Hindawi Publishing Corporation Abstract and Applied Analysis Volume 2013, Article ID 613672, 7 pages http://dx.doi.org/10.1155/2013/613672 Research Article Triple Positive Solutions of a Nonlocal Boundary Value Problem for Singular Differential Equations with p-Laplacian Jufang Wang, Changlong Yu, and Yanping Guo College of Sciences, Hebei University of Science and Technology, Shijiazhuang, Hebei 050018, China Correspondence should be addressed to Jufang Wang; wangjufang1981@126.com and Changlong Yu; changlongyu@126.com Received 22 October 2012; Revised 13 January 2013; Accepted 26 January 2013 Academic Editor: Bashir Ahmad Copyright © 2013 Jufang Wang 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 establish the existence of triple positive solutions of an m-point boundary value problem for the nonlinear singular secondorder differential equations of mixed type with a p-Laplacian operator by Leggett-William fixed point theorem. At last, we give an example to demonstrate the use of the main result of this paper. The conclusions in this paper essentially extend and improve the known results. 1. Introduction The existence and multiplicity of positive solutions for differential equations boundary value problems (BVPs) with the pLaplacian operator subject to Dirichlet, Sturm-Liouville, or nonlinear boundary value conditions have been extensively investigated in recent years; see [1–10] and the references therein. Particularly, the following differential equations with one-dimensional p-Laplacian σΈ (ππ (π’σΈ )) + π (π‘) π (π‘, π’) = 0, 0≤π‘≤1 σΈ (ππ (π’σΈ )) (π‘) + π (π‘) π × (π’ (π‘) , π’σΈ (π‘) , (ππ’) (π‘) , (ππ’) (π‘)) = 0, π’σΈ (0) = π½π’σΈ (π) , 0 ≤ π‘ ≤ 1, (3) π’ (1) = π (π’σΈ (1)) . (1) have been studied subject to different kinds of boundary conditions; see [1–4] and the references therein. The methods mainly depend on Kransnosel’skii fixed point theorem, upper and lower solution technique, Leggett-Williams fixed point theorem, and some new fixed point theorems in cones, and so forth. Recently, in [9], Kong et al. have studied the existence of triple positive solutions for the following BVP: σΈ Firstly, we confirm that the mistakes which have been pointed out in [10] exist. At the same time, we think that the value of π designed in Theorem 3.1 in [10] is not suitable, since the proof needs the condition ππ (π) ≤ π, but in fact this condition does not always hold. Motivated by the work above, in this paper, we will study the following more extensive second-order m-point BVP: σΈ (ππ (π’σΈ )) (π‘) + π (π‘) π (ππ (π’σΈ )) (π‘) + π (π‘) π × (π’ (π‘) , π’σΈ (π‘) , (ππ’) (π‘) , (ππ’) (π‘)) = 0, π’σΈ (0) = 0, and studied the existence of triple positive solutions for the following BVP: 0 ≤ π‘ ≤ 1, (2) π’ (1) = π (π’σΈ (1)) . More recently, in [10], Hu and Ma have pointed out that the equivalent integral equation of BVP (2) is wrong in [9] × (π’ (π‘) , π’σΈ (π‘) , (ππ’) (π‘) , (ππ’) (π‘)) = 0, π−2 ππ (π’σΈ (0)) = ∑ π½π ππ (π’σΈ (ππ )) , 0 ≤ π‘ ≤ 1, π’ (1) = π (π’σΈ (1)) , π=1 (4) 2 Abstract and Applied Analysis where ππ (π ) = |π |π−2 π (π > 1) is an increasing function, (ππ )−1 (π ) = ππ (π ), 1/π + 1/π = 1; 0 ≤ π½π < 1, π = 1, 2, . . . , π − 2, ∑π−2 π=1 π½π < 1, and 0 < π1 < π2 < ⋅ ⋅ ⋅ < ππ−2 ; π and π are two linear operators defined by π‘ ππ’ (π‘) = ∫ π (π‘, π ) π’ (π ) ππ , 0 1 ππ’ (π‘) = ∫ β (π‘, π ) π’ (π ) ππ , (5) 0 π’ ∈ πΆ1 [0, 1] , in which π ∈ πΆ[π·, π + ], β ∈ πΆ[π·0 , π + ], π· = {(π‘, π ) ∈ π 2 : 0 ≤ π ≤ π‘ ≤ 1}, π·0 = {(π‘, π ) ∈ π 2 : 0 ≤ π , π‘ ≤ 1}, π + = [0, +∞), π = (−∞, +∞), π0 = max{π(π‘, π ) : (π‘, π ) ∈ π·}, and β0 = max{β(π‘, π ) : (π‘, π ) ∈ π·0 }. Obviously, when π = 3, BVP (4) reduces to BVP (3), and when π = 3, π½1 = 0, BVP (4) reduces to BVP (2), so BVP (2) and BVP (3) are special cases of BVPs (4). Throughout this paper, we always suppose the following conditions hold: (C1 ) π ∈ πΆ(π + × π × π + × π + , (0, +∞)); (C2 ) π(π‘) ∈ πΆ([0, 1], π + ) may be singular at π‘ = 0, 1 and 0 < 1 ∫0 π(π‘)ππ‘ < +∞, so it is easy to see that there exists a 1 constant π > 0 such that 0 < ∫0 π(π‘)ππ‘ < ππ (π); (C3 ) π : π → π + is nonincreasing and continuous, and 0 ≤ π(V) ≤ |V| for V ∈ π . 2. Preliminary Results In this section, we firstly present some definitions, theorems, and lemmas, which will be needed in the proof of the main result. Definition 1. Let πΈ be a real Banach space. A nonempty closed convex set π ⊂ πΈ is called a cone if it satisfies the following two conditions: (i) π₯ ∈ π, π ≥ 0 implies ππ₯ ∈ π; (ii) π₯ ∈ π, −π₯ ∈ π implies π₯ = 0. Definition 2. Given a cone π in a real Banach space πΈ, a continuous map πΌ is called a concave (resp., convex) functional on π if and only if, for all π₯, π¦ ∈ π and 0 ≤ π‘ ≤ 1, it holds: πΌ(π‘π₯ + (1 − π‘)π¦) ≥ π‘πΌ(π₯) + (1 − π‘)πΌ(π¦), (resp., πΌ(π‘π₯ + (1 − π‘)π¦) ≤ π‘πΌ(π₯) + (1 − π‘)πΌ(π¦)). We consider the Banach space πΈ = πΆ1 [0, 1] equipped with norm βπ’β = max0≤π‘≤1 {βπ’(π‘)β0 , βπ’σΈ (π‘)β0 }, where βπ’β0 = max0≤π‘≤1 |π’(π‘)|. We denote, for any fixed constants π, π, π, πΆ+ [0, 1] = {π’ ∈ πΆ[0, 1] : π’(π‘) ≥ 0, π‘ ∈ [0, 1]}, π = {π’ ∈ πΈ | π’(π‘) is concave and nonincreasing on [0, 1]}, ππ = {π’ ∈ π : βπ’β < π}, π(πΌ, π, π) = {π’ ∈ π : π ≤ πΌ(π’), βπ’β < π}. It’s easy to see that π is a cone in πΈ. Theorem 3 (Leggett-William). Let π΄ : ππ → ππ be a completely continuous map and let πΌ be a nonnegative continuous concave functional on π with πΌ(π’) ≤ βπ’β for any π’ ∈ ππ . Suppose there exist constants π, π, and π with 0 < π < π < π ≤ π such that (i) {π’ ∈ π(πΌ, π, π) : πΌ(π’) > π} =ΜΈ π and πΌ(π΄π’) > π for all π’ ∈ π(πΌ, π, π); (ii) βπ΄π’β < π for all π’ ∈ ππ ; (iii) πΌ(π΄π’) > π for all π’ ∈ π(πΌ, π, π) with βπ΄π’β > π. Then π΄ has at least three fixed points π’1 , π’2 , and π’3 satisfying σ΅©σ΅© σ΅©σ΅© π < πΌ (π’2 ) , σ΅©σ΅©π’1 σ΅©σ΅© < π, (6) σ΅©σ΅© σ΅©σ΅© πΌ (π’3 ) < π. σ΅©σ΅©π’3 σ΅©σ΅© > π, σΈ Lemma 4. Suppose π¦ ∈ πΆ1 [0, 1] with (ππ (π¦σΈ )) ∈ πΏ1 [0, 1] satisfies σΈ (ππ (π¦σΈ )) (π‘) ≤ 0, π−2 ππ (π¦σΈ (0)) = ∑ π½π ππ (π¦σΈ (ππ )) , 0 ≤ π‘ ≤ 1, π¦ (1) = π (π¦σΈ (1)) . (7) π=1 Then, π¦(π‘) ≥ 0 is concave and nonincreasing on [0, 1], that is, π¦ ∈ π. σΈ Proof. Since (ππ (π¦σΈ )) (π‘) ≤ 0, we know that ππ (π¦σΈ ) is nonincreasing, that is, π¦σΈ (π‘) is nonincreasing, which means π¦(π‘) is concave. At the same time, we have π¦σΈ (π‘) ≤ π¦σΈ (0), π−2 σΈ σΈ so π¦σΈ (0) = ππ (∑π−2 π=1 π½π ππ (π¦ (ππ ))) ≤ ππ (∑π=1 π½π ππ (π¦ (0))) = σΈ σΈ σΈ ππ (∑π−2 π=1 π½π )π¦ (0), namely π¦ (0) ≤ 0. Then, π¦ (π‘) ≤ 0; that is to say, π¦(π‘) is nonincreasing. So π¦(π‘) ≥ π¦(1) = π(π¦σΈ (1)) ≥ 0. Above all, π¦ ∈ π. This completes the proof. σΈ Lemma 5. Let π¦ ∈ πΆ[0, 1] and (ππ (π’σΈ )) ∈ πΏ1 [0, 1], then, BVP σΈ (ππ (π’σΈ )) (π‘) = −π¦ (π‘) , π−2 ππ (π’σΈ (0)) = ∑ π½π ππ (π’σΈ (ππ )) , 0 ≤ π‘ ≤ 1, π’ (1) = π (π’σΈ (1)) , (8) π=1 has a unique solution 1 π’ (π‘) = ∫ ππ ( π‘ ππ π 1 π−2 ∑ π½π ∫ π¦ (π) ππ + ∫ π¦ (π) ππ) ππ 1 − π½ π=1 0 0 + π (−ππ ( where π½ = ∑π−2 π=1 π½π . ππ 1 1 π−2 ∑ π½π ∫ π¦ (π) ππ + ∫ π¦ (π) ππ)) , 1 − π½ π=1 0 0 (9) Abstract and Applied Analysis 3 Define the operator π΄ : π → πΈ by 1 (π΄π’) (π‘) = ∫ ππ ( π‘ + ππ ( 1 ππ 1 π−2 ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1 − π½ π=1 0 π + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) 0 = 2ππ ( + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) ππ 0 ππ 1 π−2 ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1 − π½ π=1 0 ππ 1 π−2 ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1 − π½ π=1 0 1 +π (−ππ ( π−2 + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) ππ 1 ∑ π½ ∫ π (π) 1−π½ π=1 π 0 0 × π (π’, π’σΈ , ππ’, ππ’) ππ σ΅¨ σ΅¨ = 2 σ΅¨σ΅¨σ΅¨σ΅¨(π΄π’)σΈ (1)σ΅¨σ΅¨σ΅¨σ΅¨ σ΅© σ΅© = 2σ΅©σ΅©σ΅©σ΅©(π΄π’)σΈ σ΅©σ΅©σ΅©σ΅©0 . (11) 1 + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ)) . 0 (10) Obviously, π΄ is well defined and π’ ∈ πΈ is a solution of BVP (4) if and only if π’ is a fixed point of π΄. Lemma 6. π΄ : π → π is completely continuous. Proof. It is similar to the proof of Lemma 2.2 in [9]. Lemma 7. For any π’ ∈ π, one has βπ΄π’β0 ≤ 2β(π΄π’)σΈ β0 , βπ΄π’β ≤ 2β(π΄π’)σΈ β0 . 1 0 ππ 1 π−2 ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1 − π½ π=1 0 π σΈ + ∫ π (π) π (π’, π’ , ππ’, ππ’) ππ) ππ 0 + π (−ππ ( π−2 ππ 1 ∑ π½ ∫ π (π) 1 − π½ π=1 π 0 × π (π’, π’σΈ , ππ’, ππ’) ππ 1 + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ)) 0 ππ 1 π−2 ≤ ∫ ππ ( ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1 − π½ π=1 0 0 1 π + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) ππ 0 3. Main Results For any πΏ ∈ (0, min{π1 , 1/2}), we define a nonnegative continuous concave function πΌ : π → π + by πΌ(π’) = minπΏ≤π‘≤(1−πΏ) π’(π‘). Obviously, the following two conclusions hold: πΌ (π’) = π’ (1 − πΏ) ≤ βπ’β0 , πΌ (π΄π’) = π΄π’ (1 − πΏ) , ∀π’ ∈ π. (12) The main result of this paper is following. Proof. From (10), we obtain β(π΄π’)β0 = ∫ ππ ( Since βπ΄π’β = max{βπ΄π’β0 , β(π΄π’)σΈ β0 }, so we have βπ΄π’β ≤ 2β(π΄π’)σΈ β0 , which completes the proof. Theorem 8. Let π0 = min0≤π‘≤1 π(π‘) and π½ = ∑π−2 π=1 π½π < 1. Suppose (C1 ), (C2 ), and (C3 ) hold. Suppose further that there exist numbers πΏ ∈ (0, min{π1 , 1/2}), π, π, π, and π such that 0 < π < π ≤ π0 πΏπ/π < π ≤ π, and (H1 ) π(π’, V, π€, π) ≤ (1 − π½)ππ (π/2π), for (π’, V, π€, π) ∈ [0, π] × [−π, 0] × [0, π0 π] × [0, β0 π]; (H2 ) π(π’, V, π€, π) ≤ (1 − π½)ππ (π/2π), for (π’, V, π€, π) ∈ [0, π] × [−π, 0] × [0, π0 π] × [0, β0 π]; (H3 ) π(π’, V, π€, π) > ππ (π/πΏπΏ), for (π’, V, π€, π) ∈ [π, π] × 1−πΏ [−π, 0] × [0, π0 π] × [0, β0 π], where πΏ = ππ (∫0 1−πΏ (H4 ) min(π’,V,π€,π)∈π½ π(π’, V, π€, π)ππ (π/(2π0 )) ∫0 1 π(π‘)ππ‘); π(π‘)ππ‘ ≥ max(π’,V,π€,π)∈π½ π(π’, V, π€, π) ∫0 π(π‘)ππ‘, where π½ = [0, π] × [−π, 0] × [0, π0 π] × [0, β0 π]. Then, BVP (4) has at least three positive solutions π’1 , π’2 , and π’3 such that σ΅©σ΅© σ΅©σ΅© σ΅©σ΅©π’1 σ΅©σ΅© < π, σ΅©σ΅© σ΅©σ΅© σ΅©σ΅©π’3 σ΅©σ΅© > π, π< min π’2 (π‘) , πΏ≤π‘<(1−πΏ) min π’3 (π‘) < π. πΏ≤π‘<(1−πΏ) (13) 4 Abstract and Applied Analysis Proof. We divide the proof into three steps. Step 1. We prove π΄ππ ⊂ ππ , π΄ππ ⊂ ππ ; that is, (ii) of Theorem 3. By Lemma 6, we have π΄ππ ⊂ π, so ∀π’ ∈ ππ , we get 0 ≤ π’(π‘) ≤ π, −π ≤ π’σΈ (π‘) ≤ 0, 0 ≤ (ππ’)(π‘) ≤ π0 π, 0 ≤ (ππ’)(π‘) ≤ β0 π. For π‘ ∈ [0, 1] and by (H2 ) β(π΄π’)β0 ≤ ππ ( 1 + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) 0 ≤ ππ ( 1 = ∫ ππ ( 0 ππ 1 π−2 ∑ π½π ∫ π (π) 1 − π½ π=1 0 ππ 1 π−2 ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1 − π½ π=1 0 1 1 ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) 1−π½ 0 ≤ ππ (ππ ( × π (π’, π’σΈ , ππ’, ππ’) ππ 1 π )) ππ (∫ π (π) ππ) 2π 0 ≤ π. (14) π σΈ + ∫ π (π) π (π’, π’ , ππ’, ππ’) ππ) ππ 0 + π (−ππ ( π−2 ππ 1 ∑ π½π ∫ π (π) 1 − π½ π=1 0 Hence, βπ΄π’β < π and π΄ππ ⊂ ππ . Similarly, we obtain π΄ππ ⊂ ππ . Step 2. We show × π (π’, π’σΈ , ππ’, ππ’) ππ 1 + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ)) 0 1 ≤ ∫ ππ ( 0 π−2 ππ 1 ∑ π½ ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1−π½ π=1 π 0 π + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) ππ 0 {π’ ∈ π (πΌ, π, π) : πΌ (π’) > π} =ΜΈ π, (15) πΌ (π΄π’) > π, (16) that is, (i) of Theorem 3. Let π’ = (π + π)/2, then π’ ∈ π(πΌ, π, π), πΌ(π’) = (π + π)/2 > π. Hence, (15) holds. For any π’ ∈ π(πΌ, π, π), we have π ≤ π’(π‘) ≤ π, −π ≤ π’σΈ (π‘) ≤ 0, 0 ≤ (ππ’)(π‘) ≤ π0 π, 0 ≤ (ππ’)(π‘) ≤ β0 π, π‘ ∈ [0, 1 − πΏ], so by (H3 ), we have πΌ (π΄π’) = min (π΄π’) (π‘) = (π΄π’) (1 − πΏ) π−2 ππ 1 + ππ ( ∑ π½ ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1 − π½ π=1 π 0 1 π‘∈[πΏ,1−πΏ] =∫ 1 1−πΏ ππ ( + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) ππ 1 π−2 = 2ππ ( ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1−π½ π=1 0 1 ππ 1 π−2 ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1−π½ π=1 0 π + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) ππ 0 0 ππ 1 π−2 +π (−ππ ( ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1−π½ π=1 0 + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) 1 + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ)) 0 1 1 ≤ 2ππ ( ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) 1−π½ 0 ≤ 2ππ (ππ ( 1 π )) ππ (∫ π (π) ππ) 2π 0 ≤ π. 0 ≥ πΏππ ( ππ 1 π−2 ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1 − π½ π=1 0 +∫ 1−πΏ 0 ππ 1 π−2 σ΅©σ΅© σ΅© σ΅©σ΅©(π΄π’)σΈ σ΅©σ΅©σ΅© = ππ ( ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ σ΅© σ΅©0 1−π½ 0 π=1 π + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) 0 ∀π’ ∈ π (πΌ, π, π) , π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) ππ 1 π−2 +π (−ππ ( ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1−π½ π=1 0 1 + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ)) 0 Abstract and Applied Analysis ≥ πΏππ (∫ 1−πΏ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) 0 ≥ πΏππ (ππ ( 5 ≥ πΏππ ( ππ 1 π−2 ∑ π½π ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 1 − π½ π=1 0 1−πΏ π )) ππ (∫ π (π) ππ) πΏπΏ 0 1−πΏ +∫ 0 = π. (17) Hence (16) holds. Step 3. We show that πΌ(π΄π’) > π for all π’ ∈ π(πΌ, π, π) with βπ΄π’β > π, that is, (iii) of Theorem 3. If π’ ∈ π(πΌ, π, π) with βπ΄π’β > π, we obtain 0 ≤ π’(π‘) ≤ π, −π ≤ π’σΈ (π‘) ≤ 0, 0 ≤ (ππ’)(π‘) ≤ π0 π, 0 ≤ (ππ’)(π‘) ≤ β0 π, for any π‘ ∈ [0, 1], and so by (H4 ), we have 1−πΏ π ππ ( ) ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 2π0 0 1 ≥ πΏππ (( 1 + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) 0 × (ππ ( ≥ ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ. = Furthermore, we have ππ ( ππ 1 π−2 ∑ π½π ∫ π (π) 1 − π½ π=1 0 × π (π’, π’σΈ , ππ’, ππ’) ππ (18) 0 × π (π’, π’σΈ , ππ’, ππ’) ππ 1 + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) π 1 + ππ ( ) 2π0 1 − π½ ππ π=1 0 0 σΈ × ∑ π½π ∫ π (π) π (π’, π’ , ππ’, ππ’) ππ 1 (19) σΈ = 2πΏπ0 π = 2πΏπ0 σ΅©σ΅© σ΅© σ΅©σ΅©(π΄π’)σΈ σ΅©σ΅©σ΅© σ΅©0 π σ΅© ≥ πΏπ0 π > πΏπ0 π π ≥ ∫ π (π) π (π’, π’ , ππ’, ππ’) ππ 0 π−2 ππ 1 ∑ π½ ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ. 1 − π½ π=1 π 0 + −1 π )) ) 2π0 ππ 2πΏπ0 1 π−2 ππ ( ∑ π½π ∫ π (π) π 1 − π½ π=1 0 1−πΏ π ) ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ 2π0 0 π−2 π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) Therefore, by Lemma 7, we have σ΅¨σ΅¨ σ΅¨ σ΅¨σ΅¨(π΄π’)σΈ (1)σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ σ΅©σ΅© σ΅© σ΅©σ΅©(π΄π’)σΈ σ΅©σ΅©σ΅© σ΅© σ΅© ≥ π. πΌ (π΄π’) = (π΄π’) (1 − πΏ) =∫ 1 1−πΏ ππ ( (20) ππ 1 π−2 ∑ π½π ∫ π (π) 1 − π½ π=1 0 × π (π’, π’σΈ , ππ’, ππ’) ππ π + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ) ππ Hence, by Theorem 3, the results of Theorem 8 hold. This completes the proof of Theorem 8. 4. Example 0 ππ 1 π−2 + π (−ππ ( ∑ π½π ∫ π (π) 1 − π½ π=1 0 × π (π’, π’σΈ , ππ’, ππ’) ππ Consider the following BVP: σ΅¨ σ΅¨ σΈ (σ΅¨σ΅¨σ΅¨σ΅¨π’σΈ σ΅¨σ΅¨σ΅¨σ΅¨ π’σΈ ) (π‘) + π (π‘) 1 × π (π’ (π‘) , π’σΈ (π‘) , (ππ’) (π‘) , (ππ’) (π‘)) = 0, 0 0 ≤ π‘ ≤ 1, + ∫ π (π) π (π’, π’σΈ , ππ’, ππ’) ππ)) 6 Abstract and Applied Analysis 2 σ΅¨σ΅¨ 2 1 σ΅¨σ΅¨ σ΅¨σ΅¨ σΈ σ΅¨σ΅¨ σΈ σ΅¨σ΅¨π’ (0)σ΅¨σ΅¨ π’ (0) = σ΅¨σ΅¨σ΅¨π’σΈ ( )σ΅¨σ΅¨σ΅¨ π’σΈ ( ) σ΅¨ σ΅¨ 4 σ΅¨σ΅¨ 5 σ΅¨σ΅¨ 5 σ΅¨ σ΅¨ 1 σ΅¨ 1 1σ΅¨ + σ΅¨σ΅¨σ΅¨σ΅¨π’σΈ ( )σ΅¨σ΅¨σ΅¨σ΅¨ π’σΈ ( ) , 4σ΅¨ 2 σ΅¨ 2 If 1 ≤ π’ ≤ 1296, −1296 ≤ V ≤ 0, 0 ≤ π€, π ≤ 1296, then π (π’, V, π€, π) > 10 √1 + 10 π’ (1) = π (π’σΈ (1)) , (21) max π (π’, V, π€, π) ≤ 10 √1600 + 10 √π 2 + sin V √π€ { { + + , 10π’10 + { { 1000 1000 1000 { { { 0 ≤ π’ ≤ 1, V ≤ 0, π€, π ≥ 0, (22) π (π’, V, π€, π) = { 3 √π { 2 + sin V √π€ { 10 { √π’ + + + , 10 { { 1000 1000 1000 { 1 ≤ π’, V ≤ 0, π€, π ≥ 0. { 3 V1/2 , π (V) = { 2 V, |V| ≥ 1, |V| < 1. Proof. Since π = √2 and π0 = 1/300, π½ = 1/2, πΏ = 9/25, π = 1/2, π = 1, π = 1296, π = 1600, π(π‘, π ) = 1 and β(π‘, π ) = 1, then we can obtain 0 < π < π ≤ (π0 πΏπ)/π < π ≤ π, and 1−9/25 πΏ = √∫ 0 ππ ( π (π‘) ππ‘ = √ ∫ 16/25 0 π 1600 ) = 320000, ) = ππ ( ππ ( 2π 2√2 (23) Next, we show that (H1 )–(H4 ) are satisfied. If 0 ≤ π’ ≤ 1/2, −1/2 ≤ V ≤ 0, 0 ≤ π€, π ≤ 1/2, then 3 1 10 2 + + 2 1000 1000 < (1 − π½) ππ ( π 1 )= . 2π 64 (24) So (H1 ) is satisfied. If 0 ≤ π’ ≤ 1600, −1600 ≤ V ≤ 0, 0 ≤ π€, π ≤ 1600, then π (π’, V, π€, π) < 10 √1600 + 3 40 × 2 + 1000 1000 < (1 − π½) ππ ( π ) = 32000. 2π 10 So (H2 ) is satisfied. π ) = 2 ⋅ 1502 , 2π0 1 ∫ π (π‘) ππ‘ = 0 ∫ 1−πΏ 0 8 π (π‘) ππ‘ = , 5 (27) 1141 . 625 Hence, it’s easy to know that (H4 ) is satisfied. So by Theorem 8, we conclude that the BVP (21) has three positive solutions π’1 , π’2 , and π’3 satisfying σ΅©σ΅© σ΅©σ΅© 1 σ΅©σ΅©π’1 σ΅©σ΅© < , 2 1< min π’2 (π‘) , πΏ≤π‘<(1−πΏ) σ΅©σ΅© σ΅©σ΅© 1 σ΅©σ΅©π’3 σ΅©σ΅© > 2 (28) min π’3 (π‘) < 1. πΏ≤π‘<(1−πΏ) This paper is supported by the Natural Science Foundation of China (10901045) and (11201112), the Natural Science Foundation of Hebei Province (A2009000664) and (A2011208012) and the Foundation of Hebei University of Science and Technology (XL200757). References 252 5 3125 π 1 ππ ( ) = ππ ( )= 2 = . πΏπΏ 9 8 648 (9/25) √8/5 π (π’, V, π€, π) < 10 ππ ( 3 40 × 2 + , 1000 1000 Acknowledgments 8 π‘−1/2 ππ‘ = √ , 5 1 π 1/2 )= , ) = ππ ( √ 2π 32 2 2 1 , 1000 min π (π’, V, π€, π) ≥ 16 0≤π‘≤ , 25 16 ≤ π‘ ≤ 1. 25 (26) So (H3 ) is satisfied. For any (π’, V, π€, π) ∈ [0, 1600] × [−1600, 0] × [0, 1600] × [0, 1600], we have where −1/2 { {π‘ , π (π‘) = { 187 9359 {− π‘+ , 2700 { 54 1 π 3125 > ππ ( ) = . 1000 πΏπΏ 648 (25) [1] J. 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