Hindawi Publishing Corporation International Journal of Analysis Volume 2013, Article ID 259418, 7 pages http://dx.doi.org/10.1155/2013/259418
Research Article Asymptotic Stability of Solutions to a Nonlinear Urysohn Quadratic Integral Equation H. H. G. Hashem1,2 and A. R. Al-Rwaily2 1 2
Faculty of Science, Alexandria University, Alexandria, Egypt College of Science & Arts, Qassim University, P.O. Box 6644 Buriadah 81999, Saudi Arabia
Correspondence should be addressed to H. H. G. Hashem;
[email protected] Received 20 October 2012; Revised 1 January 2013; Accepted 17 February 2013 Academic Editor: Seenith Sivasundaram Copyright Š 2013 H. H. G. Hashem and A. R. Al-Rwaily. 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. Here, we prove the existence of đż 1 -nondecreasing solution to a nonlinear quadratic integral equation of Urysohn type by applying the technique of weak noncompactness. Also, the asymptotic stability of solutions for that quadratic integral equation is studied.
1. Introduction Integral equations play an important role in many branches of linear and nonlinear functional analysis and their applications in the theory of elasticity, engineering, mathematical physics, and contact mixed problems, and the theory of integral equations is rapidly developing with the help of several tools of functional analysis, topology, and fixed point theory. For details, we refer to [1â23]. Quadratic integral equations often appear in many applications of real world problems, for example, in the theory of radiative transfer, kinetic theory of gases, in the theory of neutron transport, and in the traffic theory (see [12]). The quadratic integral equation can be very often encountered in many applications (see [1, 2, 6â10, 13â26]). However, in most of the previous literature, the main results are realized with the help of the technique associated with the measure of noncompactness. Instead of using the technique of measure of noncompactness, the Tychonoff fixed point theorem is used for some quadratic integral equations [20, 26]. Picard and Adomian decomposition methods are used to compare approximate and exact solutions for quadratic integral equations [13, 19, 22]. Also, nondecreasing solution of a quadratic integral of Urysohn-Stieltjes type is studied in [10]. Let đż 1 = đż 1 [0, đ] be the class of Lebesgue integrable functions on đź = [0, đ] with the standard norm.
Here, we are concerned with the nonlinear quadratic functional integral equation đĽ (đĄ) = đ (đĄ, đĽ (đ1 (đĄ))) + đ (đĄ, đĽ (đ2 (đĄ))) ĂâŤ
đź(đĄ)
0
đ˘ (đĄ, đ , đĽ (đ3 (đ ))) đđ ,
đĄ â đź,
(1)
and we prove the existence of monotonic solutions in đż 1 by using the technique of measure of noncompactness. The results of this work generalize those obtained in [18]. Finally, the asymptotic stability of solutions for the quadratic integral equation (1) is studied.
2. Preliminaries In this section, we collect some definitions and results needed in our further investigations. Assume that the function đ : đźĂ đ
â đ
satisfies Carath`eodory condition that is measurable in đĄ for any đĽ and continuous in đĽ for almost all đĄ. Then, to every function đĽ(đĄ) being measurable on the interval đź, we may assign the function (đšđĽ) (đĄ) = đ (đĄ, đĽ (đĄ)) ,
đĄ â đź.
(2)
The operator đš defined in such a way is called the superposition operator. This operator is one of the simplest and most important operators investigated in the nonlinear functional
2
International Journal of Analysis
Theorem 1. The superposition operator đš maps đż 1 into itself if and only if óľ¨ óľ¨óľ¨ âđĄ â đź (3) óľ¨óľ¨đ (đĄ, đĽ)óľ¨óľ¨óľ¨ ⤠đ (đĄ) + đ |đĽ|
Theorem 4. Let đ be a nonempty, bounded, closed, and convex subset of đ¸, and let đť : đ â đ be a continuous transformation which is a contraction with respect to the Hausdorff measure of noncompactness đ; that is, there exists a constant đź â [0, 1) such that đ(đťđ) ⤠đźđ(đ) for any nonempty subset đ of đ. Then, đť has at least one fixed point in the set đ.
and đĽ â đ
, where đ(đĄ) is a function from đż 1 and đ is a nonnegative constant.
3. Existence Theorem
analysis. For this operator, we have the following theorem due to Krasnoselâskii [3].
Now, let đ¸ be a Banach space with zero element đ and đ a nonempty bounded subset of đ¸. Moreover denote by đľđ = đľ(đ, đ) the closed ball in đ¸ centered at đ and with radius đ. In the sequel, we will need some criteria for compactness in measure; the complete description of compactness in measure was given by Bana´s [3], but the following sufficient condition will be more convenient for our purposes (see [3]). Theorem 2. Let đ be a bounded subset of đż 1 . Assume that there is a family of subsets (Ίđ )0â¤đâ¤đâđ of the interval (a,b) such that meas Ίđ = đ for every đ â [0, đ â đ], and for every đĽ â đ, đĽ(đĄ1 ) ⤠đĽ(đĄ2 ), (đĄ1 â Ίđ , đĄ2 â Ίđ ); then, the set đ is compact in measure. The measure of weak noncompactness defined by De Blasi [11, 27] is given by đ˝ (đ) = inf (đ > 0; there exists a weakly compact subset đ of đ¸ such that đ â đ + đžđ ) . (4) The function đ˝(đ) possesses several useful properties which may be found in [11]. The convenient formula for the function đ˝(đ) in đż 1 was given by Appell and De Pascale (see [27]) as follows: đ˝ (đ) = lim (sup (sup [⍠|đĽ (đĄ)| đđĄ : đˇ â [đ, đ] , đâ0
đĽâđ
đˇ
(5)
meas đˇ ⤠đ] ) ) , where the symbol meas đˇ stands for Lebesgue measure of the set đˇ. Next, we shall also use the notion of the Hausdorff measure of noncompactness đ (see [3]) defined by đ (đ) = inf (đ > 0; there exists a finite subset đ of đ¸ such that đ â đ + đžđ ) .
(6)
In the case when the set đ is compact in measure, the Hausdorff and De Blasi measures of noncompactness will be identical. Namely, we have the following (see [11, 27]). Theorem 3. Let đ be an arbitrary nonempty bounded subset of đż 1 . If đ is compact in measure, then đ˝(đ) = đ(đ). Finally, we will recall the fixed point theorem due to Bana´s [5].
Let the integral operator đť be defined as (đťđĽ) (đĄ) = âŤ
đź(đĄ)
0
đ˘ (đĄ, đ , đĽ (đ )) đđ ,
(7)
(đšđĽ) (đĄ) = đ (đĄ, đĽ (đĄ)) . Then, (1) may be written in operator form as (đ´đĽ) (đĄ) = (đšđĽ (đ1 )) (đĄ) + (đşđĽ (đ2 )) (đĄ) â
(đťđĽ (đ3 )) (đĄ) , (8) where (đşđĽ)(đĄ) = đ(đĄ, đĽ(đĄ)). Consider the following assumptions. (i) đ, đ : đź Ă đ
â đ
are functions such that đ, đ : đź Ă đ
+ â đ
+ . Moreover, the functions đ, đ satisfy Carath`eodory condition (i.e., are measurable in đĄ for all đĽ â đ
and continuous in đĽ for all đĄ â đź), and there exist two functions đ1 , đ2 â đż 1 and constants đ1 , đ2 > 0 such that óľ¨ óľ¨óľ¨ óľ¨óľ¨đ (đĄ, đĽ)óľ¨óľ¨óľ¨ ⤠đ1 (đĄ) + đ1 |đĽ| , (9) óľ¨óľ¨ óľ¨óľ¨ óľ¨óľ¨đ (đĄ, đĽ)óľ¨óľ¨ ⤠đ2 (đĄ) + đ2 |đĽ| â (đĄ, đĽ) â đź Ă đ
. Apart from this, the functions đ and đ are nondecreasing in both variables. (ii) đ˘ : đź Ă đź Ă đ
â đ
is such that đ˘(đĄ, đ , đĽ) ⼠0 for (đĄ, đ , đĽ) â đź Ă đź Ă đ
+ , and đ˘(đĄ, đ , đĽ) satisfies Carath´eodory condition (i.e., it is measurable in (đĄ, đ ) for all đĽ â đ
and continuous in đĽ for almost all (đĄ, đ ) â đź Ă đź). (iii) There exist a positive constant đ3 , a function đ3 â đż 1 , and a measurable (in both variables) function đ(đĄ, đ ) = đ : đź Ă đź â đ
+ such that |đ˘ (đĄ, đ , đĽ)| ⤠đ (đĄ, đ ) (đ3 (đĄ) + đ3 |đĽ|) âđĄ, đ â đź and for đĽ â đ
, (10) and the integral operator đž, generated by the function đ and defined by đĄ
(đžđĽ) (đĄ) = ⍠đ (đĄ, đ ) đĽ (đ ) đđ , 0
đĄ â đź,
(11)
maps continuously đż 1 into đż â on đź. (iv) đĄ â đ˘(đĄ, đ , đĽ) is a.e. nondecreasing on đź for almost all fixed đ â đź and for each đĽ â đ
+ . (v) đź : đź â đź is continuous.
International Journal of Analysis
3
(vi) đđ : đź â đź, đ = 1, 2, 3, are increasing, absolutely continuous functions on đź, and there exist positive constants đľđ , đ = 1, 2, 3, such that đđó¸ ⼠đľđ a.e. on đź.
đ óľ¨ óľ¨ óľŠ óľŠ đ ⤠óľŠóľŠóľŠđ1 óľŠóľŠóľŠ + 1 ⍠óľ¨óľ¨óľ¨đĽ (đ1 (đĄ))óľ¨óľ¨óľ¨ â
đ1ó¸ (đĄ) đđĄ đľ1 0
(vii) Let đ > â4đđ2 đ3 đľ12 đľ2 đľ3 (||đ1 || + đ â
||đ2 ||||đ3 ||), đ = ||đž||đż â , where đ = đľ1 đľ2 đľ3 â đ1 đľ2 đľ3 â đ2 đđľ1 đľ3 ||đ3 || â đđ3 đľ1 đľ2 ||đ2 ||.
+ ⍠đ2 (đĄ) ⍠đ (đĄ, đ ) đ3 (đ ) đđ đđĄ
0
0
đ
đ
0
0
+
đ đ2 đ2 (đ) óľ¨óľ¨ óľ¨ ó¸ ⍠óľ¨óľ¨đĽ (đ2 (đĄ))óľ¨óľ¨óľ¨ â
đ2 (đĄ) ⍠đ (đĄ, đ ) đ3 (đ ) đđ đđĄ đľ2 đ2 (0) 0
+
đ3 (đ) đ3 đ óľ¨ óľ¨ đ (đĄ, đ ) óľ¨óľ¨óľ¨đĽ (đ3 (đ ))óľ¨óľ¨óľ¨ â
đ3ó¸ (đ ) đđ đđĄ ⍠đ2 (đĄ) ⍠đľ3 0 đ3 (0)
+
đ2 đ3 đ2 (đ) óľ¨óľ¨ óľ¨ ó¸ ⍠óľ¨đĽ (đ2 (đĄ))óľ¨óľ¨óľ¨ â
đ2 (đĄ) đľ2 đľ3 đ2 (0) óľ¨
(14)
ĂâŤ
đ3 (đ)
đ3 (0)
= ⍠|(đ´đĽ) (đĄ)| đđĄ 0
đ
óľ¨ óľ¨ óľ¨ óľ¨ â¤ âŤ óľ¨óľ¨óľ¨đ1 (đĄ)óľ¨óľ¨óľ¨ đđĄ + đ1 ⍠óľ¨óľ¨óľ¨đĽ (đ1 (đĄ))óľ¨óľ¨óľ¨ đđĄ 0 0 đ
óľ¨ óľ¨ + ⍠(đ2 (đĄ) đđĄ + đ2 óľ¨óľ¨óľ¨đĽ (đ2 (đĄ))óľ¨óľ¨óľ¨) 0
đ đđ2 đ3 đ ⍠|đĽ (đ)| đđ â
⍠|đĽ (đ)| đđ đľ2 đľ3 0 0 óľŠ óľŠ óľŠ óľŠ óľŠ óľŠ đđ2 óľŠóľŠóľŠđ3 óľŠóľŠóľŠ óľŠ óľŠ đ ⤠óľŠóľŠóľŠđ1 óľŠóľŠóľŠ + 1 âđĽâ + đ óľŠóľŠóľŠđ2 óľŠóľŠóľŠ óľŠóľŠóľŠđ3 óľŠóľŠóľŠ + âđĽâ đľ1 đľ2 óľŠ óľŠ đđ3 óľŠóľŠóľŠđ2 óľŠóľŠóľŠ đđ2 đ3 + âđĽâ + âđĽâ2 . đľ3 đľ2 đľ3
+
óľ¨ óľ¨ đ (đĄ, đ ) (đ3 (đĄ) + đ3 óľ¨óľ¨óľ¨đĽ (đ3 (đ ))óľ¨óľ¨óľ¨) đđ đđĄ
đ óľŠ óľŠ đ óľ¨ óľ¨ â¤ óľŠóľŠóľŠđ1 óľŠóľŠóľŠ + 1 ⍠óľ¨óľ¨óľ¨đĽ (đ1 (đĄ))óľ¨óľ¨óľ¨ â
đ1ó¸ (đĄ) đđĄ đľ1 0 đ
đź(đĄ)
0
0
+ ⍠đ2 (đĄ) ⍠đ
đ (đĄ, đ ) đ3 (đ ) đđ đđĄ đź(đĄ)
óľ¨ óľ¨ + đ2 ⍠óľ¨óľ¨óľ¨đĽ (đ2 (đĄ))óľ¨óľ¨óľ¨ ⍠0 0 đ
đź(đĄ)
0
0
à ⍠đ2 (đĄ) ⍠đ
óľ¨ óľ¨ đ (đĄ, đ ) óľ¨óľ¨óľ¨đĽ (đ3 (đ ))óľ¨óľ¨óľ¨ đđ đđĄ
óľ¨ óľ¨ + đ2 đ3 ⍠óľ¨óľ¨óľ¨đĽ (đ2 (đĄ))óľ¨óľ¨óľ¨ ⍠0
đ (đĄ, đ ) đ3 (đ ) đđ đđĄ + đ3
đź(đĄ)
0
óľ¨ óľ¨ đ (đĄ, đ ) óľ¨óľ¨óľ¨đĽ (đ3 (đ ))óľ¨óľ¨óľ¨ đđ đđĄ
óľ¨ óľ¨ đ (đĄ, đ ) óľ¨óľ¨óľ¨đĽ (đ3 (đ ))óľ¨óľ¨óľ¨ â
đ3ó¸ (đ ) đđ đđĄ
đ óľŠ óľŠ đ ⤠óľŠóľŠóľŠđ1 óľŠóľŠóľŠ + 1 ⍠|đĽ (đ)| đđ đľ1 0 óľŠ óľŠ đ óľŠ óľŠ óľŠ óľŠ đđ2 óľŠóľŠóľŠđ3 óľŠóľŠóľŠ + đ óľŠóľŠóľŠđ2 óľŠóľŠóľŠ óľŠóľŠóľŠđ3 óľŠóľŠóľŠ + ⍠|đĽ (đ)| đđ đľ2 0 óľŠóľŠ óľŠóľŠ đ đđ3 óľŠóľŠđ2 óľŠóľŠ + ⍠|đĽ (đ)| đđ đľ3 0
đ
đź(đĄ)
đ
+ ⍠đ2 (đĄ) ⍠đ (đĄ, đ ) đ3 (đ ) đđ đđĄ
â(đ´đĽ) (đĄ)â
0
đ
đ1 (đ) óľŠ óľŠ đ óľ¨óľ¨ óľ¨ ó¸ ⤠óľŠóľŠóľŠđ1 óľŠóľŠóľŠ + 1 ⍠óľ¨đĽ (đ1 (đĄ))óľ¨óľ¨óľ¨ â
đ1 (đĄ) đđĄ đľ1 đ1 (0) óľ¨
which implies that
ĂâŤ
đ
đ
óľ¨ óľ¨ đ (đĄ, đ ) (đ3 (đĄ) + đ3 óľ¨óľ¨óľ¨đĽ (đ3 (đ ))óľ¨óľ¨óľ¨) đđ ,
đ
đ
óľ¨ óľ¨ óľ¨ óľ¨ + đ2 đ3 ⍠óľ¨óľ¨óľ¨đĽ (đ2 (đĄ))óľ¨óľ¨óľ¨ ⍠đ (đĄ, đ ) óľ¨óľ¨óľ¨đĽ (đ3 (đ ))óľ¨óľ¨óľ¨ đđ đđĄ 0 0
(13)
Proof. Take an arbitrary đĽ â đż 1 ; then, we get óľ¨ óľ¨ óľ¨ óľ¨ óľ¨ óľ¨ |(đ´đĽ) (đĄ)| ⤠óľ¨óľ¨óľ¨đ1 (đĄ)óľ¨óľ¨óľ¨ + đ1 óľ¨óľ¨óľ¨đĽ (đ1 (đĄ))óľ¨óľ¨óľ¨ + (đ2 (đĄ) + đ2 óľ¨óľ¨óľ¨đĽ (đ2 (đĄ))óľ¨óľ¨óľ¨) 0
0
óľ¨ óľ¨ Ă âŤ đ2 (đĄ) ⍠đ (đĄ, đ ) óľ¨óľ¨óľ¨đĽ (đ3 (đ ))óľ¨óľ¨óľ¨ đđ đđĄ
Theorem 5. Let the assumptions (i)â(vii) be satisfied. If đ1 đľ2 đľ3 + đđ2 đľ1 đľ3 ||đ3 || + đđ2 đ3 đ < đľ1 đľ2 đľ3 , then the quadratic integral equation (1) has at least one solution đĽ â đż 1 which is positive and a.e. nondecreasing on đź.
đź(đĄ)
0
đ
For the existence of at least one đż 1 -positive solution of the quadratic functional integral equation (1), we have the following theorem.
ĂâŤ
đ
óľ¨ óľ¨ + đ2 ⍠óľ¨óľ¨óľ¨đĽ (đ2 (đĄ))óľ¨óľ¨óľ¨ ⍠đ (đĄ, đ ) đ3 (đ ) đđ đđĄ + đ3 0 0
Now, let đ be a positive root of the equation óľŠ óľŠóľŠ óľŠ óľŠ óľŠ đ2 đ3 đľ1 đđ2 â đđ + đľ1 đľ2 đľ3 (óľŠóľŠóľŠđ1 óľŠóľŠóľŠ + đ â
óľŠóľŠóľŠđ2 óľŠóľŠóľŠ óľŠóľŠóľŠđ3 óľŠóľŠóľŠ) = 0, (12) and define the set đľđ = {đĽ â đż 1 : âđĽâ ⤠đ} .
đ
(15) From this estimate, we show that the operator đ´ maps the ball đľđ into itself with
đ=
óľŠ óľŠóľŠ óľŠ óľŠ óľŠ đ â âđ2 â 4đđ2 đ3 đľ12 đľ2 đľ3 (óľŠóľŠóľŠđ1 óľŠóľŠóľŠ + đ â
óľŠóľŠóľŠđ2 óľŠóľŠóľŠ óľŠóľŠóľŠđ3 óľŠóľŠóľŠ) 2đđ2 đ3 đľ1
, (16)
4
International Journal of Analysis đ óľŠ óľŠ óľŠ óľŠ óľŠ óľŠ â¤ óľŠóľŠóľŠđ1 óľŠóľŠóľŠđż 1 (đˇ) + 1 ⍠|đĽ (đ)| đđ + đóľŠóľŠóľŠđ2 óľŠóľŠóľŠđż 1 (đˇ) óľŠóľŠóľŠđ3 óľŠóľŠóľŠđż 1 đľ1 đˇ óľŠ óľŠ đđ2 óľŠóľŠóľŠđ3 óľŠóľŠóľŠđż 1 + ⍠|đĽ (đ)| đđ đľ2 đˇ óľŠóľŠ óľŠóľŠ đđ3 óľŠóľŠđ2 óľŠóľŠđż 1 (đˇ) đ + ⍠|đĽ (đ)| đđ đľ3 0
From assumption (vii) we have óľŠ óľŠóľŠ óľŠ óľŠ óľŠ 0 < đ2 â 4đđ2 đ3 đľ12 đľ2 đľ3 (óľŠóľŠóľŠđ1 óľŠóľŠóľŠ + đ â
óľŠóľŠóľŠđ2 óľŠóľŠóľŠ óľŠóľŠóľŠđ3 óľŠóľŠóľŠ) < đ2 , (17) which implies that
+
óľŠ óľŠóľŠ óľŠ óľŠ óľŠ 0 < âđ2 â 4đđ2 đ3 đľ12 đľ2 đľ3 (óľŠóľŠóľŠđ1 óľŠóľŠóľŠ + đ â
óľŠóľŠóľŠđ2 óľŠóľŠóľŠ óľŠóľŠóľŠđ3 óľŠóľŠóľŠ) < đ. (18)
đ đđ2 đ3 ⍠|đĽ (đ)| đđ â
⍠|đĽ (đ)| đđ đľ2 đľ3 đˇ 0
đ óľŠ óľŠ óľŠ óľŠ óľŠ óľŠ â¤ óľŠóľŠóľŠđ1 óľŠóľŠóľŠđż 1 (đˇ) + 1 âđĽâđż 1 (đˇ) + đóľŠóľŠóľŠđ2 óľŠóľŠóľŠđż 1 (đˇ) óľŠóľŠóľŠđ3 óľŠóľŠóľŠđż 1 đľ1 óľŠ óľŠ đđ2 óľŠóľŠóľŠđ3 óľŠóľŠóľŠđż 1 + âđĽâđż 1 (đˇ) đľ2 óľŠ óľŠ đđ3 óľŠóľŠóľŠđ2 óľŠóľŠóľŠđż 1 (đˇ) đđ2 đ3 + âđĽâ + âđĽâđż 1 (đˇ) â
âđĽâ đľ3 đľ2 đľ3
Then, đ is positive which implies that đ is a positive constant. Now, let đđ denote the subset of đľđ â đż 1 consisting of all functions which are positive and a.e. nondecreasing on đź. The set đđ is nonempty, bounded, convex, and closed (see [3, page 780]). Moreover, this set is compact in measure (see Lemma 2 in [4, page 63]). From the assumptions, we deduce that the operator đ´ maps đđ into itself. Since the operator (đđĽ)(đĄ) = đ˘(đĄ, đ , đĽ) is continuous (Theorem 1 in Section 2), then the operator đť is continuous, and, hence, the product đş.đť is continuous. Also, đš is continuous. Thus, the operator đ´ is continuous on đđ . Let đ be a nonempty subset of đđ . Fix đ > 0, and take a measurable subset đˇ â đź such that meas đˇ ⤠đ. Then, for any đĽ â đ, using the same reasoning as in [3, 4], we get
đ óľŠ óľŠ óľŠ óľŠ óľŠ óľŠ â¤ óľŠóľŠóľŠđ1 óľŠóľŠóľŠđż 1 (đˇ) + 1 âđĽâđż 1 (đˇ) + đóľŠóľŠóľŠđ2 óľŠóľŠóľŠđż 1 (đˇ) óľŠóľŠóľŠđ3 óľŠóľŠóľŠđż 1 đľ1 óľŠ óľŠ đđ2 óľŠóľŠóľŠđ3 óľŠóľŠóľŠđż 1 + âđĽâđż 1 (đˇ) đľ2 óľŠ óľŠ đđđ3 óľŠóľŠóľŠđ2 óľŠóľŠóľŠđż 1 (đˇ) đđđ2 đ3 + + âđĽâđż 1 (đˇ) . đľ3 đľ2 đľ3 (19)
âđ´đĽâđż 1 (đˇ) Since = ⍠|(đ´đĽ) (đĄ)| đđĄ
óľ¨ óľ¨ lim {sup {⍠óľ¨óľ¨óľ¨đđ (đĄ)óľ¨óľ¨óľ¨ đđĄ : đˇ â đź, meas đˇ < đ}} = 0, đˇ
đˇ
đâ0
óľ¨ óľ¨ óľ¨ óľ¨ â¤ âŤ óľ¨óľ¨óľ¨đ1 (đĄ)óľ¨óľ¨óľ¨ đđĄ + đ1 ⍠óľ¨óľ¨óľ¨đĽ (đ1 (đĄ))óľ¨óľ¨óľ¨ đđĄ đˇ đˇ óľ¨ óľ¨ + ⍠(đ2 (đĄ) đđĄ + đ2 óľ¨óľ¨óľ¨đĽ (đ2 (đĄ))óľ¨óľ¨óľ¨) đˇ đź(đĄ)
ĂâŤ
0
óľ¨ óľ¨ đ (đĄ, đ ) (đ3 (đ ) + đ3 óľ¨óľ¨óľ¨đĽ (đ3 (đ ))óľ¨óľ¨óľ¨) đđ đđĄ
đ óľŠ óľŠ óľ¨ óľ¨ â¤ óľŠóľŠóľŠđ1 óľŠóľŠóľŠđż 1 (đˇ) + 1 ⍠óľ¨óľ¨óľ¨đĽ (đ1 (đĄ))óľ¨óľ¨óľ¨ â
đ1ó¸ (đĄ) đđĄ đľ1 đˇ đ
+ ⍠đ2 (đĄ) ⍠đ (đĄ, đ ) đ3 (đ ) đđ đđĄ đˇ
0
đ
óľ¨ óľ¨ + đ2 ⍠óľ¨óľ¨óľ¨đĽ (đ2 (đĄ))óľ¨óľ¨óľ¨ ⍠đ (đĄ, đ ) đ3 (đ ) đđ đđĄ + đđ3 0 đˇ đ
óľ¨ óľ¨ Ă âŤ đ2 (đĄ) ⍠óľ¨óľ¨óľ¨đĽ (đ3 (đ ))óľ¨óľ¨óľ¨ đđ đđĄ đˇ
0
đ
óľ¨ óľ¨ óľ¨ óľ¨ + đđ2 đ3 ⍠óľ¨óľ¨óľ¨đĽ (đ2 (đĄ))óľ¨óľ¨óľ¨ ⍠óľ¨óľ¨óľ¨đĽ (đ3 (đ ))óľ¨óľ¨óľ¨ đđ đđĄ 0 đˇ
(20)
đ = 1, 2, we obtain
óľŠ óľŠ đ1 đđ2 óľŠóľŠóľŠđ3 óľŠóľŠóľŠđż 1 đđ2 đ3 đ ] đ˝ (đĽ (đĄ)) . (21) đ˝ (đ´đĽ (đĄ)) ⤠[ + + đľ1 đľ2 đľ2 đľ3
This implies that óľŠ óľŠ đ1 đđ2 óľŠóľŠóľŠđ3 óľŠóľŠóľŠđż 1 đđ2 đ3 đ đ˝ (đ´đ) ⤠[ + + ] đ˝ (đ) , đľ1 đľ2 đľ2 đľ3
(22)
where đ˝ is the De Blasi measure of weak noncompactness. Keeping in mind Theorem 3, we can write (22) in the form óľŠ óľŠ đ1 đđ2 óľŠóľŠóľŠđ3 óľŠóľŠóľŠđż 1 đđ2 đ3 đ (23) + ] đ (đ) , đ (đ´đ) ⤠[ + đľ1 đľ2 đľ2 đľ3 where đ is the Hausdorff measure of noncompactness. Since (đ1 /đľ1 ) + (đđ2 ||đ3 ||đż 1 /đľ2 ) + (đđ2 đ3 đ/đľ2 đľ3 ) < 1, from Theorem 4 follows that đ´ is contraction with respect to the measure of noncompactness đ. Thus, đ´ has at least one fixed point in đđ which is a solution of the quadratic functional integral equation.
International Journal of Analysis
5 for any đĄ â đź, using (ââ), we have
4. Asymptotic Stability of the Quadratic Integral Equation
đ
We shall show that the solution of the quadratic integral equation (1) is asymptotically stable on R+ .
óľ¨ óľ¨ óľŠ óľŠóľŠ óľŠóľŠđĽ â đŚóľŠóľŠóľŠ = ⍠óľ¨óľ¨óľ¨đĽ (đĄ) â đŚ (đĄ)óľ¨óľ¨óľ¨ đđĄ 0
óľ¨ óľ¨óľ¨ óľ¨óľ¨đĽ (đĄ) â đŚ (đĄ)óľ¨óľ¨óľ¨ ⤠đ.
(27)
Then, óľŠ óľŠóľŠ óľŠóľŠđĽ â đŚóľŠóľŠóľŠ
óľŠ óľŠ óľŠ óľŠ 2 óľŠóľŠ óľŠóľŠ óľŠóľŠ óľŠóľŠ 2đđ2 đ óľŠóľŠóľŠđ3 óľŠóľŠóľŠ 2đđ đ2 đ3 2đđđ3 óľŠóľŠóľŠđ2 óľŠóľŠóľŠ ⤠[2đ óľŠóľŠđ2 óľŠóľŠ óľŠóľŠđ3 óľŠóľŠ + + + ] đľ2 đľ2 đľ3 đľ3
(â) There exist constants đ1 and đ2 satisfying that óľ¨ óľ¨ óľ¨óľ¨ óľ¨ óľ¨óľ¨đ (đĄ, đĽ) â đ (đĄ, đŚ)óľ¨óľ¨óľ¨ ⤠đ1 óľ¨óľ¨óľ¨đĽ â đŚóľ¨óľ¨óľ¨ , óľ¨ óľ¨óľ¨ óľ¨ óľ¨ óľ¨óľ¨đ (đĄ, đĽ) â đ (đĄ, đŚ)óľ¨óľ¨óľ¨ ⤠đ2 óľ¨óľ¨óľ¨đĽ â đŚóľ¨óľ¨óľ¨ ,
óľŠ óľŠ đđ óľŠ óľŠóľŠ óľŠ Ă [óľŠóľŠóľŠđ3 óľŠóľŠóľŠ + 3 ] + 2đ óľŠóľŠóľŠđ2 óľŠóľŠóľŠ óľŠóľŠóľŠđ3 óľŠóľŠóľŠ đľ3 óľŠ óľŠ óľŠ óľŠ 2đđ2 đ óľŠóľŠóľŠđ3 óľŠóľŠóľŠ 2đđ2 đ2 đ3 2đđđ3 óľŠóľŠóľŠđ2 óľŠóľŠóľŠ + + + . đľ2 đľ2 đľ3 đľ3
(24)
Proof. Let đ be defined by (16), and consider the following assumptions.
đ1 óľŠóľŠ óľŠ đđ2 óľŠóľŠ óľŠ óľŠđĽ â đŚóľŠóľŠóľŠ + óľŠđĽ â đŚóľŠóľŠóľŠ đľ1 óľŠ đľ2 óľŠ
â¤
Definition 6. The function đĽ is said to be asymptotically stable solution of (1) if for any đ > 0 there exists đó¸ = đó¸ (đ) > 0 such that for every đĄ ⼠đó¸ and for every other solution đŚ of (1),
(25)
âđĄ â đź, đĽ, đŚ â đ
+ .
óľ¨óľ¨ óľ¨óľ¨ â1 đ1 đđđ3 đ2 đ2 đ óľ¨óľ¨óľ¨óľ¨óľ¨óľ¨đ3 óľ¨óľ¨óľ¨óľ¨óľ¨óľ¨ â
[1 â â â ] đľ1 đľ2 đľ3 đľ2 ⤠đ,
đĄ â đź. (28)
+ 2đđ2 đđľ1 đľ3 ||đ2 || + (ââ) 2đđľ1 đľ2 đľ3 ||đ2 ||||đ3 || 2đđđ3 đľ1 đľ2 ||đ2 || + 2đđ2 đ2 đ3 đľ1 < đ(đľ1 đľ2 đľ3 â đ1 đľ2 đľ3 â đđ2 đľ1 đľ3 ||đ3 || â đđđ2 đ3 đľ1 ). For solutions đĽ = đĽ(đĄ) and đŚ = đŚ(đĄ) of (1) in đľđ , by the assumptions (â) and (ââ), we deduce that óľ¨ óľ¨óľ¨ óľ¨óľ¨đĽ (đĄ) â đŚ (đĄ)óľ¨óľ¨óľ¨ óľ¨ óľ¨ = óľ¨óľ¨óľ¨(đ´đĽ) (đĄ) â (đ´đŚ) (đĄ)óľ¨óľ¨óľ¨ óľ¨ óľ¨ â¤ óľ¨óľ¨óľ¨đ (đĄ, đĽ (đ1 (đĄ))) â đ (đĄ, đŚ (đ1 (đĄ)))óľ¨óľ¨óľ¨ óľ¨ óľ¨ + óľ¨óľ¨óľ¨đ (đĄ, đĽ (đ2 (đĄ))) â đ (đĄ, đŚ (đ2 (đĄ)))óľ¨óľ¨óľ¨ ĂâŤ
đź(đĄ)
0
5. Applications As particular cases of Theorem 5, we can obtain theorems on the existence of positive and a.e. nondecreasing solutions belonging to the space đż 1 (đź) of the following quadratic integral equations. (1) If đź(đĄ) = 1, then we obtain the quadratic integral equation đĽ (đĄ) = đ (đĄ, đĽ (đ1 (đĄ))) + đ (đĄ, đĽ (đ2 (đĄ))) 1
à ⍠đ˘ (đĄ, đ , đĽ (đ3 (đ ))) đđ ,
óľ¨óľ¨ óľ¨ óľ¨óľ¨đ˘ (đĄ, đ , đŚ (đ3 (đ )))óľ¨óľ¨óľ¨ đđ
0
óľ¨óľ¨ óľ¨ óľ¨óľ¨ óľ¨óľ¨đ˘ (đĄ, đ , đŚ (đ3 (đ ))) â đ˘ (đĄ, đ , đĽ (đ3 (đ )))óľ¨óľ¨óľ¨óľ¨ đđ 0 óľ¨óľ¨ óľ¨óľ¨ óľ¨ óľ¨óľ¨ óľ¨óľ¨ ⤠đ1 óľ¨óľ¨đĽ (đ1 (đĄ)) â đŚ (đ1 (đĄ))óľ¨óľ¨ + đ2 óľ¨óľ¨đĽ (đ2 (đĄ)) â đŚ (đ2 (đĄ))óľ¨óľ¨óľ¨ đź(đĄ)
đ
óľ¨ óľ¨ Ă âŤ đ (đĄ, đ ) (đ3 (đ ) + đ3 óľ¨óľ¨óľ¨đŚ (đ3 (đ ))óľ¨óľ¨óľ¨) đđ
(29)
1
đĽ (đĄ) = đ (đĄ) + đ (đĄ, đĽ (đ2 (đĄ))) ⍠đ˘ (đĄ, đ , đĽ (đ3 (đ ))) đđ , 0
(30)
đĄ â đź. (3) If đ(đĄ, đĽ) = đ(đĄ), đ˘(đĄ, đ , đĽ) = â(đĄ, đĽ), đź(đĄ) = 1, and đ(đĄ, đ ) = 1, then we obtain the quadratic integral equation
0
óľ¨ óľ¨ + 2 (đ2 (đĄ) + đ2 óľ¨óľ¨óľ¨đŚ (đ2 (đĄ))óľ¨óľ¨óľ¨)
1
đ
óľ¨ óľ¨ Ă âŤ đ (đĄ, đ ) (đ3 (đ ) + đ3 óľ¨óľ¨óľ¨đĽ (đ3 (đ ))óľ¨óľ¨óľ¨) đđ ; 0
đĄ â đź.
(2) If đź(đĄ) = 1 and đ(đĄ, đĽ) = đ(đĄ), then we obtain the quadratic integral equation
óľ¨ óľ¨ + óľ¨óľ¨óľ¨đ (đĄ, đŚ (đ2 (đĄ)))óľ¨óľ¨óľ¨ ĂâŤ
That is, the solution đĽ = đĽ(đĄ) of (1) is asymptotically stable on đ
+ . This completes the proof.
đĽ (đĄ) = đ (đĄ) + ⍠â (đ , đĽ (đ3 (đ ))) đđ , 0
(26)
which was proved by Bana´s in [4].
đĄ â đź,
(31)
6
International Journal of Analysis (4) If đ(đĄ, đĽ) = 0, then we obtain the functional equation đĽ (đĄ) = đ (đĄ, đĽ (đ1 (đĄ))) ,
đĄ â đź,
(32)
which is the same results proved by Bana´s in [3]. (5) If đ(đĄ, đĽ) = đ(đĄ), and đ˘(đĄ, đ , đĽ) = đ(đĄ, đ )â(đĄ, đĽ), then we obtain the quadratic integral equation 1
đĽ (đĄ) = đ (đĄ) + đ (đĄ, đĽ (đĄ)) ⍠đ (đĄ, đ ) â (đ , đĽ (đ3 (đ ))) đđ , 0
(33)
đĄ â đź, which is the same result proved in [16]. (6) If đ(đĄ, đĽ) = đ(đĄ), đ˘(đĄ, đ , đĽ) = â(đĄ, đĽ), and đź(đĄ) = đĄ, then we obtain the quadratic integral equation đĄ
đĽ (đĄ) = đ (đĄ) + đ (đĄ, đĽ (đĄ)) ⍠â (đ , đĽ (đ3 (đ ))) đđ , 0
đĄ â đź, (34)
which is the same result proved in [18]. Example 7. Let us consider the quadratic integral equation of Urysohn type having the form đĽ (đĄ) = đ (đĄ) + đĽ (đĄ) âŤ
1
0
đĄ đ˘ (đĄ, đ , đĽ (đ )) đđ , đĄ+đ
đĄ â [0, 1] . (35)
This equation represents the Hammerstein counterpart of the famous Chandrasekhar quadratic integral equation which has numerous application (cf. [1, 2, 6, 24]). It arose originally in connection with scattering through a homogeneous semiinfinite plane atmosphere [24]. In case đ(đĄ) = 1 and đ˘(đĄ, đ , đĽ(đ )) = đđ(đ )đĽ(đ ), đ is a positive constant. Then, (35) has the form đĽ (đĄ) = 1 + đđĽ (đĄ) âŤ
1
0
đĄđ (đ ) đĽ (đ ) đđ . đĄ+đ
(36)
In order to apply our results, we have to impose an additional condition that the so-called âcharacteristicâ function đ is continuous on đź. In this case, đ = (1ââ1 â 4đđ1 )/2đđ, and the assumption (vii) may be reduced to 4đđ1 ⤠1 where supđ âđź đ(đ ) = đ1 . Example 8. Consider the following quadratic functional integral equation: 1 1 đĽ (sin (đĄ2 + 3đĄ))] đĽ (đĄ) = đĽ (đĄ) + [đĄ + 6 3+đĄ đĄ
à ⍠[1 + 0
1 đĽ (sin (đ 2 + 4đ ))] đđ đĄ â [0, 1] . 3+đ (37)
Taking 1 đ (đĄ, đĽ) = đĽ (đĄ) , 6
đ (đĄ, đĽ) = 1 +
đ˘ (đĄ, đ , đĽ) = đĄ + then we can easily deduce that
1 đĽ, 3+đĄ
1 đĽ, 3+đĄ
(38)
(i) |đ˘(đĄ, đ , đĽ)| ⤠1 + (1/4)|đĽ| and |đ(đĄ, đĽ)| ⤠đĄ + (1/4)|đĽ| ( i.e., đź(đĄ) = đĄ, đ1 (đĄ) = 0, đ2 (đĄ) = đĄ, and đ3 (đĄ) = 1 which implies that ||đ1 || = 0, ||đ2 || = ||đ3 || = 1, and đ1 = 1/6, đ2 = đ3 = 1/4); (ii) đ1 (đĄ) = đĄ, đ2 (đĄ) = sin(đĄ2 + 3đĄ), and đ3 (đĄ) = sin(đĄ2 + 4đĄ), and then đ1ó¸ (đĄ) = 1, đ2ó¸ (đĄ) = (2đĄ + 3) cos(đĄ2 + 3đĄ) > 2, and đ3ó¸ (đĄ) = (2đĄ + 4) cos(đĄ2 + 4đĄ) > 3 (i.e., đľ1 = 1/2, đľ2 = 2, đľ3 = 3, and đ = 1). Now, we will calculate đ. Then, đ = 2.30228 > 0 and (đ1 /đľ1 ) + (đđ2 ||đ3 ||đż 1 /đľ2 ) + (đđ2 đ3 đ/đľ2 đľ3 ) = 0.48231546246258117 < 1. Thus, all the assumptions of Theorem 5 are satisfied; so, the quadratic functional integral equation (37) possesses at least one solution being positive, a.e. nondecreasing, and integrable in [0, 1].
Acknowledgments This work is supported by Deanship for Scientific Research, Qassim University. The authors express their gratitude to Deanship for Scientific Research, Qassim University, for their hospitality and their support. The authors are thankful to Professor A. M. A. El-Sayed for his help and encouragement.
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