Research Article Solvability of a Fourth-Order Boundary Value Problem with

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Hindawi Publishing Corporation
Journal of Applied Mathematics
Volume 2013, Article ID 782363, 7 pages
http://dx.doi.org/10.1155/2013/782363
Research Article
Solvability of a Fourth-Order Boundary Value Problem with
Integral Boundary Conditions
Hui Li, Libo Wang, and Minghe Pei
Department of Mathematics, Beihua University, Jilin City 132013, China
Correspondence should be addressed to Minghe Pei; peiminghe@163.com
Received 21 December 2012; Accepted 13 February 2013
Academic Editor: Meng Fan
Copyright © 2013 Hui Li et al. 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 investigate the existence of solutions and positive solutions for a nonlinear fourth-order differential equation with inte1
gral boundary conditions of the form π‘₯(4) (𝑑) = 𝑓(𝑑, π‘₯(𝑑), π‘₯σΈ€  (𝑑), π‘₯σΈ€ σΈ€  (𝑑), π‘₯σΈ€ σΈ€ σΈ€  (𝑑)), 𝑑 ∈ [0, 1], π‘₯(0) = π‘₯σΈ€  (1) = 0, π‘₯σΈ€ σΈ€  (0) = ∫0 β„Ž(𝑠, π‘₯(𝑠),
σΈ€ 
σΈ€ σΈ€ 
σΈ€ σΈ€ σΈ€ 
4
3
π‘₯ (𝑠), π‘₯ (𝑠))d𝑠, π‘₯ (1) = 0, where 𝑓 ∈ 𝐢([0, 1] × R ), β„Ž ∈ 𝐢([0, 1] × R ). By using a fixed point theorem due to D. O’Regan, the
existence of solutions and positive solutions for the previous boundary value problems is obtained. Meanwhile, as applications,
some examples are given to illustrate our results.
1. Introduction
with the integral boundary conditions
It is well known that fourth-order boundary value problems
(BVPs) arise in a variety of different areas of the flexibility
mechanics and engineering physics and thus have been extensively studied; for instance, see [1–29] and references therein.
Boundary value problems with integral boundary conditions
appear in heat conduction, thermoelasticity, chemical engineering underground water flow, and plasma physics; see [12,
14, 21, 24, 26, 29] and references therein.
Motivated by the previous works and [30], in this paper,
we consider fully nonlinear fourth-order differential equation
π‘₯(4) (𝑑) = 𝑓 (𝑑, π‘₯ (𝑑) , π‘₯σΈ€  (𝑑) , π‘₯σΈ€ σΈ€  (𝑑) , π‘₯σΈ€ σΈ€ σΈ€  (𝑑)) ,
𝑑 ∈ [0, 1] ,
(1)
subject to the integral boundary conditions
π‘₯ (0) = π‘₯σΈ€  (1) = 0,
1
π‘₯σΈ€ σΈ€  (0) = ∫ β„Ž (𝑠, π‘₯ (𝑠) , π‘₯σΈ€  (𝑠) , π‘₯σΈ€ σΈ€  (𝑠)) d𝑠,
0
(2)
π‘₯σΈ€ σΈ€ σΈ€  (1) = 0,
1
π‘₯σΈ€ σΈ€  (0) = ∫ β„Ž (𝑠, π‘₯ (𝑠)) d𝑠,
0
(4)
π‘₯σΈ€ σΈ€ σΈ€  (1) = 0,
where 𝑓 and β„Ž are continuous functions.
We notice that if β„Ž ≡ 0 in problems (1), (2) and (3), (4),
then the models are known as the one endpoint simply supported and the other one sliding clamped beam. The study of
this class of problems was considered by some authors via
various methods; we refer the reader to the papers [2, 5, 8,
11, 22].
The aim of this paper is to establish the existence results
of solutions and positive solutions for problems (1), (2) and
(3), (4), respectively. By positive solution, we mean a solution
π‘₯(𝑑) such that π‘₯(𝑑) > 0 for 𝑑 ∈ (0, 1]. Our main tool is the
fixed point theorem due to D. O’Regan [31].
2. Preliminary
as well as its simplified form
π‘₯(4) (𝑑) = 𝑓 (𝑑, π‘₯ (𝑑)) ,
π‘₯ (0) = π‘₯σΈ€  (1) = 0,
𝑑 ∈ [0, 1] ,
(3)
In this section, we present some lemmas which are needed for
our main results.
2
Journal of Applied Mathematics
Let 𝐢[0, 1] denote the Banach space of real-valued continuous functions on [0, 1] with the norm ||π‘₯||0 := max𝑑∈[0,1] |π‘₯(𝑑)|.
𝐢𝑛 [0, 1] is the Banach space of 𝑛 times continuously differentiable functions defined on [0, 1], with the norm ||π‘₯||𝐢𝑛 :=
max{||π‘₯(𝑖) ||0 , 𝑖 = 0, 1, . . . , 𝑛}.
Throughout this paper, we always assume that 𝑓 : [0, 1] ×
R4 → R = (−∞, +∞) (or [0, 1]×R → R) and β„Ž : [0, 1]×R3 → R
(or [0, 1] × R → R) are continuous.
We consider a priori bound of solutions of the following
one-parameter family of boundary value problem:
π‘₯(4) (𝑑) = πœ†π‘“ (𝑑, π‘₯ (𝑑) , π‘₯σΈ€  (𝑑) , π‘₯σΈ€ σΈ€  (𝑑) , π‘₯σΈ€ σΈ€ σΈ€  (𝑑)) ,
𝑑 ∈ [0, 1] ,
(5)
σΈ€ 
π‘₯ (0) = π‘₯ (1) = 0,
1
π‘₯σΈ€ σΈ€  (0) = πœ† ∫ β„Ž (𝑠, π‘₯ (𝑠) , π‘₯σΈ€  (𝑠) , π‘₯σΈ€ σΈ€  (𝑠)) d𝑠,
0
(6)
(𝐻π‘₯) (𝑑) = β„Ž (𝑑, π‘₯ (𝑑) , π‘₯σΈ€  (𝑑) , π‘₯σΈ€ σΈ€  (𝑑)) ,
𝑑 ∈ [0, 1] .
(11)
Also, define an operator 𝑇 : 𝐢3 [0, 1] → 𝐢[0, 1] × R4 as
1
(𝑇π‘₯) (𝑑) = ((𝐹π‘₯) (𝑑) , 0, 0, ∫ (𝐻π‘₯) (𝑠) d𝑠, 0) .
0
(12)
Simple computations yield the following lemma.
Lemma 2. BVP (5), (6) is equivalent to the abstract equation
π‘₯ = πœ†πΏ−1 𝑇π‘₯
(13)
in 𝐢3 [0, 1]; that is, π‘₯ ∈ 𝐢4 [0, 1] is a solution of BVP (5), (6) if
and only if π‘₯ ∈ 𝐢3 [0, 1] is a solution of the integral equation
1
1
0
0
π‘₯ (𝑑) = πœ† [∫ 𝐺 (𝑑, 𝑠) (𝐹π‘₯) (𝑠) d𝑠 + ∫ πœ‘ (𝑑, π‘₯ (𝑠)) d𝑠] , (14)
σΈ€ σΈ€ σΈ€ 
π‘₯ (1) = 0,
where 0 ≤ πœ† ≤ 1. Simple computations lead to the following
lemma.
Lemma 1. BVP (5), (6) with πœ† = 0 has only the trivial solution,
and the corresponding Green function 𝐺(𝑑, 𝑠) exists and is given
by
{
{
(𝑠 −
{
{
𝐺 (𝑑, 𝑠) = {
{
{
{(𝑠 −
{
and 𝐻 : 𝐢3 [0, 1] → 𝐢[0, 1] induced by β„Ž as
where πœ‘(𝑑, π‘₯(𝑠)) = 𝑔(𝑑)(𝐻π‘₯)(𝑠).
Let us denote the operators 𝑃1 , 𝑃2 as
1
(𝑃1 π‘₯) (𝑑) = ∫ 𝐺 (𝑑, 𝑠) (𝐹π‘₯) (𝑠) d𝑠,
0
1
𝑑3
1 2
𝑠 )𝑑 − ,
2
6
(𝑃2 π‘₯) (𝑑) = ∫ πœ‘ (𝑑, π‘₯ (𝑠)) d𝑠.
0 ≤ 𝑑 ≤ 𝑠 ≤ 1;
𝑑3 1
1 2
𝑠 ) 𝑑 − + (𝑑 − 𝑠)3 , 0 ≤ 𝑠 ≤ 𝑑 ≤ 1.
2
6 6
(7)
0
(15)
(16)
Then, 𝐿−1 𝑇 can be written as
𝐿−1 𝑇 = 𝑃1 + 𝑃2 .
(17)
Now, define a linear operator 𝐿 : 𝐢4 [0, 1] → 𝐢[0, 1] × R4
Now, we can easily give some properties of the Green
function 𝐺(𝑑, 𝑠) and 𝑔(𝑑) by direct computation.
(𝐿π‘₯) (𝑑) = (π‘₯(4) (𝑑) , π‘₯ (0) , π‘₯σΈ€  (1) , π‘₯σΈ€ σΈ€  (0) , π‘₯σΈ€ σΈ€ σΈ€  (1)) ,
Lemma 3. Let 𝐺(𝑑, 𝑠) be as in Lemma 1 and 𝑔(𝑑) = (1/2)𝑑2 − 𝑑.
Then,
by
𝑑 ∈ [0, 1] .
(8)
(1) 0 ≤ 𝐺(𝑑, 𝑠) ≤ max0≤𝑑,𝑠≤1 𝐺(𝑑, 𝑠) = 1/3, 𝑑, 𝑠 ∈ [0, 1];
Then, we can easily show that 𝐿 is a Fredholm operator with
index zero, and its inverse 𝐿−1 : 𝐢[0, 1]×R4 → 𝐢4 [0, 1] is given
by
1
𝐿−1 (𝑦, π‘Ž, 𝑏, 𝑐, 𝑑) (𝑑) = ∫ 𝐺 (𝑑, 𝑠) 𝑦 (𝑠) d𝑠 + π‘Ž + 𝑏𝑑 + 𝑐𝑔 (𝑑)
0
1
1
+ d ( 𝑑3 − 𝑑) ,
6
2
𝑑 ∈ [0, 1] ,
(9)
where 𝑔(𝑑) = (1/2)𝑑 − 𝑑.
Define Nemytskii operators 𝐹 : 𝐢3 [0, 1] → 𝐢[0, 1] induced
by 𝑓 as
σΈ€ σΈ€ 
σΈ€ σΈ€ σΈ€ 
(𝐹π‘₯) (𝑑) = 𝑓 (𝑑, π‘₯ (𝑑) , π‘₯ (𝑑) , π‘₯ (𝑑) , π‘₯ (𝑑)) ,
𝑑 ∈ [0, 1] ,
(10)
πœ•
) 𝐺 (𝑑, 𝑠)
πœ•π‘‘
{𝑠 − ( 1 ) 𝑠2 − ( 1 ) 𝑑2 , 0 ≤ 𝑑 ≤ 𝑠 ≤ 1;
={
2
2
𝑠
−
𝑑𝑠,
0 ≤ 𝑠 ≤ 𝑑 ≤ 1;
{
0≥(
2
σΈ€ 
0≤(
(18)
πœ•2
) 𝐺 (𝑑, 𝑠)
πœ•π‘‘2
−𝑑,
={
−𝑠,
0 ≤ 𝑑 ≤ 𝑠 ≤ 1;
0 ≤ 𝑠 ≤ 𝑑 ≤ 1;
(19)
(2) 𝑔(𝑑) ≤ 0, 𝑔󸀠 (𝑑) ≤ 0, 𝑔󸀠󸀠 (𝑑) = 1, 𝑔󸀠󸀠󸀠 (𝑑) = 0, 𝑑 ∈ [0, 1];
(3) ||𝑔||0 = 1/2, ||𝑔󸀠 ||0 = 1, ||𝑔󸀠󸀠 ||0 = 1, ||𝑔󸀠󸀠󸀠 ||0 = 0,
||𝑔||𝐢3 = 1.
Journal of Applied Mathematics
3
Lemma 4. Suppose that
(i) for each fixed (𝑑, π‘₯2 , π‘₯3 ) ∈ [0, 1] × R2 , 𝑓(𝑑, π‘₯0 , π‘₯1 , π‘₯2 ,
π‘₯3 ) is nondecreasing in π‘₯0 and π‘₯1 ;
(ii) there exists a constant 𝑀 > 0 such that for |π‘₯| > 𝑀,
𝑑 ∈ [0, 1],
π‘₯𝑓 (𝑑, −π‘₯, −π‘₯, π‘₯, 0) > 0;
󡄨󡄨
󡄨
σ΅„¨σ΅„¨β„Ž (𝑑, π‘₯0 , π‘₯1 , π‘₯2 ) − β„Ž (𝑑, 𝑦0 , 𝑦1 , 𝑦2 )󡄨󡄨󡄨
󡄨
󡄨
≤ 𝜎 (max {󡄨󡄨󡄨π‘₯𝑖 − 𝑦𝑖 󡄨󡄨󡄨 , 𝑖 = 0, 1, 2})
(21)
for all (𝑑, π‘₯0 , π‘₯1 , π‘₯2 ), (𝑑, 𝑦0 , 𝑦1 , 𝑦2 ) ∈ [0, 1] × R3 .
Then, any solution π‘₯ = π‘₯(𝑑) of BVP (5), (6) satisfies
(22)
−1
where π‘Ÿ = (1 − 𝛽) ||β„Ž(⋅, 0, 0, 0)||0 .
π‘₯σΈ€ σΈ€  (𝑑1 ) , 0) > 0.
(27)
We may assume that π‘₯σΈ€ σΈ€  (𝑑1 ) > 0; then, π‘₯(4) (𝑑1 ) > 0. Thus, by
the continuity of π‘₯(4) (𝑑) on [0, 1], there exists 𝛿 > 0 such that
π‘₯(4) (𝑑) > 0 for 𝑑 ∈ (𝑑1 − 𝛿, 𝑑1 ] ⊂ [0, 1]. Since π‘₯σΈ€ σΈ€ σΈ€  (𝑑1 ) = 0,
it follows that π‘₯σΈ€ σΈ€ σΈ€  (𝑑) < 0 for 𝑑 ∈ (𝑑1 − 𝛿, 𝑑1 ]; namely, π‘₯σΈ€ σΈ€  (𝑑) is
decreasing on (𝑑1 −𝛿, 𝑑1 ], which contradicts the fact that π‘₯σΈ€ σΈ€  (𝑑)
attains its positive maximum value at 𝑑 = 𝑑1 . In summary,
inequality (23) is true, which implies from π‘₯(0) = π‘₯σΈ€  (1) = 0
that
𝑖 = 0, 1, 𝑑 ∈ [0, 1] .
(28)
This completes the proof of the lemma.
Remark 5. In Lemma 4, if condition (i) is replaced by
(iσΈ€  ), there exists a constant 𝑀 > 0 such that whenever
|π‘₯2 | > 𝑀 and all (𝑑, π‘₯0 , π‘₯1 ) ∈ [0, 1] × R2 ,
Proof. Let us first show that
∀𝑑 ∈ [0, 1] .
(23)
Note that if πœ† = 0 in (5) and (6), then BVP (5), (6) has only the
trivial solution, and thus (23) holds. Hence, we may assume
that πœ† ∈ [0, 1]. Suppose now that (23) is not true. Then, there
exists 𝑑0 ∈ [0, 1] such that |π‘₯σΈ€ σΈ€  (𝑑0 )| > 𝑀 + π‘Ÿ. Let
󡄨
󡄨
󡄨
󡄨
𝐾 := 󡄨󡄨󡄨󡄨π‘₯σΈ€ σΈ€  (𝑑1 )󡄨󡄨󡄨󡄨 = max 󡄨󡄨󡄨󡄨π‘₯σΈ€ σΈ€  (𝑑)󡄨󡄨󡄨󡄨 .
𝑑∈[0,1]
(24)
Then, 𝐾 > 𝑀 + π‘Ÿ, and from π‘₯(0) = π‘₯σΈ€  (1) = 0, we have
󡄨󡄨 (𝑖) 󡄨󡄨
󡄨󡄨π‘₯ (𝑑)󡄨󡄨 ≤ 𝐾,
󡄨
󡄨
≥ πœ†π‘₯σΈ€ σΈ€  (𝑑1 ) 𝑓 (𝑑1 , −π‘₯σΈ€ σΈ€  (𝑑1 ) , −π‘₯σΈ€ σΈ€  (𝑑1 ) ,
󡄨󡄨 (𝑖) 󡄨󡄨
󡄨󡄨π‘₯ (𝑑)󡄨󡄨 ≤ 𝑀 + π‘Ÿ,
󡄨
󡄨
𝑖 = 0, 1, 2, 𝑑 ∈ [0, 1] ,
󡄨󡄨 σΈ€ σΈ€  󡄨󡄨
󡄨󡄨π‘₯ (𝑑)󡄨󡄨 ≤ 𝑀 + π‘Ÿ,
󡄨
󡄨
π‘₯σΈ€ σΈ€  (𝑑1 ) π‘₯(4) (𝑑1 ) = πœ†π‘₯σΈ€ σΈ€  (𝑑1 ) 𝑓 (𝑑1 , π‘₯ (𝑑1 ) , π‘₯σΈ€  (𝑑1 ) , π‘₯σΈ€ σΈ€  (𝑑1 ) , 0)
(20)
(iii) there exist 𝛽 ∈ (0, 1) and nondecreasing continuous
function 𝜎 : [0, +∞) → [0, +∞) such that 𝜎(𝑒) ≤ 𝛽𝑒
for 𝑒 > 0, and
󡄨󡄨 (𝑖) 󡄨󡄨
󡄨󡄨π‘₯ (𝑑)󡄨󡄨 ≤ 𝑀 + π‘Ÿ,
󡄨
󡄨
which is a contradiction, and thus 𝑑1 ∈ (0, 1]. Furthermore,
by definition of 𝑑1 and (6), we have π‘₯σΈ€ σΈ€ σΈ€  (𝑑1 ) = 0. Hence, from
assumptions (i) and (ii) and (25), we have
𝑖 = 0, 1, ∀𝑑 ∈ [0, 1] .
(25)
σΈ€ σΈ€ 
It is easy to see that 𝑑1 ∈ [0, 1]. In fact, if 𝑑1 = 0, then |π‘₯ (0)| =
𝐾. From (6) and (iii), it follows that for some 𝜁 ∈ [0, 1],
󡄨󡄨 1
󡄨󡄨
󡄨
󡄨
󡄨
󡄨
𝐾 = 󡄨󡄨󡄨󡄨π‘₯σΈ€ σΈ€  (0)󡄨󡄨󡄨󡄨 = πœ† 󡄨󡄨󡄨󡄨∫ β„Ž (𝑠, π‘₯ (𝑠) , π‘₯σΈ€  (𝑠) , π‘₯σΈ€ σΈ€  (𝑠)) d𝑠󡄨󡄨󡄨󡄨
󡄨󡄨 0
󡄨󡄨
󡄨
󡄨
≤ σ΅„¨σ΅„¨σ΅„¨σ΅„¨β„Ž (𝜁, π‘₯ (𝜁) , π‘₯σΈ€  (𝜁) , π‘₯σΈ€ σΈ€  (𝜁))󡄨󡄨󡄨󡄨
󡄨
󡄨
≤ σ΅„¨σ΅„¨σ΅„¨σ΅„¨β„Ž (𝜁, π‘₯ (𝜁) , π‘₯σΈ€  (𝜁) , π‘₯σΈ€ σΈ€  (𝜁)) − β„Ž (𝜁, 0, 0, 0)󡄨󡄨󡄨󡄨
󡄨
󡄨
+ σ΅„¨σ΅„¨σ΅„¨β„Ž (𝜁, 0, 0, 0)󡄨󡄨󡄨
π‘₯2 𝑓 (𝑑, π‘₯0 , π‘₯1 , π‘₯2 , 0) > 0;
(29)
then, the conclusion of Lemma 4 remains true.
The following fixed point result due to D. O’Regan plays
a crucial role.
Lemma 6 (see [31]). Let π‘ˆ be an open set in a closed, convex
set 𝐢 of a Banach space 𝐸. Assume that 0 ∈ π‘ˆ, 𝑃(π‘ˆ) is bounded,
and 𝑃 : π‘ˆ → 𝐢 is given by 𝑃 = 𝑃1 + 𝑃2 , where 𝑃1 : π‘ˆ → 𝐸 is
continuous and completely continuous and 𝑃2 : π‘ˆ → 𝐸 is a
nonlinear contraction. Then, either
(A1 ) 𝑃 has a fixed point in π‘ˆ, or
(A2 ) there is a point 𝑒 ∈ πœ•π‘ˆ and πœ† ∈ (0, 1) with 𝑒 = πœ†π‘ƒ(𝑒).
3. Main Results
Firstly in this section, we state and prove our existence results
of solutions for BVP (1), (2).
Theorem 7. Suppose that
(i) for each fixed (𝑑, π‘₯2 , π‘₯3 ) ∈ [0, 1] × R2 , 𝑓(𝑑, π‘₯0 , π‘₯1 , π‘₯2 ,
π‘₯3 ) is nondecreasing in π‘₯0 and π‘₯1 ;
(ii) there exists a constant 𝑀 > 0 such that for |π‘₯| > 𝑀,
𝑑 ∈ [0, 1],
≤ 𝛽𝐾 + (1 − 𝛽) π‘Ÿ
< 𝛽𝐾 + (1 − 𝛽) 𝐾 = 𝐾,
(26)
π‘₯𝑓 (𝑑, −π‘₯, −π‘₯, π‘₯, 0) > 0;
(30)
4
Journal of Applied Mathematics
(iii) there exist 𝛽 ∈ (0, 1) and nondecreasing continuous
function 𝜎 : [0, +∞) → [0, +∞) such that 𝜎(𝑒) ≤ 𝛽𝑒
for 𝑒 > 0, and
󡄨
󡄨󡄨
σ΅„¨σ΅„¨β„Ž (𝑑, π‘₯0 , π‘₯1 , π‘₯2 ) − β„Ž (𝑑, 𝑦0 , 𝑦1 , 𝑦2 )󡄨󡄨󡄨
󡄨
󡄨
≤ 𝜎 (max {󡄨󡄨󡄨π‘₯𝑖 − 𝑦𝑖 󡄨󡄨󡄨 , 𝑖 = 0, 1, 2})
(31)
for all (𝑑, π‘₯0 , π‘₯1 , π‘₯2 ), (𝑑, 𝑦0 , 𝑦1 , 𝑦2 ) ∈ [0, 1] × R3 ;
(iv) 𝑓(𝑑, π‘₯0 , π‘₯1 , π‘₯2 , π‘₯3 ) satisfies the Nagumo condition; that
is, there exists a positive-valued continuous function
+∞
Φ(𝑠) on [0, +∞) with ∫0 (𝑠d𝑠/Φ(𝑠)) = +∞ such that
󡄨 󡄨
󡄨󡄨
󡄨
󡄨󡄨𝑓 (𝑑, π‘₯0 , π‘₯1 , π‘₯2 , π‘₯3 )󡄨󡄨󡄨 ≤ Φ (󡄨󡄨󡄨π‘₯3 󡄨󡄨󡄨)
−1
(33)
Then, BVP (1), (2) has at least one solution.
Proof. Let π‘₯ be a possible solution of BVP (5), (6). We now
show that
󡄨󡄨 σΈ€ σΈ€ σΈ€  󡄨󡄨
󡄨󡄨π‘₯ (𝑑)󡄨󡄨 ≤ 𝑁,
󡄨
󡄨
𝑑 ∈ [0, 1] ,
(34)
𝑁
0
where 𝑁 := max{𝑁0 , 2(𝑀 + π‘Ÿ)} and ∫𝑀+π‘Ÿ
(𝑠d𝑠/Φ(𝑠)) = 2(𝑀 +
π‘Ÿ) + 1.
Suppose that (34) is not true. Then, there exists 𝑑1 ∈ [0, 1)
such that |π‘₯σΈ€ σΈ€ σΈ€  (𝑑1 )| > 𝑁. Since π‘₯σΈ€ σΈ€ σΈ€  (1) = 0, then there exists πœ‰,
πœ‚ (𝑑1 < πœ‰ < πœ‚ < 1) such that
󡄨󡄨 σΈ€ σΈ€ σΈ€  󡄨󡄨
󡄨󡄨 σΈ€ σΈ€ σΈ€  󡄨󡄨
󡄨󡄨π‘₯ (πœ‚)󡄨󡄨 = 𝑀 + π‘Ÿ,
󡄨󡄨π‘₯ (πœ‰)󡄨󡄨 = 𝑁,
󡄨
󡄨
󡄨
󡄨
󡄨󡄨 σΈ€ σΈ€ σΈ€  󡄨󡄨
𝑀 + π‘Ÿ < 󡄨󡄨󡄨π‘₯ (𝑑)󡄨󡄨󡄨 < 𝑁, ∀𝑑 ∈ (πœ‰, πœ‚) .
(35)
Therefore, π‘₯σΈ€ σΈ€ σΈ€  (𝑑) is positive or negative on (πœ‰, πœ‚) by the
continuity of the π‘₯σΈ€ σΈ€ σΈ€  (𝑑). Hence, from assumption (iv), the
definition of 𝑁, and Lemma 4, we can get the following
contradiction:
𝑁
𝑠d𝑠
𝑠d𝑠
≤∫
𝑀+π‘Ÿ Φ (𝑠)
𝑀+π‘Ÿ Φ (𝑠)
󡄨
󡄨󡄨 πœ‰ σΈ€ σΈ€ σΈ€ 
󡄨 π‘₯ (𝑑) π‘₯(4) (𝑑) d𝑑 󡄨󡄨󡄨
≤ 󡄨󡄨󡄨󡄨∫
󡄨 󡄨󡄨
󡄨
󡄨󡄨 πœ‚ Φ (󡄨󡄨󡄨π‘₯σΈ€ σΈ€ σΈ€  (𝑑)󡄨󡄨󡄨) 󡄨󡄨󡄨
2 (𝑀 + π‘Ÿ) + 1 = ∫
Consequently, from Lemma 3, we have
σ΅„¨σ΅„¨σ΅„¨πœ‘ (𝑑, π‘₯ (𝑠)) − πœ‘ (𝑑, 𝑦 (𝑠))󡄨󡄨󡄨 = 󡄨󡄨󡄨𝑔 (𝑑) (𝐻π‘₯) (𝑠) − 𝑔 (𝑑) (𝐻𝑦) (𝑠)󡄨󡄨󡄨
󡄨
󡄨 󡄨
󡄨
σ΅„©σ΅„© σ΅„©σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©
≤ 󡄩󡄩𝑔󡄩󡄩0 𝜎 (σ΅„©σ΅„©π‘₯ − 𝑦󡄩󡄩𝐢3 )
1 σ΅„©
σ΅„©
≤ 𝛽󡄩󡄩󡄩π‘₯ − 𝑦󡄩󡄩󡄩𝐢3 ,
2
𝑁0
𝑑, 𝑠 ∈ [0, 1] ,
∀π‘₯, 𝑦 ∈ 𝐢3 [0, 1] .
(38)
(32)
for all (𝑑, π‘₯0 , π‘₯1 , π‘₯2 , π‘₯3 ) ∈ [0, 1] × [−𝑀 − π‘Ÿ, 𝑀 + π‘Ÿ]3 × R,
where
π‘Ÿ = (1 − 𝛽) β€–β„Ž (⋅, 0, 0, 0)β€–0 .
We now show that 𝑃2 : Ω → 𝐢3 [0, 1] is a nonlinear contraction. In fact, from assumption (iii), we have
󡄨󡄨󡄨(𝐻π‘₯) (𝑑) − (𝐻𝑦) (𝑑)󡄨󡄨󡄨 ≤ 𝜎 (σ΅„©σ΅„©σ΅„©π‘₯ − 𝑦󡄩󡄩󡄩 3 ) ,
󡄩𝐢
σ΅„©
󡄨
󡄨
(37)
3
𝑑 ∈ [0, 1] , ∀π‘₯, 𝑦 ∈ 𝐢 [0, 1] .
Similarly, for all π‘₯, 𝑦 ∈ 𝐢3 [0, 1],
󡄨󡄨
󡄨
󡄨󡄨 πœ•πœ‘ (𝑑, π‘₯ (𝑠)) πœ•πœ‘ (𝑑, 𝑦 (𝑠)) 󡄨󡄨󡄨 σ΅„©σ΅„© σΈ€  σ΅„©σ΅„©
󡄨󡄨
󡄨󡄨 ≤ 󡄩󡄩𝑔 σ΅„©σ΅„© 𝜎 (σ΅„©σ΅„©σ΅„©σ΅„©π‘₯ − 𝑦󡄩󡄩󡄩󡄩𝐢3 )
−
󡄨󡄨
󡄨󡄨 σ΅„© σ΅„©0
πœ•π‘‘
πœ•π‘‘
󡄨
󡄨
σ΅„©
σ΅„©
≤ 𝛽󡄩󡄩󡄩π‘₯ − 𝑦󡄩󡄩󡄩𝐢3 , 𝑑, 𝑠 ∈ [0, 1] ,
󡄨󡄨󡄨 πœ•2 πœ‘ (𝑑, π‘₯ (𝑠)) πœ•2 πœ‘ (𝑑, 𝑦 (𝑠)) 󡄨󡄨󡄨 σ΅„© σΈ€ σΈ€  σ΅„©
󡄨󡄨 ≤ 󡄩󡄩𝑔 σ΅„©σ΅„© 𝜎 (σ΅„©σ΅„©σ΅„©π‘₯ − 𝑦󡄩󡄩󡄩 3 )
󡄨󡄨
−
󡄨󡄨 σ΅„©σ΅„© σ΅„©σ΅„©0 σ΅„©
󡄨󡄨
󡄩𝐢
2
2
πœ•π‘‘
πœ•π‘‘
󡄨󡄨
󡄨󡄨
σ΅„©
σ΅„©
≤ 𝛽󡄩󡄩󡄩π‘₯ − 𝑦󡄩󡄩󡄩𝐢3 , 𝑑, 𝑠 ∈ [0, 1] ,
󡄨󡄨󡄨 πœ•3 πœ‘ (𝑑, π‘₯ (𝑠)) πœ•3 πœ‘ (𝑑, 𝑦 (𝑠)) 󡄨󡄨󡄨
󡄨󡄨 = 0, 𝑑, 𝑠 ∈ [0, 1] .
󡄨󡄨
−
󡄨󡄨
󡄨󡄨
πœ•π‘‘3
πœ•π‘‘3
󡄨󡄨
󡄨󡄨
(39)
Hence,
σ΅„©σ΅„©
σ΅„©σ΅„©
󡄩󡄩𝑃2 π‘₯ − 𝑃2 𝑦󡄩󡄩𝐢3
σ΅„©σ΅„©
(𝑖)
(𝑖) σ΅„©
σ΅„©
= max {σ΅„©σ΅„©σ΅„©(𝑃2 π‘₯) − (𝑃2 𝑦) σ΅„©σ΅„©σ΅„© , 𝑖 = 0, 1, 2, 3} (40)
σ΅„©0
σ΅„©
σ΅„©σ΅„©
σ΅„©σ΅„©
3
≤ 𝛽󡄩󡄩π‘₯ − 𝑦󡄩󡄩𝐢3 , ∀π‘₯, 𝑦 ∈ 𝐢 [0, 1] .
Since all possible solutions of BVP (5), (6) satisfy ||π‘₯||𝐢3 ≤
𝑁 < 𝑅, it follows that there is no π‘₯ ∈ πœ•Ω and πœ† ∈ (0, 1) such
that π‘₯ = πœ†πΏ−1 𝑇π‘₯. We conclude that (A2 ) of Lemma 6 does not
hold. Consequently, 𝐿−1 𝑇 = 𝑃1 + 𝑃2 has a fixed point, which
is a solution of BVP (1), (2). This completes the proof of the
theorem.
Remark 8. In Theorem 7, if condition (i) is replaced by
(36)
πœ‚
󡄨
󡄨
󡄨
󡄨
≤ ∫ 󡄨󡄨󡄨󡄨π‘₯σΈ€ σΈ€ σΈ€  (𝑑)󡄨󡄨󡄨󡄨 d𝑑 = 󡄨󡄨󡄨󡄨π‘₯σΈ€ σΈ€  (πœ‚) − π‘₯σΈ€ σΈ€  (πœ‰)󡄨󡄨󡄨󡄨
πœ‰
≤ 2 (𝑀 + π‘Ÿ) .
Therefore, inequality (34) holds.
Let Ω := {π‘₯ ∈ 𝐢3 [0, 1] : ||π‘₯||𝐢3 < 𝑁 + 1 =: 𝑅}. It follows
easily from the properties of the Green function and the continuity of 𝑓 that the operator 𝑃1 : Ω → 𝐢3 [0, 1] is completely
continuous.
(iσΈ€  ) there exists a constant 𝑀 > 0 such that whenever
|π‘₯2 | > 𝑀 and all (𝑑, π‘₯0 , π‘₯1 ) ∈ [0, 1] × R2 ,
π‘₯2 𝑓 (𝑑, π‘₯0 , π‘₯1 , π‘₯2 , 0) > 0,
(41)
then the conclusion of Theorem 7 remains true.
Remark 9. In Theorem 7, if 𝑓 ≥ 0 ≥ β„Ž and 𝑓(𝑑, 0, 0, 0, 0) ≡ΜΈ 0,
then all the solutions of BVP (1), (2) are monotone and positive. This is clear because by Lemma 3 we have π‘₯ = 𝑃1 π‘₯+𝑃2 π‘₯ ≥
0, π‘₯σΈ€  = (𝑃1 π‘₯)σΈ€  + (𝑃2 π‘₯)σΈ€  ≥ 0 and π‘₯σΈ€ σΈ€  = (𝑃1 π‘₯)σΈ€ σΈ€  + (𝑃2 π‘₯)σΈ€ σΈ€  ≤ 0.
Next, we consider the existence of solutions and positive
solutions for BVP (3), (4).
Journal of Applied Mathematics
5
Theorem 10. Suppose that
(i) there exists Ψ : [0, +∞) → [0, +∞) being continuous
and nondecreasing such that
󡄨
󡄨󡄨
(42)
󡄨󡄨𝑓 (𝑑, π‘₯)󡄨󡄨󡄨 ≤ Ψ (|π‘₯|) , ∀ (𝑑, π‘₯) ∈ [0, 1] × R;
(ii) there exists 𝛽 ∈ (0, 2) such that
󡄨
󡄨󡄨
σ΅„¨σ΅„¨β„Ž (𝑑, π‘₯) − β„Ž (𝑑, 𝑦)󡄨󡄨󡄨
󡄨
󡄨
≤ 𝛽 󡄨󡄨󡄨π‘₯ − 𝑦󡄨󡄨󡄨 , ∀ (𝑑, π‘₯, 𝑦) ∈ [0, 1] × R2 ;
(43)
which contradicts (iii). Hence, (A2 ) of Lemma 6 does not
hold, and consequently 𝐿−1 𝑇 = 𝑃1 +𝑃2 has a fixed point which
is a solution of BVP (3), (4). This completes the proof of the
theorem.
Remark 11. In Theorem 10, if 𝑓 ≥ 0 ≥ β„Ž and 𝑓(𝑑, 0) ≡ΜΈ 0, then
all the solutions of BVP (3), (4) are monotone and positive.
Now, we consider BVP (3), (4) with linear boundary conditions as
β„Ž (𝑑, π‘₯ (𝑑)) = 𝑙 (𝑑) π‘₯ (𝑑) ,
(iii) there exists 𝛾 > 0 such that
𝐾 (𝑑, 𝑠) = 𝑔 (𝑑) 𝑙 (𝑠) ,
(44)
1
(𝑃2 π‘₯) (𝑑) = ∫ 𝐾 (𝑑, 𝑠) π‘₯ (𝑠) d𝑠.
Then, BVP (3), (4) has at least one solution.
0
Proof. It is easy to see that π‘₯ ∈ 𝐢4 [0, 1] is a solution of BVP
(3), (4) if and only if π‘₯ ∈ 𝐢[0, 1] is a solution of the integral
equation (14) with πœ† = 1. Moreover, 𝑃1 is completely continuous, and 𝑃2 is a nonlinear contraction.
It follows from (15), (i), and Lemma 3 that ∀π‘₯ ∈ 𝐢[0, 1],
1
󡄨
󡄨󡄨
󡄨󡄨(𝑃1 π‘₯) (𝑑)󡄨󡄨󡄨 ≤ ∫ 𝐺 (𝑑, 𝑠) Ψ (|π‘₯ (𝑠)|) d𝑠
0
1
≤ Ψ (β€–π‘₯β€–0 ) ,
3
(𝑑, 𝑠) ∈ [0, 1] × [0, 1] .
1
(i) 𝐾0 := (1/2) ∫0 |𝑙(𝑠)|d𝑠 < 1;
(ii) there exists Ψ : [0, +∞) → [0, +∞) being continuous
and nondecreasing such that
󡄨
󡄨󡄨
󡄨󡄨𝑓 (𝑑, π‘₯)󡄨󡄨󡄨 ≤ Ψ (|π‘₯|) ,
(45)
lim sup
𝜌 → +∞
Also, (16), (ii), and Lemma 3 yield
(52)
Theorem 12. Suppose that
𝑑 ∈ [0, 1] .
∀ (𝑑, π‘₯) ∈ [0, 1] × R,
Ψ (𝜌)
< 3 (1 − 𝐾0 ) .
𝜌
(53)
Then, the nonlinear fourth-order differential equation (3) with
boundary conditions
1
󡄨
󡄨
󡄨󡄨
󡄨
󡄨󡄨(𝑃2 π‘₯) (𝑑)󡄨󡄨󡄨 ≤ ∫ 󡄨󡄨󡄨𝑔 (𝑑) (𝐻π‘₯) (𝑠)󡄨󡄨󡄨 d𝑠
0
π‘₯ (0) = π‘₯σΈ€  (1) = 0,
1
σ΅„© σ΅„©
≤ 󡄩󡄩󡄩𝑔󡄩󡄩󡄩0 ∫ (|β„Ž (𝑠, π‘₯ (𝑠)) − β„Ž (𝑠, 0)| + |β„Ž (𝑠, 0)|) d𝑠
1
π‘₯σΈ€ σΈ€  (0) = ∫ 𝑙 (𝑠) π‘₯ (𝑠) d𝑠,
0
0
∀π‘₯ ∈ 𝐢 [0, 1] , 𝑑 ∈ [0, 1] .
(46)
From (14), (45), and (46), we have that all possible solutions
of π‘₯ = πœ†(𝑃1 + 𝑃2 )π‘₯ satisfy
1
1
|π‘₯ (𝑑)| ≤ Ψ (β€–π‘₯β€–0 ) + (𝛽‖π‘₯β€–0 + β„Ž0 ) ,
3
2
(51)
Then,
where β„Ž0 = max0≤𝑑≤1 |β„Ž(𝑑, 0)|.
1
(𝛽‖π‘₯β€–0 + β„Ž0 ) ,
2
(50)
where 𝑙(⋅) ∈ 𝐢[0, 1]. Define
Ψ (𝛾) + (3/2) β„Ž0
1
< 3 (1 − 𝛽) ,
𝛾
2
≤
𝑑 ∈ [0, 1] ,
𝑑 ∈ [0, 1] .
(47)
Let Ω := {π‘₯ ∈ 𝐢[0, 1] : ||π‘₯||0 < 𝛾}. Then, Ω is open in
𝐢[0, 1], 0 ∈ Ω, and (𝑃1 + 𝑃2 )(Ω) is bounded. Suppose that
π‘₯ ∈ πœ•Ω and πœ† ∈ (0, 1) satisfy π‘₯ = πœ†(𝑃1 +𝑃2 )π‘₯. Then, ||π‘₯||0 = 𝛾,
and (i) and (47) lead to
1
1
𝛾 ≤ Ψ (𝛾) + (𝛽𝛾 + β„Ž0 ) ;
3
2
(48)
Ψ (𝛾) + (3/2) β„Ž0
1
≥ 3 (1 − 𝛽) ,
𝛾
2
(49)
that is,
(54)
π‘₯σΈ€ σΈ€ σΈ€  (1) = 0
has at least one solution.
Proof. Notice that the existence of solutions of BVP (3), (54)
is equivalent to the existence of fixed points of operator equation
π‘₯ = 𝑃1 π‘₯ + 𝑃2 π‘₯.
(55)
As a linear operator on 𝐢[0, 1], from (52) and (i), we get
||𝑃2 || = 𝐾0 < 1, which implies that 𝐼 − 𝑃2 is invertible and its
inverse is given by
−1
(𝐼 − 𝑃2 )
∞
= ∑ 𝑃2𝑛
𝑛=0
1
σ΅„©
−1 σ΅„©
with σ΅„©σ΅„©σ΅„©σ΅„©(𝐼 − 𝑃2 ) σ΅„©σ΅„©σ΅„©σ΅„© ≤
.
1 − 𝐾0
(56)
Hence, we see from (55) that π‘₯ is a solution of BVP (3), (54)
if and only if π‘₯ is a fixed point of the completely continuous
operator 𝑆 = (𝐼 − 𝑃2 )−1 𝑃1 .
6
Journal of Applied Mathematics
Let us show that there exists 𝜌∗ > 0 such that any solution
π‘₯ of operator equation π‘₯ = πœ†π‘†π‘₯ (πœ† ∈ (0, 1)) satisfies ||π‘₯||0 < 𝜌∗ .
In fact, any solution π‘₯ of π‘₯ = πœ†π‘†π‘₯ (πœ† ∈ (0, 1)) satisfies
−1
1
π‘₯ (𝑑) = πœ†(𝐼 − 𝑃2 ) ∫ 𝐺 (𝑑, 𝑠) 𝑓 (𝑠, π‘₯ (𝑠)) d𝑠,
(57)
0
1
Ψ (β€–π‘₯β€–0 ) .
3 (1 − 𝐾0 )
1
Ψ (𝜌) ,
3 (1 − 𝐾0 )
∀𝜌 ≥ 𝜌∗ .
(59)
Comparing (58) and (59), we see that ||π‘₯||0 < 𝜌∗ .
Now, let Ω = {π‘₯ ∈ 𝐢[0, 1] : ||π‘₯||0 < 𝜌∗ }. By the LeraySchauder continuation theorem 𝑆 has a fixed point in Ω,
which is a solution of BVP (3), (54). This completes the proof
of the theorem.
Remark 13. In Theorem 12, if 𝑓 ≥ 0 ≥ 𝑙 and 𝑓(𝑑, 0) ≡ΜΈ 0, then
all the solutions of BVP (3), (54) are monotone and positive
since all the solutions of BVP (3), (54) satisfy
π‘₯ (𝑑) =
∞
1
( ∑ 𝑃2𝑛 ) ∫
0
𝑛=0
𝐺 (𝑑, 𝑠) 𝑓 (𝑠, π‘₯ (𝑠)) d𝑠 ≥ 0
on [0, 1] ,
σΈ€ 
σΈ€ 
(𝑑))
σΈ€ σΈ€ 
2
+ (π‘₯σΈ€ σΈ€ σΈ€  (𝑑)) ,
1 1√
2
∫ 1 + (π‘₯σΈ€ σΈ€  (𝑠)) d𝑠,
2 0
where π‘ž(𝑑) ∈ 𝐢([0, 1], [0, (1/8)]).
Let
𝑓 (𝑑, π‘₯) = π‘ž (𝑑) π‘₯2 + 1
on [0, 1] × R,
3
1
ln
2 1 + π‘₯2
on [0, 1] × R,
β„Ž (𝑑, π‘₯) =
1
Ψ (π‘₯) = π‘₯2 + 1 on [0, +∞) ,
8
3
𝛽= ,
2
(67)
𝛾 = 3.
(63)
3
1
π‘₯σΈ€ σΈ€  (0) = ∫ (𝑠2 − 4𝑠) π‘₯ (𝑠) d𝑠,
0
𝑓 (𝑑, π‘₯) = π‘ž (𝑑) √π‘₯2 + 1
3
𝑑∈[0,1]
𝑙 (𝑑) = 𝑑2 − 4𝑑
2
1
𝑓 (𝑑, π‘₯0 , π‘₯1 , π‘₯2 , π‘₯3 ) = 𝑑2 π‘₯03 + π‘₯15 + π‘₯2 𝑒π‘₯2 + π‘₯32
2
on [0, 1] × R4 ,
on [0, +∞) .
(68)
(69)
π‘₯σΈ€ σΈ€ σΈ€  (1) = 0,
3
on [0, 1] × R3 ,
𝑑 ∈ [0, 1] ,
π‘₯ (0) = π‘₯σΈ€  (1) = 0,
on [0, 1] × R,
Ψ (π‘₯) = ( max π‘ž (𝑑)) √π‘₯2 + 1
Let
1
β„Ž (𝑑, π‘₯0 , π‘₯1 , π‘₯2 ) = √1 + π‘₯22
2
π‘₯(4) (𝑑) = π‘ž (𝑑) √(π‘₯ (𝑑))2 + 1,
where π‘ž(𝑑) ∈ 𝐢([0, 1], [0, +∞)).
Let
π‘₯σΈ€ σΈ€ σΈ€  (1) = 0.
1
𝜎 (𝑒) = 𝑒
2
π‘₯σΈ€ σΈ€ σΈ€  (1) = 0,
𝑑 ∈ [0, 1] ,
π‘₯ (0) = π‘₯σΈ€  (1) = 0,
π‘₯σΈ€ σΈ€  (0) =
(66)
Example 16. Consider the fourth-order boundary value problem
σΈ€ σΈ€ 
2
1
3 1
d𝑠,
∫ ln
2 0 1 + (π‘₯ (𝑠))2
π‘₯σΈ€ σΈ€  = (𝑃1 π‘₯) + (𝑃2 π‘₯) ≤ 0.
(61)
Example 14. Consider the fourth-order boundary value problem
5
1
π‘₯(4) (𝑑) = 𝑑2 (π‘₯ (𝑑))3 + (π‘₯σΈ€  (𝑑))
2
(62)
σΈ€ σΈ€ 
π‘₯σΈ€ σΈ€  (0) =
It is easy to check that all the assumptions in Theorem 10 and
Remark 11 are satisfied. Hence, BVP (65), (66) has at least one
monotone positive solution.
Finally, we give some examples to illustrate our results.
+ π‘₯σΈ€ σΈ€  (𝑑) 𝑒(π‘₯
(65)
(60)
and thus
π‘₯σΈ€  = (𝑃1 π‘₯) + (𝑃2 π‘₯) ≥ 0,
𝑑 ∈ [0, 1] ,
π‘₯ (0) = π‘₯σΈ€  (1) = 0,
(58)
The condition lim sup𝜌 → +∞ (Ψ(𝜌)/𝜌) < 3(1−𝐾0 ) implies that
there exists 𝜌∗ > 0 such that (Ψ(𝜌)/𝜌) < 3(1 − 𝐾0 ) for all
𝜌 ≥ 𝜌∗ ; that is,
𝜌>
Example 15. Consider the fourth-order boundary value problem
π‘₯(4) (𝑑) = π‘ž (𝑑) (π‘₯(𝑑))2 + 1,
and, hence, by (ii) and Lemma 3, we have
β€–π‘₯β€–0 ≤
It is easy to check that all the assumptions in Theorem 7 are
satisfied. Hence, BVP (62), (63) has at least one solution.
(64)
on [0, +∞) ,
(70)
on [0, 1] .
It is easy to check that all the assumptions in Theorem 12 and
Remark 13 are satisfied. Hence, BVP (68), (69) has at least one
monotone positive solution.
Acknowledgment
This work was supported by NSFC (11126339).
Journal of Applied Mathematics
References
[1] R. P. Agarwal and Y. M. Chow, “Iterative methods for a fourth
order boundary value problem,” Journal of Computational and
Applied Mathematics, vol. 10, no. 2, pp. 203–217, 1984.
[2] Z. Bai, “The upper and lower solution method for some fourthorder boundary value problems,” Nonlinear Analysis. Theory,
Methods & Applications, vol. 67, no. 6, pp. 1704–1709, 2007.
[3] A. Cabada and F. M. Minhós, “Fully nonlinear fourth-order
equations with functional boundary conditions,” Journal of
Mathematical Analysis and Applications, vol. 340, no. 1, pp. 239–
251, 2008.
[4] M. A. Del Pino and R. F. Manásevich, “Existence for a fourthorder boundary value problem under a two-parameter nonresonance condition,” Proceedings of the American Mathematical
Society, vol. 112, no. 1, pp. 81–86, 1991.
[5] J. Du and M. Cui, “Constructive proof of existence for a class of
fourth-order nonlinear BVPs,” Computers & Mathematics with
Applications, vol. 59, no. 2, pp. 903–911, 2010.
[6] J. Ehme, P. W. Eloe, and J. Henderson, “Upper and lower solution methods for fully nonlinear boundary value problems,”
Journal of Differential Equations, vol. 180, no. 1, pp. 51–64, 2002.
[7] D. Franco, D. O’Regan, and J. Perán, “Fourth-order problems
with nonlinear boundary conditions,” Journal of Computational
and Applied Mathematics, vol. 174, no. 2, pp. 315–327, 2005.
[8] H. Feng, D. Ji, and W. Ge, “Existence and uniqueness of solutions for a fourth-order boundary value problem,” Nonlinear
Analysis. Theory, Methods & Applications, vol. 70, no. 10, pp.
3561–3566, 2009.
[9] J. R. Graef and L. Kong, “A necessary and sufficient condition
for existence of positive solutions of nonlinear boundary value
problems,” Nonlinear Analysis. Theory, Methods & Applications,
vol. 66, no. 11, pp. 2389–2412, 2007.
[10] M. R. Grossinho and St. A. Tersian, “The dual variational principle and equilibria for a beam resting on a discontinuous nonlinear elastic foundation,” Nonlinear Analysis. Theory, Methods
& Applications, vol. 41, no. 3-4, pp. 417–431, 2000.
[11] C. P. Gupta, “Existence and uniqueness theorems for the bending of an elastic beam equation,” Applicable Analysis, vol. 26, no.
4, pp. 289–304, 1988.
[12] T. Jankowski, “Positive solutions for fourth-order differential
equations with deviating arguments and integral boundary conditions,” Nonlinear Analysis. Theory, Methods & Applications,
vol. 73, no. 5, pp. 1289–1299, 2010.
[13] D. Jiang, W. Gao, and A. Wan, “A monotone method for constructing extremal solutions to fourth-order periodic boundary
value problems,” Applied Mathematics and Computation, vol.
132, no. 2-3, pp. 411–421, 2002.
[14] P. Kang, Z. Wei, and J. Xu, “Positive solutions to fourthorder singular boundary value problems with integral boundary
conditions in abstract spaces,” Applied Mathematics and Computation, vol. 206, no. 1, pp. 245–256, 2008.
[15] Y. Li, “Positive solutions of fourth-order boundary value problems with two parameters,” Journal of Mathematical Analysis
and Applications, vol. 281, no. 2, pp. 477–484, 2003.
[16] X.-L. Liu and W.-T. Li, “Existence and multiplicity of solutions
for fourth-order boundary value problems with three parameters,” Mathematical and Computer Modelling, vol. 46, no. 3-4,
pp. 525–534, 2007.
[17] Y. Liu, “Multiple positive solutions of nonlinear singular boundary value problem for fourth-order equations,” Applied Mathematics Letters, vol. 17, no. 7, pp. 747–757, 2004.
7
[18] S. Lu and S. Jin, “Existence of periodic solutions for a fourthorder P-Laplacian equation with a deviating argument,” Journal
of Computational and Applied Mathematics, vol. 230, no. 2, pp.
513–520, 2009.
[19] T. F. Ma, “Positive solutions for a beam equation on a nonlinear
elastic foundation,” Mathematical and Computer Modelling, vol.
39, no. 11-12, pp. 1195–1201, 2004.
[20] R. Ma and J. Xu, “Bifurcation from interval and positive solutions of a nonlinear fourth-order boundary value problem,”
Nonlinear Analysis. Theory, Methods & Applications, vol. 72, no.
1, pp. 113–122, 2010.
[21] R. Ma and T. Chen, “Existence of positive solutions of fourthorder problems with integral boundary conditions,” Boundary
Value Problems, vol. 2011, Article ID 297578, 17 pages, 2011.
[22] F. Minhós, T. Gyulov, and A. I. Santos, “Lower and upper solutions for a fully nonlinear beam equation,” Nonlinear Analysis.
Theory, Methods & Applications, vol. 71, no. 1-2, pp. 281–292,
2009.
[23] P. K. Palamides, “Uniqueness of monotone positive solutions
for singular boundary value problems,” Communications on
Applied Nonlinear Analysis, vol. 9, no. 3, pp. 79–89, 2002.
[24] P. Pietramala, “A note on a beam equation with nonlinear
boundary conditions,” Boundary Value Problems, vol. 2011,
Article ID 376782, 14 pages, 2011.
[25] M. Pei and S. K. Chang, “Monotone iterative technique and
symmetric positive solutions for a fourth-order boundary value
problem,” Mathematical and Computer Modelling, vol. 51, no. 910, pp. 1260–1267, 2010.
[26] J. R. L. Webb, G. Infante, and D. Franco, “Positive solutions
of nonlinear fourth-order boundary-value problems with local
and non-local boundary conditions,” Proceedings of the Royal
Society of Edinburgh A, vol. 138, no. 2, pp. 427–446, 2008.
[27] Z. Wei, “A class of fourth order singular boundary value
problems,” Applied Mathematics and Computation, vol. 153, no.
3, pp. 865–884, 2004.
[28] Q. Yao, “Positive solutions for eigenvalue problems of fourthorder elastic beam equations,” Applied Mathematics Letters, vol.
17, no. 2, pp. 237–243, 2004.
[29] X. Zhang and W. Ge, “Positive solutions for a class of boundaryvalue problems with integral boundary conditions,” Computers
& Mathematics with Applications, vol. 58, no. 2, pp. 203–215,
2009.
[30] A. Boucherif, S. M. Bouguima, N. Al-Malki, and Z. Benbouziane, “Third order differential equations with integral
boundary conditions,” Nonlinear Analysis. Theory, Methods &
Applications, vol. 71, no. 12, pp. e1736–e1743, 2009.
[31] D. O’Regan, “Fixed-point theory for the sum of two operators,”
Applied Mathematics Letters, vol. 9, no. 1, pp. 1–8, 1996.
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