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Miskolc Mathematical Notes HU e-ISSN 1787-2413 Vol. 19 (2018), No. 1, pp. 241–247 DOI: 10.18514/MMN.2018.2541

STABILITY OF TRIVIAL TORUS OF NONLINEAR MULTIFREQUENCY SYSTEMS VIA SIGN-DEFINITE

QUADRATIC FORMS

PETRO FEKETA, OLENA A. KAPUSTIAN, AND MYKOLA M. PERESTYUK Received 28 February, 2018

Abstract. This paper studies stability properties of the trivial invariant torus of a class of non- linear extensions of dynamical systems on torus. Two theorems on exponential stability and instability of the invariant torus in terms of quadratic forms that are sign-definite in nonwander- ing set of the dynamical system have been proven.

2010Mathematics Subject Classification: 34C46; 34C45; 34D35 Keywords: invariant tori, multifrequency oscillations, stability

1. INTRODUCTION

Fundamental results of the qualitative theory of multifrequency oscillations, in particular, the problems of the existence and stability of invariant sets of dynamical systems defined in the direct product ofm-dimensional torus andn-dimensional Eu- clidean space, have been developed by A. M. Samoilenko and summarized in [12].

In [6], the stability properties of invariant tori have been studied in terms of sign- definite quadratic forms. In this paper, we establish new conditions for exponential stability and instability of the trivial invariant torus of nonlinear extension of dy- namical system on torus which are formulated in terms of quadratic forms that are sign-definite not on the entire surface of the torus, but in nonwandering set [7] of dynamical system on torus only. The corresponding results for linear extensions of dynamical systems on torus have been obtained in [1,3,8–11].

2. MOTIVATION AND PROBLEM STATEMENT

We consider a system of ordinary differential equations defined in the direct product ofm-dimensional torusTmandn-dimensional Euclidean spaceRn

d'

dt Da.'/; dx

dt DP .'; x/x; (2.1)

c 2018 Miskolc University Press

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where'D.'1; : : : ; 'm/T 2Tm,xD.x1; : : : ; xn/T 2Rn, functionP is continuous in TmRnand for everyx2RnP .; x/; a./2C.Tm/;C.Tm/is a space of continuous 2-periodic with respect to each of the component'v,vD1; : : : ; mfunctions defined onTm.

We assume that the following conditions hold:

9M > 0such that8.'; x/2TmRn kP .'; x/k MI (2.2) 8r > 09LDL.r/ > 0such that8x0; x00;kx0k r;kx00k r;8'2Tm

P .'; x00/ P .'; x0/ L

x00 x0

I (2.3)

9A > 0 8'0; '002Tm

a.'00/ a.'0/ A

'00 '0

: (2.4)

Condition (2.4) guarantees that the system d'

dt Da.'/ (2.5)

generates a dynamical system onTm, which we will denote by't.'/.

Definition 1([7]). A point '2Tm is called a nonwandering point of dynamical system (2.5) if there exist a neighbourhoodU.'/and a moment of timeT DT .'/ > 0 such that

U.'/\'t.U.'//D¿ 8tT:

Let us denote by˝a set of all nonwandering points of dynamical system (2.5). Since Tmis a compact set, the set˝is nonempty, invariant, and compact subset ofTm[12].

Additionally, the following holds:

Lemma 1([7]). For any" > 0there existT ."/ > 0andN."/ > 0such that for any '62˝the corresponding trajectory't.'/ spends only a finite time that is bounded byT ."/outside the"-neighbourhood of the set˝, and leaves this set not more than N."/times.

Definition 2([12]). Trivial invariant torus xD0; '2Tm

of the system (2.1) is called exponentially stable if there exist constantsK > 0, > 0, andı > 0such that for all'2Tmand for allx02Rn,kx0k ıit holds that

8t0 kx.t; '; x0/k Kkx0ke t; (2.6) wherex.t; '; x0/is a solution to the Cauchy problem

dx

dt DP .'t.'/; x/x; x.0/Dx0: (2.7) In [5], the conditions for the exponential stability of the trivial invariant torus of the system (2.1) have been established in terms of the properties of function'7!P .'; 0/

in the nonwandering set˝of dynamical system (2.5):

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Lemma 2([5]). Let

8'2˝ .'; 0/ < 0; (2.8)

where.'; x/is the largest eigenvalue of the matrix P .'; x/O D 1

2

P .'; x/CPT.'; x/

:

Then, the trivial invariant torus of system(2.1)is exponentially stable.

The following example demonstrates the case when the trivial invariant torus is exponentially stable (this will be proven in Theorem1), however the condition (2.8) does not hold.

Example1. Consider a system defined inT1R2 d'

dt D sin2' 2

; (2.9)

dx1

dxdt2

dt

! D

sin.'Cx1Cx2/x1 x2

x1 sin.x1 x2 '/x2

: (2.10)

Dynamical system on torusT1that are generated by (2.9) has a nonwandering set

˝D f'D0g: However, the matrix

P .0;O 0/N D 0 0

0 0

does not fulfill condition (2.8).

The main results of this paper are theorems on exponential stability and instability of the trivial torus of the systems of a class (2.9) with conditions given in terms of quadratic forms that are sign-definite in nonwandering set˝of dynamical system on torus only.

3. MAIN RESULTS

For any'2Tm,x2Rnlet us denote S .'; x/O D@S.'; x/

@' a.'/C@S.'; x/

@x .P .'; x/x/

CS.'; x/P .'; x/CPT.'; x/S.'; x/;

(3.1)

whereSDS.'; x/is a symmetric matrix of a classC1.TmRn/.

Theorem 1. Let there exist a symmetric matrixSDS.'; x/of the classC1.Tm Rn/such that

8'2˝ S.'; 0/ > 0; S .'; 0/ < 0:O (3.2) Then, the trivial torus of system(2.1)is exponentially stable.

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Proof. Due to the conditions (3.2) and continuous dependence of the polyno- mialFLs roots on the coefficients [4], we get that for somer > 0, > 0the following inequalities hold

8'2Or.˝/ 8x2Rn;kxk< r S.'; x/E; S .'; x/O E: (3.3) Also, there exists a constantCDC.r/ > 0such that for all'2Tmand for allx2Rn, kxk r

kS.'; x/k C k OS .'; x/k C: (3.4) Denote by

V .'; x/D.S.'; x/x; x/: (3.5)

Let

'2Or.˝/ and 8s0 's.'/2Or.˝/:

Then, for the solution to (2.7)x.t /Dx.t; '; x0/withkx0k< rthe following estimate kx.t /k< rholds fort2Œ0; T /,0 < T C1. Hence, from (3.3),

kx.t /k2V .'t.'/; x.t //Ckx.t /k2; d

dtV .'t.'/; x.t // kx.t /k2 hold fort2Œ0; T /. From the last inequalities we get that

V .'t.'/; x.t //V '; x0 e Ct:

Hence, there exist constantsK1> 0and1> 0such that8t2Œ0; T /

kx.t /k K1kx0ke 1t: (3.6) Forkx0k< Kr

1 we obtain thatT D C1and the inequality (3.6) holds for allt0.

Now, let'2Or.˝/, but there existst1> 0such that

8t2Œ0; t1/ 't.'/2Or.˝/; 't1.'/62Or.˝/:

From Lemma1, there exist

N.'; r/N.r/; fi.'; r/gN.';r/iD1 C1; fti.'; r/gN.';r/iD1 N.';r/C1

X

iD1

i.'; r/DWT .'; r/T .r/

such that

't.'/2Or.˝/

8t2.0; t1/[

N.';r/ 1

[

kD1

Xk

iD1

.iCti/;

k

X

iD1

.iCtiC1/ [

N.';r/

X

iD1

.iCti/;C1 :

(3.7)

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Then, fort2Œ0; t1

kx.t /k K1kx0ke 1t < r if kx0k< r K1

:

Fort2Œt1; t1C1, from (2.2) and Wazewski inequality [2], kx.t /k kx.t1/keM.t t1/

K1kx0ke.1CM /1e 1t

< r if kx0k< r K1e.1CM /1: Fort2Œt1C1; t1C1Ct2,

kx.t /k K12kx0ke.1CM /1e 1t < r if kx0k< r K12e.1CM /1: Continuing this process, due to (3.7), finally we get:

for KWDK1N.r/e.CM /T .r/; ıWD r

K1N.r/e.CM /T .r/

; kx0k< ı;

8t0 kx.t /k Kkx0ke 1t: (3.8) Now, let us consider the case of'62Or.˝/. In this case,

802.0; T .r// '0.'/2Or.˝/

and

8t2Œ0; 0 kx.t /k kx0ke.MC1/T .r/ke 1t: Then, for

O

KDKe.CM /T .r/; ıOD ı e.CM /T .r/

we obtain the required estimate (2.6). This completes the proof.

Example 2 (revisited). Let us illustrate the usage of Theorem 1 for the system (2.9), (2.10). Let

SDS.'; x/D 2 1

1 1

> 0

Then,

S .0;O 0/N D

2 1

1 2

< 0

which guarantee exponential stability of the trivial invariant torus.

The following theorem provides sufficient conditions for instability of the trivial torus of system (2.1) in terms of sign-definite on the set˝quadratic forms.

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Theorem 2. Let there exist a symmetric matrixSDS.'; x/of the classC1.Tm Rn/ such that for the matrix (3.1) and for the quadratic form (3.5) the following conditions hold:

8'2˝ S .'; 0/ > 0;O (3.9)

8ı > 09x02Rn; kx0k< ı; 9'02˝ such that V .'0; x0/ > 0: (3.10) Then, the trivial torus of system(2.1)is unstable.

Proof. From (3.9) and (3.3),9ˇ > 0and9r > 0such that 8'2˝ 8x2Rn;kxk< r S .'; x/O ˇE:

Let for arbitraryı > 0(ı < r), the correspondingx0,'0are from the condition (3.10), andx.t /Dx.t; '0; x0/is the solution to the Cauchy problem (2.7). Next, we show that9t1> 0such thatkx.t1/k Dr. This will be sufficient to prove instability.

Suppose the opposite: Let

8t0 kx.t /k< r:

Then, for the functionv.t /DV .'t.'0/; x.t //we have:

d

dtv.t /ˇkx.t /k2: (3.11)

From the condition (3.10),v.0/DV .'0; x0/D˛ > 0. Hence,

8t0 v.t /˛: (3.12)

Then,9" > 0such that 8t0kx.t /k ". Really, if it is not so then there exists a sequencetk! 1such thatkx.tk/k !0. Finally,

v.tk/D S.'tk.'0/; x.tk//x.tk/; x.tk/

Ckx.tk/k2!0;

where constantC > 0is from (3.4), which contradicts (3.12).

Then, from (3.11):

v.t /˛C"2t 8t0:

Hence,8t0

kx.t /k2 1

C ˛C"2t :

The latter estimate implies the existence oft1> 0such thatkx.t1/k Dr. This com-

pletes the proof.

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REFERENCES

[1] F. Asrorov, Y. Perestyuk, and P. Feketa, “On the stability of invariant tori of a class of dynamical systems with the Lappo-Danilevskii condition,”Memoirs on Differential Equations and Mathem- atical Physics, vol. 72, pp. 15–25, 2017.

[2] B. Demidovich, “Lektsii po matematicheskoi teorii ustoichivosti.” Moskau: Verlag ‘Nauka’.

Hauptredaktion f¨ur physikalisch-mathematische Literatur. 472 S. (1967)., 1967.

[3] P. Feketa and Y. Perestyuk, “Perturbation theorems for a multifrequency system with pulses.”J.

Math. Sci., New York, vol. 217, no. 4, pp. 515–524, 2016, doi:10.1007/s10958-016-2988-6.

[4] R. A. Horn and C. R. Johnson,Matrix analysis., 2nd ed. Cambridge: Cambridge University Press, 2013.

[5] O. Kapustyan, F. Asrorov, and Y. Perestyuk, “On exponential stability of the trivial torus for a certain class of nonlinear impulsive systems,”Nonlinear Oscil., vol. 20, no. 4, pp. 502–508, 2017.

[6] Y. A. Mitropolsky, A. M. Samoilenko, and V. L. Kulik,Dichotomies and stability in nonautonom- ous linear systems. CRC Press, 2002.

[7] V. Nemytskii and V. Stepanov, “Qualitative theory of differential equations.” (Princeton Mathem- atical Series). New Jersey: Princeton University Press. VIII, 523 p. (1960)., 1960.

[8] M. M. Perestyuk and Y. M. Perestyuk, “On the stability of toroidal manifold for one class of dynamical systems,”Journal of Mathematical Sciences, vol. 228, no. 3, pp. 314–322, 2018, doi:

10.1007/s10958-017-3623-x.

[9] M. Perestyuk and P. Feketa, “Invariant manifolds of one class of systems of impulsive differential equations.”Nonlinear Oscil., N.Y., vol. 13, no. 2, pp. 260–273, 2010, doi:10.1007/s11072-010- 0112-2.

[10] M. Perestyuk and P. Feketa, “On preservation of the invariant torus for multifrequency systems.”

Ukr. Math. J., vol. 65, no. 11, pp. 1661–1669, 2014, doi:10.1007/s11253-014-0887-x.

[11] M. Perestyuk and P. Feketa, “Invariant sets of impulsive differential equations with particularities in!-limit set.”Abstr. Appl. Anal., vol. 2011, p. 14, 2011, doi:10.1155/2011/970469.

[12] A. Samoilenko,Elements of the mathematical theory of multi-frequency oscillations. Dordrecht etc.: Kluwer Academic Publishers, 1991.

Authors’ addresses

Petro Feketa

University of Kaiserslautern, Department of Mechanical and Process Engineering, Gottlieb-Daimler- Straße, Postfach 3049, 67663 Kaiserslautern, Germany

E-mail address:petro.feketa@mv.uni-kl.de

Olena A. Kapustian

Taras Shevchenko National University of Kyiv, Faculty of Computer Science and Cybernetics, Volodymyrska Street 64, 01601 Kyiv, Ukraine

E-mail address:olena.kap@gmail.com

Mykola M. Perestyuk

Taras Shevchenko National University of Kyiv, Faculty of Mechanics and Mathematics, Volodymyrska Street 64, 01601 Kyiv, Ukraine

E-mail address:perestyuknn@gmail.com

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