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Article

Existence Results for Systems of Nonlinear Second-Order and Impulsive Differential Equations with Periodic Boundary

1
Department of Mathematics, College of Science, University of Ha’il, Ha’il 55473, Saudi Arabia
2
Department of Mathematics, Faculty of Mathematics and Informatics, University of Science and Technology of Oran Mohamed-Boudiaf (USTOMB), El Mnaouar, P.O. Box 1505, Bir El Djir 31000, Oran, Algeria
3
Department of Mathematics, College of Science, King Khalid University, P.O. Box 9004, Abha 61413, Saudi Arabia
4
Department of Mathematics, College of Sciences and Arts in Ar-Rass, Qassim University, Saudi Arabia
*
Author to whom correspondence should be addressed.
Mathematics 2023, 11(24), 4907; https://doi.org/10.3390/math11244907
Submission received: 2 November 2023 / Revised: 5 December 2023 / Accepted: 6 December 2023 / Published: 8 December 2023
(This article belongs to the Special Issue Mathematical Methods for Nonlinear Dynamics)

Abstract

:
A class for systems of nonlinear second-order differential equations with periodic impulse action are considered. An urgent problem for this class of differential equations is the problem of the quantitative study (existence) in the case when the phase space of the equation is, in the general case, some Banach space. In this work, sufficient conditions for the existence of solutions for a system with parameters are obtained. The results are obtained by using fixed point theorems for operators on a cone. Our approach is based on Schaefer’s fixed point theorem more precisely. In addition, the existence of positive solutions is also investigated.

1. Introduction and Some Historical Review

Differential equations with impulse action are an important subclass of hybrid systems, i.e., systems of differential equations that merge continuous and discrete time dynamics. They are a new direction in differential equations theory, which has many applications to models of mathematical problems in mechanics, biology, and engineering [1,2]. The very important problem for this type of system is the question of the qualitative properties of solutions. The fundamentals of the theory of the stability of solutions to problems of differential equations with impulse action are presented in [3], where a direct Lyapunov method for this type of problem was also developed. Certain of the relevant results are generalized in monograph [4] using piecewise differentiable auxiliary functions. The works [5,6] show the universality of the direct Lyapunov method in this class of auxiliary functions. In [7], stability conditions for solutions of a nonlinear system with impulse action were obtained based on two auxiliary functions. It is shown that the obtained stability conditions generalize theorems from the monograph [3]. Relevant and important from a practical point of view is the question of the stability for systems of differential equations with impulse action in critical cases. In [8], the problem of generalizing the reduction principle for certain classes of systems of differential equations with impulse action is considered. This principle is a very important tool for study of critical cases; actually, it is reduced to the study of the qualitative properties for a system on the central manifold. Studying the properties of a system of differential equations on a central manifold requires a certain skill of the researcher, since there are no general research methods.
We consider a system of nonlinear second-order and impulsive differential equations with the periodic boundary
u λ 2 u = f 1 ( t , u , v , θ ) , t J = [ 0 , 2 π ] , t t k , k 1 , m N , v λ 2 v = f 2 ( t , u , v , θ ) t J , t t k , k 1 , m N , u ( t k + ) u ( t k ) = I k 1 ( u ( t k ) , v ( t k ) ) , k 1 , m N , v ( t k + ) v ( t k ) = I k 2 ( u ( t k ) , v ( t k ) ) , k 1 , m N , u ( t k + ) u ( t k ) = I ¯ k 1 ( u ( t k ) , v ( t k ) ) , k 1 , m N , v ( t k + ) v ( t k ) = I ¯ k 2 ( u ( t k ) , v ( t k ) ) , k 1 , m N , u ( t = 0 ) = u ( t = 2 π ) , u ( t = 0 ) = u ( t = 2 π ) , v ( t = 0 ) = v ( t = 2 π ) , v ( t = 0 ) = v ( 2 π ) ,
where n , m N = n , n + 1 , . . . , m , for all n , m N , λ R * , u = u ( t ) , v = v ( t ) , and θ is a real parameter, f 1 , f 2 C 0 ( J × R × R , R ) are given functions, I k i , I ¯ k i C ( R × R , R ) , t k J , 0 = t 0 < t 1 < < t m < t m + 1 = 2 π , u ( t k + ) = lim h 0 + u ( t k + h ) and u ( t k ) = lim h 0 + u ( t k h ) represent the right and left limits of u ( t ) at t = t k . It is well known that much research has been conducted on the question of the existence of solutions for a system of impulsive differential equations; see, for example, [9,10,11,12,13]. In [9,14], the existence of solutions for systems with a nonlocal coupled nonlinear initial condition is studied owing to the different fixed point principles. In this work, in particular, the problem of the existence of positive solutions for the original system of differential equations in second order with impulse action is reduced to the study of a system of nonlinear differential equations with impulse action with equidistant moments of impulse action. The purpose of this work is to develop some existing ideas for differential equations with impulse action. At the same time, along with the ideas in the work [15], new ideas are proposed related to the second-order differential equations with impulse action, see Refs. [16,17,18].
The paper proceeds as follows. After the introduction and position of problem, in Section 2, we recall some related definitions and facts, which will be useful in our analysis. In Section 3, we use the Perov and Schaefer’s type to obtain additional existence results. In Section 4, some existence results based on the Krasnosel’skii-type Theorem in generalized Banach spaces is obtained. Our study concludes with a discussion.

2. Statement of the Problem and Auxiliary Results

Let us recall some important results on the existence of linear/nonlinear impulsive systems, which are generalized in this paper. To this end, let us first set
J 0 = [ 0 , t 1 ] , J k = ( t k , t k + 1 ] , k 1 , m N ,
and let u k be the restriction of the function u to J k . We consider the space C ( J , R ) to be the Banach space of all continuous functions from J into R with the norm
u = sup t J | u ( t ) | .
L 1 ( J , R ) denotes the Banach space of measurable functions u C 0 ( J , R ) , which are Bochner integrable and normed by
u L 1 = J | u ( t ) | d t .
AC i ( J , R ) is the space of i-times differentiable functions u C 0 ( J , R ) , whose i t h derivative, u i , is absolutely continuous
PC ( J , R ) = u C 0 ( J , R ) : u is continuous everywhere except for some at which u ( t k ) and u ( t k + ) exist , and u ( t k ) = u ( t k ) , k 1 , m N .
Clearly, PC is a Banach space with the norm
u PC = sup t J | u ( t ) | .
Let PC ( J , R ) × PC ( J , R ) be endowed with the vector norm . defined by
w = ( u PC , v PC ) , w = ( u , v ) ,
where for u PC ( J , R ) , we set u PC = sup t J | u ( t ) | ; it is obvious that ( PC × PC , . ) is a generalized Banach space.
u = ( u 1 , u 2 , , u n ) , v = ( v 1 , v 2 , , v n ) R n , and we note the partial order relation,
u v u i v i , i 1 , n N .
Let X , d i i 1 , n N be a finite sequence of metric. Let the map d C 0 ( X × X , R n ) be given by
d ( u , v ) = d 1 ( u , v ) , . . . , d n ( u , v ) ,
and the pair ( X , d ) is called a generalized metric space.
Let . i be an end sequence of norms on u, let the map u C 0 ( X , R n ) be given by
u = u 1 , . . . , u n ,
and the pair ( X , . ) is called a generalized norms space.
Remark 1.
Let ( X , . ) be a generalized norms space, abd we pose
d ( u , v ) = u v , u , v X ;
then, ( X , . ) is a generalized norms space.
Theorem 1
([19]). Let M M n × n ( R + ) , and the next claims are equivalent:
(a)
M is convergent towards 0,
(b)
M k 0 as k ,
(c)
The matrix ( I d M ) is nonsingular, and ( I d M ) 1 = k = 0 k = I k ,
(d)
The matrix ( I d M ) is nonsingular, and ( I d M ) 1 has nonnegative elements.
Let ( X , d ) be a generalized metric space. An operator N C 0 ( X , X ) is said to be contractive associated with d on X, if there exists a convergent to 0 matrix M, such that
d ( T ( u ) , T ( v ) ) M d ( u , v ) , u , v X .
The function f C 0 ( [ 0 , 1 ] × R × R , R ) is an L 1 -Carathéodory function, if
  • t f ( t , u , v ) is measurable for any ( u , v ) R 2 ,
  • ( u , v ) f ( t , . , . ) is a continuous almost everywhere 0 t 1 ,
  • For r 1 , r 2 > 0 , there exists ϕ r 1 , r 2 L 1 ( [ 0 , + [ ) , so that | f ( t , u , v ) | ϕ r 1 , r 2 ( t ) , ( u , v ) R 2 , with | u | r 1 , | v | r 2 and almost everywhere t [ 0 , 1 ] .
Theorem 2
([15], page 149). Let X be a generalized Banach space, and let T : X X be a completely continuous map. If the set
Φ = { u X : u = λ 1 T u , f o r s o m e λ 1 ( 0 , 1 ) }
is bounded, then T has a fixed point.
Then, we recall the vectorial version of the fixed point Theorem, see [20].
Theorem 3
(Perov fixed point Theorem). Let ( X , d ) be a complete generalized metric space and T C 0 ( X , X ) be a contractive operator with Lipschitz matrix M. Then, T has a unique fixed point u, and for each u 0 X ,
d ( T k ( u 0 , u ) M k ( I d M ) 1 d ( u 0 , T ( u 0 ) ) , w h e r e k N .

3. Existence of Solutions

A sufficient condition is given to prove the existence of solutions to (1) owing to Perov’s fixed point Theorem. We state without proof the next Lemma 1, which is useful to transform problem (1) into a fixed point problem. Its proof is not difficult.
Lemma 1.
Let u , v PC ( J , R ) C 1 ( ( t k , t k + 1 ) , k 0 , m N be a solution of (1), if and only if u , v PC ( J , R ) is a solution of the following impulsive integral equation
u ( t ) = 0 2 π H ( t , s ) f 1 ( t , u ( s ) , v ( s ) , θ ) d s k = 1 m H ( t , t k ) I k 1 ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k 1 ( u ( t k ) , v ( t k ) ) , t J ,
and
v ( t ) = 0 2 π H ( t , s ) f 2 ( t , u ( s ) , v ( s ) , θ ) d s k = 1 m H ( t , t k ) I k 2 ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k 2 ( u ( t k ) , v ( t k ) ) , t J ,
where
H ( t , s ) = 1 2 λ ( e 2 λ π 1 ) e λ ( t s ) + e λ ( 2 π t + s ) , 0 s < t 2 π , e λ ( s t ) + e λ ( 2 π s + t ) , 0 t < s 2 π ,
and
L ( t , s ) = t H ( t , s ) = 1 2 ( e 2 λ π 1 ) e λ ( 2 π t + s ) e λ ( t s ) , 0 s < t 2 π , e λ ( s t ) e λ ( 2 π s + t ) , 0 t < s 2 π .
We assume that
( H 1 )
There exist constants a f i , b f i R + for each i = 1 , 2 , such that
| f i ( t , u , v , θ ) f i ( t , u ¯ , v ¯ , θ ) | a f i | u u ¯ | + b f i | v v ¯ | ,
for each t J and all u , u ¯ , v , v ¯ R .
( H 2 )
There exist d k i , d k i + 1 , d ¯ k i , d ¯ k i + 1 R + for each k 1 , m N , i = 1 , 2 , such that
| I k i ( u , v ) I k i ( u ¯ , v ¯ ) | d k i | u u ¯ | + d k i + 1 | v v ¯ | | I ¯ k i ( u , v ) I ¯ k i ( u ¯ , v ¯ ) | d ¯ k i | u u ¯ | + d ¯ k i + 1 | v v ¯ | ,
for each t J and all u , u ¯ , v , v ¯ R .
Theorem 4.
Assume that ( H 1 ) ( H 2 ) are satisfied, and the matrix
M t r i x = q 1 q ¯ 1 q 2 q ¯ 2 M 2 × 2 ( R + ) ,
where
q 1 = 2 π sup ( t , s ) J 2 ( H ( t , s ) ) a f 1 + k = 1 m d k 1 sup t J | H ( t , t k ) | + d ¯ k 1 sup t J | L ( t , t k ) | ,
q ¯ 1 = 2 π sup ( t , s ) J 2 ( H ( t , s ) ) b f 1 + k = 1 m d k 2 sup t J | H ( t , t k ) | + d ¯ k 2 sup t J | L ( t , t k ) | ,
and
q 2 = 2 π sup ( t , s ) J 2 ( H ( t , s ) ) a f 2 + k = 1 m d k 2 sup t J | H ( t , t k ) | + d ¯ k 3 sup t J | L ( t , t k ) | ,
q ¯ 2 = 2 π sup ( t , s ) J 2 ( H ( t , s ) ) b f 2 + k = 1 m d k 2 sup t J | H ( t , t k ) | + d ¯ k 3 sup t J | L ( t , t k ) | .
If M t r i x converges to 0, then the problem (1) has a solution on J .
Proof. 
Consider the operator
N : PC × PC PC × PC ( u , v ) N 1 ( t , u , v ) , N 2 ( t , u , v ) ,
N 1 ( u , v ) ( t ) = 0 2 π H ( t , s ) f 1 ( t , u ( s ) , v ( s ) , θ ) d s k = 1 m H ( t , t k ) I k 1 ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k 1 ( u ( t k ) , v ( t k ) ) , t J ,
and
N 2 ( u , v ) ( t ) = 0 2 π H ( t , s ) f 2 ( t , u ( s ) , v ( s ) , θ ) d s k = 1 m H ( t , t k ) I k 2 ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k 2 ( u ( t k ) , v ( t k ) ) , t J .
We use Theorem 3 to prove that N has a fixed point. Indeed, let ( u , v ) , ( u ¯ , v ¯ ) PC × PC . Then, we have, for each t J ,
N 1 ( t , u , v ) N 1 ( t , u ¯ , v ¯ ) 2 π sup ( t , s ) J 2 ( H ( t , s ) ) a f 1 u u ¯ PC + b f 1 v v ¯ PC + k = 1 m d k 1 sup t J | H ( t , t k ) | + d ¯ k 1 sup t J | L ( t , t k ) | u u ¯ PC + k = 1 m d k 2 sup t J | H ( t , t k ) | + d ¯ k 2 sup t J | L ( t , t k ) | v v ¯ PC 2 π sup ( t , s ) J 2 ( H ( t , s ) ) a f 1 + k = 1 m d k 1 sup t J | H ( t , t k ) | + d ¯ k 1 sup t J | L ( t , t k ) | u u ¯ PC + 2 π sup ( t , s ) J 2 ( H ( t , s ) ) b f 1 + k = 1 m d k 2 sup t J | H ( t , t k ) | + d ¯ k 2 sup t J | L ( t , t k ) | v v ¯ PC .
Thus,
N 1 ( t , u , v ) N 1 ( t , u ¯ , v ¯ ) PC q 1 u u ¯ PC + q ¯ 1 v v ¯ PC .
Similarly, we have
N 2 ( t , u , v ) N 2 ( t , u ¯ , v ¯ ) PC q 2 u u ¯ PC + q ¯ 2 v v ¯ PC .
Hence,
N ( u , v ) N ( u ¯ , v ¯ ) PC = N 1 ( ( u , v ) N 1 ( u ¯ , v ¯ ) PC N 2 ( u , v ) N 2 ( u ¯ , v ¯ ) PC q 1 q ¯ 1 q 2 q ¯ 2 u u ¯ PC v v ¯ PC .
This implies that
N ( u , v ) N ( u ¯ , v ¯ ) PC M t r i x u u ¯ PC v v ¯ PC . ( u , v ) , ( u ¯ , v ¯ ) PC × PC .
From the Perov fixed point Theorem, the mapping N has a unique fixed ( u , v ) PC × PC , which is the unique solution of problem (1). This completes the proof. □

Existence Results

In this section, we state our main existence results for problem (1). To this end, we assume
( H 3 )
There exist a function p i L 1 ( J , R + ) and constants 0 α i , β i < 1 , such that
| f i ( t , u , v , θ ) | p f i ( t ) | u | α i + p ¯ f i ( t ) | v | β i ,
t J and u , v R ,   i = 1 , 2 .
( H 4 )
There exist constants d k i , d k i + 1 , d ¯ k i , d ¯ k i + 1 R + for each k 1 , m N , i = 1 , 2 and a constants 0 α i , β i < 1 such that
| I k i ( u , v ) | d k i | u | α i + d k i + 1 | v | β i | I ¯ k i ( u , v ) | d ¯ k i | u | α i + d ¯ k i + 1 | v | β i ,
t J and all u , v R , i = 1 , 2 .
( H 5 )
f i C 0 ( J × R × R , R ) is a Carath e ´ odory function, and I k i , I ¯ k i C ( R × R , R ) .
Theorem 5.
Assume that ( H 3 ) ( H 5 ) hold. Then, (1) has at least one solution on J . Moreover, the solution set
S = ( u , v ) PC × PC : ( u , v ) i s t h e s o l u t i o n o f ( 1 ) ,
and it is compact.
Proof. 
Clearly, the fixed points of N are solutions to (1), where N is defined in Theorem 4. In order to apply Theorem 2, we first show that N is completely continuous. The proof is given in several steps.
Step 1: 
N = ( N 1 , N 2 ) is continuous.
Let ( u n , v n ) be a sequence, such that ( u n , v n ) ( u , v ) PC × PC , as n . Since f 1 , f 2 is a Carath e ´ odory function, by the Lebesgue dominated convergence Theorem, we obtain
| N 1 ( u n , v n ) ( t ) N 1 ( u , v ) ( t ) | sup ( t , s ) J 2 | H ( t , s ) | 0 2 π | f 1 ( t , u n ( s ) , v n ( s ) , θ ) f 1 ( t , u ( s ) , v ( s ) , θ ) | d s + k = 1 m sup t J | H ( t , t k ) | | I k 1 ( u n ( t k ) , v n ( t k ) ) I k 1 ( u ( t k ) , v ( t k ) ) | + k = 1 m sup t J | L ( t , t k ) | | I ¯ k 1 ( u n ( t k ) , v n ( t k ) ) I ¯ k 1 ( u ( t k ) , v ( t k ) ) | 0 ,
as n . Similarly,
| N 2 ( u n , v n ) ( t ) N 2 ( u , v ) ( t ) | sup ( t , s ) J 2 | H ( t , s ) | 0 2 π | f 2 ( t , u n ( s ) , v n ( s ) , θ ) f 2 ( t , u ( s ) , v ( s ) , θ ) | d s + k = 1 m sup t J | H ( t , t k ) | | I k 2 ( u n ( t k ) , v n ( t k ) ) I k 2 ( u ( t k ) , v ( t k ) ) | + k = 1 m sup t J | L ( t , t k ) | | I ¯ k 2 ( u n ( t k ) , v n ( t k ) ) I ¯ k 2 ( u ( t k ) , v ( t k ) ) | 0 ,
when n . Then, N is continuous.
Step 2: 
N maps bounded sets into bounded sets in PC × PC . It is enough to show that q > 0 , there exists l > 0 , such that for each
( u , v ) B q = { ( u , v ) PC × PC : u PC q , v q } .
We obtain
N ( u , v ) PC l = ( l 1 , l 2 ) .
Then, for each t J , we obtain
| N 1 ( u , v ) ( t ) | sup ( t , s ) J 2 | H ( t , s ) | q α 1 0 2 π p f 1 ( s ) d s + q β 1 0 2 π p ¯ f 1 ( s ) d s + k = 1 m sup t J | H ( t , t k ) | d k 1 q α 1 + d k 2 q β 1 + k = 1 m sup t J | L ( t , t k ) | d ¯ k 1 q α 1 + d ¯ k 2 q β 1 ,
which implies that
N 1 ( u , v ) PC sup ( t , s ) J 2 | H ( t , s ) | q α 1 p f 1 L 1 + q β 1 p ¯ f 1 L 1 + k = 1 m sup t J | H ( t , t k ) | d k 1 q α 1 + d k 2 q β 1 + k = 1 m sup t J | L ( t , t k ) | d ¯ k 1 q α 1 + d ¯ k 2 q β 1 = 1 .
Similarly, we have
N 2 ( u , v ) PC sup ( t , s ) J 2 | H ( t , s ) | q α 1 p f 2 L 1 + q β 1 p ¯ f 2 L 1 + k = 1 m sup t J | H ( t , t k ) | d k 2 q α 2 + d k 3 q β 2 + k = 1 m sup t J | L ( t , t k ) | d ¯ k 2 q α 2 + d ¯ k 3 q β 2 = 2 .
Step 3: 
N maps bounded sets into the equi-continuous one of PC × PC . We set t 1 , t 2 J , t 1 , t 2 > 0 , and t 1 < t 2 with B q as a bounded set of PC × PC , the same as in Step 2. Let u , v B q ; then, for t J , we obtain
| N 1 ( u , v ) ( t 2 ) N 1 ( u , v ) ( t 1 ) | q α 1 0 t 1 | H ( t 2 , s ) H ( t 1 , s ) | p f 1 ( s ) d s + q β 1 0 t 1 | H ( t 2 , s ) H ( t 1 , s ) | p ¯ f 1 ( s ) d s + q α 1 t 1 t 2 | H ( t 2 , s ) | p f 1 ( s ) d s + q β 1 t 1 t 2 | H ( t 2 , s ) | p ¯ f 1 ( s ) d s + t 1 < t < t 2 | H ( t 2 , t k ) H ( t 1 , t k ) | ( d k 1 q α 1 + d k 2 q β 1 ) + t 1 < t < t 2 | L ( t 2 , t k ) L ( t 1 , t k ) | ( d ¯ k 1 q α 1 + d ¯ k 2 q β 1 ) ,
and
| N 2 ( u , v ) ( t 2 ) N 2 ( u , v ) ( t 1 ) | q α 1 0 t 1 | H ( t 2 , s ) H ( t 1 , s ) | p f 2 ( s ) d s + q β 1 0 t 1 | H ( t 2 , s ) H ( t 1 , s ) | p ¯ f 2 ( s ) d s + q α 1 t 1 t 2 | H ( t 2 , s ) | p f 2 ( s ) d s + q β 1 t 1 t 2 | H ( t 2 , s ) | p ¯ f 2 ( s ) d s + t 1 < t < t 2 | H ( t 2 , t k ) H ( t 1 , t k ) | ( d k 2 q α 2 + d k 3 q β 2 ) + t 1 < t < t 2 | L ( t 2 , t k ) L ( t 1 , t k ) | ( d ¯ k 2 q α 2 + d ¯ k 3 q β 2 ) .
The term in the RHS tends to 0, as t 2 t 1 goes to 0.
This proves the equi-continuity for the case where t t i , i 1 , m + 1 N . It remains to examine the equi-continuity at t = t i . First, we prove equi-continuity at t = t i . Fix ν 1 > 0 , such that { t k : k i } [ t i ν 1 , t i + ν 1 ] = . For 0 < h < ν 1 , we obtain
| N 1 ( u , v ) ( t i ) N 1 ( u , v ) ( t i h ) | q α 1 0 t i h | H ( t i , s ) H ( t i h , s ) | p f 1 ( s ) d s + q β 1 0 t i h | H ( t i , s ) H ( t i h , s ) | p ¯ f 1 ( s ) d s + q α 1 t i h t i | H ( t i , s ) | p f 1 ( s ) d s + q β 1 t i h t i | H ( t i , s ) | p ¯ f 1 ( s ) d s + k = 1 i 1 | H ( t i , t k ) H ( t i h , t k ) | ( d k 1 q α 1 + d k 2 q β 1 ) + k = 1 i 1 | L ( t i , t k ) L ( t i h , t k ) | ( d ¯ k 1 q α 1 + d ¯ k 2 q β 1 ) .
The RHS tends to 0, as h goes to 0.
Next, we prove equi-continuity at t = t i + . We fix ν 2 > 0 , so that
{ t k : k i } [ t i ν 2 , t i + ν 2 ] = .
For 0 < h < ν 2 , we obtain
| N 1 ( u , v ) ( t i + h ) N 1 ( u , v ) ( t i ) | q α 1 0 t i | H ( t i + h , s ) H ( t i , s ) | p f 1 ( s ) d s + q β 1 0 t i | H ( t i + h , s ) H ( t i , s ) | p ¯ f 1 ( s ) d s + q α 1 t i t i + h | H ( t i + h , s ) | p f 1 ( s ) d s + q β 1 t i t i + h | H ( t i + h , s ) | p ¯ f 1 ( s ) d s + 0 < t k t i | H ( t i + h , t k ) G ( t i , t k ) | ( d k 1 q α 1 + d k 2 q β 1 ) + t i < t t i + h | H ( t i + h , t k ) | ( d k 1 q α 1 + d k 2 q β 1 ) + 0 < t k t i | L ( t i + h , t k ) L ( t i , t k ) | ( d ¯ k 1 q α 1 + d ¯ k 2 q β 1 ) + t i < t t i + h | L ( t i + h , t k ) | d ¯ k ( d ¯ k 1 q α 1 + d ¯ k 2 q β 1 ) .
The RHS tends to 0, as h goes to 0.
As a consequence of Steps 1 to 3 and the Arzela–Ascoli Theorem, we can conclude that N : PC × PC PC × PC is a completely continuous operator.
Step 4: 
Now, it remains to show that the set
E = ( u , v ) PC × PC : u = μ N 1 ( u , v ) , v = μ N 2 ( u , v ) , for some 0 < μ < 1
is bounded. Let u , v E ; then, u = μ N 1 ( u , v ) and v = μ N 2 ( u , v ) , for 0 < μ < 1 . Thus, for t J , we obtain
| u ( t ) | 0 2 π sup ( t , s ) J 2 | H ( t , s ) | p f 1 ( s ) | u ( s ) | α 1 + p ¯ f 1 ( s ) | v ( s ) | β 1 d s + k = 1 m sup t J | H ( t , t k ) | d k 1 | u ( t k ) | α 1 + d k 2 | v ( t k ) | β 1 + k = 1 m sup t J | L ( t , t k ) | d ¯ k 1 | u ( t k ) | α 1 + d ¯ k 2 | v ( t k ) | β 1 .
This implies by ( H 3 ) ( H 5 ) that for each t J and v Γ ( N ) , we have
u PC sup ( t , s ) J 2 | H ( t , s ) | p f 1 L 1 u PC γ + p ¯ f 1 L 1 v PC γ + k = 1 m sup t J | G ( t , t k ) | d k 1 u PC γ + d k 2 v PC γ + k = 1 m sup t J | L ( t , t k ) | d ¯ k 1 u PC γ + d ¯ k 2 v PC γ .
Similarly, we have
v PC sup ( t , s ) J 2 | H ( t , s ) | p f 2 L 1 u PC γ + p ¯ f 2 L 1 v PC γ + k = 1 m sup t J | H ( t , t k ) | d k 2 u PC γ + d k 3 v PC γ + k = 1 m sup t J | L ( t , t k ) | d ¯ k 2 u PC γ + d ¯ k 3 v PC γ .
Thus,
u PC + v PC H * ( p f 1 L 1 + p f 2 L 1 ) + G * ( d k 1 + d k 2 ) + L * ( d ¯ k 1 + d ¯ k 2 ) u PC γ + H * ( p ¯ f 1 L 1 + p ¯ f 2 L 1 ) + G * ( d k 2 + d k 3 ) + L * ( d ¯ k 2 + d ¯ k 3 ) v PC γ K * u PC γ + v PC γ K * u PC + v PC γ ,
where
γ = max { α i , β i } ,
and
K 1 = H * ( p f 1 L 1 + p f 2 L 1 ) + G * ( d k 1 + d k 2 ) + L * ( d ¯ k 1 + d ¯ k 2 ) ,
and
K 2 = H * ( p ¯ f 1 L 1 + p ¯ f 2 L 1 ) + G * ( d k 2 + d k 3 ) + L * ( d ¯ k 2 + d ¯ k 3 ) ,
and
K * = max { K 1 , K 2 } .
If
u PC + v PC > 1 ,
we obtain
u PC + v PC K * 1 1 γ = ψ * .
Consequently,
u PC max { 1 , ψ * } = d ¯ * and v PC max { 1 , ψ * } = d ¯ * .
This proves that E is bounded. By Theorem 2, we deduce that N has a fixed point ( u , v ) , which is a solution to (1).
Step 5: 
Now, we show that the set
S = { ( u , v ) PC × PC : ( u , v ) is solution of ( 1 ) } ,
and it is compact. Let ( u n , v n ) n N be a sequence in S; we put B = ( u n , v n ) : n N PC × PC . Then, from earlier parts of the proof of this Theorem, we conclude that B is bounded and equicontinuous. Then, from the Ascoli–Arzela Theorem, we can conclude that B is compact. Hence, ( u n , v n ) n N has a subsequence ( u n , v n ) n m N S , such that ( u n m , v n m ) converges to ( u , v ) . Let
u 0 ( t ) = 0 2 π H ( t , s ) f 1 ( t , u ( s ) , v ( s ) , θ ) d s k = 1 m H ( t , t k ) I k 1 ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k 1 ( u ( t k ) , v ( t k ) ) , t J ,
and
v 0 ( t ) = 0 2 π H ( t , s ) f 2 ( t , u ( s ) , v ( s ) , θ ) d s k = 1 m H ( t , t k ) I k 2 ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k 2 ( u ( t k ) , v ( t k ) ) , t J ,
and
| u n m t u 0 ( t ) | 0 2 π | H ( t , s ) | | f 1 ( t , u n m ( s ) , v n m ( s ) , θ ) f 1 ( t , u ( s ) , v ( s ) , θ ) | d s + k = 1 m | H ( t , t k ) | | I k 1 ( u n m ( s ) , v n m ( t k ) ) I k ( u ( t k ) , v ( t k ) ) | + k = 1 m | L ( t , t k ) | | I ¯ k 1 ( u n m ( s ) , v n m ( t k ) ) I ¯ k ( u ( t k ) , v ( t k ) ) | .
As n m , u n m u 0 , and then
u ( t ) = 0 2 π H ( t , s ) f 1 ( t , u ( s ) , v ( s ) , θ ) d s k = 1 m H ( t , t k ) I k 1 ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k 1 ( u ( t k ) , v ( t k ) ) , t J ,
and
v ( t ) = 0 2 π H ( t , s ) f 2 ( t , u ( s ) , v ( s ) , θ ) d s k = 1 m H ( t , t k ) I k 2 ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k 2 ( u ( t k ) , v ( t k ) ) , t J .
Thus, S is compact. This completes the proof. □

4. Positive Solutions

For k 1 , m N , we assume
u λ 2 u = θ g 1 ( t ) h 1 ( u , v ) = f 1 ( t , u , v , θ ) , t J = [ 0 , 2 π ] , t t k , v λ 2 v = θ g 2 ( t ) h 2 ( u , v ) = f 2 ( t , u , v , θ ) , t J = [ 0 , 2 π ] , t t k , u ( t k + ) u ( t k ) = I k 1 ( u ( t k ) , v ( t k ) ) , k 1 , m N , v ( t k + ) v ( t k ) = I k 2 ( u ( t k ) , v ( t k ) ) , k 1 , m N , u ( t k + ) u ( t k ) = I ¯ k 1 ( u ( t k ) , v ( t k ) ) , k 1 , m N , v ( t k + ) v ( t k ) = I ¯ k 2 ( u ( t k ) , v ( t k ) ) , k 1 , m N , u ( t = 0 ) = u ( t = 2 π ) , u ( t = 0 ) = u ( t = 2 π ) , v ( t = 0 ) = v ( t = 2 π ) , v ( t = 0 ) = v ( t = 2 π ) ,
where g i i = 1 , 2 : J R , h i i = 1 , 2 : R × R R are given functions. Our goal of this part is the existence of positive solutions of (2).
Lemma 2.
Assume that all the conditions of Theorem 4 are satisfied and
(H6)
For each u , v R and k 1 , m N , I k 1 ( u , v ) 0 ,
(H7)
For each u , v R , i = 1 , 2 , and t J ,
g i ( t ) h i ( u , v ) 0 .
(H8)
For each u , v R , t J , and k 1 , m N ,
L ( t , t k ) I ¯ k 1 ( u , v ) 0
Then, problem (2) has a unique positive solution on J .
Proof. 
Consider the operator
N : PC × PC PC × PC ( u , v ) N 1 ( t , u , v ) , N 2 ( t , u , v )
N 1 ( t , u , v ) = θ 0 2 π H ( t , s ) g 1 ( s ) h 1 ( u ( s ) , v ( s ) ) d s k = 1 m H ( t , t k ) I k 1 ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k 1 ( u ( t k , v ( t k ) ) , t J ,
and
N 2 ( t , u , v ) = θ 0 2 π H ( t , s ) g 1 ( s ) h 2 ( u ( s ) , v ( s ) ) d s k = 1 m H ( t , t k ) I k 2 ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k 2 ( u ( t k , v ( t k ) ) , t J .
We prove that the fixed points of N are positive solutions to (2). Indeed, assume that ( u , v ) PC × PC is a fixed point of N. It is clear that
u ( t ) = θ 0 2 π H ( t , s ) g 1 ( s ) h 1 ( u ( s ) , v ( s ) ) d s k = 1 m H ( t , t k ) I k 1 ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k 1 ( u ( t k , v ( t k ) ) , t J ,
and
v ( t ) = θ 0 2 π H ( t , s ) g 2 ( s ) h 2 ( u ( s ) , v ( s ) ) d s k = 1 m H ( t , t k ) I k 2 ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k 2 ( u ( t k , v ( t k ) ) , t J ,
which imply that ( u , v ) is a solution of (2).
If ( u , v ) is a fixed point of N, then ( H 6 ) through ( H 8 ) imply that ( u ( t ) , v ( t ) ) ( 0 , 0 ) , for each t J .
As in Theorem 3, we can show that N is a contraction; so, by Perov’s, we conclude that N has a unique fixed point ( u , v ) , which is a positive solution of problem (2). This completes the proof. □
Let X be a real generalized Banach space. A nonempty closed convex set K E is a cone, if it satisfies the following two conditions
( i )
If v K and λ 0 , then λ v K ,
( i i )
If v , v K , then v = 0 .
K is a solid cone, if I n t K , where I n t K is the interior of K .
Remark 2.
Any cone K X induces a partial ordering < on E given by
u < v v u K .
Theorem 6
([21]). Let X be a real generalized Banach space, K X a cone of X, and R > 0 . Let K R = u K : | | u | | < R , and let N : K R C be a completely continuous operator, where r ( 0 , R ) . If
(i)
| | N ( u ) | | < | | u | | , u K r ,
(ii)
| | N ( u ) | | > | | u | | , u K R ,
then N has at least two fixed points u , v , K R , such that
| | u | | < r , r < | | v | | R .
Let K 1 , K 2 be a solid cone of a real Banach space X and
N : I n t K 1 × I n t K 2 I n t K 1
be an operator; it is said that N is called an α -concave operator, if
N ( t u , t v ) t α N ( u , v ) , for any ( u , v ) i n K and 0 < t < 1 , α 0 , 1 .
Let K i i = 1 , 2 be a solid cone of a real Banach space X and
N : I n t K 1 × I n t K 2 I n t K 1 × I n t K 2
be an operator; it is said that N is called an α -concave operator, if N i i = 1 , 2 is called an α -concave operator, with N = N 1 , N 2 .
Lemma 3
([22]). Let K be a normal solid cone of a real Banach space X, and
N : I n t K × I n t K I n t K × I n t K
be α-concave increasing operator. Then, N has only one fixed point in I n t K × I n t K .
By Lemma 3, we deduce the following Corollary
Corollary 1.
Let K 1 , K 2 are a solid cone of a real Banach space X and
N : I n t K 1 × I n t K 2 I n t K 1 × I n t K 2 ,
is α-concave increasing operator. Then N has only one fixed point in I n t K 1 × I n t K 2 .
Theorem 7.
Assume ( H 6 ) ( H 8 ) and the following conditions are satisfied:
f i i = 1 , 2 : R + × R + R ,
is nondecreasing function and I k i , I ¯ k i : R + × R + R are decreasing functions, with
0 2 π H ( t , s ) g i ( s ) h i ( u ( s ) , v ( s ) ) d s > 0 , H ( t , t k ) I k i ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k i ( u ( t k ) , v ( t k ) ) < 0 , f i ( η u , η v ) η α f i ( u , v ) , I k i ( η u , η v ) η α I k i ( u , v ) , I ¯ k ( η u , η v ) η α I ¯ k i ( u , v ) ,
u , v > 0 , t J , i = 1 , 2 , 0 < η < 1 , where 0 α < 1 , i = 1 , 2 .
Then, problem (2) has a unique positive solution ( u θ ( t ) , v θ ( t ) ) .
Proof. 
We pose
K 1 = { u PC : u ( t ) 0 for t J } and K 2 = { v PC : v ( t ) 0 , for t J } .
Then, K 1 , K 2 are cones in PC , by ( H 6 ) through ( H 8 ) , which imply that, N i ( K 1 × K 2 ) K i , for i = 1 , 2 . We assert that
N : I n t K 1 × I n t K 2 I n t K 1 × I n t K 2
is an α -concave increasing operator. Indeed,
N i ( η u , η v ) = θ 0 2 π H ( t , s ) g i ( s ) h i ( η u ( s ) , η v ( s ) ) d s k = 1 m H ( t , t k ) I k i ( η u ( t k ) , η v ( t k ) ) + L ( t , t k ) I ¯ k i ( η u ( t k ) , η v ( t k ) ) η α θ 0 2 π H ( t , s ) g i ( s ) h i ( u ( s ) , v ( s ) ) d s η α k = 1 m H ( t , t k ) I k i ( u ( t k ) , v ( t k ) ) + L ( t , t k ) I ¯ k i ( u ( t k ) , v ( t k ) ) η α N i ( u , v ) , for any 0 < η < 1 ,
where 0 α < 1 . Since f i ( u , v ) is nondecreasing and I k i , I ¯ k i are decreasing, then
N i ( u 1 , v 1 ) ( t ) = θ 0 2 π H ( t , s ) g i ( s ) h i ( u 1 ( s ) , v 1 ( s ) ) d s k = 1 m H ( t , t k ) I k i ( u 1 ( t k ) , v 1 ( t k ) ) + L ( t , t k ) I ¯ k i ( u 1 ( t k ) , v 1 ( t k ) ) θ 0 2 π H ( t , s ) g i ( s ) h i ( u 2 ( s ) , v 2 ( s ) ) d s k = 1 m H ( t , t k ) I k i ( u 2 ( t k ) , v 2 ( t k ) ) + L ( t , t k ) I ¯ k i ( u 2 ( t k ) , v 2 ( t k ) ) = N i ( u 2 , v 2 ) ( t ) , for ( u 1 , v 1 ) ( u 2 , v 2 ) , ( u 1 , v 1 ) , ( u 2 , v 2 ) C × C .
By Corollary 1, N has a unique fixed point ( u θ , v θ ) I n t K 1 × I n t K 2 . This completes the proof of the Theorem. □
Now, we seek a solution to problem (2) via the Krasnosel’skii twin fixed point Theorem.
Theorem 8.
Assume ( H 3 ) ( H 8 ) and the following conditions are satisfied:
( H 9 )
There exist R 1 , R 2 > 0 and r 1 , r 2 > 0 , with r 1 < R 1 and r 2 < R 2 , such that
θ sup ( t , s ) J 2 | H ( t , s ) | g 1 h 1 * ( r 1 , r 2 ) + k = 1 m sup t J | H ( t , t k ) | ( d k 1 r 1 α 1 + d k 2 r 2 β 1 ) + k = 1 m sup t J | L ( t , t k ) | ( d ¯ k 1 r 1 α 1 + d ¯ k 2 r 2 β 1 ) < r 1 θ sup ( t , s ) J 2 | H ( t , s ) | g 2 h 2 * ( r 1 , r 2 ) + k = 1 m sup t J | H ( t , t k ) | ( d k 2 r 1 α 2 + d k 3 r 2 β 2 ) + k = 1 m sup t J | L ( t , t k ) | ( d ¯ k 2 r 1 α 2 + d ¯ k 3 r 2 β 2 ) < r 2 ,
where
h i * ( r 1 , r 2 ) = sup ( u , v ) ( 0 , r 1 ] × ( 0 , r 2 ] | h i ( u , v ) | , i = 1 , 2 ,
min t [ 0 , 2 π ] θ 0 2 π H ( t , s ) g 1 ( s ) h 1 ( μ 1 ( s ) , μ 2 ( s ) ) d s k = 1 m H ( t , t k ) I k 1 ( μ 1 ( t k ) , μ 2 ( t k ) ) + L ( t , t k ) I ¯ k 1 ( μ 1 ( t k ) , μ 2 ( t k ) ) > R 1 , if ( r 1 , r 2 ) < ( μ 1 , μ 2 ) min t [ 0 , 2 π ] θ 0 2 π H ( t , s ) g 2 ( s ) h 2 ( μ 1 ( s ) , μ 2 ( s ) ) d s k = 1 m H ( t , t k ) I k 2 ( μ 1 ( t k ) , μ 2 ( t k ) ) + L ( t , t k ) I ¯ k 2 ( μ 1 ( t k ) , μ 2 ( t k ) ) > R 2 , if ( r 1 , r 2 ) < ( μ 1 , μ 2 ) .
Then, problem (2) has at least two positive solutions ( u 1 , v 1 ) , ( u 2 , v 2 ) , such that
u 1 < r 1 , v 1 < r 2 a n d r 1 < u 2 R 1 , r 2 < v 2 R 2 .
Proof. 
Let K 1 , K 2 be a cone defined in (3). Then, ( H 6 ) through ( H 8 ) imply that N ( K 1 , K 2 ) K 1 , K 2 . For any R 1 , R 2 > 0 ,
K R 1 = u K 1 : u < R 1 ,
and
K R 2 = v K : v < R 2 .
Using ( H 4 ) ( H 7 ) , we can show that N C 1 ( K R 1 × K R 2 , K 1 × K 2 is a completely continuous operator.
We should deal with the hypotheses of the Krasnosel’skii twin fixed point Theorem 6.
Claim 1:  ( N 1 ( u , v ) PC , N 2 ( u , v ) PC ) < ( u PC , v PC ) , ( u , v ) K r 1 × K r 2 , where
K r 1 = { u K : u < r 1 } and K r 2 = { v K : v < r 2 } .
For ( u , v ) K r 1 × K r 2 , from ( H 6 ) , ( H 7 ) and ( H 9 ) , we have
| N 1 ( u , v ) ( t ) | θ 0 2 π | H ( t , s ) | | g 1 ( s ) h 1 ( u ( s ) , v ( s ) ) | d s + k = 1 m | H ( t , t k ) | | I k 1 ( u ( t k ) , v ( t k ) ) | + k = 1 m | L ( t , t k ) | | I ¯ k 1 ( u ( t k ) , v ( t k ) ) | θ sup ( t , s ) J 2 | H ( t , s ) | g 1 h 1 * ( r 1 , r 2 ) + k = 1 m sup t J | H ( t , t k ) | ( d k 1 r 1 α 1 + d k 2 r 2 β 1 ) + k = 1 m sup t J | L ( t , t k ) | ( d ¯ k 1 r 1 α 1 + d ¯ k 2 r 2 β 1 ) < r 1 = u PC .
Similarly, we have
| N 2 ( u , v ) ( t ) | θ sup ( t , s ) J 2 | H ( t , s ) | g 2 h 2 * ( r 1 , r 2 ) + k = 1 m sup t J | H ( t , t k ) | ( d k 2 r 1 α 2 + d k 3 r 2 β 2 ) + k = 1 m sup t J | L ( t , t k ) | ( d ¯ k 2 r 1 α 2 + d ¯ k 3 r 2 β 2 ) < r 2 = v PC .
Thus,
N 1 ( u , v ) PC < u PC and N 2 ( u , v ) PC < v PC , for each ( u , v ) K r 1 × C r 2 .
Claim 2:  ( N 1 ( u , v ) PC , N 2 ( u , v ) PC ) > ( u PC , v PC ) , ( u , v ) ( C R 1 , C R 2 ) , for ( u , v ) K R 1 × K R 2 , and we have u PC = R 1 , v PC = R 2 ; then, r 1 < u PC = R 1 , r 2 < v PC = R 2 , and from ( H 9 ) , we have
N 1 ( u , v ) ( t ) min t [ 0 , 2 π ] θ 0 2 π H ( t , s ) g 1 ( s ) h 1 ( μ 1 ( s ) , μ 2 ( s ) ) d s k = 1 m H ( t , t k ) I k 1 ( μ 1 ( t k ) , μ 2 ( t k ) ) + L ( t , t k ) I ¯ k 1 ( μ 1 ( t k ) , μ 2 ( t k ) ) > R 1 = u PC .
Similarly, we have
N 2 ( u , v ) ( t ) min t [ 0 , 2 π ] θ 0 2 π H ( t , s ) g 2 ( s ) h 2 ( μ 1 ( s ) , μ 2 ( s ) ) d s k = 1 m H ( t , t k ) I k 2 ( μ 1 ( t k ) , μ 2 ( t k ) ) + L ( t , t k ) I ¯ k 2 ( μ 1 ( t k ) , μ 2 ( t k ) ) > R 2 = v PC .
Thus,
N 1 ( u , v ) PC > u PC and N 2 ( u , v ) PC > v PC , for each ( u , v ) K R 1 × K R 2 .
Then, problem (2) has at least two positive solutions ( u 1 , v 1 ) , ( u 2 , v 2 ) K R 1 × K R 2 , such that
u 1 < r 1 , v 1 < r 2 r 1 < u 2 R 1 , r 2 < v 2 R 2 .
This completes the proof. □

5. Conclusions and Discussion of the Results

Sufficient conditions for the existence of solutions to systems of nonlinear second-order differential equations with periodic impulse action are constructed. The proposed Schaefer’s fixed point theorem is quite effective in studying in such cases for systems of nonlinear differential equations. Necessary and sufficient conditions for the existence of positive solutions are also established.

Practical Significance

Transient processes in electrical circuits are modeled using degenerate differential equations or differential algebraic equations. Taking into account pulsed effects on currents and voltages in an electrical circuit at fixed times significantly complicates the study of transient regimes. The obtained theoretical results make it possible to indicate the necessary and sufficient conditions for the existence of the stated problem (1), which can model electrical circuits with pulsed effects. The development of the mathematical theory of this type of system is associated with practical problems in the theory of control for complex systems and the widespread introduction of digital technologies, see [23,24,25].
Extending these results to consider the question of stability (Qualitative studies) will make it possible to advance the study in this direction.

Author Contributions

Writing—original draft preparation, A.B.C. and M.F.; writing—review and editing, A.M., K.Z. and M.B.; Supervision, K.Z. All authors have read and agreed to the published version of the manuscript.

Funding

This research was funded by King Khalid University through large research project under grant number R.G.P.2/252/44.

Data Availability Statement

No new data were created or analyzed in this study. Data sharing is not applicable to this article.

Acknowledgments

The authors extend their appreciation to the Deanship of Scientific Research at King Khalid University for funding this work.

Conflicts of Interest

The authors declare that they have no conflict of interest.

References

  1. Hsu, C.S. Impulsive parametric excitation. J. Appl. Mech. 1972, 39, 551–558. [Google Scholar] [CrossRef]
  2. Slynko, V.I. Stability of Motion of Mechanical Systems: Hybrid Models. Ph.D. Thesis, University of Wuerzburg, Wuerzburg, Germany, 2009. [Google Scholar]
  3. Samoilenko, A.M.; Perestyuk, N.A. Differential Equations with Impulse Action; Vishcha School: Kyiv, Ukraine, 1987. [Google Scholar]
  4. Lakshmikantham, V.; Bainov, D.D.; Simeonov, P.S. Theory of Impulsive Differential Equations; World Science: Singapore, 1989. [Google Scholar]
  5. Ignatiev, A.O. On asymptotic stability and instability with respect to a part of variable solutions of systems with impulse action. Sibirsk. Mat. Mag. 2008, 49, 125–133. [Google Scholar]
  6. Gladilina, R.I.; Ignatiev, A.O. On necessary and sufficient conditions for the stability of invariant sets of nonlinear impulse systems. Prikl. Mech. 2008, 44, 132–142. [Google Scholar]
  7. Martynyuk, A.A.; Slynko, V.I. On the stability of motion of a nonlinear impulse system. Prikl. Mech. 2004, 40, 112–122. [Google Scholar]
  8. Chernikova, O.S. Reduction principle for systems of differential equations with impulse action. Ukr. Mat. Mag. 1982, 34, 601–607. [Google Scholar]
  9. Wang, J.; Zhang, Y. Solvability of fractional order differential systems with general nonlocal conditions. J. Appl. Math. Comput. 2014, 45, 199–222. [Google Scholar] [CrossRef]
  10. Nica, O.; Precup, R. On the nonlocal initial value problem for first order differential systems. Stud. Univ. Babes -Bolyai Math. 2011, 56, 125–137. [Google Scholar]
  11. Bolojan-Nica, O.; Infante, G.; Precup, R. Existence results for systems with coupled nonlocal initial conditions. Nonli. Anal. 2014, 4, 231–242. [Google Scholar] [CrossRef]
  12. Nica, O. Initial-value problems for first-order differential systems with general nonlocal conditions. Electron. J. Diff. Equ. 2012, 2012, 1–15. [Google Scholar]
  13. Bolojan, O.; Precup, R. Implicit first order differential systems with nonlocal conditions. Electron. J. Qual. Theory Differ. Equ. 2014, 69, 1–13. [Google Scholar] [CrossRef]
  14. Graef, J.R.; Kadari, H.; Ouahab, A.; Oumansour, A. Existence results for systems of second-order impulsive differential equations. Acta Math. Univ. Comen. 2019, 88, 51–66. [Google Scholar]
  15. Graef, J.; Henderson, J.; Ouahab, A. Topological Methods for Differential Equations and Inclusions; CRC Press: Boca Raton, FL, USA, 2019. [Google Scholar]
  16. Svetlin, G.G.; Zennir, K. Existence of solutions for a class of nonlinear impulsive wave equations. Ric. Mat. 2022, 71, 211–225. [Google Scholar]
  17. Svetlin, G.G.; Zennir, K.; Bouhali, K.; Alharbi, R.; Altayeb, Y.; Biomy, M. Existence of solutions for impulsive wave equations. AIMS Math. 2023, 8, 8731–8755. [Google Scholar]
  18. Svetlin, G.G.; Zennir, K. Boundary Value Problems on Time Scales; Chapman and Hall/CRC Press: New York, NY, USA, 2021; Volume I, p. 692. [Google Scholar]
  19. Perov, A.I. On the Cauchy problem for a system of ordinary differential equations. Pribliz. Met. Reshen. Diff. Uravn. 1964, 2, 115–134. [Google Scholar]
  20. Precup, R. Methods in Nonlinear Integral Equations; Kluwer: Dordrecht, The Netherlands, 2002. [Google Scholar]
  21. Heikkil, S.; Lakshmikantham, V. Monotone iterative techniques for discontinuous nonlinear differential equations. In Monographs and Textbooks in Pure and Applied Mathematics; Marcel Dekker: New York, NY, USA, 1994; Volume 181. [Google Scholar]
  22. Guo, D.J. The fixed point and eigenvalue of a class of concave and convex operator. Chin. Sci. Bull. 1985, 15, 1132–1135. [Google Scholar]
  23. Clark, W.; Bloch, A. The bouncing penny and nonholonomic impacts. In Proceedings of the 2019 IEEE 58th Conference on Decision and Control (CDC), Nice, France, 11–13 December 2019; pp. 2114–2119. [Google Scholar]
  24. Goodman, J.R.; Colombo, L.J. On the Existence and Uniqueness of Poincaré Maps for Systems with Impulse Effects. IEEE Trans. Automat. Control. 2019, 65, 1815–1821. [Google Scholar] [CrossRef]
  25. Ibort, A.; de Leon, M.; Lacomba, E.A.; Martin de Diego, D.; Pi-tanga, P. Mechanical systems subjected to impulsive constraints. J. Phys. A Math. Gen. 1997, 30, 5835–5854. [Google Scholar] [CrossRef]
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Moumen, A.; Benaissa Cherif, A.; Ferhat, M.; Bouye, M.; Zennir, K. Existence Results for Systems of Nonlinear Second-Order and Impulsive Differential Equations with Periodic Boundary. Mathematics 2023, 11, 4907. https://doi.org/10.3390/math11244907

AMA Style

Moumen A, Benaissa Cherif A, Ferhat M, Bouye M, Zennir K. Existence Results for Systems of Nonlinear Second-Order and Impulsive Differential Equations with Periodic Boundary. Mathematics. 2023; 11(24):4907. https://doi.org/10.3390/math11244907

Chicago/Turabian Style

Moumen, Abdelkader, Amin Benaissa Cherif, Mohamed Ferhat, Mohamed Bouye, and Khaled Zennir. 2023. "Existence Results for Systems of Nonlinear Second-Order and Impulsive Differential Equations with Periodic Boundary" Mathematics 11, no. 24: 4907. https://doi.org/10.3390/math11244907

APA Style

Moumen, A., Benaissa Cherif, A., Ferhat, M., Bouye, M., & Zennir, K. (2023). Existence Results for Systems of Nonlinear Second-Order and Impulsive Differential Equations with Periodic Boundary. Mathematics, 11(24), 4907. https://doi.org/10.3390/math11244907

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