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R E S E A R C H

Open Access

Solvability of second order linear

differential equations in the sequence

space

n(

φ

)

Abdullah Alotaibi

1

, M. Mursaleen

1,2*

and Badriah A.S. Alamri

1

*Correspondence: [email protected] 1Operator Theory and Applications Research Group, Department of Mathematics, Faculty of Science, King Abdulaziz University, Jeddah, Saudi Arabia

2Department of Mathematics, Aligarh Muslim University, Aligarh, India

Abstract

We apply the concept of measure of noncompactness to study the existence of solution of second order differential equations with initial conditions in the sequence spacen(

φ

).

MSC: Primary 47H09; 47H10; secondary 34A34

Keywords: Measure of noncompactness; Darbo’s fixed point theorem; Sequence spaces; Infinite system of second order differential equations

1 Introduction and preliminaries

In recent years, the notion of measure of noncompactness has been effectively utilized in sequence spaces for different classes of differential equations (see [4,5,8,11–15]). By applying this notion, Aghajani and Pourhadi [2] investigated the infinite system of second-order differential equations in an1-space. Since then Mohiuddine et al. [10] and Banaś et al. [6] focused on this system in the sequence spacep.

A measure of noncompactness is a nonnegative real-valued map defined on a collection of bounded subsets of a normed (metric) space which maps the class of relatively compact sets (known as kernel) to zero, while other sets are mapped to a positive value. There are several ways to define this notion on a given space. The widely used approach is the axiomatic one, introduced in [3], which is given below.

LetMEdenote the family of all nonempty bounded subsets of a Banach spaceEandNE

be its subfamily consisting of all relatively compact sets. LetB(x,r) denote the closed ball centered atxwith radiusrandBr=B(θ,r).

We recall the following definition given in [3].

Definition 1.1([3, Definition 3.1.3]) A mappingμ: ME−→R+ is called ameasure of

noncompactness(MNC for short) if

(i) kerμis nonempty and a subset ofNE.

(ii) μ(X)≤μ(Y)forXY.

(iii) μ(X) =μ(X).

(iv) μ(ConvX) =μ(X).

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(v) For allλ∈[0, 1],

μλX+ (1 –λ)Yλμ(X) + (1 –λ)μ(Y).

(vi) If(Xn)n∈Nis a sequence of closed sets fromMEsatisfying

Xn+1⊂Xn for alln∈N and μ(Xn)→0 asn→ ∞,

then

X∞= ∞

n=1

Xn=∅.

Definition 1.2([5, Definition 3.1.3]) For a measure of noncompactnessμinE, the map-pingG:BE−→Eis said to be aμE-contractionif there exists a constant 0 <k< 1 such

that

μG(Y)≤(Y) (1.1)

for any bounded closed subsetYB.

Darbo [7] used the idea of measure of noncompactness to obtain a new fixed point the-orem which generalizes the Banach contraction principle and assures the existence of a fixed point concerning the so-called condensing operators.

Theorem 1.1([7]) Letbe a nonempty,closed,bounded,and convex subset of a Banach space E,and letG: →be a continuous mapping such that there exists a constantθ ∈ [0, 1)with the propertyμ(G())≤θ μ().ThenGhas a fixed point in.

The following definition was given in [1] which is a generalization of Meir–Keeler con-traction (MKC) given in [9].

Definition 1.3([1]) For an arbitrary measure of noncompactnessμon a Banach spaceX, we say that an operatorT:BBis a Meir–Keeler condensing operator if for any> 0 there existsδ> 0 such that

μ(E) <+δμT(E)< (1.2)

for any bounded subsetEofB; whereBis a nonempty subset ofX.

Now we state the following theorem for Meir–Keeler condensing operators which will be applied in our main results.

Theorem 1.2([1]) Letμbe an arbitrary measure of noncompactness on a Banach space X.

IfT:BB is a continuous and Meir–Keeler condensing operator,thenThas at least one fixed point and the set of all fixed points ofTin B is compact,where B is a nonempty,

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2 The sequence spacen(

φ

)

We denote by Cthe space of finite sets of distinct positive integers. For any σC, we defineα(σ) ={αn(σ)}such thatαn(σ) is 1 ifnis inσ; and 0 elsewhere. Write

Cr=

σC: ∞

n=1

αn(σ)≤r

,

and define

=φ= (φk) : 0 <φ1≤φnφn+1and (n+ 1)φnnφn+1 .

Sargent [16] defined the following sequence spaces which were further studied in [11]. WriteS(x) for the set of all sequences that are rearrangements ofx. Forφ,

m(φ) =

x= (xk) :xm(φ)=sup

r≥1

sup

σCr

1 φr

kσ

|xk|

<∞

,

n(φ) =

x= (xk) :xn(φ)= sup

uS(x)

k=1

|uk|φk

<∞

,

whereφk=φkφk–1. Note that, for alln∈N={1, 2, 3, . . .},m(φ) =1,n(φ) =∞ifφn= 1;

andm(φ) =∞,n(φ) =1ifφn=n.

We have the following important result.

Theorem 2.1([12]) For any bounded subsetQof n(φ),we have

χ(Q) = lim

k→∞supxQ

sup

uS(x)

n=k

|un|φn

,

whereχ(Q) denotes theHausdorff measure of noncompactnessof the setQwhich is de-fined by

χ(Q) :=inf

> 0 :Q

n

i=1

B(xi,ri),xiX,ri<(i= 1, 2, . . .)

.

3 Infinite system of second order differential equations inn(

φ

)

We study the following infinite system:

d2u

i

dt2 = –fi

t,u1(t),u2(t),u3(t), . . .

; ui(0) =ui(T) = 0,t∈[0,T],i= 1, 2, 3 . . . (3.1)

LetC(I,R) be the space of all continuous real functions on the intervalI= [a,b] and

C2(I,R) be the class of functions with the second continuous derivative onI. A function

u= (ui)∈C2(I,R) is a solution of (3.1) if and only ifuC(I,R) is a solution of the system

of integral equations

ui(t) =

T

0

G(t,s)fi

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wherefi(t,u)∈C(I×R∞,R),i= 1, 2, 3, . . . ; and the Green’s function associated with (3.1)

is given by

G(t,s) =

⎧ ⎨ ⎩

t

T(Ts), 0≤tsT, s

T(Tt), 0≤stT.

(3.3)

From (3.2) and (3.3)

ui(t) =

t

0

s

T(Tt)fi

s,u(s)ds+

T

t

t

T(Ts)fi

s,u(s)ds.

Now compute

d

dtui(t) = –

1

T t

0

sfi

s,u(s)ds+ 1

T

T

t

(Ts)fi

s,u(s)ds.

Again differentiating we get

d2u

i(t)

dt2 = – 1

T

tfi

t,u(t)+ 1

T(tT)fi

t,u(t)) = –fi

t,u(t)).

The solution of the infinite system (3.1) in the sequence space1was discussed by Agha-jani and Pourhadi [2] by establishing a generalization of Darbo type fixed point theorem using the concept ofα-admissibility function and Schauder’s fixed point theorem. Here, we determine the solvability of system (3.1) in Banach sequence spacesn(φ). Our result is more general than that of [2].

Assume that

(i) The functionsfiare defined on the setI×R∞and take real values. The operatorf

defined on the spaceI×n(φ)inton(φ)as

(t,u)→(fu)(t) =f1

t,u(t),f2

t,u(t),f3

t,u(t), . . .

is such that the class of all functions((fu)(t))tIis equicontinuous at every point of

the spacen(φ).

(ii) The following inequality holds:

fn

t,u1(t),u2(t),u3(t), . . .≤gn(t) +hn(t)un(t),

wheregn(t)andhn(t)are real functions defined and continuous onIsuch that

k=1gk(t)φkconverges uniformly onIand the sequence(hn(t))is equibounded

onI.

Write

G=sup

tI

k=1

gk(t)φk

and

H= sup

n∈N,tI

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Theorem 3.1 Let conditions(i)(ii)hold.Then system(3.1)has at least one solution u(t) = course a nonempty, bounded, closed, and convex subset ofn(φ). Consider the operator

F= (Fi) onC(I,B¯) defined as follows. FortI,

Also since (Fiu)(t) satisfies the boundary conditions, we have

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and

Pourhadi [2] but our proof is quite different.

4 Example

In order to illustrate the above result, we provide the following example.

Example4.1 Let us consider the system of second order differential equations

d considered system (3.1). Clearly j

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Notice that, for anytI= [0,T], (fk(t,u(t)))∈n(φ) if (uk(t))∈n(φ). Moreover, we have

which implies continuity as in assumption (i). Now, we show that assumption (ii) is satis-fied.

j4 is continuous and

Thus, from Theorem3.1, for a suitable value ofr1(as discussed in Theorem3.1) the operatorFas defined in Theorem3.1onB¯(u0,r

1) has a fixed pointu(t) = ((ui(t))∈n(φ),

which is a solution of system (4.1).

Funding

This project was funded by the Deanship of Scientific Research (DSR) at King Abdulaziz University, Jeddah, under grant No. RG-18-130-37. The authors, therefore, acknowledge with thanks DSR for technical and financial support.

Competing interests

The authors declare that they have no competing interests.

Authors’ contributions

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Publisher’s Note

Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Received: 13 June 2018 Accepted: 18 September 2018

References

1. Aghajani, A., Mursaleen, M., Haghighi, A.S.: A fixed point theorem for Meir–Keeler condensing operator via measure of noncompactness. Acta Math. Sci.35B(3), 552–556 (2015)

2. Aghajani, A., Pourhadi, E.: Application of measure of noncompactness to1-solvability of infinite systems of second order differential equations. Bull. Belg. Math. Soc. Simon Stevin22(1), 105–118 (2015)

3. Bana´s, J., Goebel, K.: Measures of Noncompactness in Banach Spaces. Lecture Notes in Pure and Applied Mathematics, vol. 60. Dekker, New York (1980)

4. Bana´s, J., Lecko, M.: Solvability of infinite systems of differential equations in Banach sequence spaces. J. Comput. Appl. Math.137, 363–375 (2001)

5. Bana´s, J., Mursaleen, M.: Sequence Spaces and Measure of Noncompactness with Applications to Differential and Integral Equation. Springer, India (2014)

6. Bana´s, J., Mursaleen, M., Rizvi, S.M.H.: Existence of solutions to a boundary-value problem for an infinite system of differential equations. Electron. J. Differ. Equ.2017, 262 (2017)

7. Darbo, G.: Punti uniti in transformazioni a condominio non compatto. Rend. Semin. Mat. Univ. Padova24, 84–92 (1955)

8. Das, A., Hazarika, B., Arab, R., Mursaleen, M.: Solvability of the infinite system of integral equations in two variables in the sequence spacesc0and1. J. Comput. Appl. Math.326, 183–192 (2017)

9. Meir, A., Keeler, E.: A theorem on contraction mappings. J. Math. Anal. Appl.28, 326–329 (1969)

10. Mohiuddine, S.A., Srivastava, H.M., Alotaibi, A.: Application of measures of noncompactness to the infinite system of second-order differential equations inpspaces. Adv. Differ. Equ.2016, 317 (2016)

11. Mursaleen, M.: On some geometric properties of a sequence space related tolp. Bull. Aust. Math. Soc.67, 343–347 (2003)

12. Mursaleen, M.: Application of measure of noncompactness to infinite system of differential equations. Can. Math. Bull.56, 388–394 (2013)

13. Mursaleen, M., Bilalov, B., Rizvi, S.M.H.: Applications of measures of noncompactness to infinite system of fractional differential equations. Filomat31(11), 3421–3432 (2017)

14. Mursaleen, M., Mohiuddine, S.A.: Applications of measure of noncompactness to the infinite system of differential equations inpspaces. Nonlinear Anal.75, 2111–2115 (2012)

15. Mursaleen, M., Rizvi, S.M.H.: Solvability of infinite system of second order differential equations inc0and1by Meir–Keeler condensing operator. Proc. Am. Math. Soc.144(10), 4279–4289 (2016)

References

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