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) (π‘) = π(π‘, π₯(π‘), π₯σΈ (π‘), π₯σΈ σΈ (π‘), π₯σΈ σΈ σΈ (π‘)), π‘ ∈ [0, 1], π₯(0) = π₯σΈ (1) = 0, π₯σΈ σΈ (0) = ∫0 β(π , π₯(π ), σΈ σΈ σΈ σΈ σΈ σΈ 4 3 π₯ (π ), π₯ (π ))dπ , π₯ (1) = 0, where π ∈ πΆ([0, 1] × R ), β ∈ πΆ([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) (π‘) = π (π‘, π₯ (π‘) , π₯σΈ (π‘) , π₯σΈ σΈ (π‘) , π₯σΈ σΈ σΈ (π‘)) , π‘ ∈ [0, 1] , (1) subject to the integral boundary conditions π₯ (0) = π₯σΈ (1) = 0, 1 π₯σΈ σΈ (0) = ∫ β (π , π₯ (π ) , π₯σΈ (π ) , π₯σΈ σΈ (π )) dπ , 0 (2) π₯σΈ σΈ σΈ (1) = 0, 1 π₯σΈ σΈ (0) = ∫ β (π , π₯ (π )) dπ , 0 (4) π₯σΈ σΈ σΈ (1) = 0, where π and β are continuous functions. We notice that if β ≡ 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₯(π‘) such that π₯(π‘) > 0 for π‘ ∈ (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) (π‘) = π (π‘, π₯ (π‘)) , π₯ (0) = π₯σΈ (1) = 0, π‘ ∈ [0, 1] , (3) In this section, we present some lemmas which are needed for our main results. 2 Journal of Applied Mathematics Let πΆ[0, 1] denote the Banach space of real-valued continuous functions on [0, 1] with the norm ||π₯||0 := maxπ‘∈[0,1] |π₯(π‘)|. πΆπ [0, 1] is the Banach space of π times continuously differentiable functions defined on [0, 1], with the norm ||π₯||πΆπ := max{||π₯(π) ||0 , π = 0, 1, . . . , π}. Throughout this paper, we always assume that π : [0, 1] × R4 → R = (−∞, +∞) (or [0, 1]×R → R) and β : [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) (π‘) = ππ (π‘, π₯ (π‘) , π₯σΈ (π‘) , π₯σΈ σΈ (π‘) , π₯σΈ σΈ σΈ (π‘)) , π‘ ∈ [0, 1] , (5) σΈ π₯ (0) = π₯ (1) = 0, 1 π₯σΈ σΈ (0) = π ∫ β (π , π₯ (π ) , π₯σΈ (π ) , π₯σΈ σΈ (π )) dπ , 0 (6) (π»π₯) (π‘) = β (π‘, π₯ (π‘) , π₯σΈ (π‘) , π₯σΈ σΈ (π‘)) , π‘ ∈ [0, 1] . (11) Also, define an operator π : πΆ3 [0, 1] → πΆ[0, 1] × R4 as 1 (ππ₯) (π‘) = ((πΉπ₯) (π‘) , 0, 0, ∫ (π»π₯) (π ) dπ , 0) . 0 (12) Simple computations yield the following lemma. Lemma 2. BVP (5), (6) is equivalent to the abstract equation π₯ = ππΏ−1 ππ₯ (13) in πΆ3 [0, 1]; that is, π₯ ∈ πΆ4 [0, 1] is a solution of BVP (5), (6) if and only if π₯ ∈ πΆ3 [0, 1] is a solution of the integral equation 1 1 0 0 π₯ (π‘) = π [∫ πΊ (π‘, π ) (πΉπ₯) (π ) dπ + ∫ π (π‘, π₯ (π )) dπ ] , (14) σΈ σΈ σΈ π₯ (1) = 0, where 0 ≤ π ≤ 1. Simple computations lead to the following lemma. Lemma 1. BVP (5), (6) with π = 0 has only the trivial solution, and the corresponding Green function πΊ(π‘, π ) exists and is given by { { (π − { { πΊ (π‘, π ) = { { { {(π − { and π» : πΆ3 [0, 1] → πΆ[0, 1] induced by β as where π(π‘, π₯(π )) = π(π‘)(π»π₯)(π ). Let us denote the operators π1 , π2 as 1 (π1 π₯) (π‘) = ∫ πΊ (π‘, π ) (πΉπ₯) (π ) dπ , 0 1 π‘3 1 2 π )π‘ − , 2 6 (π2 π₯) (π‘) = ∫ π (π‘, π₯ (π )) dπ . 0 ≤ π‘ ≤ π ≤ 1; π‘3 1 1 2 π ) π‘ − + (π‘ − π )3 , 0 ≤ π ≤ π‘ ≤ 1. 2 6 6 (7) 0 (15) (16) Then, πΏ−1 π can be written as πΏ−1 π = π1 + π2 . (17) Now, define a linear operator πΏ : πΆ4 [0, 1] → πΆ[0, 1] × R4 Now, we can easily give some properties of the Green function πΊ(π‘, π ) and π(π‘) by direct computation. (πΏπ₯) (π‘) = (π₯(4) (π‘) , π₯ (0) , π₯σΈ (1) , π₯σΈ σΈ (0) , π₯σΈ σΈ σΈ (1)) , Lemma 3. Let πΊ(π‘, π ) be as in Lemma 1 and π(π‘) = (1/2)π‘2 − π‘. Then, by π‘ ∈ [0, 1] . (8) (1) 0 ≤ πΊ(π‘, π ) ≤ max0≤π‘,π ≤1 πΊ(π‘, π ) = 1/3, π‘, π ∈ [0, 1]; Then, we can easily show that πΏ is a Fredholm operator with index zero, and its inverse πΏ−1 : πΆ[0, 1]×R4 → πΆ4 [0, 1] is given by 1 πΏ−1 (π¦, π, π, π, π) (π‘) = ∫ πΊ (π‘, π ) π¦ (π ) dπ + π + ππ‘ + ππ (π‘) 0 1 1 + d ( π‘3 − π‘) , 6 2 π‘ ∈ [0, 1] , (9) where π(π‘) = (1/2)π‘ − π‘. Define Nemytskii operators πΉ : πΆ3 [0, 1] → πΆ[0, 1] induced by π as σΈ σΈ σΈ σΈ σΈ (πΉπ₯) (π‘) = π (π‘, π₯ (π‘) , π₯ (π‘) , π₯ (π‘) , π₯ (π‘)) , π‘ ∈ [0, 1] , (10) π ) πΊ (π‘, π ) ππ‘ {π − ( 1 ) π 2 − ( 1 ) π‘2 , 0 ≤ π‘ ≤ π ≤ 1; ={ 2 2 π − π‘π , 0 ≤ π ≤ π‘ ≤ 1; { 0≥( 2 σΈ 0≤( (18) π2 ) πΊ (π‘, π ) ππ‘2 −π‘, ={ −π , 0 ≤ π‘ ≤ π ≤ 1; 0 ≤ π ≤ π‘ ≤ 1; (19) (2) π(π‘) ≤ 0, πσΈ (π‘) ≤ 0, πσΈ σΈ (π‘) = 1, πσΈ σΈ σΈ (π‘) = 0, π‘ ∈ [0, 1]; (3) ||π||0 = 1/2, ||πσΈ ||0 = 1, ||πσΈ σΈ ||0 = 1, ||πσΈ σΈ σΈ ||0 = 0, ||π||πΆ3 = 1. Journal of Applied Mathematics 3 Lemma 4. Suppose that (i) for each fixed (π‘, π₯2 , π₯3 ) ∈ [0, 1] × R2 , π(π‘, π₯0 , π₯1 , π₯2 , π₯3 ) is nondecreasing in π₯0 and π₯1 ; (ii) there exists a constant π > 0 such that for |π₯| > π, π‘ ∈ [0, 1], π₯π (π‘, −π₯, −π₯, π₯, 0) > 0; σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨β (π‘, π₯0 , π₯1 , π₯2 ) − β (π‘, π¦0 , π¦1 , π¦2 )σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ ≤ π (max {σ΅¨σ΅¨σ΅¨π₯π − π¦π σ΅¨σ΅¨σ΅¨ , π = 0, 1, 2}) (21) for all (π‘, π₯0 , π₯1 , π₯2 ), (π‘, π¦0 , π¦1 , π¦2 ) ∈ [0, 1] × R3 . Then, any solution π₯ = π₯(π‘) of BVP (5), (6) satisfies (22) −1 where π = (1 − π½) ||β(⋅, 0, 0, 0)||0 . π₯σΈ σΈ (π‘1 ) , 0) > 0. (27) We may assume that π₯σΈ σΈ (π‘1 ) > 0; then, π₯(4) (π‘1 ) > 0. Thus, by the continuity of π₯(4) (π‘) on [0, 1], there exists πΏ > 0 such that π₯(4) (π‘) > 0 for π‘ ∈ (π‘1 − πΏ, π‘1 ] ⊂ [0, 1]. Since π₯σΈ σΈ σΈ (π‘1 ) = 0, it follows that π₯σΈ σΈ σΈ (π‘) < 0 for π‘ ∈ (π‘1 − πΏ, π‘1 ]; namely, π₯σΈ σΈ (π‘) is decreasing on (π‘1 −πΏ, π‘1 ], which contradicts the fact that π₯σΈ σΈ (π‘) attains its positive maximum value at π‘ = π‘1 . In summary, inequality (23) is true, which implies from π₯(0) = π₯σΈ (1) = 0 that π = 0, 1, π‘ ∈ [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 π > 0 such that whenever |π₯2 | > π and all (π‘, π₯0 , π₯1 ) ∈ [0, 1] × R2 , Proof. Let us first show that ∀π‘ ∈ [0, 1] . (23) Note that if π = 0 in (5) and (6), then BVP (5), (6) has only the trivial solution, and thus (23) holds. Hence, we may assume that π ∈ [0, 1]. Suppose now that (23) is not true. Then, there exists π‘0 ∈ [0, 1] such that |π₯σΈ σΈ (π‘0 )| > π + π. Let σ΅¨ σ΅¨ σ΅¨ σ΅¨ πΎ := σ΅¨σ΅¨σ΅¨σ΅¨π₯σΈ σΈ (π‘1 )σ΅¨σ΅¨σ΅¨σ΅¨ = max σ΅¨σ΅¨σ΅¨σ΅¨π₯σΈ σΈ (π‘)σ΅¨σ΅¨σ΅¨σ΅¨ . π‘∈[0,1] (24) Then, πΎ > π + π, and from π₯(0) = π₯σΈ (1) = 0, we have σ΅¨σ΅¨ (π) σ΅¨σ΅¨ σ΅¨σ΅¨π₯ (π‘)σ΅¨σ΅¨ ≤ πΎ, σ΅¨ σ΅¨ ≥ ππ₯σΈ σΈ (π‘1 ) π (π‘1 , −π₯σΈ σΈ (π‘1 ) , −π₯σΈ σΈ (π‘1 ) , σ΅¨σ΅¨ (π) σ΅¨σ΅¨ σ΅¨σ΅¨π₯ (π‘)σ΅¨σ΅¨ ≤ π + π, σ΅¨ σ΅¨ π = 0, 1, 2, π‘ ∈ [0, 1] , σ΅¨σ΅¨ σΈ σΈ σ΅¨σ΅¨ σ΅¨σ΅¨π₯ (π‘)σ΅¨σ΅¨ ≤ π + π, σ΅¨ σ΅¨ π₯σΈ σΈ (π‘1 ) π₯(4) (π‘1 ) = ππ₯σΈ σΈ (π‘1 ) π (π‘1 , π₯ (π‘1 ) , π₯σΈ (π‘1 ) , π₯σΈ σΈ (π‘1 ) , 0) (20) (iii) there exist π½ ∈ (0, 1) and nondecreasing continuous function π : [0, +∞) → [0, +∞) such that π(π’) ≤ π½π’ for π’ > 0, and σ΅¨σ΅¨ (π) σ΅¨σ΅¨ σ΅¨σ΅¨π₯ (π‘)σ΅¨σ΅¨ ≤ π + π, σ΅¨ σ΅¨ which is a contradiction, and thus π‘1 ∈ (0, 1]. Furthermore, by definition of π‘1 and (6), we have π₯σΈ σΈ σΈ (π‘1 ) = 0. Hence, from assumptions (i) and (ii) and (25), we have π = 0, 1, ∀π‘ ∈ [0, 1] . (25) σΈ σΈ It is easy to see that π‘1 ∈ [0, 1]. In fact, if π‘1 = 0, then |π₯ (0)| = πΎ. From (6) and (iii), it follows that for some π ∈ [0, 1], σ΅¨σ΅¨ 1 σ΅¨σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅¨ πΎ = σ΅¨σ΅¨σ΅¨σ΅¨π₯σΈ σΈ (0)σ΅¨σ΅¨σ΅¨σ΅¨ = π σ΅¨σ΅¨σ΅¨σ΅¨∫ β (π , π₯ (π ) , π₯σΈ (π ) , π₯σΈ σΈ (π )) dπ σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ 0 σ΅¨σ΅¨ σ΅¨ σ΅¨ ≤ σ΅¨σ΅¨σ΅¨σ΅¨β (π, π₯ (π) , π₯σΈ (π) , π₯σΈ σΈ (π))σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ ≤ σ΅¨σ΅¨σ΅¨σ΅¨β (π, π₯ (π) , π₯σΈ (π) , π₯σΈ σΈ (π)) − β (π, 0, 0, 0)σ΅¨σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ + σ΅¨σ΅¨σ΅¨β (π, 0, 0, 0)σ΅¨σ΅¨σ΅¨ π₯2 π (π‘, 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 be an open set in a closed, convex set πΆ of a Banach space πΈ. Assume that 0 ∈ π, π(π) is bounded, and π : π → πΆ is given by π = π1 + π2 , where π1 : π → πΈ is continuous and completely continuous and π2 : π → πΈ is a nonlinear contraction. Then, either (A1 ) π has a fixed point in π, or (A2 ) there is a point π’ ∈ ππ and π ∈ (0, 1) with π’ = ππ(π’). 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 (π‘, π₯2 , π₯3 ) ∈ [0, 1] × R2 , π(π‘, π₯0 , π₯1 , π₯2 , π₯3 ) is nondecreasing in π₯0 and π₯1 ; (ii) there exists a constant π > 0 such that for |π₯| > π, π‘ ∈ [0, 1], ≤ π½πΎ + (1 − π½) π < π½πΎ + (1 − π½) πΎ = πΎ, (26) π₯π (π‘, −π₯, −π₯, π₯, 0) > 0; (30) 4 Journal of Applied Mathematics (iii) there exist π½ ∈ (0, 1) and nondecreasing continuous function π : [0, +∞) → [0, +∞) such that π(π’) ≤ π½π’ for π’ > 0, and σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨β (π‘, π₯0 , π₯1 , π₯2 ) − β (π‘, π¦0 , π¦1 , π¦2 )σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ ≤ π (max {σ΅¨σ΅¨σ΅¨π₯π − π¦π σ΅¨σ΅¨σ΅¨ , π = 0, 1, 2}) (31) for all (π‘, π₯0 , π₯1 , π₯2 ), (π‘, π¦0 , π¦1 , π¦2 ) ∈ [0, 1] × R3 ; (iv) π(π‘, π₯0 , π₯1 , π₯2 , π₯3 ) satisfies the Nagumo condition; that is, there exists a positive-valued continuous function +∞ Φ(π ) on [0, +∞) with ∫0 (π dπ /Φ(π )) = +∞ such that σ΅¨ σ΅¨ σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨π (π‘, π₯0 , π₯1 , π₯2 , π₯3 )σ΅¨σ΅¨σ΅¨ ≤ Φ (σ΅¨σ΅¨σ΅¨π₯3 σ΅¨σ΅¨σ΅¨) −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 σ΅¨σ΅¨ σΈ σΈ σΈ σ΅¨σ΅¨ σ΅¨σ΅¨π₯ (π‘)σ΅¨σ΅¨ ≤ π, σ΅¨ σ΅¨ π‘ ∈ [0, 1] , (34) π 0 where π := max{π0 , 2(π + π)} and ∫π+π (π dπ /Φ(π )) = 2(π + π) + 1. Suppose that (34) is not true. Then, there exists π‘1 ∈ [0, 1) such that |π₯σΈ σΈ σΈ (π‘1 )| > π. Since π₯σΈ σΈ σΈ (1) = 0, then there exists π, π (π‘1 < π < π < 1) such that σ΅¨σ΅¨ σΈ σΈ σΈ σ΅¨σ΅¨ σ΅¨σ΅¨ σΈ σΈ σΈ σ΅¨σ΅¨ σ΅¨σ΅¨π₯ (π)σ΅¨σ΅¨ = π + π, σ΅¨σ΅¨π₯ (π)σ΅¨σ΅¨ = π, σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅¨σ΅¨ σΈ σΈ σΈ σ΅¨σ΅¨ π + π < σ΅¨σ΅¨σ΅¨π₯ (π‘)σ΅¨σ΅¨σ΅¨ < π, ∀π‘ ∈ (π, π) . (35) Therefore, π₯σΈ σΈ σΈ (π‘) is positive or negative on (π, π) by the continuity of the π₯σΈ σΈ σΈ (π‘). Hence, from assumption (iv), the definition of π, and Lemma 4, we can get the following contradiction: π π dπ π dπ ≤∫ π+π Φ (π ) π+π Φ (π ) σ΅¨ σ΅¨σ΅¨ π σΈ σΈ σΈ σ΅¨ π₯ (π‘) π₯(4) (π‘) dπ‘ σ΅¨σ΅¨σ΅¨ ≤ σ΅¨σ΅¨σ΅¨σ΅¨∫ σ΅¨ σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ π Φ (σ΅¨σ΅¨σ΅¨π₯σΈ σΈ σΈ (π‘)σ΅¨σ΅¨σ΅¨) σ΅¨σ΅¨σ΅¨ 2 (π + π) + 1 = ∫ Consequently, from Lemma 3, we have σ΅¨σ΅¨σ΅¨π (π‘, π₯ (π )) − π (π‘, π¦ (π ))σ΅¨σ΅¨σ΅¨ = σ΅¨σ΅¨σ΅¨π (π‘) (π»π₯) (π ) − π (π‘) (π»π¦) (π )σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅¨ σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅© ≤ σ΅©σ΅©πσ΅©σ΅©0 π (σ΅©σ΅©π₯ − π¦σ΅©σ΅©πΆ3 ) 1 σ΅© σ΅© ≤ π½σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅©πΆ3 , 2 π0 π‘, π ∈ [0, 1] , ∀π₯, π¦ ∈ πΆ3 [0, 1] . (38) (32) for all (π‘, π₯0 , π₯1 , π₯2 , π₯3 ) ∈ [0, 1] × [−π − π, π + π]3 × R, where π = (1 − π½) ββ (⋅, 0, 0, 0)β0 . We now show that π2 : Ω → πΆ3 [0, 1] is a nonlinear contraction. In fact, from assumption (iii), we have σ΅¨σ΅¨σ΅¨(π»π₯) (π‘) − (π»π¦) (π‘)σ΅¨σ΅¨σ΅¨ ≤ π (σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© 3 ) , σ΅©πΆ σ΅© σ΅¨ σ΅¨ (37) 3 π‘ ∈ [0, 1] , ∀π₯, π¦ ∈ πΆ [0, 1] . Similarly, for all π₯, π¦ ∈ πΆ3 [0, 1], σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨ ππ (π‘, π₯ (π )) ππ (π‘, π¦ (π )) σ΅¨σ΅¨σ΅¨ σ΅©σ΅© σΈ σ΅©σ΅© σ΅¨σ΅¨ σ΅¨σ΅¨ ≤ σ΅©σ΅©π σ΅©σ΅© π (σ΅©σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅©σ΅©πΆ3 ) − σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅© σ΅©0 ππ‘ ππ‘ σ΅¨ σ΅¨ σ΅© σ΅© ≤ π½σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅©πΆ3 , π‘, π ∈ [0, 1] , σ΅¨σ΅¨σ΅¨ π2 π (π‘, π₯ (π )) π2 π (π‘, π¦ (π )) σ΅¨σ΅¨σ΅¨ σ΅© σΈ σΈ σ΅© σ΅¨σ΅¨ ≤ σ΅©σ΅©π σ΅©σ΅© π (σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅© 3 ) σ΅¨σ΅¨ − σ΅¨σ΅¨ σ΅©σ΅© σ΅©σ΅©0 σ΅© σ΅¨σ΅¨ σ΅©πΆ 2 2 ππ‘ ππ‘ σ΅¨σ΅¨ σ΅¨σ΅¨ σ΅© σ΅© ≤ π½σ΅©σ΅©σ΅©π₯ − π¦σ΅©σ΅©σ΅©πΆ3 , π‘, π ∈ [0, 1] , σ΅¨σ΅¨σ΅¨ π3 π (π‘, π₯ (π )) π3 π (π‘, π¦ (π )) σ΅¨σ΅¨σ΅¨ σ΅¨σ΅¨ = 0, π‘, π ∈ [0, 1] . σ΅¨σ΅¨ − σ΅¨σ΅¨ σ΅¨σ΅¨ ππ‘3 ππ‘3 σ΅¨σ΅¨ σ΅¨σ΅¨ (39) Hence, σ΅©σ΅© σ΅©σ΅© σ΅©σ΅©π2 π₯ − π2 π¦σ΅©σ΅©πΆ3 σ΅©σ΅© (π) (π) σ΅© σ΅© = max {σ΅©σ΅©σ΅©(π2 π₯) − (π2 π¦) σ΅©σ΅©σ΅© , π = 0, 1, 2, 3} (40) σ΅©0 σ΅© σ΅©σ΅© σ΅©σ΅© 3 ≤ π½σ΅©σ΅©π₯ − π¦σ΅©σ΅©πΆ3 , ∀π₯, π¦ ∈ πΆ [0, 1] . Since all possible solutions of BVP (5), (6) satisfy ||π₯||πΆ3 ≤ π < π , it follows that there is no π₯ ∈ πΩ and π ∈ (0, 1) such that π₯ = ππΏ−1 ππ₯. We conclude that (A2 ) of Lemma 6 does not hold. Consequently, πΏ−1 π = π1 + π2 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 σ΅¨ σ΅¨ σ΅¨ σ΅¨ ≤ ∫ σ΅¨σ΅¨σ΅¨σ΅¨π₯σΈ σΈ σΈ (π‘)σ΅¨σ΅¨σ΅¨σ΅¨ dπ‘ = σ΅¨σ΅¨σ΅¨σ΅¨π₯σΈ σΈ (π) − π₯σΈ σΈ (π)σ΅¨σ΅¨σ΅¨σ΅¨ π ≤ 2 (π + π) . Therefore, inequality (34) holds. Let Ω := {π₯ ∈ πΆ3 [0, 1] : ||π₯||πΆ3 < π + 1 =: π }. It follows easily from the properties of the Green function and the continuity of π that the operator π1 : Ω → πΆ3 [0, 1] is completely continuous. (iσΈ ) there exists a constant π > 0 such that whenever |π₯2 | > π and all (π‘, π₯0 , π₯1 ) ∈ [0, 1] × R2 , π₯2 π (π‘, π₯0 , π₯1 , π₯2 , 0) > 0, (41) then the conclusion of Theorem 7 remains true. Remark 9. In Theorem 7, if π ≥ 0 ≥ β and π(π‘, 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₯ = π1 π₯+π2 π₯ ≥ 0, π₯σΈ = (π1 π₯)σΈ + (π2 π₯)σΈ ≥ 0 and π₯σΈ σΈ = (π1 π₯)σΈ σΈ + (π2 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 σ΅¨ σ΅¨σ΅¨ (42) σ΅¨σ΅¨π (π‘, π₯)σ΅¨σ΅¨σ΅¨ ≤ Ψ (|π₯|) , ∀ (π‘, π₯) ∈ [0, 1] × R; (ii) there exists π½ ∈ (0, 2) such that σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨β (π‘, π₯) − β (π‘, π¦)σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ ≤ π½ σ΅¨σ΅¨σ΅¨π₯ − π¦σ΅¨σ΅¨σ΅¨ , ∀ (π‘, π₯, π¦) ∈ [0, 1] × R2 ; (43) which contradicts (iii). Hence, (A2 ) of Lemma 6 does not hold, and consequently πΏ−1 π = π1 +π2 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 π ≥ 0 ≥ β and π(π‘, 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 (π‘, π₯ (π‘)) = π (π‘) π₯ (π‘) , (iii) there exists πΎ > 0 such that πΎ (π‘, π ) = π (π‘) π (π ) , (44) 1 (π2 π₯) (π‘) = ∫ πΎ (π‘, π ) π₯ (π ) dπ . Then, BVP (3), (4) has at least one solution. 0 Proof. It is easy to see that π₯ ∈ πΆ4 [0, 1] is a solution of BVP (3), (4) if and only if π₯ ∈ πΆ[0, 1] is a solution of the integral equation (14) with π = 1. Moreover, π1 is completely continuous, and π2 is a nonlinear contraction. It follows from (15), (i), and Lemma 3 that ∀π₯ ∈ πΆ[0, 1], 1 σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨(π1 π₯) (π‘)σ΅¨σ΅¨σ΅¨ ≤ ∫ πΊ (π‘, π ) Ψ (|π₯ (π )|) dπ 0 1 ≤ Ψ (βπ₯β0 ) , 3 (π‘, π ) ∈ [0, 1] × [0, 1] . 1 (i) πΎ0 := (1/2) ∫0 |π(π )|dπ < 1; (ii) there exists Ψ : [0, +∞) → [0, +∞) being continuous and nondecreasing such that σ΅¨ σ΅¨σ΅¨ σ΅¨σ΅¨π (π‘, π₯)σ΅¨σ΅¨σ΅¨ ≤ Ψ (|π₯|) , (45) lim sup π → +∞ Also, (16), (ii), and Lemma 3 yield (52) Theorem 12. Suppose that π‘ ∈ [0, 1] . ∀ (π‘, π₯) ∈ [0, 1] × R, Ψ (π) < 3 (1 − πΎ0 ) . π (53) Then, the nonlinear fourth-order differential equation (3) with boundary conditions 1 σ΅¨ σ΅¨ σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨(π2 π₯) (π‘)σ΅¨σ΅¨σ΅¨ ≤ ∫ σ΅¨σ΅¨σ΅¨π (π‘) (π»π₯) (π )σ΅¨σ΅¨σ΅¨ dπ 0 π₯ (0) = π₯σΈ (1) = 0, 1 σ΅© σ΅© ≤ σ΅©σ΅©σ΅©πσ΅©σ΅©σ΅©0 ∫ (|β (π , π₯ (π )) − β (π , 0)| + |β (π , 0)|) dπ 1 π₯σΈ σΈ (0) = ∫ π (π ) π₯ (π ) dπ , 0 0 ∀π₯ ∈ πΆ [0, 1] , π‘ ∈ [0, 1] . (46) From (14), (45), and (46), we have that all possible solutions of π₯ = π(π1 + π2 )π₯ satisfy 1 1 |π₯ (π‘)| ≤ Ψ (βπ₯β0 ) + (π½βπ₯β0 + β0 ) , 3 2 (51) Then, where β0 = max0≤π‘≤1 |β(π‘, 0)|. 1 (π½βπ₯β0 + β0 ) , 2 (50) where π(⋅) ∈ πΆ[0, 1]. Define Ψ (πΎ) + (3/2) β0 1 < 3 (1 − π½) , πΎ 2 ≤ π‘ ∈ [0, 1] , π‘ ∈ [0, 1] . (47) Let Ω := {π₯ ∈ πΆ[0, 1] : ||π₯||0 < πΎ}. Then, Ω is open in πΆ[0, 1], 0 ∈ Ω, and (π1 + π2 )(Ω) is bounded. Suppose that π₯ ∈ πΩ and π ∈ (0, 1) satisfy π₯ = π(π1 +π2 )π₯. Then, ||π₯||0 = πΎ, and (i) and (47) lead to 1 1 πΎ ≤ Ψ (πΎ) + (π½πΎ + β0 ) ; 3 2 (48) Ψ (πΎ) + (3/2) β0 1 ≥ 3 (1 − π½) , πΎ 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₯ = π1 π₯ + π2 π₯. (55) As a linear operator on πΆ[0, 1], from (52) and (i), we get ||π2 || = πΎ0 < 1, which implies that πΌ − π2 is invertible and its inverse is given by −1 (πΌ − π2 ) ∞ = ∑ π2π π=0 1 σ΅© −1 σ΅© with σ΅©σ΅©σ΅©σ΅©(πΌ − π2 ) σ΅©σ΅©σ΅©σ΅© ≤ . 1 − πΎ0 (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 π = (πΌ − π2 )−1 π1 . 6 Journal of Applied Mathematics Let us show that there exists π∗ > 0 such that any solution π₯ of operator equation π₯ = πππ₯ (π ∈ (0, 1)) satisfies ||π₯||0 < π∗ . In fact, any solution π₯ of π₯ = πππ₯ (π ∈ (0, 1)) satisfies −1 1 π₯ (π‘) = π(πΌ − π2 ) ∫ πΊ (π‘, π ) π (π , π₯ (π )) dπ , (57) 0 1 Ψ (βπ₯β0 ) . 3 (1 − πΎ0 ) 1 Ψ (π) , 3 (1 − πΎ0 ) ∀π ≥ π∗ . (59) Comparing (58) and (59), we see that ||π₯||0 < π∗ . Now, let Ω = {π₯ ∈ πΆ[0, 1] : ||π₯||0 < π∗ }. By the LeraySchauder continuation theorem π 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 π ≥ 0 ≥ π and π(π‘, 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₯ (π‘) = ∞ 1 ( ∑ π2π ) ∫ 0 π=0 πΊ (π‘, π ) π (π , π₯ (π )) dπ ≥ 0 on [0, 1] , σΈ σΈ (π‘)) σΈ σΈ 2 + (π₯σΈ σΈ σΈ (π‘)) , 1 1√ 2 ∫ 1 + (π₯σΈ σΈ (π )) dπ , 2 0 where π(π‘) ∈ πΆ([0, 1], [0, (1/8)]). Let π (π‘, π₯) = π (π‘) π₯2 + 1 on [0, 1] × R, 3 1 ln 2 1 + π₯2 on [0, 1] × R, β (π‘, π₯) = 1 Ψ (π₯) = π₯2 + 1 on [0, +∞) , 8 3 π½= , 2 (67) πΎ = 3. (63) 3 1 π₯σΈ σΈ (0) = ∫ (π 2 − 4π ) π₯ (π ) dπ , 0 π (π‘, π₯) = π (π‘) √π₯2 + 1 3 π‘∈[0,1] π (π‘) = π‘2 − 4π‘ 2 1 π (π‘, π₯0 , π₯1 , π₯2 , π₯3 ) = π‘2 π₯03 + π₯15 + π₯2 ππ₯2 + π₯32 2 on [0, 1] × R4 , on [0, +∞) . (68) (69) π₯σΈ σΈ σΈ (1) = 0, 3 on [0, 1] × R3 , π‘ ∈ [0, 1] , π₯ (0) = π₯σΈ (1) = 0, on [0, 1] × R, Ψ (π₯) = ( max π (π‘)) √π₯2 + 1 Let 1 β (π‘, π₯0 , π₯1 , π₯2 ) = √1 + π₯22 2 π₯(4) (π‘) = π (π‘) √(π₯ (π‘))2 + 1, where π(π‘) ∈ πΆ([0, 1], [0, +∞)). Let π₯σΈ σΈ σΈ (1) = 0. 1 π (π’) = π’ 2 π₯σΈ σΈ σΈ (1) = 0, π‘ ∈ [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 dπ , ∫ ln 2 0 1 + (π₯ (π ))2 π₯σΈ σΈ = (π1 π₯) + (π2 π₯) ≤ 0. (61) Example 14. Consider the fourth-order boundary value problem 5 1 π₯(4) (π‘) = π‘2 (π₯ (π‘))3 + (π₯σΈ (π‘)) 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 (π‘) π(π₯ (65) (60) and thus π₯σΈ = (π1 π₯) + (π2 π₯) ≥ 0, π‘ ∈ [0, 1] , π₯ (0) = π₯σΈ (1) = 0, (58) The condition lim supπ → +∞ (Ψ(π)/π) < 3(1−πΎ0 ) implies that there exists π∗ > 0 such that (Ψ(π)/π) < 3(1 − πΎ0 ) for all π ≥ π∗ ; that is, π> Example 15. Consider the fourth-order boundary value problem π₯(4) (π‘) = π (π‘) (π₯(π‘))2 + 1, and, hence, by (ii) and Lemma 3, we have βπ₯β0 ≤ 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. 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