Hindawi Publishing Corporation Abstract and Applied Analysis Volume 2013, Article ID 792431, 9 pages http://dx.doi.org/10.1155/2013/792431 Research Article Relaxation Problems Involving Second-Order Differential Inclusions Adel Mahmoud Gomaa1,2 1 2 Taibah University, Faculty of Applied Science, Department of Applied Mathematics, Al-Madinah, Saudi Arabia Mathematics Department, Faculty of Science, Helwan University, Cairo, Egypt Correspondence should be addressed to Adel Mahmoud Gomaa; gomaa 5@hotmail.com Received 12 November 2012; Accepted 12 March 2013 Academic Editor: Malisa R. Zizovic Copyright © 2013 Adel Mahmoud Gomaa. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. We present relaxation problems in control theory for the second-order differential inclusions, with four boundary conditions, Μ ∈ πΉ(π‘, π’(π‘), π’(π‘)) Μ Μ ∈ πΉ(π‘, π’(π‘), π’(π‘)) Μ π’(π‘) a.e. on [0, 1]; π’(0) = 0, π’(π) = π’(π) = π’(1) and, with π ≥ 3 boundary conditions, π’(π‘) a.e. on Μ = 0, π’(1) = ∑π−2 π π’(π ), where 0 < π < π < 1, 0 < π < π < ⋅ ⋅ ⋅ < π < 1 and πΉ is a multifunction from [0, 1] × Rπ × [0, 1]; π’(0) π π 1 2 π−2 π=1 π π R to the nonempty compact convex subsets of R . We have results that improve earlier theorems. and, with π ≥ 3 boundary conditions, 1. Introduction Second-order differential inclusions of three boundary conditions were studied by many authors [1–6], using Hartmantype functions. Such a function was first introduced by [7] for two boundary conditions. Moreover, in [8] we consider second-order differential inclusions with four boundary conditions, π’Μ (π‘) ∈ πΉ (π‘, π’ (π‘) , π’Μ (π‘)) , π’ (0) = π₯0 , a.e. on [0, π] , π’ (π) = π’ (π) = π’ (π) , (1) where 0 < π < π < π and πΉ is a multifunction from [0, π] × Rπ × Rπ to the nonempty compact subsets of Rπ , while in [9] we study four-point boundary value problems for differential inclusions and differential equations with and without multivalued moving constraints. In the present paper, we study relaxation results for the second-order differential inclusions, with four boundary conditions, π’Μ (π‘) ∈ πΉ (π‘, π’ (π‘) , π’Μ (π‘)) , π’Μ (0) = 0, a.e. on [0, 1] , π−2 π’ (1) = ∑ ππ π’ (ππ ) , (π) π=1 where 0 < π < π < 1, 0 < π1 < π2 < ⋅ ⋅ ⋅ < ππ−2 < 1, and πΉ is a multifunction from [0, 1] × Rπ × Rπ to the non-empty compact subsets of Rπ . In conjunction with Problem (π) and Problem (π) we also consider the following problems: π’Μ (π‘) ∈ ext πΉ (π‘, π’ (π‘) , π’Μ (π‘)) , π’ (0) = 0, π’ (π) = π’ (π) = π’ (1) , π’Μ (π‘) ∈ ext πΉ (π‘, π’ (π‘) , π’Μ (π‘)) , π’Μ (0) = 0, a.e. on [0, 1] , π−2 (ππ ) a.e. on [0, 1] , π’ (1) = ∑ ππ π’ (ππ ) . (ππ ) π=1 π’Μ (π‘) ∈ πΉ (π‘, π’ (π‘) , π’Μ (π‘)) , π’ (0) = 0, a.e. on [0, 1] , π’ (π) = π’ (π) = π’ (1) (π) Μ By ext πΉ(π‘, π’(π‘), π’(π‘)), we denote the set of extreme points of Μ πΉ(π‘, π’(π‘), π’(π‘)). 2 Abstract and Applied Analysis 2. Notations and Preliminaries Throughout this paper we let πΌ = [0, 1] and 0 < π1 < π2 < ⋅ ⋅ ⋅ < ππ−2 < 1. We will use the following definitions, notations, and summarize some results. (i) A multifunction πΉ from a metric space (π, π) to the set ππ (π) of all closed subsets of another metric space π is lower semicontinuous (l. s. c.) at π₯0 ∈ π if for every open subset π in π with πΉ(π₯0 ) ∩ π =ΜΈ 0 there exists an open subset π in π such that π₯0 ∈ π and πΉ(π₯) ∩ π =ΜΈ 0 for all π₯ ∈ π. πΉ is l. s. c. if it is l. s. c. at each π₯0 ∈ π. (ii) πΉ is upper semicontinuous (u. s. c.) at π₯0 ∈ π if for every open subset π in π and containing πΉ(π₯0 ) there exists an open subset π in π such that π₯0 ∈ π and πΉ(π₯) ⊆ π, for all π₯ ∈ π. πΉ is u. s. c. if it is u. s. c. at each π₯0 ∈ π. (iii) A multifunction πΉ from πΌ into the set ππ (π) of all closed subsets of π is measurable if for all π₯ ∈ π the function π‘ → π(π₯, πΉ(π‘)) = inf{β π₯ − π¦ β: π¦ ∈ πΉ(π‘)} is measurable [10–13]. (iv) Let (Ω, Σ) be a measurable space and π a separable Banach space. We say that πΉ : Ω → ππ (π) is graph measurable if ππ (πΉ) = {(π§, π₯) ∈ Ω × π : π₯ ∈ πΉ (π§)} ∈ Σ × B (π) , (2) where B(π) is the Borel π-field of π. For further details we refer to [14–16]. (v) πΉ is continuous if it is lower and upper semicontinuous. (vi) For each π΄, π΅ ∈ ππ (π), the Hausdorff metric is defined by ππ» (π΄, π΅) = max [sup π (π, π΅) , sup π (π, π΄)] . π∈π΄ π∈π΅ (3) It is known that the space (ππ (π), ππ») is a generalized metric space, if the sets are not bounded (see, for instance, [14, 15]). (vii) A multifunction πΉ is Hausdorff continuous (ππ»continuous) if it is continuous from π into the metric space (ππ (π), ππ»). (viii) If πΉ has compact values in π, then πΉ is ππ»-continuous if and only if it is continuous [14, 17]. (ix) We denote by πππ (Rπ ) the nonempty compact convex subsets of Rπ . (x) The Banach spaces πΆ(πΌ, Rπ ), πΆ1 (πΌ, Rπ ), and πΆ2 (πΌ, Rπ ) endowed with the norms βπ’βπΆ = max |π’ (π‘)| , π‘∈πΌ βπ’βπΆ1 = max {βπ’βπΆ, βπ’βΜ πΆ} , βπ’βπΆ2 = max {βπ’βπΆ, βπ’βΜ πΆ, βπ’βΜ πΆ} , (4) respectively. (xi) πΏ1π€ (πΌ, Rπ ) denotes the space πΏ1 (πΌ, Rπ ) equipped with weak norm β ⋅βπ€ which is defined by σ΅©σ΅© π σ΅©σ΅© σ΅© σ΅© (5) βββπ€ = sup {σ΅©σ΅©σ΅©σ΅©∫ β (π‘) ππ‘σ΅©σ΅©σ΅©σ΅© : 0 ≤ π ≤ π ≤ 1} . σ΅©σ΅© π σ΅©σ΅© (xii) π2,1 (πΌ, Rπ ) is the Sobolev space of functions π’ : πΌ → π Μ ∈ R , π’ and π’Μ are both absolutely continuous functions so π’(π‘) πΏ1 (πΌ, Rπ ) and it is equipped with the norm βπ’βπ2,1 (πΌ,Rπ ) = βπ’βπΏ1 (πΌ,Rπ ) + βπ’βΜ πΏ1 (πΌ,Rπ ) + βπ’βΜ πΏ1 (πΌ,Rπ ) . π (xiii) Let π : πΌ → 2R be a multifunction and πΏπ 1 = {β ∈ πΏ1 (πΌ, Rπ ) : β(π‘) ∈ π (π‘)}. (xiv) By a solution of (π) (resp., of (ππ )) we mean a funcΜ = β(π‘) a.e. on πΌ with β ∈ tion π’ ∈ π2,1 (πΌ, Rπ ) such that π’(π‘) 1 1 (resp., β ∈ πΏ πΏπΉ(⋅,π’(⋅), Μ Μ ) and π’(0) = 0, π’(π) = π’(⋅)) extπΉ(⋅,π’(⋅),π’(⋅)) π’(π) = π’(1). (xv) By a solution of (π) (resp., of (ππ )) we mean a funcΜ = β(π‘) a.e. on πΌ with β ∈ tion π’ ∈ π2,1 (πΌ, Rπ ) such that π’(π‘) 1 1 Μ (resp., β ∈ πΏ = 0, π’(1) = πΏπΉ(⋅,π’(⋅), Μ Μ ) and π’(0) π’(⋅)) extπΉ(⋅,π’(⋅),π’(⋅)) π−2 ∑π=1 ππ π’(ππ ). (xvi) In the sequel by Δ π (resp., Δ ππ ) we denote the solution set of Problem (π) (resp., of Problem (ππ )). Moreover, by Δ π (resp., Δ ππ ) we denote the solution set of Problem (π) (resp., of Problem (ππ )). Definition 1. Let πΈ be a Banach space and let π be a metric space. A multifunction πΊ : πΌ × π → πππ (πΈ) has the ScorzaDragoni property (the SD-property) if for every π > 0 there exists a closed set π΄ ⊂ πΌ such that the Lebesgue measure π(πΌ \ π΄) is less than π and πΊ|π΄×π is continuous. The multifunction πΊ is called integrably bounded on compacta in π if, for any compact subset π ⊂ π, we can find an integrable function ππ : πΌ → R+ such that sup{β π¦ β : π¦ ∈ πΊ(π‘, π§)} ≤ ππ(π‘), for almost every π§ ∈ π. Theorem 2 (see [18]). Let π be a complete metric space, πΈ a separable Banach space, πΈπ the Banach space πΈ endowed with the weak topology, π : πΌ × π → πππ (πΈπ ), and πΎ a compact 1 subset of πΆ(πΌ, π). Furthermore, let π : πΎ → 2πΏ (πΌ,πΈ) be a multifunction defined by π (π¦) = {π ∈ πΏ1 (πΌ, πΈ) : π (π‘) ∈ π (π‘, π¦ (π‘)) π.π. ππ πΌ} . (6) If π has the SD-property and is integrably bounded on compacta in π, then the set π΄ πΎ = {π ∈ πΆ (πΎ, πΏ1π€ (πΌ, πΈ)) : π (π¦) ∈ π (π¦) ∀π¦ ∈ πΎ} (7) is nonempty complete subset of the space πΆ(πΎ, πΏ1π€ (πΌ, πΈ)). Moreover, π΄ πΎ = π΄ ext πΎ where πΏ1π€ (πΌ, πΈ) is the space of equivalence classes of Bochner-integrable functions V : πΌ → πΈ with the π‘ norm β Vβπ€ = supπ‘∈π β ∫0 V(π )ππ β and π΄ ext πΎ = {π ∈ πΆ (πΎ, πΏ1π€ (πΌ, πΈ)) : π (π¦) ∈ extπ (π¦) ∀π¦ ∈ πΎ} . (8) Lemma 3 (see [19]). For π such that 1 < π < ∞ let {π’π , π’}π∈N ⊆ πΏπ (πΌ, Rπ ), supπ∈N β π’π βπ < ∞ and π’π → π’ with respect to the weak norm β ⋅βπ€ . Then π’π → π’ weakly in πΏπ (πΌ, Rπ ). Next we state a preliminary lemma, for 0 < π < π < 1, which is useful in the study of four boundary problems for the differential equations and the differential inclusions, and Abstract and Applied Analysis 3 moreover we summarize some properties of a Hartman-type function. Lemma 4 (see [8]). Let πΊ : πΌ × πΌ → R be the function defined as follows: as 0 ≤ π‘ < π, −π { { { { { {−π‘ { { { { πΊ (π‘, π) = { π‘ (π − π) + (π − π) { { { π−π { { { { { {1 − π {1 − π when π ≤ π‘ < π, ππ 0 ≤ π ≤ π‘ (9) ππ π < π ≤ 1, ππ π < π ≤ π‘ ππ π‘ < π ≤ π ππ π < π ≤ 1, (10) ππ 0 ≤ π ≤ π (ii) ππ»(πΉ(π‘, π₯, π¦), πΉ(π‘, π₯σΈ , π¦σΈ )) ≤ πΌ1 (π‘) β π₯ − π₯σΈ β +πΌ2 (π‘) β π¦ − π¦σΈ β a.e. with πΌ1 , πΌ2 ∈ πΏ1 (πΌ, R+ ) and β πΌ1 + πΌ2 β< 1/2, ππ π < π ≤ π (iii) for each (π‘, π₯, π¦) ∈ πΌ × Rπ × Rπ , ππ π < π ≤ π‘ ππ π‘ < π ≤ 1. (11) ∀π‘ ∈ πΌ; (12) π‘ 0 0 ∫ πΊ (π‘, π) π€ (π) ππ = ∫ (π‘ − π) π€ (π) ππ π π‘ (π − π) + (π − π) +∫ π€ (π) ππ π−π 0 +∫ 1 π 1−π π€ (π) ππ; 1−π (iii) supπ‘,π∈πΌ |πΊ(π‘, π)| ≤ 2, supπ‘,π∈πΌ |ππΊ(π‘, π)/ππ‘| ≤ 1. (15) with π, π1 , π2 ∈ πΏπ (πΌ, R+ ) 1 < π < ∞, (iv) the spectral radius, π(πΏ), is less than 1. Then for each solution π’ ∈ Δ ππ , there is a sequence (π’π (⋅))π∈N ⊂ Δ π converging to π’(⋅) in (πΆ1 (πΌ, Rπ ), β ⋅βπΆ1 ). π’Μ (π‘) = β (π‘) , π π‘ (π − π) (π‘ + 1) −∫ π€ (π) ππ π−π 0 σ΅© σ΅©σ΅© σ΅©σ΅©πΉ (π‘, π₯, π¦)σ΅©σ΅©σ΅© = sup {βVβ : V ∈ πΉ (π‘, π₯, π¦)} σ΅© σ΅© ≤ π (π‘) + π1 (π‘) βπ₯β + π2 (π‘) σ΅©σ΅©σ΅©π¦σ΅©σ΅©σ΅© Proof. From [9, Theorem 2.1], we obtain Δ ππ =ΜΈ 0. Moreover, we can say that β πΉ(π‘, π₯, π¦) β≤ π1 (π‘) a.e. on πΌ for some π1 ∈ πΏπ (πΌ, R+ ). Let π’ ∈ Δ π . Then (ii) if π€ ∈ πΏ1 (πΌ, Rπ ), then for all π‘ ∈ πΌ, 1 Theorem 5. Let πΉ : πΌ×Rπ ×Rπ → πππ (Rπ ) be a multifunction such that (i) for each (π₯, π¦) ∈ Rπ × Rπ , the multifunction πΉ(⋅, π₯, π¦) is measurable, (i) If π’ ∈ π2,1 (πΌ, Rπ ) with π’(0) = π₯0 , π’(1) = π’(π) = π’(π), then 0 If π1 = π2 = 0, then clearly πΏ = 0. We note that if K = {(β1 , β2 ) ∈ πΆ(πΌ, R) × πΆ(πΌ, R) : β1 (π‘), β2 (π‘) ≥ 0, ∀π‘ ∈ πΌ}, then πΏ(K) ⊆ K. Moreover, the spectral radius π(πΏ) = lim β πΏπ β1/π is an eigenvalue of πΏ with an eigenvector in K [20]. In this section, both Theorems 5 and 7 improve [19, Theorem 4.1] with [21, Theorem 6]. Indeed in [19] Papageorgiou considered (π) and (ππ ) with the two boundary conditions π’(0) = π’(1) = 0 and in [21] Ibrahim and Gomaa study the same problems with three boundary conditions π’(0) = π₯0 , π’(π) = π’(1). Then the following hold. π’ (π‘) = π₯0 + ∫ πΊ (π‘, π) π’Μ (π) ππ, (14) 3. Relaxation Theorems ππ 0 ≤ π ≤ π lastly if π ≤ π‘ ≤ 1, 1 0 σ΅¨ σ΅¨ ππΊ (π‘, π) σ΅¨σ΅¨σ΅¨ π (π‘) = ∫ σ΅¨σ΅¨σ΅¨ σ΅¨ (π (π) π (π) + π2 (π) π (π)) ππ. ππ‘ σ΅¨σ΅¨σ΅¨ 1 0 σ΅¨σ΅¨ ππ π < π ≤ π −π { { { { { { π (π − π‘ − 1) + π (π‘ − π + 1) { { { { { π−π { πΊ (π‘, π) = { 1 − π { + (π‘ − π) { { { 1−π { { { { 1−π { { { 1 { −π π π (π‘) = ∫ |πΊ (π‘, π)| (π1 (π) π (π) + π2 (π) π (π)) ππ, π σ΅¨σ΅¨ ππ π‘ < π ≤ π −π { { { { { π (π‘ − π + 1) + π (π − π‘ − 1) { { { { { π−π { { πΊ (π‘, π) = { { π‘ (π − π) + (π − π) { { { { { π−π { { { { 1 − π { {1 − π Let π1 , π2 , π ∈ πΏπ (πΌ, R+ ), 1 < π < ∞, and let πΏ be a linear operator from πΆ(πΌ, R) × πΆ(πΌ, R) to πΆ(πΌ, R) × πΆ(πΌ, R) defined by πΏ(π, π) = (π, π) such that, for all π‘ ∈ πΌ, a.e. on πΌ, π’ (0) = 0, π’ (π) = π’ (π) = π’ (1) , (13) (16) Μ where β(π‘) ∈ πΉ(π‘, π’(π‘), π’(π‘)) a.e. on πΌ. Assume that π : πΏ1 (πΌ, Rπ ) → πΆ1 (πΌ, Rπ ) is a function such that, for each β ∈ πΏ1 (πΌ, Rπ ), π(β) ∈ π1,2 (πΌ, Rπ ) is the unique solution of the second-order differential equation π’Μ (π‘) = β (π‘) , a.e. on πΌ, π’ (0) = 0, π’ (π) = π’ (π) = π’ (1) . (πβ ) 4 Abstract and Applied Analysis Let S = {π’ ∈ πΏ1 (πΌ, Rπ ) : β π’(π‘) β≤ π1 (π‘) a.e. on πΌ}. It is easy to see that π(S) is convex. Let (π’π )π∈N be a sequence in π(S). Hence, π’π ∈ π2,1 (πΌ, Rπ ) with π’π (0) = π₯0 , π’π (π) = π’π (π) = π’π (17) and π‘ π’π (π‘) = π₯0 + ∫ (π‘ − π) π’Μπ (π) ππ π for each V ∈ π(S). Define a multifunction π : π(S) → 1 π 2πΏ (πΌ,R ) by π (π’) = {π ∈ πΏ1 (πΌ, Rπ ) : π (π‘) ∈ πΉ(π‘, π’ (π‘) , π’Μ (π‘)) a.e. on πΌ} . (22) 0 π π‘ (π − π) (π‘ + 1) π’Μπ (π) ππ −∫ π−π 0 π π‘ (π − π) + (π − π) +∫ π’Μπ (π) ππ π−π 0 1 +∫ π (17) 1−π π’Μ (π) ππ. 1−π π lim π π→∞ π Then, 1 lim π’π (π‘) = ∫ πΊ (π‘, π) π’Μ (π) ππ = π’ (π‘) , π→∞ Assume that π = Rπ × Rπ and set a multifunction π : πΌ × Rπ π → 2 such that π(π‘, (π₯, π¦)) = πΉ(π‘, π₯, π¦). From Theorem 3.1 in [23], π has SD-property. π has nonempty convex values. Let (ππ )π∈N be a sequence in π (π’) for some π’ ∈ π(S). So, for each π‘ ∈ πΌ, 0 (18) which means that π(S) is a compact subset of πΆ1 (πΌ, Rπ ). Set Pπ (π‘) = {π₯ ∈ πΉ (π‘, V (π‘) , VΜ (π‘)) : ββ (π‘) − π₯β < π + π (β (π‘) , πΉ (π‘, V (π‘) , VΜ (π‘)))} , (19) where π > 0 and V ∈ π(S). Hence, for each π‘ ∈ πΌ, Pπ (π‘) =ΜΈ 0. Assume that B(πΌ) and B(Rπ ) are the Borel π-fields of πΌ and Rπ , respectively. From condition, (π) the function Μ Μ π‘ → πΉ(π‘, V(π‘), V(π‘)) is measurable. Hence, πππΉ(⋅, V(⋅), V(⋅)) ∈ Μ B(πΌ) × B(Rπ ) and (π‘, π₯) → ππ(β(π‘), πΉ(π‘, V(π‘), V(π‘)))− β β(π‘) − π₯ β is measurable in π‘ and continuous in π₯ that is jointly measurable. Thus, by Aumann’s selection theorem, there exists a measurable selection π π of Pπ such that π π (π‘) ∈ Pπ (π‘) for each π‘ ∈ πΌ. Now we define a multifunction Qπ : 1 π π(S) → 2πΏ (πΌ,R ) by the following: Qπ (V) σ΅© σ΅©σ΅© σ΅©σ΅©π’π (π‘) − π’ (π‘)σ΅©σ΅©σ΅© 1σ΅© σ΅©σ΅© π‘ ≤ ∫ σ΅©σ΅©σ΅©[∫ (π‘ − π) (ππ (π) − β (π)) ππ σ΅© 0 0 σ΅© π −∫ 0 ≤ π + πΌ1 (π‘) βπ’ (π‘) − V (π‘)β + πΌ2 (π‘) βπ’Μ (π‘) − VΜ (π‘)β π‘ (π − π) (π‘ + 1) (ππ (π) − β (π)) ππ π−π π π‘ (π − π) + (π − π) (ππ (π) − β (π)) ππ π−π 0 σ΅©σ΅© 1 1−π σ΅© +∫ (ππ (π) − β (π)) ππ]σ΅©σ΅©σ΅©σ΅© ππ σ΅©σ΅© π 1−π ββ (π‘) − π₯β < π + π (β (π‘) , πΉ (π‘, V (π‘) , VΜ (π‘))) a.e. on πΌ} , (20) σ΅© σ΅©σ΅© σ΅©σ΅©β (π‘) − ππ (V) (π‘)σ΅©σ΅©σ΅© ≤ π + π (β (π‘) , πΉ (π‘, V (π‘) , VΜ (π‘))) (23) 1 because πΉ has closed values in Rπ . Therefore, π ∈ πΏπΉ(⋅,π’(⋅), Μ π’(⋅)) π which implies that π (⋅) has compact values in R . We can apply Theorem 2 to find a continuous function π : π(S) → πΏ1π€ (πΌ, Rπ ) such that π(π’) ∈ ext(π (π’)), for all π’ ∈ π(S). We Μ see that π(π’)(π‘) ∈ ext(π(π‘, (π’(π‘), π’(π‘)))) [24], hence π(π’)(π‘) ∈ Μ extπΉ(π‘, π’(π‘), π’(π‘)) a.e. on πΌ. Assume that π : π(S) → π1,2 (πΌ, Rπ ) is the function which for each π’ ∈ π(S), π(π’) = π(π(π’)). For each π’ ∈ π(S), we have β π(π’)(π‘) β≤ π1 and so π(π’) ∈ S. Then, π is a function from π(S) into π(S) and also we see that π is continuous [19]. Now let ππ → 0, πππ = ππ and ππ = πππ . Then, for each π ∈ N, the function ππππ is a continuous function from the compact set π(S) into itself. From Schauder’s fixed point theorem, ππππ has a fixed point 1 1 π’π , but extπΏπΉ(⋅,V(⋅), = πΏextπΉ(⋅,V(⋅), [24] so π’π ∈ Δ ππ . By Μ Μ V(⋅)) V(⋅)) passing to a subsequence if necessary, we may assume that π’π → π’Μ in πΆ1 (πΌ, Rπ ). Then, we obtain 1 : = {π₯ ∈ πΏπΉ(⋅,V(⋅), Μ V(⋅)) with Qπ (V)(π‘) =ΜΈ 0 for each V ∈ π(S). From [22, Proposition 4], Qπ is π. π . π. and clearly has decomposable values. Applying [22, Theorem 3], we have a continuous selection ππ of Qπ . Therefore, (π‘) = π (π‘) ∈ πΉ (π‘, π’ (π‘) , π’Μ (π‘)) +∫ 1 π‘ 0 0 σ΅© σ΅© ≤ ∫ [∫ (π‘ − π) σ΅©σ΅©σ΅©ππ (π) − ππ (π)σ΅©σ΅©σ΅© ππ π‘ σ΅© σ΅© + ∫ (π‘ − π) σ΅©σ΅©σ΅©β (π) − ππ (π)σ΅©σ΅©σ΅© ππ 0 a.e. on πΌ. (21) +∫ From Theorem 2, we find a continuous function ππ : π(S) → 1 and β ππ (V)−ππ (V) β< πΏ1π€ (πΌ, Rπ ) such that ππ (V) ∈ extπΏπΉ(⋅,V(⋅), Μ V(⋅)) +∫ π 0 π 0 π‘ (π − π) (π‘ + 1) (ππ (π) − ππ (π)) ππ π−π π‘ (π − π) (π‘ + 1) σ΅©σ΅© σ΅© σ΅©σ΅©β (π) − ππ (π)σ΅©σ΅©σ΅© ππ π−π Abstract and Applied Analysis +∫ 1 π +∫ 1 π 5 1 − π σ΅©σ΅© σ΅© σ΅©π (π) − ππ (π)σ΅©σ΅©σ΅© ππ 1−πσ΅© π +∫ π 0 1 − π σ΅©σ΅© σ΅© σ΅©β (π) − ππ (π)σ΅©σ΅©σ΅© ππ] ππ . 1−πσ΅© (24) +∫ 1 π But ππ −ππ → 0 with respect to the norm β ⋅βπ€ from Lemma 3 we get ππ − ππ → 0 weakly in πΏ1 (πΌ, Rπ ). So we have π‘ (π − π) (π‘ + 1) (πΌ1 (π) βπ’ (π) − π’Μ (π)β π−π σ΅© σ΅© ΜΜ (π)σ΅©σ΅©σ΅©σ΅©) ππ +πΌ2 (π) σ΅©σ΅©σ΅©σ΅©π’Μ (π) − π’ 1−π (πΌ (π) βπ’ (π) − π’Μ (π)β 1−π 1 σ΅© σ΅© ΜΜ (π)σ΅©σ΅©σ΅©σ΅©) ππ] ππ +πΌ2 (π) σ΅©σ΅©σ΅©σ΅©π’Μ (π) − π’ π‘ ≤ βπ’− π’ΜβπΆ1 (πΌ,Rπ ) (∫ (π‘−π) (πΌ1 (π)+πΌ2 (π)) ππ 0 π‘ σ΅© σ΅© ∫ (π‘ − π) σ΅©σ΅©σ΅©ππ (π) − ππ (π)σ΅©σ΅©σ΅© ππ π π‘ (π−π) (π‘+1) +∫ 0 +∫ π 0 +∫ 1 π π‘ (π − π) (π‘ + 1) σ΅©σ΅© σ΅© σ΅©σ΅©ππ (π) − ππ (π)σ΅©σ΅©σ΅© ππ π−π (25) π‘ 0 0 1 +∫ π 1 − π σ΅©σ΅© σ΅© σ΅©π (π) − ππ (π)σ΅©σ΅©σ΅© ππ σ³¨→ 0. 1−πσ΅© π (πΌ1 (π)+πΌ2 (π)) ππ 1−π (πΌ (π) + πΌ2 (π)) ππ) 1−π 1 1 = βπ’− π’ΜβπΆ1 (πΌ,Rπ ) ∫ |πΊ (π‘, π)| (πΌ1 (π)+πΌ2 (π)) ππ 0 σ΅© σ΅© ≤ 2βπ’ − π’ΜβπΆ1 (πΌ,Rπ ) σ΅©σ΅©σ΅©πΌ1 (π) + πΌ2 (π)σ΅©σ΅©σ΅© . Moreover, 1 π−π 0 (27) Since by assumption (ii), β πΌ1 + πΌ2 β< 1/2 we get π’ = π’Μ. So π’π → π’ in πΆ1 (πΌ, Rπ ) and π’ ∈ Δππ where the closure is taken in πΆ1 (πΌ, Rπ ) which means that Δ π ⊆ Δππ . Therefore, the proof is complete if we show that Δ π is closed. Indeed if Vπ ∈ Δ π and Vπ → V in πΆ1 (πΌ, Rπ ), then Vπ = π(π¦π ) for 1 π¦π ∈ πΏπΉ(⋅,V(⋅), Μ . From assumption (iii) and the DunfordV(⋅)) Pettis theorem, {π¦π }π∈N is weakly sequentially compact in πΏ1 (πΌ, Rπ ). So we can say that {π¦π }π∈N in πΏ1 (πΌ, Rπ ). By [25, Theorem 3.1], we get σ΅© σ΅© ∫ [∫ (π‘ − π) σ΅©σ΅©σ΅©β (π) − ππ (π)σ΅©σ΅©σ΅© ππ π +∫ 0 +∫ 1 π 1 π‘ 0 0 π‘ (π − π) (π‘ + 1) (ππ (π) − ππ (π)) ππ π−π 1 − π σ΅©σ΅© σ΅© σ΅©β (π) − ππ (π)σ΅©σ΅©σ΅© ππ] ππ 1−πσ΅© σ΅© σ΅© ≤ ∫ [∫ (π‘ − π) (ππ + πΌ1 (π) σ΅©σ΅©σ΅©π’ (π) − π’π (π)σ΅©σ΅©σ΅© σ΅© σ΅© +πΌ2 (π) σ΅©σ΅©σ΅©π’Μ (π) − π’Μπ (π)σ΅©σ΅©σ΅©) π +∫ 0 π¦ (π‘) ∈ conv lim{π¦π (π‘)}π∈N ⊆ conv lim πΉ (π‘, Vπ (π‘) , VΜπ (π‘)) π‘ (π − π) (π‘ + 1) σ΅© σ΅© (ππ + πΌ1 (π) σ΅©σ΅©σ΅©π’ (π) − π’π (π)σ΅©σ΅©σ΅© π−π σ΅© σ΅© +πΌ2 (π) σ΅©σ΅©σ΅©π’Μ (π) − π’Μπ (π)σ΅©σ΅©σ΅©) 1 1−π σ΅© σ΅© +∫ (ππ + πΌ1 (π) σ΅©σ΅©σ΅©π’ (π) − π’π (π)σ΅©σ΅©σ΅© π 1−π σ΅© σ΅© +πΌ2 (π) σ΅©σ΅©σ΅©π’Μ (π) − π’Μπ (π)σ΅©σ΅©σ΅©)] ππ . = πΉ (π‘, V (π‘) , VΜ (π‘)) a.e. on πΌ. (28) Moreover, π(π¦π ) → π(π¦) in πΏ1 (πΌ, Rπ ) for π¦ ∈ πΏ1 (πΌ, Rπ ) Μ and π¦(π‘) ∈ πΉ(π‘, V(π‘), V(π‘)) a.e. on πΌ. Hence, V ∈ Δ π ; that is Δ π is closed in πΆ1 (πΌ, Rπ ). (26) Now we consider the following assumptions: As π → ∞, we have (π΄ 1 ) π½ ∈ (0, π/2), ππ > 0 and ∑π−2 π=1 ππ < 1; π’ (π‘) − π’ (π‘)β βΜ 1 π‘ 0 0 ≤ ∫ [∫ (π‘ − π) (πΌ1 (π) βπ’ (π) − π’Μ (π)β σ΅© σ΅© ΜΜ (π)σ΅©σ΅©σ΅©σ΅©) ππ +πΌ2 (π) σ΅©σ΅©σ΅©σ΅©π’Μ (π) − π’ π−2 (π΄ 2 ) ∑π−2 π=1 ππ cos π½ππ − cos π½ > 0 and πΎπ = 1/ ∑π=1 ππ cos π½ππ − cos π½; (π΄ 3 ) πΆ0 = (sin π½/π½)(1 + πΎπ ) and πΆ1 = min{πΎπ + 1, πΎπ sin2 π½}; 6 Abstract and Applied Analysis Μ = 0, π’(1) = ∑π−2 (π΄ 4 ) π = {π’ ∈ πΆ2 (πΌ, Rπ ) : π’(0) π=1 ππ π’(ππ )}; Proof. (ii) Since πG (π‘, π ) ππ‘ (π΄ 5 ) G : πΌ × πΌ → R is defined by cos π½ (π‘ − π ) ={ 0 G (π‘, π ) 1 { sin π½ (π‘ − π ) = {π½ {0 if 0 ≤ π ≤ π‘ ≤ 1 if 0 ≤ π ≤ π‘ ≤ 1 if 0 ≤ π‘ ≤ π ≤ 1 π−2 if 0 ≤ π‘ ≤ π ≤ 1 π−2 { { sin π½ (1 − π ) − ∑ ππ sin π½ (ππ − π ) , { { { π=1 { { { { { if 0 ≤ π ≤ π1 , { { { { { π−2 { { { { sin π½ − π ) − ∑ ππ sin π½ (ππ − π ) , (1 { { { { π=2 { { { { < π ≤ π2 , if π { 1 { { { { π−2 { { { { sin π½ (1 − π ) − ∑ ππ sin π½ (ππ − π ) , { { { { π=3 { πΎπ + cos π½π‘ { if π < π ≤ π3 , 2 { π½ { { { { .. { { { . { { { π−2 { { { { sin π½ − π ) − ∑ ππ sin π½ (ππ − π ) , (1 { { { { π=π { { { { if π < π ≤ ππ , { π−1 { { { { { .. { { . { { { { {sin π½ (1 − π ) , { { { { if ππ−2 < π ≤ 1. { (29) { { sin π½ (1−π )− ∑ππ sin π½ (ππ − π ), { { { π=1 { { { { { if 0 ≤ π ≤ π1 , { { { { { π−2 { { { { sin π½ ∑ππ sin π½ (ππ − π ), (1−π )− { { { { π=2 { { { { < π ≤ π2 , if π { 1 { { { { π−2 { { {sin π½ (1−π )− ∑π sin π½ (π − π ), { { π π { { { π=3 { − πΎπ sin π½π‘ { if π2 < π ≤ π3 , { { { { . { { .. { { { { { π−2 { { { { sin π½ ∑ππ sin π½ (ππ − π ), (1−π )− { { { { π=π { { { { < π ≤ ππ , if π { π−1 { { { { { .. { { . { { { { { sin π½ (1 − π ) , { { { { if ππ−2 < π ≤ 1, { (31) then supπ‘,π ∈πΌ πG(π‘, π )/ππ‘ ≤ 1 + πΎπ . Furthermore, πG (π‘, π ) ππ‘ π−2 ≥ πΎπ sin π½π‘ [ ∑ ππ sin (ππ − π ) − sin π½ (1 − π½)] (32) π=1 Lemma 6 (see [26]). If the assumptions (π΄ 1 )–(π΄ 5 ) hold, then Theorem 7. Assume that the assumptions (π΄ 1 ) and (π΄ 2 ) hold. Let πΉ be a multifunction from πΌ × Rπ × Rπ to πππ (Rπ ) satisfying the following conditions: (ii) supπ‘,π ∈πΌ |πG(π‘, π )/ππ‘| ≤ πΆ1 , (iii) for each π₯ ∈ πΆ1 (πΌ, Rπ ) there exists a unique function π’π₯ ∈ π such that 1 0 1 1 ≥ −πΎπ sin π½ and thus supπ‘,π ∈πΌ |πG(π‘, π )/ππ‘| ≤ πΆ1 . (i) 0 ≤ G(π‘, π ) ≤ πΆ0 for all (π‘, π ) ∈ πΌ × πΌ, π’π₯ (π‘) = ∫ G (π‘, π ) π₯ (π ) ππ , 2 (30) (iv) (∫0 |G(π‘, π )|π ππ )1/π ≤ πΆ0 and (∫0 |(πG/ππ‘)(π‘, π )|π ππ )1/π ≤ πΆ1 . (a) for each (π₯, π¦) ∈ R × R, the multifunction πΉ(⋅, π₯, π¦) is measurable; (b) for each π‘ ∈ πΌ, the function (π₯, π¦) → πΉ(π‘, π₯, π¦) is continuous with respect to the Hausdorff metric ππ»; (c) for each (π‘, π₯, π¦) ∈ πΌ × Rπ × Rπ σ΅©σ΅©σ΅©πΉ (π‘, π₯, π¦)σ΅©σ΅©σ΅© ≤ sup {βVβ : V ∈ πΉ (π‘, π₯, π¦)} σ΅© σ΅© (33) σ΅© σ΅© ≤ π (π‘) + π1 (π‘) βπ₯β + π2 (π‘) σ΅©σ΅©σ΅©π¦σ΅©σ΅©σ΅© ; (d) the spectral radius π(πΏ) of πΏ is less than one. Then Problem (ππ ) admits a solution in π. Abstract and Applied Analysis 7 Proof. We can say that β πΉ(π‘, π₯, π¦) β≤ π1 (π‘) a.e. on πΌ for some π1 ∈ πΏπ (πΌ, R+ ) [9]. Let π₯ ∈ πΆ1 (πΌ, Rπ ) and let π’ ∈ πΆ2 (πΌ, Rπ ) be the unique solution of the problem π’Μ (π‘) = π₯ (π‘) , π’Μ (0) = 0, π’Μ (π‘) = β (π‘) , a.e. on πΌ, π−2 π’ (1) = ∑ ππ π’ (ππ ) . 1 From Lemma 6, we have π’(π‘) = ∫0 G(π‘, π )π₯(π )ππ , ∀π‘ ∈ πΌ. Thus, we define a function π : πΆ1 (πΌ, Rπ ) → πΆ2 (πΌ, Rπ ) such that π(π₯) is the unique solution of (∗). Let a.e. on πΌ, (πβ ) π−2 π’Μ (0) = 0, (∗) π=1 1 β ∈ πΆ1 (πΌ, Rπ ), πσΈ (β) ∈ πΆ2 (πΌ, Rπ ) is the unique solution of the second-order differential equation π’ (1) = ∑ ππ π’ (ππ ) . π=1 Let π = {π’ ∈ πΆ1 (πΌ, Rπ ) :β π’(π‘) β≤ π1 (π‘) a.e. on πΌ}. So πσΈ (π) is convex. Let (π’π )π∈N be a sequence in πσΈ (π). Hence, π’π ∈ πΆ2 (πΌ, Rπ ) with π’π (0) = 0, π’Μπ (0) = 0, π’π (1) = ∑π−2 π=1 ππ π’π (ππ ). Then from Lemma 6, 1 lim π’π (π‘) = ∫ G (π‘, π) π’Μ (π) ππ = π’ (π‘) , π V = {π₯ ∈ πΆ (πΌ, R ) : βπ₯ (π‘)β ≤ π1 (π‘) a.e. on πΌ} . π→∞ (34) From the Dunford-Pettis theorem, V is weakly compact and then π(V) is convex and compact subset of πΆ2 (πΌ, Rπ ). Let 1 π Y = Rπ × Rπ . If K = π(V), R : K → 2πΏ (πΌ,R ) and π M : πΌ × Y → 2R , where R(π’) = {π ∈ πΏ1 (πΌ, Rπ ) : π(π‘) ∈ Μ πΉ(π‘, π’(π‘), π’(π‘)) a.e. on πΌ} and M(π‘, (π₯, π¦)) = πΉ(π‘, π₯, π¦), then M has SD-property [23]. It is easy to show that R is nonempty and convex subset of πΏ1 (πΌ, Rπ ). If ππ is a sequence in R(π’) for some π’ ∈ K, then limπ → ∞ ππ (π‘) = π(π‘) ∈ Μ πΉ(π‘, π’(π‘), π’(π‘)), where the values of πΉ are closed. Therefore, the values of R are weakly compact. According to Theorem 5 there exists a continuous function π : K → πΏ1π€ (πΌ, Rπ ) with π(π’) ∈ ext(R(π’)), for all π’ ∈ K. Thus, π(π’)(π‘) ∈ Μ ext(M(π‘, π’(π‘), π’(π‘))) a.e. on πΌ [24] which implies π(π’)(π‘) ∈ Μ ext(πΉ(π‘, π’(π‘), π’(π‘))) a.e. on πΌ. If π’ ∈ π(V), then β π(π’)(π‘) β≤ π1 and so π(π’) ∈ V. Put π : π(V) → π2,1 (πΌ, Rπ ) such that π(π’) = π(π(π’)), thus π is a continuous function from π(V) into π(V) [19]. From Schauder’s fixed point theorem, there exists π₯ ∈ π(V) such that π₯ = π(π₯) = π(π(π₯)) which Μ ∈ means that there is π₯ ∈ π ⊆ πΆ2 (πΌ, Rπ ) such that π₯(π‘) Μ ext(πΉ(π‘, π₯(π‘), π₯(π‘))). Theorem 8. In the setting of Theorem 7, if one replaces condition (b) by the following condition: (b)σΈ ππ»(πΉ(π‘, π₯, π¦), πΉ(π‘, π₯σΈ , π¦σΈ )) ≤ π1 β π₯ − π₯σΈ β + π2 β π¦ − π¦σΈ β a.e. with π1 ≥ 0, π2 ≥ 0 and |π1 + π2 | < 1/2πΆ0 . Then Δ ππ is nonempty and Δ ππ = Δ π where the closure taken in πΆ2 (πΌ, Rπ ). 0 (36) hence, πσΈ (π) is a compact subset of πΆ2 (πΌ, Rπ ). Set Qπ (π‘) = {π₯ ∈ πΉ (π‘, V (π‘) , VΜ (π‘)) : ββ (π‘) − π₯β < π + π (β (π‘) , πΉ (π‘, V (π‘) , VΜ (π‘)))} , (37) where π > 0 and V ∈ πσΈ (π). Hence, for each π‘ ∈ πΌ, Qπ (π‘) =ΜΈ 0. Assume that B(πΌ) and B(Rπ ) are the Borel π-fields of πΌ and Rπ , respectively. From condition (i), the function Μ Μ π‘ → πΉ(π‘, V(π‘), V(π‘)) is measurable. Hence, πππΉ(⋅, V(⋅), V(⋅)) ∈ Μ B(πΌ) × B(Rπ ) and (π‘, π₯) → ππ(β(π‘), πΉ(π‘, V(π‘), V(π‘)))− β β(π‘) − π₯ β is measurable in π‘ and continuous in π₯ that is jointly measurable. Thus, by Aumann’s selection theorem, there exists a measurable selection π π of Qπ such that π π (π‘) ∈ Qπ (π‘) for each π‘ ∈ πΌ. Now we define a multifunction Qπ : 1 π πσΈ (π) → 2πΆ (πΌ,R ) by the following: 1 Qπ (V) = {π₯ ∈ πΏπΉ(⋅,V(⋅), : ββ (π‘) − π₯β Μ V(⋅)) < π + π (β (π‘) , πΉ (π‘, V (π‘) , VΜ (π‘))) a.e. on πΌ} , (38) with Qπ (V)(π‘) =ΜΈ 0 for each V ∈ πσΈ (π). From [22, Proposition 4], Qπ is π. π . π. and clearly has decomposable values. Applying [22, Theorem 3], we have a continuous selection ππ of Qπ . Therefore, σ΅© σ΅©σ΅© σ΅©σ΅©β (π‘) − ππ (V) (π‘)σ΅©σ΅©σ΅© ≤ π + π (β (π‘) , πΉ (π‘, V (π‘) , VΜ (π‘))) ≤ π + π1 (π‘) βπ’ (π‘) − V (π‘)β Proof. From Theorem 7, we have Δ ππ =ΜΈ 0. Moreover, β πΉ(π‘, π₯, π¦) β≤ π1 (π‘) a.e. on πΌ for some π1 ∈ πΏπ (πΌ, R+ ). Let π’ ∈ Δ π. Then + π2 (π‘) βπ’Μ (π‘) − VΜ (π‘)β a.e. on πΌ. (39) (35) From Theorem 2, we find a continuous function ππσΈ : 1 and π (π) → πΏ1π€ (πΌ, Rπ ) such that ππσΈ (V) ∈ ext πΏπΉ(⋅,V(⋅), Μ V(⋅)) σΈ σΈ β ππ (V) − ππ (V) β< π for each V ∈ π (π). Define a multifunction 1 π π σΈ : πσΈ (π) → 2πΆ (πΌ,R ) by Μ where β(π‘) ∈ πΉ(π‘, π’(π‘), π’(π‘)) a.e. on πΌ. Assume that πσΈ : πΆ1 (πΌ, Rπ ) → πΆ2 (πΌ, Rπ ) is a function such that, for each π σΈ (π’) = {π ∈ πΆ1 (πΌ, Rπ ) : π (π‘) ∈ πΉ (π‘, π’ (π‘) , π’Μ (π‘)) a.e. on πΌ} . (40) π’Μ (π‘) = β (π‘) , π’Μ (0) = 0, a.e. on πΌ, π−2 π’ (1) = ∑ ππ π’ (ππ ) , σΈ π=1 8 Abstract and Applied Analysis As in Theorem 5, let π = Rπ × Rπ and set a multifunction Rπ π : πΌ×π → 2 such that π(π‘, (π₯, π¦)) = πΉ(π‘, π₯, π¦). From [23, Theorem 3.1], π has SD-property. π σΈ has nonempty convex values. Let (ππ )π∈N be a sequence in π σΈ (π’) for some π’ ∈ πσΈ (π). So, for each π‘ ∈ πΌ, lim π (π‘) = π (π‘) ∈ πΉ (π‘, π’ (π‘) , π’Μ (π‘)) (41) π→∞ π 1 because πΉ has closed values in Rπ . Therefore, π ∈ πΏπΉ(⋅,π’(⋅), Μ π’(⋅)) σΈ π which implies π (⋅) has compact values in R . We can apply Theorem 2 to find a continuous function πσΈ : πσΈ (π) → πΏ1π€ (πΌ, Rπ ) such that πσΈ (π’) ∈ ext(π σΈ (π’)), for all π’ ∈ πσΈ (π). Μ We see that πσΈ (π’)(π‘) ∈ ext(π(π‘, (π’(π‘), π’(π‘)))) [24], hence Μ a.e. on πΌ. Assume that πσΈ : πσΈ (π’)(π‘) ∈ extπΉ(π‘, π’(π‘), π’(π‘)) πσΈ (π) → πΆ2 (πΌ, Rπ ) is the function which for each π’ ∈ πσΈ (π), πσΈ (π’) = π(πσΈ (π’)). For each π’ ∈ πσΈ (π), we have β πσΈ (π’)(π‘) β≤ π1 and so πσΈ (π’) ∈ π. Then, πσΈ is a function from πσΈ (π) into πσΈ (π) and also we see that πσΈ is continuous [19]. Now let ππ → 0, πππ = ππ and ππσΈ = ππσΈ π . Then, for each π ∈ N, the function πσΈ πππσΈ is a continuous function from the compact set πσΈ (π) into itself. From Schauder’s fixed point theorem, ππππσΈ has 1 1 = πΏextπΉ(⋅,V(⋅), [24] so a fixed point π’π , but ext πΏπΉ(⋅,V(⋅), Μ Μ V(⋅)) V(⋅)) 2 π’π ∈ Δ ππ . Assume that π’π → π’Μ in πΆ (πΌ, Rπ ). From Lemma 6, we obtain 1 1 σ΅© σΈ σ΅© σ΅© σ΅©σ΅© σ΅©σ΅©π’π (π‘) − π’ (π‘)σ΅©σ΅©σ΅© ≤ ∫ [∫ |G (π‘, π)| σ΅©σ΅©σ΅©σ΅©π π (π) − ππ (π)σ΅©σ΅©σ΅©σ΅© ππ 0 0 1 σ΅© σ΅© + ∫ |G (π‘, π)| σ΅©σ΅©σ΅©(ππ (π) − β (π))σ΅©σ΅©σ΅© ππ] ππ . 0 (42) ππσΈ But − ππ → 0 with respect to the norm β ⋅βπ€ and from Lemma 3 we get ππσΈ − ππ → 0 weakly in πΆ1 (πΌ, Rπ ). So we have 1 σ΅© σ΅© ∫ |G (π‘, π)| σ΅©σ΅©σ΅©σ΅©ππσΈ (π) − ππ (π)σ΅©σ΅©σ΅©σ΅© ππ σ³¨→ 0. 0 (43) Moreover, as π → ∞ we have 1 π’ (π‘)−π’ (π‘)β ≤ βπ’ − π’ΜβπΆ1 (πΌ,Rπ ) ∫ |G (π‘, π)| (π1 (π)+π2 (π)) ππ βΜ 0 σ΅© σ΅© ≤ βπ’ − π’ΜβπΆ1 (πΌ,Rπ ) σ΅©σ΅©σ΅©π1 (π) + π2 (π)σ΅©σ΅©σ΅© πΆ0 . (44) Since by assumption (ii), β π1 + π2 β < 1/2πΆ0 , thus from Lemma 6, we get π’ = π’Μ. So π’π → π’ in πΆ2 (πΌ, Rπ ) and π’ ∈ Δππ where the closure is taken in πΆ2 (πΌ, Rπ ) which means that Δ π ⊆ Δππ . If Vπ ∈ Δ π and Vπ → V in πΆ2 (πΌ, Rπ ), then Vπ = πσΈ (π¦π ) for π¦π ∈ πΏπΉ1 σΈ (⋅,V(⋅),V(⋅)) Μ . From assumption (iii) and the Dunford-Pettis theorem, {π¦π }π∈N is weakly sequentially compact in πΆ2 (πΌ, Rπ ). By [25, Theorem 3.1], we get π¦ (π‘) ∈ conv lim{π¦π (π‘)}π∈N ⊆ conv lim πΉ (π‘, Vπ (π‘) , VΜπ (π‘)) = πΉ (π‘, V (π‘) , VΜ (π‘)) a.e. on πΌ. (45) Moreover, πσΈ (π¦π ) → πσΈ (π¦) in πΆ2 (πΌ, Rπ ) for π¦ ∈ πΆ2 (πΌ, Rπ ) Μ and π¦(π‘) ∈ πΉ(π‘, V(π‘), V(π‘)) a.e. on πΌ. Hence, V ∈ Δ π; that is, Δ π 2 π is closed in πΆ (πΌ, R ). Acknowledgments The author is deeply indebted and thankful to the deanship of the scientific research and his helpful and distinct team of employees at Taibah University, Al-Madinah Al-Munawarah, Saudia Arabia. This research work was supported by a Grant no. 3029/1434. References [1] A. M. Gomaa, Set-valued functions and set-valued differential equations [Ph.D. thesis], Faculty of Science, Cairo University, 1999. [2] A. G. Ibrahim and A. M. Gomaa, “Existence theorems for a functional multivalued three-point boundary value problem of second order,” Journal of the Egyptian Mathematical Society, vol. 8, no. 2, pp. 155–168, 2000. [3] A. G. Ibrahim and A. G. Gomaa, “Extremal solutions of classes of multivalued differential equations,” Applied Mathematics and Computation, vol. 136, no. 2-3, pp. 297–314, 2003. [4] A. M. Gomaa, “On the solution sets of three-point boundary value problems for nonconvex differential inclusions,” Journal of the Egyptian Mathematical Society, vol. 12, no. 2, pp. 97–107, 2004. [5] D. L. Azzam, C. Castaing, and L. Thibault, “Three boundary value problems for second order differential inclusions in Banach spaces,” Control and Cybernetics, vol. 31, no. 3, pp. 659– 693, 2002. [6] B. Satco, “Second order three boundary value problem in Banach spaces via Henstock and Henstock-Kurzweil-Pettis integral,” Journal of Mathematical Analysis and Applications, vol. 332, no. 2, pp. 919–933, 2007. [7] P. Hartman, Ordinary Differential Equations, John Wiley and Sons, New York, NY, USA, 1964. [8] A. M. Gomaa, “On the solution sets of four-point boundary value problems for nonconvex differential inclusions,” International Journal of Geometric Methods in Modern Physics, vol. 8, no. 1, pp. 23–37, 2011. [9] A. M. Gomaa, “On four-point boundary value problems for differential inclusions and differential equations with and without multivalued moving constraints,” Czechoslovak Mathematical Journal, vol. 62, no. 137, pp. 139–154, 2012. [10] C. J. Himmelberg and F. S. Van Vleck, “Selection and implicit function theorems for multifunctions with Souslin graph,” Bulletin de l’AcadeΜmie Polonaise des Sciences, vol. 19, pp. 911–916, 1971. [11] C. J. Himmelberg and F. S. Van Vleck, “Some selection theorems for measurable functions,” Canadian Journal of Mathematics, vol. 21, pp. 394–399, 1969. [12] C. J. Himmelberg and F. S. Van Vleck, “Extreme points of multifunctions,” Indiana University Mathematics Journal, vol. 22, pp. 719–729, 1973. [13] K. Kuratowski and C. Ryll-Nardzewski, “A general theorem on selectors,” Bulletin de l’AcadeΜmie Polonaise des Sciences, vol. 13, pp. 397–403, 1965. [14] E. Klein and A. C. Thompson, Theory of Correspondences, John Wiley and Sons, New York, NY, USA, 1984. [15] C. Castaing and M. Valadier, Convex Analysis and Measurable Multifunctions, vol. 580 of Lecture Notes in Mathematics, Springer, Berlin, Germany, 1977. Abstract and Applied Analysis [16] J.-P. Aubin and A. Cellina, Differential Inclusions Set-Valued Maps and Viability Theory, vol. 264, Springer, Berlin, Germany, 1984. [17] F. S. De Blasi and J. Myjak, “On continuous approximations for multifunctions,” Pacific Journal of Mathematics, vol. 123, no. 1, pp. 9–31, 1986. [18] A. A. Tolstonogov, “Extremal selectors of multivalued mappings and the “bang-bang” principle for evolution inclusions,” Bulletin de l’AcadeΜmie Polonaise des Sciences, SeΜrie des Sciences MatheΜmatiques, vol. 317, no. 3, pp. 589–593, 1991. [19] D. Kravvaritis and N. S. Papageorgiou, “Boundary value problems for nonconvex differential inclusions,” Journal of Mathematical Analysis and Applications, vol. 185, no. 1, pp. 146–160, 1994. [20] S. R. Bernfeld and V. Lakshmikantham, An Introduction to Nonlinear Boundary Value, Academic Press, New York, NY, USA, 1974. [21] A. G. Ibrahim and A. M. Gomaa, “Topological properties of the solution sets of some differential inclusions,” Pure Mathematics and Applications, vol. 10, no. 2, pp. 197–223, 1999. [22] A. Bressan and G. Colombo, “Extensions and selections of maps with decomposable values,” Studia Mathematica, vol. 90, no. 1, pp. 69–86, 1988. [23] N. S. Papageorgiou, “On measurable multifunctions with applications to random multivalued equations,” Mathematica Japonica, vol. 32, no. 3, pp. 437–464, 1987. [24] M. Benamara, Point ExtreΜmaux, Multi-applications et Fonctionelles InteΜgrales [M.S. thesis], UniversiteΜ de Grenoble, 1975. [25] N. S. Papageorgiou, “Convergence theorems for Banach space valued integrable multifunctions,” International Journal of Mathematics and Mathematical Sciences, vol. 10, no. 3, pp. 433– 442, 1987. [26] L. X. Truong, L. T. P. Ngoc, and N. T. Long, “Positive solutions for an π-point boundary-value problem,” Electronic Journal of Differential Equations, vol. 2008, no. 111, 10 pages, 2008. 9 Advances in Operations Research Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Advances in Decision Sciences Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Mathematical Problems in Engineering Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Journal of Algebra Hindawi Publishing Corporation http://www.hindawi.com Probability and Statistics Volume 2014 The Scientific World Journal Hindawi Publishing Corporation http://www.hindawi.com Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 International Journal of Differential Equations Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Volume 2014 Submit your manuscripts at http://www.hindawi.com International Journal of Advances in Combinatorics Hindawi Publishing Corporation http://www.hindawi.com Mathematical Physics Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Journal of Complex Analysis Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 International Journal of Mathematics and Mathematical Sciences Journal of Hindawi Publishing Corporation http://www.hindawi.com Stochastic Analysis Abstract and Applied Analysis Hindawi Publishing Corporation http://www.hindawi.com Hindawi Publishing Corporation http://www.hindawi.com International Journal of Mathematics Volume 2014 Volume 2014 Discrete Dynamics in Nature and Society Volume 2014 Volume 2014 Journal of Journal of Discrete Mathematics Journal of Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Applied Mathematics Journal of Function Spaces Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Optimization Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014