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BY 4.0 license Open Access Published by De Gruyter December 17, 2021

Absolute Stability of Neutral Systems with Lurie Type Nonlinearity

  • Josef Diblík EMAIL logo , Denys Ya Khusainov , Andriy Shatyrko , Jaromír Baštinec and Zdeněk Svoboda

Abstract

The paper studies absolute stability of neutral differential nonlinear systems

x˙(t)=Axt+Bxtτ+Dx˙tτ+bf(σ(t)),σ(t)=cTx(t),t0

where x is an unknown vector, A, B and D are constant matrices, b and c are column constant vectors, 𝜏 > 0 is a constant delay and f is a Lurie-type nonlinear function satisfying Lipschitz condition. Absolute stability is analyzed by a general Lyapunov-Krasovskii functional with the results compared with those previously known.

MSC 2010: 93D22; 93D05; 34K20; 34K25; 34K12

1 Introduction

The paper considers absolute stability of a system of nonlinear differential equations of neutral type

(1.1) x˙(t)=Ax(t)+Bx(tτ)+Dx˙(tτ)+bf(σ(t)),t0

where x=(x1, ⋅, xn)T:[−τ, ∞) → ℝn, A, B and D are n × n constant matrices, b is an n-dimensional column constant vector, 𝜏 > 0 is a constant delay, f:RR , f(0)=0, is a Lurie-type nonlinear function satisfying Lipschitz condition,

(1.2) σ(t):=cTx(t)

and c is a column n-dimensional constant vector where the superscript T denotes the transpose of a vector (or a matrix).

1.1 On absolute stability

The problem of absolute stability was formulated in 1944 by Lurie and Postnikov in [39]. In [1,8], generalizations of the problem are carried out, and the well-known Aizermann hypothesis [1, 49] formulated (some scholars still adhere to referring to the problems associated with absolute stability as Lurie nonlinear control system ones). The initial period of studying the theory of absolute stability is associated with the name of its founder [39,40], who tried to solve the problem with the direct Lyapunov method by means of a Lyapunov function of the “quadratic form plus the integral of nonlinearity" type. This classical method for investigating absolute stability using Lyapunov’s functions was used by many authors [1 ,40, 41, 42, 60]. Since the mid 1960's the intensive development in the theory of absolute stability has included the so-called frequency method, initiated by Popov [21, 22,43,45]. In addition to the direct use of so called Popov’s criterion for the study of absolute stability, special methods for its application are sought and analogous frequency criteria are formulated [2, 25]. An in-depth analysis of both of the above methods, a study of the relationship between them, and a number of new original approaches are contained in the numerous publications by Yakubovich and his followers [21, 22, 34, 59]. When constructing mathematical models of real systems for a more precise description of the operation of systems, there is a need to consider equations with delay and, in general, neutral type equations (for a recent overview we refer to [48]). Unfortunately, time-delay phenomenon can frequently degrade performance of control systems or even can lead to instability. Therefore, the research of stability in general and, particularly, absolute stability of time-delay Lurie systems is of important significance [10,11,17, 19, 26, 28, 29, 30, 32,35,47]. In [31], Krasovskii replaces Lyapunov functions by what is now called Lyapunov-Krasovskii functionals, which find ample applications in setting out the conditions of stability. Numerous ingenious constructions have been published of such functionals, often using the so-called Razumihin condition [50]. In particular, we refer to [5,9,20, 46, 51, 52, 53, 56, 58,]. Surveys and overviews of the methods and results related to absolute stability achieved since the birth of the theory in 1944 can be found, for example, in [2, 21,32, 33, 34]). Note that a positivity-based approach, closely related to the concept of the Lyapunov functions, which uses the nonnegativity of entries of the Cauchy matrices, is developed in [3, 4, 6, 7,12,13, 15]. The above methods are widely used in investigating the stability of neutral differential equations. For recent results we also refer to [14,16,24,36,54,55, 57] and to the references therein.

1.2 Preliminaries, the problem considered, and the paper structure

Throughout the paper we use the following restriction on the nonlinearity of f (not mentioning this explicitly when formulating results). Namely, assume that there exists a k > 0 such that

(1.3) kωf(ω)f(ω)>0,ω0.

Such a nonlinearity is often said to be of a Lurie type or, based on a geometrical interpretation of (1.3), we also say that f satisfies a sectorial-condition.

Let φ:[−τ, 0] → ℝn be a continuously differentiable vector-function. In addition to system (1.1), consider an initial condition

(1.4) xt=φt,x˙t=φ˙t,t[τ,0].

A solution of the problem (1.1), (1.4) is understood within the meaning of the following definition.

Definition 1

A function x:[−τ, ∞) → ℝn is called a solution of (1.1), (1.4) if it is continuous on [−τ, ∞), continuously differentiable on [−τ, ∞)∖{τ s, s=0, 1, ⋅}, satisfying (1.1) on [0, ∞)∖{τ s, s=0, 1, ⋅}, and satisfying (1.4).

The existence of a solution of the problem (1.1), (1.6) on [−τ, ∞) within the meaning of Definition 1, its uniqueness and continuous dependence on initial values (1.4) are the consequences of the linearity of the first three terms in the right-hand side of (1.1), the Lipschitzeanity of f and the sectorial condition (1.3).

For a vector y=(y1,,yn)T:[τ,)Rn , the following norms are used in the paper

y(t)=i=1nyi2(t)1/2,ift[τ,),yt,τ=maxτs0y(s+t),ift[0,),yt,τ,ς=tτteςts|y(s)|2ds1/2,ift[0,),

where 𝜍 > 0 is a constant. If B is a symmetric positive-definite matrix, denote by λmax(B) , λmin(B) its maximal and minimal eigenvalues. We also use a norm of a square matrix A , induced by above Euclidean norm of a vector, computed by formula

(1.5) A=λmax(ATA)1/2.

Listed below are the definitions of stability used.

Definition 2

The zero solution of system (1.1) is exponentially stable in the metric C0 if, for the solution x:[−τ, ∞) → ℝn of (1.1), (1.4) we have

(1.6) xtF0(φ,φ˙)eη0t,t0,

where F0 is a positive definite functional and 𝜂0 > 0 is a constant.

Definition 3

The zero solution of system (1.1) is exponentially stable in the metric C1, if it is stable in the metric C0 and, for t ∈ [0, ∞)∖{τ s, s=0, 1, ⋅},

(1.7) x˙tF1(φ,φ˙)eη1t,

where F1 is a positive definite functional and 𝜂1 > 0 is a constant.

Definition 4

The system (1.1) is said to be absolutely stable if its zero solution is exponentially stable in the metric C1 for an arbitrary function f, satisfying (1.3).

In the present paper we solve the problem of the absolute stability of system (1.1) within the meaning of Definition 4. The paper is structured as follows. First, the exponential C0 stability of (1.1) is studied in part 2 with the main result of this part being Theorem 1. Its proof is carried out by the Lyapunov-Krasovskii method of functionals using a special functional V. Such an approach needs the positivity of a matrix (the matrix S below) appearing in the estimate of the derivative of the functional V along solutions of (1.1) . Second, the exponential C1 stability of (1.1) is studied in part 3. The proof of the main result of this part (Theorem 2) is based on the possibility to exclude the delayed derivative term Dx˙(tτ) from (1.1), considering then (in an admissible domain) only the delayed system derived instead (Lemma 1). Then, the final statement (Theorem 3) is formulated. The results are illustrated by an example in part 4. The paper is concluded by part 5 with comments and conclusions concerning the approach used. Relations with the investigations of other authors are discussed as well.In the formulations of the theorems on C0 or C1 exponential stability, functionals Fi and constants ηi, i=0, 1 are defined explicitly with their constructions following from the methods of proofs.

2 Exponential C0 Stability

Below, we give conditions for C0 exponential stability of (1.1) . From the proof, an estimate of the convergence of solutions follows as well. To solve the problem of absolute stability within the meaning of Definition 4 for system (1.1) under restriction (1.3) , the Lyapunov-Krasovskii functional (2.1) will be used of the quadratic type with respect to both the current coordinates and their derivatives,

(2.1) V(x(t))=xTtHx(t)+tτteς1tsxTsG1x(s)ds+tτteς2tsx˙TsG2x˙sds+β0σtf(s)ds.

In (2.1), t=0, x is a solution of system (1.1), H, G1, G2 are positive-definite symmetric matrices, ς1>0,ς2>0 and β⩾0. The condition (1.3) and the well-known properties of quadratic forms imply the two-sided estimate of functional (2.1)

(2.2) λminHxt2+λmin(G1)xt,τ,ς1+λmin(G2)x˙t,τ,ς2V(x(t))λmaxH+12βkc2xt2+tτteς1tsxT(s)G1x(s)ds+tτteς2tsx˙T(s)G2x˙sdsλmaxH+12βkc2xt2+λmax(G1)xt,τ,ς1+λmax(G2)x˙t,τ,ς2.

These will be used in the paper. We also use the notation

λH:=1λmin(H)λmax(H)+12βkc2,λHG1:=λmax(G1)λmin(H),λHG2:=λmax(G2)λmin(H).

The stability result formulated below depends, among others, on the positive definiteness of an auxiliary (3n + 1)  ×  (3n + 1) matrix S. This matrix depends on matrices, vectors and constants used in (1.1) –(1.3) , (2.1) and on a parameter ν⩾0, not yet involved. In other words, the elements of S are constructed using β, ς1, ς2, k, ν, b, c, A, B, D, H, G1, G2, formally

S=S(β,ς1,ς2,k,ν,b,c,A,B,D,H,G1,G2).

In its block form, the matrix S is defined as

S:=S11S12S13S14S12TS22S23S24S13TS23TS33S34S14TS24TS34TS44

with block-matrices

S11:=ATHHAG1ATG2A,S12:=HBATG2B,S13:=HDATG2D,S14:=HbATG2b12βAT+νIc,S22:=eς1τG1BTG2B,S23:=BTG2D,S24:=BTG2b+12βc,S33:=eς2τG2DTG2D,S34:=DTG2b+12βc,S44:=bTG2bβcTb+νk

where I in S14 is the unit n × n matrix.

Theorem 1

If there exist non-negative constants β, ν, positive constants ς1, ς2 and positive definite symmetric matrices H, G1 and G2 such that the matrix S is positive definite, then the zero solution of system (1.1) is exponentially stable in the metric C0 and the solution of the problem (1.1), (1.4) satisfies

(2.3) xtλHφ(0)+λHG1φ0,τ,ς1+λHG2φ˙0,τ,ς2eγt/2,

where t ∈ [0, ∞) and fixed number γ satisfies

(2.4) 0<γγ:=min{ς1,ς2,δ},δ:=λminSλmax(H)+12βkc2.

Proof. The proof splits into two parts. In part i), an estimate of the total derivative of the functional (2.1) along solutions of the system (1.1) is computed. Part ii) deals with the exponential stability of solutions to system (1.1) in the metrix C0.

i) Let us calculate the total derivative of the functional (2.1) along solutions of (1.1) . Assuming t ∈ [0, ∞)∖{τ s, s=0, 1, ⋅}, we have

ddtVx(t)=Ax(t)+Bx(tτ)+Dx˙(tτ)+bfσtTHxt+xTtHAx(t)+Bx(tτ)+Dx˙(tτ)+bfσt+xT(t)G1x(t)eς1τxTtτG1x(tτ)+x˙T(t)G2x˙(t)eς2τx˙TtτG2x˙(tτ)ς1tτteς1tsxTsG1x(s)dsς2tτteς2tsx˙TsG2x˙(s)ds+βfσtcTAxt+Bxtτ+Dx˙tτ+bfσt.

Before writing this derivative in a form with the matrix S, we rewrite it using system (1.1) as follows

(2.5) ddtVx(t)=Ax(t)+Bx(tτ)+Dx˙(tτ)+bfσtTHxt+xTtHAx(t)+Bx(tτ)+Dx˙(tτ)+bfσt+xT(t)G1x(t)eς1τxTtτG1x(tτ)+Axt+Bxtτ+Dx˙tτ+bfσtTG2Axt+Bxtτ+Dx˙tτ+bfσteς2τx˙tτG2x˙tτς1tτteς1tsxTsG1x(s)dsς2tτteς2tsx˙TsG2x˙(s)ds+βfσtcTAxt+Bxtτ+Dx˙tτ+bfσt.

Define an auxiliary vector

X(t):=xT(t)xT(tτ)x˙T(tτ)f(σ(t)).

Now, all the non-integral terms in the right-hand side of the last expression can be written using this vector and the matrix S. Omitting technicalities, it can be verified term by term that the identity

Ax(t)+Bx(tτ)+Dx˙(tτ)+bfσtTHxt+xTtHAx(t)+Bx(tτ)+Dx˙(tτ)+bfσt+xT(t)G1x(t)eς1τxTtτG1x(tτ)+Axt+Bxtτ+Dx˙tτ+bfσtTG2Axt+Bxtτ+Dx˙tτ+bfσteς2τx˙tτG2x˙tτ+βfσtcTAxt+Bxtτ+Dx˙tτ+bfσtX(t)SXT(t)νσt1kfσtfσt

holds. Then, (2.5) can be written as

(2.6) ddtVx(t)=X(t)SXT(t)νσt1kfσtfσtς1tτteς1tsxTsG1x(s)dsς2tτteς2tsx˙TsG2x˙(s)ds.

Due to (1.3),

(2.7) νσt1kfσtfσt<0.

As S is positive definite, we have

(2.8) d d t V x ( t ) λ min S x ( t ) 2 + x ( t τ ) 2 + x ˙ t τ 2 + f 2 σ t ς 1 t τ t e ς 1 t s x T s G 1 x ( s ) d s ς 2 t τ t e ς 2 t s x ˙ T s G 2 x ˙ ( s ) d s λ min S x t 2 ς 1 t τ t e ς 1 t s x T s G 1 x ( s ) d s ς 2 t τ t e ς 2 t s x ˙ T s G 2 x ˙ ( s ) d s .

ii) Prove the exponential stability of the solutions to system (1.1) in the metrix C0. Below we analyze two cases dealing with ςδ and ς < δ where ς:=min{ς1,ς2}>0 .

ii1) Let ςδ . Then, from inequality (2.2), we get

λmaxH+12βkc2x(t)2V(x(t))+tτteς1tsxT(s)G1x(s)ds+tτteς2tsx˙T(s)G2x˙sds

and

xt21λmax(H)+12βkc2Vx(t)+1λmax(H)+12βkc2tτteς1tsxTsG1x(s)ds+tτteς2tsx˙TsG2x˙(s)ds.

Inequality (2.8) yields

ddtVx(t)λminS1λmax(H)+12βkc2Vxt+1λmax(H)+12βkc2tτteς1tsxTsG1x(s)ds+tτteς2tsx˙TsG2x˙(s)dsς1tτteς1tsxTsG1x(s)dsς2tτteς2tsx˙TsG2x˙(s)ds

or

ddtVx(t)δVxtς1δtτteς1tsxT(s)G1x(s)dsς2δtτteς2tsx˙T(s)G2x˙(s)ds.

We get,

ddtVx(t)δVxt.

Integrating this inequality over (0, t), which is a correct operation because the set of isolated points {t=τ s, s=0, 1, ⋅} is countable, for t=0, we obtain

(2.9) VxtV(φ(0))eδt.

ii2) Let ς < δ. Rewrite the right-hand part of the inequality (2.2) as follows

tτteς1tsxT(s)G1x(s)dstτteς2tsx˙T(s)G2x˙(s)dsVxt+λmaxH+12βkc2x(t)2.

Now, using (2.8), we get

ddtV(x(t))λminSxt2ςtτteς1tsxTsG1x(s)dsςtτteς2tsx˙TsG2x˙(s)dsλminSxt2+ςVxt+λmax(H)+12kc2xt2=ςVxtλminSςλmax(H)+12βkc2xt2=ςVxt(δς)λmax(H)+12βkc2xt2.

Then,

ddtVxtςVxt

and integrating this inequality over (0, t), we obtain (as in ii1))

(2.10) VxtVφ(0)eςt,t0.

From (2.9) and (2.10) we deduce that, in both cases ii1), ii2) considered, we have

(2.11) VxtVφ(0)eγt,t0.

Utilizing (2.2) and (2.11), we get (the below inequalities hold for t≥0 as well)

λminH|x(t)|2+λminG1xt,τ,ς2+λminG2x˙t,τ,ς2VxtVφ(0)eγtλmaxH+12βkc2φ(0)2+λmaxG1φ0,τ,ς2λmaxH+12βkc2+λmaxGφ˙0,τ,ς2eγt,

hence, it follows that

|x(t)|21λmin(H)λmax(H)+12βkc2φ(0)2+λmax(G1)φ0,τ,ς2λmaxH+12βkc2+λmaxG2φ˙0,τ,ς2eγt.

Now, after a simple estimation of the right-hand side,

|xt|F0(φ,φ˙)eγt/2

where

F0(φ,φ˙):=λHφ(0)+λHG1x0,τ,ς+λHG2φ˙0,τ,ς.

Put η0=γ/2. Inequality (2.3) is proved. The zero solution of (1.1) is C0 exponentially stable within the meaning of Definition 2 since (1.6) holds. □

3 Exponential C1 Stability and Absolute Stability

To prove the exponential stability in metric C1, we need the following lemma providing a formula transforming neutral system (1.1) to a delayed one of the Volterra type.

Lemma 1

Let m ∈ {1, 2, ⋅} be fixed. Then, for t ∈ ((m − 1)τ, mτ), the solution of the problem (1.1), (1.4) satisfies the equation

(3.1) x˙(t)=Dmx˙(tmτ)+Ax(t)+i=1m1Di1DA+Bx(tiτ)+Dm1Bx(tmτ)+i=0m1Dibfσtiτ.

Proof. We will prove the lemma by induction. Let x(t) be the solution of problem (1.1), (1.4). Then, for m=1, the lemma holds because formula (3.1) coincides with initial system (1.1) . Let us recall that, if we deal with a sum of the form i=10 , then, by customary definitions, we set such sum equal to zero. This concerns the first sum in (3.1).Assuming that the conclusion of the lemma holds for m=j−1 where j=2 is a fixed natural number, we will show that, then, it holds for m=j as well. For m=j−1, t ∈ ((j − 2)τ, (j − 1)τ), we get from (3.1)

(3.2) x˙(t)=Dj1x˙(t(j1)τ)+Ax(t)+i=1j2Di1DA+Bx(tiτ)+Dj2Bx(t(j1)τ)+i=0j2Dibfσtiτ.

If m=j and t ∈ ((j − 1)τ, jτ), then, using (1.1), we get for the term x˙(t(j1)τ) in (3.2):

(3.3) x˙(t(j1)τ)=Dx˙(tjτ)+Ax(t(j1)τ)+Bx(tjτ)+bfσt(j1)τ.

Finally, substituting (3.3) into the right-hand side of (3.2), we derive

x˙(t)=Dj1Dx˙(tjτ)+Ax(t(j1)τ)+Bx(tjτ)+bfσt(j1)τ+Ax(t)+i=1j2Di1DA+Bx(tiτ)+Dj2Bx(t(j1)τ)+i=0j2Dibfσtiτ=Djx˙(tjτ)+Ax(t)+i=1j1Di1DA+Bx(tiτ)+Dj1Bx(tjτ)+i=0j1Dibfσtiτ,

i.e., the formula (3.1) holds for m=j as well. □

Theorem 2

Let the hypotheses of Theorem 1, where γ is fixed, hold and let

(3.4) 0<|D|eγτ/2<1.

Then, the zero solution of the system (1.1) is exponentially stable in the metric C1 and the solution of the problem (1.1), (1.4) satisfies

(3.5) x˙tMλHφ(0)+BDφ0,τ+MλHG1φ0,τ,ς1+φ˙0,τ+MλHG2φ˙0,τ,ς2BDeγt/2,

where t ∈ [0, ∞)∖{τ s, s=0, 1, ⋅} and

M:=A+bck+DA+B+Dbck1Deγτ/2.

Proof. By Theorem 1, the zero solution of the system (1.1) is exponentially stable in the metric C0. We show that the zero solution of (1.1) is also C1 exponentially stable. As it follows from formula (3.1) in Lemma 1, for t ∈ ((m − 1)τ, mτ), m=1, 2, ⋅, we have

x˙tDmx˙0,τ+Axt+DA+Bi=1m1Di1xtiτ+Dm1Bx0,τ+i=0m1Dibfσtiτ.

From (1.3) and (1.2) we derive ∣f(σ(t − iτ))∣ ⩽ kσ(t − iτ)∣ ⩽ kcx(t − iτ) ∣ and, therefore,

(3.6) x˙tDmx˙0,τ+A+bkcxt+i=1m1Di1DA+B+|D||b|k|c|xtiτ+Dm1Bx0,τ.

Let us estimate ∣x(t)∣ and ∣x(t − iτ) ∣ in (3.6) by formula (2.3). We obtain

(3.7) |x˙(t)|Dmφ˙0,τ+Dm1Bφ0,τ+A+|b|kcλHφ(0)+λHG1φ0,τ,ς1+λHG2φ˙0,τ,ς2eγt/2+DA+B+DbkcD1i=1m1Dieiγτ/2λHφ(0)+λHG1φ0,τ,ς1+λHG2φ˙0,τ,ς2eγt/2=Dmφ˙0,τ+Dm1Bφ0,τ+A+|b|k|c|λHφ(0)+λHG1φ0,τ,ς1+λHG2φ˙0,τ,ς2eγt/2+DA+B+Dbkc1Deγτ/21Dm1e(m1)γτ/2λHφ(0)+λHG1φ0,τ,ς1+λHG2φ˙0,τ,ς2eγt/2.

Since t ∈ ((m − 1)τ, mτ), then ∣Dm ⩽ exp((t/τ)ln∣ D∣). We have

Dmφ˙0,τ+Dm1Bφ0,τφ˙0,τ+BDφ0,τexptτln1|D|

and, by (3.4),

Dmφ˙0,τ+Dm1Bφ0,τφ˙0,τ+BDφ0,τeγt/2.

From (3.7), we get

(3.8) x˙tφ˙0,τ+BDφ0,τeγt/2+A+|b|kc+DA+B+Dbkc1|D|eγτ/21|D|m1e(m1)γτ/2λHφ(0)+λHG1φ0,τ,ς1+λHG2φ˙0,τ,ς2eγt/2.

Then, for any admissible m, inequality (3.8) with the term

|D|m1e(m1)γτ/2

omitted, yields

|x˙(t)|F1(φ,φ˙)eγt/2

where

F1(φ,φ˙):=MλHφ(0)+BDφ0,τ+MλHG1φ0,τ,ς1+φ˙0,τ+MλHG2φ˙0,τ,ς2.

Inequality (3.5) is proved. The zero solution of (1.1) is C1 exponentially stable within the meaning of Definition 3 where η1=γ/2 and (1.7) holds. □

The following theorem on absolute stability of system (1.1) within the meaning of Definition 4 directly follows from Theorem 1 and Theorem 2.

Theorem 3

If the hypotheses of Theorems 1 and 2 hold, then the zero solution of the system (1.1) is absolutely stable.

4 Example

We will investigate system (1.1) where n=2, τ=1,

A = 3 2 1 0 , B = 0 0.74035 0.74035 0 , D = 0.1 0 0 0.1 , b = c = 0 , 01 0.01 T , σ ( t ) = c T x ( t ) = 0.01 x 1 ( t ) 0.01 x 2 ( t ) ,

i.e., the system

(4.1) x˙1(t)=0.1x˙1(t1)3x1(t)2x2(t)+0.74035x2(t1)+0.01f(σ(t)),
(4.2) x˙2(t)=0.1x˙2(t1)+1x1(t)2x2(t)+0.74035x1(t1)0.01f(σ(t)),

with initial conditions (1.4). Set ς1=0.01, ς2=0.001, k=1, ν=0.1, β=0.01 and

G1=0.50.10.10.2,G2=0.06000.06,H=0.670.430.430.67.

Part of the below numerical computations was performed by MATLAB. For the eigenvalues of matrices G1, G2 and H, we get λmin(G1q 0.1697, λmax(G1q 0.5303, λmin(G2)=λmax(G2)=0.06, λmin(H)=0.24, λmax(H)=1.1. The matrix S takes the form

S2.06001.50000.36270.36270.04900.04900.00031.50001.28000.49600.22950.03100.06700.00420.36270.49600.46710.099000.00440.00050.36270.22950.09900.16510.004400.00050.04900.031000.00440.059300.00010.04900.06700.0044000.05930.00010.00030.00420.00050.00050.00010.00010.0999

and λmin(S)≐ 0.00000407. Because all eigenvalues are positive, matrix S is positive definite. Further we have

λH=1λmin(H)λmax(H)+12βkc24.5833,λHG1=λmax(G1)λmin(H)2.2095,λHG2=λmax(G2)λmin(H)=0.25,δ=λminSλmax(H)+12βkc23.7026106,γ=minς1,ς2,δ=δ

Moreover

|A|3.7025,|B|=0.74035,|D|=0.1,|DA+B|0.9186,|b|=|c|0.0141.

Because

γ<2τ1ln|D|4.6052

we set γ ≔ γ ** in (3.4). Then M≐ 4.7233. All hypotheses of Theorem 1 and of Theorem 2 are satisfied and, consequently, the zero solution of (4.1), (4.2) is exponentially stable in the metric C0 and in the metric C1. Finally, from (2.3), (2.4) and (3.5), it follows that the inequalities

xtλHφ(0)+λHG1φ0,τ,ς1+λHG2φ˙0,τ,ς2eγt/24.5834φ(0)+2.2095φ0,1,0.01+0.25φ˙0,1,0.001e0.000001851t,x˙tMλHφ(0)+BDφ0,τ+MλHG1φ0,τ,ς1+φ˙0,τ+MλHG2φ˙0,τ,ς2BDeγt/24.72334.5834φ(0)+7.4φ0,1+4.72332.2095φ0,1,0.01+φ˙0,1+4.72330.25φ˙0,1,0.001BDe0.000001851t

hold on [0, ∞) and on [0, ∞)∖{s, s=0, 1, ⋅} respectively. By Theorem 3, the zero solution of the system (4.1), (4.2) is absolutely stable.

Remark 1

System (4.1), (4.2) is considered in [5,38,44,56] with omitted nonlinearity (f ≡ 0), the same matrices A, D and with the matrix

B=α0110,

where α is a constant. In [44] asymptotic stability is established for |α|<0.4 while, in [38], for |α|<0.533 and, in [56] as the authors state, for ∣α ∣⩽1. In these papers no estimates are given related to the convergence of solutions or their derivatives. Exponential stability with explicit formulas estimating the convergence of solutions and their derivatives is given in [5] for ∣α ∣⩽0.6213. The present example gives exponential stability and explicit formulas estimating the convergence of solutions and their derivatives for ∣α ∣⩽0.74035.

5 Comments and Conclusions

The direct Lyapunov method is widely used for the stability analysis of functional differential systems. Its successful application substantially depends on an ingenious construction of Lyapunov-Krasovskii functional, suitable for the problem considered. As a rule, in the investigation of nonlinear neutral type control systems, functionals are used in the form of the sum of a quadratic form of terms on the right-hand side of the given system, a quadratic form of a “prehistory" and an integral of the nonlinearity. For example, in [27, 51], in the case of system (1.1), the following one is used:

(5.1) V(x(t))=x(t)Dx(tτ)THx(t)Dx(tτ)+tτteςtsxT(s)Gx(s)ds+β0σtf(s)ds

where H and G are positive definite matrices, 𝜍 > 0 and 𝛽 > 0. However, applying functional (5.1) or any such functional type, does not result in an estimate of the norm ∣x(t)∣ of solutions, but rather in the integral norm ∥ xt, τ, ς. Many authors use method of functionals or other methods to state the fact of asymptotic stability only because their approach does not give an explicit estimate of the norm ∣x(t)∣ or |x˙(t)| (such as formulas (2.3), (3.5) in Theorem 1 and Theorem 2). We refer, e.g., to [7,18,23,37,56]. Functional (2.1) is more general than some of the previously ones used to investigate neutral equations. For example, functionals used in [5, 35,52,53] are, if the systems considered are reduced to the form (1.1), its particular cases.

Let us discuss some specific properties of our approach. By an appropriate choice of the coefficient ν in the blocks S43 and S44 of the matrix S, in some cases, the positive definiteness of S can be achieved. Such a parameter is involved because of the sectorial condition (1.3) used in the proof (inequality (2.7)). The block-matrix S11 contains the expression −ATHHA. By the well-known result on Lyapunov matrix equations, if system x˙(t)=Ax(t) is asymptotically stable, then, for any positive definite symmetric matrix Q, there exists a unique positive definite symmetric matrix H such that −ATHHA=−Q. This fact can be, in principle, used when the derivative of the functional V along trajectories is estimated (see (2.5), (2.6)). We did not use such a possibility preferring consideration with the matrix S giving more general results. The parameters ς1, ς2 in the exponential multipliers exp(−ς1(t − s)), exp(−ς2(t − s)) in the definition of V(x (t)) by (2.1) have an impact on diagonal block-matrices S22, S33 and, moreover, as suggested by formulas (2.4), (3.5), on the speed of convergence of the vanishing solutions. As it follows from the proof of Theorem 1, part ii2), formula (2.10) (and computations above this formula), the assumption 𝜍1 > 0 𝜍2 > 0 cannot be replaced by ς1⩾0, ς2⩾0. If ς1=0 or if ς2=0 then, proceeding by the scheme of the proof, we are not able to prove an exponential stability and construct explicit formulas estimating solutions and their derivatives.

In Theorem 2 we assumed ∣D∣=≠ 0. This is a quite natural assumption because if ∣D∣=0, then, by (1.5), all eigenvalues of the matrix DTD are zeroes. Consequently, D=Θ, where Θ is n × n zero matrix and (1.1) becomes a delayed rather than neutral system and can be investigated with a functional defined by (2.1) if the integral with kernel defined by the derivatives is omitted. In many investigations when neutral systems such as (1.1) are considered, assumption |D|<1 is necessary. In the present paper, this inequality follows from formula (3.4) in Theorem 2. In Theorem 1, a block-structured matrix S is applied. Although the latter assumption is not explicitly formulated (and is not explicitly used in its proof), it is probably implied by the positivity of S.

It is an open question, whether a functional Vp(x(t))=eptV(x(t)) , where p is a suitable real parameter and V(x (t)) is defined by formula (2.1), can be used to estimate solutions to system (1.1) in non-stable cases.Further progress can be achieved as well if the approach used is extended to systems (1.1) with the sum of nonlinearities i=1sbifi(σi(t)) , σi(t)=ciTx(t) of a Lurie type instead of only one such nonlinearity. Another challenge is a possible generalization of the results to systems with variable matrices and delays and to fractional differential systems as well.


E-mail: josef.diblik@ceitec.vutbr.cz

E-mail: jaromir.bastinec@ceitec.vutbr.cz

E-mail: zdenek.svoboda@ceitec.vutbr.cz


Acknowledgement

The research has been supported by the Czech Science Foundation under the project 19-23815S. The work was realized in CEITEC - Central European Institute of Technology with research infrastructure supported by the project CZ.1.05/1.1.00/02.0068 financed from European Regional Development Fund. The authors would like to express their sincere gratitude to the editor and referees for their comments, which have improved the present paper in many aspects.

  1. Conflict of interest

    Authors state no conflict of interest.

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Received: 2021-10-15
Accepted: 2021-11-01
Published Online: 2021-12-17

© 2021 Josef Diblík et al., published by De Gruyter

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