Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2013, Article ID 157043, 8 pages http://dx.doi.org/10.1155/2013/157043 Research Article Positive Solutions for Discrete Boundary Value Problems to One-Dimensional π-Laplacian with Delay Linjun Wang and Xumei Chen Faculty of Science, Jiangsu University, Zhenjiang 212013, China Correspondence should be addressed to Xumei Chen; chenxumei@ujs.edu.cn Received 23 April 2013; Accepted 20 June 2013 Academic Editor: Junjie Wei Copyright © 2013 L. Wang and X. Chen. 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 study the existence of positive solutions for discrete boundary value problems to one-dimensional π-Laplacian with delay. The proof is based on the Guo-Krasnoselskii fixed-point theorem in cones. Two numerical examples are also provided to illustrate the theoretical results. π Let π = − ∫π 2 π‘−(π−1)/(π−1) ππ‘, V(π ) = π’(π(π )), and π = 1. Introduction The π-Laplacian differential equations have been vastly applied in many fields such as non-Newtonian mechanics, economics, ecology, neural networks, and nonlinear flow laws, [1–5]. One of the important examples was described in [6]. Let π₯ = (π₯1 , π₯2 ) be the two Cartesian coordinates in the plane of the glacier occupying the Lipschitzian domain Ω, we denote by π’(π₯) the horizontal velocity component of the ice at the point π₯. After a rescaling of the physical velocity of the ice, π’ satisfies the following equation: − div (π (|∇π’|) ∇π’) = π, in Ω, (1) where π is a hydrostatic pressure force acting on the glacier and π is a function resulting from a constitutive law for the ice. The typical case of (1) is the following equation: div (ππ (∇π’)) + π (|π₯|) π (π’) = 0, π₯∈ π΅ (0, π 2 ) , π΅ (0, π 1 ) (2) where ππ (π ) = |π |π−2 π with π > 1 and π΅(0, π π ) ⊂ Rπ are the open balls centred about the origin with radius π π , respectively. People are interested to consider the positive radial solutions of (2), and then (2) can be reduced to the following form [7]: σΈ π1−π (ππ−1 ππ (π’σΈ )) + π (π) π (π’ (π)) = 0, π 1 < π < π 2 . (3) π − ∫π 2 π‘−(π−1)/(π−1) ππ‘. Then (3) is transformed to 1 σΈ (ππ (VσΈ (π ))) + ππ(π−1)/(π−1) (π ) π (π (π )) π (V (π )) = 0, (4) π < π < 0. With variable change π‘ = 1−π /π and π¦(π‘) = V(π ), (4) reads σΈ (ππ (π¦σΈ (π‘))) + π (π‘) π (π¦ (π‘)) = 0, 0 < π‘ < 1, (5) where π(π‘) = (−π)π π(π(π−1))/(π−1) [π(1 − π‘)]π[π(π(1 − π‘))]. Equation (5) is a typical type of one-dimensional π-Laplacian equation. In the real world, some processes are more reasonably described as π-Laplacian differential equations with delay [2, 8, 9]. The reason is that the differential of the unknown solutions depends not only on the values of the unknown solutions at the current time but also on the values prior to that. Such equations, to a certain extent, reflect much more exactly the physical reality than the equations without delay. In reality, (5) is applied together with some boundary value conditions, see for example, [1, 4, 8–11]. By using the Guo-Krasnoselskii fixed-point theorem, Jin and Yin [9] 2 Journal of Applied Mathematics proved the existence of one positive solutions for the following boundary value problem of one-dimensional π-Laplacian with delay σΈ (ππ (π’σΈ (π‘))) + ππ (π‘, π’ (π‘ − π)) = 0, π’ (1) = 0, π’ (π‘) = 0, 0 < π‘ < 1, π > 0, (6) −π ≤ π‘ ≤ 0. Based on a fixed-point approach, Bai and Xu [8] obtained the existence of positive solutions for problem (6) with π(π‘, π’) having some singularities. The main motivation of our work is twofold. The one is to prove the existence of positive solutions for discrete boundary value problems with delay. It is of interest to note here that the existence of single and multiple positive solutions for discrete boundary value problems to one-dimensional π-Laplacian have been studied in great detail in the literature [12–18] and the references therein. However, there are few papers dealing with the existence of positive solutions for discrete boundary value problems to one-dimensional π-Laplacian with delay. The other motivation is coming from the numerical solutions of problem (6). In order to get the numerical solutions of problem (6), we can apply the standard Euler method to discretize problem (6) and approximate its solutions numerically. An immediate and natural question arises if the corresponding difference equation together with boundary conditions has positive solutions. Motivated by above, our purpose in this paper is to show the existence of positive solutions for the discretization equations of problem (6). Namely, we will prove the existence of positive solutions of the following problem: Δ (ππ (Δπ’ (π − 1))) + ππ (π) π (π, π’ (π − π0 )) = 0, π ∈ {1, 2, . . . , π} , π’ (π + 1) = 0, π’ (π) = 0, π ∈ {−π0 , −π0 + 1, . . . , 0} , (7) where Δπ’(π) = π’(π + 1) − π’(π) and π0 is a positive integer. This paper is organized as follows. In Section 2, we introduce some basic definitions and then we state the GuoKrasnoselskii fixed-point theorem. In Section 3, we write a representation for a solution to problem (7) in terms of the fixed point of an appropriate operator. Then we prove that problem (7) has a positive solution with π belonging to an open interval by employing the fixed-point theorem. In Section 4, two numerical examples are presented to illustrate the theoretical results. 2. Preliminaries In this section, we introduce some basic definitions and recall the Guo-Krasnoselskii fixed-point theorem which plays a fundamental role in our subsequent analysis. For convenience, we will let Z(π, π) denote {π, π + 1, . . . , π}, where π < π ∈ Z. A sequence (π’(π))π+1 π=−π0 is said to be a positive solution of (7), if it satisfies (7) with π’(π) > 0, π ∈ Z(1, π + 1). We collect some properties of the function ππ (⋅). Lemma 1. ππ (π ) is increasing in π and (ππ )−1 = ππ , with 1/π + 1/π = 1; ππ (π 1 ⋅ π 2 ) = ππ (π 1 ) ⋅ ππ (π 2 ). Definition 2. Let πΈ be a real Banach space. A nonempty closed convex set πΎ ⊂ πΈ is called a cone if (i) π₯ ∈ πΎ and π ≥ 0 imply ππ₯ ∈ πΎ, (ii) π₯ ∈ πΎ and −π₯ ∈ π imply π₯ = π. Theorem 3 (see [19]). Let πΈ be a Banach space and πΎ ⊂ πΈ a cone. Assume Ω1 , Ω2 are bounded open subsets of πΈ with π ∈ Ω1 , Ω1 ⊂ Ω2 , and let π : πΎ β(Ω2 \ Ω1 ) → πΎ be a completely continuous operator such that one of the following holds: (i) βππ’β ≤ βπ’β, π’ ∈ πΎ ∩ πΩ1 , βππ’β ≥ βπ’β, π’ ∈ πΎ ∩ πΩ2 ; (ii) βππ’β ≥ βπ’β, π’ ∈ πΎ ∩ πΩ1 , βππ’β ≤ βπ’β, π’ ∈ πΎ ∩ πΩ2 . Then π has a fixed point in πΎ β(Ω2 \ Ω1 ). 3. Existence of Positive Solutions In this section, we study the existence of positive solutions for the following equation with delay: Δ (ππ (Δπ’ (π − 1))) + ππ (π) π (π, π’ (π − π0 )) = 0, π ∈ Z (1, π) , (8) subject to the boundary condition π’ (π + 1) = 0, π’ (π) = 0, π ∈ Z (−π0 , 0) . (9) We assume that (A1) π : Z(1, π + 1) × R → R+ is a continuous function (R+ denotes the set of nonnegative reals); (A2) π(⋅) is a positive function defined on Z(1, π + 1), ∑π+1 π=1 π(π) < ∞. Remark 4. Recall that a map π : Z(1, π + 1) × R → R+ is continuous if it is continuous as a map of the topological space Z(1, π + 1) × R into the topological space R+ . Throughout this paper, the topology on Z(1, π + 1) will be the discrete topology. Rewrite (8) as Δ (ππ (Δπ’ (π − 1))) = −ππ (π) π (π, π’ (π − π0 )) . (10) Summing up (10) with respect to π from π to π leads to π−1 ππ (Δπ’ (π − 1)) − ππ (Δπ’ (0)) = − ∑ ππ (π) π (π, π’ (π − π0 )) . π=1 (11) Noticing Lemma 1, we have π−1 Δπ’ (π − 1) = ππ (ππ (Δπ’ (0)) − ∑ ππ (π) π (π, π’ (π − π0 ))) . π=1 (12) Journal of Applied Mathematics 3 Summing up (12) with respect to π from 1 to π and noticing the boundary condition (9) lead to π π−1 π=1 π=1 π’ (π) = ∑ ππ (ππ (Δπ’ (0)) − ∑ ππ (π) π (π, π’ (π − π0 ))) , Then by substituting (19) in (21), we obtain π+1 π−1 π=π+1 π=π1 +1 π’ (π) = ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) − π) , π > π1 − 1. (13) where Δπ’(0) satisfies Since (19) is the solution of (14), we have π+1 π−1 πΉ (π₯) = ∑ ππ (ππ (π₯) − ∑ ππ (π) π (π, π’ (π − π0 ))) = 0. π=1 π=1 π+1 π1 π=1 π=1 πΉ (π₯) = ∑ ππ (ππ (ππ (∑ππ (π) π (π, π’ (π − π0 )) + π)) (14) π−1 Obviously, πΉ(π₯) is continuous and strictly increasing. We have − ∑ ππ (π) π (π, π’ (π − π0 )) ) = 0. π=1 (23) π+1 πΉ (ππ ( ∑ ππ (π) π (π, π’ (π − π0 )))) > 0. (15) πΉ (0) < 0, (22) π=1 Namely, Thus, there exists a unique solution to (14) π+1 π1 π=1 π=1 ∑ ππ ((∑ππ (π) π (π, π’ (π − π0 )) + π) π+1 ππ’ ∈ (0, ππ ( ∑ ππ (π) π (π, π’ (π − π0 )))) . (16) π=1 π−1 (24) − ∑ ππ (π) π (π, π’ (π − π0 )) ) = 0. Let π=1 π π (π) = ππ (∑ππ (π) π (π, π’ (π − π0 ))) . (17) π=1 Since π(π) is increasing and π(0) = 0, we have ππ’ ∈ (π(0), π(π + 1)). There exists π1 ∈ Z(0, π) that satisfied Thus, π1 π1 π=1 π=π ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) + π) π1 ππ (∑ππ (π) π (π, π’ (π − π0 ))) π+1 π−1 π=π1 +1 π=π1 +1 (25) = ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) − π) . π=1 (18) π1 +1 ≤ ππ’ < ππ ( ∑ ππ (π) π (π, π’ (π − π0 ))) . π=1 Therefore, if π’(π) is a positive solution of the boundary value problems (8) and (9), then it can be expressed by π’ (π) Hence, π1 ππ’ = ππ (∑ππ (π) π (π, π’ (π − π0 )) + π) , (19) π=1 where π ∈ [0, ππ(π1 + 1)π(π1 + 1, π’(π1 + 1 − π0 ))). By (13) and (19), together with the definition of the positive solution, it is easy to get π π1 π=1 π=π π’ (π) = ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) + π) , π < π1 + 1. (20) Similarly, summing up (12) with respect to π from π + 1 to π + 1 and noticing (9), we have π+1 π’ (π) = − ∑ ππ (ππ (Δπ’ (0)) π=π+1 π−1 − ∑ ππ (π) π (π, π’ (π − π0 ))) , π=1 π > π1 − 1. (21) π π1 { { ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) + π) , { { { π=1 π=π { { { { { { π ∈ Z (1, π1 ) , { { { { { π+1 π−1 { = { ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) − π) , { { π=π+1 π=π1 +1 { { { { { { π ∈ Z (π1 + 1, π) , { { { { { { { { 0, π ∈ Z (−π0 , 0) , π = π + 1, { (26) where π ∈ [0, ππ(π1 + 1)π(π1 + 1, π’(π1 + 1 − π0 ))). Let πΆ(Z(−π0 , π + 1), R) denote the class of maps π’ continuous on Z(−π0 , π + 1) (discrete topology). We introduce a function space πΈ, namely, πΈ = {π’ ∈ πΆ (Z (−π0 , π + 1) , R) , π’ (π + 1) = 0; π’ (π) = 0, π ∈ Z (−π0 , 0)} (27) 4 Journal of Applied Mathematics with norm β ⋅ β given by βπ’β = maxπ∈Z(−π0 ,π+1) |π’(π)|. Then (πΈ, β ⋅ β) is a Banach space. Define a cone πΎ ⊂ πΈ as follows: πΎ = {π’ ∈ πΈ : π’ (π) ≥ π (π) βπ’β , π ∈ Z (0, π + 1)} , For convenience, we introduce some notations: (28) π∞ = lim sup max π’ → ∞ π∈Z(1,π+1) (29) π1 { { ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) + π) , { { { π=1 π=π { { { { { { π ∈ Z (1, π1 ) , { { { { { π−1 { π+1 = { ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) − π) , { { π=π+1 π=π1 +1 { { { { { { π ∈ Z (π1 + 1, π) , { { { { { { { { 0, π ∈ Z (−π0 , 0) , π = π + 1, { (30) where π ∈ [0, ππ(π1 + 1)π(π1 + 1, π’(π1 + 1 − π0 ))). Lemma 5. Suppose that (π»1) and (π»2) hold. Then the operator π : πΎ → πΎ is completely continuous. π (π, π’) . π’π−1 Theorem 6. Suppose that (A1) and (A2) hold. Assume that the delay time is appropriately small, say π0 is a positive integer not bigger than [π/2]. If π∞ > 0, π0 < ∞, then there exists at least one positive solution to the boundary value problems (8) and (9) for π ∈ (max{π1 , π2 }, π), where π1 = 1 π∞ ⋅ (∑[π/2] π=2 ππ (∑[π/2] π=π π−1 π (π + π0 ) (π (π)) )) π−1 , (33) π2 = 1 π∞ ⋅ π+1−π0 (∑π=2+[π/2] ππ (∑π−1 π=1+[π/2] π−1 π (π + π0 ) ((π (π)) π−1 )) , (34) π= 1 π0 π−1 ⋅ ((π + 1) ππ (∑π+1 π=1 π (π))) ; (35) while if π0 > 0, π∞ < ∞, then for any π ∈ (max{π1 , π2 }, π), where 1 , π1 = π−1 π−1 [π/2] [π/2] π0 ⋅ (∑π=2 ππ (∑π=π π (π + π0 ) (π (π)) )) π2 Proof. For any π’ ∈ πΎ, it is easily to check = Δ (ππ (Δ (ππ’) (π − 1))) − ππ ((ππ’) (π) − (ππ’) (π − 1)) (32) If π’ is a positive solution of problems (8) and (9), then it is a fixed point of π. So the existence of positive solution is transformed into the existence of fixed point. The following theorem is the main result of this paper. (ππ’) (π) = ππ ((ππ’) (π + 1) − (ππ’) (π)) π (π, π’) , π’π−1 π∈Z(1,π+1) π (π, π’) π0 = lim inf min , + π’ → 0 π∈Z(1,π+1) π’π−1 Moreover, for any π’ ∈ πΎ, we have π’(π) ≥ (1/(π + 1))βπ’β, π ∈ Z(1, π). For any π’ ∈ πΎ, define an operator π on πΎ by π π0 = lim sup max π’ → 0+ π+1−π π , } π+1 π π π { , π ∈ Z (1, [ ]) , { {π 2 ={ {π + 1 − π π { , π ∈ Z ([ ] + 1, π) . { π+1 2 π (π, π’) , π’π−1 π’ → ∞ π∈Z(1,π+1) where π(π) = min{(π + 1 − π)/(π + 1), π/π}. From the definition of π(π), we have π (π) = min { min π∞ = lim inf (31) = −ππ (π) π (π, π’ (π − π0 )) ≤ 0. According to Lemma 3.2 in [1], we have (ππ’)(π) ≥ π(π)βππ’β. Thus, π(πΎ) ⊂ πΎ. Moreover, ππ and π are both continuous, and πΈ is a finite space. This implies that the operator π is a completely continuous. This completes the proof. 1 π0 ⋅ π= π+1−π0 (∑π=2+[π/2] ππ (∑π−1 π=1+[π/2] π−1 π (π + π0 ) (π (π)) 1 π∞ ⋅ ((π + 1) ππ (∑π+1 π=1 π (π))) π−1 π−1 )) , , (36) problems (8) and (9) admit at least one positive solution π’ ∈ πΎ. Proof. From Lemma 5, we see that π : πΎ → πΎ is a completely continuous operator. Since π ∈ (max{π1 , π2 }, π), there exists an π > 0 such that max {π1π , π2π } ≤ π ≤ ππ , (37) Journal of Applied Mathematics 5 where 1/(π−1) ≤ max {(π (π0 + π)) π1π = 1 (π∞ − π) ⋅ (∑[π/2] π=2 ππ (∑[π/2] π=π π−1 π (π + π0 ) (π (π)) )) π−1 , π2π = (π (π0 + π)) ≤ (π (π0 + π)) 1 (π∞ − π) ⋅ ππ (∑π−1 π=1+[π/2] π (π + π0 ) (π (π)) π−1 1 ππ = (π0 π−1 + π) ⋅ ((π + 1) ππ (∑π+1 π=1 π (π))) )) π−1 (38) Let π be fixed. By π0 < ∞, there exists an π1 > 0 such that for 0 ≤ π’ ≤ π1 , 0 π (π, π’) ≤ (π + π) π’ π−1 , π ∈ Z (1, π + 1) . (39) π−1 , π ∈ Z (1, π+1) . (40) In view of Lemma 1 and the definition of operator π, we further have βππ’β = max {(ππ’) (π1 ) , (ππ’) (π1 + 1)} . (41) π=1 π=π π+1 π−1 π=π1 +2 π=π1 +1 βπ’β ∑ ππ ( ∑ π (π))} βπ’β (π + 1) ππ ( ∑ π (π)) ≤ βπ’β . π=1 (42) Μ2 > Next, by π∞ > 0, it is easy to see that there exists an π Μ 0 such that for all π’ > π2 , π (π, π’) ≥ (π∞ − π) π’π−1 , π ∈ Z (1, π + 1) . (43) Μ2 }. Let Ω2 = {π’ ∈ πΈ, βπ’β < Take π2 = max{2π1 , (π+1)π π2 }. For any π’ ∈ πΎ ∩ πΩ2 , we have Let Ω1 = {π’ ∈ πΈ : βπ’β < π1 }. Then for any π’ ∈ πΎ ∩ πΩ1 , we have π (π, π’ (π−π0 )) ≤ (π0 +π) (π’ (π−π0 )) 1/(π−1) , . π1 +1 π+1 1/(π−1) π+1−π0 (∑π=2+[π/2] π1 βπ’β ∑ ππ ( ∑ π (π)) , π (π, π’ (π − π0 )) ≥ (π∞ − π) (π’ (π − π0 )) π−1 , (44) ∀π ∈ Z (π0 + 2, π + 1) . Thus, if π1 < π0 + [π/2], we have βππ’β = max {(ππ’) (π1 ) , (ππ’) (π1 + 1)} ≥ (ππ’) (π1 + 1) π+1 π−1 π=π1 +2 π=π1 +1 = ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) − π) Thus, βππ’β = max {(ππ’) (π1 ) , (ππ’) (π1 + 1)} π1 π1 π=1 π=π π1 π=π1 +1 ≥ ≥ βπ’β π=π1 +1 π1 +1 π=1 π=π π−1 π−1 0 π=π1 +1 π−1 ∑ π=[π/2]+1 π+1−π0 ∑ ππ ( )} × π+1−π0 ∑ π=[π/2]+2 ππ ( ) ππ (π + π0 ) (π∞ − π) (π’ (π))π−1 ) π−1 π−1 ∑ π=[π/2]+1 1/(π−1) ≥ (π (π∞ − π)) ), π−1 ππ (π) (π∞ − π) (π’ (π − π0 )) ππ ( π=[π/2]+2 ∑ ππ ( ∑ ππ (π) (π + π) (π’ (π − π0 )) π=π1 +2 ∑ π−1 ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )))} π+1 π+1−π0 π=[π/2]+2 ≤ max { ∑ ππ ( ∑ ππ (π) (π0 + π) (π’ (π − π0 )) ππ (π) π (π, π’ (π − π0 ))) π−1 ∑ π=π0 +[π/2]+1 π=π π1 π−1 ×( π1 +1 π=π1 +2 ∑ π=π0 +[π/2]+1 ππ ∑ π−1 π+1 π−1 π=π0 +[π/2]+2 ≤ max { ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 ))) , π=1 π+1 ≥ ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) − π)} π=π1 +2 ππ ( ∑ π=π0 +[π/2]+2 = max { ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) + π) , π+1 π+1 ≥ ππ (π + π0 ) (π∞ − π) (π (π)) ) βπ’β π−1 ∑ π=[π/2]+1 π−1 π (π + π0 ) (π (π)) ) ≥ βπ’β ; (45) 6 Journal of Applied Mathematics while if π1 ≥ π0 + [π/2], then we have If π1 < π0 + [π/2], we have βππ’β βππ’β = max {(ππ’) (π1 ) , (ππ’) (π1 + 1)} = max {(ππ’) (π1 ) , (ππ’) (π1 + 1)} ≥ (ππ’) (π1 ) π1 π1 π=1 π=π ≥ (ππ’) (π1 + 1) = ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) + π) ≥ π0 +[π/2] π0 +[π/2] π=π0 +2 π=π ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 ))) [π/2] [π/2] π=2 π=π (46) ≥ (π (π∞ − π)) [π/2] βπ’β π+1 ∑ π+1 ∑ π=π0 +[π/2]+2 [π/2] π−1 ) ≥ βπ’β . π=π π−1 ππ ( π=[π/2]+2 π−1 ππ ( ππ (π + π0 ) (π0 − π) (π (π)) ∑ π−1 ) π=[π/2]+1 1/(π−1) ∑ ) π=π0 +[π/2]+1 ∑ π+1−π0 π−1 ππ (π) (π0 − π) (π’ (π − π0 )) ∑ ≥ (π (π0 − π)) × ππ (π) π (π, π’ (π − π0 ))) ∑ π=π0 +[π/2]+1 π=[π/2]+2 (47) π−1 ππ ( π+1−π0 ≥ βπ’β max {π1π , π2π } ≤ π ≤ ππ , ππ ( βπ’β π−1 ∑ π=[π/2]+1 π (π + π0 ) (π (π)) π−1 ) ≥ βπ’β . (51) Conversely, if π1 ≥ π0 + [π/2], then we have βππ’β where = max {(ππ’) (π1 ) , (ππ’) (π1 + 1)} 1 (π0 − π) ⋅ (∑[π/2] π=2 ππ (∑[π/2] π=π π−1 π (π + π0 ) (π (π)) π−1 )) , ≥ (ππ’) (π1 ) π1 π1 π=1 π=π = ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) + π) π2π = π=π1 +1 π=π0 +[π/2]+2 Combining the two estimates above, we deduce βππ’β ≥ βπ’β, when π’ ∈ πΎ∩πΩ1 . Therefore, by Theorem 3, π has a fixed point π’ ∈ πΎ ∩ (Ω2 \ Ω1 ). Namely, π’(π‘) is a positive solution of problems (8) and (9). The proof of the second half is parallel to above. There exists an π > 0 such that π1π = π=π1 +2 ≥ × ∑ ππ ( ∑ π(π + π0 ) (π (π)) π=2 π−1 ≥ ≥ ∑ ππ ( ∑ ππ (π + π0 ) (π∞ − π) (π’ (π))π−1 ) 1/(π−1) π+1 = ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) − π) 1 , π−1 π−1 π+1−π0 π−1 (π0 − π) ⋅ (∑π=2+[π/2] ππ (∑π=1+[π/2] π (π + π0 ) (π (π)) )) ππ = 1 (π∞ + π) ⋅ ((π + 1) ππ (∑π+1 π=1 π−1 π (π))) . (48) Let π be fixed. By π0 > 0, then it is not difficult to choose an π1 > 0 such that 0 ≤ π’ ≤ π1 , π (π, π’) ≥ (π0 − π) π’π−1 , π ∈ Z (1, π + 1) . (49) Let Ω1 = {π’ ∈ πΈ, βπ’β < π1 }. Then for π’ ∈ πΎ ∩ πΩ1 , it can be obtained that π (π, π’ (π − π0 )) ≥ (π0 − π) (π’ (π − π0 )) π−1 , ≥ π ∈ Z (1, π + 1) . (50) π0 +[π/2] π0 +[π/2] π=π0 +2 π=π ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 ))) [π/2] [π/2] π=2 π=π ≥ ∑ ππ ( ∑ ππ (π + π0 ) (π0 − π) (π’ (π))π−1 ) 1/(π−1) ≥ (π (π0 − π)) [π/2] [π/2] π=2 π=π π−1 βπ’β ∑ ππ ( ∑ π (π + π0 ) (π (π)) ) ≥ βπ’β . (52) Μ2 π Μ2 > 0 such that for π’ > Next, by π∞ < ∞, there exists π π (π, π’) ≤ (π∞ + π) π’π−1 , π ∈ Z (1, π + 1) . (53) Journal of Applied Mathematics 7 If π is bounded, then there exists an π1 > 0 such that π(π, π’) ≤ π1 for π ∈ Z(1, π + 1), 0 ≤ π’ < ∞. Take π2 = max{2π1 , (ππ1 )1/(π−1) (π + 1) ππ (∑π+1 π=1 π(π))} and Ω2 = {π’ ∈ πΈ, βπ’β < π2 }. Then for any π’ ∈ πΎ ∩ πΩ2 , we have βππ’β π1 +1 π=1 π=π π+1 π−1 π=π1 +2 π=π1 +1 ∑ ππ ( ∑ ππ (π) π (π0 , π2 ))} 1/(π−1) ≤ max {(π (π∞ + π)) = max {(ππ’) (π1 ) , (ππ’) (π1 + 1)} π1 π1 ≤ max { ∑ ππ ( ∑ ππ (π) π (π0 , π2 )) , π1 π1 +1 π=1 π=π π2 ∑ ππ ( ∑ π (π)) , π1 = max { ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) + π) , π=1 1/(π−1) (π (π∞ + π)) π=π π+1 π+1 π−1 π=π1 +2 π=π1 +1 π2 ∑ ππ ( ∑ π (π))} π−1 ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) − π)} π=π1 +2 π=π1 +1 1/(π−1) ≤ (π + 1) (π (π∞ + π)) π+1 π2 ππ ( ∑ π (π)) ≤ π2 = βπ’β . π=1 π1 π1 +1 (55) π=1 π=π Therefore, by Theorem 3, π has a fixed point π’ ∈ πΎ∩(Ω2 \ Ω1 ). Namely, π’ is a positive solution of problema (8) and (9). This completes the proof. ≤ max { ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 ))) , π+1 π−1 π=π1 +2 π=π1 +1 ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )))} π1 π1 +1 π=1 π=π 4. Numerical Illustration ≤ max { ∑ ππ ( ∑ ππ (π) π1 ) , π+1 π−1 π=π1 +2 π=π1 +1 In this section, we present two numerical experiments to illustrate our results. Example 7. Consider the following boundary value problem: ∑ ππ ( ∑ ππ (π) π1 )} 1/(π−1) ≤ (π + 1) (ππ1 ) π’ (π + 1) − 2π’ (π) + π’ (π − 1) + π (π) π (π, π’ (π − 5)) = 0, π+1 π ∈ Z (1, 99) , ππ ( ∑ π (π)) ≤ π2 = βπ’β . π=1 (54) While if π is unbounded, it is not difficult to see that there Μ2 }, π0 ∈ Z(1, π) such that 0 ≤ π’ ≤ exists an π2 > max{2π1 , π π2 , π(π, π’) ≤ π(π0 , π2 ). Take Ω2 = {π’ ∈ πΈ : βπ’β < π2 }, then for π’ ∈ πΎ ∩ πΩ2 , we get π’ (100) = 0, π’ (π) = 0, π ∈ Z (−5, 0) , (56) where π(π) = π/100, π(π, π’(π − 5)) = (1/100)2 (π’(π − 5))2 . It is easy to see that π∞ = +∞, π0 = 0. By Theorem 6, problem (56) has a positive solution. In Figure 1, we show the numerical solution to problem (56). Example 8. Consider the following boundary value problem βππ’β = max {(ππ’) (π1 ) , (ππ’) (π1 + 1)} π1 π1 π=1 π=π = max { ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) + π) , π+1 π−1 π=π1 +2 π=π1 +1 ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )) − π)} π1 π1 +1 π=1 π=π ≤ max { ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 ))) , π+1 π−1 π=π1 +2 π=π1 +1 ∑ ππ ( ∑ ππ (π) π (π, π’ (π − π0 )))} Δπ4 (Δπ’ (π − 1)) + π (π) π (π, π’ (π − 3)) = 0, π’ (100) = 0, π’ (π) = 0, π ∈ Z (1, 99) , π ∈ Z (−3, 0) , (57) where π(π) ≡ 1, π(π, π’(π − 3)) = (1/100)4 (π’(π − 3))2 . We check that π∞ = 0, π0 = +∞. Then applying Theorem 6, problem (57) has a positive solution. Numerically, we obtain the solution of problem (57) which is shown in Figure 1. Acknowledgments This work is supported by Tian Yuan Fund of China (11226308), NNSF of China (11071102), Natural Science Fund for Colleges and Universities in Jiangsu Province (11KJD110001), the Research Fund (10JDG124) for Highlevel 8 Journal of Applied Mathematics 25 [5] 20 15 [6] u 10 [7] 5 0 −20 0 20 40 n 60 80 100 [8] (a) The numerical solution to problem (56) [9] 0.018 0.016 0.014 [10] 0.012 u 0.01 [11] 0.008 0.006 [12] 0.004 0.002 [13] 0 −20 0 20 40 n 60 80 100 (b) The numerical solution to problem (57) [14] Figure 1: The figures of the numerical solutions. [15] Group of Jiangsu University, and Postdoctoral Science Foundation (2011M500874, 1002030C). References [16] [1] D. Q. Jiang, J. F. Chu, D. O’Regan, and R. P. Agarwal, “Positive solutions for continuous and discrete boundary value problems to the one-dimension p-Laplacian,” Mathematical Inequalities & Applications, vol. 7, no. 4, pp. 523–534, 2004. [17] [2] W.-T. Li and H.-F. 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