Research Article Relaxation Problems Involving Second-Order Differential Inclusions Adel Mahmoud Gomaa

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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,
̈ ∈ 𝐹(𝑑, 𝑒(𝑑), 𝑒(𝑑))
Μ‡
̈ ∈ 𝐹(𝑑, 𝑒(𝑑), 𝑒(𝑑))
Μ‡
𝑒(𝑑)
a.e. on [0, 1]; 𝑒(0) = 0, 𝑒(πœ‚) = 𝑒(πœƒ) = 𝑒(1) and, with π‘š ≥ 3 boundary conditions, 𝑒(𝑑)
a.e. on
Μ‡ = 0, 𝑒(1) = ∑π‘š−2
π‘Ž
𝑒(πœ‰
),
where
0
<
πœ‚
<
πœƒ
<
1,
0
<
πœ‰
<
πœ‰
<
⋅
⋅
⋅
<
πœ‰
<
1
and
𝐹
is
a
multifunction
from
[0,
1]
×
R𝑛 ×
[0, 1]; 𝑒(0)
𝑖
𝑖
1
2
π‘š−2
𝑖=1
𝑛
𝑛
R to the nonempty compact convex subsets of R . We have results that improve earlier theorems.
and, with π‘š ≥ 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‘’Μˆ (𝑑) ∈ 𝐹 (𝑑, 𝑒 (𝑑) , 𝑒̇ (𝑑)) ,
𝑒 (0) = π‘₯0 ,
a.e. on [0, 𝑇] ,
𝑒 (πœ‚) = 𝑒 (πœƒ) = 𝑒 (𝑇) ,
(1)
where 0 < πœ‚ < πœƒ < 𝑇 and 𝐹 is a multifunction from [0, 𝑇] ×
R𝑛 × R𝑛 to the nonempty compact subsets of R𝑛 , 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‘’Μˆ (𝑑) ∈ 𝐹 (𝑑, 𝑒 (𝑑) , 𝑒̇ (𝑑)) ,
𝑒̇ (0) = 0,
a.e. on [0, 1] ,
π‘š−2
𝑒 (1) = ∑ π‘Žπ‘– 𝑒 (πœ‰π‘– ) ,
(𝑄)
𝑖=1
where 0 < πœ‚ < πœƒ < 1, 0 < πœ‰1 < πœ‰2 < ⋅ ⋅ ⋅ < πœ‰π‘š−2 < 1, and
𝐹 is a multifunction from [0, 1] × R𝑛 × R𝑛 to the non-empty
compact subsets of R𝑛 .
In conjunction with Problem (𝑃) and Problem (𝑄) we also
consider the following problems:
π‘’Μˆ (𝑑) ∈ ext 𝐹 (𝑑, 𝑒 (𝑑) , 𝑒̇ (𝑑)) ,
𝑒 (0) = 0,
𝑒 (πœ‚) = 𝑒 (πœƒ) = 𝑒 (1) ,
π‘’Μˆ (𝑑) ∈ ext 𝐹 (𝑑, 𝑒 (𝑑) , 𝑒̇ (𝑑)) ,
𝑒̇ (0) = 0,
a.e. on [0, 1] ,
π‘š−2
(𝑃𝑒 )
a.e. on [0, 1] ,
𝑒 (1) = ∑ π‘Žπ‘– 𝑒 (πœ‰π‘– ) .
(𝑄𝑒 )
𝑖=1
π‘’Μˆ (𝑑) ∈ 𝐹 (𝑑, 𝑒 (𝑑) , 𝑒̇ (𝑑)) ,
𝑒 (0) = 0,
a.e. on [0, 1] ,
𝑒 (πœ‚) = 𝑒 (πœƒ) = 𝑒 (1)
(𝑃)
Μ‡
By ext 𝐹(𝑑, 𝑒(𝑑), 𝑒(𝑑)),
we denote the set of extreme points of
Μ‡
𝐹(𝑑, 𝑒(𝑑), 𝑒(𝑑)).
2
Abstract and Applied Analysis
2. Notations and Preliminaries
Throughout this paper we let 𝐼 = [0, 1] and 0 < πœ‰1 <
πœ‰2 < ⋅ ⋅ ⋅ < πœ‰π‘š−2 < 1. We will use the following definitions,
notations, and summarize some results.
(i) A multifunction 𝐹 from a metric space (𝑋, 𝑑) to the set
𝑃𝑓 (π‘Œ) of all closed subsets of another metric space π‘Œ is lower
semicontinuous (l. s. c.) at π‘₯0 ∈ 𝑋 if for every open subset 𝑉
in π‘Œ with 𝐹(π‘₯0 ) ∩ 𝑉 =ΜΈ 0 there exists an open subset π‘ˆ in 𝑋
such that π‘₯0 ∈ π‘ˆ and 𝐹(π‘₯) ∩ 𝑉 =ΜΈ 0 for all π‘₯ ∈ π‘ˆ. 𝐹 is l. s. c. if
it is l. s. c. at each π‘₯0 ∈ 𝑋.
(ii) 𝐹 is upper semicontinuous (u. s. c.) at π‘₯0 ∈ 𝑋 if for
every open subset 𝑉 in π‘Œ and containing 𝐹(π‘₯0 ) there exists
an open subset π‘ˆ in 𝑋 such that π‘₯0 ∈ π‘ˆ and 𝐹(π‘₯) ⊆ 𝑉, for all
π‘₯ ∈ π‘ˆ. 𝐹 is u. s. c. if it is u. s. c. at each π‘₯0 ∈ 𝑋.
(iii) A multifunction 𝐹 from 𝐼 into the set 𝑃𝑓 (𝑋) of all
closed subsets of 𝑋 is measurable if for all π‘₯ ∈ 𝑋 the function
𝑑 → 𝑑(π‘₯, 𝐹(𝑑)) = inf{β€– π‘₯ − 𝑦 β€–: 𝑦 ∈ 𝐹(𝑑)} is measurable
[10–13].
(iv) Let (Ω, Σ) be a measurable space and 𝑋 a separable
Banach space. We say that 𝐹 : Ω → 𝑃𝑓 (𝑋) is graph measurable if
π‘”π‘Ÿ (𝐹) = {(𝑧, π‘₯) ∈ Ω × π‘‹ : π‘₯ ∈ 𝐹 (𝑧)} ∈ Σ × B (𝑋) ,
(2)
where B(𝑋) is the Borel 𝜎-field of 𝑋. For further details we
refer to [14–16].
(v) 𝐹 is continuous if it is lower and upper semicontinuous.
(vi) For each 𝐴, 𝐡 ∈ 𝑃𝑓 (𝑋), the Hausdorff metric is
defined by
𝑑𝐻 (𝐴, 𝐡) = max [sup 𝑑 (π‘Ž, 𝐡) , sup 𝑑 (𝑏, 𝐴)] .
π‘Ž∈𝐴
𝑏∈𝐡
(3)
It is known that the space (𝑃𝑓 (𝑋), 𝑑𝐻) is a generalized
metric space, if the sets are not bounded (see, for instance,
[14, 15]).
(vii) A multifunction 𝐹 is Hausdorff continuous (𝑑𝐻continuous) if it is continuous from 𝑋 into the metric space
(𝑃𝑓 (π‘Œ), 𝑑𝐻).
(viii) If 𝐹 has compact values in π‘Œ, then 𝐹 is 𝑑𝐻-continuous if and only if it is continuous [14, 17].
(ix) We denote by π‘ƒπ‘˜π‘ (R𝑛 ) the nonempty compact convex
subsets of R𝑛 .
(x) The Banach spaces 𝐢(𝐼, R𝑛 ), 𝐢1 (𝐼, R𝑛 ), and 𝐢2 (𝐼, R𝑛 )
endowed with the norms
‖𝑒‖𝐢 = max |𝑒 (𝑑)| ,
𝑑∈𝐼
‖𝑒‖𝐢1 = max {‖𝑒‖𝐢, ‖𝑒‖̇ 𝐢} ,
‖𝑒‖𝐢2 = max {‖𝑒‖𝐢, ‖𝑒‖̇ 𝐢, β€–π‘’β€–Μˆ 𝐢} ,
(4)
respectively.
(xi) 𝐿1𝑀 (𝐼, R𝑛 ) denotes the space 𝐿1 (𝐼, R𝑛 ) equipped with
weak norm β€– ⋅‖𝑀 which is defined by
σ΅„©σ΅„© 𝑏
σ΅„©σ΅„©
σ΅„©
σ΅„©
(5)
β€–β„Žβ€–π‘€ = sup {σ΅„©σ΅„©σ΅„©σ΅„©∫ β„Ž (𝑑) 𝑑𝑑󡄩󡄩󡄩󡄩 : 0 ≤ π‘Ž ≤ 𝑏 ≤ 1} .
σ΅„©σ΅„© π‘Ž
σ΅„©σ΅„©
(xii) π‘Š2,1 (𝐼, R𝑛 ) is the Sobolev space of functions 𝑒 : 𝐼 →
𝑛
̈ ∈
R , 𝑒 and 𝑒̇ are both absolutely continuous functions so 𝑒(𝑑)
𝐿1 (𝐼, R𝑛 ) and it is equipped with the norm β€–π‘’β€–π‘Š2,1 (𝐼,R𝑛 ) =
‖𝑒‖𝐿1 (𝐼,R𝑛 ) + ‖𝑒‖̇ 𝐿1 (𝐼,R𝑛 ) + β€–π‘’β€–Μˆ 𝐿1 (𝐼,R𝑛 ) .
𝑛
(xiii) Let 𝑅 : 𝐼 → 2R be a multifunction and 𝛿𝑅1 = {β„Ž ∈
𝐿1 (𝐼, R𝑛 ) : β„Ž(𝑑) ∈ 𝑅(𝑑)}.
(xiv) By a solution of (𝑃) (resp., of (𝑃𝑒 )) we mean a func̈ = β„Ž(𝑑) a.e. on 𝐼 with β„Ž ∈
tion 𝑒 ∈ π‘Š2,1 (𝐼, R𝑛 ) such that 𝑒(𝑑)
1
1
(resp.,
β„Ž
∈
𝛿
𝛿𝐹(⋅,𝑒(⋅),
Μ‡
Μ‡ ) and 𝑒(0) = 0, 𝑒(πœ‚) =
𝑒(⋅))
ext𝐹(⋅,𝑒(⋅),𝑒(⋅))
𝑒(πœƒ) = 𝑒(1).
(xv) By a solution of (𝑄) (resp., of (𝑄𝑒 )) we mean a func̈ = β„Ž(𝑑) a.e. on 𝐼 with β„Ž ∈
tion 𝑒 ∈ π‘Š2,1 (𝐼, R𝑛 ) such that 𝑒(𝑑)
1
1
Μ‡
(resp.,
β„Ž
∈
𝛿
= 0, 𝑒(1) =
𝛿𝐹(⋅,𝑒(⋅),
Μ‡
Μ‡ ) and 𝑒(0)
𝑒(⋅))
ext𝐹(⋅,𝑒(⋅),𝑒(⋅))
π‘š−2
∑𝑖=1 π‘Žπ‘– 𝑒(πœ‰π‘– ).
(xvi) In the sequel by Δ π‘ƒ (resp., Δ π‘ƒπ‘’ ) we denote the solution set of Problem (𝑃) (resp., of Problem (𝑃𝑒 )). Moreover,
by Δ π‘„ (resp., Δ π‘„π‘’ ) we denote the solution set of Problem (𝑄)
(resp., of Problem (𝑄𝑒 )).
Definition 1. Let 𝐸 be a Banach space and let π‘Œ be a metric
space. A multifunction 𝐺 : 𝐼 × π‘Œ → π‘ƒπ‘π‘˜ (𝐸) has the ScorzaDragoni property (the SD-property) if for every πœ€ > 0 there
exists a closed set 𝐴 ⊂ 𝐼 such that the Lebesgue measure πœ‡(𝐼 \
𝐴) is less than πœ€ and 𝐺|𝐴×π‘Œ is continuous. The multifunction
𝐺 is called integrably bounded on compacta in π‘Œ if, for any
compact subset 𝑄 ⊂ π‘Œ, we can find an integrable function
πœ‡π‘„ : 𝐼 → R+ such that sup{β€– 𝑦 β€– : 𝑦 ∈ 𝐺(𝑑, 𝑧)} ≤ πœ‡π‘„(𝑑), for
almost every 𝑧 ∈ 𝑄.
Theorem 2 (see [18]). Let π‘Œ be a complete metric space, 𝐸 a
separable Banach space, 𝐸𝜎 the Banach space 𝐸 endowed with
the weak topology, 𝑀 : 𝐼 × π‘Œ → π‘ƒπ‘π‘˜ (𝐸𝜎 ), and 𝐾 a compact
1
subset of 𝐢(𝐼, π‘Œ). Furthermore, let 𝑅 : 𝐾 → 2𝐿 (𝐼,𝐸) be a multifunction defined by
𝑅 (𝑦) = {𝑔 ∈ 𝐿1 (𝐼, 𝐸) : 𝑔 (𝑑) ∈ 𝑀 (𝑑, 𝑦 (𝑑)) π‘Ž.𝑒. π‘œπ‘› 𝐼} .
(6)
If 𝑀 has the SD-property and is integrably bounded on
compacta in π‘Œ, then the set
𝐴 𝐾 = {𝑓 ∈ 𝐢 (𝐾, 𝐿1𝑀 (𝐼, 𝐸)) : 𝑓 (𝑦) ∈ 𝑅 (𝑦) ∀𝑦 ∈ 𝐾}
(7)
is nonempty complete subset of the space 𝐢(𝐾, 𝐿1𝑀 (𝐼, 𝐸)). Moreover, 𝐴 𝐾 = 𝐴 ext 𝐾 where 𝐿1𝑀 (𝐼, 𝐸) is the space of equivalence
classes of Bochner-integrable functions V : 𝐼 → 𝐸 with the
𝑑
norm β€– V‖𝑀 = sup𝑑∈𝑇 β€– ∫0 V(𝑠)𝑑𝑠 β€– and
𝐴 ext 𝐾 = {𝑓 ∈ 𝐢 (𝐾, 𝐿1𝑀 (𝐼, 𝐸)) : 𝑓 (𝑦) ∈ ext𝑅 (𝑦) ∀𝑦 ∈ 𝐾} .
(8)
Lemma 3 (see [19]). For 𝑝 such that 1 < 𝑝 < ∞ let {𝑒𝑛 , 𝑒}𝑛∈N ⊆
𝐿𝑝 (𝐼, R𝑛 ), sup𝑛∈N β€– 𝑒𝑛 ‖𝑝 < ∞ and 𝑒𝑛 → 𝑒 with respect to the
weak norm β€– ⋅‖𝑀 . Then 𝑒𝑛 → 𝑒 weakly in 𝐿𝑝 (𝐼, R𝑛 ).
Next we state a preliminary lemma, for 0 < πœ‚ < πœƒ < 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 𝐺 : 𝐼 × πΌ → R be the function defined
as follows:
as 0 ≤ 𝑑 < πœ‚,
−𝜏
{
{
{
{
{
{−𝑑
{
{
{
{
𝐺 (𝑑, 𝜏) = { 𝑑 (𝜏 − πœƒ) + (𝜏 − πœ‚)
{
{
{
πœƒ−πœ‚
{
{
{
{
{
{1 − 𝜏
{1 − πœƒ
when πœ‚ ≤ 𝑑 < πœƒ,
𝑖𝑓 0 ≤ 𝜏 ≤ 𝑑
(9)
𝑖𝑓 πœƒ < 𝜏 ≤ 1,
𝑖𝑓 πœ‚ < 𝜏 ≤ 𝑑
𝑖𝑓 𝑑 < 𝜏 ≤ πœƒ
𝑖𝑓 πœƒ < 𝜏 ≤ 1,
(10)
𝑖𝑓 0 ≤ 𝜏 ≤ πœ‚
(ii) 𝑑𝐻(𝐹(𝑑, π‘₯, 𝑦), 𝐹(𝑑, π‘₯σΈ€  , 𝑦󸀠 )) ≤ 𝛼1 (𝑑) β€– π‘₯ − π‘₯σΈ€  β€– +𝛼2 (𝑑)
β€– 𝑦 − 𝑦󸀠 β€– a.e. with 𝛼1 , 𝛼2 ∈ 𝐿1 (𝐼, R+ ) and β€– 𝛼1 + 𝛼2 β€–<
1/2,
𝑖𝑓 πœ‚ < 𝜏 ≤ πœƒ
(iii) for each (𝑑, π‘₯, 𝑦) ∈ 𝐼 × R𝑛 × R𝑛 ,
𝑖𝑓 πœƒ < 𝜏 ≤ 𝑑
𝑖𝑓 𝑑 < 𝜏 ≤ 1.
(11)
∀𝑑 ∈ 𝐼;
(12)
𝑑
0
0
∫ 𝐺 (𝑑, 𝜏) 𝑀 (𝜏) π‘‘πœ = ∫ (𝑑 − 𝜏) 𝑀 (𝜏) π‘‘πœ
πœƒ
𝑑 (𝜏 − πœƒ) + (𝜏 − πœ‚)
+∫
𝑀 (𝜏) π‘‘πœ
πœƒ−πœ‚
0
+∫
1
πœƒ
1−𝜏
𝑀 (𝜏) π‘‘πœ;
1−πœƒ
(iii) sup𝑑,𝜏∈𝐼 |𝐺(𝑑, 𝜏)| ≤ 2, sup𝑑,𝜏∈𝐼 |πœ•πΊ(𝑑, 𝜏)/πœ•π‘‘| ≤ 1.
(15)
with π‘Ž, 𝑐1 , 𝑐2 ∈ 𝐿𝑝 (𝐼, R+ ) 1 < 𝑝 < ∞,
(iv) the spectral radius, π‘Ÿ(𝐿), is less than 1.
Then for each solution 𝑒 ∈ Δ π‘ƒπ‘’ , there is a sequence (π‘’π‘š (⋅))π‘š∈N ⊂
Δ π‘ƒ converging to 𝑒(⋅) in (𝐢1 (𝐼, R𝑛 ), β€– ⋅‖𝐢1 ).
π‘’Μˆ (𝑑) = β„Ž (𝑑) ,
πœ‚
𝑑 (𝜏 − πœ‚) (𝑑 + 1)
−∫
𝑀 (𝜏) π‘‘πœ
πœƒ−πœ‚
0
σ΅„©
σ΅„©σ΅„©
󡄩󡄩𝐹 (𝑑, π‘₯, 𝑦)σ΅„©σ΅„©σ΅„© = sup {β€–Vβ€– : V ∈ 𝐹 (𝑑, π‘₯, 𝑦)}
σ΅„© σ΅„©
≤ π‘Ž (𝑑) + 𝑐1 (𝑑) β€–π‘₯β€– + 𝑐2 (𝑑) 󡄩󡄩󡄩𝑦󡄩󡄩󡄩
Proof. From [9, Theorem 2.1], we obtain Δ π‘ƒπ‘’ =ΜΈ 0. Moreover,
we can say that β€– 𝐹(𝑑, π‘₯, 𝑦) β€–≤ π‘Ž1 (𝑑) a.e. on 𝐼 for some π‘Ž1 ∈
𝐿𝑝 (𝐼, R+ ). Let 𝑒 ∈ Δ π‘ƒ . Then
(ii) if 𝑀 ∈ 𝐿1 (𝐼, R𝑛 ), then for all 𝑑 ∈ 𝐼,
1
Theorem 5. Let 𝐹 : 𝐼×R𝑛 ×R𝑛 → π‘ƒπ‘˜π‘ (R𝑛 ) be a multifunction
such that
(i) for each (π‘₯, 𝑦) ∈ R𝑛 × R𝑛 , the multifunction 𝐹(⋅, π‘₯, 𝑦)
is measurable,
(i) If 𝑒 ∈ π‘Š2,1 (𝐼, R𝑛 ) with 𝑒(0) = π‘₯0 , 𝑒(1) = 𝑒(πœƒ) = 𝑒(πœ‚),
then
0
If 𝑐1 = 𝑐2 = 0, then clearly 𝐿 = 0. We note that if K =
{(β„Ž1 , β„Ž2 ) ∈ 𝐢(𝐼, R) × πΆ(𝐼, R) : β„Ž1 (𝑑), β„Ž2 (𝑑) ≥ 0, ∀𝑑 ∈ 𝐼}, then
𝐿(K) ⊆ K. Moreover, the spectral radius π‘Ÿ(𝐿) = lim β€– 𝐿𝑛 β€–1/𝑛
is an eigenvalue of 𝐿 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 (𝑃) and (𝑃𝑒 ) with the two boundary conditions
𝑒(0) = 𝑒(1) = 0 and in [21] Ibrahim and Gomaa study
the same problems with three boundary conditions 𝑒(0) =
π‘₯0 , 𝑒(πœ‚) = 𝑒(1).
Then the following hold.
𝑒 (𝑑) = π‘₯0 + ∫ 𝐺 (𝑑, 𝜏) π‘’Μˆ (𝜏) π‘‘πœ,
(14)
3. Relaxation Theorems
𝑖𝑓 0 ≤ 𝜏 ≤ πœ‚
lastly if πœƒ ≤ 𝑑 ≤ 1,
1
0
󡄨
󡄨 πœ•πΊ (𝑑, 𝜏) 󡄨󡄨󡄨
𝑔 (𝑑) = ∫ 󡄨󡄨󡄨
󡄨 (𝑐 (𝜏) 𝑓 (𝜏) + 𝑐2 (𝜏) 𝑔 (𝜏)) π‘‘πœ.
πœ•π‘‘ 󡄨󡄨󡄨 1
0 󡄨󡄨
𝑖𝑓 πœ‚ < 𝜏 ≤ πœƒ
−𝜏
{
{
{
{
{
{
πœ‚ (𝜏 − 𝑑 − 1) + 𝜏 (𝑑 − πœƒ + 1)
{
{
{
{
{
πœƒ−πœ‚
{
𝐺 (𝑑, 𝜏) = { 1 − 𝜏
{
+ (𝑑 − 𝜏)
{
{
{
1−πœƒ
{
{
{
{
1−𝜏
{
{
{
1
{ −πœƒ
𝑇
𝑓 (𝑑) = ∫ |𝐺 (𝑑, 𝜏)| (𝑐1 (𝜏) 𝑓 (𝜏) + 𝑐2 (𝜏) 𝑔 (𝜏)) π‘‘πœ,
𝑇 󡄨󡄨
𝑖𝑓 𝑑 < 𝜏 ≤ πœ‚
−𝜏
{
{
{
{
{
𝜏 (𝑑 − πœƒ + 1) + πœ‚ (𝜏 − 𝑑 − 1)
{
{
{
{
{
πœƒ−πœ‚
{
{
𝐺 (𝑑, 𝜏) = {
{
𝑑 (𝜏 − πœƒ) + (𝜏 − πœ‚)
{
{
{
{
{
πœƒ−πœ‚
{
{
{
{
1
−
𝜏
{
{1 − πœƒ
Let 𝑐1 , 𝑐2 , π‘Ž ∈ 𝐿𝑝 (𝐼, R+ ), 1 < 𝑝 < ∞, and let 𝐿 be a
linear operator from 𝐢(𝐼, R) × πΆ(𝐼, R) to 𝐢(𝐼, R) × πΆ(𝐼, R)
defined by 𝐿(𝑓, 𝑔) = (𝑓, 𝑔) such that, for all 𝑑 ∈ 𝐼,
a.e. on 𝐼,
𝑒 (0) = 0, 𝑒 (πœ‚) = 𝑒 (πœƒ) = 𝑒 (1) ,
(13)
(16)
Μ‡
where β„Ž(𝑑) ∈ 𝐹(𝑑, 𝑒(𝑑), 𝑒(𝑑))
a.e. on 𝐼. Assume that 𝑓 :
𝐿1 (𝐼, R𝑛 ) → 𝐢1 (𝐼, R𝑛 ) is a function such that, for each
β„Ž ∈ 𝐿1 (𝐼, R𝑛 ), 𝑓(β„Ž) ∈ π‘Š1,2 (𝐼, R𝑛 ) is the unique solution of
the second-order differential equation
π‘’Μˆ (𝑑) = β„Ž (𝑑) ,
a.e. on 𝐼,
𝑒 (0) = 0, 𝑒 (πœ‚) = 𝑒 (πœƒ) = 𝑒 (1) .
(π‘ƒβ„Ž )
4
Abstract and Applied Analysis
Let S = {𝑒 ∈ 𝐿1 (𝐼, R𝑛 ) : β€– 𝑒(𝑑) β€–≤ π‘Ž1 (𝑑) a.e. on 𝐼}. It is easy
to see that 𝑓(S) is convex. Let (𝑒𝑛 )𝑛∈N be a sequence in 𝑓(S).
Hence, 𝑒𝑛 ∈ π‘Š2,1 (𝐼, R𝑛 ) with 𝑒𝑛 (0) = π‘₯0 , 𝑒𝑛 (πœ‚) = 𝑒𝑛 (πœƒ) = 𝑒𝑛
(17) and
𝑑
𝑒𝑛 (𝑑) = π‘₯0 + ∫ (𝑑 − 𝜏) π‘’Μˆπ‘› (𝜏) π‘‘πœ
πœ€ for each V ∈ 𝑓(S). Define a multifunction 𝑅 : 𝑓(S) →
1
𝑛
2𝐿 (𝐼,R ) by
𝑅 (𝑒) = {𝑔 ∈ 𝐿1 (𝐼, R𝑛 ) : 𝑔 (𝑑) ∈ 𝐹(𝑑, 𝑒 (𝑑) , 𝑒̇ (𝑑)) a.e. on 𝐼} .
(22)
0
πœ‚
𝑑 (𝜏 − πœ‚) (𝑑 + 1)
π‘’Μˆπ‘› (𝜏) π‘‘πœ
−∫
πœƒ−πœ‚
0
πœƒ
𝑑 (𝜏 − πœƒ) + (𝜏 − πœ‚)
+∫
π‘’Μˆπ‘› (𝜏) π‘‘πœ
πœƒ−πœ‚
0
1
+∫
πœƒ
(17)
1−𝜏
π‘’Μˆ (𝜏) π‘‘πœ.
1−πœƒ 𝑛
lim 𝑔
𝑛→∞ 𝑛
Then,
1
lim 𝑒𝑛 (𝑑) = ∫ 𝐺 (𝑑, 𝜏) π‘’Μˆ (𝜏) π‘‘πœ = 𝑒 (𝑑) ,
𝑛→∞
Assume that
π‘Œ = R𝑛 × R𝑛 and set a multifunction 𝑀 : 𝐼 ×
R𝑛
π‘Œ → 2 such that 𝑀(𝑑, (π‘₯, 𝑦)) = 𝐹(𝑑, π‘₯, 𝑦). From Theorem 3.1 in [23], 𝑀 has SD-property. 𝑅 has nonempty convex
values. Let (𝑔𝑛 )𝑛∈N be a sequence in 𝑅(𝑒) for some 𝑒 ∈ 𝑓(S).
So, for each 𝑑 ∈ 𝐼,
0
(18)
which means that 𝑓(S) is a compact subset of 𝐢1 (𝐼, R𝑛 ). Set
Pπœ€ (𝑑) = {π‘₯ ∈ 𝐹 (𝑑, V (𝑑) , VΜ‡ (𝑑)) : β€–β„Ž (𝑑) − π‘₯β€– < πœ€
+ 𝑑 (β„Ž (𝑑) , 𝐹 (𝑑, V (𝑑) , VΜ‡ (𝑑)))} ,
(19)
where πœ€ > 0 and V ∈ 𝑓(S). Hence, for each 𝑑 ∈ 𝐼,
Pπœ€ (𝑑) =ΜΈ 0. Assume that B(𝐼) and B(R𝑛 ) are the Borel 𝜎-fields
of 𝐼 and R𝑛 , respectively. From condition, (𝑖) the function
Μ‡
Μ‡
𝑑 → 𝐹(𝑑, V(𝑑), V(𝑑))
is measurable. Hence, π‘”π‘ŸπΉ(⋅, V(⋅), V(⋅))
∈
Μ‡
B(𝐼) × B(R𝑛 ) and (𝑑, π‘₯) → πœ€π‘‘(β„Ž(𝑑), 𝐹(𝑑, V(𝑑), V(𝑑)))−
β€– β„Ž(𝑑) − π‘₯ β€– is measurable in 𝑑 and continuous in π‘₯ that
is jointly measurable. Thus, by Aumann’s selection theorem,
there exists a measurable selection π‘ πœ€ of Pπœ€ such that π‘ πœ€ (𝑑) ∈
Pπœ€ (𝑑) for each 𝑑 ∈ 𝐼. Now we define a multifunction Qπœ€ :
1
𝑛
𝑓(S) → 2𝐿 (𝐼,R ) by the following:
Qπœ€ (V)
σ΅„©
σ΅„©σ΅„©
󡄩󡄩𝑒𝑛 (𝑑) − 𝑒 (𝑑)σ΅„©σ΅„©σ΅„©
1σ΅„©
σ΅„©σ΅„© 𝑑
≤ ∫ σ΅„©σ΅„©σ΅„©[∫ (𝑑 − 𝜏) (πœ‰π‘› (𝜏) − β„Ž (𝜏)) π‘‘πœ
σ΅„© 0
0 σ΅„©
πœ‚
−∫
0
≤ πœ€ + 𝛼1 (𝑑) ‖𝑒 (𝑑) − V (𝑑)β€–
+ 𝛼2 (𝑑) ‖𝑒̇ (𝑑) − VΜ‡ (𝑑)β€–
𝑑 (𝜏 − πœ‚) (𝑑 + 1)
(πœ‰π‘› (𝜏) − β„Ž (𝜏)) π‘‘πœ
πœƒ−πœ‚
πœƒ
𝑑 (𝜏 − πœƒ) + (𝜏 − πœ‚)
(πœ‰π‘› (𝜏) − β„Ž (𝜏)) π‘‘πœ
πœƒ−πœ‚
0
σ΅„©σ΅„©
1
1−𝜏
σ΅„©
+∫
(πœ‰π‘› (𝜏) − β„Ž (𝜏)) π‘‘πœ]σ΅„©σ΅„©σ΅„©σ΅„© 𝑑𝑠
σ΅„©σ΅„©
πœƒ 1−πœƒ
β€–β„Ž (𝑑) − π‘₯β€– < πœ€ + 𝑑 (β„Ž (𝑑) , 𝐹 (𝑑, V (𝑑) , VΜ‡ (𝑑))) a.e. on 𝐼} ,
(20)
σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©β„Ž (𝑑) − π‘†πœ€ (V) (𝑑)σ΅„©σ΅„©σ΅„© ≤ πœ€ + 𝑑 (β„Ž (𝑑) , 𝐹 (𝑑, V (𝑑) , VΜ‡ (𝑑)))
(23)
1
because 𝐹 has closed values in R𝑛 . Therefore, 𝑔 ∈ 𝛿𝐹(⋅,𝑒(⋅),
Μ‡
𝑒(⋅))
𝑛
which implies that 𝑅(⋅) has compact values in R . We can
apply Theorem 2 to find a continuous function πœƒ : 𝑓(S) →
𝐿1𝑀 (𝐼, R𝑛 ) such that πœƒ(𝑒) ∈ ext(𝑅(𝑒)), for all 𝑒 ∈ 𝑓(S). We
Μ‡
see that πœƒ(𝑒)(𝑑) ∈ ext(𝑀(𝑑, (𝑒(𝑑), 𝑒(𝑑))))
[24], hence πœƒ(𝑒)(𝑑) ∈
Μ‡
ext𝐹(𝑑, 𝑒(𝑑), 𝑒(𝑑))
a.e. on 𝐼. Assume that πœ‚ : 𝑓(S) →
π‘Š1,2 (𝐼, R𝑛 ) is the function which for each 𝑒 ∈ 𝑓(S), πœ‚(𝑒) =
𝑔(πœƒ(𝑒)). For each 𝑒 ∈ 𝑓(S), we have β€– πœƒ(𝑒)(𝑑) β€–≤ π‘Ž1 and so
πœƒ(𝑒) ∈ S. Then, πœ‚ is a function from 𝑓(S) into 𝑓(S) and also
we see that πœ‚ is continuous [19]. Now let πœ€π‘› → 0, π‘†πœ€π‘› = 𝑆𝑛
and πœ‰π‘› = πœ‰πœ€π‘› . Then, for each 𝑛 ∈ N, the function π‘“π‘œπœ‰π‘› is a
continuous function from the compact set 𝑓(S) into itself.
From Schauder’s fixed point theorem, π‘“π‘œπœ‰π‘› has a fixed point
1
1
𝑒𝑛 , but ext𝛿𝐹(⋅,V(⋅),
= 𝛿ext𝐹(⋅,V(⋅),
[24] so 𝑒𝑛 ∈ Δ π‘ƒπ‘’ . By
Μ‡
Μ‡
V(⋅))
V(⋅))
passing to a subsequence if necessary, we may assume that
𝑒𝑛 → 𝑒̂ in 𝐢1 (𝐼, R𝑛 ). Then, we obtain
1
:
= {π‘₯ ∈ 𝛿𝐹(⋅,V(⋅),
Μ‡
V(⋅))
with Qπœ€ (V)(𝑑) =ΜΈ 0 for each V ∈ 𝑓(S). From [22, Proposition 4],
Qπœ€ is 𝑙. 𝑠. 𝑐. and clearly has decomposable values. Applying
[22, Theorem 3], we have a continuous selection π‘†πœ€ of Qπœ€ .
Therefore,
(𝑑) = 𝑔 (𝑑) ∈ 𝐹 (𝑑, 𝑒 (𝑑) , 𝑒̇ (𝑑))
+∫
1
𝑑
0
0
σ΅„©
σ΅„©
≤ ∫ [∫ (𝑑 − 𝜏) σ΅„©σ΅„©σ΅„©πœ‰π‘› (𝜏) − 𝑆𝑛 (𝜏)σ΅„©σ΅„©σ΅„© π‘‘πœ
𝑑
σ΅„©
σ΅„©
+ ∫ (𝑑 − 𝜏) σ΅„©σ΅„©σ΅„©β„Ž (𝜏) − 𝑆𝑛 (𝜏)σ΅„©σ΅„©σ΅„© π‘‘πœ
0
a.e. on 𝐼.
(21)
+∫
From Theorem 2, we find a continuous function πœ‰πœ€ : 𝑓(S) →
1
and β€– π‘†πœ€ (V)−πœ‰πœ€ (V) β€–<
𝐿1𝑀 (𝐼, R𝑛 ) such that πœ‰πœ€ (V) ∈ ext𝛿𝐹(⋅,V(⋅),
Μ‡
V(⋅))
+∫
πœ‚
0
πœ‚
0
𝑑 (𝜏 − πœ‚) (𝑑 + 1)
(πœ‰π‘› (𝜏) − 𝑆𝑛 (𝜏)) π‘‘πœ
πœƒ−πœ‚
𝑑 (𝜏 − πœ‚) (𝑑 + 1) σ΅„©σ΅„©
σ΅„©
σ΅„©σ΅„©β„Ž (𝜏) − 𝑆𝑛 (𝜏)σ΅„©σ΅„©σ΅„© π‘‘πœ
πœƒ−πœ‚
Abstract and Applied Analysis
+∫
1
πœƒ
+∫
1
πœƒ
5
1 − 𝜏 σ΅„©σ΅„©
σ΅„©
σ΅„©πœ‰ (𝜏) − 𝑆𝑛 (𝜏)σ΅„©σ΅„©σ΅„© π‘‘πœ
1−πœƒσ΅„© 𝑛
+∫
πœ‚
0
1 − 𝜏 σ΅„©σ΅„©
σ΅„©
σ΅„©β„Ž (𝜏) − 𝑆𝑛 (𝜏)σ΅„©σ΅„©σ΅„© π‘‘πœ] 𝑑𝑠.
1−πœƒσ΅„©
(24)
+∫
1
πœƒ
But πœ‰π‘› −𝑆𝑛 → 0 with respect to the norm β€– ⋅‖𝑀 from Lemma 3
we get πœ‰π‘› − 𝑆𝑛 → 0 weakly in 𝐿1 (𝐼, R𝑛 ). So we have
𝑑 (𝜏 − πœ‚) (𝑑 + 1)
(𝛼1 (𝜏) ‖𝑒 (𝜏) − 𝑒̂ (𝜏)β€–
πœƒ−πœ‚
σ΅„©
σ΅„©
Μ‚Μ‡ (𝜏)σ΅„©σ΅„©σ΅„©σ΅„©) π‘‘πœ
+𝛼2 (𝜏) 󡄩󡄩󡄩󡄩𝑒̇ (𝜏) − 𝑒
1−𝜏
(𝛼 (𝜏) ‖𝑒 (𝜏) − 𝑒̂ (𝜏)β€–
1−πœƒ 1
σ΅„©
σ΅„©
Μ‚Μ‡ (𝜏)σ΅„©σ΅„©σ΅„©σ΅„©) π‘‘πœ] 𝑑𝑠
+𝛼2 (𝜏) 󡄩󡄩󡄩󡄩𝑒̇ (𝜏) − 𝑒
𝑑
≤ ‖𝑒− 𝑒̂‖𝐢1 (𝐼,R𝑛 ) (∫ (𝑑−𝜏) (𝛼1 (𝜏)+𝛼2 (𝜏)) π‘‘πœ
0
𝑑
σ΅„©
σ΅„©
∫ (𝑑 − 𝜏) σ΅„©σ΅„©σ΅„©πœ‰π‘› (𝜏) − 𝑆𝑛 (𝜏)σ΅„©σ΅„©σ΅„© π‘‘πœ
πœ‚ 𝑑 (𝜏−πœ‚) (𝑑+1)
+∫
0
+∫
πœ‚
0
+∫
1
πœƒ
𝑑 (𝜏 − πœ‚) (𝑑 + 1) σ΅„©σ΅„©
σ΅„©
σ΅„©σ΅„©πœ‰π‘› (𝜏) − 𝑆𝑛 (𝜏)σ΅„©σ΅„©σ΅„© π‘‘πœ
πœƒ−πœ‚
(25)
𝑑
0
0
1
+∫
πœƒ
1 − 𝜏 σ΅„©σ΅„©
σ΅„©
σ΅„©πœ‰ (𝜏) − 𝑆𝑛 (𝜏)σ΅„©σ΅„©σ΅„© π‘‘πœ 󳨀→ 0.
1−πœƒσ΅„© 𝑛
(𝛼1 (𝜏)+𝛼2 (𝜏)) π‘‘πœ
1−𝜏
(𝛼 (𝜏) + 𝛼2 (𝜏)) π‘‘πœ)
1−πœƒ 1
1
= ‖𝑒− 𝑒̂‖𝐢1 (𝐼,R𝑛 ) ∫ |𝐺 (𝑑, 𝜏)| (𝛼1 (𝜏)+𝛼2 (𝜏)) π‘‘πœ
0
σ΅„©
σ΅„©
≤ 2‖𝑒 − 𝑒̂‖𝐢1 (𝐼,R𝑛 ) 󡄩󡄩󡄩𝛼1 (𝜏) + 𝛼2 (𝜏)σ΅„©σ΅„©σ΅„© .
Moreover,
1
πœƒ−πœ‚
0
(27)
Since by assumption (ii), β€– 𝛼1 + 𝛼2 β€–< 1/2 we get 𝑒 = 𝑒̂.
So 𝑒𝑛 → 𝑒 in 𝐢1 (𝐼, R𝑛 ) and 𝑒 ∈ Δ𝑃𝑒 where the closure is
taken in 𝐢1 (𝐼, R𝑛 ) which means that Δ π‘ƒ ⊆ Δ𝑃𝑒 . Therefore, the
proof is complete if we show that Δ π‘ƒ is closed. Indeed if
V𝑛 ∈ Δ π‘ƒ and V𝑛 → V in 𝐢1 (𝐼, R𝑛 ), then V𝑛 = 𝑓(𝑦𝑛 ) for
1
𝑦𝑛 ∈ 𝛿𝐹(⋅,V(⋅),
Μ‡ . From assumption (iii) and the DunfordV(⋅))
Pettis theorem, {𝑦𝑛 }𝑛∈N is weakly sequentially compact in
𝐿1 (𝐼, R𝑛 ). So we can say that {𝑦𝑛 }𝑛∈N in 𝐿1 (𝐼, R𝑛 ). By [25,
Theorem 3.1], we get
σ΅„©
σ΅„©
∫ [∫ (𝑑 − 𝜏) σ΅„©σ΅„©σ΅„©β„Ž (𝜏) − 𝑆𝑛 (𝜏)σ΅„©σ΅„©σ΅„© π‘‘πœ
πœ‚
+∫
0
+∫
1
πœƒ
1
𝑑
0
0
𝑑 (𝜏 − πœ‚) (𝑑 + 1)
(πœ‰π‘› (𝜏) − 𝑆𝑛 (𝜏)) π‘‘πœ
πœƒ−πœ‚
1 − 𝜏 σ΅„©σ΅„©
σ΅„©
σ΅„©β„Ž (𝜏) − 𝑆𝑛 (𝜏)σ΅„©σ΅„©σ΅„© π‘‘πœ] 𝑑𝑠
1−πœƒσ΅„©
σ΅„©
σ΅„©
≤ ∫ [∫ (𝑑 − 𝜏) (πœ€π‘› + 𝛼1 (𝜏) 󡄩󡄩󡄩𝑒 (𝜏) − 𝑒𝑛 (𝜏)σ΅„©σ΅„©σ΅„©
σ΅„©
σ΅„©
+𝛼2 (𝜏) 󡄩󡄩󡄩𝑒̇ (𝜏) − 𝑒̇𝑛 (𝜏)σ΅„©σ΅„©σ΅„©)
πœ‚
+∫
0
𝑦 (𝑑) ∈ conv lim{𝑦𝑛 (𝑑)}𝑛∈N ⊆ conv lim 𝐹 (𝑑, V𝑛 (𝑑) , V̇𝑛 (𝑑))
𝑑 (𝜏 − πœ‚) (𝑑 + 1)
σ΅„©
σ΅„©
(πœ€π‘› + 𝛼1 (𝜏) 󡄩󡄩󡄩𝑒 (𝜏) − 𝑒𝑛 (𝜏)σ΅„©σ΅„©σ΅„©
πœƒ−πœ‚
σ΅„©
σ΅„©
+𝛼2 (𝜏) 󡄩󡄩󡄩𝑒̇ (𝜏) − 𝑒̇𝑛 (𝜏)σ΅„©σ΅„©σ΅„©)
1
1−𝜏
σ΅„©
σ΅„©
+∫
(πœ€π‘› + 𝛼1 (𝜏) 󡄩󡄩󡄩𝑒 (𝜏) − 𝑒𝑛 (𝜏)σ΅„©σ΅„©σ΅„©
πœƒ 1−πœƒ
σ΅„©
σ΅„©
+𝛼2 (𝜏) 󡄩󡄩󡄩𝑒̇ (𝜏) − 𝑒̇𝑛 (𝜏)σ΅„©σ΅„©σ΅„©)] 𝑑𝑠.
= 𝐹 (𝑑, V (𝑑) , VΜ‡ (𝑑))
a.e. on 𝐼.
(28)
Moreover, 𝑓(𝑦𝑛 ) → 𝑓(𝑦) in 𝐿1 (𝐼, R𝑛 ) for 𝑦 ∈ 𝐿1 (𝐼, R𝑛 )
Μ‡
and 𝑦(𝑑) ∈ 𝐹(𝑑, V(𝑑), V(𝑑))
a.e. on 𝐼. Hence, V ∈ Δ π‘ƒ ; that is Δ π‘ƒ
is closed in 𝐢1 (𝐼, R𝑛 ).
(26)
Now we consider the following assumptions:
As 𝑛 → ∞, we have
(𝐴 1 ) 𝛽 ∈ (0, πœ‹/2), π‘Žπ‘– > 0 and ∑π‘š−2
𝑖=1 π‘Žπ‘– < 1;
𝑒 (𝑑) − 𝑒 (𝑑)β€–
β€–Μ‚
1
𝑑
0
0
≤ ∫ [∫ (𝑑 − 𝜏) (𝛼1 (𝜏) ‖𝑒 (𝜏) − 𝑒̂ (𝜏)β€–
σ΅„©
σ΅„©
Μ‚Μ‡ (𝜏)σ΅„©σ΅„©σ΅„©σ΅„©) π‘‘πœ
+𝛼2 (𝜏) 󡄩󡄩󡄩󡄩𝑒̇ (𝜏) − 𝑒
π‘š−2
(𝐴 2 ) ∑π‘š−2
𝑖=1 π‘Žπ‘– cos π›½πœ‰π‘– − cos 𝛽 > 0 and πΎπ‘š = 1/ ∑𝑖=1 π‘Žπ‘–
cos π›½πœ‰π‘– − cos 𝛽;
(𝐴 3 ) 𝐢0 = (sin 𝛽/𝛽)(1 + πΎπ‘š ) and 𝐢1 = min{πΎπ‘š + 1,
πΎπ‘š sin2 𝛽};
6
Abstract and Applied Analysis
Μ‡ = 0, 𝑒(1) = ∑π‘š−2
(𝐴 4 ) 𝑆 = {𝑒 ∈ 𝐢2 (𝐼, R𝑛 ) : 𝑒(0)
𝑖=1 π‘Žπ‘– 𝑒(πœ‰π‘– )};
Proof. (ii) Since
πœ•G (𝑑, 𝑠)
πœ•π‘‘
(𝐴 5 ) G : 𝐼 × πΌ → R is defined by
cos 𝛽 (𝑑 − 𝑠)
={
0
G (𝑑, 𝑠)
1
{ sin 𝛽 (𝑑 − 𝑠)
= {𝛽
{0
if 0 ≤ 𝑠 ≤ 𝑑 ≤ 1
if 0 ≤ 𝑠 ≤ 𝑑 ≤ 1
if 0 ≤ 𝑑 ≤ 𝑠 ≤ 1
π‘š−2
if 0 ≤ 𝑑 ≤ 𝑠 ≤ 1
π‘š−2
{
{
sin 𝛽 (1 − 𝑠) − ∑ π‘Žπ‘– sin 𝛽 (πœ‰π‘– − 𝑠) ,
{
{
{
𝑖=1
{
{
{
{
{
if 0 ≤ 𝑠 ≤ πœ‰1 ,
{
{
{
{
{
π‘š−2
{
{
{
{
sin
𝛽
−
𝑠)
−
∑ π‘Žπ‘– sin 𝛽 (πœ‰π‘– − 𝑠) ,
(1
{
{
{
{
𝑖=2
{
{
{
{
<
𝑠
≤
πœ‰2 ,
if
πœ‰
{
1
{
{
{
{
π‘š−2
{
{
{
{
sin 𝛽 (1 − 𝑠) − ∑ π‘Žπ‘– sin 𝛽 (πœ‰π‘– − 𝑠) ,
{
{
{
{
𝑖=3
{
πΎπ‘š
+
cos 𝛽𝑑 {
if
πœ‰
<
𝑠
≤
πœ‰3 ,
2
{
𝛽
{
{
{
{
..
{
{
{
.
{
{
{
π‘š−2
{
{
{
{
sin
𝛽
−
𝑠)
−
∑ π‘Žπ‘– sin 𝛽 (πœ‰π‘– − 𝑠) ,
(1
{
{
{
{
𝑖=π‘˜
{
{
{
{
if
πœ‰
<
𝑠
≤ πœ‰π‘˜ ,
{
π‘˜−1
{
{
{
{
{
..
{
{
.
{
{
{
{
{sin 𝛽 (1 − 𝑠) ,
{
{
{
{
if πœ‰π‘š−2 < 𝑠 ≤ 1.
{
(29)
{
{
sin 𝛽 (1−𝑠)− ∑π‘Žπ‘– sin 𝛽 (πœ‰π‘– − 𝑠),
{
{
{
𝑖=1
{
{
{
{
{
if
0
≤
𝑠
≤ πœ‰1 ,
{
{
{
{
{
π‘š−2
{
{
{
{
sin
𝛽
∑π‘Žπ‘– sin 𝛽 (πœ‰π‘– − 𝑠),
(1−𝑠)−
{
{
{
{
𝑖=2
{
{
{
{
<
𝑠
≤ πœ‰2 ,
if
πœ‰
{
1
{
{
{
{
π‘š−2
{
{
{sin 𝛽 (1−𝑠)− ∑π‘Ž sin 𝛽 (πœ‰ − 𝑠),
{
{
𝑖
𝑖
{
{
{
𝑖=3
{
− πΎπ‘š sin 𝛽𝑑 {
if πœ‰2 < 𝑠 ≤ πœ‰3 ,
{
{
{
{ .
{
{
..
{
{
{
{
{
π‘š−2
{
{
{
{
sin
𝛽
∑π‘Žπ‘– sin 𝛽 (πœ‰π‘– − 𝑠),
(1−𝑠)−
{
{
{
{
𝑖=π‘˜
{
{
{
{
<
𝑠 ≤ πœ‰π‘˜ ,
if
πœ‰
{
π‘˜−1
{
{
{
{
{
..
{
{
.
{
{
{
{
{
sin
𝛽 (1 − 𝑠) ,
{
{
{
{
if πœ‰π‘š−2 < 𝑠 ≤ 1,
{
(31)
then sup𝑑,𝑠∈𝐼 πœ•G(𝑑, 𝑠)/πœ•π‘‘ ≤ 1 + πΎπ‘š . Furthermore,
πœ•G (𝑑, 𝑠)
πœ•π‘‘
π‘š−2
≥ πΎπ‘š sin 𝛽𝑑 [ ∑ π‘Žπ‘– sin (πœ‰π‘– − 𝑠) − sin 𝛽 (1 − 𝛽)]
(32)
𝑖=1
Lemma 6 (see [26]). If the assumptions (𝐴 1 )–(𝐴 5 ) hold, then
Theorem 7. Assume that the assumptions (𝐴 1 ) and (𝐴 2 ) hold.
Let 𝐹 be a multifunction from 𝐼 × R𝑛 × R𝑛 to π‘ƒπ‘˜π‘ (R𝑛 ) satisfying
the following conditions:
(ii) sup𝑑,𝑠∈𝐼 |πœ•G(𝑑, 𝑠)/πœ•π‘‘| ≤ 𝐢1 ,
(iii) for each π‘₯ ∈ 𝐢1 (𝐼, R𝑛 ) there exists a unique function
𝑒π‘₯ ∈ 𝑆 such that
1
0
1
1
≥ −πΎπ‘š sin 𝛽
and thus sup𝑑,𝑠∈𝐼 |πœ•G(𝑑, 𝑠)/πœ•π‘‘| ≤ 𝐢1 .
(i) 0 ≤ G(𝑑, 𝑠) ≤ 𝐢0 for all (𝑑, 𝑠) ∈ 𝐼 × πΌ,
𝑒π‘₯ (𝑑) = ∫ G (𝑑, 𝑠) π‘₯ (𝑠) 𝑑𝑠,
2
(30)
(iv) (∫0 |G(𝑑, 𝑠)|π‘˜ 𝑑𝑠)1/π‘˜ ≤ 𝐢0 and (∫0 |(πœ•G/πœ•π‘‘)(𝑑, 𝑠)|π‘˜ 𝑑𝑠)1/π‘˜
≤ 𝐢1 .
(a) for each (π‘₯, 𝑦) ∈ R × R, the multifunction 𝐹(⋅, π‘₯, 𝑦) is
measurable;
(b) for each 𝑑 ∈ 𝐼, the function (π‘₯, 𝑦) → 𝐹(𝑑, π‘₯, 𝑦) is
continuous with respect to the Hausdorff metric 𝑑𝐻;
(c) for each (𝑑, π‘₯, 𝑦) ∈ 𝐼 × R𝑛 × R𝑛
󡄩󡄩󡄩𝐹 (𝑑, π‘₯, 𝑦)σ΅„©σ΅„©σ΅„© ≤ sup {β€–Vβ€– : V ∈ 𝐹 (𝑑, π‘₯, 𝑦)}
σ΅„©
σ΅„©
(33)
σ΅„© σ΅„©
≤ π‘Ž (𝑑) + 𝑐1 (𝑑) β€–π‘₯β€– + 𝑐2 (𝑑) 󡄩󡄩󡄩𝑦󡄩󡄩󡄩 ;
(d) the spectral radius π‘Ÿ(𝐿) of 𝐿 is less than one.
Then Problem (𝑄𝑒 ) admits a solution in 𝑆.
Abstract and Applied Analysis
7
Proof. We can say that β€– 𝐹(𝑑, π‘₯, 𝑦) β€–≤ π‘Ž1 (𝑑) a.e. on 𝐼 for some
π‘Ž1 ∈ 𝐿𝑝 (𝐼, R+ ) [9]. Let π‘₯ ∈ 𝐢1 (𝐼, R𝑛 ) and let 𝑒 ∈ 𝐢2 (𝐼, R𝑛 ) be
the unique solution of the problem
π‘’Μˆ (𝑑) = π‘₯ (𝑑) ,
𝑒̇ (0) = 0,
π‘’Μˆ (𝑑) = β„Ž (𝑑) ,
a.e. on 𝐼,
π‘š−2
𝑒 (1) = ∑ π‘Žπ‘– 𝑒 (πœ‰π‘– ) .
1
From Lemma 6, we have 𝑒(𝑑) = ∫0 G(𝑑, 𝑠)π‘₯(𝑠)𝑑𝑠, ∀𝑑 ∈ 𝐼.
Thus, we define a function 𝑓 : 𝐢1 (𝐼, R𝑛 ) → 𝐢2 (𝐼, R𝑛 ) such
that 𝑓(π‘₯) is the unique solution of (∗). Let
a.e. on 𝐼,
(π‘„β„Ž )
π‘š−2
𝑒̇ (0) = 0,
(∗)
𝑖=1
1
β„Ž ∈ 𝐢1 (𝐼, R𝑛 ), 𝑓󸀠 (β„Ž) ∈ 𝐢2 (𝐼, R𝑛 ) is the unique solution of
the second-order differential equation
𝑒 (1) = ∑ π‘Žπ‘– 𝑒 (πœ‰π‘– ) .
𝑖=1
Let 𝑆 = {𝑒 ∈ 𝐢1 (𝐼, R𝑛 ) :β€– 𝑒(𝑑) β€–≤ 𝑏1 (𝑑) a.e. on 𝐼}. So 𝑓󸀠 (𝑆)
is convex. Let (𝑒𝑛 )𝑛∈N be a sequence in 𝑓󸀠 (𝑆). Hence, 𝑒𝑛 ∈
𝐢2 (𝐼, R𝑛 ) with 𝑒𝑛 (0) = 0, 𝑒̇𝑛 (0) = 0, 𝑒𝑛 (1) = ∑π‘š−2
𝑖=1 π‘Žπ‘– 𝑒𝑛 (πœ‰π‘– ).
Then from Lemma 6,
1
lim 𝑒𝑛 (𝑑) = ∫ G (𝑑, 𝜏) π‘’Μˆ (𝜏) π‘‘πœ = 𝑒 (𝑑) ,
𝑛
V = {π‘₯ ∈ 𝐢 (𝐼, R ) : β€–π‘₯ (𝑑)β€– ≤ π‘Ž1 (𝑑) a.e. on 𝐼} .
𝑛→∞
(34)
From the Dunford-Pettis theorem, V is weakly compact and
then 𝑓(V) is convex and compact subset of 𝐢2 (𝐼, R𝑛 ). Let
1
𝑛
Y = R𝑛 × R𝑛 . If K = 𝑓(V), R : K → 2𝐿 (𝐼,R ) and
𝑛
M : 𝐼 × Y → 2R , where R(𝑒) = {𝑔 ∈ 𝐿1 (𝐼, R𝑛 ) : 𝑔(𝑑) ∈
Μ‡
𝐹(𝑑, 𝑒(𝑑), 𝑒(𝑑))
a.e. on 𝐼} and M(𝑑, (π‘₯, 𝑦)) = 𝐹(𝑑, π‘₯, 𝑦), then
M has SD-property [23]. It is easy to show that R is
nonempty and convex subset of 𝐿1 (𝐼, R𝑛 ). If 𝑓𝑛 is a sequence
in R(𝑒) for some 𝑒 ∈ K, then lim𝑛 → ∞ 𝑓𝑛 (𝑑) = 𝑓(𝑑) ∈
Μ‡
𝐹(𝑑, 𝑒(𝑑), 𝑒(𝑑)),
where the values of 𝐹 are closed. Therefore,
the values of R are weakly compact. According to Theorem 5
there exists a continuous function π‘Ÿ : K → 𝐿1𝑀 (𝐼, R𝑛 )
with π‘Ÿ(𝑒) ∈ ext(R(𝑒)), for all 𝑒 ∈ K. Thus, π‘Ÿ(𝑒)(𝑑) ∈
Μ‡
ext(M(𝑑, 𝑒(𝑑), 𝑒(𝑑)))
a.e. on 𝐼 [24] which implies π‘Ÿ(𝑒)(𝑑) ∈
Μ‡
ext(𝐹(𝑑, 𝑒(𝑑), 𝑒(𝑑)))
a.e. on 𝐼. If 𝑒 ∈ 𝑓(V), then β€– π‘Ÿ(𝑒)(𝑑) β€–≤ π‘Ž1
and so π‘Ÿ(𝑒) ∈ V. Put πœƒ : 𝑓(V) → π‘Š2,1 (𝐼, R𝑛 ) such that
πœƒ(𝑒) = 𝑓(π‘Ÿ(𝑒)), thus πœƒ is a continuous function from 𝑓(V)
into 𝑓(V) [19]. From Schauder’s fixed point theorem, there
exists π‘₯ ∈ 𝑓(V) such that π‘₯ = πœƒ(π‘₯) = 𝑓(π‘Ÿ(π‘₯)) which
̈
∈
means that there is π‘₯ ∈ 𝑆 ⊆ 𝐢2 (𝐼, R𝑛 ) such that π‘₯(𝑑)
Μ‡
ext(𝐹(𝑑, π‘₯(𝑑), π‘₯(𝑑))).
Theorem 8. In the setting of Theorem 7, if one replaces condition (b) by the following condition:
(b)σΈ€  𝑑𝐻(𝐹(𝑑, π‘₯, 𝑦), 𝐹(𝑑, π‘₯σΈ€  , 𝑦󸀠 )) ≤ π‘˜1 β€– π‘₯ − π‘₯σΈ€  β€– +
π‘˜2 β€– 𝑦 − 𝑦󸀠 β€– a.e. with π‘˜1 ≥ 0, π‘˜2 ≥ 0 and |π‘˜1 + π‘˜2 | < 1/2𝐢0 .
Then Δ π‘„π‘’ is nonempty and Δ π‘„π‘’ = Δ π‘„ where the closure
taken in 𝐢2 (𝐼, R𝑛 ).
0
(36)
hence, 𝑓󸀠 (𝑆) is a compact subset of 𝐢2 (𝐼, R𝑛 ). Set
Qπœ€ (𝑑) = {π‘₯ ∈ 𝐹 (𝑑, V (𝑑) , VΜ‡ (𝑑)) :
β€–β„Ž (𝑑) − π‘₯β€– < πœ€ + 𝑑 (β„Ž (𝑑) , 𝐹 (𝑑, V (𝑑) , VΜ‡ (𝑑)))} ,
(37)
where πœ€ > 0 and V ∈ 𝑓󸀠 (𝑆). Hence, for each 𝑑 ∈ 𝐼,
Qπœ€ (𝑑) =ΜΈ 0. Assume that B(𝐼) and B(R𝑛 ) are the Borel 𝜎-fields
of 𝐼 and R𝑛 , respectively. From condition (i), the function
Μ‡
Μ‡
𝑑 → 𝐹(𝑑, V(𝑑), V(𝑑))
is measurable. Hence, π‘”π‘ŸπΉ(⋅, V(⋅), V(⋅))
∈
Μ‡
B(𝐼) × B(R𝑛 ) and (𝑑, π‘₯) → πœ€π‘‘(β„Ž(𝑑), 𝐹(𝑑, V(𝑑), V(𝑑)))−
β€– β„Ž(𝑑) − π‘₯ β€– is measurable in 𝑑 and continuous in π‘₯ that
is jointly measurable. Thus, by Aumann’s selection theorem,
there exists a measurable selection π‘ πœ€ of Qπœ€ such that π‘ πœ€ (𝑑) ∈
Qπœ€ (𝑑) for each 𝑑 ∈ 𝐼. Now we define a multifunction Qπœ€ :
1
𝑛
𝑓󸀠 (𝑆) → 2𝐢 (𝐼,R ) by the following:
1
Qπœ€ (V) = {π‘₯ ∈ 𝛿𝐹(⋅,V(⋅),
: β€–β„Ž (𝑑) − π‘₯β€–
Μ‡
V(⋅))
< πœ€ + 𝑑 (β„Ž (𝑑) , 𝐹 (𝑑, V (𝑑) , VΜ‡ (𝑑))) a.e. on 𝐼} ,
(38)
with Qπœ€ (V)(𝑑) =ΜΈ 0 for each V ∈ 𝑓󸀠 (𝑆). From [22, Proposition 4],
Qπœ€ is 𝑙. 𝑠. 𝑐. and clearly has decomposable values. Applying
[22, Theorem 3], we have a continuous selection π‘†πœ€ of Qπœ€ .
Therefore,
σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©β„Ž (𝑑) − π‘†πœ€ (V) (𝑑)σ΅„©σ΅„©σ΅„© ≤ πœ€ + 𝑑 (β„Ž (𝑑) , 𝐹 (𝑑, V (𝑑) , VΜ‡ (𝑑)))
≤ πœ€ + π‘˜1 (𝑑) ‖𝑒 (𝑑) − V (𝑑)β€–
Proof. From Theorem 7, we have Δ π‘„π‘’ =ΜΈ 0. Moreover,
β€– 𝐹(𝑑, π‘₯, 𝑦) β€–≤ 𝑏1 (𝑑) a.e. on 𝐼 for some 𝑏1 ∈ 𝐿𝑝 (𝐼, R+ ).
Let 𝑒 ∈ Δ π‘„. Then
+ π‘˜2 (𝑑) ‖𝑒̇ (𝑑) − VΜ‡ (𝑑)β€–
a.e. on 𝐼.
(39)
(35)
From Theorem 2, we find a continuous function πœ‰πœ€σΈ€  :
1
and
𝑓 (𝑆) → 𝐿1𝑀 (𝐼, R𝑛 ) such that πœ‰πœ€σΈ€  (V) ∈ ext 𝛿𝐹(⋅,V(⋅),
Μ‡
V(⋅))
σΈ€ 
σΈ€ 
β€– π‘†πœ€ (V) − πœ‰πœ€ (V) β€–< πœ€ for each V ∈ 𝑓 (𝑆). Define a multifunction
1
𝑛
𝑅󸀠 : 𝑓󸀠 (𝑆) → 2𝐢 (𝐼,R ) by
Μ‡
where β„Ž(𝑑) ∈ 𝐹(𝑑, 𝑒(𝑑), 𝑒(𝑑))
a.e. on 𝐼. Assume that 𝑓󸀠 :
𝐢1 (𝐼, R𝑛 ) → 𝐢2 (𝐼, R𝑛 ) is a function such that, for each
𝑅󸀠 (𝑒) = {𝑔 ∈ 𝐢1 (𝐼, R𝑛 ) : 𝑔 (𝑑) ∈ 𝐹 (𝑑, 𝑒 (𝑑) , 𝑒̇ (𝑑)) a.e. on 𝐼} .
(40)
π‘’Μˆ (𝑑) = β„Ž (𝑑) ,
𝑒̇ (0) = 0,
a.e. on 𝐼,
π‘š−2
𝑒 (1) = ∑ π‘Žπ‘– 𝑒 (πœ‰π‘– ) ,
σΈ€ 
𝑖=1
8
Abstract and Applied Analysis
As in Theorem 5,
let π‘Œ = R𝑛 × R𝑛 and set a multifunction
R𝑛
𝑀 : 𝐼×π‘Œ → 2 such that 𝑀(𝑑, (π‘₯, 𝑦)) = 𝐹(𝑑, π‘₯, 𝑦). From [23,
Theorem 3.1], 𝑀 has SD-property. 𝑅󸀠 has nonempty convex
values. Let (𝑔𝑛 )𝑛∈N be a sequence in 𝑅󸀠 (𝑒) for some 𝑒 ∈ 𝑓󸀠 (𝑆).
So, for each 𝑑 ∈ 𝐼,
lim 𝑔 (𝑑) = 𝑔 (𝑑) ∈ 𝐹 (𝑑, 𝑒 (𝑑) , 𝑒̇ (𝑑))
(41)
𝑛→∞ 𝑛
1
because 𝐹 has closed values in R𝑛 . Therefore, 𝑔 ∈ 𝛿𝐹(⋅,𝑒(⋅),
Μ‡
𝑒(⋅))
σΈ€ 
𝑛
which implies 𝑅 (⋅) has compact values in R . We can apply
Theorem 2 to find a continuous function πœƒσΈ€  : 𝑓󸀠 (𝑆) →
𝐿1𝑀 (𝐼, R𝑛 ) such that πœƒσΈ€  (𝑒) ∈ ext(𝑅󸀠 (𝑒)), for all 𝑒 ∈ 𝑓󸀠 (𝑆).
Μ‡
We see that πœƒσΈ€  (𝑒)(𝑑) ∈ ext(𝑀(𝑑, (𝑒(𝑑), 𝑒(𝑑))))
[24], hence
Μ‡
a.e. on 𝐼. Assume that πœ‚σΈ€  :
πœƒσΈ€  (𝑒)(𝑑) ∈ ext𝐹(𝑑, 𝑒(𝑑), 𝑒(𝑑))
𝑓󸀠 (𝑆) → 𝐢2 (𝐼, R𝑛 ) is the function which for each 𝑒 ∈ 𝑓󸀠 (𝑆),
πœ‚σΈ€  (𝑒) = 𝑔(πœƒσΈ€  (𝑒)). For each 𝑒 ∈ 𝑓󸀠 (𝑆), we have β€– πœƒσΈ€  (𝑒)(𝑑) β€–≤ 𝑏1
and so πœƒσΈ€  (𝑒) ∈ 𝑆. Then, πœ‚σΈ€  is a function from 𝑓󸀠 (𝑆) into 𝑓󸀠 (𝑆)
and also we see that πœ‚σΈ€  is continuous [19]. Now let πœ€π‘› → 0,
π‘†πœ€π‘› = 𝑆𝑛 and πœ‰π‘›σΈ€  = πœ‰πœ€σΈ€ π‘› . Then, for each 𝑛 ∈ N, the function
𝑓󸀠 π‘œπœ‰π‘›σΈ€  is a continuous function from the compact set 𝑓󸀠 (𝑆)
into itself. From Schauder’s fixed point theorem, π‘“π‘œπœ‰π‘›σΈ€  has
1
1
= 𝛿ext𝐹(⋅,V(⋅),
[24] so
a fixed point 𝑒𝑛 , but ext 𝛿𝐹(⋅,V(⋅),
Μ‡
Μ‡
V(⋅))
V(⋅))
2
𝑒𝑛 ∈ Δ π‘ƒπ‘’ . Assume that 𝑒𝑛 → 𝑒̂ in 𝐢 (𝐼, R𝑛 ). From Lemma 6,
we obtain
1
1
σ΅„© σΈ€ 
σ΅„©
σ΅„©
σ΅„©σ΅„©
󡄩󡄩𝑒𝑛 (𝑑) − 𝑒 (𝑑)σ΅„©σ΅„©σ΅„© ≤ ∫ [∫ |G (𝑑, 𝜏)| σ΅„©σ΅„©σ΅„©σ΅„©πœ‰ 𝑛 (𝜏) − 𝑆𝑛 (𝜏)σ΅„©σ΅„©σ΅„©σ΅„© π‘‘πœ
0
0
1
σ΅„©
σ΅„©
+ ∫ |G (𝑑, 𝜏)| σ΅„©σ΅„©σ΅„©(𝑆𝑛 (𝜏) − β„Ž (𝜏))σ΅„©σ΅„©σ΅„© π‘‘πœ] 𝑑𝑠.
0
(42)
πœ‰π‘›σΈ€ 
But − 𝑆𝑛 → 0 with respect to the norm β€– ⋅‖𝑀 and from
Lemma 3 we get πœ‰π‘›σΈ€  − 𝑆𝑛 → 0 weakly in 𝐢1 (𝐼, R𝑛 ). So we have
1
σ΅„©
σ΅„©
∫ |G (𝑑, 𝜏)| σ΅„©σ΅„©σ΅„©σ΅„©πœ‰π‘›σΈ€  (𝜏) − 𝑆𝑛 (𝜏)σ΅„©σ΅„©σ΅„©σ΅„© π‘‘πœ 󳨀→ 0.
0
(43)
Moreover, as 𝑛 → ∞ we have
1
𝑒 (𝑑)−𝑒 (𝑑)β€– ≤ ‖𝑒 − 𝑒̂‖𝐢1 (𝐼,R𝑛 ) ∫ |G (𝑑, 𝜏)| (π‘˜1 (𝜏)+π‘˜2 (𝜏)) π‘‘πœ
β€–Μ‚
0
σ΅„©
σ΅„©
≤ ‖𝑒 − 𝑒̂‖𝐢1 (𝐼,R𝑛 ) σ΅„©σ΅„©σ΅„©π‘˜1 (𝜏) + π‘˜2 (𝜏)σ΅„©σ΅„©σ΅„© 𝐢0 .
(44)
Since by assumption (ii), β€– π‘˜1 + π‘˜2 β€– < 1/2𝐢0 , thus from
Lemma 6, we get 𝑒 = 𝑒̂. So 𝑒𝑛 → 𝑒 in 𝐢2 (𝐼, R𝑛 ) and 𝑒 ∈ Δ𝑄𝑒
where the closure is taken in 𝐢2 (𝐼, R𝑛 ) which means that
Δ π‘ƒ ⊆ Δ𝑃𝑒 . If V𝑛 ∈ Δ π‘„ and V𝑛 → V in 𝐢2 (𝐼, R𝑛 ), then
V𝑛 = 𝑓󸀠 (𝑦𝑛 ) for 𝑦𝑛 ∈ 𝛿𝐹1 σΈ€  (⋅,V(⋅),V(⋅))
Μ‡ . From assumption (iii) and
the Dunford-Pettis theorem, {𝑦𝑛 }𝑛∈N is weakly sequentially
compact in 𝐢2 (𝐼, R𝑛 ). By [25, Theorem 3.1], we get
𝑦 (𝑑) ∈ conv lim{𝑦𝑛 (𝑑)}𝑛∈N ⊆ conv lim 𝐹 (𝑑, V𝑛 (𝑑) , V̇𝑛 (𝑑))
= 𝐹 (𝑑, V (𝑑) , VΜ‡ (𝑑))
a.e. on 𝐼.
(45)
Moreover, 𝑓󸀠 (𝑦𝑛 ) → 𝑓󸀠 (𝑦) in 𝐢2 (𝐼, R𝑛 ) for 𝑦 ∈ 𝐢2 (𝐼, R𝑛 )
Μ‡
and 𝑦(𝑑) ∈ 𝐹(𝑑, V(𝑑), V(𝑑))
a.e. on 𝐼. Hence, V ∈ Δ π‘„; that is, Δ π‘„
2
𝑛
is closed in 𝐢 (𝐼, 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.
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