(ProQuest: ... denotes non-US-ASCII text omitted.)
Jiqiang Jiang 1 and Lishan Liu 1,2 and Yonghong Wu 2
Recommended by Cengiz Çinar
1, School of Mathematical Sciences, Qufu Normal University, Qufu 273165, China
2, Department of Mathematics and Statistics, Curtin University of Technology, Perth, WA 6845, Australia
Received 25 March 2012; Accepted 15 May 2012
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.
1. Introduction
Boundary value problems for ordinary differential equations arise in different areas of applied mathematics and physics and so on. Fourth-order differential equations boundary value problems, including those with the p -Laplacian operator, have their origin in beam theory [1, 2], ice formation [3, 4], fluids on lungs [5], brain warping [6, 7], designing special curves on surfaces [8], and so forth. In beam theory, more specifically, a beam with a small deformation, a beam of a material that satisfies a nonlinear power-like stress and strain law, and a beam with two-sided links that satisfies a nonlinear powerlike elasticity law can be described by fourth order differential equations along with their boundary value conditions. For more background and applications, we refer the reader to the work by Timoshenko [9] on elasticity, the monograph by Soedel [10] on deformation of structure, and the work by Dulcska [11] on the effects of soil settlement. Due to their wide applications, the existence and multiplicity of positive solutions for fourth-order (including p -Laplacian operator) boundary value problems has also attracted increasing attention over the last decades; see [12-33] and references therein. In [28], Zhang and Liu studied the following singular fourth-order four-point boundary value problem [figure omitted; refer to PDF] where [varphi]p (x)=|x|p-2 x , p>1 , 0<ξ , η<1 , 0...4;a , b<1 , f∈C((0,1)×(0,∞),(0,∞)) , f(t,x) may be singular at t=0 and/or t=1 and x=0 . The authors gave sufficient conditions for the existence of one positive solution by using the upper and lower solution method, fixed point theorems, and the properties of the Green function.
In [32], Zhang et al. discussed the existence and nonexistence of symmetric positive solutions of the following fourth-order boundary value problem with integral boundary conditions: [figure omitted; refer to PDF] where [varphi]p (x)=|x|p-2 x , p>1 , w∈L1 [0,1] is nonnegative, symmetric on the interval [0,1],f:[0,1]×[0,+∞)[arrow right][0,+∞) is continuous, f(1-t,x)=f(t,x) for all (t,x)∈[0,1]×[0,+∞) , and g,h∈L1 [0,1] are nonnegative, symmetric on [0,1] .
Motivated by the work of the above papers, in this paper, we study the existence of positive solutions of the following singular fourth-order boundary value system with integral boundary conditions: [figure omitted; refer to PDF] where λ and μ are positive parameters, [varphi]pi (x)=|x|pi -2 x , pi >1 , [varphi]qi =[varphi]pi -1 , 1/pi +1/qi =1 , ξi ,ηi :[0,1][arrow right]...+ (i=1,2) are nondecreasing functions of bounded variation, and the integrals in (1.3) are Riemann-Stieltjes integrals, f1 :[0,1]×...0+ ×...+ [arrow right]...+ and f2 :[0,1]×...+ ×...0+ [arrow right]...+ are two continuous functions, and f1 (t,x,y) may be singular at x=0 while f2 (t,x,y) may be singular at y=0 ; a1 , a2 :(0,1)[arrow right]...+ are continuous and may be singular at t=0 and/or t=1 , in which ...+ =[0,+∞) , ...0+ =(0,+∞) .
Compared to previous results, our work presented in this paper has the following new features. Firstly, our study is on singular nonlinear differential systems, that is, a1 and a2 in (1.3) are allowed to be singular at t=0 and/or t=1 , meanwhile f1 (t,x,y) is allowed to be singular at x=0 while f2 (t,x,y) is allowed to be singular at y=0 , which bring about many difficulties. Secondly, the main tools used in this paper is a fixed-point theorem in cones, and the results obtained are the conditions for the existence of solutions to the more general system (1.3). Thirdly, the techniques used in this paper are approximation methods, and a special cone has been developed to overcome the difficulties due to the singularity and to apply the fixed-point theorem. Finally, we discuss the boundary value problem with integral boundary conditions, that is, system (1.3) including fourth-order three-point, multipoint and nonlocal boundary value problems as special cases. To our knowledge, very few authors studied the existence of positive solutions for p -Laplacian fourth-order differential equation with boundary conditions involving Riemann-Stieltjes integrals. Hence we improve and generalize the results of previous papers to some degree, and so it is interesting and important to study the existence of positive solutions for system (1.3).
The rest of this paper is organized as follows. In Section 2, we present some lemmas that are used to prove our main results. In Section 3, the existence of positive solution for system (1.3) is established by using the fixed point theory in cone. Finally, in Section 4, one example is also included to illustrate the main results.
Definition 1.1.
A vector (u,v)∈(C2 [0,1]∩C4 (0,1))×(C2 [0,1]∩C4 (0,1)) is said to be a positive solution of system (1.3) if and only if (u,v) satisfies (1.3) and u(t)>0 , v(t)...5;0 or u(t)...5;0 , v(t)>0 for any t∈(0,1) .
Let K be a cone in a Banach space E . For 0<r<R<+∞ , let Kr ={x∈K:||x||<r} , ∂Kr ={x∈K:||x||=r} , and K¯r,R ={x∈K:r...4;||x||...4;R} . The proof of the main theorem of this paper is based on the fixed point theory in cone. We list one lemma [34, 35] which is needed in our following argument.
Lemma 1.2.
Let K be a positive cone in real Banach space E and T:K¯r,R [arrow right]K a completely continuous operator. If the following conditions hold
(i) ||Tx||...4;||x|| for x∈∂KR ;
(ii) there exists e∈∂K1 such that x...0;Tx+me for any x∈∂Kr and m>0 . Then T has a fixed point in K¯r,R .
Remark 1.3.
If (i) and (ii) are satisfied for x∈∂Kr and x∈∂KR , respectively. Then Lemma 1.2 is still true.
2. Preliminaries and Lemmas
The basic space used in this paper is E=C[0,1]×C[0,1] . Obviously, the space E is a Banach space if it is endowed with the norm as follows: [figure omitted; refer to PDF]
for any (u,v)∈E . Denote C+ [0,1]={u∈C[0,1]:u(t)...5;0, 0...4;t...4;1} . For convenience, we list the following assumptions:
(H1 ) : a1 ,a2 :(0,1)[arrow right]...+ are continuous and [figure omitted; refer to PDF] where e(s)=s(1-s) , s∈[0,1] .
(H2 ) : ξi ,ηi :[0,1][arrow right]...+ (i=1,2) are nondecreasing functions of bounded variation, and αi ∈[0,1) , βi ∈[0,1) , where [figure omitted; refer to PDF]
(H3 ) : f1 :[0,1]×...0+ ×...+ [arrow right]...+ , f2 :[0,1]×...+ ×...0+ [arrow right]...+ are continuous and satisfy [figure omitted; refer to PDF]
where g1 ,h2 :[0,1]×R0+ [arrow right]R+ are continuous and nonincreasing in the second variable, and g2 ,h1 :[0,1]×R+ [arrow right]R+ are continuous and for any constant r>0 , [figure omitted; refer to PDF]
Similar to the proof of Lemmas 2.1 and 2.2 in [32], the following two lemmas are valid.
Lemma 2.1.
If (H2 ) holds, then for any y∈L(0,1) , the boundary value problem [figure omitted; refer to PDF] has a unique solution [figure omitted; refer to PDF] where [figure omitted; refer to PDF]
Lemma 2.2.
If (H2 ) holds, then for any z∈L(0,1) , the boundary value problem [figure omitted; refer to PDF] has a unique solution [figure omitted; refer to PDF] where [figure omitted; refer to PDF]
Remark 2.3.
For t , s∈[0,1] , we have [figure omitted; refer to PDF]
Remark 2.4.
If (H2 ) holds, it is easy to testify Hi (t,s) defined by (2.8) that: [figure omitted; refer to PDF] where [figure omitted; refer to PDF]
Remark 2.5.
From (2.11), we can prove that the properties of Ki (t,s) (i=1,2) are similar to those of Hi (t,s) (i=1,2) .
Lemma 2.6.
For x>0 , y>0 , we have [figure omitted; refer to PDF]
Proof.
The proof of this lemma is easy, and we omit it.
Let [figure omitted; refer to PDF] where [figure omitted; refer to PDF]
It is easy to see that K is a cone of E . For any 0<r<R , let Kr,R ={(u,v)∈K:r<||u||<R, r<||v||<R} .
Remark 2.7.
By the definition of ρi , σi , γi , νi (i=1,2) , we have 0<Λ<1 .
To overcome singularity, we consider the following approximate problem of (1.3): [figure omitted; refer to PDF] where n is a positive integer and [figure omitted; refer to PDF]
Clearly, fin ∈C([0,1]×...+ ×...+ ,...+ ) (i=1,2) .
By Lemmas 2.1 and 2.2, for each n∈... , λ>0 , μ>0 , let us define operators Anλ :K[arrow right]C[0,1] , Bnμ :K[arrow right]C[0,1] , and Tn :K[arrow right]E by [figure omitted; refer to PDF] and Tn (u,v)=(Anλ (u,v),Bnμ (u,v)) , respectively.
Lemma 2.8.
Assume that (H1 ) - (H3 ) hold, then for each λ>0 , μ>0 , n∈... , Tn :K¯r,R [arrow right]K is a completely continuous operator.
Proof.
Let λ>0 , μ>0 , and n∈... be fixed. For any (u,v)∈K , by (2.21), we have [figure omitted; refer to PDF] which implies that Anλ is nonnegative and concave on [0,1] . Similarly, by (2.22) we can obtain that Bnμ is nonnegative and concave on [0,1] . For any (u,v)∈K and t∈[0,1] , it follows from (2.13) that [figure omitted; refer to PDF]
Thus [figure omitted; refer to PDF]
On the other hand, by (2.13) and (2.18), we have [figure omitted; refer to PDF]
This implies that [figure omitted; refer to PDF]
Similar to (2.27), we also have [figure omitted; refer to PDF]
Therefore, Tn (K)⊂K .
Next, we prove that Tn :K¯r,R [arrow right]K is completely continuous. Suppose (um ,vm )∈K¯r,R and (u0 ,v0 )∈K¯r,R with ||(um ,vm )-(u0 ,v0 )||[arrow right]0 (m[arrow right]∞) . We notice that t∈[0,1] fin (t,um (t),vm (t))-fin (t,u0 (t),v0 (t))[arrow right]0 (m[arrow right]∞) . Using the Lebesgue dominated convergence theorem, we have [figure omitted; refer to PDF]
Therefore, [figure omitted; refer to PDF]
Similarly, we also have [figure omitted; refer to PDF]
So Anλ :K¯r,R [arrow right]C[0,1] and Bnβ :K¯r,R [arrow right]C[0,1] are continuous. Therefore, Tn :K¯r,R [arrow right]K is also continuous.
Let D⊂K¯r,R be any bounded set, then for any (u,v)∈D , we have (u,v)∈K , r...4;||u||...4;R , r...4;||v||...4;R , and then 0<Λr...4;u(τ)...4;R , 0<Λr...4;v(τ)...4;R for any τ∈[0,1] . By (H3 ) , we have [figure omitted; refer to PDF]
It is easy to show that Anλ (D) is uniformly bounded. In order to show that Tn is a compact operator, we only need to show that Anλ (D) is equicontinuous. By the uniformly continuity of H1 (t,s) on [0,1]×[0,1] , for all [straight epsilon]>0 , there is δ>0 such that for any t1 , t2 , s∈[0,1] and |t1 -t2 |<δ , we have [figure omitted; refer to PDF]
This together with (2.15) and (2.32) implies [figure omitted; refer to PDF]
This means that Anλ (D) is equicontinuous. By the Arzela-Ascoli theorem, Anλ (D) is a relatively compact set and that Anλ :K¯r,R [arrow right]C[0,1] is a completely continuous operator.
In the same way, we can show that Bnμ :K¯r,R [arrow right]C[0,1] is also completely continuous, and so Tn :K¯r,R [arrow right]K is completely continuous. Now since λ , μ , and n are given arbitrarily, the conclusion of this lemma is valid.
3. Main Results
For notational convenience, we denote by [figure omitted; refer to PDF] where α denotes 0 or ∞ . The main results of this paper are the following.
Theorem 3.1.
Assume that (H1 ) - (H3 ) hold. Then we have:
(C1 ) : If f10 , f1∞ , f20 ∈(0,∞) and M1 /f1∞ <N1 /f10 , then for each λ∈(M1 /f1∞ ,N1 /f10 ) , μ∈(0,N2 /f20 ) , the system (1.3) has at least one positive solution.
(C2 ) : If f10 , f20 , f2∞ ∈(0,∞) and M2 /f2∞ <N2 /f20 , then for each λ∈(0,N1 /f10 ) , μ∈(M2 /f2∞ ,N2 /f20 ) , the system (1.3) has at least one positive solution.
(C3 ) : If f10 =0 , f1∞ =∞ , 0<f20 <∞ , then for each λ∈(0,∞) , μ∈(0,N2 /f20 ) , the system (1.3) has at least one positive solution.
(C4 ) : If 0<f10 <∞ , f20 =0 , f2∞ =∞ , then for each λ∈(0,N1 /f10 ) , μ∈(0,∞) , the system (1.3) has at least one positive solution.
(C5 ) : If fi0 =0 , fi∞ =∞ (i=1,2) , then for each λ∈(0,∞) , μ∈(0,∞) , the system (1.3) has at least one positive solution.
(C6 ) : If 0<f10 <∞ , f1∞ =∞ or f2∞ =∞ , 0<f20 <∞ , then for each λ∈(0,N1 /f10 ) , μ∈(0,N2 /f20 ) , the system (1.3) has at least one positive solution.
(C7 ) : If f10 =0 , 0<f1∞ <∞ , and f10 =0 , 0<f2∞ <∞ , then for each λ∈(M1 /f1∞ ,∞) , μ∈(0,∞) or λ∈(0,∞) , μ∈(M2 /f2∞ ,∞) , the system (1.3) has at least one positive solution.
Proof.
We only prove the condition in which (C1 ) holds. The other cases can be proved similarly.
Let λ∈(M1 /f1∞ ,N1 /f10 ) , μ∈(0,N2 /(f20 )) , choose [straight epsilon]1 >0 such that f1∞ -[straight epsilon]1 >0 and [figure omitted; refer to PDF]
It follows from fi0 ∈(0,∞) of (C1 ) that there exists r1 >0 such that for any t∈[0,1] , [figure omitted; refer to PDF]
Let Kr1 ={(u,v)∈K:||u||<r1 ,||v||<r1 } . For any (u,v)∈∂Kr1 , n>1/r1 , by (2.13), (3.3), we have [figure omitted; refer to PDF]
Similarly, we also have [figure omitted; refer to PDF]
Therefore, we have [figure omitted; refer to PDF]
On the other hand, by f1∞ >f1∞ -[straight epsilon]1 >0 , there exists R0 >0 such that [figure omitted; refer to PDF]
Let R1 >max {2r1 ,Λ-1R0 } , KR1 ={(u,v)∈K:||u||<R1 ,||v||<R1 } . Next, we take ([straight phi]1 ,[straight phi]2 )=(1,1)∈∂K1 , and for any (u,v)∈∂KR1 , m>0 , n∈... , we will show [figure omitted; refer to PDF]
Otherwise, there exist (u0 ,v0 )∈∂KR1 and m0 >0 such that [figure omitted; refer to PDF]
From (u0 ,v0 )∈∂KR1 , we know that ||u0 ||=R1 or ||v0 ||=R1 . Without loss of generality, we may suppose that ||u0 ||=R1 , then u0 (τ)...5;Λ||u0 ||=ΛR1 >R0 for any τ∈[0,1] . So, by (2.13), (3.8), we have [figure omitted; refer to PDF]
This implies that R1 >R1 , which is a contradiction. This yields that (3.9) holds. By (3.7), (3.9), and Lemma 1.2, for any n>1/r1 and λ∈(M1 /f1∞ ,N1 /f10 ) , μ∈(0,N2 /f20 ) , we obtain that Tn has a fixed point (un ,vn ) in K¯r1 ,R1 satisfying r1 <||un ||<R1 , r1 <||vn ||<R1 .
Let {(un ,vn )}n...5;n1 be the sequence of solutions of boundary value problems (2.19), where n1 >1/r1 is a fixed integer. It is easy to see that they are uniformly bounded. Next we show that {un }n...5;n1 are equicontinuous on [0,1] . From (un ,vn )∈K¯r1 ,R1 , we know that R1 ...5;un (τ)...5;Λ||un ||...5;Λr1 , R1 ...5;vn (τ)...5;Λ||vn ||...5;Λr1 , τ∈[0,1] . For any [straight epsilon]>0 , by the continuous of H1 (t,s) in [0,1]×[0,1] , there exists δ1 >0 such that for any t1 , t2 , s∈[0,1] and |t1 -t2 |<δ1 , we have [figure omitted; refer to PDF]
This combining with (2.15), (2.32) implies that for any t1 , t2 ∈[0,1] and |t1 -t2 |<δ1 , we have [figure omitted; refer to PDF]
Similarly, {vn }n...5;n1 are also equicontinuous on [0,1] . By the Ascoli-Arzela theorem, the sequence {(un ,vn )}n...5;n1 has a subsequence being uniformly convergent on [0,1] . From Lemma 2.2, we know that [figure omitted; refer to PDF]
Since the properties of Ki (t,s) (i=1,2) are similar to those of Hi (t,s) (i=1,2) , so (un[variant prime][variant prime] ,vn[variant prime][variant prime] ) have the similar properties of (un ,vn ) , that is, (un[variant prime][variant prime] ,vn[variant prime][variant prime] ) also has a subsequence being uniformly convergent on [0,1] . Without loss of generality, we still assume that {(un ,vn )}n...5;n1 itself uniformly converges to (u,v) on [0,1] and {(un[variant prime][variant prime] ,vn[variant prime][variant prime] )}n...5;n1 itself uniformly converges to (u[variant prime][variant prime] ,v[variant prime][variant prime] ) on [0,1] , respectively. Since {(un ,vn )}n...5;n1 ∈K¯r1 ,R1 ⊂K , so we have un ...5;0 , vn ...5;0 . By (2.19), we have [figure omitted; refer to PDF]
From (3.15) and (3.16), we know that {un [variant prime] (1/2)}n...5;n1 , {vn [variant prime] (1/2)}n...5;n1 , {un [variant prime][variant prime] (1/2)}n...5;n1 , {vn [variant prime][variant prime] (1/2)}n...5;n1 , {un [variant prime][variant prime][variant prime] (1/2)}n...5;n1 , {vn [variant prime][variant prime][variant prime] (1/2)}n...5;n1 are bounded sets. Without loss of generality, we may assume (un [variant prime] (1/2),vn [variant prime] (1/2))[arrow right](c1 ,d1 ),(un [variant prime][variant prime] (1/2),vn [variant prime][variant prime] (1/2)) [arrow right](c2 ,d2 ),(un [variant prime][variant prime][variant prime] (1/2),vn [variant prime][variant prime][variant prime] (1/2))[arrow right](c3 ,d3 ) as n[arrow right]∞ . Then by (3.15), (3.16), and the Lebesgue dominated convergence theorem, we have [figure omitted; refer to PDF]
By (3.17) and (3.18), direct computation shows that [figure omitted; refer to PDF]
On the other hand, (u,v) satisfies the boundary condition of (1.3). In fact, un (0)=un (1)=∫01 ...un (s)dξ1 (s) , vn (0)=vn (1)=∫01 ...vn (s)dξ2 (s) , [varphi]p1 (un[variant prime][variant prime] (0))=[varphi]p1 (un[variant prime][variant prime] (1))=∫01 ...[varphi]p1 (un[variant prime][variant prime] (s))dη1 (s) , [varphi]p2 (vn[variant prime][variant prime] (0))=[varphi]p2 (vn[variant prime][variant prime] (1))=∫01 ...[varphi]p2 (vn[variant prime][variant prime] (s))dη2 (s) , and so the conclusion holds by letting n[arrow right]∞ .
Theorem 3.2.
Assume that (H1 ) - (H3 ) hold. Then we have:
(D1 ) : If f10 , f1∞ , f2∞ ∈(0,∞) and M1 /f10 <N1 /f1∞ , then for each λ∈(M1 /f10 ,N1 /f1∞ ) , μ∈(0,N2 /f2∞ ) , the system (1.3) has at least one positive solution.
(D2 ) : If f1∞ , f20 , f2∞ ∈(0,∞) and M2 /f20 <N2 /f2∞ , then for each λ∈(0,N1 /f1∞ ) , μ∈(M2 /f20 ,N2 /f2∞ ) , the system (1.3) has at least one positive solution.
(D3 ) : If f10 =∞ , f1∞ =0 , 0<f2∞ <∞ , then for each λ∈(0,∞) , μ∈(0,N2 /(f2∞ )) , the system (1.3) has at least one positive solution.
(D4 ) : If 0<f1∞ <∞ , f20 =∞ , f2∞ =0 , then for each λ∈(0,N1 /f1∞ ) , μ∈(0,∞) , the system (1.3) has at least one positive solution.
(D5 ) : If fi0 =∞ , fi∞ =0 (i=1,2) , then for each λ∈(0,∞) , μ∈(0,∞) , the system (1.3) has at least one positive solution.
(D6 ) : If 0<f1∞ <∞ , f10 =∞ or f20 =∞ , 0<f2∞ <∞ , then for each λ∈(0,N1 /f1∞ ) , μ∈(0,N2 /f2∞ ) , the system (1.3) has at least one positive solution.
(D7 ) : If f1∞ =0 , 0<f10 <∞ , and f2∞ =0 , 0<f20 <∞ , then for each λ∈(M1 /f10 ,∞) , μ∈(0,∞) or λ∈(0,∞) , μ∈(M2 /f20 ,∞) , the system (1.3) has at least one positive solution.
Proof.
We may suppose that condition (D1 ) holds. Similarly, we can prove the other cases.
Let λ∈(M1 /f10 ,N1 /f1∞ ) , μ∈(0,N2 /f2∞ ) . We can choose [straight epsilon]2 >0 such that N1 -[straight epsilon]2 >0 , N2 -[straight epsilon]2 >0 and [figure omitted; refer to PDF]
It follows from (D1 ) and (2.16) that there exists R2* >0 such that for any t∈[0,1] [figure omitted; refer to PDF]
Let R2 =Λ-1R2* , KR2 ={(u,v)∈K:||u||<R2 , ||v||<R2 } . For any (u,v)∈∂KR2 , n∈... , by (2.13), (3.21), we have [figure omitted; refer to PDF]
Similarly, by (3.22) we have ||Bnμ (u,v)||<R2 . Therefore, [figure omitted; refer to PDF]
On the other hand, choose [straight epsilon]3 >0 such that M1 +[straight epsilon]3 <λf10 . By the condition f10 ∈(0,∞) of (D1 ) and (2.16), there exists r2* >0 such that [figure omitted; refer to PDF]
Let 0<r2 <min {R2 ,r2* } , Kr2 ={(u,v)∈K:||u||<r2 , ||v||<r2 } . Next, we take ([straight phi]1 ,[straight phi]2 )=(1,1)∈∂K1 , n>1/r2 , and for any (u,v)∈∂Kr2 , m>0 , we will show [figure omitted; refer to PDF]
Otherwise, there exist (u0 ,v0 )∈∂Kr2 and m0 >0 such that [figure omitted; refer to PDF]
From (u0 ,v0 )∈∂Kr2 , we know that ||u0 ||=r2 or ||v0 ||=r2 . Without loss of generality, we may suppose that ||u0 ||=r2 , then u0 (τ)...5;Λ||u0 ||...5;Λr2 for any τ∈[0,1] . So, we have [figure omitted; refer to PDF]
This implies that r2 >r2 , which is a contradiction. This yields that (3.26) holds. By (3.24), (3.26), and Lemma 1.2, for any n>1/r2 and λ∈(M1 /f10 ,N1 /f1∞ ) , μ∈(0,N2 /f2∞ ) , we obtain that Tn has a fixed point (un ,vn ) in K¯r2 ,R2 and r2 <||un ||<R2 , r2 <||vn ||<R2 . The rest of proof is similar to Theorem 3.1.
4. An Example
Example 4.1.
We consider system (1.3) with p1 =3/2 , p2 =7/3 , a1 (t)=1/(t(1-t) , a2 (t)=1/((1-t) t) , [figure omitted; refer to PDF]
Obviously, a1 , a2 are singular at t=0 and t=1 , f1 (t,u,v) is singular at u=0 and f2 (t,u,v) is singular at v=0 . Choose g1 (t,u)=(t2 +1)/u , h1 (t,v)=1+sin (v2 +v+t) , g2 (t,u)=2+sin (u+ln (t+1)) , and h2 (t,v)=(t4 +t+3)/[radical]v . Let [figure omitted; refer to PDF]
By direct calculation, we have α1 =1/4 , α2 =1/3 , β1 =3/5 , β2 =4/7 , ∫01 ...e(s)ai (s)ds=(2/3) (i=1,2) . It is easy to check that f10 =f20 =∞ , f1∞ =f2∞ =0 , and the conditions (H1 ) - (H3 ) and (D5 ) are satisfied. By Theorem 3.2, system (1.3) has at least one positive solution provided λ , μ∈(0,+∞) .
Remark 4.2.
Example 4.1 not only implies that f1 (t,u,v) , f2 (t,u,v) can be singular at u=0 and v=0 , respectively, but also indicates that there is a large number of functions that satisfy the conditions of Theorem 3.2. In addition, the condition (D5 ) is also easy to check.
Acknowledgments
The first and second authors were supported financially by the National Natural Science Foundation of China (11071141, 11126231) and the Natural Science Foundation of Shandong Province of China (ZR2009AL014, ZR2011AQ008). The third author was supported financially by the Australia Research Council through an ARC Discovery Project Grant.
[1] F. Bernis, "Compactness of the support in convex and nonconvex fourth order elasticity problems," Nonlinear Analysis , vol. 6, no. 11, pp. 1221-1243, 1982.
[2] D. G. Zill, M. R. Cullen Differential Equations and Boundary Value Problems: Computing and Modeling , Brooks Cole, 2001., 5th.
[3] T. G. Myers, J. P. F. Charpin, "A mathematical model for atmospheric ice accretion and water flow on a cold surface," International Journal of Heat and Mass Transfer , vol. 47, no. 25, pp. 5483-5500, 2004.
[4] T. G. Myers, J. P. F. Charpin, S. J. Chapman, "The flow and solidification of a thin fluid film on an arbitrary three-dimensional surface," Physics of Fluids , vol. 14, no. 8, pp. 2788-2803, 2002.
[5] D. Halpern, O. E. Jensen, J. B. Grotberg, "A theoretical study of surfactant and liquid delivery into the lung," Journal of Applied Physiology , vol. 85, no. 1, pp. 333-352, 1998.
[6] F. Mémoli, G. Sapiro, P. Thompson, "Implicit brain imaging,", supplement 1 NeuroImage , vol. 23, pp. S179-S188, 2004.
[7] A. Toga Brain Warping , Academic Press, New York, NY, USA, 1998.
[8] M. Hofer, H. Pottmann, "Energy-minimizing splines in manifolds," in Proceedings of the ACM Transactions on Graphics (SIGGRAPH '04), pp. 284-293, August 2004.
[9] S. P. Timoshenko Theory of Elastic Stability , McGraw-Hill, New York, NY, USA, 1961.
[10] W. Soedel Vibrations of Shells and Plates , Marcel Dekker, New York, NY, USA, 1993.
[11] E. Dulcska Soil Settlement Effects on Buildings , vol. 69, of Developments in Geotechnical Engineering, Elsevier, Amsterdam, The Netherlands, 1992.
[12] Z. Bai, "Existence and multiplicity of positive for a fourth-order p -Laplacian equation," Applied Mathematics and Mechanics , vol. 22, no. 12, pp. 1476-1480, 2001.
[13] Z. Bai, B. Huang, W. Ge, "The iterative solutions for some fourth-order p -Laplace equation boundary value problems," Applied Mathematics Letters , vol. 19, no. 1, pp. 8-14, 2006.
[14] Z. Bai, H. Wang, "On positive solutions of some nonlinear fourth-order beam equations," Journal of Mathematical Analysis and Applications , vol. 270, no. 2, pp. 357-368, 2002.
[15] Z. Cheng, J. Ren, "Periodic solutions for a fourth-order Rayleigh type p -Laplacian delay equation," Nonlinear Analysis , vol. 70, no. 1, pp. 516-523, 2009.
[16] M. Feng, "Multiple positive solutions of fourth-order impulsive differential equations with integral boundary conditions and one-dimensional p -laplacian," Boundary Value Problems , vol. 2011, 2011.
[17] J. R. Graef, L. Kong, "Necessary and sufficient conditions for the existence of symmetric positive solutions of singular boundary value problems," Journal of Mathematical Analysis and Applications , vol. 331, no. 2, pp. 1467-1484, 2007.
[18] J. R. Graef, C. Qian, B. Yang, "A three point boundary value problem for nonlinear fourth order differential equations," Journal of Mathematical Analysis and Applications , vol. 287, no. 1, pp. 217-233, 2003.
[19] Z. Guo, J. Yin, Y. Ke, "Multiplicity of positive solutions for a fourth-order quasilinear singular differential equation," Electronic Journal of Qualitative Theory of Differential Equations , vol. 27, pp. 1-15, 2010.
[20] S. Lu, S. Jin, "Existence of periodic solutions for a fourth-order p -Laplacian equation with a deviating argument," Journal of Computational and Applied Mathematics , vol. 230, no. 2, pp. 513-520, 2009.
[21] Y. Luo, Z. Luo, "Symmetric positive solutions for nonlinear boundary value problems with p -Laplacian operator," Applied Mathematics Letters , vol. 23, no. 6, pp. 657-664, 2010.
[22] S. Jin, S. Lu, "Periodic solutions for a fourth-order p -Laplacian differential equation with a deviating argument," Nonlinear Analysis , vol. 69, no. 5-6, pp. 1710-1718, 2008.
[23] G. Shi, X. Meng, "Monotone iterative for fourth-order p -Laplacian boundary value problems with impulsive effects," Applied Mathematics and Computation , vol. 181, no. 2, pp. 1243-1248, 2006.
[24] Z. Wang, L. Qian, S. Lu, "On the existence of periodic solutions to a fourth-order p -Laplacian differential equation with a deviating argument," Nonlinear Analysis , vol. 11, no. 3, pp. 1660-1669, 2010.
[25] J. Xu, Z. Yang, "Positive solutions for a fourth order p -Laplacian boundary value problem," Nonlinear Analysis , vol. 74, no. 7, pp. 2612-2623, 2011.
[26] J. Yang, Z. Wei, "Existence of positive solutions for fourth-order m -point boundary value problems with a one-dimensional p -Laplacian operator," Nonlinear Analysis , vol. 71, no. 7-8, pp. 2985-2996, 2009.
[27] J. Zhang, G. Shi, "Positive solutions for fourth-order singular p -Laplacian boundary value problems," Applicable Analysis , vol. 85, no. 11, pp. 1373-1382, 2006.
[28] X. Zhang, L. Liu, "Positive solutions of fourth-order four-point boundary value problems with p -Laplacian operator," Journal of Mathematical Analysis and Applications , vol. 336, no. 2, pp. 1414-1423, 2007.
[29] X. Zhang, L. Liu, "A necessary and sufficient condition for positive solutions for fourth-order multi-point boundary value problems with p -Laplacian," Nonlinear Analysis , vol. 68, no. 10, pp. 3127-3137, 2008.
[30] X. Zhang, Y. Cui, "Positive solutions for fourth-order singular p -Laplacian differential equations with integral boundary conditions," Boundary Value Problems , vol. 2010, 2010.
[31] X. Zhang, M. Feng, W. Ge, "Existence results for nonlinear boundary-value problems with integral boundary conditions in Banach spaces," Nonlinear Analysis , vol. 69, no. 10, pp. 3310-3321, 2008.
[32] X. Zhang, M. Feng, W. Ge, "Symmetric positive solutions for p -Laplacian fourth-order differential equations with integral boundary conditions," Journal of Computational and Applied Mathematics , vol. 222, no. 2, pp. 561-573, 2008.
[33] X. Zhang, W. Ge, "Positive solutions for a class of boundary-value problems with integral boundary conditions," Computers & Mathematics with Applications , vol. 58, no. 2, pp. 203-215, 2009.
[34] D. Guo, V. Lakshmikantham Nonlinear Problems in Abstract Cone , Academic Press, New York, NY, USA, 1988.
[35] K. Deimling Nonlinear Functional Analysis , Springer, New York, NY, USA, 1985.
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer
Copyright © 2012 Jiqiang Jiang et al. Jiqiang Jiang 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.
Abstract
This paper investigates the existence of positive solutions for a class of singular p -Laplacian fourth-order differential equations with integral boundary conditions. By using the fixed point theory in cones, explicit range for λ and μ is derived such that for any λ and μ lie in their respective interval, the existence of at least one positive solution to the boundary value system is guaranteed.
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer