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International Journal of Engineering Inventions
e-ISSN: 2278-7461, p-ISSN: 2319-6491
Volume 2, Issue 2 (January 2013) PP: 57-64
www.ijeijournal.com P a g e | 57
Periodic Solutions for Nonlinear Systems of Integro-
Differential Equations of Operators with Impulsive Action
Dr. Raad N. Butris
Assistant Prof. Department of Mathematics Faculty of Science University of Zakho
Iraq-Duhok-Kurdistan Region
Abstract:- In this paper we investigate the existence and approximation of the construction of periodic solutions
for nonlinear systems of integro-differential equation of operators with impulsive action, by using the
numerical-analytic method for periodic solutions which is given by Samoilenko. This investigation leads us to
the improving and extending to the above method and expands the results gained by Butris.
Keyword and Phrases:- Numerical-analytic methods existence of periodic solutions, nonlinear integro-
differential equations, subjected to impulsive action of operators.
I. INTRODUCTION
They are many subjects in mechanics, physics, biology, and other subjects in science and engineering
requires the investigation of periodic solution of integro-differential equations with impulsive action of various
types and their systems in particular, they are many works devoted to problems of the existence of periodic
solutions of integro-differential equations with impulsive action . samoilenko[5,6] assumed a numerical analytic
method to study to periodic solution for ordinary differential equation and this method include uniformly
sequences of periodic functionsโ€™ as Intel studies [2,3,4,7,8].
The present work continues the investigations in this direction. These investigations lead us to the
improving and extending the above method and expand the results gained by Butris [1].
๐‘‘๐‘ฅ
๐‘‘๐‘ก
= ๐‘“(๐‘ก, ๐‘ฅ, ๐ด๐‘ฅ, ๐ต๐‘ฅ, ๐‘”(๐‘ก, ๐‘ฅ ๐‘  , ๐ด๐‘ฅ ๐‘  , ๐ต๐‘ฅ(๐‘ ))๐‘‘๐‘ 
๐‘ก
๐‘กโˆ’๐‘‡
), ๐‘ก โ‰  ๐‘ก๐‘–
ฮ”๐‘ฅ ๐‘ก=๐‘ก ๐‘–
= ๐ผ๐‘–(๐‘ฅ, ๐ด๐‘ฅ, ๐ต๐‘ฅ, ๐‘” ๐‘ , ๐‘ฅ ๐‘  , ๐ด๐‘ฅ ๐‘  , ๐ต๐‘ฅ ๐‘  ๐‘‘๐‘ 
๐‘ก
๐‘กโˆ’๐‘‡
)
โ‹ฏ(1.1)
Where ๐‘ฅ โˆˆ ๐ท โŠ‚ ๐‘… ๐‘›
, ๐ท is closed bounded domain.
The vector functions ๐‘“(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค) and ๐‘”(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง) are defined on the domain
๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค โˆˆ ๐‘…1
ร— ๐ท ร— ๐ท1 ร— ๐ท2 ร— ๐ท3 = โˆ’โˆž,โˆž ร— ๐ท ร— ๐ท1 ร— ๐ท2 ร— ๐ท3 โ‹ฏ 1.2
Which are piecewise continuous functions in ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค and periodic in ๐‘ก of period ๐‘‡, where ๐ท1, ๐ท2 and ๐ท3 are
bounded domain subset of Euclidean spaces ๐‘… ๐‘š
.
Let ๐ผ๐‘– ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค be continuous vector functions, defined on the domain (1.2) and
๐ผ๐‘–+๐‘ ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค = ๐ผ๐‘– ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค , ๐‘ก๐‘–+๐‘ = ๐‘ก๐‘– + ๐‘‡ โ‹ฏ 1.3
For all ๐‘– โˆˆ ๐‘ง+
, ๐‘ฅ โˆˆ ๐ท, ๐‘ฆ โˆˆ ๐ท1, ๐‘ง โˆˆ ๐ท2, ๐‘ค โˆˆ ๐ท3 and for some number ๐‘ .
Let the operators A and B transform any piecewise continuous functions from the domain ๐ท to the piecewise
contiuous function in the domain ๐ท1 and ๐ท2 respectively. Moreover ๐ด๐‘ฅ ๐‘ก + ๐‘‡ = ๐ด๐‘ฅ(๐‘ก) and ๐ต๐‘ฅ ๐‘ก + ๐‘‡ =
๐ต๐‘ฅ ๐‘ก .
Suppose that ๐‘“ ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค , ๐‘” ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง , ๐ผ๐‘–(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค) and the operators A, B satisfy the following
inequalities:
๐‘“ ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค โ‰ค ๐‘€, ๐ผ๐‘–(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค) โ‰ค ๐‘, โ‹ฏ 1.4
๐‘“ ๐‘ก, ๐‘ฅ1, ๐‘ฆ1, ๐‘ง1, ๐‘ค1 โˆ’ ๐‘“ ๐‘ก, ๐‘ฅ2, ๐‘ฆ2, ๐‘ง2, ๐‘ค2 โ‰ค ๐พ( ๐‘ฅ1 โˆ’ ๐‘ฅ2 + ๐‘ฆ1 โˆ’ ๐‘ฆ2 +
๐‘ง1 โˆ’ ๐‘ง2 + ๐‘ค1 โˆ’ ๐‘ค2 )
๐‘” ๐‘ก, ๐‘ฅ1, ๐‘ฆ1, ๐‘ง1 โˆ’ ๐‘” ๐‘ก, ๐‘ฅ2, ๐‘ฆ2, ๐‘ง2 โ‰ค ๐‘„( ๐‘ฅ1 โˆ’ ๐‘ฅ2 + ๐‘ฆ1 โˆ’ ๐‘ฆ2 + ๐‘ง1 โˆ’ ๐‘ง2 )
โ‹ฏ 1.5
And
๐ผ๐‘– ๐‘ก, ๐‘ฅ1, ๐‘ฆ1, ๐‘ง1, ๐‘ค1 โˆ’ ๐ผ๐‘– ๐‘ก, ๐‘ฅ2, ๐‘ฆ2, ๐‘ง2, ๐‘ค2 โ‰ค ๐ฟ( ๐‘ฅ1 โˆ’ ๐‘ฅ2 + ๐‘ฆ1 โˆ’ ๐‘ฆ2 +
๐‘ง1 โˆ’ ๐‘ง2 + ๐‘ค1 โˆ’ ๐‘ค2 ) โ‹ฏ 1.6
Periodic Solutions for Nonlinear Systems of Integro-Differential Equationsโ€ฆ
www.ijeijournal.com P a g e | 58
๐ด๐‘ฅ1 ๐‘ก โˆ’ ๐ด๐‘ฅ2 ๐‘ก โ‰ค ๐บ ๐‘ฅ1 ๐‘ก โˆ’ ๐‘ฅ2 ๐‘ก
๐ต๐‘ฅ1 ๐‘ก โˆ’ ๐ต๐‘ฅ2 ๐‘ก โ‰ค ๐ป ๐‘ฅ1 ๐‘ก โˆ’ ๐‘ฅ2 ๐‘ก
โ‹ฏ 1.7
For all ๐‘ก โˆˆ ๐‘…1
, ๐‘ฅ, ๐‘ฅ1, ๐‘ฅ2 โˆˆ ๐ท, ๐‘ฆ, ๐‘ฆ1, ๐‘ฆ2 โˆˆ ๐ท1, ๐‘ง, ๐‘ง1, ๐‘ง2 โˆˆ ๐ท2 and ๐‘ค, ๐‘ค1, ๐‘ค2 โˆˆ ๐ท3 where ๐‘€, ๐‘, ๐พ, ๐‘„, ๐ฟ and ๐บ, ๐ป are a
positive constants.
Consider the matrix
ฮ› =
๐พ1
๐‘‡
3
๐พ1
๐‘๐‘‡๐พ2 2๐‘๐พ2
โ‹ฏ 1.8
Where
๐พ1 = ๐พ 1 + ๐บ + ๐ป + ๐‘„ 1 + ๐บ + ๐ป , ๐พ2 = ๐ฟ[1 + ๐บ + ๐ป + ๐‘„(1 + ๐บ + ๐ป)]
We define the non-empty sets as follows
๐ท๐‘“ = ๐ท โˆ’ ๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
)
๐ท1๐‘“ = ๐ท1 โˆ’ ๐บ๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
)
โ‹ฏ 1.9
and
๐ท2๐‘“ = ๐ท2 โˆ’ ๐ป๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
)
๐ท3๐‘“ = ๐ท3 โˆ’ ๐‘„๐‘€
๐‘‡2
2
(1 +
4๐‘
๐‘‡
)
โ‹ฏ 1.10
Furthermore, we suppose that the greatest Eigen-value ๐œ† ๐‘š๐‘Ž๐‘ฅ of the matrix ฮ› does not exceed unity, i.e.
ฮ› = ๐พ1
๐‘‡
2
+ ๐‘๐พ2(2 + ๐พ1
๐‘‡
2
) < 1 โ‹ฏ 1.11
Lemma 2.1. Let ๐‘“(๐‘ก) be a continuous (piecewise continuous) vector function in the interval 0 โ‰ค ๐‘ก โ‰ค ๐‘‡. Then
(๐‘“ ๐‘  โˆ’
1
๐‘‡
๐‘ก
0
๐‘“(๐‘ )๐‘‘๐‘ )๐‘‘๐‘ 
๐‘‡
0
โ‰ค ๐›ผ ๐‘ก max
๐‘กโˆˆ 0,๐‘‡
๐‘“ ๐‘ก ,
Where ๐›ผ ๐‘ก = 2๐‘ก(1 โˆ’
๐‘ก
๐‘‡
) . (For the proof see [3]) .
Assume that
๐ด๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 = ๐‘ฆ ๐‘š ๐‘ก, ๐‘ฅ0 , ๐ต๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 = ๐‘ง ๐‘š ๐‘ก, ๐‘ฅ0 and
๐‘ค ๐‘š ๐‘ก, ๐‘ฅ0 = ๐‘”(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐ด๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐ต๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 )๐‘‘๐‘  ,
๐‘ก
๐‘กโˆ’๐‘‡
๐‘š = 0,1,2, โ‹ฏ
II. APPROXIMATE SOLUTION
The investigation of a periodic approximate solution of the system (1.1) makes essential use of the
statements and estimates given below.
Theorem 2.1. If the system of integro-differential equations with impulsive action(1.1) satisfy the inequalities
(1.3) to (1.7) and the conditions (1.8), (1.10) has a periodic solution ๐‘ฅ = ๐‘ฅ ๐‘ก, ๐‘ฅ0 , passing through the point
0, ๐‘ฅ0 , ๐‘ฅ0 โˆˆ ๐ท๐‘“ ,
๐ด๐‘ฅ0 โˆˆ ๐ท1๐‘“ and ๐ต๐‘ฅ0 โˆˆ ๐ท2๐‘“ , then the sequence of functions:
๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 = ๐‘ฅ0 + [๐‘“(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0
๐‘ก
0
) โˆ’
โˆ’
1
๐‘‡
๐‘”(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 )
๐‘‡
0
๐‘‘๐‘ ]๐‘‘๐‘  +
+ ๐ผ๐‘–
0<๐‘ก ๐‘–<๐‘ก
(๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 ) โˆ’
โˆ’
๐‘ก
๐‘‡
๐ผ๐‘–(๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 )
๐‘
๐‘–=1
โ‹ฏ 2.1
With
๐‘ฅ0 ๐‘ก, ๐‘ฅ0 = ๐‘ฅ0 , ๐‘š = 0,1,2, โ‹ฏ
Periodic Solutions for Nonlinear Systems of Integro-Differential Equationsโ€ฆ
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is periodic in ๐‘ก of period ๐‘‡, and uniformly convergent as ๐‘š โ†’ โˆž in
๐‘ก, ๐‘ฅ0 โˆˆ ๐‘…1
ร— ๐ท๐‘“ = โˆ’โˆž,โˆž ร— ๐ท๐‘“ โ‹ฏ 2.2
To the vector function ๐‘ฅ0
(๐‘ก, ๐‘ฅ0) defined on the domain (1.2), which is periodic in ๐‘ก of period ๐‘‡ and satisfying
the system of integral equation
๐‘ฅ ๐‘ก, ๐‘ฅ0 = ๐‘ฅ0 + [๐‘“(๐‘ , ๐‘ฅ ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘ , ๐‘ฅ0
๐‘ก
0
) โˆ’
โˆ’
1
๐‘‡
๐‘”(๐‘ , ๐‘ฅ ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘ , ๐‘ฅ0 )
๐‘‡
0
๐‘‘๐‘ ]๐‘‘๐‘  +
+ ๐ผ๐‘–
0<๐‘ก ๐‘–<๐‘ก
(๐‘ฅ ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘ก๐‘–, ๐‘ฅ0 ) โˆ’
โˆ’
๐‘ก
๐‘‡
๐ผ๐‘–(๐‘ฅ ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘ก๐‘–, ๐‘ฅ0 )
๐‘
๐‘–=1
โ‹ฏ 2.3
Which a unique solution of the system (1.1) provided that
๐‘ฅ0
๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ0 โ‰ค
๐‘€๐‘‡
2
(1 +
4๐‘
๐‘‡
) โ‹ฏ 2.4
and
๐‘ฅ0
๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ ๐‘š (๐‘ก, ๐‘ฅ0) โ‰ค ๐œ† ๐‘š
1 โˆ’ ๐œ† โˆ’1
๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
) โ‹ฏ 2.5
for all ๐‘š โ‰ฅ 1, ๐‘ก โˆˆ ๐‘…1
, where the eigen-value ๐œ† of the matrix ฮ” is a positive fraction less than one.
Proof. Consider the sequence of functions ๐‘ฅ1 ๐‘ก, ๐‘ฅ0 , ๐‘ฅ2 ๐‘ก, ๐‘ฅ0 , โ‹ฏ, ๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 , โ‹ฏ,
defined by recurrence relation (2.1). Each of the functions of the sequence is periodic in ๐‘ก of period ๐‘‡.
Now, by Lemma 1.1, we have
๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ0 = ๐‘ฅ0 + [๐‘“(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0
๐‘ก
0
) โˆ’
โˆ’
1
๐‘‡
๐‘”(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 )
๐‘‡
0
๐‘‘๐‘ ]๐‘‘๐‘  +
+ ๐ผ๐‘–
0<๐‘ก ๐‘–<๐‘ก
(๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 ) โˆ’
โˆ’
๐‘ก
๐‘‡
๐ผ๐‘–(๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 )
๐‘
๐‘–=1
โˆ’ ๐‘ฅ0 โ‰ค
โ‰ค (1 โˆ’
๐‘ก
๐‘‡
) ๐‘“(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 )
๐‘ก
0
๐‘‘๐‘  +
+
๐‘ก
๐‘‡
๐‘“(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 ) ๐‘‘๐‘ 
๐‘‡
๐‘ก
+
+ ๐ผ๐‘–
0<๐‘ก ๐‘–<๐‘ก
(๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 ) +
+
๐‘ก
๐‘‡
๐ผ๐‘– ๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 โ‰ค
๐‘
๐‘–=1
โ‰ค ๐›ผ ๐‘ก ๐‘€ + 2๐‘๐‘€
โ‰ค ๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
) โ‹ฏ 2.6
From (1.7) and (2.4), we have
๐ด๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 โˆ’ ๐ด๐‘ฅ0 โ‰ค ๐‘„๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
)
๐ต๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 โˆ’ ๐ต๐‘ฅ0 โ‰ค ๐ป๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
)
โ‹ฏ 2.7
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for all ๐‘ฅ0 โˆˆ ๐ท๐‘“.
Also
๐‘ค ๐‘š ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ค0(๐‘ก, ๐‘ฅ0) = ๐‘” ๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐ด๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐ต๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 ๐‘‘๐‘  โˆ’
๐‘ก
๐‘กโˆ’๐‘‡
โˆ’ ๐‘” ๐‘ , ๐‘ฅ0, ๐ด๐‘ฅ0, ๐ต๐‘ฅ0 ๐‘‘๐‘ 
๐‘ก
๐‘กโˆ’๐‘‡
โ‰ค
โ‰ค ๐พ( ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ฅ0 + ๐ด๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 โˆ’ ๐ด๐‘ฅ0 +
๐‘ก
๐‘กโˆ’๐‘‡
๐ต๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 โˆ’ ๐ต๐‘ฅ0 )๐‘‘๐‘ 
โ‰ค [๐พ(๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
) + ๐บ๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
) + ๐ป๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
))
๐‘ก
๐‘กโˆ’๐‘‡
]๐‘‘๐‘ 
= ๐พ๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
)(1 + ๐บ + ๐ป) โ‹ฏ 2.8
For ๐‘š = 1, in (2.1), we get
๐‘ฅ2 ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ1(๐‘ก, ๐‘ฅ0) โ‰ค (1 โˆ’
๐‘ก
๐‘‡
) ๐พ( ๐‘ฅ1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ฅ0 + ๐‘ฆ1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ฆ0(๐‘ , ๐‘ฅ0)
๐‘ก
0
+ ๐‘ง1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ง0(๐‘ , ๐‘ฅ0) + ๐‘ค1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ค0(๐‘ , ๐‘ฅ0) )๐‘‘๐‘  +
+
๐‘ก
๐‘‡
๐พ( ๐‘ฅ1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ฅ0 + ๐‘ฆ1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ฆ0(๐‘ , ๐‘ฅ0)
๐‘‡
๐‘ก
+
+ ๐‘ง1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ง0(๐‘ , ๐‘ฅ0) + ๐‘ค1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ค0(๐‘ , ๐‘ฅ0) )๐‘‘๐‘  +
+ ๐ฟ
0<๐‘ก ๐‘–<๐‘ก
๐‘ฅ1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ฅ0 + ๐‘ฆ1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ฆ0(๐‘ก๐‘–, ๐‘ฅ0) +
+ ๐‘ง1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ง0(๐‘ก๐‘–, ๐‘ฅ0) + ๐‘ค1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ค0(๐‘ก๐‘–, ๐‘ฅ0) ) +
+
๐‘ก
๐‘‡
๐ฟ
๐‘
๐‘–=1
( ๐‘ฅ1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ฅ0 + ๐‘ฆ1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ฆ0(๐‘ก๐‘–, ๐‘ฅ0) +
+ ๐‘ง1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ง0(๐‘ก๐‘–, ๐‘ฅ0) + ๐‘ค1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ค0(๐‘ก๐‘–, ๐‘ฅ0) ) +
โ‰ค (1 โˆ’
๐‘ก
๐‘‡
) [๐พ(1 + ๐บ + ๐ป + ๐‘„(๐ฟ + ๐บ + ๐ป))
๐‘ก
0
๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
)]๐‘‘๐‘  +
+
๐‘ก
๐‘‡
[๐พ(1 + ๐บ + ๐ป + ๐‘„(๐ฟ + ๐บ + ๐ป))
๐‘‡
๐‘ก
๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
)]๐‘‘๐‘  +
+[๐ฟ(1 + ๐บ + ๐ป + ๐‘„(๐ฟ + ๐บ + ๐ป))]๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
) โ‰ค
โ‰ค ๐›ผ(๐‘ก)[๐พ(1 + ๐บ + ๐ป + ๐‘„(๐ฟ + ๐บ + ๐ป))]๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
) +
+๐ฟ๐‘๐‘€๐‘‡(1 + ๐บ + ๐ป + ๐‘„(๐ฟ + ๐บ + ๐ป))(1 +
4๐‘
๐‘‡
) โ‰ค
โ‰ค ๐‘1 ๐›ผ ๐‘ก + ๐‘€1 = ๐‘1
๐‘‡
2
+ ๐‘€1 โ‹ฏ 2.10
If the following inequality is true
๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ ๐‘šโˆ’1(๐‘ก, ๐‘ฅ0) โ‰ค ๐‘ ๐‘šโˆ’1 ๐›ผ ๐‘ก + ๐‘€ ๐‘šโˆ’1
โ‰ค ๐‘ ๐‘šโˆ’1
๐‘‡
2
+ ๐‘€ ๐‘šโˆ’1 โ‹ฏ 2.11
for all ๐‘š = 1,2, โ‹ฏ .
then, we shall to prove that
๐‘ฅ ๐‘š+1 ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ ๐‘š (๐‘ก, ๐‘ฅ0) โ‰ค ๐พ1(๐‘ ๐‘šโˆ’1
๐‘‡
2
+ ๐‘€ ๐‘šโˆ’1)๐›ผ(๐‘ก) + 2๐‘๐พ2(๐‘ ๐‘šโˆ’1
๐‘‡
2
+ ๐‘€ ๐‘šโˆ’1)
โ‹ฏ 2.12
for all ๐‘š = 0,1,2, โ‹ฏ .
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By mathematical induction, we have
๐‘ฅ ๐‘š+1 ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ ๐‘š (๐‘ก, ๐‘ฅ0) โ‰ค ๐‘ ๐‘š ๐›ผ ๐‘ก + ๐‘€ ๐‘š โ‰ค
๐‘‡
2
๐‘ ๐‘š + ๐‘€ ๐‘š , โ‹ฏ 2.13
Where
๐‘ ๐‘š+1 = ๐พ1
๐‘‡
2
๐‘ ๐‘š + ๐พ1 ๐‘€ ๐‘š ,
๐‘€ ๐‘š+1 = ๐‘๐พ2 ๐‘‡๐‘ ๐‘š + 2๐‘๐พ2 ๐‘€ ๐‘š , ๐‘0 = ๐‘€ , ๐‘€0 = 2๐‘๐‘€ .
โ‹ฏ 2.14
๐‘š = 0,1,2, โ‹ฏ.
It is sufficient to show that all solutions of (2.14) approach zero as ๐‘š โ†’ โˆž , i.e. it is necessary and sufficient that
the eigen values of the matrix ฮ› are assumed to be within a unit circle.
It is well-known that the characteristic equation of the matrix ฮ› is
๐พ1
๐‘‡
2
+ ๐‘๐พ2(2 + ๐พ1
๐‘‡
2
) < 1 โ‹ฏ 2.15
and this ensures that the sequence of functions (2.1) is convergent uniformly on the domain (2.2) as ๐‘š โ†’ โˆž .
Let
lim
๐‘šโ†’โˆž
๐‘ฅ ๐‘š (๐‘ก, ๐‘ฅ0) = ๐‘ฅโˆž ๐‘ก, ๐‘ฅ0 โ‹ฏ 2.13
Since the sequence of functions (2.2) is periodic in ๐‘ก of period ๐‘‡, then the limiting is also periodic in ๐‘ก of period
๐‘‡.
Moreover, B lemma 1.1 and (2.15) and the following inequality
๐‘ฅ ๐‘š+1 ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ ๐‘š (๐‘ก, ๐‘ฅ0) โ‰ค ๐‘ฅ ๐‘š+๐‘–+1 ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ ๐‘š+๐‘–(๐‘ก, ๐‘ฅ0) โ‰ค
๐‘˜โˆ’1
๐‘–=0
โ‰ค ๐œ† ๐‘š+๐‘–
๐‘˜โˆ’1
๐‘–=0
๐‘€
๐‘‡
2
(1 +
4๐‘
๐‘‡
)
the inequalities (2.4) and (2.5) are satisfied for all ๐‘š โ‰ฅ 0 .
Finally, we have to show that ๐‘ฅ(๐‘ก, ๐‘ฅ0) is unique solution of (1.1). on the contrary, we suppose that there is at
least two different solutions ๐‘ฅ(๐‘ก, ๐‘ฅ0) and ๐‘Ÿ(๐‘ก, ๐‘ฅ0) of (1.1).
From (2.3), the following inequality holds:
๐‘ฅ ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘Ÿ ๐‘ก, ๐‘ฅ0 โ‰ค (1 โˆ’
๐‘ก
๐‘‡
) ๐พ1
๐‘ก
0
๐‘ฅ ๐‘ , ๐‘ฅ0 โˆ’ ๐‘Ÿ ๐‘ , ๐‘ฅ0 ๐‘‘๐‘  +
+
๐‘ก
๐‘‡
๐พ1 ๐‘ฅ ๐‘ , ๐‘ฅ0 โˆ’ ๐‘Ÿ ๐‘ , ๐‘ฅ0
๐‘‡
๐‘ก
๐‘‘๐‘  + ๐พ2
0<๐‘ก ๐‘–<๐‘ก
๐‘ฅ ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘Ÿ ๐‘ก๐‘–, ๐‘ฅ0 +
+
๐‘ก
๐‘‡
๐พ2
๐‘
๐‘–=1
๐‘ฅ ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘Ÿ ๐‘ก๐‘–, ๐‘ฅ0 โ‹ฏ 2.16
Setting ๐‘ฅ ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘Ÿ ๐‘ก, ๐‘ฅ0 = ๐‘• ๐‘ก , the inequality (2.16) can be written as:
๐‘•(๐‘ก) โ‰ค (1 โˆ’
๐‘ก
๐‘‡
) ๐พ1
๐‘ก
0
๐‘•(๐‘ )๐‘‘๐‘  +
๐‘ก
๐‘‡
๐พ1 ๐‘•(๐‘ )
๐‘‡
๐‘ก
๐‘‘๐‘  + ๐พ2
0<๐‘ก ๐‘–<๐‘ก
๐‘•(๐‘ก๐‘–) +
๐‘ก
๐‘‡
๐พ2
๐‘
๐‘–=1
๐‘•(๐‘ก๐‘–)
Let max ๐‘กโˆˆ[0,๐‘‡] ๐‘•(๐‘ก) = ๐‘•0 โ‰ฅ 0 . By iteration, we get:
๐‘• ๐‘ก โ‰ค ๐‘ ๐‘š ๐›ผ ๐‘ก + ๐‘€ ๐‘š โ‹ฏ 2.17
From (2.14), we have:
๐‘ ๐‘š+1
๐‘€ ๐‘š+1
= ๐พ1
๐‘‡
2
๐พ1
๐‘๐‘‡๐พ2 2๐‘๐พ2
๐‘ ๐‘š
๐‘€ ๐‘š
โ‹ฏ 2.18
which satisfies the initial conditions ๐‘0 = 0, ๐‘€0 = ๐‘•0 That is
๐‘ ๐‘š
๐‘€ ๐‘š
=
๐พ1
๐‘‡
2
๐พ1
๐‘๐‘‡๐พ2 2๐‘๐พ2
๐‘š
0
๐‘• ๐‘š
โ‹ฏ 2.19
Hence it is clear that if the condition (2.15) is satisfied then ๐‘ ๐‘š โ†’ 0 and ๐‘€ ๐‘š โ†’ 0 as ๐‘š โ†’ โˆž.
From the relation (2.17) we get ๐‘•(๐‘ก) โ‰ก 0 or ๐‘ฅ ๐‘ก, ๐‘ฅ0 = ๐‘Ÿ ๐‘ก, ๐‘ฅ0 , i.e. ๐‘ฅ(๐‘ก, ๐‘ฅ0) is a unique solution of (1.1). โˆŽ
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The problem of the existence of periodic solution of period ๐‘‡ of the system (1.1) is uniquely connected
with the existence of zeros of the function ฮ”(๐‘ฅ0) which has the form
ฮ” ๐‘ฅ0 =
1
๐‘‡
[ ๐‘“(๐‘ก, ๐‘ฅ0
๐‘ก, ๐‘ฅ0 , ๐‘ฆ0
๐‘ก, ๐‘ฅ0 , ๐‘ง0
๐‘ก, ๐‘ฅ0 , ๐‘ค0
(๐‘ก, ๐‘ฅ0))
๐‘‡
0
๐‘‘๐‘ก +
+ ๐ผ๐‘–
๐‘
๐‘–=1
(๐‘ฅ0
๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ0
๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง0
๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค0
(๐‘ก๐‘–, ๐‘ฅ0))], โ‹ฏ 3.1
since this function is approximately determined from the sequence of functions
ฮ”m ๐‘ฅ0 =
1
๐‘‡
[ ๐‘“(๐‘ก, ๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘ค ๐‘š (๐‘ก, ๐‘ฅ0))
๐‘‡
0
๐‘‘๐‘ก +
+ ๐ผ๐‘–
๐‘
๐‘–=1
(๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š (๐‘ก๐‘–, ๐‘ฅ0))] โ‹ฏ 3.2
where ๐‘ฅ0
(๐‘ก, ๐‘ฅ0) is the limiting of the sequence of functions (2.1). Also
๐‘ฆ0
๐‘ก, ๐‘ฅ0 = ๐ด๐‘ฅ0
๐‘ก, ๐‘ฅ0 , ๐‘ง0
๐‘ก, ๐‘ฅ0 = ๐ต๐‘ฅ0
(๐‘ก, ๐‘ฅ0) and
๐‘ค0
๐‘ก, ๐‘ฅ0 = ๐‘”(๐‘ , ๐‘ฅ0
๐‘ , ๐‘ฅ0 , ๐ด๐‘ฅ0
๐‘ , ๐‘ฅ0 , ๐ต๐‘ฅ0
(๐‘ , ๐‘ฅ0))
๐‘ก
๐‘กโˆ’๐‘‡
๐‘‘๐‘  .
Now, we prove the following theorem taking in to ///// that the following inequality will be satisfied for all
๐‘š โ‰ฅ 1.
ฮ” ๐‘ฅ0 โˆ’ ฮ” ๐‘š (๐‘ฅ0) โ‰ค ๐œ† ๐‘š
1 โˆ’ ๐œ† โˆ’1
(๐พ1 +
๐‘
๐‘‡
๐พ2)
๐‘€๐‘‡
2
(1 +
4๐‘
๐‘‡
) โ‹ฏ 3.3
Theorem 3.1. If the system of equations (1.1) satisfies the following conditions:
(๐‘–) the sequence of functions (3.2) has an isolated singular point ๐‘ฅ0 = ๐‘ฅ0
, ฮ” ๐‘š (๐‘ฅ0) โ‰ก 0, for all ๐‘ก โˆˆ ๐‘…1
;
(๐‘–๐‘–) the index of this point is nonzero;
(๐‘–๐‘–๐‘–) there exists a closed convex domain ๐ท4 belonging to the domain ๐ท๐‘“ and possessing a unique singular point
๐‘ฅ0
such that on it is boundary ฮ“ ๐ท4
the following inequality holds
inf
xโˆˆฮ“ ๐ท4
ฮ” ๐‘š (๐‘ฅ0
) โ‰ค ๐œ† ๐‘š
1 โˆ’ ๐œ† โˆ’1
(๐พ1 +
๐‘
๐‘‡
๐พ2)
๐‘€๐‘‡
2
(1 +
4๐‘
๐‘‡
)
for all ๐‘š โ‰ฅ 1. Then the system (1.1) has a periodic solution ๐‘ฅ = ๐‘ฅ(๐‘ก, ๐‘ฅ0) for which ๐‘ฅ 0 โˆˆ ๐ท4.
Proof. By using the inequality (3.3) we can prove the theorem is a similar way to that of theorem 2.1.2 [2].
Remark 3.1. When ๐‘… ๐‘›
= ๐‘…1
, i.e. when ๐‘ฅ0
is a scalar, theorem 3.1 can be proved by the following.
Theorem 3.2. Let the functions ๐‘“(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ฆ, ๐‘ง, ๐‘ค) and ๐ผ๐‘–(๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค) of system (1.1) are defined on the interval
[๐‘Ž, ๐‘] in ๐‘…1
. Then the function (3.2) satisfies the inequalities:
min
๐‘Ž+
๐‘€๐‘‡
2
1+
4๐‘
๐‘‡
โ‰ค๐‘ฅ0โ‰ค๐‘โˆ’
๐‘€๐‘‡
2
1+
4๐‘
๐‘‡
ฮ” ๐‘š ๐‘ฅ0
โ‰ค โˆ’ ๐œ† ๐‘š
1 โˆ’ ๐œ† โˆ’1
(๐พ1 +
๐‘
๐‘‡
๐พ2)
max
๐‘Ž+
๐‘€๐‘‡
2
1+
4๐‘
๐‘‡
โ‰ค๐‘ฅ0โ‰ค๐‘โˆ’
๐‘€๐‘‡
2
1+
4๐‘
๐‘‡
ฮ” ๐‘š ๐‘ฅ0
โ‰ฅ ๐œ† ๐‘š
1 โˆ’ ๐œ† โˆ’1
(๐พ1 +
๐‘
๐‘‡
๐พ2)
โ‹ฏ 3.4
Then (1.1) has a periodic solution in ๐‘ก of period ๐‘‡ for which
๐‘ฅ0
0 โˆˆ [๐‘Ž +
๐‘€๐‘‡
2
(1 +
4๐‘
๐‘‡
), ๐‘ โˆ’
๐‘€๐‘‡
2
(1 +
4๐‘
๐‘‡
)] .
Proof. Let ๐‘ฅ1 and ๐‘ฅ2 be any points of the interval
[๐‘Ž +
๐‘€๐‘‡
2
(1 +
4๐‘
๐‘‡
), ๐‘ โˆ’
๐‘€๐‘‡
2
(1 +
4๐‘
๐‘‡
)] such that
ฮ” ๐‘š ๐‘ฅ1 = min ฮ” ๐‘š ๐‘ฅ0
๐‘Ž+
๐‘€๐‘‡
2
1+
4๐‘
๐‘‡
โ‰ค๐‘ฅ0โ‰ค๐‘โˆ’
๐‘€๐‘‡
2
1+
4๐‘
๐‘‡
,
ฮ” ๐‘š ๐‘ฅ2 = max ฮ” ๐‘š ๐‘ฅ0
๐‘Ž+
๐‘€๐‘‡
2
1+
4๐‘
๐‘‡
โ‰ค๐‘ฅ0โ‰ค๐‘โˆ’
๐‘€๐‘‡
2
1+
4๐‘
๐‘‡
.
โ‹ฏ 3.5
By using the inequalities (3.3) and (3.4) , we have
ฮ” ๐‘š ๐‘ฅ1 = ฮ” ๐‘š ๐‘ฅ1 + ฮ” ๐‘š ๐‘ฅ1 โˆ’ ฮ” ๐‘š ๐‘ฅ1 < 0 ,
ฮ” ๐‘š ๐‘ฅ2 = ฮ” ๐‘š ๐‘ฅ2 + (ฮ” ๐‘š
๐‘ฅ2 โˆ’ ฮ” ๐‘š ๐‘ฅ2 ) > 0 .
3.6
Periodic Solutions for Nonlinear Systems of Integro-Differential Equationsโ€ฆ
www.ijeijournal.com P a g e | 63
The continuity of ฮ”(๐‘ฅ0
) and by using (3.6), there exists a point ๐‘ฅ0
, ๐‘ฅ0
โˆˆ ๐‘ฅ1, ๐‘ฅ2 , such that ฮ”(๐‘ฅ0
) โ‰ก 0,
i.e. ๐‘ฅ = ๐‘ฅ(๐‘ก, ๐‘ฅ0) is a periodic solution in ๐‘ก of period ๐‘‡ for which ๐‘ฅ0
(0) โˆˆ [๐‘Ž +
๐‘€๐‘‡
2
(1 +
4๐‘
๐‘‡
), ๐‘ โˆ’
๐‘€๐‘‡
2
(1 +
4๐‘
๐‘‡
)] . โˆŽ
Similar results can be obtained for other class of integro-differential equations of operators with impulsive
action.
In particular, the system of integro-differential equations which has the form
๐‘‘๐‘ฅ
๐‘‘๐‘ก
= ๐‘“(๐‘ก, ๐‘ฅ, ๐ด๐‘ฅ, ๐ต๐‘ฅ, ๐‘” ๐‘ , ๐‘ฅ ๐‘  , ๐ด๐‘ฅ ๐‘  , ๐ต๐‘ฅ ๐‘  ๐‘‘๐‘ 
๐‘ ๐‘ก
๐‘Ž ๐‘ก
,
, ๐น ๐‘ก, ๐‘ 
๐‘ก
โˆ’โˆž
๐‘” ๐‘ , ๐‘ฅ ๐‘  , ๐ด๐‘ฅ ๐‘  , ๐ต๐‘ฅ ๐‘  ๐‘‘๐‘  , ๐‘ก โ‰  ๐‘ก๐‘–
ฮ”๐‘ฅ = |๐‘ก=๐‘ก ๐‘–
๐ผ๐‘–(๐‘ฅ, ๐ด๐‘ฅ, ๐ต๐‘ฅ, ๐‘” ๐‘ , ๐‘ฅ ๐‘  , ๐ด๐‘ฅ ๐‘  , ๐ต๐‘ฅ ๐‘  ๐‘‘๐‘ ,
๐‘(๐‘ก ๐‘–)
๐‘Ž(๐‘ก ๐‘–)
, ๐น ๐‘ก๐‘–, ๐‘  ๐‘”(๐‘ , ๐‘ฅ ๐‘  , ๐ด๐‘ฅ ๐‘  , ๐ต๐‘ฅ(๐‘ ))๐‘‘๐‘ 
๐‘ก ๐‘–
โˆ’โˆž
)
โ‹ฏ 3.7
In this system (3.7), let the vector functions ๐‘“ ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค , ๐‘”(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง) and scalar functions ๐‘Ž ๐‘ก , ๐‘(๐‘ก)
are periodic in ๐‘ก of period ๐‘‡, defined and continuous on the domain.
๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘• โˆˆ ๐‘…1
ร— ๐บ ร— ๐บ1 ร— ๐บ2 ร— ๐บ3 ร— ๐บ4 =
= โˆ’โˆž, โˆž ร— ๐บ ร— ๐บ1 ร— ๐บ2 ร— ๐บ3 ร— ๐บ4 โ‹ฏ 3.8
Let ๐ผ๐‘– ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘• be a continuous vector function which are defined on the domain (3.8). A matrix ๐น ๐‘ก, ๐‘  is
defined and continuous in ๐‘…1
ร— ๐‘…1
and satisfies the condition ๐น ๐‘ก + ๐‘‡, ๐‘  + ๐‘‡ = ๐น ๐‘ก, ๐‘  which ๐น ๐‘ก, ๐‘  โ‰ค
๐›ฟ ๐‘’โˆ’๐›พ ๐‘กโˆ’๐‘ 
,
0 โ‰ค ๐‘  โ‰ค t โ‰ค T , where ๐›ฟ, ๐›พ are a positive constants. Suppose that the functions ๐‘“(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘•) and
๐‘” ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง , ๐ผ๐‘– ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘• are satisfying the following inequalities:
๐‘“(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘•) โ‰ค ๐‘€ , ๐‘”(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง) โ‰ค ๐‘ , โ‹ฏ 3.9
๐‘“ ๐‘ก, ๐‘ฅ1, ๐‘ฆ1, ๐‘ง1, ๐‘ค1, ๐‘•1 โˆ’ ๐‘“ ๐‘ก, ๐‘ฅ2, ๐‘ฆ2, ๐‘ง2, ๐‘ค2, ๐‘•2 โ‰ค ๐พโˆ—
( ๐‘ฅ1 โˆ’ ๐‘ฅ2 + ๐‘ฆ1 โˆ’ ๐‘ฆ2 +
+ ๐‘ง1 โˆ’ ๐‘ง2 + ๐‘ค1 โˆ’ ๐‘ค2 + ๐‘•1 โˆ’ ๐‘•2 );
๐‘” ๐‘ก, ๐‘ฅ1, ๐‘ฆ1, ๐‘ง1 โˆ’ ๐‘” ๐‘ก, ๐‘ฅ2, ๐‘ฆ2, ๐‘ง2 โ‰ค ๐‘„โˆ—
๐‘ฅ1 โˆ’ ๐‘ฅ2 + ๐‘ฆ1 โˆ’ ๐‘ฆ2 + ๐‘ง1 โˆ’ ๐‘ง2 ;
โ‹ฏ 3.10
๐ผ๐‘– ๐‘ฅ1, ๐‘ฆ1, ๐‘ง1, ๐‘ค1, ๐‘•1 โˆ’ ๐ผ๐‘– ๐‘ฅ2, ๐‘ฆ2, ๐‘ง2, ๐‘ค2, ๐‘•2 โ‰ค ๐ฟโˆ—
( ๐‘ฅ1 โˆ’ ๐‘ฅ2 + ๐‘ฆ1 โˆ’ ๐‘ฆ2 +
+ ๐‘ง1 โˆ’ ๐‘ง2 + ๐‘ค1 โˆ’ ๐‘ค2 + ๐‘•1 โˆ’ ๐‘•2 );
โ‹ฏ 3.11
and
๐ด๐‘ฅ1 ๐‘ก โˆ’ ๐ด๐‘ฅ2 ๐‘ก โ‰ค ๐บโˆ—
๐‘ฅ1 ๐‘ก โˆ’ ๐‘ฅ2 ๐‘ก ,
๐ต๐‘ฅ1 ๐‘ก โˆ’ ๐ต๐‘ฅ2 ๐‘ก โ‰ค ๐ปโˆ—
๐‘ฅ1 ๐‘ก โˆ’ ๐‘ฅ2 ๐‘ก .
โ‹ฏ 3.12
for all ๐‘ก โˆˆ ๐‘…1
, ๐‘ฅ, ๐‘ฅ1, ๐‘ฅ2 โˆˆ ๐บ, ๐‘ฆ, ๐‘ฆ1, ๐‘ฆ2 โˆˆ ๐บ1, ๐‘ง, ๐‘ง1, ๐‘ง2 โˆˆ ๐บ2, ๐‘ค, ๐‘ค1, ๐‘ค2 โˆˆ ๐บ3,
๐‘•, ๐‘•1, ๐‘•2 โˆˆ ๐บ4 , Provided that
๐ด๐‘ฅ ๐‘ก + ๐‘‡ = ๐ด๐‘ฅ ๐‘ก , ๐ต๐‘ฅ ๐‘ก + ๐‘‡ = ๐ต๐‘ฅ ๐‘ก , ๐ผ๐‘–+๐‘ ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘• = ๐ผ๐‘–(๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘•) and ๐‘ก๐‘–+๐‘ = ๐‘ก๐‘– + ๐‘‡.
Define a non-empty sets as follows:
๐บ๐‘“ = ๐บ โˆ’
๐‘€โˆ—
๐‘‡
2
(1 +
4๐‘
๐‘‡
) , ๐บ1๐‘“ = ๐บ1 โˆ’ ๐บโˆ—
๐‘€โˆ—
๐‘‡
2
(1 +
4๐‘
๐‘‡
),
๐บ2๐‘“ = ๐บ3 โˆ’ ๐ปโˆ—
๐‘€โˆ—
๐‘‡
2
(1 +
4๐‘
๐‘‡
) , ๐บ4๐‘“ = ๐บ4 โˆ’ ๐›ฝ๐‘„โˆ—
๐‘€โˆ—
๐‘‡
2
(1 +
4๐‘
๐‘‡
) ,
๐บ5๐‘“ = ๐บ5 โˆ’
๐›ฟ
๐›พ
๐‘„โˆ—
๐‘€โˆ—
๐‘‡
2
(1 +
4๐‘
๐‘‡
) .
โ‹ฏ 3.13
Furthermore, the largest Eigen-value of ๐›พ ๐‘š๐‘Ž๐‘ฅ of the matrix
ฮ“ =
๐พ1
๐‘‡
2
๐พ1
๐‘๐พ2 ๐‘‡ 2๐‘๐พ2
is less than unity, i.e.
Periodic Solutions for Nonlinear Systems of Integro-Differential Equationsโ€ฆ
www.ijeijournal.com P a g e | 64
1
2
[๐พ1
๐‘‡
3
+ 2๐‘๐พ2 + (
๐พ1 ๐‘‡
3
+ 2๐‘๐พ2)2 +
4๐‘๐พ1 ๐พ2 ๐‘‡
3
] < 1 , โ‹ฏ 3.14
where ๐พ1 = ๐พโˆ—
[1 + ๐บโˆ—
+ ๐ปโˆ—
+
๐›ฟ
๐›พ
๐‘„โˆ—
+ ๐‘„โˆ—
(1 + ๐บโˆ—
+ ๐›ฝ)],
๐พ2 = ๐ฟโˆ—
[1 + ๐บโˆ—
+ ๐ปโˆ—
+
๐›ฟ
๐›พ
๐‘„โˆ—
+ ๐‘„โˆ—
(1 + ๐บโˆ—
+ ๐›ฝ)] and ๐›ฝ = max0โ‰ค๐‘กโ‰ค๐‘‡ ๐‘ ๐‘ก โˆ’ ๐‘Ž(๐‘ก) .
Theorem 3.2. If the system of integro-differential equations with impulsive action (3.7) satisfying the above
assumptions and conditions has a periodic solution ๐‘ฅ = ๐œ“ ๐‘ก, ๐‘ฅ0 , then there exists a unique solution which is the
limit function of a uniformly convergent sequence which has the form
๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 = ๐‘ฅ0 + [๐‘“(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘• ๐‘š (๐‘ , ๐‘ฅ0)
๐‘ก
0
) โˆ’
โˆ’
1
๐‘‡
๐‘“(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘• ๐‘š (๐‘ , ๐‘ฅ0))
๐‘‡
0
๐‘‘๐‘ ]๐‘‘๐‘  +
+ ๐ผ๐‘–
0<๐‘ก ๐‘–<๐‘ก
(๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘• ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 ) โˆ’
โˆ’
๐‘ก
๐‘‡
๐ผ๐‘–(๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘• ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 )
๐‘
๐‘–=1
โ‹ฏ 3.15
with
๐‘ฅ0 ๐‘ก, ๐‘ฅ0 = ๐‘ฅ0 , ๐‘š = 0,1,2, โ‹ฏ.
The proof is a similar to that of theorem 1.1.
If we consider the following mapping
ฮ”m ๐‘ฅ0 =
1
๐‘‡
[ ๐‘“(๐‘ก, ๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘• ๐‘š (๐‘ก, ๐‘ฅ0))
๐‘‡
0
๐‘‘๐‘ก +
+ ๐ผ๐‘–
๐‘
๐‘–=1 (๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘• ๐‘š (๐‘ก๐‘–, ๐‘ฅ0))].
โ‹ฏ 3.16
Then we can state a theorem similar to theorem 2.2, provided that ๐›พ ๐‘š๐‘Ž๐‘ฅ =
1
2
[๐พ1
๐‘‡
3
+ 2๐‘๐พ2 +
(
๐พ1 ๐‘‡
3
+ 2๐‘๐พ2)2 +
4๐‘๐พ1 ๐พ2 ๐‘‡
3
] < 1 ,
Remark 3.2. It is clear that when we put ๐ผ๐‘– โ‰ก 0, we get a periodic solution for the systems (1.1) and (3.7)
without introducing impulsive action.
REFERENCES
1) Butris, R. N. , Existence of a periodic solutions for nonlinear systems of differential equations of
operators with impulsive action, Iraq,Mosul Univ J. Ed. and Sci., Vol.(15),(1994).
2) [2] Butris,R.N.and Saied El.M.On periodic solutions for certain systems of integro-differen tial
equations Iraq ,Mosul Univ., J.of Educ_and Sci., vol 31, (1998)
3) [3] Korol, I. I. , On periodic solutions of one class of systems of differential
4) equations, Ukrainian, Mathematical J. Vol.57, No. 4, (2005).
5) [4] Perestyuk ,N.A.On periodic solutions of some of differential equations. In asymptotic and
qualitative method in the theory of nonlinear oscillations. Ukrainian Academy of sciences, Kiev (1971)
6) [5] Samoilenko, A. M. and Perestyuk, N. A. , Differential equations with impulsive
7) action, Ukrainian, Kiev, (1987).
8) [6] Samoilenko, A. M. and Ronto, N. I. , Numerical-analytic methods of
9) investigating periodic solutions, Ukrainian, Kiev, (1976).
10) [7] Tian yu. and Dehong Ji. , Weigao Ge. Existence and non existence results of
11) impulsive first-order problem with integral boundary condition, J. Nonlinear
12) analysis, Vol. 71, (2009).
13) [8] Voskresenskii E.V., periodic solutions of nonlinear system sand the averaging method, translated
form differential equations . State Univ .,vol 28. No 4.(1992).

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Periodic Solutions for Nonlinear Systems of Integro-Differential Equations of Operators with Impulsive Action

  • 1. International Journal of Engineering Inventions e-ISSN: 2278-7461, p-ISSN: 2319-6491 Volume 2, Issue 2 (January 2013) PP: 57-64 www.ijeijournal.com P a g e | 57 Periodic Solutions for Nonlinear Systems of Integro- Differential Equations of Operators with Impulsive Action Dr. Raad N. Butris Assistant Prof. Department of Mathematics Faculty of Science University of Zakho Iraq-Duhok-Kurdistan Region Abstract:- In this paper we investigate the existence and approximation of the construction of periodic solutions for nonlinear systems of integro-differential equation of operators with impulsive action, by using the numerical-analytic method for periodic solutions which is given by Samoilenko. This investigation leads us to the improving and extending to the above method and expands the results gained by Butris. Keyword and Phrases:- Numerical-analytic methods existence of periodic solutions, nonlinear integro- differential equations, subjected to impulsive action of operators. I. INTRODUCTION They are many subjects in mechanics, physics, biology, and other subjects in science and engineering requires the investigation of periodic solution of integro-differential equations with impulsive action of various types and their systems in particular, they are many works devoted to problems of the existence of periodic solutions of integro-differential equations with impulsive action . samoilenko[5,6] assumed a numerical analytic method to study to periodic solution for ordinary differential equation and this method include uniformly sequences of periodic functionsโ€™ as Intel studies [2,3,4,7,8]. The present work continues the investigations in this direction. These investigations lead us to the improving and extending the above method and expand the results gained by Butris [1]. ๐‘‘๐‘ฅ ๐‘‘๐‘ก = ๐‘“(๐‘ก, ๐‘ฅ, ๐ด๐‘ฅ, ๐ต๐‘ฅ, ๐‘”(๐‘ก, ๐‘ฅ ๐‘  , ๐ด๐‘ฅ ๐‘  , ๐ต๐‘ฅ(๐‘ ))๐‘‘๐‘  ๐‘ก ๐‘กโˆ’๐‘‡ ), ๐‘ก โ‰  ๐‘ก๐‘– ฮ”๐‘ฅ ๐‘ก=๐‘ก ๐‘– = ๐ผ๐‘–(๐‘ฅ, ๐ด๐‘ฅ, ๐ต๐‘ฅ, ๐‘” ๐‘ , ๐‘ฅ ๐‘  , ๐ด๐‘ฅ ๐‘  , ๐ต๐‘ฅ ๐‘  ๐‘‘๐‘  ๐‘ก ๐‘กโˆ’๐‘‡ ) โ‹ฏ(1.1) Where ๐‘ฅ โˆˆ ๐ท โŠ‚ ๐‘… ๐‘› , ๐ท is closed bounded domain. The vector functions ๐‘“(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค) and ๐‘”(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง) are defined on the domain ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค โˆˆ ๐‘…1 ร— ๐ท ร— ๐ท1 ร— ๐ท2 ร— ๐ท3 = โˆ’โˆž,โˆž ร— ๐ท ร— ๐ท1 ร— ๐ท2 ร— ๐ท3 โ‹ฏ 1.2 Which are piecewise continuous functions in ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค and periodic in ๐‘ก of period ๐‘‡, where ๐ท1, ๐ท2 and ๐ท3 are bounded domain subset of Euclidean spaces ๐‘… ๐‘š . Let ๐ผ๐‘– ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค be continuous vector functions, defined on the domain (1.2) and ๐ผ๐‘–+๐‘ ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค = ๐ผ๐‘– ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค , ๐‘ก๐‘–+๐‘ = ๐‘ก๐‘– + ๐‘‡ โ‹ฏ 1.3 For all ๐‘– โˆˆ ๐‘ง+ , ๐‘ฅ โˆˆ ๐ท, ๐‘ฆ โˆˆ ๐ท1, ๐‘ง โˆˆ ๐ท2, ๐‘ค โˆˆ ๐ท3 and for some number ๐‘ . Let the operators A and B transform any piecewise continuous functions from the domain ๐ท to the piecewise contiuous function in the domain ๐ท1 and ๐ท2 respectively. Moreover ๐ด๐‘ฅ ๐‘ก + ๐‘‡ = ๐ด๐‘ฅ(๐‘ก) and ๐ต๐‘ฅ ๐‘ก + ๐‘‡ = ๐ต๐‘ฅ ๐‘ก . Suppose that ๐‘“ ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค , ๐‘” ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง , ๐ผ๐‘–(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค) and the operators A, B satisfy the following inequalities: ๐‘“ ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค โ‰ค ๐‘€, ๐ผ๐‘–(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค) โ‰ค ๐‘, โ‹ฏ 1.4 ๐‘“ ๐‘ก, ๐‘ฅ1, ๐‘ฆ1, ๐‘ง1, ๐‘ค1 โˆ’ ๐‘“ ๐‘ก, ๐‘ฅ2, ๐‘ฆ2, ๐‘ง2, ๐‘ค2 โ‰ค ๐พ( ๐‘ฅ1 โˆ’ ๐‘ฅ2 + ๐‘ฆ1 โˆ’ ๐‘ฆ2 + ๐‘ง1 โˆ’ ๐‘ง2 + ๐‘ค1 โˆ’ ๐‘ค2 ) ๐‘” ๐‘ก, ๐‘ฅ1, ๐‘ฆ1, ๐‘ง1 โˆ’ ๐‘” ๐‘ก, ๐‘ฅ2, ๐‘ฆ2, ๐‘ง2 โ‰ค ๐‘„( ๐‘ฅ1 โˆ’ ๐‘ฅ2 + ๐‘ฆ1 โˆ’ ๐‘ฆ2 + ๐‘ง1 โˆ’ ๐‘ง2 ) โ‹ฏ 1.5 And ๐ผ๐‘– ๐‘ก, ๐‘ฅ1, ๐‘ฆ1, ๐‘ง1, ๐‘ค1 โˆ’ ๐ผ๐‘– ๐‘ก, ๐‘ฅ2, ๐‘ฆ2, ๐‘ง2, ๐‘ค2 โ‰ค ๐ฟ( ๐‘ฅ1 โˆ’ ๐‘ฅ2 + ๐‘ฆ1 โˆ’ ๐‘ฆ2 + ๐‘ง1 โˆ’ ๐‘ง2 + ๐‘ค1 โˆ’ ๐‘ค2 ) โ‹ฏ 1.6
  • 2. Periodic Solutions for Nonlinear Systems of Integro-Differential Equationsโ€ฆ www.ijeijournal.com P a g e | 58 ๐ด๐‘ฅ1 ๐‘ก โˆ’ ๐ด๐‘ฅ2 ๐‘ก โ‰ค ๐บ ๐‘ฅ1 ๐‘ก โˆ’ ๐‘ฅ2 ๐‘ก ๐ต๐‘ฅ1 ๐‘ก โˆ’ ๐ต๐‘ฅ2 ๐‘ก โ‰ค ๐ป ๐‘ฅ1 ๐‘ก โˆ’ ๐‘ฅ2 ๐‘ก โ‹ฏ 1.7 For all ๐‘ก โˆˆ ๐‘…1 , ๐‘ฅ, ๐‘ฅ1, ๐‘ฅ2 โˆˆ ๐ท, ๐‘ฆ, ๐‘ฆ1, ๐‘ฆ2 โˆˆ ๐ท1, ๐‘ง, ๐‘ง1, ๐‘ง2 โˆˆ ๐ท2 and ๐‘ค, ๐‘ค1, ๐‘ค2 โˆˆ ๐ท3 where ๐‘€, ๐‘, ๐พ, ๐‘„, ๐ฟ and ๐บ, ๐ป are a positive constants. Consider the matrix ฮ› = ๐พ1 ๐‘‡ 3 ๐พ1 ๐‘๐‘‡๐พ2 2๐‘๐พ2 โ‹ฏ 1.8 Where ๐พ1 = ๐พ 1 + ๐บ + ๐ป + ๐‘„ 1 + ๐บ + ๐ป , ๐พ2 = ๐ฟ[1 + ๐บ + ๐ป + ๐‘„(1 + ๐บ + ๐ป)] We define the non-empty sets as follows ๐ท๐‘“ = ๐ท โˆ’ ๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) ๐ท1๐‘“ = ๐ท1 โˆ’ ๐บ๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) โ‹ฏ 1.9 and ๐ท2๐‘“ = ๐ท2 โˆ’ ๐ป๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) ๐ท3๐‘“ = ๐ท3 โˆ’ ๐‘„๐‘€ ๐‘‡2 2 (1 + 4๐‘ ๐‘‡ ) โ‹ฏ 1.10 Furthermore, we suppose that the greatest Eigen-value ๐œ† ๐‘š๐‘Ž๐‘ฅ of the matrix ฮ› does not exceed unity, i.e. ฮ› = ๐พ1 ๐‘‡ 2 + ๐‘๐พ2(2 + ๐พ1 ๐‘‡ 2 ) < 1 โ‹ฏ 1.11 Lemma 2.1. Let ๐‘“(๐‘ก) be a continuous (piecewise continuous) vector function in the interval 0 โ‰ค ๐‘ก โ‰ค ๐‘‡. Then (๐‘“ ๐‘  โˆ’ 1 ๐‘‡ ๐‘ก 0 ๐‘“(๐‘ )๐‘‘๐‘ )๐‘‘๐‘  ๐‘‡ 0 โ‰ค ๐›ผ ๐‘ก max ๐‘กโˆˆ 0,๐‘‡ ๐‘“ ๐‘ก , Where ๐›ผ ๐‘ก = 2๐‘ก(1 โˆ’ ๐‘ก ๐‘‡ ) . (For the proof see [3]) . Assume that ๐ด๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 = ๐‘ฆ ๐‘š ๐‘ก, ๐‘ฅ0 , ๐ต๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 = ๐‘ง ๐‘š ๐‘ก, ๐‘ฅ0 and ๐‘ค ๐‘š ๐‘ก, ๐‘ฅ0 = ๐‘”(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐ด๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐ต๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 )๐‘‘๐‘  , ๐‘ก ๐‘กโˆ’๐‘‡ ๐‘š = 0,1,2, โ‹ฏ II. APPROXIMATE SOLUTION The investigation of a periodic approximate solution of the system (1.1) makes essential use of the statements and estimates given below. Theorem 2.1. If the system of integro-differential equations with impulsive action(1.1) satisfy the inequalities (1.3) to (1.7) and the conditions (1.8), (1.10) has a periodic solution ๐‘ฅ = ๐‘ฅ ๐‘ก, ๐‘ฅ0 , passing through the point 0, ๐‘ฅ0 , ๐‘ฅ0 โˆˆ ๐ท๐‘“ , ๐ด๐‘ฅ0 โˆˆ ๐ท1๐‘“ and ๐ต๐‘ฅ0 โˆˆ ๐ท2๐‘“ , then the sequence of functions: ๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 = ๐‘ฅ0 + [๐‘“(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 ๐‘ก 0 ) โˆ’ โˆ’ 1 ๐‘‡ ๐‘”(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 ) ๐‘‡ 0 ๐‘‘๐‘ ]๐‘‘๐‘  + + ๐ผ๐‘– 0<๐‘ก ๐‘–<๐‘ก (๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 ) โˆ’ โˆ’ ๐‘ก ๐‘‡ ๐ผ๐‘–(๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 ) ๐‘ ๐‘–=1 โ‹ฏ 2.1 With ๐‘ฅ0 ๐‘ก, ๐‘ฅ0 = ๐‘ฅ0 , ๐‘š = 0,1,2, โ‹ฏ
  • 3. Periodic Solutions for Nonlinear Systems of Integro-Differential Equationsโ€ฆ www.ijeijournal.com P a g e | 59 is periodic in ๐‘ก of period ๐‘‡, and uniformly convergent as ๐‘š โ†’ โˆž in ๐‘ก, ๐‘ฅ0 โˆˆ ๐‘…1 ร— ๐ท๐‘“ = โˆ’โˆž,โˆž ร— ๐ท๐‘“ โ‹ฏ 2.2 To the vector function ๐‘ฅ0 (๐‘ก, ๐‘ฅ0) defined on the domain (1.2), which is periodic in ๐‘ก of period ๐‘‡ and satisfying the system of integral equation ๐‘ฅ ๐‘ก, ๐‘ฅ0 = ๐‘ฅ0 + [๐‘“(๐‘ , ๐‘ฅ ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘ , ๐‘ฅ0 ๐‘ก 0 ) โˆ’ โˆ’ 1 ๐‘‡ ๐‘”(๐‘ , ๐‘ฅ ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘ , ๐‘ฅ0 ) ๐‘‡ 0 ๐‘‘๐‘ ]๐‘‘๐‘  + + ๐ผ๐‘– 0<๐‘ก ๐‘–<๐‘ก (๐‘ฅ ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘ก๐‘–, ๐‘ฅ0 ) โˆ’ โˆ’ ๐‘ก ๐‘‡ ๐ผ๐‘–(๐‘ฅ ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘ก๐‘–, ๐‘ฅ0 ) ๐‘ ๐‘–=1 โ‹ฏ 2.3 Which a unique solution of the system (1.1) provided that ๐‘ฅ0 ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ0 โ‰ค ๐‘€๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) โ‹ฏ 2.4 and ๐‘ฅ0 ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ ๐‘š (๐‘ก, ๐‘ฅ0) โ‰ค ๐œ† ๐‘š 1 โˆ’ ๐œ† โˆ’1 ๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) โ‹ฏ 2.5 for all ๐‘š โ‰ฅ 1, ๐‘ก โˆˆ ๐‘…1 , where the eigen-value ๐œ† of the matrix ฮ” is a positive fraction less than one. Proof. Consider the sequence of functions ๐‘ฅ1 ๐‘ก, ๐‘ฅ0 , ๐‘ฅ2 ๐‘ก, ๐‘ฅ0 , โ‹ฏ, ๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 , โ‹ฏ, defined by recurrence relation (2.1). Each of the functions of the sequence is periodic in ๐‘ก of period ๐‘‡. Now, by Lemma 1.1, we have ๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ0 = ๐‘ฅ0 + [๐‘“(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 ๐‘ก 0 ) โˆ’ โˆ’ 1 ๐‘‡ ๐‘”(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 ) ๐‘‡ 0 ๐‘‘๐‘ ]๐‘‘๐‘  + + ๐ผ๐‘– 0<๐‘ก ๐‘–<๐‘ก (๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 ) โˆ’ โˆ’ ๐‘ก ๐‘‡ ๐ผ๐‘–(๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 ) ๐‘ ๐‘–=1 โˆ’ ๐‘ฅ0 โ‰ค โ‰ค (1 โˆ’ ๐‘ก ๐‘‡ ) ๐‘“(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 ) ๐‘ก 0 ๐‘‘๐‘  + + ๐‘ก ๐‘‡ ๐‘“(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 ) ๐‘‘๐‘  ๐‘‡ ๐‘ก + + ๐ผ๐‘– 0<๐‘ก ๐‘–<๐‘ก (๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 ) + + ๐‘ก ๐‘‡ ๐ผ๐‘– ๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 โ‰ค ๐‘ ๐‘–=1 โ‰ค ๐›ผ ๐‘ก ๐‘€ + 2๐‘๐‘€ โ‰ค ๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) โ‹ฏ 2.6 From (1.7) and (2.4), we have ๐ด๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 โˆ’ ๐ด๐‘ฅ0 โ‰ค ๐‘„๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) ๐ต๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 โˆ’ ๐ต๐‘ฅ0 โ‰ค ๐ป๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) โ‹ฏ 2.7
  • 4. Periodic Solutions for Nonlinear Systems of Integro-Differential Equationsโ€ฆ www.ijeijournal.com P a g e | 60 for all ๐‘ฅ0 โˆˆ ๐ท๐‘“. Also ๐‘ค ๐‘š ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ค0(๐‘ก, ๐‘ฅ0) = ๐‘” ๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐ด๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐ต๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 ๐‘‘๐‘  โˆ’ ๐‘ก ๐‘กโˆ’๐‘‡ โˆ’ ๐‘” ๐‘ , ๐‘ฅ0, ๐ด๐‘ฅ0, ๐ต๐‘ฅ0 ๐‘‘๐‘  ๐‘ก ๐‘กโˆ’๐‘‡ โ‰ค โ‰ค ๐พ( ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ฅ0 + ๐ด๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 โˆ’ ๐ด๐‘ฅ0 + ๐‘ก ๐‘กโˆ’๐‘‡ ๐ต๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 โˆ’ ๐ต๐‘ฅ0 )๐‘‘๐‘  โ‰ค [๐พ(๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) + ๐บ๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) + ๐ป๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ )) ๐‘ก ๐‘กโˆ’๐‘‡ ]๐‘‘๐‘  = ๐พ๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ )(1 + ๐บ + ๐ป) โ‹ฏ 2.8 For ๐‘š = 1, in (2.1), we get ๐‘ฅ2 ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ1(๐‘ก, ๐‘ฅ0) โ‰ค (1 โˆ’ ๐‘ก ๐‘‡ ) ๐พ( ๐‘ฅ1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ฅ0 + ๐‘ฆ1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ฆ0(๐‘ , ๐‘ฅ0) ๐‘ก 0 + ๐‘ง1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ง0(๐‘ , ๐‘ฅ0) + ๐‘ค1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ค0(๐‘ , ๐‘ฅ0) )๐‘‘๐‘  + + ๐‘ก ๐‘‡ ๐พ( ๐‘ฅ1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ฅ0 + ๐‘ฆ1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ฆ0(๐‘ , ๐‘ฅ0) ๐‘‡ ๐‘ก + + ๐‘ง1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ง0(๐‘ , ๐‘ฅ0) + ๐‘ค1 ๐‘ , ๐‘ฅ0 โˆ’ ๐‘ค0(๐‘ , ๐‘ฅ0) )๐‘‘๐‘  + + ๐ฟ 0<๐‘ก ๐‘–<๐‘ก ๐‘ฅ1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ฅ0 + ๐‘ฆ1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ฆ0(๐‘ก๐‘–, ๐‘ฅ0) + + ๐‘ง1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ง0(๐‘ก๐‘–, ๐‘ฅ0) + ๐‘ค1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ค0(๐‘ก๐‘–, ๐‘ฅ0) ) + + ๐‘ก ๐‘‡ ๐ฟ ๐‘ ๐‘–=1 ( ๐‘ฅ1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ฅ0 + ๐‘ฆ1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ฆ0(๐‘ก๐‘–, ๐‘ฅ0) + + ๐‘ง1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ง0(๐‘ก๐‘–, ๐‘ฅ0) + ๐‘ค1 ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘ค0(๐‘ก๐‘–, ๐‘ฅ0) ) + โ‰ค (1 โˆ’ ๐‘ก ๐‘‡ ) [๐พ(1 + ๐บ + ๐ป + ๐‘„(๐ฟ + ๐บ + ๐ป)) ๐‘ก 0 ๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ )]๐‘‘๐‘  + + ๐‘ก ๐‘‡ [๐พ(1 + ๐บ + ๐ป + ๐‘„(๐ฟ + ๐บ + ๐ป)) ๐‘‡ ๐‘ก ๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ )]๐‘‘๐‘  + +[๐ฟ(1 + ๐บ + ๐ป + ๐‘„(๐ฟ + ๐บ + ๐ป))]๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) โ‰ค โ‰ค ๐›ผ(๐‘ก)[๐พ(1 + ๐บ + ๐ป + ๐‘„(๐ฟ + ๐บ + ๐ป))]๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) + +๐ฟ๐‘๐‘€๐‘‡(1 + ๐บ + ๐ป + ๐‘„(๐ฟ + ๐บ + ๐ป))(1 + 4๐‘ ๐‘‡ ) โ‰ค โ‰ค ๐‘1 ๐›ผ ๐‘ก + ๐‘€1 = ๐‘1 ๐‘‡ 2 + ๐‘€1 โ‹ฏ 2.10 If the following inequality is true ๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ ๐‘šโˆ’1(๐‘ก, ๐‘ฅ0) โ‰ค ๐‘ ๐‘šโˆ’1 ๐›ผ ๐‘ก + ๐‘€ ๐‘šโˆ’1 โ‰ค ๐‘ ๐‘šโˆ’1 ๐‘‡ 2 + ๐‘€ ๐‘šโˆ’1 โ‹ฏ 2.11 for all ๐‘š = 1,2, โ‹ฏ . then, we shall to prove that ๐‘ฅ ๐‘š+1 ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ ๐‘š (๐‘ก, ๐‘ฅ0) โ‰ค ๐พ1(๐‘ ๐‘šโˆ’1 ๐‘‡ 2 + ๐‘€ ๐‘šโˆ’1)๐›ผ(๐‘ก) + 2๐‘๐พ2(๐‘ ๐‘šโˆ’1 ๐‘‡ 2 + ๐‘€ ๐‘šโˆ’1) โ‹ฏ 2.12 for all ๐‘š = 0,1,2, โ‹ฏ .
  • 5. Periodic Solutions for Nonlinear Systems of Integro-Differential Equationsโ€ฆ www.ijeijournal.com P a g e | 61 By mathematical induction, we have ๐‘ฅ ๐‘š+1 ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ ๐‘š (๐‘ก, ๐‘ฅ0) โ‰ค ๐‘ ๐‘š ๐›ผ ๐‘ก + ๐‘€ ๐‘š โ‰ค ๐‘‡ 2 ๐‘ ๐‘š + ๐‘€ ๐‘š , โ‹ฏ 2.13 Where ๐‘ ๐‘š+1 = ๐พ1 ๐‘‡ 2 ๐‘ ๐‘š + ๐พ1 ๐‘€ ๐‘š , ๐‘€ ๐‘š+1 = ๐‘๐พ2 ๐‘‡๐‘ ๐‘š + 2๐‘๐พ2 ๐‘€ ๐‘š , ๐‘0 = ๐‘€ , ๐‘€0 = 2๐‘๐‘€ . โ‹ฏ 2.14 ๐‘š = 0,1,2, โ‹ฏ. It is sufficient to show that all solutions of (2.14) approach zero as ๐‘š โ†’ โˆž , i.e. it is necessary and sufficient that the eigen values of the matrix ฮ› are assumed to be within a unit circle. It is well-known that the characteristic equation of the matrix ฮ› is ๐พ1 ๐‘‡ 2 + ๐‘๐พ2(2 + ๐พ1 ๐‘‡ 2 ) < 1 โ‹ฏ 2.15 and this ensures that the sequence of functions (2.1) is convergent uniformly on the domain (2.2) as ๐‘š โ†’ โˆž . Let lim ๐‘šโ†’โˆž ๐‘ฅ ๐‘š (๐‘ก, ๐‘ฅ0) = ๐‘ฅโˆž ๐‘ก, ๐‘ฅ0 โ‹ฏ 2.13 Since the sequence of functions (2.2) is periodic in ๐‘ก of period ๐‘‡, then the limiting is also periodic in ๐‘ก of period ๐‘‡. Moreover, B lemma 1.1 and (2.15) and the following inequality ๐‘ฅ ๐‘š+1 ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ ๐‘š (๐‘ก, ๐‘ฅ0) โ‰ค ๐‘ฅ ๐‘š+๐‘–+1 ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘ฅ ๐‘š+๐‘–(๐‘ก, ๐‘ฅ0) โ‰ค ๐‘˜โˆ’1 ๐‘–=0 โ‰ค ๐œ† ๐‘š+๐‘– ๐‘˜โˆ’1 ๐‘–=0 ๐‘€ ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) the inequalities (2.4) and (2.5) are satisfied for all ๐‘š โ‰ฅ 0 . Finally, we have to show that ๐‘ฅ(๐‘ก, ๐‘ฅ0) is unique solution of (1.1). on the contrary, we suppose that there is at least two different solutions ๐‘ฅ(๐‘ก, ๐‘ฅ0) and ๐‘Ÿ(๐‘ก, ๐‘ฅ0) of (1.1). From (2.3), the following inequality holds: ๐‘ฅ ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘Ÿ ๐‘ก, ๐‘ฅ0 โ‰ค (1 โˆ’ ๐‘ก ๐‘‡ ) ๐พ1 ๐‘ก 0 ๐‘ฅ ๐‘ , ๐‘ฅ0 โˆ’ ๐‘Ÿ ๐‘ , ๐‘ฅ0 ๐‘‘๐‘  + + ๐‘ก ๐‘‡ ๐พ1 ๐‘ฅ ๐‘ , ๐‘ฅ0 โˆ’ ๐‘Ÿ ๐‘ , ๐‘ฅ0 ๐‘‡ ๐‘ก ๐‘‘๐‘  + ๐พ2 0<๐‘ก ๐‘–<๐‘ก ๐‘ฅ ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘Ÿ ๐‘ก๐‘–, ๐‘ฅ0 + + ๐‘ก ๐‘‡ ๐พ2 ๐‘ ๐‘–=1 ๐‘ฅ ๐‘ก๐‘–, ๐‘ฅ0 โˆ’ ๐‘Ÿ ๐‘ก๐‘–, ๐‘ฅ0 โ‹ฏ 2.16 Setting ๐‘ฅ ๐‘ก, ๐‘ฅ0 โˆ’ ๐‘Ÿ ๐‘ก, ๐‘ฅ0 = ๐‘• ๐‘ก , the inequality (2.16) can be written as: ๐‘•(๐‘ก) โ‰ค (1 โˆ’ ๐‘ก ๐‘‡ ) ๐พ1 ๐‘ก 0 ๐‘•(๐‘ )๐‘‘๐‘  + ๐‘ก ๐‘‡ ๐พ1 ๐‘•(๐‘ ) ๐‘‡ ๐‘ก ๐‘‘๐‘  + ๐พ2 0<๐‘ก ๐‘–<๐‘ก ๐‘•(๐‘ก๐‘–) + ๐‘ก ๐‘‡ ๐พ2 ๐‘ ๐‘–=1 ๐‘•(๐‘ก๐‘–) Let max ๐‘กโˆˆ[0,๐‘‡] ๐‘•(๐‘ก) = ๐‘•0 โ‰ฅ 0 . By iteration, we get: ๐‘• ๐‘ก โ‰ค ๐‘ ๐‘š ๐›ผ ๐‘ก + ๐‘€ ๐‘š โ‹ฏ 2.17 From (2.14), we have: ๐‘ ๐‘š+1 ๐‘€ ๐‘š+1 = ๐พ1 ๐‘‡ 2 ๐พ1 ๐‘๐‘‡๐พ2 2๐‘๐พ2 ๐‘ ๐‘š ๐‘€ ๐‘š โ‹ฏ 2.18 which satisfies the initial conditions ๐‘0 = 0, ๐‘€0 = ๐‘•0 That is ๐‘ ๐‘š ๐‘€ ๐‘š = ๐พ1 ๐‘‡ 2 ๐พ1 ๐‘๐‘‡๐พ2 2๐‘๐พ2 ๐‘š 0 ๐‘• ๐‘š โ‹ฏ 2.19 Hence it is clear that if the condition (2.15) is satisfied then ๐‘ ๐‘š โ†’ 0 and ๐‘€ ๐‘š โ†’ 0 as ๐‘š โ†’ โˆž. From the relation (2.17) we get ๐‘•(๐‘ก) โ‰ก 0 or ๐‘ฅ ๐‘ก, ๐‘ฅ0 = ๐‘Ÿ ๐‘ก, ๐‘ฅ0 , i.e. ๐‘ฅ(๐‘ก, ๐‘ฅ0) is a unique solution of (1.1). โˆŽ III. EXISTENCE OF SOLUTION
  • 6. Periodic Solutions for Nonlinear Systems of Integro-Differential Equationsโ€ฆ www.ijeijournal.com P a g e | 62 The problem of the existence of periodic solution of period ๐‘‡ of the system (1.1) is uniquely connected with the existence of zeros of the function ฮ”(๐‘ฅ0) which has the form ฮ” ๐‘ฅ0 = 1 ๐‘‡ [ ๐‘“(๐‘ก, ๐‘ฅ0 ๐‘ก, ๐‘ฅ0 , ๐‘ฆ0 ๐‘ก, ๐‘ฅ0 , ๐‘ง0 ๐‘ก, ๐‘ฅ0 , ๐‘ค0 (๐‘ก, ๐‘ฅ0)) ๐‘‡ 0 ๐‘‘๐‘ก + + ๐ผ๐‘– ๐‘ ๐‘–=1 (๐‘ฅ0 ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ0 ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง0 ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค0 (๐‘ก๐‘–, ๐‘ฅ0))], โ‹ฏ 3.1 since this function is approximately determined from the sequence of functions ฮ”m ๐‘ฅ0 = 1 ๐‘‡ [ ๐‘“(๐‘ก, ๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘ค ๐‘š (๐‘ก, ๐‘ฅ0)) ๐‘‡ 0 ๐‘‘๐‘ก + + ๐ผ๐‘– ๐‘ ๐‘–=1 (๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š (๐‘ก๐‘–, ๐‘ฅ0))] โ‹ฏ 3.2 where ๐‘ฅ0 (๐‘ก, ๐‘ฅ0) is the limiting of the sequence of functions (2.1). Also ๐‘ฆ0 ๐‘ก, ๐‘ฅ0 = ๐ด๐‘ฅ0 ๐‘ก, ๐‘ฅ0 , ๐‘ง0 ๐‘ก, ๐‘ฅ0 = ๐ต๐‘ฅ0 (๐‘ก, ๐‘ฅ0) and ๐‘ค0 ๐‘ก, ๐‘ฅ0 = ๐‘”(๐‘ , ๐‘ฅ0 ๐‘ , ๐‘ฅ0 , ๐ด๐‘ฅ0 ๐‘ , ๐‘ฅ0 , ๐ต๐‘ฅ0 (๐‘ , ๐‘ฅ0)) ๐‘ก ๐‘กโˆ’๐‘‡ ๐‘‘๐‘  . Now, we prove the following theorem taking in to ///// that the following inequality will be satisfied for all ๐‘š โ‰ฅ 1. ฮ” ๐‘ฅ0 โˆ’ ฮ” ๐‘š (๐‘ฅ0) โ‰ค ๐œ† ๐‘š 1 โˆ’ ๐œ† โˆ’1 (๐พ1 + ๐‘ ๐‘‡ ๐พ2) ๐‘€๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) โ‹ฏ 3.3 Theorem 3.1. If the system of equations (1.1) satisfies the following conditions: (๐‘–) the sequence of functions (3.2) has an isolated singular point ๐‘ฅ0 = ๐‘ฅ0 , ฮ” ๐‘š (๐‘ฅ0) โ‰ก 0, for all ๐‘ก โˆˆ ๐‘…1 ; (๐‘–๐‘–) the index of this point is nonzero; (๐‘–๐‘–๐‘–) there exists a closed convex domain ๐ท4 belonging to the domain ๐ท๐‘“ and possessing a unique singular point ๐‘ฅ0 such that on it is boundary ฮ“ ๐ท4 the following inequality holds inf xโˆˆฮ“ ๐ท4 ฮ” ๐‘š (๐‘ฅ0 ) โ‰ค ๐œ† ๐‘š 1 โˆ’ ๐œ† โˆ’1 (๐พ1 + ๐‘ ๐‘‡ ๐พ2) ๐‘€๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) for all ๐‘š โ‰ฅ 1. Then the system (1.1) has a periodic solution ๐‘ฅ = ๐‘ฅ(๐‘ก, ๐‘ฅ0) for which ๐‘ฅ 0 โˆˆ ๐ท4. Proof. By using the inequality (3.3) we can prove the theorem is a similar way to that of theorem 2.1.2 [2]. Remark 3.1. When ๐‘… ๐‘› = ๐‘…1 , i.e. when ๐‘ฅ0 is a scalar, theorem 3.1 can be proved by the following. Theorem 3.2. Let the functions ๐‘“(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ฆ, ๐‘ง, ๐‘ค) and ๐ผ๐‘–(๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค) of system (1.1) are defined on the interval [๐‘Ž, ๐‘] in ๐‘…1 . Then the function (3.2) satisfies the inequalities: min ๐‘Ž+ ๐‘€๐‘‡ 2 1+ 4๐‘ ๐‘‡ โ‰ค๐‘ฅ0โ‰ค๐‘โˆ’ ๐‘€๐‘‡ 2 1+ 4๐‘ ๐‘‡ ฮ” ๐‘š ๐‘ฅ0 โ‰ค โˆ’ ๐œ† ๐‘š 1 โˆ’ ๐œ† โˆ’1 (๐พ1 + ๐‘ ๐‘‡ ๐พ2) max ๐‘Ž+ ๐‘€๐‘‡ 2 1+ 4๐‘ ๐‘‡ โ‰ค๐‘ฅ0โ‰ค๐‘โˆ’ ๐‘€๐‘‡ 2 1+ 4๐‘ ๐‘‡ ฮ” ๐‘š ๐‘ฅ0 โ‰ฅ ๐œ† ๐‘š 1 โˆ’ ๐œ† โˆ’1 (๐พ1 + ๐‘ ๐‘‡ ๐พ2) โ‹ฏ 3.4 Then (1.1) has a periodic solution in ๐‘ก of period ๐‘‡ for which ๐‘ฅ0 0 โˆˆ [๐‘Ž + ๐‘€๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ), ๐‘ โˆ’ ๐‘€๐‘‡ 2 (1 + 4๐‘ ๐‘‡ )] . Proof. Let ๐‘ฅ1 and ๐‘ฅ2 be any points of the interval [๐‘Ž + ๐‘€๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ), ๐‘ โˆ’ ๐‘€๐‘‡ 2 (1 + 4๐‘ ๐‘‡ )] such that ฮ” ๐‘š ๐‘ฅ1 = min ฮ” ๐‘š ๐‘ฅ0 ๐‘Ž+ ๐‘€๐‘‡ 2 1+ 4๐‘ ๐‘‡ โ‰ค๐‘ฅ0โ‰ค๐‘โˆ’ ๐‘€๐‘‡ 2 1+ 4๐‘ ๐‘‡ , ฮ” ๐‘š ๐‘ฅ2 = max ฮ” ๐‘š ๐‘ฅ0 ๐‘Ž+ ๐‘€๐‘‡ 2 1+ 4๐‘ ๐‘‡ โ‰ค๐‘ฅ0โ‰ค๐‘โˆ’ ๐‘€๐‘‡ 2 1+ 4๐‘ ๐‘‡ . โ‹ฏ 3.5 By using the inequalities (3.3) and (3.4) , we have ฮ” ๐‘š ๐‘ฅ1 = ฮ” ๐‘š ๐‘ฅ1 + ฮ” ๐‘š ๐‘ฅ1 โˆ’ ฮ” ๐‘š ๐‘ฅ1 < 0 , ฮ” ๐‘š ๐‘ฅ2 = ฮ” ๐‘š ๐‘ฅ2 + (ฮ” ๐‘š ๐‘ฅ2 โˆ’ ฮ” ๐‘š ๐‘ฅ2 ) > 0 . 3.6
  • 7. Periodic Solutions for Nonlinear Systems of Integro-Differential Equationsโ€ฆ www.ijeijournal.com P a g e | 63 The continuity of ฮ”(๐‘ฅ0 ) and by using (3.6), there exists a point ๐‘ฅ0 , ๐‘ฅ0 โˆˆ ๐‘ฅ1, ๐‘ฅ2 , such that ฮ”(๐‘ฅ0 ) โ‰ก 0, i.e. ๐‘ฅ = ๐‘ฅ(๐‘ก, ๐‘ฅ0) is a periodic solution in ๐‘ก of period ๐‘‡ for which ๐‘ฅ0 (0) โˆˆ [๐‘Ž + ๐‘€๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ), ๐‘ โˆ’ ๐‘€๐‘‡ 2 (1 + 4๐‘ ๐‘‡ )] . โˆŽ Similar results can be obtained for other class of integro-differential equations of operators with impulsive action. In particular, the system of integro-differential equations which has the form ๐‘‘๐‘ฅ ๐‘‘๐‘ก = ๐‘“(๐‘ก, ๐‘ฅ, ๐ด๐‘ฅ, ๐ต๐‘ฅ, ๐‘” ๐‘ , ๐‘ฅ ๐‘  , ๐ด๐‘ฅ ๐‘  , ๐ต๐‘ฅ ๐‘  ๐‘‘๐‘  ๐‘ ๐‘ก ๐‘Ž ๐‘ก , , ๐น ๐‘ก, ๐‘  ๐‘ก โˆ’โˆž ๐‘” ๐‘ , ๐‘ฅ ๐‘  , ๐ด๐‘ฅ ๐‘  , ๐ต๐‘ฅ ๐‘  ๐‘‘๐‘  , ๐‘ก โ‰  ๐‘ก๐‘– ฮ”๐‘ฅ = |๐‘ก=๐‘ก ๐‘– ๐ผ๐‘–(๐‘ฅ, ๐ด๐‘ฅ, ๐ต๐‘ฅ, ๐‘” ๐‘ , ๐‘ฅ ๐‘  , ๐ด๐‘ฅ ๐‘  , ๐ต๐‘ฅ ๐‘  ๐‘‘๐‘ , ๐‘(๐‘ก ๐‘–) ๐‘Ž(๐‘ก ๐‘–) , ๐น ๐‘ก๐‘–, ๐‘  ๐‘”(๐‘ , ๐‘ฅ ๐‘  , ๐ด๐‘ฅ ๐‘  , ๐ต๐‘ฅ(๐‘ ))๐‘‘๐‘  ๐‘ก ๐‘– โˆ’โˆž ) โ‹ฏ 3.7 In this system (3.7), let the vector functions ๐‘“ ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค , ๐‘”(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง) and scalar functions ๐‘Ž ๐‘ก , ๐‘(๐‘ก) are periodic in ๐‘ก of period ๐‘‡, defined and continuous on the domain. ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘• โˆˆ ๐‘…1 ร— ๐บ ร— ๐บ1 ร— ๐บ2 ร— ๐บ3 ร— ๐บ4 = = โˆ’โˆž, โˆž ร— ๐บ ร— ๐บ1 ร— ๐บ2 ร— ๐บ3 ร— ๐บ4 โ‹ฏ 3.8 Let ๐ผ๐‘– ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘• be a continuous vector function which are defined on the domain (3.8). A matrix ๐น ๐‘ก, ๐‘  is defined and continuous in ๐‘…1 ร— ๐‘…1 and satisfies the condition ๐น ๐‘ก + ๐‘‡, ๐‘  + ๐‘‡ = ๐น ๐‘ก, ๐‘  which ๐น ๐‘ก, ๐‘  โ‰ค ๐›ฟ ๐‘’โˆ’๐›พ ๐‘กโˆ’๐‘  , 0 โ‰ค ๐‘  โ‰ค t โ‰ค T , where ๐›ฟ, ๐›พ are a positive constants. Suppose that the functions ๐‘“(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘•) and ๐‘” ๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง , ๐ผ๐‘– ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘• are satisfying the following inequalities: ๐‘“(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘•) โ‰ค ๐‘€ , ๐‘”(๐‘ก, ๐‘ฅ, ๐‘ฆ, ๐‘ง) โ‰ค ๐‘ , โ‹ฏ 3.9 ๐‘“ ๐‘ก, ๐‘ฅ1, ๐‘ฆ1, ๐‘ง1, ๐‘ค1, ๐‘•1 โˆ’ ๐‘“ ๐‘ก, ๐‘ฅ2, ๐‘ฆ2, ๐‘ง2, ๐‘ค2, ๐‘•2 โ‰ค ๐พโˆ— ( ๐‘ฅ1 โˆ’ ๐‘ฅ2 + ๐‘ฆ1 โˆ’ ๐‘ฆ2 + + ๐‘ง1 โˆ’ ๐‘ง2 + ๐‘ค1 โˆ’ ๐‘ค2 + ๐‘•1 โˆ’ ๐‘•2 ); ๐‘” ๐‘ก, ๐‘ฅ1, ๐‘ฆ1, ๐‘ง1 โˆ’ ๐‘” ๐‘ก, ๐‘ฅ2, ๐‘ฆ2, ๐‘ง2 โ‰ค ๐‘„โˆ— ๐‘ฅ1 โˆ’ ๐‘ฅ2 + ๐‘ฆ1 โˆ’ ๐‘ฆ2 + ๐‘ง1 โˆ’ ๐‘ง2 ; โ‹ฏ 3.10 ๐ผ๐‘– ๐‘ฅ1, ๐‘ฆ1, ๐‘ง1, ๐‘ค1, ๐‘•1 โˆ’ ๐ผ๐‘– ๐‘ฅ2, ๐‘ฆ2, ๐‘ง2, ๐‘ค2, ๐‘•2 โ‰ค ๐ฟโˆ— ( ๐‘ฅ1 โˆ’ ๐‘ฅ2 + ๐‘ฆ1 โˆ’ ๐‘ฆ2 + + ๐‘ง1 โˆ’ ๐‘ง2 + ๐‘ค1 โˆ’ ๐‘ค2 + ๐‘•1 โˆ’ ๐‘•2 ); โ‹ฏ 3.11 and ๐ด๐‘ฅ1 ๐‘ก โˆ’ ๐ด๐‘ฅ2 ๐‘ก โ‰ค ๐บโˆ— ๐‘ฅ1 ๐‘ก โˆ’ ๐‘ฅ2 ๐‘ก , ๐ต๐‘ฅ1 ๐‘ก โˆ’ ๐ต๐‘ฅ2 ๐‘ก โ‰ค ๐ปโˆ— ๐‘ฅ1 ๐‘ก โˆ’ ๐‘ฅ2 ๐‘ก . โ‹ฏ 3.12 for all ๐‘ก โˆˆ ๐‘…1 , ๐‘ฅ, ๐‘ฅ1, ๐‘ฅ2 โˆˆ ๐บ, ๐‘ฆ, ๐‘ฆ1, ๐‘ฆ2 โˆˆ ๐บ1, ๐‘ง, ๐‘ง1, ๐‘ง2 โˆˆ ๐บ2, ๐‘ค, ๐‘ค1, ๐‘ค2 โˆˆ ๐บ3, ๐‘•, ๐‘•1, ๐‘•2 โˆˆ ๐บ4 , Provided that ๐ด๐‘ฅ ๐‘ก + ๐‘‡ = ๐ด๐‘ฅ ๐‘ก , ๐ต๐‘ฅ ๐‘ก + ๐‘‡ = ๐ต๐‘ฅ ๐‘ก , ๐ผ๐‘–+๐‘ ๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘• = ๐ผ๐‘–(๐‘ฅ, ๐‘ฆ, ๐‘ง, ๐‘ค, ๐‘•) and ๐‘ก๐‘–+๐‘ = ๐‘ก๐‘– + ๐‘‡. Define a non-empty sets as follows: ๐บ๐‘“ = ๐บ โˆ’ ๐‘€โˆ— ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) , ๐บ1๐‘“ = ๐บ1 โˆ’ ๐บโˆ— ๐‘€โˆ— ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ), ๐บ2๐‘“ = ๐บ3 โˆ’ ๐ปโˆ— ๐‘€โˆ— ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) , ๐บ4๐‘“ = ๐บ4 โˆ’ ๐›ฝ๐‘„โˆ— ๐‘€โˆ— ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) , ๐บ5๐‘“ = ๐บ5 โˆ’ ๐›ฟ ๐›พ ๐‘„โˆ— ๐‘€โˆ— ๐‘‡ 2 (1 + 4๐‘ ๐‘‡ ) . โ‹ฏ 3.13 Furthermore, the largest Eigen-value of ๐›พ ๐‘š๐‘Ž๐‘ฅ of the matrix ฮ“ = ๐พ1 ๐‘‡ 2 ๐พ1 ๐‘๐พ2 ๐‘‡ 2๐‘๐พ2 is less than unity, i.e.
  • 8. Periodic Solutions for Nonlinear Systems of Integro-Differential Equationsโ€ฆ www.ijeijournal.com P a g e | 64 1 2 [๐พ1 ๐‘‡ 3 + 2๐‘๐พ2 + ( ๐พ1 ๐‘‡ 3 + 2๐‘๐พ2)2 + 4๐‘๐พ1 ๐พ2 ๐‘‡ 3 ] < 1 , โ‹ฏ 3.14 where ๐พ1 = ๐พโˆ— [1 + ๐บโˆ— + ๐ปโˆ— + ๐›ฟ ๐›พ ๐‘„โˆ— + ๐‘„โˆ— (1 + ๐บโˆ— + ๐›ฝ)], ๐พ2 = ๐ฟโˆ— [1 + ๐บโˆ— + ๐ปโˆ— + ๐›ฟ ๐›พ ๐‘„โˆ— + ๐‘„โˆ— (1 + ๐บโˆ— + ๐›ฝ)] and ๐›ฝ = max0โ‰ค๐‘กโ‰ค๐‘‡ ๐‘ ๐‘ก โˆ’ ๐‘Ž(๐‘ก) . Theorem 3.2. If the system of integro-differential equations with impulsive action (3.7) satisfying the above assumptions and conditions has a periodic solution ๐‘ฅ = ๐œ“ ๐‘ก, ๐‘ฅ0 , then there exists a unique solution which is the limit function of a uniformly convergent sequence which has the form ๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 = ๐‘ฅ0 + [๐‘“(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘• ๐‘š (๐‘ , ๐‘ฅ0) ๐‘ก 0 ) โˆ’ โˆ’ 1 ๐‘‡ ๐‘“(๐‘ , ๐‘ฅ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ , ๐‘ฅ0 , ๐‘• ๐‘š (๐‘ , ๐‘ฅ0)) ๐‘‡ 0 ๐‘‘๐‘ ]๐‘‘๐‘  + + ๐ผ๐‘– 0<๐‘ก ๐‘–<๐‘ก (๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘• ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 ) โˆ’ โˆ’ ๐‘ก ๐‘‡ ๐ผ๐‘–(๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘• ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 ) ๐‘ ๐‘–=1 โ‹ฏ 3.15 with ๐‘ฅ0 ๐‘ก, ๐‘ฅ0 = ๐‘ฅ0 , ๐‘š = 0,1,2, โ‹ฏ. The proof is a similar to that of theorem 1.1. If we consider the following mapping ฮ”m ๐‘ฅ0 = 1 ๐‘‡ [ ๐‘“(๐‘ก, ๐‘ฅ ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก, ๐‘ฅ0 , ๐‘• ๐‘š (๐‘ก, ๐‘ฅ0)) ๐‘‡ 0 ๐‘‘๐‘ก + + ๐ผ๐‘– ๐‘ ๐‘–=1 (๐‘ฅ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ฆ ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ง ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘ค ๐‘š ๐‘ก๐‘–, ๐‘ฅ0 , ๐‘• ๐‘š (๐‘ก๐‘–, ๐‘ฅ0))]. โ‹ฏ 3.16 Then we can state a theorem similar to theorem 2.2, provided that ๐›พ ๐‘š๐‘Ž๐‘ฅ = 1 2 [๐พ1 ๐‘‡ 3 + 2๐‘๐พ2 + ( ๐พ1 ๐‘‡ 3 + 2๐‘๐พ2)2 + 4๐‘๐พ1 ๐พ2 ๐‘‡ 3 ] < 1 , Remark 3.2. It is clear that when we put ๐ผ๐‘– โ‰ก 0, we get a periodic solution for the systems (1.1) and (3.7) without introducing impulsive action. REFERENCES 1) Butris, R. N. , Existence of a periodic solutions for nonlinear systems of differential equations of operators with impulsive action, Iraq,Mosul Univ J. Ed. and Sci., Vol.(15),(1994). 2) [2] Butris,R.N.and Saied El.M.On periodic solutions for certain systems of integro-differen tial equations Iraq ,Mosul Univ., J.of Educ_and Sci., vol 31, (1998) 3) [3] Korol, I. I. , On periodic solutions of one class of systems of differential 4) equations, Ukrainian, Mathematical J. Vol.57, No. 4, (2005). 5) [4] Perestyuk ,N.A.On periodic solutions of some of differential equations. In asymptotic and qualitative method in the theory of nonlinear oscillations. Ukrainian Academy of sciences, Kiev (1971) 6) [5] Samoilenko, A. M. and Perestyuk, N. A. , Differential equations with impulsive 7) action, Ukrainian, Kiev, (1987). 8) [6] Samoilenko, A. M. and Ronto, N. I. , Numerical-analytic methods of 9) investigating periodic solutions, Ukrainian, Kiev, (1976). 10) [7] Tian yu. and Dehong Ji. , Weigao Ge. Existence and non existence results of 11) impulsive first-order problem with integral boundary condition, J. Nonlinear 12) analysis, Vol. 71, (2009). 13) [8] Voskresenskii E.V., periodic solutions of nonlinear system sand the averaging method, translated form differential equations . State Univ .,vol 28. No 4.(1992).