Научная статья на тему 'RESEARCH OF THE ASYMPTOTIC EQUILIBRIUM OF TIME-DELAY SYSTEMS BY JUNCTION OF LYAPUNOV - KRASOVSKII AND RAZUMIKHIN APPROACHES'

RESEARCH OF THE ASYMPTOTIC EQUILIBRIUM OF TIME-DELAY SYSTEMS BY JUNCTION OF LYAPUNOV - KRASOVSKII AND RAZUMIKHIN APPROACHES Текст научной статьи по специальности «Математика»

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Ключевые слова
TIME-DELAY SYSTEMS / ASYMPTOTIC STABILITY / ASYMPTOTIC QUIESCENT POSITION / LYAPUNOV - KRASOVSKII FUNCTIONALS

Аннотация научной статьи по математике, автор научной работы — Kuptsova Svetlana E., Kuptsov Sergey Yu.

The nonlinear time-delay systems are considered and the limiting Behavior of their solutions is investigated. The case in which the solutions have a trivial equilibrium that may not be an invariant set of the system is studied. The junction of Lyapunov - Krasovskii and Razumikhin approaches is applied to obtain sufficient conditions for the existence of an asymptotic quiescent position in the large. In the case when a general system has a trivial solution, new sufficient conditions for its asymptotic stability are obtained. Examples, that illustrate the application of the obtained results, are given.

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Текст научной работы на тему «RESEARCH OF THE ASYMPTOTIC EQUILIBRIUM OF TIME-DELAY SYSTEMS BY JUNCTION OF LYAPUNOV - KRASOVSKII AND RAZUMIKHIN APPROACHES»

2022 ВЕСТНИК САНКТ-ПЕТЕРБУРГСКОГО УНИВЕРСИТЕТА Т. 18. Вып. 2

ПРИКЛАДНАЯ МАТЕМАТИКА. ИНФОРМАТИКА. ПРОЦЕССЫ УПРАВЛЕНИЯ

ПРИКЛАДНАЯ МАТЕМАТИКА

UDC 517.929.4 MSC 34K20

Research of the asymptotic equilibrium of time-delay systems by junction of Lyapunov — Krasovskii and Razumikhin approaches

S. E. Kuptsova1, S. Yu. Kuptsov2

1 St Petersburg State University, 7-9, Universitetskaya nab., St Petersburg, 199034, Russian Federation

2 OOO "OGS Russia", 21a, Gakkelevskaya ul., St Petersburg, 197227, Russian Federation

For citation: Kuptsova S. E., Kuptsov S. Yu. Research of the asymptotic equilibrium of time-delay systems by junction of Lyapunov — Krasovskii and Razumikhin approaches. Vestnik of Saint Petersburg University. Applied Mathematics. Computer Science. Control Processes, 2022, vol. 18, iss. 2, pp. 198-208. https://doi.org/10.21638/11701/spbul0.2022.201

The nonlinear time-delay systems are considered and the limiting behavior of their solutions is investigated. The case in which the solutions have a trivial equilibrium that may not be an invariant set of the system is studied. The junction of Lyapunov — Krasovskii and Razumikhin approaches is applied to obtain sufficient conditions for the existence of an asymptotic quiescent position in the large. In the case when a general system has a trivial solution, new sufficient conditions for its asymptotic stability are obtained. Examples, that illustrate the application of the obtained results, are given.

Keywords: time-delay systems, asymptotic stability, asymptotic quiescent position, Lyapu-nov — Krasovskii functionals.

1. Introduction. The second Lyapunov method is the main tool to analyze the qualitative behavior of the solutions of differential equations. For the differential equations with delay, this method includes two approaches as follows. In accordance with the Krasovskii approach [1,2], Lyapunov — Krasovskii functionals are constructed as Lyapunov functions for stability analysis. In accordance with the Razumikhin approach [3,4] the motion equations are studied using the classical Lyapunov function but its derivative along the trajectories of the system is estimated not on the whole set of its integral curves but on some subset. The junction of these approaches is also successfully used to analyze the stability of time-delay systems. In [5-7], the idea was proposed to replace the positive definiteness of the functional with this condition on the special Razumikhin-type set of functions only while retaining the other classical conditions. This made it possible to

© St Petersburg State University, 2022

obtain sufficient conditions for the asymptotic stability of time-delay systems of general form, as well as necessary and sufficient conditions for the asymptotic stability of linear time-delay systems.

In this paper we investigate the issue of the existence of an asymptotic quiescent position in nonlinear time-delay systems. The concept of an asymptotic quiescent position for the systems of differential equations was introduced by Zubov in [8] for studying the motions with a limiting behavior for infinitely increasing times in which the limit sets are not the invariant sets of the initial differential equations. A number of papers are devoted to this topic, see, for example, [9-11]. For time-delay systems, the concept of an asymptotic quiescent position was introduced in [12], and in papers [13, 14] some sufficient condition for it existence have been established. In this paper we present a modification of the sufficient conditions for the existence of an asymptotic quiescent position. The main idea is to add to the condition of positive definiteness of the functional one more condition, which must be satisfied on the special Razumikhin-type set of functions. This made it possible to weaken the restrictions on the derivative of the functional with respect to the solutions of the system (in comparison with [12]), but at the same time strengthened the restriction on the choice of the functional itself. In general terms, the difference between the result obtained in [12] and the one presented here is most easily demonstrated by-systems with perturbations of the following type:

x = F (t,xt) + R(t,xt),

where the system

x = F (t, xt)

has an asymptotically stable trivial solution, and a functional R(t, xt) such that

\\R(t,xt)\\ < Y(t) —> 0 as t —>

In [12], the existence of an asymptotic quiescent position is guaranteed by the condition of the convergence of the improper integral of the function j(t). In the present paper, this condition is not needed. However, on the functional V(t,xt), with the help of which the system is investigated, an additional condition is imposed, the essence of which is as follows: V must be an increasing function of the norm \\x\\h.

2. Preliminaries. Consider the time-delay system

x = f (t,x(t),x(t - h)), (1)

where x(t) e Rn and the time-delay h > 0. Let the vector--valued function f (t, x, y) be defined for t > 0 x e Rn and y e Rn. We assume that this function is continuous in

xy

From now on we assume that initial functions belong to the space of continuous vector functions C([-h, 0],Rn) and denote X = C([-h, 0],Rn), R+ = {t e R1 | t > 0}. It is well known from [15], that the above restrictions on the right-hand side of system (1) ensure the existence and uniqueness of a solution x(t, t0, y) for any t0 e R+ and y e X. For given to e R+ and y e X the state of the system at time t is defined as

xt(to,y) = x(t + s, to, y), s e [-h, 0].

From now on we use the Euclidian norm for vectors, and for functions y e X we use the uniform norm:

\\y\\h = suP \\y(s)\\.

s£[-h,0]

Definition 1. The position x = 0 is called a asymptotic quiescent position in the large if all solutions of system (1) are defined on the set t > t0 and

\\x(t,to,p)\\—> 0 as t —>

Let the function X(t) be defined and continuous for each t e R+.

Definition 2. A function W(t, x) is called negative definite on the set ||x|| > X(t) if the following conditions are satisfied:

a) W(t, x) is continuous in the variables on the set t e R+, x e Rn;

b) W(t,x) < -W1(x) on the ||x|| > X(t), where a function W1(x) is continuous and

x e Rn

Let a functional V(t, p) be defined on the set X for each t e R+. This functional will be understood as a mapping V : R+ x X ^ R1.

Definition 3. The functional V(t, p) is said to be continuous on the set R+ x X if for any e > 0 t e R+ and p e X there exists a value S > 0 such that, for any t e R+ and ^ e Xwith \t - t\ + Hp - <S, \V(t,p) - V(t,^)\ <e.

If we substitute a solution x(t,t0,p) into the functional V we get a function v(t) = V(t,xt(to, p)).

Definition 4. The derivative of the functional V(t,xt) along the solution x(t,t0,p) is the functional W(t,xt) which satisfies the following condition:

V(t) = W (t,xt(to,p)).

This identity should hold for all t > t0 for which the right-hand side is defined. Such a functional W(t, xt), if it exists, will be denoted by V\(1)(t,xt). And in this case the V(t, xt)

3. Sufficient condition for the existence of asymptotic quiescent position in the large. Let us suppose for each H > 0 the function f (t,x,y) is uniformly bounded in t > 0 on the set ||x|| < H, ||y|| < H, and introduce the set

S = {p e X | ||p(s)|| < Hp(0)l s e [-h,0)}.

Theorem 1. Let V(t,xt) and W(t,xt) be continuous on the set R+ x X junctionals satisfying the conditions:

• V1( Hx(t)H) < V (t,xt) < V2( HxtHh), where the func tionsV1(r) an dV2(r) are positive definite on the set r > 0, and V1 (r) ^ as r ^

• there exi sts S > 0 such th at v(t) > v(£) for all £ e [t - S,t) an d xt e S;

• V\(1)(t,xt) = W(t,xt) < W1(t,x), where the function W1(t,x) is negative definite on the set ||x|| > A(t);

• lim sup W\(t, x) < 0;

||z||<A(t)

• X(t) e C0([0, X(t) > 0 and X(t) ^ 0 as t ^

then x = 0 is asymptotic quiescent position in the large for trajectories of system (1).

Proof. We consider an arbitrary t0 > 0 and an arbitrary initial function p(t) e C0[t0 - h,t0]. By virtue of the conditions of the theorem, the functionals V(t,xt) and W(t, xt) are defined and continuous on the set R+ x X, consequently, for v(t) = V(t, xt(t0,p)) the equality V(t) = w(t) = W(t,xt(t0,p)) will be satisfied over the entire interval of the existence of the solution t e [t0, T(t0, p)). Thus, for all a Mid b from

[to, T(t0, y)) we have

b

v(b) = v(a) ^y w(t) dt. (2)

a

It's clear that T(t0, y) may be equal to For the sake of simplicity we denote x(t, t0, y) by x(t). □

1. Let us prove that x(t) is defined on the interval [t0, Assume the converse. Let there exists a moment of time t* > t0 such that x(t) is defined for all t e [t0,t*) and not defined for t = t*. Then, on the one hand, either there exist a constant H0 > 0 and a sequence Tk ^ t* — 0 such th at \\x(Tk )\\ < H0 for all k > 1, that contradicts the existence and uniqueness theorem of the main initial problem, or

\\x(t)\\ —»as t —> t* — 0.

Then from the first condition of the theorem it follows that

v(t) —> as t —> t* — 0. (3)

On the other hand, from the fifth condition of the theorem it follows that there exists ti > t0 such that \\x(t)\\ > X(t) for all t e [t1,t*). Therefore, using the third condition of the theorem, we have v(t) < v(t1) for all t e [t1,t*), that contradicts relation (3).

2. Let us prove that x(t) is bounded on the interval [t0, From the fifth condition of the theorem it follows that there exists a constant L1 > 0 such th at X(t) < L1 for all t > 0. Let L2 > 0 be a constat such that \\y\\h ^ L^^d L = max{L1, L2}. Assume that x(t) is unbounded on the set t > t0, then there exists a moment of time T > t0 such that \\x(T)\\ = 2L and \\x(t)\\ < 2L for all t e [t0,T). This means that xT e S, consequently, v(T) > 0. (It follows from second condition of Theorem 1.) But by virtue of third condition of the theorem we have v(T) < 0. This contradiction means that x(t) < 2L for all t > t0.

3. Let us prove that x(t) ^ 0 as t ^ Assume the converse. Let there exist a value a > 0 and sequenee tk ^ as k ^ such that

\\x(tk)\\ > a for all k > 1. (4)

Two situations are possible:

(A) there exists T1 > t0 such th at \\x(t)\\ > X(t) for all t > T1;

(B) there exists sequence of intervals (Tk,Tk), Tk ^ as k ^ such that \\x(t)\\ < X(t) for any t e (Tk,Tk), and \\x(t)\\ > X(t) for any t e [tk,Tk+1].

Remark 1. The function X(t) ^ 0 as t ^ consequently, for any a > 0 it is possible to find a moment of time T2 > 0 such th at X(t) < a/2 for all t > T2. Let there exist 9\ and 02, T2 < 0\ < 02, having the property that ||x(0i)|| = f, ||x(02)|| = a and ||x(t)|| G [§,«] as t e [0it92\. In this case for each t e [0i,02], x(t) belongs to the set ||x|| > A(t) on which the function W\{t,x) is negative definite. Then there exist a positive definite in Rn function W(x) such that W\{t,x) < — W(x) on the set ||x|| > A(t).

For any /31 > ^d f32 > 0 A < we define a value

7(/3i,/32)= min W(x), 7 > 0.

Applying the relation (2) in the limits from ^ to 02 and third condition of the theorem, we obtain

O2 O2

v{e2)-v{e1)^ i Wi{T,x{T))d,T iw{x{T))d,T ^-1{e2-ei). (5)

We denote nij = sup \fi(t, x, y)\ on the set t > 0, ||x|| < 2 L, \\y\\ <2 L, M = y/m\ + ... + to2 and applying Lagrange's theorem on the mean value, estimate the length of [0i,02]:

a

-<C||x(02)-x(0i)

\

J2(xi(02) - Xi(e1))2 = (02 - 0l)

i=1

52f?(MSi),x(Si - h)) <

i=1

< (02 - 0i)^m2 + ... + m2 = M(02 - 01).

Here xi(r ) is i-th coordinate of the vector-function x(t ) and & G [0i,02], i = l,...,n. Thus,

a

<6>

Let us consider the situation (A). There are two cases of situation (A): (Al) there exist ai > 0 Mid T3 > Ti such that ||x(t)|| G [ai, 2L] for all t > T3; (A2) there exists sequence tk ^ as k ^ such that Hx(tk)|| ^ 0 as k ^ In case (Al) there exists T > T3 such that X(t) < a1 for t > T. So x(t) belongs to the set ||x|| > X(t) as t > T, then, by virtue of Remark 1, we have

t t v(t) -v(T) < J Wi(t, x(t)) dr W(x(r))dr < -7(0:1, 2L)(t - T).

T T

This inequality contradicts the non-negativity of the function v(t) for t > T + ^p-.

In case (A2) there exist a value a > 0 and a sequence of segments [0k, 0k], 01 > T, 9k ->• +cx) as k ->• +cx) such that ||x(0fc)|| = a/2, ||x(0fc)|| = a and ||x(t)|| G [§,«] as t G [0k ,0k ]. Applying Remark 1, for each t > T2, we get

t m(t)

v(t) < v(0i)+ Wi(t,x(t )) dT < v(0i) - 7 (a/2,a)YJ(0k — 0k), (7)

e\ k=

where m(t) ^ as t ^ By virtue of Remark 1 and estimate (6), for all k > 1 the following inequality holds:

0^ — Oh —TTi

2M

consequently, the right-hand side of inequality (7) tends to —to as t ^ This contra-

v(t)

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(A) is impossible.

Let us consider situation (B). First we define a value e = , where a, 7, M

are the values defined in Remark I. Further, without loss of generality, we assume that

tk | x( t) |

two cases of situation (B):

(Bl) there exists a number k*, tk* > T2 such th at xtk, G S;

(B2) for any number k such that tk > T2, there exists t g [tk — h,tk) such that

l|x(T)|| > llx(tk)||. (8)

In case (Bl), on the one hand, from the second condition of the theorem it follows that v(tk*) > 0. On the other hand, \\x(tk* )|| > \(tk*), consequently, v(tk*) < 0. Thus, case (Bl) is impossible.

In case (B2) we note that \\x(tk)\\ g [a, 2L] and denote values

ni = min Vi(r) and n2 = max V2(r).

re[a,2L] re[a,2L]

Then, by virtue of first condition of the theorem, v(tk) G [ni,n2] and, consequently, there exist a value n G [ni,n2] and sequence v(tks) ^ n as s ^ Therefore, for the selected number e there exists natural number s* such that

n - e < v(tks) < n + e for all s > s*. (9)

Let us note that on the set s > s* it is possible to find a segment [tks ,tks+1 ] such that

[tks ,tks+1 ^U^,Tm) = 0. (10)

m=l

Let [tks,tks+1 ] be the segment that satisfies condition (10), then there exists a natural number ls > 1 such that this segment can be represented as follows:

ls-l

[^ks tks + 1 ] = [fks+i tks+i+l] tks+ls = tks + 1

i=0

Let us consider a segment [tks +i,tks+i+i] and note that either \\x(t)\\ > X(t) for t G

[tks+i,tks+i+l], then

v(tks+i+l) - v(tks+i) < 0, (11)

or there exist intervals (Tm,Tm) G [tks+i,tks+i+i], m = 1,...,pu such that \\x(t)\\ < X(t) for t G (Tm, Tm ). From the fourth condition of the theorem it follows that there exists a continuous and non-negative as t G R+ function A(t) satisfying the following conditions: (CI) A(t) > sup Wi(t,x); M<\(t)

(C2) A(t) ^ 0 as t ^ +<x.

From (C2) we have that there exist a moment of time T4 > T2 such that

a+h

J A(t) dt < 4e for all a > T4. (12)

a

From (4) and (8) it follows that there exist quantities ^ > ^d S2 > 0 such that (Dl) \x(tks+i + Si)\\ = a aid \x(tks+i+l - ¿2)\ = a; (D2) \\x(t)\\ <aast G [tks+i + Si,tks+i+i - S2]; (D3) 0 < tks+i+i - S2 - tks+i + Si <h.

From (Dl) and (D2) it follows that there exists ^ G [tks+i + S^ Ti^d Z2 G [Tpi,tks+i+i - S2] such that \\x((i)\\ = a/2, \\x(t)\\ G [a/2,a] as t G [tks+i + Su(i] and \\x(Z2)\\ = a/2, \\x(t)\\ G [a/2,a] as t G [Z2,tks+i+i - ¿2]; and from (D3) we have 121m=l(Tm - Tm) < h. Applying relation (2) in the limits from tks+i to tks+i+i, for each i G [0, ls - 1] we get:

Cl C2

(tks+i+i) - v(tks +i) ^ J w1(t) dt + J w1(t) dt + J w1 (t) dt +

tks+i tks+i + Si Zl

tks +i+1 — ¿2 tks+i+1

+ J wi(t) dt + J wi(t) dt = Ii + I2 + I3 + I4 + I5,

(2 tks+i+1—S2

here wi(t) = Wi(t,x(t)). Let us estimate each torn of this sum on the set s > s* and tks > T4:

• Ii < ^d I5 < 0 by virtue of the third condition of the theorem;

• !■> s' —"'tya!22^a and /4 s' —"'tya!22^a by virtue of inequalities (5) and (6) of Remark 1;

• to estimate I3, we represent the segment [Zi,Z2] the Mowing form [Zi,Z2] = toil) ^2, where fii = {t G [Zi ,Z2] \ \\x(t)\\ > X(t )},and to = {t G [Zi,Z2 ] | \\x(t)\\ < X(t)}. Then, using relation (12), inequality (C1) and the third condition of the theorem, we get

I3 = J wi(t) dt + J wi (t) dt wi (t) dt A(t) dt < 4e.

Q2

Consequently, for each i G [0,ls - 1^, for each s > s* and for each tks > T4 the inequality holds

v(tks +i+i) - v(tks+i) < -4e. (13)

Thus, using relation (2) in the limits from tks to tks+1 and also (9)—(11), (13), we obtain the following contradiction:

tks+i+1

ls-i

-2e < v(tks+1) - v(tks ) = Y^ / wi(t) dt< -4lse < -4e.

i = 0 tks+i

So the situation (B) is impossible and x(t) —> 0 as t ^ The theorem is proved.

4. Sufficient condition of asymptotic stability. Further we abandon the condition uniformly boundedness of the vector-function f (t, x, y) with respect to t > 0 on the set \\x\\ < H, \\y\\ < H, and assume that system (1) has a trivial solution.

Theorem 2. Let V(t,xt) and W(t,xt) be continuous on the set R+ x X junctionals satisfying the conditions:

• \\x(t)\\) < V (t,xt) < V2^\\xt\\h), where the func tionsVi(r) an dV2(r) are positive definite on the set r > 0, and 0 < r < H;

• there exists S > 0 such that v(t) > v(£) for all £ G [t - S,t) and xt G S;

• V\(i)(t,xt) = W(t,xt) < Wi(t,x), where the function Wi(t,x) is negative definite on the set X(t) < ||x|| < H;

• lim sup W\(t, x) < 0;

boo

ж

l<A(t)

• X(t) G C0([0, X(t) > 0 md X(t) ^ 0 as t ^

then the trivial solution of the system (1) is asymptotically stable.

Proof. Let us show that the trivial solution of system (1) is Lyapunov stable, i. e. for every e > 0 Mid t0 > 0 there exists S = S(e,t0) > 0 such that for any initial functions y G X, \\y\\h < S, we have ||x(t,t0,^>)|| < e for all t > t0. □

Let us set an arbitrary number e > 0. From firth condition of Theorem 2 it follows that there exists a moment T > to such that X(t) < e/2 as t > T. Since x(t,t0, p) depends continuously on p (see, for example [15]), by the values e and T we can find a number S e (0,e) such that if \\p\\h < J, then ||x(t,t0,p)|| < e/2 for all t e [t0,T],

Suppose, that there exists t* > T such th at ^(t^to, p)|| = e. And let t* be the first moment when the solution x(t,t0,p) reaches the sphere \\x\\ = e.

Then on one side xt.t e ^d v(t*) > 0; and on the other side v(t*) < 0 by virtue of third condition of Theorem 2. This contradiction proofs the Lyapunov stability of trivial solution of system (1).

The proof of the asymptotic stability of the trivial solution will repeat the proof of the third item of Theorem 1, with the only difference that estimate (6) can be obtained using the fact that system (1) has a trivial solution and the right-hand side of system (1) satisfies the Lipschitz condition. The theorem is proved.

Remark 2. Note that the verification of the second condition of the above theorems in the general case seems to be very difficult. However, it can be easily verified for a wide class of functionals.

Examples. In this part, the application of the above theorems is illustrated by the examples of scalar nonlinear differential-difference equation. Let us consider the equation

x = -2x3(t) + x3(t -h)+ 1 (14)

v 1 +1

and the functional

t

V = x4(t)+ J x6(s) ds. (15)

t-h

This functional is continuous in the sense of Definition 3 and satisfies the first condition of

Theorem 1, where Vi(\\x\\) = ||x\\4 and V2(\\x\\h) = \\x\\h + fo\\x\\h- The second condition

of Theorem 1 is satisfies too, since if xt e S, then x4 (t) > x4 (£) as £ e [t — h,t) and,

t

consequently, the function 7(t) = f x6(s) ds satisfies the condition j(t) > 0. Thus,

t-h

a value S from second condition of Theorem 1 there exists. The functional W(t,xt) = —7x6(t) + Ax3(t)x3(t — h) + ttj^j —x6(t — h) is also continuous in the sense of Definition 3. Along an arbitrary solution x(t) = x(t,t0,p) of equation (14) the function v(t) that can be found using the basic rules of differentiation, coincides with W(t,xt(t0,p)). Then, by-virtue of Definition 4, we have

V\{u)(t,xt)= W (t,xt),

4x3(t)

where

W{t, xt) = —7x6(t) + 4x3(t)x3(t -h)+ ;; w - xti(t -h) =

ГШ

—3x6(t) - (2 x3(t) - x3(t - h)f + igl < —3x6(t) + = Wl(t, x(t)).

If we put

Wi{t,x) = - 3x6 + 4^= and A(t) — 2

n+t v 7 ^TTt'

then we get

5 2

W\{t,x) < —7:x& 011 the set \x\ >

2 a/ 1 + t

Thus, the function Wi (t, x) is negative definite on the set \x\ > X(t):

32

sup Wi(t, x) < - —> 0 as t —> +oo,

M<A(t) (v1+1)2

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consequently, the forth condition of Theorem 1 is satisfies too. Therefore, all hypotheses of Theorem 1 are true, and the position x = 0 is a asymptotic quiescent position in the large for equation (14). Let us note that

/sup Wi(t, x) dr = / —, — dr = +oo,

IMKAM u ' ; J (^1+7)2

0

so we cannot apply Theorem 1 from [12], at least if we use the same functional V and the same function X(t).

Let us consider the equation

x = -2х3Ше* + x3(t -h)+ XJ-L (16)

л/TTt

and the functional (15). Repeating the reasoning from the previous example, we get

4x4(t)

V\{16)(t, xt) = —7eix6(t) + 4x3(t)x3(t - h) + -x6(t-h)^

V1 +1

< —3x6(t) - (2x3(t) - x3(t - h)f + i^E < —3x6(t) + i^E = W^xitj). If we put

4t4 2

Wi (t, x) = -3x6 + and A(t)

ут+t v 7 ^T+t'

then we get

2

Wi{t,x) < —2x on the set |ж| >

yT+t

Thus, the function Wi (t, x) is negative definite on the set \x\ > X(t):

64

sup W\(t,x) ^--> 0 as t +oo,

M<A(t) 1+t

consequently, all conditions of Theorem 2 are satisfies and therefore, the trivial solution of equation (16) is asymptotically stable.

5. Conclusion. This paper contains the further research of the problem of the existence of asymptotic equilibrium in time-delay systems, which was started in [12].The synthesis of Lyapunov — Krasovsky and Razumikhin approaches made it possible to weaken the restrictions on the functional W(t,xt), in comparison with [12]. Thus, it turned out to be possible to solve the question of the existence of asymptotic equilibrium for a wider class of systems.

References

1. Krasovskii N. N. Nekotorye zadachi teorii ustoichivosti dvizheniya [Some problems in the theory of motion stability}. Moscow, Fizmatlit Publ., 1959, 211 p. (In Russian)

2. Alexandrova I. V., Zhabko A. P. Funkcionaly Lyapunova — Krasovskogo dlya odnorodnyh sistem s neskol'kimi zapazdyvaniyami [Lyapunov — Krasovskii functionals for homogeneous systems with multiple delays]. Vestnik of Saint Petersburg University. Applied Mathematics. Computer Science. Control Processes, 2021, vol. 17, iss. 2, pp. 183-195. https://doi.org/10.21638/11701/spbul0.2021.208 (In Russian)

3. Razumikhin B. S. On stability of delayed systems. J. Appl. Math. Mech., 1956, vol. 56, no. 2, pp. 500-512.

4. Razumikhin B. S. The application of Lyapunov's method to problems in the stability of systems with delay. Autom. Remote Control, 1960, vol. 21, no. 6, pp. 740-748.

5. Medvedeva I. V., Zhabko A. P. Synthesis of Razumikhin and Lyapunov — Krasovskii approaches to stability analysis of time-delay systems. Automatica, 2015, vol. 51, no. 1, pp. 372-377.

6. Alexandrova I. V., Zhabko A. P. At the junction of Lyapunov — Krasovskii and Razumikhin approaches. 15 Jul. 2018 IFAC-PapersOnLine, 2018. https://doi.Org/10.1016/j.ifacol.2018.07.214

7. Alexandrova I. V., Zhabko A. P. Lyapunov direct method for homogeneous time delay systems. 15 Dec. 2019 I FA C-Papers Online, 2019. https://doi.Org/10.1016/j.ifacol.2019.12.210

8. Zubov V. I. Kolebaniya i volny [Oscillations and waves]. Leningrad, Leningrad State University Press, 1989, 416 p. (In Russian)

9. Kuptsova S. E. Asimptoticheskie invariantnye mnozhestva [Asymptotically invariant sets]. Trudy 37 Mczhdunarodnoi konferencii "Protsessy upravleniya i ustoichivosti" [Proceedings 37th Intern. Conference "Control Processes and Stability"], 2006, pp. 50-56. (In Russian)

10. Kuptsova S. E. On asymptotic behavior of the solutions of systems of nonlinear time-varying differential equations. Middle Volga Mathematical Society Journal, 2006, vol. 8, no. 1, pp. 235-243.

11. Zhabko A. P., Tikhomirov O. G., Chizhova O. N. Ustoichivost' asimptoticheskogo polozheniya pokoya vozmushchyonnyh odnorodnyh nestatsionarnyh sistem [Stability of asymptotic equilibrium of perturbed homogeneous time-varying systems]. Middle Volga Mathematical Society Journal, 2018, vol. 20, no. 1, pp. 13-22. (In Russian)

12. Kuptsova S. E., Kuptsov S. Yu., Stepenko N. А. О predel'nom povedenii reshenii sistem diffe-rentsial'nykh uravnenii s zapazdyvaiushchim argumentom [On the limiting behavior of the solutions of systems of differential equations with delayed argument]. Vestnik of Saint Petersburg University. Applied Mathematics. Computer Science. Control Processes, 2018, vol. 14, iss. 2, pp. 173-182. https://doi.org/10.21638/11701/spbul0.2018.205 (In Russian)

13. Zaranik U. P., Kuptsova S. E., Stepenko N. A. Dostatochnye usloviya sushchestvovaniya asimptoticheskogo polozheniya pokoya v sistemah s zapazdyvaniem [Sufficient conditions for the existence of an asymptotic quiescent position in time-delay systems]. Middle Volga Mathematical Society Journal, 2018, vol. 20, no. 2, pp. 175-186. (In Russian)

14. Kuptsova S. E., Stepenko N. A., Kuptsov S. Yu. Sufficient conditions for the existence of asymptotic quiescent position for one class of differential-difference systems. Automation and Remote Control, 2019, vol. 80, pp. 1016-1025. https://doi.org/10.1134/S000511791906002X

15. Kharitonov V. L. Time-delay systems: Lyapunov functionals and matrices. Basel, Birkhauser, 2013, 322 p.

Received: November 19, 2021.

Accepted: May 05, 2022.

Authors' information:

Svetlana E. Kuptsova — PhD in Physics and Mathematics, Associate Professor; sekuptsova@yandex.ru

Sergey Yu. Kuptsov — PhD in Physics and Mathematics, Mathematician-Programmer; srgkuptsov@yandex.ru

Синтез подходов Разумихина и Ляпунова — Красовского при исследовании асимптотического равновесия в системах с запаздыванием

С. Е. Купцова1, С. Ю. Купцов2

1 Санкт-Петербургский государственный университет, Российская Федерация, 199034, Санкт-Петербург, Университетская наб., 7-9

2 ООО «ОГС Руссия», Российская Федерация, 197227, Санкт-Петербург, Гаккелевская ул., 21а

Для цитирования: Kuptsova S. Е., Kuptsov S. Yu. Research of the asymptotic equilibrium of time-delay systems by junction of Lyapunov — Krasovskii and Razumikhin approaches // Вестник Санкт-Петербургского университета. Прикладная математика. Информатика. Процессы управления. 2022. Т. 18. Вып. 2. С. 198-208. https://doi.org/10.21638/11701/spbul0.2022.201

В статье изучаются нелинейные системы с запаздывающим аргументом и исследуется предельное поведение их решений. Рассмотрен случай, когда решения стремятся к нулевому предельному положению, которое, в свою очередь, может не быть инвариантным множеством системы. На стыке подходов Ляпунова — Красовского и Разу-михина получены достаточные условия существования асимптотического положения покоя в целом. В случае, когда система имеет тривиальное решение, определены новые достаточные условия его асимптотической устойчивости. Приведены примеры, иллюстрирующие применение приведенных результатов.

Ключевые слова: системы с запаздыванием, асимптотическая устойчивость, асимптотическое положение покоя, метод функционалов Ляпунова—Красовского, подход Ра-зумихина.

Контактная информация:

Купцова Светлана Евгеньевна — канд. физ.-мат. наук; доц.; sekuptsova@yandex.ru Купцов Сергей Юрьевич — канд. физ.-мат. наук; srgkuptsov@yandex.ru

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