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Article

On a Nonlocal Boundary Value Problem of a State-Dependent Differential Equation

Faculty of Science, Alexandria University, Alexandria 21500, Egypt
*
Author to whom correspondence should be addressed.
These authors contributed equally to this work.
Mathematics 2021, 9(21), 2800; https://doi.org/10.3390/math9212800
Submission received: 17 October 2021 / Revised: 2 November 2021 / Accepted: 3 November 2021 / Published: 4 November 2021
(This article belongs to the Section Difference and Differential Equations)

Abstract

:
In this paper, the existence of absolutely continuous solutions and some properties will be studied for a nonlocal boundary value problem of a state-dependent differential equation. The infinite-point boundary condition and the Riemann–Stieltjes integral condition will also be considered. Some examples will be provided to illustrate our results.

1. Introduction

The delay differential equations serve as an important branch of nonlinear analysis that has many applications in most fields. Usually, the deviation of the arguments depends only on the time (see [1,2,3,4,5,6]); however, when the deviation of the arguments depends upon the state variable x and also the time t is incredibly important theoretically and practically, this type of equations is known as self-reference or state-dependent equations. Equations with state-dependent delays have gained great attention to specialists since they have many application models, like the two-body problem of classical electrodynamics, even have numerous applications within the class of problems that have past memories, as an example, in hereditary phenomena, see [7,8]. Several papers studied this kind of equations, (see [9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24] ).
Eder [12], where the author studied the problem
x ( t ) = x x ( t ) , t [ a , b ] and x ( t 0 ) = x o .
The existence and the uniqueness of the solution of the problem
x ( t ) = f ( t , x ( x ( t ) ) ) , t [ a , b ] x ( 0 ) = x o
were studied by Buicá [11].
In [16], the assumptions of [11], have been relaxed and generalized to the equation
x ( t ) = g ( t , 0 t f s , x ( x ( s ) ) d s ) , t [ 0 , T ] ,
where f satisfies Carathéodory condition.
In [14,15], some other results have been obtained for the problem
d x ( t ) d t = h 1 ( t , x ( h 2 ( t , x ( t ) ) ) ) , a . e . t ( 0 , T ] , x ( 0 ) = x o .
EL-Sayed and Ebead [17] studied the IVP of state-dependent hybrid functional differential equation
d d t x ( t ) a ( t ) h 1 ( t , x ( x ( φ ( t ) ) ) = h 2 ( t , x ( x ( φ ( t ) ) ) , t [ 0 , T ]
with the initial data
x ( 0 ) = a ( 0 ) .
Our aim in this work is to study the m-point boundary value problem (BVP)
d x ( t ) d t = f t , x ( x ( ϕ ( t ) ) ) a . e . t ( 0 , T ]
k = 1 m a k x ( t k ) = x o , τ k [ 0 , T ] , a k > 0 .
The existence and the uniqueness have been proved for the BVP (1) and (2). Moreover, we show that the solution of our problem depends continuously on x 0 and on the nonlocal data a k . Furthermore, we study (1) with the nonlocal integral condition
0 T x ( s ) d h ( s ) = x o ,
where h : [ 0 , T ] [ 0 , T ] is an increasing function. Finally, we study (1) with the infinite point boundary condition
k = 1 a k x ( τ k ) = x o ,
where k = 1 a k is convergent.

2. Main Results

Consider the BVP (1) and (2) under the following hypothesis:
( i )  
f: [ 0 , T ] × [ 0 , T ] R + satisfies Carathéodory condition.
( i i )  
There exist m : [ 0 , T ] R + bounded measurable function and a constant b > 0 such that
f ( t , x ) m ( t ) + b x ,
where, m ( t ) M .
( i i i )  
L T A x o T ( 1 2 L ) and L = ( M + b T ) [ 0 , 1 3 ) , where A = 1 / k = 1 m a k and M is a positive constant such that | m ( t ) | M .
( i v )  
ϕ : [ 0 , T ] [ 0 , T ] is continuous and ϕ ( t ) t .

2.1. Integral Representation

Lemma 1.
The BVP (1) and (2) and the integral equation
x ( t ) = A [ x o k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s ] + 0 t f s , x ( x ( ϕ ( s ) ) ) d s , t [ 0 , T ]
are equivalent.
Proof. 
Integrating (1), we obtain
x ( t ) = x ( 0 ) + 0 t f s , x ( x ( ϕ ( s ) ) ) d s
and
k = 1 m a k x ( τ k ) = x ( 0 ) k = 1 m a k + k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s ,
then we can get
x ( 0 ) = A x o k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s
and
x ( t ) = A x o k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s + 0 t f s , x ( x ( ϕ ( s ) ) ) d s .
Conversely, differentiating (5), we obtain
d x ( t ) d t = d d t 0 t f s , x ( x ( ϕ ( s ) ) ) d s = f t , x ( x ( ϕ ( t ) ) ) d s a . e . t [ 0 , T ] .
Furthermore, from (5), we can show that
k = 1 m a k x ( τ k ) = x o .
Hence, the BVP (1) and (2) and the integral Equation (5) are equivalent. □

2.2. Existence of Solution

Define the set S L by
S L = x C [ 0 , T ] : | x ( t 2 ) x ( t 1 ) | L | t 2 t 1 |
Theorem 1.
Let the hypothesis (i)–(iv) be held, then (1) and (2) has a solution x S L C [ 0 , T ] .
Proof. 
Define the operator F by
F x ( t ) = A x o k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s + 0 t f s , x ( x ( ϕ ( s ) ) ) d s , t [ 0 , T ] .
Let x S L , then we have
| F x ( t ) | = | A x o k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s + 0 t f s , x ( x ( ϕ ( s ) ) ) d s | A x o + A k = 1 m a k 0 τ k | f s , x ( x ( ϕ ( s ) ) ) | d s + 0 t | f s , x ( x ( ϕ ( s ) ) ) | d s A x o + A k = 1 m a k 0 τ k { m ( s ) + b | x ( x ( ϕ ( s ) ) ) | } d s + 0 t { m ( s ) + b | x ( x ( ϕ ( s ) ) ) | } d s A x o + A k = 1 m a k ( M + b T ) 0 τ k d s + ( M + b T ) 0 t d s A x o + 2 L T T .
Hence, { F x } is uniformly bounded.
Let x S L and t 1 , t 2 [ 0 , T ] with t 1 < t 2 such that | t 2 t 1 | < δ , then
| F x ( t 2 ) F x ( t 1 ) | = | 0 t 2 f s , x ( x ( ϕ ( s ) ) ) d s 0 t 1 f s , x ( x ( ϕ ( s ) ) ) d s | = | t 1 t 2 f s , x ( x ( ϕ ( s ) ) ) d s | t 1 t 2 | f s , x ( x ( ϕ ( s ) ) ) | d s t 1 t 2 { m ( s ) + b | x ( x ( ϕ ( s ) ) ) | } d s ( M + b T ) | t 2 t 1 | = L | t 2 t 1 | .
This proves that F : S L S L and { F x } are equi-continuous.
By Arzela–Ascoli Theorem ([25] p. 54), we find that F is compact.
Let { x n } S L such that x n x a s n on [ 0 , T ] (i.e., | x n ( t ) x ( t ) | ϵ 1 ). This implies that | x n ( x ( ϕ ( t ) ) ) x ( x ( ϕ ( t ) ) ) | ϵ 2 for arbitrary ϵ 1 , ϵ 2 0 , then
| x n ( x n ( ϕ ( t ) ) ) x ( x ( ϕ ( t ) ) ) | | x n ( x n ( ϕ ( t ) ) ) x n ( x ( ϕ ( t ) ) ) | + | x n ( x ( ϕ ( t ) ) ) x ( x ( ϕ ( t ) ) ) | L | x n ( ϕ ( t ) ) x ( ϕ ( t ) ) | + | x n ( x ( ϕ ( t ) ) ) x ( x ( ϕ ( t ) ) ) | L ϵ 1 + ϵ 2 = ϵ
and
x n ( x n ( ϕ ( t ) ) ) ) ( x ( x ( ϕ ( t ) ) ) ) i n S L a s n .
Now the function f is continuous in the second argument, then
f t , x n ( x n ( ϕ ( t ) ) ) f t , x ( x ( ϕ ( t ) ) ) .
Using assumption ( i i ) and Lebesgues dominated convergence theorem ([26] p. 151), we get
lim n 0 t f s , x n ( x n ( ϕ ( s ) ) ) d s = 0 t f s , x ( x ( ϕ ( s ) ) ) d s .
Similarly,
lim n 0 τ k f s , x n ( x n ( ϕ ( s ) ) ) d s = 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s .
Now we have
lim n F x n ( t ) = A x o k = 1 m a k 0 τ k f s , x n ( x n ( ϕ ( s ) ) ) d s + 0 t f s , x n ( x n ( ϕ ( s ) ) ) d s = A x o k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s + 0 t f s , x ( x ( ϕ ( s ) ) ) d s = F x ( t ) .
This proves that F is continuous.
Applying Schauder Theorem [27], there is a solution x C [ 0 , T ] of (5). This means that the BVP (1) and (2) has at least one solution x A C [ 0 , T ] . □

2.3. Riemann-Stieltjes Integral

Let x A C [ 0 , T ] be a solution of BVP (1) and (2), then we can formulate the next theorem.
Theorem 2.
Let the hypothesis (i)–(iv) hold. Let h : [ 0 , T ] [ 0 , T ] be an increasing function, then there is a solution x A C [ 0 , T ] of (1) with the Riemann–Stieltjes integral condition (3) and this solution given by
x ( t ) = 1 h ( T ) h ( 0 ) x o 0 T 0 t f s , x ( x ( ϕ ( s ) ) ) d s d h ( t ) + 0 t f s , x ( x ( ϕ ( s ) ) ) d s , t [ 0 , T ] .
Proof. 
Let a k = h ( t k ) h ( t k 1 ) , 0 = t 0 < t 1 < t 2 < . . . < t m = T ) and τ k ( t k 1 , t k ) , then the multi-point nonlocal condition (2) will be
k = 1 m x ( τ k ) h ( t k ) h ( t k 1 ) = x o and k = 1 m a k = h ( T ) h ( 0 ) .
Hence,
lim m k = 1 m a k x ( τ k ) = lim m k = 1 m x ( τ k ) h ( t k ) h ( t k 1 ) = 0 T x ( t ) d h ( t ) = x o
and
x ( t ) = 1 h ( T ) h ( 0 ) x o lim m k = 1 m h ( t k ) h ( t k 1 ) 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s + 0 t f s , x ( x ( ϕ ( s ) ) ) d s = 1 h ( T ) h ( 0 ) x o 0 T 0 t f s , x ( x ( ϕ ( s ) ) ) d s d h ( t ) + 0 t f s , x ( x ( ϕ ( s ) ) ) d s
which is the solution of (1) with the Riemann–Stieltjes integral condition (3). This completes the proof. □

2.4. Infinite-Point Boundary Condition

Let x A C [ 0 , T ] be a solution of the BVP (1) and (2). Then, we can formulate the next theorem.
Theorem 3.
Let the assumptions (i)–(iv) be satisfied. Assume that the series:
k = 1 a k = 1 B
is convergent. Then, there is a solution x A C [ 0 , T ] of (1) and (4), and this solution is given by
x ( t ) = B x o k = 1 a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s + 0 t f s , x ( x ( ϕ ( s ) ) ) d s .
Proof. 
Assume that x A C [ 0 , T ] be a solution of the BVP (1) and (2), thus we have
| a k x ( τ k ) | a k x
and
| a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s | a k 0 τ k | f s , x ( x ( ϕ ( s ) ) ) | d s a k 0 τ k ( M + b T ) d s a k L T .
Using the comparison test, we deduce that the series
k = 1 a k x ( τ k ) a n d k = 1 a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s
are convergent. Then as m in (5), we get
x ( t ) = x o k = 1 a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s B + 0 t f s , x ( x ( ϕ ( s ) ) ) d s .
Furthermore, we have
k = 1 a k x ( τ k ) = B 1 B x 0 B 1 B k = 1 a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s + k = 1 a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s = x 0 .
This proves that the solution of (8) satisfies (1) under infinite-point boundary condition (4). This completes the proof. □

3. Uniqueness of the Solution

Here we prove the uniqueness of the solution of the BVP (1) and (2). Assume that
( 1 )
| f ( t , u ) f ( t , v ) | b | u v | .
( 2 )
| f ( t , 0 ) | M .
Theorem 4.
Let the hypothesis ( 1 ), ( 2 ), (iii), and (iv) be held. If 2 b ( L + 1 ) T < 1 , then the solution x A C [ 0 , T ] of the BVP (1) and (2) is unique.
Proof. 
By putting y = 0 in ( 1 ) and using ( 2 ) , we obtain
| f ( t , x ) | b | x | + | f ( t , 0 ) | b | x | + M ,
thus we deduce that all assumptions of Theorem 1 are satisfied. Then the BVP (1) and (2) has a solution.
Now, let x , y be two solutions of (1) and (2), then
| x ( t ) y ( t ) | = | A x o k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s + 0 t f s , x ( x ( ϕ ( s ) ) ) d s A x o k = 1 m a k 0 τ k f s , y ( y ( ϕ ( s ) ) ) d s 0 t f s , y ( y ( ϕ ( s ) ) ) d s | A | k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s k = 1 m a k 0 τ k f s , y ( y ( ϕ ( s ) ) ) d s | + 0 t | f s , x ( x ( ϕ ( s ) ) ) f s , y ( y ( ϕ ( s ) ) ) | d s A k = 1 m a k 0 τ k | f s , x ( x ( ϕ ( s ) ) ) f s , y ( y ( ϕ ( s ) ) ) | d s + 0 t | f s , x ( x ( ϕ ( s ) ) ) f s , y ( y ( ϕ ( s ) ) ) | d s A k = 1 m a k b 0 τ k | x ( x ( ϕ ( s ) ) ) y ( y ( ϕ ( s ) ) ) | + b 0 t | x ( x ( ϕ ( s ) ) ) y ( y ( ϕ ( s ) ) ) | d s .
However,
| x ( x ( ϕ ( s ) ) ) y ( y ( ϕ ( s ) ) ) | = | x ( x ( ϕ ( s ) ) ) y ( y ( ϕ ( s ) ) ) + x ( y ( ϕ ( s ) ) ) x ( y ( ϕ ( s ) ) ) | L | x ( ϕ ( s ) ) ) y ( ϕ ( s ) ) | + | x ( y ( ϕ ( s ) ) ) y ( y ( ϕ ( s ) ) ) | L x y + x y = ( L + 1 ) x y .
Using (9), we get
| x ( t ) y ( t ) | A k = 1 m a k b ( L + 1 ) x y 0 τ k d s + b ( L + 1 ) x y 0 t d s b ( L + 1 ) x y A k = 1 m a k τ k + b ( L + 1 ) x y t b ( L + 1 ) T ( A k = 1 m a k + 1 ) x y ,
thus we have
x y 1 2 b ( L + 1 ) T 0 .
Since 2 b ( L + 1 ) T < 1 , then we get x = y and the solution of the BVP (1) and (2) is unique. □

4. Continuous Dependence

Definition 1.
The solution of (1) and (2) depends continuously on x o if ϵ 1 > 0 , δ 1 ( ϵ 1 ) > 0 such that
| x o x o * | δ 1 x x * ϵ 1 ,
x * is the unique solution of the BVP
d x * ( t ) d t = f t , x * ( x * ( ϕ ( t ) ) ) a . e . t ( 0 , T ]
and
k = 1 m a k x * ( τ k ) = x 0 * , τ k ( 0 , T ] , a k > 0 .
Theorem 5.
Let the hypothesis of Theorem 4 be held. Then the solution of BVP (1) and (2) depends continuously on x o .
Proof. 
Consider the two solutions x , x * of (1) and (2) and (10) and (11), respectively, thus we have
| x ( t ) x * ( t ) | = | A x o k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s + 0 t f s , x ( x ( ϕ ( s ) ) ) d s A x o * k = 1 m a k 0 τ k f s , x * ( x * ( ϕ ( s ) ) ) d s 0 t f s , x * ( x * ( ϕ ( s ) ) ) d s | = | A ( x o x o * ) + A k = 1 m a k 0 τ k f s , x * ( x * ( ϕ ( s ) ) ) f s , x ( x ( ϕ ( s ) ) ) d s + 0 t f s , x ( x ( ϕ ( s ) ) ) f s , x * ( x * ( ϕ ( s ) ) ) d s | A | x o x o * | + A k = 1 m a k 0 τ k | f s , x ( x ( ϕ ( s ) ) ) f s , x * ( x * ( ϕ ( s ) ) ) | d s + 0 t | f s , x ( x ( ϕ ( s ) ) ) f s , x * ( x * ( ϕ ( s ) ) ) | d s A δ 1 + b A k = 1 m a k 0 τ k | x ( x ( ϕ ( s ) ) ) x * ( x * ( ϕ ( s ) ) ) | d s . + b 0 t | x ( x ( ϕ ( s ) ) ) x * ( x * ( ϕ ( s ) ) ) | d s .
Using (9), we get
| x ( t ) x * ( t ) | A δ 1 + b A k = 1 m a k ( L + 1 ) x x * 0 τ k d s + b ( L + 1 ) x x * 0 t d s A δ 1 + 2 b T ( L + 1 ) x x * ,
thus we have
x x * 1 2 b T ( L + 1 ) A δ 1
x x * A δ 1 1 2 b T ( L + 1 ) = ϵ 1 .
Since 2 b T ( L + 1 ) < 1 , then the result follows. □
Definition 2.
The solution of the BVP (1) and (2) depends continuously on the nonlocal data a k if ϵ 2 > 0 , δ 2 ( ϵ 2 ) > 0 such that
| a k a k * | δ 2 x x * ϵ 2 ,
x * is the unique solution of the BVP
d x * ( t ) d t = f t , x * ( x * ( ϕ ( t ) ) ) a . e . t ( 0 , T ]
and
k = 1 m a k * x * ( τ k ) = x o , τ k ( 0 , T ] , a k * > 0 .
Theorem 6.
Let the hypothesis of Theorem 4 be hold, then the solution of BVP (1) and (2) depends continuously on a k .
Proof. 
Consider the two solutions x , x * of BVP (1) and (2) and (12) and (13), respectively, thus we have
| x ( t ) x * ( t ) | = | A x o k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s + 0 t f s , x ( x ( ϕ ( s ) ) ) d s A * x o k = 1 m a k * 0 τ k f s , x * ( x * ( ϕ ( s ) ) ) d s 0 t f s , x * ( x * ( ϕ ( s ) ) ) d s | x o | A A * | + 0 t | f s , x ( x ( ϕ ( s ) ) ) f s , x * ( x * ( ϕ ( s ) ) ) | d s + | A k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s A * k = 1 m a k * 0 τ k f s , x * ( x * ( ϕ ( s ) ) ) d s | x o A A * k = 1 m | a k a k * | + b 0 t | x ( x ( ϕ ( s ) ) ) x * ( x * ( ϕ ( s ) ) ) | d s + | A k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s A k = 1 m a k * 0 τ k f s , x * ( x * ( ϕ ( s ) ) ) d s | + | A k = 1 m a k * 0 τ k f s , x * ( x * ( ϕ ( s ) ) ) d s A * k = 1 m a k * 0 τ k f s , x * ( x * ( ϕ ( s ) ) ) d s | x o A A * δ m + b ( L + 1 ) T x x * + | A A * | | k = 1 m a k * 0 τ k f s , x * ( x * ( ϕ ( s ) ) ) d s | + A | k = 1 m a k 0 τ k f s , x ( x ( ϕ ( s ) ) ) d s k = 1 m a k 0 τ k f s , x * ( x * ( ϕ ( s ) ) ) d s | + A | k = 1 m a k 0 τ k f s , x * ( x * ( ϕ ( s ) ) ) d s k = 1 m a k * 0 τ k f s , x * ( x * ( ϕ ( s ) ) ) d s | x o A A * δ m + b ( L + 1 ) T x x * + A A * δ m k = 1 m a k * 0 τ k | f s , x * ( x * ( ϕ ( s ) ) ) | d s + A k = 1 m a k 0 τ k | f s , x ( x ( ϕ ( s ) ) ) f s , x * ( x * ( ϕ ( s ) ) ) | d s + A | k = 1 m a k k = 1 m a k * | 0 τ k | f s , x * ( x * ( ϕ ( s ) ) ) | d s x o A A * δ m + b ( L + 1 ) T x x * + A A * δ m k = 1 m a k * 0 τ k ( M + b | x * ( x * ( ϕ ( s ) ) ) | ) d s + A b k = 1 m a k 0 τ k | x ( x ( ϕ ( s ) ) ) x * ( x * ( ϕ ( s ) ) ) | d s + A δ m 0 τ k ( M + b | x * ( x * ( ϕ ( s ) ) ) | ) d s x o A A * δ m + 2 b ( L + 1 ) T x x * + 2 A δ m L T .
Then, we obtain
x x * 1 2 b T ( L + 1 ) x o A A * δ m + 2 A δ m L T
and
x x * x o A A * m + 2 A m L T δ 1 2 b T ( L + 1 ) = ϵ 2 .
Since 2 b T ( L + 1 ) < 1 , then the solution of the BVP (1) and (2) depends continuously on a k .

5. Examples

Example 1.
Consider the nonlinear self-reference differential equation
d x ( t ) d t = 1 14 e t 2 cos 2 2 t + ln ( 1 + | x ( x ( β t ) ) | ) 15 t a . e . t ( 0 , 3 ]
with the infinite point nonlocal boundary condition
k = 1 1 k 2 x 3 k 1 k 2 + 1 = 1.7 ,
where β ( 0 , 1 ) , here we have ϕ ( t ) = β t , A = 1 k = 1 1 k 2 = 6 π 2 and x o = 1.7 .
It is clear that series k = 1 1 k 2 is convergent. Now set
f t , x ( x ( ϕ ( t ) ) ) = 1 14 e t 2 cos 2 2 t + ln ( 1 + | x ( x ( β t ) ) | ) 15 t .
Then
f t , x ( x ( ϕ ( t ) ) ) 1 14 e t 2 cos 2 2 t + 1 12 x ( x ( β t ) ) ,
thus we have
m ( t ) = 1 14 e t 2 cos 2 t ,
hence M = 1 14 , b = 1 12 , L = 9 28 [ 0 , 1 3 ] .
Furthermore, we have 27 28 = L T < A x o 1.0335 < T ( 1 2 L ) = 15 14 .
Therefore, from Theorem 3, the BVP (14) and (15) has at least one solution x [ 0 , 3 ] .
Example 2.
Consider the nonlinear self-reference differential equation
d x ( t ) d t = 1 16 t 3 e t 2 cos 2 ( 3 ( t + 1 ) ) + 1 9 ( x ( x ( t 4 ) ) ) 2 1 + x ( x ( t 4 ) ) + e t | sin ( x ( x ( t 4 ) ) ) | x ( x ( t 4 ) ) 3 a . e . t ( 0 , 1 ]
with the infinite point nonlocal boundary condition
k = 1 2 3 k x 2 k 1 k 2 = 1 .
Here, we have ϕ ( t ) = t 4 , A = 1 k = 1 2 3 k = 1 2 and x o = 1 .
The series k = 1 2 3 k is convergent. Now set
f t , x ( x ( ϕ ( t ) ) ) = 1 16 t 3 e t 2 cos 2 ( 3 ( t + 1 ) ) + 1 9 ( x ( x ( t 4 ) ) ) 2 1 + x ( x ( t 4 ) ) + e t | sin ( x ( x ( t 4 ) ) ) | x ( x ( t 4 ) ) 3 .
Then
| f t , x ( x ( ϕ ( t ) ) ) | 1 16 t 3 e t 2 cos 2 ( 3 ( t + 1 ) ) + 4 27 x ( x ( t 4 ) ) .
thus we have,
m ( t ) = 1 16 t 3 e t 2 cos 2 ( 3 ( t + 1 ) ) ,
so we get M = 1 16 , b = 4 27 , L = 91 432 [ 0 , 1 / 3 ] .
Hence, 91 432 = L T < A x o = 0.5 < T ( 1 2 L ) = 125 216 .
Therefore, from Theorem 3, the BVP (16) and (17) has at least one solution x [ 0 , 1 ] .
Example 3.
Consider the nonlinear self-reference differential equation
d x ( t ) d t = 1 9 e 2 t t 2 + 1 + 1 17 e t 2 x ( x ( t 2 ) ) cos 2 x ( x ( t 2 ) ) + t 4 x ( x ( t 2 ) ) a . e . t ( 0 , 1 ]
with the nonlocal integral condition
0 1 x ( s ) d ( t ) = 1 3 .
Here, we have ϕ ( t ) = t 2 , the function h : [ 0 , 1 ] [ 0 , 1 ] such that h ( t ) = t is an increasing function, furthermore, we have A = 1 and x o = 1 3 .
Now set
f t , x ( x ( ϕ ( t ) ) ) = 1 9 e 2 t t 2 + 1 + 1 17 e t 2 x ( x ( t 2 ) ) cos 2 x ( x ( t 2 ) ) + t 4 x ( x ( t 2 ) ) .
Then
f t , x ( x ( ϕ ( t ) ) ) 1 9 e 2 t t 2 + 1 + 2 17 x ( x ( t 2 ) ) ,
thus we have
m ( t ) = 1 9 e 2 t t 2 + 1 ,
so we get M = 1 9 , b = 2 17 , L = 35 125 [ 0 , 1 / 3 ] .
Furthermore, 35 153 = L T < A x o = 1 3 < T ( 1 2 L ) = 83 153 .
Therefore, from Theorem 2, the BVP (18) and (19) has at least one solution x [ 0 , 1 ] .

6. Conclusions

In this paper, we introduce a nonlocal boundary value problem with deviating argument depending on both the state variable x and the time t; this case is of importance in theory and practice and also has many application models. Here we have proved, the existence of absolutely continuous solutions for the nonlocal problem (1)–(2). The sufficient conditions for the uniqueness have been given and the continuous dependence has been proved. Generalization for the boundary condition (2) to (3) and (4) has been proved. Some examples; to illustrate the obtained results; have been given. Moreover, we have generalized the results in [11,12,18].

Author Contributions

These authors contributed equally to this work. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Acknowledgments

The authors would like to thank the editor and the referees for their positive comments and useful suggestions which have improved this manuscript.

Conflicts of Interest

The authors declare no conflict of interest.

References

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El-Sayed, A.; Hamdallah, E.; Ebead, H. On a Nonlocal Boundary Value Problem of a State-Dependent Differential Equation. Mathematics 2021, 9, 2800. https://doi.org/10.3390/math9212800

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El-Sayed A, Hamdallah E, Ebead H. On a Nonlocal Boundary Value Problem of a State-Dependent Differential Equation. Mathematics. 2021; 9(21):2800. https://doi.org/10.3390/math9212800

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El-Sayed, Ahmed, Eman Hamdallah, and Hanaa Ebead. 2021. "On a Nonlocal Boundary Value Problem of a State-Dependent Differential Equation" Mathematics 9, no. 21: 2800. https://doi.org/10.3390/math9212800

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