email protected] of Mathematics,Harbin Institute of Technology,Harbin, ChinaFull list of author information isavailable at the end of the article
AbstractThis work mainly studies the robust stability analysis and design of a controller foruncertain neutral stochastic nonlinear systems with time-delay. Using a modifiedLyapunovβKrasovskii functional and the free-weighting matrices technique, weestablish some new delay-dependent criteria in terms of linear matrix inequality (LMI).The innovative point of this work is that we generalize the robust stability analysis ofnonlinear stochastic time-delay systems to the uncertain neutral stochastic systems.Due to the added derivative term of time-delay, the proposed scheme can be appliedmore widely. Finally, numerical examples are provided to validate the derived results.
Keywords: Uncertain neutral stochastic systems; One-sided Lipschitz condition;LyapunovβKrasovskii functional; Linear matrix inequality (LMI)
1 IntroductionTime-delay systems are widely used to model concrete systems in engineering sciences,such as biology, chemistry, mechanics [1β3]. Time-delay systems, with the rate of currentstate affected by past state, are negative for the analysis and design of control systemssince they may be responsible for performance degradation and instability [4, 5]. There aremany valuable results about stability conditions for time-delay systems [6β9]. Generally,the delay-dependent stability condition is less conservative than the delay-independentone. Thus, pursuing the delay-dependent stability condition motivates the present study[10β14].
Over the past years, the Brownian motion phenomenon has been common in biol-ogy, economics, and engineering applications. Considerable attention has been devoted tostochastic systems governed by ItΓ΄ stochastic differential equations, where the noises aredescribed by Brownian motion [15, 16]. A large number of works that focused on stochas-tic time-delay systems have been published; see, for example, [17β20]. Wang et al. in [19]considered the problems of non-fragile robust stochastic stabilization and robust Hβ con-trol for uncertain stochastic nonlinear time-delay systems. Both the robust stability anal-ysis and non-fragile robust control for a class of uncertain stochastic nonlinear time-delaysystems that satisfy a one-sided Lipschitz condition were investigated in [17]. Based onthe stochastic LyapunovβKrasovskii stability approach, the problem of stochastic stabilityanalysis was investigated for Hβ control of uncertain stochastic Markovian jump systems
Β© The Author(s) 2018. This article is distributed under the terms of the Creative Commons Attribution 4.0 International License(http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in anymedium, pro-vided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, andindicate if changes were made.
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 2 of 19
(SMJSs) with mixed time-varying delays [18]; meanwhile, some delay-dependent sufficientconditions on the stochastic stability and Ξ³ -disturbance attenuation were presented.
The neutral stochastic systems can effectively model a class of physical dynamical sys-tems, since the mathematical models of them include the time-delays of state and itsderivative. These models have received considerable attention recently [21β25]. In fact,neutral stochastic systems are applied widely in automatic control, aircraft stabilization,lossless transmission lines, and system of turbojet engine [26β28]. Both the stability anal-ysis and synthesis of neutral stochastic systems have been extensively studied [29β36].By using the generalized integral inequality and the nonnegative local martingale conver-gence theorem, the authors in [30] investigated the exponential stability and the almostsure exponential stability of neutral stochastic delay systems (NSDSs) with Markovianswitching. The authors in [33] constructed a new sliding surface functional and consid-ered the Hβ sliding mode control (SMC) for uncertain neutral stochastic systems withMarkovian jumping parameters and time-varying delays. Using a delayed output-feedbackcontrol method, Karimi et al. in [36] designed a controller, which guarantees Hβ synchro-nization of the second-order neutral master and slave systems.
On the other hand, a useful one-sided Lipschitz condition was developed in [37]. Sincethe nonlinear part satisfying this condition can make positive contributions to the stabilityof systems, we can easily solve the observer design problem for nonlinear systems [17, 38β40]. Inspired by the above works, we investigate the robust stability of neutral stochastictime-delay nonlinear systems with one-sided Lipschitz condition.
In this paper, we propose a class of uncertain neutral stochastic nonlinear systems.Since the systems have a derivative term of time-delay of state, they can be used in lotsof fields. We investigate the nonlinear function with both one-sided Lipschitz conditionand a quadratic inner-bounded condition. Firstly, a delay-dependent sufficient conditionis proposed by constructing an appropriate LyapunovβKrasovskii functional based on thefree-weighting matrices method. Secondly, we construct a memory-less non-fragile state-feedback controller to guarantee asymptotical stability of the closed-loop systems. Finally,we present some numerical examples to illustrate the advantages and effectiveness of ourresults and find that the proposed method is less conservative.
The organization of this paper is given as follows. In the next section, we recall somenotations, lemmas, and definitions of stochastic differential equations. In Sect. 3, themain problems are formulated. In Sect. 4, we give two delay-dependent sufficient con-ditions for uncertain neutral stochastic nonlinear time-delay systems. In Sect. 5, we de-sign a memory-less non-fragile state-feedback controller to guarantee that the closed-loopsystems are asymptotically stable, and in Sect. 6, we present two numerical examples todemonstrate the validity of the mentioned method. The last section contains a conclusion.
2 Notations and preliminariesIn this section, we introduce some basic concepts, properties, and notations. These basicfacts can be found in any introductory book on stochastic differential equations; see, forexample, [41β43].
Throughout this paper, let (Ξ© ,F ,P) be a complete probability space with a filtration{Ft}tβ₯0 satisfying the usual conditions (i.e., the filtration contains all P-null sets and isright continuous). B(t) is a one-dimensional Brownian motion defined on the probabilityspace adapted to the filtration. Rn and R
mΓn denote the n-dimensional Euclidean space
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 3 of 19
and the set of all mΓn real matrices, respectively. βΒ·β2 stands for the usual L2[0,β) norm.The inner product of vectors x and y in R
n is denoted by < x, y > or xT y. Let C2,1(Rn ΓR+;R+) denote the family of all real-valued functions V (x(t), t) defined on R
n Γ R+ suchthat they are continuously twice differentiable in x and once in t. C([βΟ , 0];Rn) denotesthe space of all continuous Rn-valued functions Ο defined on [βΟ , 0] with a norm βΟβ =supβΟβ€ΞΈβ€0|Ο(ΞΈ )|. The notation P > 0 means that P is real symmetric and positive definite;the asterisk βββ denotes a matrix that can be inferred by symmetry and the superscriptβTβ represents the transpose of a matrix or a vector. In a matrix, (i, j) denotes an (i, j)-block element of the matrix. The notation E{Β·} represents the mathematical expectationoperator. I denotes the identity matrix of compatible dimension.
Definition 2.1 ([17]) The nonlinear function f (x, y) is said to be one-sided Lipschitz ifthere exist Ξ±1,Ξ±2 βR such that
β¨f (x, y), x
β© β€ Ξ±1xT x + Ξ±2yT y (1)
for βx, y βRn, where constants Ξ±1 and Ξ±2 are positive, zero, or even negative, and they are
called one-sided Lipschitz constants for f (x, y) with respect to x and y.
Definition 2.2 ([17]) The nonlinear function f (x, y) is called quadratic inner-bounded inthe region C if, for any x, y β C, there exist constants Ξ²1, Ξ²2, and Ξ³ such that
f (x, y)T f (x, y) β€ Ξ²1xT x + Ξ²2yT y + Ξ³β¨x, f (x, y)
β©. (2)
Lemma 2.1 (Schur complement [43]) For a given symmetric matrix
S =
[S11 S12
ST12 S22
]
,
the following conditions are equivalent:(1) S < 0,(2) S11 < 0, S22 β ST
12Sβ111 S12 < 0,
(3) S22 < 0, S11 β S12Sβ122 ST
12 < 0.
Lemma 2.2 ([44]) Let E βRn, G βR
n, and Ξ΅ > 0. Then we have
ET G + GT E β€ Ξ΅GT G + Ξ΅β1ET E.
Lemma 2.3 (S-procedure [45]) Denote the set Z = {z}, and let F (z), y1(z), y1(z), . . . , yk(z)be some functions or functionals. Further define the domain D as follows:
D ={
z βZ : y1(z) β₯ 0, y2(z) β₯ 0, . . . , yk(z) β₯ 0}
,
and the two following conditions:(1) F (z) > 0,βz βD,
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 4 of 19
(2) β Ξ΅1 β₯ 0, Ξ΅2 β₯ 0, . . . , Ξ΅k β₯ 0 such that
S(Ξ΅, z) = F (z) βkβ
i=1
Ξ΅iyi(z) > 0, βz βZ .
Then (2) implies (1). The procedure of replacing (1) by (2) is called the S-procedure.
3 Problem formulationConsider the following uncertain neutral stochastic time-delay system described in ItΓ΄βsform:
β§βͺβͺβͺβͺβͺβͺβͺβͺβ¨
βͺβͺβͺβͺβͺβͺβͺβͺβ©
d[x(t) β Cx(t β Ο (t))]
= [(A + A(t))x(t) + (AΟ + AΟ (t))x(t β Ο (t))
+ f (x(t), x(t β Ο (t)) + Uu(t)] dt
+ [(H + H(t))x(t) + (HΟ + HΟ (t))x(t β Ο (t))] dB(t),
x(t) = Ο(t), t β [βΟ , 0],
(3)
where x(t) βRn is the state vector, u(t) βR
p is the control input, and Ο (t) is the unknowntime-varying delay satisfying 0 β€ Ο (t) < Ο and Ο (t) β€ d with real constants Ο , d. f (x(t), x(t βΟ (t))) βR
n is a nonlinear function with respect to the state x(t) and the delayed state x(t βΟ (t)), f (0, 0) = 0. Ο(t) β C([βΟ , 0];Rn) is a continuous vector-valued initial function, andB(t) is a one-dimensional Brownian motion satisfying
E{
dB(t)}
= 0, E{
dB(t)}2 = dt,
in which A, AΟ , C, H , HΟ βRnΓn, and U βR
nΓp are known real constant matrices of appro-priate dimensions. Moreover, A(t), AΟ (t), H(t), and HΟ (t) are unknown matricesrepresenting time-varying parameter uncertainties and are assumed to be of the form
[A(t) AΟ (t)H(t) HΟ (t)
]
=
[E1
E2
]
F(t)[G1 G2
], (4)
where E1, E2, G1, andG2 are known real constant matrices and F(t) is an unknown time-varying matrix function satisfying
FT (t)F(t) β€ I, βt βR+. (5)
The parameter uncertainties A(t), AΟ (t), H(t), and HΟ (t) are said to be admissibleif both (4) and (5) hold [17].
4 Robust stability analysisLet
h(t) = F(t)[G1x(t) + G2x
(t β Ο (t)
)],
h1(t) = Ax(t) + AΟ x(t β Ο (t)
)+ f
(x(t), x
(t β Ο (t)
))+ E1h(t) + Uu(t).
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 5 of 19
System (3) can be rewritten as follows:β§β¨
β©d[x(t) β Cx(t β Ο (t))] = h1(t) dt + [Hx(t) + HΟ x(t β Ο (t)) + E2h(t)] dB(t),
h(t)T h(t) β€ [G1x(t) + G2x(t β Ο (t))]T [G1x(t) + G2x(t β Ο (t))].(6)
We will consider the problem of robust stability for time-varying delay system (6) withu(t) = 0.
Theorem 4.1 Consider the neutral stochastic time-delay system (6) with u(t) = 0. The non-linear function f (x(t), x(t βΟ (t))) satisfies (1) and (2). For given scalars Ο and d, if there existmatrices P > 0, W1 > 0, W2 > 0, R > 0, Mi > 0 (i = 1, . . . , 5), and Nj (j = 1, . . . , 4) of appropri-ate dimensions and positive scalars Ξ΅1, Ξ΅2, Ξ΅3 satisfying the following LMIs:
β‘
β’β’β’β’β’β’β’β’β’β’β’β’β’β’β’β£
Ξ©11 Ξ©12 0 NT2 0 Ξ©16 Ξ©17 AT R M1
β Ξ©22 NT3 Ξ©24 NT
4 βCT P Ξ©27 ATΟ R M2
β β Ξ©33 Ξ©34 Ξ©35 0 0 0 M3
β β β Ξ©44 Ξ©45 0 0 0 M4
β β β β Ξ©55 0 0 0 M5
β β β β β βΞ΅3I 0 R 0β β β β β β Ξ©77 ET
1 R 0β β β β β β β βΟβ1R 0β β β β β β β β βM
β€
β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0, (7)
where
Ξ©11 = PA + AT P + HT PH + W1 + W2 + Ξ΅1GT1 G1 + Ξ΅2Ξ±1I + Ξ΅3Ξ²1I,
Ξ©12 = PAΟ β AT PC + HT PHΟ + NT1 + Ξ΅1GT
1 G2,
Ξ©16 = P β12Ξ΅2I +
12Ξ΅3Ξ³ I, Ξ©17 = PE1 + HT PE2,
Ξ©22 = βCT PAΟ β ATΟ PC + HT
Ο PHΟ β (1 β d)W1
β N1(C + I) β (C + I)T NT1 + Ξ΅1GT
2 G2 + Ξ΅2Ξ±2I + Ξ΅3Ξ²2I,
Ξ©24 = N1C β CT NT2 β NT
2 , Ξ©27 = βCT PE1 + HTΟ PE2
Ξ©33 = βW2 β N3 β NT3 , Ξ©34 = βN3C, Ξ©35 = N3C β NT
4 ,
Ξ©44 = N2C + CT NT2 , Ξ©45 = βCT NT
4 , Ξ©55 = N4C + CT NT4 ,
Ξ©77 = ET2 PE2 β Ξ΅1I, M = diag
{Οβ1M1, Οβ1M2, Οβ1M3, Οβ1M4, Οβ1M5
},
M1 = [M1, 0, 0, 0, 0], M2 = [0, M2, 0, 0, 0], M3 = [0, 0, M3, 0, 0],
M4 = [0, 0, 0, M4, 0], M5 = [0, 0, 0, 0, M5],
Ξ =
β‘
β’β’β’β’β’β’β’β’β£
βM1 0 0 0 0 0β βM2 0 0 0 0β β βM3 0 0 βN3
β β β βM4 0 0β β β β βM5 βN4
β β β β β βR
β€
β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0, (8)
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 6 of 19
Ξ =
β‘
β’β’β’β’β’β’β’β’β£
βM1 0 0 0 0 0β βM2 0 0 0 βN1
β β βM3 0 0 0β β β βM4 0 βN2
β β β β βM5 0β β β β β βR
β€
β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0, (9)
then the null solution of the stochastic time-delay system (6) is asymptotically stable in themean square.
Proof Choose the following LyapunovβKrasovskii functional:
V(x(t), t
)=
4β
i=1
Vi, (10)
where
V1 =[x(t) β Cx
(t β Ο (t)
)]T P[x(t) β Cx
(t β Ο (t)
)], V2 =
β« t
tβΟ (t)xT (s)W1x(s) ds,
V3 =β« t
tβΟ
xT (s)W2x(s) ds, V4 =β« 0
βΟ
β« t
t+ΞΈ
hT1 (s)Rh1(s) ds dΞΈ .
Using ItΓ΄βs formula [41], we obtain the stochastic differential of V (x(t), t) as follows:
dV(x(t), t
)
= LV(x(t), t
)dt + 2
[x(t) β Cx
(t β Ο (t)
)]T P[Hx(t) + HΟ x
(t β Ο (t)
)+ E2h(t)
]dB(t),
={
2[x(t) β Cx
(t β Ο (t)
)]T P[Ax(t) + AΟ x
(t β Ο (t)
)+ f
(x(t), x
(t β Ο (t)
))+ E1h(t)
]
+[Hx(t) + HΟ x
(t β Ο (t)
)+ E2h(t)
]T P[Hx(t) + HΟ x
(t β Ο (t)
)+ E2h(t)
]
+ xT (t)W1x(t) β (1 β Ο (t)xT(t β Ο (t)
)W1x
(t β Ο (t)
)
+ xT (t)W2x(t) β xT (t β Ο )W2x(t β Ο )
+ ΟhT1 (t)Rh1(t) β
β« t
tβΟ
hT1 (s)Rh1(s)ds
}dt
+{
2[x(t) β Cx
(t β Ο (t)
)]T P[Hx(t) + HΟ x
(t β Ο (t)
)+ E2h(t)
]}dB(t). (11)
Taking the expectation of both sides of (11), we have
E dV(x(t), t
)= ELV
(x(t), t
)dt. (12)
Set
xΟ
(t β Ο (t)
) β‘ x(t β Ο (t) β Ο
(t β Ο (t)
)),
xΟ (t β Ο ) β‘ x(t β Ο β Ο (t β Ο )
).
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 7 of 19
Using the NewtonβLeibniz formula and the free-weighting matrices technique, we canderive the following equations:
2[xT(
t β Ο (t))N1 + xT
Ο
(t β Ο (t)
)N2
][x(t) β Cx
(t β Ο (t)
)β x
(t β Ο (t)
)+ CxΟ
(t β Ο (t)
)
ββ« t
tβΟ (t)h1(s) ds β
β« t
tβΟ (t)
(Hx(s) + HΟ x
(s β Ο (s)
)+ E2h(s)
)dB(s)
]= 0, (13)
2[xT (t β Ο )N3 + xT
Ο (t β Ο )N4][
x(t β Ο (t)
)β CxΟ
(t β Ο (t)
)β x(t β Ο ) + CxΟ (t β Ο )
ββ« tβΟ (t)
tβΟ
h1(s) ds ββ« tβΟ (t)
tβΟ
(Hx(s) + HΟ x
(s β Ο (s)
)+ E2h(s)
)dB(s)
]= 0, (14)
where Nj (j = 1, . . . , 4) are arbitrary matrices with appropriate dimensions. Using the prop-erties of the stochastic integral [41], we have
E{[
xT(t β Ο (t)
)N1 + xT
Ο
(t β Ο (t)
)N2
] β« t
tβΟ (t)
(Hx(s) + HΟ x
(s β Ο (s)
)+ E2h(s)
)dB(s)
}= 0,
E{[
xT (t β Ο )N3 + xΟ (t β Ο )NT4] β« tβΟ (t)
tβΟ
(Hx(s) + HΟ x
(s β Ο (s)
)+ E2h(s)
)dB(s)
}= 0.
Adding the left-hand sides of (13) and (14) onto LV (x(t), t), (12) is transformed to
E dV(x(t), t
)= ELV
(x(t), t
)dt, (15)
where
LV(x(t), t
)
= LV(x(t), t
)+ 2
[xT(
t β Ο (t))N1 + xT
Ο
(t β Ο (t)
)N2
][x(t)
β Cx(t β Ο (t)
)β x
(t β Ο (t)
)+ CxΟ
(t β Ο (t)
)β
β« t
tβΟ (t)h1(s) ds
]
+ 2[xT (t β Ο )N3 + xT
Ο (t β Ο )N4]
Γ[
x(t β Ο (t)
)β CxΟ
(t β Ο (t)
)β x(t β Ο ) + CxΟ (t β Ο ) β
β« tβΟ (t)
tβΟ
h1(s) ds]
. (16)
For Ο (t) β€ d, we have
LV(x(t), t
)
= LV(x(t), t
)+ 2
[xT(
t β Ο (t))N1 + xT
Ο
(t β Ο (t)
)N2
][x(t)
β Cx(t β Ο (t)
)β x
(t β Ο (t)
)+ CxΟ
(t β Ο (t)
)β
β« t
tβΟ (t)z(s) ds
]
+ 2[xT (t β Ο )N3 + xT
Ο (t β Ο )N4]
Γ[
x(t β Ο (t)
)β CxΟ
(t β Ο (t)
)β x(t β Ο ) + CxΟ (t β Ο ) β
β« tβΟ (t)
tβΟ
h1(s) ds]
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 8 of 19
β€{
2[x(t) β Cx
(t β Ο (t)
)]T P[Ax(t) + AΟ x
(t β Ο (t)
)+ f
(x(t), x
(t β Ο (t)
))
+ E1h(t)]
+[Hx(t) + HΟ x
(t β Ο (t)
)+ E2h(t)
]T P
Γ [Hx(t) + HΟ x
(t β Ο (t)
)+ E2h(t)
]+ xT (t)W1x(t)
β (1 β d)xT(t β Ο (t)
)W1x
(t β Ο (t)
)+ xT (t)W2x(t)
β xT (t β Ο )W2x(t β Ο ) + ΟhT1 (t)Rh1(t) β
β« tβΟ (t)
tβΟ
hT1 (s)Rh1(s) ds
ββ« t
tβΟ (t)hT
1 (s)Rh1(s) ds}
+ 2[xT(
t β Ο (t))N1 + xT
Ο
(t β Ο (t)
)N2
]
Γ[
x(t) β Cx(t β Ο (t)
)β x
(t β Ο (t)
)+ CxΟ
(t β Ο (t)
)β
β« t
tβΟ (t)h1(s) ds
]
+ 2[xT (t β Ο )N3 + xT
Ο (t β Ο )N4]
Γ[
x(t β Ο (t)
)β CxΟ
(t β Ο (t)
)β x(t β Ο ) + CxΟ (t β Ο ) β
β« tβΟ (t)
tβΟ
h1(s) ds]
. (17)
On the other hand, by using the one-sided Lipschitz (1) and the quadratically inner-bounded condition (2), we obtain the following inequalities:
Ξ±1xT (t)x(t) + Ξ±2xT(t β Ο (t)
)x(t β Ο (t)
)β xT (t)f
(x(t), x
(t β Ο (t)
)) β₯ 0, (18)
Ξ²1xT (t)x(t) + Ξ²2xT(t β Ο (t)
)x(t β Ο (t)
)β f
(x(t), x
(t β Ο (t)
))T f(x(t), x
(t β Ο (t)
))
+ Ξ³ xT (t)f(x(t), x
(t β Ο (t)
)) β₯ 0. (19)
Using the S-procedure in (17), we obtain that LV (x(t), t) < 0 is satisfied if there existpositive scalars Ξ΅1, Ξ΅2, Ξ΅3 satisfying
LV(x(t), t
)+ Ξ΅1
[G1x(t) + G2x
(t β Ο (t)
)]T[G1x(t) + G2x
(t β Ο (t)
)]β Ξ΅1h(t)T h(t)
+ Ξ΅2Ξ±1xT (t)x(t) + Ξ΅2Ξ±2xT(t β Ο (t)
)x(t β Ο (t)
)β Ξ΅2xT (t)f
(x(t), x
(t β Ο (t)
))
+ Ξ΅3Ξ²1xT (t)x(t) + Ξ΅3Ξ²2xT(t β Ο (t)
)x(t β Ο (t)
)β Ξ΅3f
(x(t), x
(t β Ο (t)
))T
Γ f(x(t), x
(t β Ο (t)
))+ Ξ΅3Ξ³ xT (t)f
(x(t), x
(t β Ο (t)
))< 0. (20)
Moreover, the following formula holds for any positive definite matrix M1(M2, . . . , M5)of appropriate dimensions:
ΟxT (t)M1x(t) ββ« t
tβΟ
xT (t)M1x(t) ds = 0. (21)
We can decompose the integration interval [t βΟ , t] into two subintervals that are [t βΟ , t βΟ (t)] and [t β Ο (t), t], and let
ΞΎT (t) =[xT (t)xT(
t β Ο (t))xT (t β Ο )xT
Ο
(t β Ο (t)
)xT
Ο (t β Ο )f T(x(t), x
(t β Ο (t)
))hT (t)
],
Ξ·T (t, s) =[xT (t)xT(
t β Ο (t))xT (t β Ο )xT
Ο
(t β Ο (t)
)xT
Ο (t β Ο )hT1 (s)
].
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 9 of 19
Combining the above formula (21) and rearranging (20), we have the following inequality:
ΞΎT (t)Ωξ (t) + ΟhT1 (t)Rh1(t)
+β« tβΟ (t)
tβΟ
Ξ·T (t, s)ΞΞ·(t, s) ds +β« t
tβΟ (t)Ξ·T (t, s)Ξ Ξ·(t, s) ds < 0, (22)
where
Ξ© =
β‘
β’β’β’β’β’β’β’β’β’β’β’β£
Ξ©11 Ξ©12 0 NT2 0 Ξ©16 PE1 + HT PE2
β Ξ©22 NT3 Ξ©24 NT
4 βCT P βCT PE1 + HTΟ PE2
β β Ξ©33 Ξ©34 Ξ©35 0 0β β β Ξ©44 Ξ©45 0 0β β β β Ξ©55 0 0β β β β β βΞ΅3I 0β β β β β β ET
2 PE2 β Ξ΅1I
β€
β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0, (23)
Ξ =
β‘
β’β’β’β’β’β’β’β’β£
βM1 0 0 0 0 0β βM2 0 0 0 0β β βM3 0 0 βN3
β β β βM4 0 0β β β β βM5 βN4
β β β β β βR
β€
β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0,
Ξ =
β‘
β’β’β’β’β’β’β’β’β£
βM1 0 0 0 0 0β βM2 0 0 0 βN1
β β βM3 0 0 0β β β βM4 0 βN2
β β β β βM5 0β β β β β βR
β€
β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0.
Ξ©11 = PA + AT P + HT PH + W1 + W2 + Ξ΅1GT1 G1 + ΟM1 + Ξ΅2Ξ±1I + Ξ΅3Ξ²1I,
Ξ©12 = PAΟ β AT PC + HT PHΟ + NT1 + Ξ΅1GT
1 G2,
Ξ©16 = P β12Ξ΅2I +
12Ξ΅3Ξ³ I,
Ξ©22 = βCT PAΟ β ATΟ PC + HT
Ο PHΟ β (1 β d)W1 β N1(C + I) β (C + I)T NT1
+ Ξ΅1GT2 G2 + ΟM2 + Ξ΅2Ξ±2I + Ξ΅3Ξ²2I,
Ξ©24 = N1C β CT NT2 β NT
2 ,
Ξ©33 = βW2 + ΟM3 β N3 β NT3 ,
Ξ©34 = βN3C,
Ξ©35 = N3C β NT4 ,
Ξ©44 = N2C + CT NT2 + ΟM4,
Ξ©45 = βCT NT4 ,
Ξ©55 = N4C + CT NT4 + ΟM5.
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 10 of 19
Utilizing the Schur complement Lemma 2.1, (23) is equivalent to the following LMI:
Ξ© =
β‘
β’β’β’β’β’β’β’β’β’β’β’β’β’β’β’β£
Ξ©11 Ξ©12 0 NT2 0 Ξ©16 Ξ©17 AT M1
β Ξ©22 NT3 Ξ©24 NT
4 βCT P Ξ©27 ATΟ M2
β β Ξ©33 Ξ©34 Ξ©35 0 0 0 M3
β β β Ξ©44 Ξ©45 0 0 0 M4
β β β β Ξ©55 0 0 0 M5
β β β β β βΞ΅3I 0 I 0β β β β β β Ξ©77 ET
1 0β β β β β β β βΟβ1Rβ1 0β β β β β β β β βM
β€
β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0, (24)
Ξ©11 = PA + AT P + HT PH + W1 + W2 + Ξ΅1GT1 G1 + Ξ΅2Ξ±1I + Ξ΅3Ξ²1I,
Ξ©12 = PAΟ β AT PC + HT PHΟ + NT1 + Ξ΅1GT
1 G2,
Ξ©16 = P β12Ξ΅2I +
12Ξ΅3Ξ³ I, Ξ©17 = PE1 + HT PE2,
Ξ©22 = βCT PAΟ β ATΟ PC + HT
Ο PHΟ β (1 β d)W1
β N1(C + I) β (C + I)T NT1 + Ξ΅1GT
2 G2 + Ξ΅2Ξ±2I + Ξ΅3Ξ²2I,
Ξ©24 = N1C β CT NT2 β NT
2 , Ξ©27 = βCT PE1 + HTΟ PE2,
Ξ©33 = βW2 β N3 β NT3 Ξ©34 = βN3C, Ξ©35 = N3C β NT
4 ,
Ξ©44 = N2C + CT NT2 , Ξ©45 = βCT NT
4 , Ξ©55 = N4C + CT NT4 ,
Ξ©77 = ET2 PE2 β Ξ΅1I, M = diag
{Οβ1M1, Οβ1M2, Οβ1M3, Οβ1M4, Οβ1M5
},
M1 = [M1, 0, 0, 0, 0], M2 = [0, M2, 0, 0, 0], M3 = [0, 0, M3, 0, 0],
M4 = [0, 0, 0, M4, 0], M5 = [0, 0, 0, 0, M5].
Pre-and post-multiplying (24) by diag{I, I, I, I, I, I, I, R, I}, we obtain LMI (7). Combiningwith Ξ < 0 and Ξ < 0, we find that ELV (ΞΎ (t), t) < 0, i.e., it guarantees the asymptotic sta-bility of system (6) in the mean square. οΏ½
If the uncertain parameters A(t), AΟ (t), H(t), and HΟ (t) in system (6) are equalto zero, the system is simplified to the following deterministic stochastic system:
β§βͺβͺβͺβͺβͺβ¨
βͺβͺβͺβͺβͺβ©
d[x(t) β Cx(t β Ο (t))]
= [Ax(t) + AΟ x(t β Ο (t)) + f (x(t), x(t β Ο (t)) + Uu(t)] dt
+ [Hx(t) + HΟ x(t β Ο (t))] dB(t),
x(t) = Ο(t), t β [βΟ , 0].
(25)
The following conclusion of the robust asymptotic stability is obtained by Theorem 4.1for the deterministic stochastic system (25).
Corollary 4.1 Consider the stochastic time-delay system (25). The nonlinear functionf (x(t), x(t β Ο (t))) satisfies (1) and (2). For given scalars Ο and d, if there exist matrices
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 11 of 19
P > 0, W1 > 0, W2 > 0, R > 0, Mi > 0 (i = 1, . . . , 5), and matrices Nj (j = 1, . . . , 4) of appropri-ate dimensions and positive scalars Ξ΅1, Ξ΅2, Ξ΅3 satisfying the following LMIs:
β‘
β’β’β’β’β’β’β’β’β’β’β’β’β’β£
Ξ©11 Ξ©12 0 NT2 0 Ξ©16 AT R M1
β Ξ©22 NT3 Ξ©24 NT
4 βCT P ATΟ R M2
β β Ξ©33 βN3C Ξ©35 0 0 M3
β β β Ξ©44 βCT NT4 0 0 M4
β β β β Ξ©55 0 0 M5
β β β β β βΞ΅3I R 0β β β β β β βΟβ1R 0β β β β β β β βM
β€
β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0, (26)
where
Ξ©11 = PA + AT P + HT PH + W1 + W2 + Ξ΅2Ξ±1I + Ξ΅3Ξ²1I,
Ξ©12 = PAΟ β AT PC + HT PHΟ + NT1 , Ξ©16 = P β
12Ξ΅2I +
12Ξ΅3Ξ³ I,
Ξ©22 = βCT PAΟ β ATΟ PC + HT
Ο PHΟ β (1 β d)W1
β N1(C + I) β (C + I)T NT1 + Ξ΅2Ξ±2I + Ξ΅3Ξ²2I,
Ξ©24 = N1C β CT NT2 β NT
2 , Ξ©33 = βW2 β N3 β NT3 ,
Ξ©35 = N3C β NT4 , Ξ©44 = N2C + CT NT
2 , Ξ©55 = N4C + CT NT4 ,
M = diag{Οβ1M1, Οβ1M2, Οβ1M3, Οβ1M4, Οβ1M5
},
M1 = [M1, 0, 0, 0, 0], M2 = [0, M2, 0, 0, 0], M3 = [0, 0, M3, 0, 0],
M4 = [0, 0, 0, M4, 0], M5 = [0, 0, 0, 0, M5],
Ξ =
β‘
β’β’β’β’β’β’β’β’β£
βM1 0 0 0 0 0β βM2 0 0 0 0β β βM3 0 0 βN3
β β β βM4 0 0β β β β βM5 βN4
β β β β β βR
β€
β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0, (27)
Ξ =
β‘
β’β’β’β’β’β’β’β’β£
βM1 0 0 0 0 0β βM2 0 0 0 βN1
β β βM3 0 0 0β β β βM4 0 βN2
β β β β βM5 0β β β β β βR
β€
β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0, (28)
the null solution of the stochastic time-delay system (25) is asymptotically stable in themean square.
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 12 of 19
5 Non-fragile robust state feedback controller designIn this section, we consider the design of a non-fragile state-feedback controller:
u(t) = K(t)x(t) =(K + K(t)
)x(t), (29)
guaranteeing the robust stability for the closed-loop system (3). K is the controller gain,and K(t) represents the gain perturbations with the following assumption:
K(t) = E3F(t)G3, (30)
where E3 and G3 are given real constant matrices with appropriate dimensions.
Theorem 5.1 Consider the stochastic time-delay system (6). The nonlinear functionf (x(t), x(t β Ο (t))) satisfies (1) and (2). For given scalars Ο and d, if there exist matricesP > 0, W1 > 0, W2 > 0, R > 0, Mi > 0 (i = 1, . . . , 5), and matrices Nj (j = 1, . . . , 4) of appropri-ate dimensions and positive scalars Ξ΅1, Ξ΅2, Ξ΅3, Ξ΅4, and Ο satisfying the following LMIs:
β‘
β’β’β’β’β’β’β’β’β’β’β’β’β’β’β’β’β’β’β’β’β£
Ξ©11 Ξ©12 0 NT2 0 Ξ©16 Ξ©17 AT R M1 J1 0
β Ξ©22 NT3 Ξ©24 NT
4 βCT P Ξ©27 ATΟ R M2 0 0
β β Ξ©33 Ξ©34 Ξ©35 0 0 0 M3 0 0β β β Ξ©44 Ξ©45 0 0 0 M4 0 0β β β β Ξ©55 0 0 0 M5 0 0β β β β β βΞ΅3I 0 R 0 0 0β β β β β β Ξ©77 ET
1 R 0 0 0β β β β β β β βΟβ1R 0 0 L1
β β β β β β β β βM 0 0β β β β β β β β β βJ 0β β β β β β β β β β βL
β€
β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0, (31)
Ξ =
β‘
β’β’β’β’β’β’β’β’β£
βM1 0 0 0 0 0β βM2 0 0 0 0β β βM3 0 0 βN3
β β β βM4 0 0β β β β βM5 βN4
β β β β β βR
β€
β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0, (32)
Ξ =
β‘
β’β’β’β’β’β’β’β’β£
βM1 0 0 0 0 0β βM2 0 0 0 βN1
β β βM3 0 0 0β β β βM4 0 βN2
β β β β βM5 0β β β β β βR
β€
β₯β₯β₯β₯β₯β₯β₯β₯β¦
< 0, (33)
where
Ξ©11 = PA + AT P + HT PH + W1 + W2 + Ξ΅1GT1 G1 + Ξ΅2Ξ±1I + Ξ΅3Ξ²1I + 2Ξ΅4GT
3 G3,
Ξ©12 = PAΟ β AT PC + HT PHΟ + NT1 + Ξ΅1GT
1 G2,
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 13 of 19
Ξ©16 = P β12Ξ΅2I +
12Ξ΅3Ξ³ I,
Ξ©17 = PE1 + HT PE2,
Ξ©22 = βCT PAΟ β ATΟ PC + HT
Ο PHΟ β (1 β d)W1 β N1C β CT NT1 β N1
β NT1 + Ξ΅1GT
2 G2 + Ξ΅2Ξ±2I + Ξ΅3Ξ²2I,
Ξ©24 = N1C β CT NT2 β NT
2 ,
Ξ©27 = βCT PE1 + HTΟ PE2, Ξ©33 = βW2 β NT
3 β N3, Ξ©34 = βN3C,
Ξ©35 = N3C β NT4 , Ξ©44 = N2C + CT NT
2 , Ξ©45 = βCT NT4 ,
Ξ©55 = N4C + CT NT4 , Ξ©77 = ET
2 PE2 β Ξ΅1I,
M = diag{Οβ1M1, Οβ1M2, Οβ1M3, Οβ1M4, Οβ1M5
},
M1 = [M1, 0, 0, 0, 0], M2 = [0, M2, 0, 0, 0], M3 = [0, 0, M3, 0, 0],
M4 = [0, 0, 0, M4, 0], M5 = [0, 0, 0, 0, M5], J = diag
{12Ο I, Ξ΅4I,Ο I
},
J1 = [PU , PUE3, PU], L = diag{Ξ΅4I,Ο I}, L1 = [RUE3, RU],
the closed-loop systems are asymptotically stable in the mean square with the non-fragilestate-feedback controller K = Ο β1BT P.
Proof By using the controller K = Ο β1UT P and letting
h1(t) =(A + U
(K + K(t)
))x(t) + AΟ x
(t β Ο (t)
)+ f
(x(t), x
(t β Ο (t)
))+ E1h(t),
system (6) can be rewritten as follows:
β§βͺβͺβ¨
βͺβͺβ©
d[x(t) β Cx(t β Ο (t))]
= h1(t) dt + [Hx(t) + HΟ x(t β Ο (t)) + E2h(t)] dB(t),
h(t)T h(t) β€ [G1x(t) + G2x(t β Ο (t))]T [G1x(t) + G2x(t β Ο (t))].
(34)
Similar to Theorem 4.1, ELV (ΞΎ (t), t) < 0 is guaranteed by the following matrix inequalityΞ© < 0:
Ξ© =
β‘
β’β’β’β’β’β’β’β’β’β’β’β’β’β’β’β£
Ξ©11 Ξ©12 0 NT2 0 Ξ©16 Ξ©17 Ξ©18 M1
β Ξ©22 NT3 Ξ©24 NT
4 CT P Ξ©27 ATΟ M2
β β Ξ©33 βN3C Ξ©35 0 0 0 M3
β β β Ξ©44 βCT NT4 0 0 0 M4
β β β β Ξ©55 0 0 0 M5
β β β β β βΞ΅3I 0 I 0β β β β β β Ξ©77 ET
1 0β β β β β β β βΟβ1Rβ1 0β β β β β β β β βM
β€
β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β¦
,
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 14 of 19
where
Ξ©11 = P(A + UK) + (A + UK)T P + HT PH + W1 + W2 + Ξ΅1GT1 G1
+ Ξ΅2Ξ±1I + Ξ΅3Ξ²1I + PUE3F(t)G3 + GT3 FT (t)ET
3 UT P,
Ξ©12 = PAΟ β AT PC + HT PHΟ + NT1 + Ξ΅1GT
1 G2,
Ξ©16 = P β12Ξ΅2I +
12Ξ΅3Ξ³ I,
Ξ©17 = PE1 + HT PE2,
Ξ©18 = AT R + KT UT R + G3FT (t)ET3 UT R,
Ξ©22 = βCT PAΟ β ATΟ PC + HT
Ο PHΟ β (1 β d)W1 β N1C β CT NT1 β N1 β NT
1
+ Ξ΅1GT2 G2 + Ξ΅2Ξ±2I + Ξ΅3Ξ²2I,
Ξ©24 = N1C β CT NT2 β NT
2 ,
Ξ©27 = βCT PE1 + HTΟ PE2, Ξ©33 = βW2 β NT
3 β N3, Ξ©35 = N3C β NT4 ,
Ξ©44 = N2C + CT NT2 , Ξ©55 = N4C + CT NT
4 , Ξ©77 = ET2 PE2 β Ξ΅1I
M = diag{Οβ1M1, Οβ1M2, Οβ1M3, Οβ1M4, Οβ1M5
},
M1 = [M1, 0, 0, 0, 0], M2 = [0, M2, 0, 0, 0], M3 = [0, 0, M3, 0, 0],
M4 = [0, 0, 0, M4, 0], M5 = [0, 0, 0, 0, M5].
According to condition (30), we have
Ξ© = Ξ© + EFG + GT FT ET + K R + RT KT ,
where
Ξ© =
β‘
β’β’β’β’β’β’β’β’β’β’β’β’β’β’β’β£
Ξ©11 Ξ©12 0 NT2 0 Ξ©16 Ξ©17 AT R M1
β Ξ©22 NT3 Ξ©24 NT
4 βCT P Ξ©27 ATΟ M2
β β Ξ©33 βN3C N3C β NT4 0 0 0 M3
β β β Ξ©44 Ξ©45 0 0 0 M4
β β β β Ξ©55 0 0 0 M5
β β β β β βΞ΅3I 0 I 0β β β β β β Ξ©77 ET
1 0β β β β β β β βΟβ1Rβ1 0β β β β β β β β βM
β€
β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β₯β¦
,
where
Ξ©11 = P(A + UK) + (A + UK)T P + HT PH + W1 + W2 + Ξ΅1GT1 G1 + Ξ΅2Ξ±1I + Ξ΅3Ξ²1I,
Ξ©12 = PAΟ β AT PC + HT PHΟ + NT1 + Ξ΅1GT
1 G2,
Ξ©16 = P β12Ξ΅2I +
12Ξ΅3Ξ³ I, Ξ©17 = PE1 + HT PE2,
Ξ©22 = βCT PAΟ β ATΟ PC + HT
Ο PHΟ β (1 β d)W1 β N1C β CT NT1 β N1 β NT
1
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 15 of 19
+ Ξ΅1GT2 G2 + Ξ΅2Ξ±2I + Ξ΅3Ξ²2I,
Ξ©24 = N1C β CT NT2 β NT
2 ,
Ξ©27 = βCT PE1 + HTΟ PE2,
Ξ©33 = βW2 β NT3 β N3,
Ξ©44 = N2C + CT NT2 ,
Ξ©45 = βCT NT4 ,
Ξ©55 = N4C + CT NT4 ,
Ξ©77 = ET2 PE2 β Ξ΅1I,
M = diag{Οβ1M1, Οβ1M2, Οβ1M3, Οβ1M4, Οβ1M5
}, M1 = [M1, 0, 0, 0, 0],
M2 = [0, M2, 0, 0, 0], M3 = [0, 0, M3, 0, 0],
M4 = [0, 0, 0, M4, 0], M5 = [0, 0, 0, 0, M5].
Other notations are defined by (28), and E = {(PUE3)1,1, (RUE3)8,2} denotes a block matrixwith appropriate dimensions whose all nonzero blocks are the (1, 1)-block PUE3, the (8, 2)-block RUE3, and all other blocks are zero matrices. Similarly, G = {(G3)1,1, (G3)2,1}, K ={(KT )1,1}, R = {(UT R)1,8}. According to Lemma 2.2, for any scalars Ξ΅4 > 0 and Ο > 0, wehave
Ξ© < Ξ© + Ξ΅β14 EET + Ξ΅4GT G + Ο KKT + Ο β1RT R. (35)
Let K = Ο β1UT P, using the Schur Lemma 2.1, we arrive at
Ξ© + Ξ΅β14 EET + Ξ΅4GT G + Ο KKT + Ο β1RT R < 0
if LMI (31) is satisfied. οΏ½
6 Two illustrative numerical examplesIn order to illustrate the flexibility and reduced conservativeness of the proposed results,we present two numerical examples in this section.
Example 6.1 [17] Consider the neutral stochastic time-delay nonlinear system (25) with
A =
[β1.2 0.1β0.1 β1
]
, AΟ =
[β0.6 0.7β1 β0.8
]
,
and the following nonlinear function that satisfies the one-sided Lipschitz (1) and thequadratically innerbounded conditions (2):
f(x(t), x
(t β Ο (t)
))=
[0.1
sin2(x2β2)x1(tβΟ (t))0.1
sin1(x1β2)x2(tβΟ (t))
]
,
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 16 of 19
with Ξ±1 = 0.5, Ξ±2 = 0.005, Ξ³ = 5,Ξ²1 = β2.5, Ξ²2 = β0.015 (see [17]). We consider the coeffi-cient matrix C as follows:
C =
[β0.1 0.09
β0.02 β1
]
.
By Corollary 4.1, we can obtain the allowable upper bound of the time-delay Ο = 3.0345 forthe above systems, which is greater than the previous result (the allowable upper boundΟ = 2.2487 in [17]). Comparing the allowable values of the systems, we see that our resultare less conservative. Since our system considers neutral stochastic systems with deriva-tives of state time-delay, our results may have more extensive applications.
Example 6.2 Consider the uncertain neutral stochastic nonlinear time-delay system (3)with
A =
[β2.0 0.00.0 β0.9
]
, AΟ =
[β1.0 0.0β1.0 β1.0
]
,
C =
[0.05 00.1 0.05
]
, B =
[12
]
,
H =
[β0.3 0.10.1 0.2
]
, HΟ =
[β0.2 0.20.3 β0.2
]
,
E1 =
[0.2 00 0.2
]
, E2 =
[0.2 00 0.2
]
, E3 =[0.2 0.2
],
G1 =
[0.2 00 0.2
]
, G2 =
[0.2 00 0.2
]
, G3 =
[0.2 00 0.2
]
.
Selecting the same nonlinear function f (x(t), x(t β Ο (t))) as Example 6.1 and lettingd = 1.1, we solve LMIs (31), (32), and (33) to obtain the allowable bound Ο = 3.2106. Hence,for any time-delay Ο satisfying 0 < Ο β€ 3.2106, there exists a non-fragile state-feedbackcontroller such that the closed-loop systems are asymptotically stable in the mean square.For this example, if we choose the time-delay as Ο = 2, according to Theorem 5.1, we canobtain a set of solutions as follows:
P =
[4.4021 β0.9004
β0.9004 0.8275
]
,
W1 =
[1.6119 β0.0127
β0.0127 2.6697
]
, W2 =
[28.4346 β0.5875β0.5875 28.2063
]
,
R =
[1.8078 β0.6499
β0.6499 0.8340
]
,
N1 =
[β0.0561 β0.1719β0.1719 0.0351
]
, N2 =
[β0.0367 β0.0039β0.0039 β0.0085
]
,
N3 =
[β0.0114 β0.1333β0.1333 0.0285
]
, N4 =
[β0.0190 β0.0003β0.0003 β0.0034
]
,
Ma and Li Journal of Inequalities and Applications (2018) 2018:293 Page 17 of 19
M1 =
[9.9084 β0.2109
β0.2109 10.0265
]
, M2 =
[0.4494 0.01970.0197 0.8863
]
,
M3 =
[10.1539 β0.1770β0.1770 10.2906
]
, M4 =
[0.0014 0.00040.0004 0.0003
]
,
M5 = 1.0 Γ 10β3
[0.4711 0.08750.0875 0.0850
]
,
Ξ΅1 = 8.9466, Ξ΅2 = 1.0763 Γ 103, Ξ΅3 = 255.2072, Ξ΅4 = 29.2135,
Ο = 38.2553,
and the desired state-feedback matrix K = Ο β1BT P = [0.0680 0.0197].
7 ConclusionsIn this work, the robust stability has been investigated for neutral stochastic time-delaysystems with disturbance, uncertainties, and one-sided Lipschitz nonlinearity. The para-metric uncertainties are assumed to be time-varying and norm bounded. Firstly, the al-lowable upper bound of time-delay has been obtained, which is a less conservative result.Secondly, based on Lyapunov stability, a novel non-fragile state-feedback controller hasbeen designed to guarantee the robust stability of the closed-loop systems. Finally, twonumerical examples have been given to illustrate the effectiveness of the proposed controlscheme.
AcknowledgementsThe authors would like to express their deep gratitude to the referee for his/her careful reading and invaluable comments.
FundingMaβs work was supported by the Fundamental Research Funds in Heilongjiang Provincial Universities (Nos. 135209246and 135209259). In the first funder (No. 135209246), the first author was the first participant and undertook thetheoretical proof of the work; in the second funder (No. 135209259), the first author was the fourth participant who hasundertaken the numerical simulation of this work. Maβs work was also supported by the Science and TechnologyPlanning Project Fund of Qiqihar (No. GYGG-201718). Liβs work was supported by the National Natural Science Foundationof China (No. 61873071).
Competing interestsThe authors declare that they have no competing interests.
Authorsβ contributionsTM carried out the robust stability analysis and synthesis in this work. LL participated in the design and coordination andhelped to analyze the manuscript. All authors read and approved the final manuscript.
Author details1Department of Mathematics, Harbin Institute of Technology, Harbin, China. 2Department of Mathematics, QiqiharUniversity, Qiqihar, China.
Publisherβs NoteSpringer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Received: 29 May 2018 Accepted: 18 October 2018
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