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R E S E A R C H

Open Access

New results on reachable set bounding for

linear time delay systems with polytopic

uncertainties via novel inequalities

Hao Chen

1,2*

and Shouming Zhong

2

*Correspondence: [email protected]

1School of Mathematical Sciences, Huaibei Normal University, Huaibei, 235000, China

2School of Mathematical Sciences, University of Electronic Science and Technology of China, Chengdu, 611731, China

Abstract

This work is further focused on analyzing a bound for a reachable set of linear uncertain systems with polytopic parameters. By means of L-K functional theory and novel inequalities, some new conditions which are expressed in the form of LMIs are derived. It should be noted that novel inequalities can improve upper bounds of Jensen inequalities, which yields less conservatism of systems. Consequently, some numerical examples demonstrate that the authors’ results are somewhat more effective and advantageous compared with the previous results.

Keywords: reachable set; polytopic uncertainties; Lyapunov-Krasovskii (L-K) functional; linear matrix inequality (LMI)

1 Introduction

It is well known that reachable set estimation was first researched in the late s for state estimations. The reachable set is a hot issue since the time due to its important and wide application in the design of controller and aircraft collision avoidance and peak-to-peak gain minimization problems. The reachable set of dynamic differential systems with delay and disturbance is a set that contains all the reachable trajectories from origin by outside peak input values [–]. In the real world, as for dynamic systems, there are two phenomena that cannot be avoided: time delays and uncertainties [–]. In fact, delays and the coefficients of differential equations in modeling progresses are obtained only ap-proximately [–]. There are already some relevant outstanding results about reachable set estimation of dynamic systems. However, we think it is necessary to obtain a more tighter bound for a reachable set.

As pointed out in [–], an equation of one class can be transformed to an equation belonging to the external form of the other class. Thus, it is natural to classify the equa-tions according to the properties of operators generated by the equaequa-tions. In this paper, uncertain polytopic delayed linear systems with disturbances will be studied.

All the results about reachable set bounding are in the term of linear matrix inequali-ties (LMIs). The authors give an ellipsoid condition of the reachable set for linear systems without any delay []. The authors Fridman and Shaked improved the model []. They studied the linear systems with varying delays with peak inputs and got LMIs conditions of an ellipsoid by using the Razumikhin theory. After that, Kim got a more exact condition

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by constructing the modified Lyapunov-Razumikhin functionals []. Combining the de-composition technique, Nam derived a modified reachable set bound []. Actually, the reachable set is not an ellipsoid and it is only a closed set. Zuo et al. gave a non-ellipsoidal bound of a reachable set for linear time-delayed systems by the means of the maximal Lyapunov functionals and the Razumikhin method [].

It should be noted that discrete delay is varying ≤τ(t)≤τin most previous literature. That is, the lower bound of discrete delay is . In fact,τ(t) varyingτmτ(t)≤τM may

describe the delay more exactly. In order to control the behavior of the system better, we hope to propose tighter reachable set estimation. Park, Lee and Lee proposed some novel inequalities which can be used to estimate integrations []. Therefore, those inequalities can be employed to estimate some integration terms of Lyapunov functionals for dynamic systems. Motivated by the above mentioned discussions, we consider the linear time-varying delay systems with polytopic uncertainties. Using novel inequalities, we derive a modified reachable set bound for the linear system with discrete delayτmτ(t)≤τM.

Moreover, four examples are given to demonstrate the effectiveness and advantage of our results.

In this paper, the used notations are listed as follows. Real matrixP>  (≥) denotes thatPis a symmetric positive definite matrix (positive semi-definite). Superscript ‘T’ is transposition of a vector and a matrix;∗means the elements below the main diagonal in a symmetric block matrix;Iis an identity matrix; ‘–’ in tables means that there is no feasible solution for linear matrix inequalities.

2 Preliminaries

Consider uncertain polytopic delayed linear systems with disturbances in the form

˙

z(t) = (A+A)z(t) + (D+D)ztτ(t)+ (B+B)w(t),

z(t) = , t∈[–τM, ],

()

wherez(t)Rnis a state vector;w(t)Rmis outside disturbance.A,ARn×n,D,DRn×n,B,BRn×m.A,D,Bare known matrices.A,D,Bare uncertain matrices.τ(t)

is time delay.

Discrete delayτ(t) and disturbancew(t) are assumed to be as follows:

τmτ(t)≤τM, ≤ ˙τ(t)≤μ< ,

wT(t)w(t)≤wm, whereμ,wmare constant.

The uncertainty parameter matrices are expressed by a linear convex-hull of matrices Ai,BiandDi

A=

N

i=

θi(t)Ai, B= N

i=

θi(t)Bi, D= N

i=

θi(t)Di

withθi(t)∈[, ] and

N

i=θi(t) = ,∀t> .Ai,BiandDiare known matrices.

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Lemma ([]) As for the well-defined integralab((tt))f(t,s)ds,the following relation known as the Leibniz rule holds:

d dt

b(t)

a(t)

f(t,s)ds=b(t)f˙ t,b(t)a(t)f˙ t,a(t) +

b(t)

a(t)

∂tf(t,s)ds.

Lemma ([]) For a positive definite matrix R> and a differentiable function{z(u)|u∈ [a,b]},the following inequalities hold:

(b–a)

b

a

zT(s)Rz(s)dsξT

R –R

∗ R

ξ,

(b–a)

b

a

˙

zT(s)Rz(s)˙ ds dθξT ⎡ ⎢ ⎢ ⎢ ⎣

R –R R –R

∗ R –R R

∗ ∗ R –R

∗ ∗ ∗ R

⎤ ⎥ ⎥ ⎥ ⎦ξ,

b

a

b

θ

˙

zT(s)Rz(s)˙ ds dθξT ⎡ ⎢ ⎣

R R –R

∗ R –R

∗ ∗ R

⎤ ⎥ ⎦ξ,

where

ξT=

ba

b

a

zT(s)ds,  (b–a)

b

a

b

θ

zT(s)ds dθ

,

ξT=

zT(b),zT(a),  ba

b

a

zT(s)ds,  (b–a)

b

a

b

θ

zT(s)ds dθ

,

ξT=

zT(b),  ba

b

a

zT(s)ds,  (b–a)

b

a

b

θ

zT(s)ds dθ

.

Lemma ([]) Let V be a Lyapunov function for system()with wT(t)w(t)w

m.If

˙

V+αVα w

m

wT(t)w(t)≤,

then V≤.

3 Main results

In this section, we will firstly consider a reachable set for uncertain parameter matrices

A= ,D= ,B=  in system (), namely,

˙

z(t) =Az(t) +Dztτ(t)+Bw(t), z(t) = , t∈[–h, ]. ()

After that, we will consider a reachable set for uncertain system ().

Ifτmτ(t)≤τM,τ˙(t)≤μ< , we get the reachable set bounding for dynamic system

() in Theorem .

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α> such that the following inequality holds:

= ⎡ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎣

              ∗              ∗ ∗        ,   ∗ ∗ ∗       ,  

∗ ∗ ∗ ∗        

∗ ∗ ∗ ∗ ∗       

∗ ∗ ∗ ∗ ∗ ∗    ,  

∗ ∗ ∗ ∗ ∗ ∗ ∗     

∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗    

∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗    

∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗    

∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗  

⎤ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎦

≤, ()

where

=αP+PA+ATP+R+M– e–ατmQ– e–ατmM – e–ατMM

+NA+ATNT+ATNA+ATNTA,

=PD+ND+ATND+ATNTD, = e–ατmQ,

= –e–ατmQ– e–ατmM, = –e–ατMM,

= e–ατmQ+ e–ατmM,

= e–ατMM,  = –N–ATNTATN,

 =PB+NB+ATNB+ATNTB,

= –( –μ)e–ατMM+DTND+DTNTD,

 = –DTNTDTN,  =DTNB+DTNTB,

=eατmR–eατmR– e–ατmQ– e–ατMQ,

= e–ατMQ, = e–ατmQ, = –e–ατMQ,

= –e–ατmQ,  = e–ατMQ,

= –e–ατMR– e–ατMQ, = e–ατMQ,  = –e–ατMQ,

= –e–ατmQ– e–ατmM, = e–ατmQ+ e–ατmM,

= –e–ατMM, = e–ατMM,

= –e–ατMQ,  = e–ατMQ,

= –e–ατmQ– e–ατmM,

= –e–ατMM,  = –e–ατMQ,

 = (τm)Q+ (τMτm)Q+N+NT,  = –NBNTB,

 = –

α

w

m

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Then the reachable sets of system()are bounded in a ball B(,r) ={zRn|zr}with

r=√ 

λmin(P)

. ()

Proof Construct the Lyapunov-Krasovskii functional

V(zt) =

i= Vi(zt),

where

V(zt) =zT(t)Pz(t),

V(zt) =

t

tτm

(st)zT(s)Rz(s)ds+

tτm

tτM

(st)zT(s)Rz(s)ds,

V(zt) =

t

tτ(t)

(st)zT(s)Mz(s)ds,

V(zt) =τm

τm

t

t+θ

(st)z˙T(s)Q˙z(s)ds,

V(zt) = (τMτm)

τm

τM

t

t+θ

(st)z˙T(s)Q˙z(s)ds,

V(zt) =

t

tτm

t

θ

t

λ

(st)˙zT(s)M

z(s)˙ ds dθdλ

+

t

tτM

t

θ

t

λ

(st)z˙T(s)M

z(s)˙ ds dθdλ.

Computing the derivative ofV(zt) of model (), we have

˙

V(zt) = zT(t)Pz(t) = –˙ αV(zt) + zT(t)P˙z(t) +αzT(t)Pz(t)

= –αV(zt) +αzT(t)Pz(t) + zT(t)P

Az(t) +Dztτ(t)+Bw(t), ()

˙

V(zt) = –αV(zt) +zT(t)Rz(t) +eατmzT(t–τm)Rz(tτm)

eατmzT(tτ

m)Rz(tτm) –eατMzT(t–τM)Rz(tτM), ()

˙

V(zt) = –αV(zt) +zT(t)Mz(t) –

 –τ˙(t)eατ(t)zTtτ(t)Mz

tτ(t)

≤–αV(zt) +zT(t)Mz(t) – ( –μ)e–ατMzT

tτ(t)Mz

tτ(t), ()

˙

V(zt) = –αV(zt) +τm˙zT(t)Qz(t) –˙ τm

t

tτm

(stzT(s)Qz(s)˙ ds

≤–αV(zt) +τmz˙T(t)Qz(t) –˙ eατmτm

t

tτm

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By using Lemma ,

˙

V(zt)≤–αV(zt) +τmz˙T(t)Qz(t)˙

eατmζT  ⎡ ⎢ ⎢ ⎢ ⎣

Q –Q Q –Q

∗ Q –Q Q

∗ ∗ Q –Q

∗ ∗ ∗ Q

⎤ ⎥ ⎥ ⎥

ζ, ()

whereζT= (zT(t),zT(tτ m),τm

t tτmz

T(s)ds,τm

t tτm

t

θzT(s)ds dθ),

˙

V(zt)

= –αV(zt) + (τMτm)z˙T(t)Qz(t) – (˙ τMτm)

tτm

tτM

(stzT(s)Qz(s)˙ ds ≤–αV(zt)

+ (τMτm)z˙T(t)Q˙z(t) –eατM(τMτm)

tτm

tτM

(stzT(s)Qz(s)˙ ds. ()

By using Lemma ,

˙

V(zt)≤–αV(zt) + (τMτm)z˙T(t)Qz(t)˙

eατMζT  ⎡ ⎢ ⎢ ⎢ ⎣

Q –Q Q –Q

∗ Q –Q Q

∗ ∗ Q –Q

∗ ∗ ∗ Q

⎤ ⎥ ⎥ ⎥

ζ, ()

where

ζT=

zT(t–τm),zT(t–τM),

τMτm

tτm

tτM

zT(s)ds,  (τMτm)

tτm

tτM

tτm

θ

zT(s)ds dθ

,

˙

V(zt) = –αV(zt) +

 τ

m˙z(t)Mz(t) +˙  τ

Mz(t)M˙ ˙z(t)

t

tτm

t

θ

(st)z˙T(s)M

z(s)˙ ds dθ

t

tτM

t

θ

(st)˙zT(s)M

˙z(s)ds dθ

≤–αV(zt) +

 τ

mz(t)M˙ z(t) +˙  τ

Mz(t)M˙ z(t)˙ – e–ατm

t

tτm

t

θ

˙

zT(s)Mz(s)˙ ds dθ

– e–ατM

t

tτM

t

θ

˙

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In the light of Lemma ,

˙

V(zt)≤–αV(zt) +

 τ

mz(t)M˙ z(t) +˙  τ

Mz(t)M˙ z(t)˙

– e–ατmζT

⎡ ⎢ ⎣

M M –M

∗ M –M

∗ ∗ M

⎤ ⎥ ⎦ζ

– e–ατMζT

⎡ ⎢ ⎣

M M –M

∗ M –M

∗ ∗ M

⎤ ⎥

ζ, ()

where

ξT=

zT(t), 

τm

t

tτm

zT(s)ds,

τ

m

t

tτm

t

θ

zT(s)ds dθ

,

ξT=

zT(t), 

τM

t

tτM

zT(s)ds,

τM

t

tτM

t

θ

zT(s)ds dθ

.

Certainly, the following equations hold:

–˙z(t) +Az(t)

+Dztτ(t)+Bw(t)TN

–˙z(t) +Az(t) +Dztτ(t)+Bw(t)= ,

zT(t)N

–˙z(t) +Az(t) +Dztτ(t)+Bw(t)= ,

()

whereN,Nare matrices with appropriate dimensions. Through ()-() and ()()()(), one gets

˙

V(zt) +V˙(zt) +V˙(zt) +V˙(zt) +V˙(zt) +V˙(zt) –

α

w

m

wT(t)w(t)

≤–αV(zt) –αV(zt) –αV(zt) –αV(zt) –αV(zt) –αV(zt) +ζT(t)ζ(t).

That is,

˙

V(zt) –

α

w

m

wT(t)w(t)≤–αV(zt) +ζT(t)ζ(t).

Then one has

˙

V(zt) +αV(zt) –

α

w

m

wT(t)w(t)≤ζT(t)ζ(t), ()

where

ζT(t) =

zT(t),zTtτ(t),zT(t–τm),zT(t–τM),

τm

t

tτm

zT(s)ds,

τM

t

tτM

zT(s)ds,

τMτm

tτm

tτM

zT(s)ds,

τ

m

t

tτm

t

θ

zT(s)ds dθ, 

τM

t

tτM

t

θ

zT(s)ds dθ,  (τMτm)

tτm

tτM

tτm

θ

zT(s)ds dθ,z˙T(t),wT(t)

.

For () holding, we getV˙ +αVα

wmw

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Thus, according to Lemma , one hasV(zt)≤.

It is easy to see

zT(t)Pz(t) =V(zt)≤V(zt) +V(zt) +V(zt) +V(zt) +V(zt) +V(zt) =V(zt).

Furthermore, by using the spectral property for symmetric positive definite matrixP, we get

λmin(P)z(t)≤V(zt). ()

Therefore,z(t)r=√  λmin(P)

due to ().

Next, let us consider the polytopic uncertain linear system (). Reachable set bounding of system () is got and stated in Theorem .

Theorem  If there exist appropriate dimension matrices P> ,R> ,R> ,Q> , Q> ,M > ,M> ,M> ,appropriate dimensions matrices N,N,and a scalar

α> ,such that the following inequalities hold(i= , , . . . ,N):

i=

⎡ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎢ ⎣

i i ii ii i i  i

i          i  i

∗ ∗ i i ii i,i  

∗ ∗ ∗ i   i   ,i  

∗ ∗ ∗ ∗ i   i    

∗ ∗ ∗ ∗ ∗ i   i   

∗ ∗ ∗ ∗ ∗ ∗ i   ,i  

∗ ∗ ∗ ∗ ∗ ∗ ∗ i    

∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ i   

∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗  i  

∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗  i  i

∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗ ∗  i

⎤ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎥ ⎦

≤, ()

where

i=αPi+Pi(A+Ai) + (A+Ai)TPi+R+M– e–ατmQ– e–ατmM– e–ατMM +N(A+Ai) + (A+Ai)TNT+ (A+Ai)TN(A+Ai) + (A+Ai)TNT(A+Ai),

i=Pi(D+Di) +N(D+Di) + (A+Ai)TN(D+Di) + (A+Ai)TNT(D+Di),

i= e–ατmQ, i= –e–ατmQ– e–ατmM,

i= –e–ατMM, i= e–ατmQ+ e–ατmM,

i= e–ατMM,  i= –N– (A+Ai)TNT– (A+Ai)TN,

 i=Pi(B+Bi) +N(B+Bi) + (A+Ai)TNB+ (A+Ai)TNT(B+Bi),

i= –( –μ)e–ατMM+ (D+Di)TN(D+Di) + (D+Di)TNT(D+Di),

 i= –(D+Di)TNT– (D+Di)TN,  i= (D+Di)TNB+ (D+Di)TNTB

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i= e–ατMQ, i= e–ατmQ, i= –e–ατMQ,

i= –e–ατmQ,  i= e–ατMQ,

i= –e–ατMR– e–ατMQ, i= e–ατMQ,  i= –e–ατMQ,

i= –e–ατmQ– e–ατmM, i= e–ατmQ+ e–ατmM,

i= –e–ατMM, i= e–ατMM,

i= –e–ατMQ,  i= e–ατMQ,

= –e–ατmQ– e–ατmM,

= –e–ατMM,  i= –e–ατMQ,

 i= (τm)Q+ (τMτm)Q+N+NT,  i= –N(B+Bi) –NT(B+Bi),

 i= –

α

w

m

+ (B+Bi)TN(B+Bi) + (B+Bi)TNT(B+Bi).

Then the reachable sets of system()are bounded in a ball B(,r) ={zRn|zr}with

r=√ 

λmin(Pi)

, i= , , . . . ,n. ()

Proof In progress in Theorem , replacing matrixAby Ni=θi(t)(A+Ai), matrixBby

N

i=θi(t)(B+Bi), matrixDby

N

i=θi(t)(D+Di), one can easily get the conclusion.

Remark  In this paper, the discrete delayτmτ(t)≤τMis of a more general scope than

≤τ(t)≤τconsidered in [, , ].

Remark  The novel inequalities in Lemma  lead to tighter bounds than the Jensen in-equality. By means of novel inequalities in Lemma , to estimate integral terms in Lya-punov functionals, better bounds for a reachable set are proposed in this paper.

Remark  To compute the smallest bound of a reachable set for linear dynamic systems (), we solve the optimization problem for a positive scalarδ> :

min δ¯

¯

δ=

δ

s.t.

⎧ ⎨ ⎩

(a) PδI,

(b) inequality ()/() in Theorem /.

()

Remark  The novel inequalities in Lemma  may be used to study the reachable set

problem for a linear neutral system, even for a non-linear neutral system.

Remark  In references [, , ], they used conventional Jensen inequalities –(h– h)

th

thz

T(s)Pz(s)ds–(th

thz(s)ds)

TP(th

thz(s)ds) and –

(h–h)

h

h

th

t+θ zT(s)× Rz(s)ds dθ ≤ –(–h

h

th

t+θ zT(s)ds dθ)R(

h

h

th

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bound in this study is more accurate than those in references. Therefore, the conservatism in our work is less than the existing ones.

Remark  It should be noted that if there are more accurate inequalities to estimate the

bound ofabzT(s)Rz(s)ds,b

a z˙T(s)R˙z(s)ds dθ,

b a

b

θ ˙zT(s)Rz(s)˙ ds dθ, there is still room for further improvement of the proposed results to reduce the conservatism of systems.

Remark  Some literature works researched the stability of second order delay

differen-tial equations; see, for example, references [–]. In the future, reachable set bounding for second order delay differential equations may be a hot issue, and methods similar to those in this paper may be used to estimate reachable set bounding for second order delay differential equations.

4 Examples

In order to compare the obtained results with those in the literature, we provide several numerical examples in the following.

Example  Consider the uncertain time-varying delayed system in [, ]:

A+A=

–   –.

, A+A=

–   –.

, D+D=

–  – –.

,

D+D=

–  – –.

, B+B=

–. 

=B+B, wT(t)w(t)≤.

()

[image:10.595.133.481.365.439.2]

We consider two cases for discrete delayτ(t): ≤τ(t)≤.,τ˙(t)≤μ<  and ≤τ(t)≤ .,τ˙(t)≤μ< . Letμbe different values, we computeδ¯’s by using optimization problem (). The computedδ¯’s are listed in Table  for the forward case and in Table  for the backward case. From Tables  and , we know that the proposed result in Theorem  is tighter than the ones in references [, ].

Table 1 δ¯’s in Example 1 for 0≤τ(t)≤0.7,τ˙(t)≤μ

μ

0 0.1 0.2 0.3 0.4 0.5 0.6 0.9

[22] 2.97 3.30 3.85 4.85 6.93 12.84 53.86

-[27] 1.89 1.94 2.00 2.08 2.19 2.35 2.60 3.51

[image:10.595.115.480.673.732.2]

Theorem 2 1.38 1.51 1.59 1.63 1.70 1.81 1.94 2.05

Table 2 δ¯’s in Example 1 for 0≤τ(t)≤0.75,τ˙(t)≤μ

μ

0 0.1 0.2 0.3 0.4 0.5 0.6 0.9

[22] 3.34 3.79 4.53 5.88 8.85 18.36 127.70

-[27] 2.28 2.35 2.45 2.57 2.68 2.85 4.62 5.57

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[image:11.595.117.479.160.261.2]

Table 3 δ¯’s in Example 2 for 0≤τ(t)≤0.1,τ˙(t)≤μ

Method [21] [22] [2] Theorem 2

¯

δ - - 2.8686×104 7.0825

Table 4 Computedr’s of Example 4 for different values ofτwithμ= 0

τ

0.1 0.3 0.5 0.7 0.9

[8] √0.83 √1.28 √1.94 √2.90 √4.46

[4] √0.74 √0.92 √1.36 √2.30 √3.51

[10] √0.68 √0.80 √0.97 √1.64 √3.22

[2] √0.66 √0.75 √0.94 √1.61 √3.14

[3] √0.66 √0.75 √0.94 √1.61 √3.14

[22] √0.66 √0.75 √0.94 √1.61 √3.14

Theorem 2 √0.57 √0.68 √0.81 √1.43 √2.10

Example  Consider the following uncertain model in [, , ] with parameters:

A+A=

 –.  –.

, A+A=

 –.  –.

,

D+D=

–. –.  .

=D+D,

B+B=

– 

=B+B, μ= , τm= , τM= ., wT(t)w(t)≤.

()

Whenμare different values, we solve inequalities () to getδ¯sforτmτ(t)≤τM,

˙

τ(t)≤μwithτm= ,τM= .. To compare with the results in [, , ], we list computed

results by using Theorem  in Table . One can see that there are no feasible solutions by employing the methods in [, ], and one can see easily that the proposed method has more application area.

Example  Consider the following delayed system () with parameters:

˙

z(t) =

–   –.

z(t) +

–  – –.

ztτ(t)+

–. 

w(t), ()

andwT(t)w(t).

By using the method in Theorem , we list computedr’s for different values ofτ(t) with

μ=  in Table . We can see that bounds computed in this paper are tighter than those of references [–, , , ]. Of course, it decreases the conservatism of systems.

Example  Consider the following uncertain delayed system:

A+A=

–   –.

, A+A=

–   –.

, D+D=

–  – –.

,

D+D=

–  – –.

, B+B=

–. 

=B+B, wT(t)w(t)≤,

[image:11.595.136.472.311.416.2]
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[image:12.595.117.477.82.226.2]

Figure 1 The reachable set of Example 4.

and time delay .≤τ(t)≤.,μ= .. The reachable set of system () is plotted in Figure  withP=

. –. –. .

.

Remark  In the reference [], Domoshnitsky discussed the stability of more

compli-cated linear neutral systems with uncertain coefficients and uncertain delays. In further work, we will study reachable set bounding for this type of linear neutral systems.

5 Conclusions

Firstly, we study uncertain linear systems with polytopic parameters. By using L-K func-tional and novel inequalities to estimate integral terms in L-K funcfunc-tional, some novel suf-ficient conditions for a bounded reachable set of uncertain systems are obtained. Then, we use some examples to show that our methods in Theorems  and  are effective and have less conservatism compared with reported conditions. Furthermore, the method in this work may be extended to compute a reachable set of linear neutral systems, and it may even be used to deal with stability of linear systems and non-linear systems in the future.

Acknowledgements

This work was supported by the Natural Science Foundation of the Anhui Higher Education Institutions of China (Nos. KJ2016A625, KJ2016A555), the National Natural Science Foundation of China (Nos. 61603272, 11526149), the Youth Fund Project of Tianjin Natural Science Foundation (No. 16JCQNJC03900).

Competing interests

The authors declare that they have no competing interests.

Authors’ contributions

All authors contributed equally to the manuscript, read and approved the final manuscript.

Publisher’s Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Received: 13 February 2017 Accepted: 24 October 2017 References

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Figure

Table 2 δ¯’s in Example 1 for 0 ≤ τ(t) ≤ 0.75, ˙τ(t) ≤ μ
Table 4 Computed r’s of Example 4 for different values of τ with μ = 0
Figure 1 The reachable set of Example 4.

References

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