• 検索結果がありません。

Introduction The search for the existence of positive solutions and multiple positive solu- tions to nonlinear fractional boundary value problems has expanded greatly over the past decade

N/A
N/A
Protected

Academic year: 2022

シェア "Introduction The search for the existence of positive solutions and multiple positive solu- tions to nonlinear fractional boundary value problems has expanded greatly over the past decade"

Copied!
10
0
0

読み込み中.... (全文を見る)

全文

(1)

ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu

FRACTIONAL-ORDER BOUNDARY VALUE PROBLEM WITH STURM-LIOUVILLE BOUNDARY CONDITIONS

DOUGLAS R. ANDERSON, RICHARD I. AVERY

Abstract. Using the new conformable fractional derivative, which differs from the Riemann-Liouville and Caputo fractional derivatives, we reformu- late the second-order conjugate boundary value problem in this new setting.

Utilizing the corresponding positive fractional Green’s function, we apply a functional compression-expansion fixed point theorem to prove the existence of a positive solution. We then compare our results favorably to those based on the Riemann-Liouville fractional derivative.

1. Introduction

The search for the existence of positive solutions and multiple positive solu- tions to nonlinear fractional boundary value problems has expanded greatly over the past decade; for some recent examples please see [3-9,11,14,15,17-20]. In all of these works and the references cited therein, however, the definition of the fractional derivative used is either the Caputo or the Riemann-Liouville fractional derivative, involving an integral expression and the gamma function. Recently [10, 11, 14] a new definition has been formulated and dubbed the conformable fractional deriva- tive. In this paper, we use this fractional derivative of orderα, given by

Dαf(t) := lim

ε→0

f(teεt−α)−f(t)

ε , Dαf(0) = lim

t→0+Dαf(t); (1.1) note that iff is differentiable, then

Dαf(t) =t1−αf0(t), (1.2)

wheref0(t) = limε→0[f(t+ε)−f(t)]/ε. Using this new definition of the fractional derivative, we investigate a conformable fractional boundary value problem with Sturm-Liouville boundary conditions. With the fractional differential equation and fractional boundary conditions established, we find the corresponding Green’s func- tion and prove its positivity under appropriate assumptions. This work thus sets the stage for employing a functional compression-expansion fixed point theorem to prove the existence of a positive solution to the special case of conjugate boundary conditions. We then compare our existence result to that of Bai and L¨u [3].

2000Mathematics Subject Classification. 26A33.

Key words and phrases. Conformable fractional derivative; boundary value problem;

positivity; Green’s function; conjugate conditions.

c

2015 Texas State University - San Marcos.

Submitted October 25, 2014. Published January 29, 2015.

1

(2)

2. Two Iterated Fractional Derivatives

We begin by considering two iterated fractional derivatives in the differential op- erator, together with two-point boundary conditions, as illustrated in the nonlinear boundary value problem

−DβDαx(t) =f(t, x(t)), 0≤t≤1, (2.1) γx(0)−δDαx(0) = 0 =ηx(1) +ζDαx(1), (2.2) whereα, β∈(0,1] and the derivatives are conformable fractional derivatives (1.1), withγ, δ, η, ζ ≥0 and d:=ηδ+γζ+γη/α >0. Note that ifxis α-differentiable andt1−αx0 isβ-differentiable, then using (1.2) we could rewrite (2.1) as

−t1−β t1−αx0(t)0

=f(t, x(t)), 0≤t≤1,

where the prime indicates the derivatived/dt. Before we find Green’s function for (2.1), (2.2), and prove that it is positive, we first define theβ-fractional integral.

Definition 2.1. Let β ∈ (0,1] and 0 ≤ a < b. A function f : [a, b] → R is β-fractional integrable on [a, b] if the integral

Z b a

f(s)dβs:=

Z b a

f(s)sβ−1ds

exists and is finite. Thus the integral can be interpreted either as a Riemann- Stieltjes integral or an improper Riemann integral.

Theorem 2.2. Let α, β ∈ (0,1]. The corresponding Green’s function for the ho- mogeneous problem

−DβDαx(t) = 0 satisfying the boundary conditions (2.2)is given by

G(t, s) = (1

d[δ+γαsα][ζ+αη(1−tα)], s≤t,

1

d[δ+γαtα][ζ+αη(1−sα)], t≤s,

(2.3) where we assume the parameters satisfyγ, δ, η, ζ ≥0 andd=ηδ+γζ+γη/α >0.

Proof. We will show that

x(t) = Z 1

0

G(t, s)h(s)dβs,

forGgiven by (2.3), is a solution to the linear boundary value problem

−DβDαx(t) =h(t) with boundary conditions (2.2).

For anyt∈[0,1], using the branches of (2.3) we have x(t) = 1

d[ζ+ η

α(1−tα)]

Z t 0

[δ+γ

αsα]h(s)dβs +1

d[δ+γ αtα]

Z 1 t

[ζ+ η

α(1−sα)]h(s)dβs.

Taking theα-fractional derivative yields Dαx(t) =−η

d Z t

0

[δ+γ

αsα]h(s)dβs+γ d

Z 1 t

[ζ+η

α(1−sα)]h(s)dβs.

(3)

Checking the first boundary condition, we see that γx(0)−δDαx(0) = 0.

Moreover, in checking the second boundary condition we get ηx(1) +ζDαx(1) = 0.

Taking theβ-fractional derivative of theα-fractional derivative yields DβDαx(t) =−η

d[δ+γ

αtα]h(t)tβ−1t1−β−γ d[ζ+η

α(1−tα)]h(t)tβ−1t1−β

=−1

dh(t)[ηδ+γζ+γη

α] =−h(t),

which is what we set out to prove.

Corollary 2.3 (Fractional conjugate and right-focal problems). Let α, β ∈(0,1].

The corresponding Green’s function for the homogeneous problem

−DβDαx(t) = 0

satisfying the conjugate boundary conditionsx(0) =x(1) = 0is given by

G(t, s) = (1

αsα(1−tα), s≤t,

1

αtα(1−sα), t≤s,

(2.4) and the corresponding Green’s function for the homogeneous problem

−DβDαx(t) = 0

satisfying the right-focal-type boundary conditionsx(0) =Dαx(1) = 0 is given by

G(t, s) = (1

αsα, s≤t,

1

αtα, t≤s.

(2.5) Remark 2.4. Note that the conformable fractional Green’s function based on (1.1) and given above for the conjugate boundary conditions in (2.4) differs from that found for example in Bai and L¨u [3], where the Riemann-Liouville fractional derivative is used.

Theorem 2.5 (Bounds on Green’s function). ForG(t, s) given in (2.3), we have the following bounds. First,

g1(t)G(s, s)< G(t, s)≤G(s, s) (2.6) fort, s∈[0,1], where

g1(t) := minnαδ+γtα

αδ+γ ,αζ+η(1−tα) αζ+η

o

. (2.7)

Next, for integersn≥3,

1 min

n≤t≤1−1nG(t, s)≥g2(s)G(s, s) (2.8) forg2 given by

g2(s) :=

αζ+η(1−(1−1/n)α)

αζ+η(1−sα) , s∈[0, r]

αδ+γ(1/n)α

αδ+γsα , s∈[r,1]

(2.9)

(4)

for the constant

r= αγζ+γη+αδη(n−1)α

(αδη+αγζ+γη)nα−γη(n−1)α+γη 1/α

∈(1 n,1− 1

n], (2.10) wherer= 1−1/n if γ= 0. Finally, we also have

min

1 n≤t≤1−n1

G(t, s)≥g3G(s, s) (2.11) for the constantg3 given by

g3≡minnαζ+η(1−(1−1/n)α)

αζ+η ,αδ+γ(1/n)α αδ+γ

o

(2.12) for allα∈(0,1].

Proof. It is straightforward to see that G(t, s) G(s, s) =

ζ+ηα(1−tα)

ζ+αη(1−sα), s≤t,

δ+αγtα

δ+γαsα, t≤s;

(2.13) this expression yields both inequalities in (2.6) forg1 as in (2.7).

Next, let

u(t, s) = 1 d[δ+ γ

αtα][ζ+η

α(1−sα)], so that

G(t, s) =

(u(s, t), s≤t, u(t, s), t≤s.

Letrbe given by (2.10). Then we have

1 min

n≤t≤1−1n

G(t, s) =





u(s,1−1/n), s∈[0,1/n], min{u(s,1−1/n), u(1/n, s)}, s∈[1/n,1−1/n],

u(1/n, s), s∈[1−1/n,1],

=

(u(s,1−1/n), s∈[0, r], u(1/n, s), s∈[r,1],

= (1

d[δ+αγsα][ζ+αη(1−(1−1/n)α)], s∈[0, r],

1

d[δ+αγ(1/n)α][ζ+ηα(1−sα)], s∈[r,1], whereris given in (2.10). By the monotonicity of G(t, s), we have

0≤t≤1max G(t, s) =G(s, s) =1 d[δ+ γ

αsα][ζ+ η

α(1−sα)], s∈[0,1].

Therefore if we takeg2 as in (2.9), thenG(t, s) satisfies (2.8). Now since αζ+η(1−(1−1/n)α)

αζ+η(1−sα) ≥ αζ+η(1−(1−1/n)α)

αζ+η , s∈[0, r]

and

αδ+γ(1/n)α

αδ+γsα ≥ αδ+γ(1/n)α

αδ+γ , s∈[r,1],

we could in (2.8) use the constantg3given in (2.12) instead of (2.9). This constant is well defined and strictly positive, sinced >0 in (2.3) implies neitherδandγnor

η andζ can simultaneously be zero.

(5)

Remark 2.6. For conjugate boundary conditions, γ = η = 1 and δ =ζ = 0; if α= 1 and n= 4, then g3 ≡1/4, the constant used in [13, (3.4)]. For right-focal boundary conditions,γ =ζ= 1 andδ=η= 0, so that clearlyg3≡(1/n)α for all α∈ (0,1] and all integers n ≥3. In the conjugate case specifically, the constant bound (2.12) is new for fractional derivatives, as the standard Riemann-Liouville fractional derivative does not allow one to calculate a single constant bound; see [3, Remark 2.2].

The following corollary is needed in Section 4 for the main existence theorem and example found there.

Corollary 2.7. Let α, β∈(0,1]. For everys∈[0,1]we have max

t∈[0,1]G(t, s)≤ 1 1−(3/4)α

min

t∈[1/4,3/4]G(t, s), whereG(t, s)is the Green’s function (2.4)for the homogeneous problem

−DβDαx(t) = 0

satisfying the conjugate boundary conditionsx(0) =x(1) = 0.

Proof. By (2.4), maxt∈[0,1]G(t, s) =G(s, s). Then min

t∈[14,34]

G(t, s) G(s, s) =

(1−tα

1−sα, 0≤s≤t≤3/4

tα

sα, 1/4≤t≤s≤1

1−(3/4)α

1−(0)α , 0≤s≤3/4

(1/4)α

(1)α , 1/4≤s≤1

= 1−(3/4)α,

since (1/4)α≥1−(3/4)αfor allα∈(0,1]. One could also use (2.11) and (2.12).

3. Fixed point preliminaries

In this section we will state the fixed point theorem and the definitions that are used in the fixed point theorem which will be used to verify the existence of a positive solution to the fractional-order boundary value problem with conjugate boundary conditions.

Definition 3.1. Let E be a real Banach space. A nonempty closed convex set P ⊂Eis called acone if it satisfies the following two conditions:

(i) x∈P, λ≥0 impliesλx∈P;

(ii) x∈P,−x∈P impliesx= 0.

Every coneP ⊂Einduces an ordering in E given by x≤y if and only if y−x∈P.

Definition 3.2. An operator is called completely continuous if it is continuous and maps bounded sets into precompact sets.

Definition 3.3. A mapξis said to be a nonnegative continuous concave functional on a coneP of a real Banach spaceE ifξ:P →[0,∞) is continuous and

ξ(tx+ (1−t)y)≥tξ(x) + (1−t)ξ(y)

(6)

for all x, y ∈ P and t ∈ [0,1]. Similarly we say the map φ is a nonnegative continuous convex functional on a conePof a real Banach spaceEifφ:P →[0,∞) is continuous and

φ(tx+ (1−t)y)≤tφ(x) + (1−t)φ(y)

for allx, y∈P andt∈[0,1]. We say the mapψis a sub-linear functional if ψ(tx)≤tψ(x) for allx∈P, t∈[0,1].

Definition 3.4. LetP be a cone in a real Banach space E and Ω be a bounded open subset ofE with 0∈Ω. Then a continuous functionalφ:P →[0,∞) is said to satisfy property (A1) if one of the following conditions hold:

(i) φis convex,φ(0) = 0,φ(x)6= 0 ifx6= 0, and infx∈P∩∂Ωφ(x)>0, (ii) φis sublinear,φ(0) = 0,φ(x)6= 0 ifx6= 0, and infx∈P∩∂Ωφ(x)>0, (iii) φis concave and unbounded.

Definition 3.5. LetP be a cone in a real Banach space E and Ω be a bounded open subset ofE with 0∈Ω. Then a continuous functionalφ:P →[0,∞) is said to satisfy property (A2) if one of the following conditions hold:

(i) φis convex,φ(0) = 0 andφ(x)6= 0 ifx6= 0, (ii) φis sublinear,φ(0) = 0 andφ(x)6= 0 ifx6= 0,

(iii) φ(x+y)≥φ(x) +φ(y) for allx, y∈P, φ(0) = 0,φ(x)6= 0 ifx6= 0.

The following theorem is Avery, Henderson, and O’Regan’s functional compres- sion-expansion fixed point theorem [2], which generalized the functional compres- sion fixed point theorems of Anderson-Avery [1] and Sun-Zhang [17].

Theorem 3.6. LetΩ1andΩ2 be two bounded open sets in a Banach SpaceEsuch that0∈Ω1 andΩ1⊆Ω2 andP is a cone inE. SupposeA:P∩(Ω2−Ω1)→P is completely continuous, ξ andψ are nonnegative continuous functionals onP, and one of the two conditions:

(K1) ξ satisfies property (A1) with ξ(Ax) ≥ξ(x), for all x ∈ P∩∂Ω1, and ψ satisfies property (A2)with ψ(Ax)≤ψ(x), for allx∈P∩∂Ω2 , or (K2) ξ satisfies property (A2) with ξ(Ax) ≤ξ(x), for all x ∈ P∩∂Ω1, and ψ

satisfies property (A1)with ψ(Ax)≥ψ(x), for allx∈P∩∂Ω2, is satisfied. ThenA has at least one fixed point inP∩(Ω2−Ω1).

4. Existence of a positive solution

Let the Banach spaceE=C[0,1] be endowed with the maximum norm, kxk= max

0≤t≤1|x(t)|, and define the coneP ⊂Eby

P =n

x∈E:xis nonnegative on [0,1], and kxk ≤ 1

1−(3/4)α

min

t∈[1/4,3/4]x(t)o .

Let the nonnegative continuous functionalsφandψ be defined on the coneP by ψ(x) = min

t∈[1/4,3/4]x(t) and (4.1)

φ(x) = max

t∈[0,1]x(t) =kxk. (4.2)

(7)

The following theorem is our main result.

Theorem 4.1. Letα, β∈(0,1]and suppose there exists positive numbers randR such that 0< 1−(3/4)1 α

r < R, and suppose f satisfies the following conditions:

(i) f(s, x)≤R(α+β)(2α+β)for all s∈[0,1]and all x∈[0, R], (ii) f(s, x)≥rN for alls∈[1/4,3/4]and for all x∈[r,1−(3/4)r α], where

N =

1− 3 4

αZ 3/4 1/4

G(s, s)dβs−1

and

1− 3 4

αZ 3/4 1/4

G(s, s)dβs= 1− 3

4

αn 3 4

α+β 1

α+β −(3/4)α 2α+β i

− 1 4

α+β 1

α+β − (1/4)α 2α+β

o

Then, the second order conjugate boundary value problem has at least one positive solution x such that

r≤ min

t∈[1/4,3/4]x(t) and max

t∈[0,1]x(t)≤R.

Proof. Define the completely continuous operatorAby Ax(t) =

Z 1 0

G(t, s)f(s, x(s))dβs

then if we can show thatAhas a fixed point inPthen we have verified the existence of a positive solution. Let x ∈ P, then from properties of G(t, s) we have that Ax(t)≥0 and

φ(Ax) = max

t∈[0,1]

Z 1 0

G(t, s)f(s, x(s))dβs

≤ 1 1−(3/4)α

min

t∈[1/4,3/4]

Z 1 0

G(t, s)f(s, x(s))dβs

= 1

1−(3/4)α

ψ(Ax);

thus,Ax∈P and we have verified thatA:P→P.

For allx∈P we haveψ(x)≤φ(x), thus if we let

1={x:ψ(x)< r} and Ω2={x:φ(x)< R}

we have that 0∈Ω1 and Ω1⊆Ω2, since ifx∈Ω1 then min

t∈[1/4,3/4]x(t)≤r hence sincex∈P we have

max

t∈[0,1]x(t)≤ 1 1−(3/4)α

min

t∈[1/4,3/4]x(t)≤ 1 1−(3/4)α

r < R.

Clearly Ω1and Ω2 being bounded open subsets ofP.

(8)

Claim 1: Ifx∈P∩∂Ω2, then φ(Ax)≤φ(x). Letx∈∂Ω2, thusφ(x) =Rhence by condition (i) we have

φ(Ax) = max

t∈[0,1]

Z 1 0

G(t, s)f(s, x(s))dβs

≤R(α+β)(2α+β) Z 1

0

G(s, s)dβs

=R=φ(x).

Claim 2: If x∈ P∩∂Ω1, thenψ(Ax)≥ψ(x). Letx∈∂Ω1, thus ψ(x) =r and kxk ≤ r

1−(34)α, hence by condition (ii) we have ψ(Ax) = min

t∈[1/4,3/4]

Z 1 0

G(t, s)f(s, x(s))dβs

≥rN 1− 3

4

αZ 3/4 1/4

G(s, s)dβs

=r=ψ(x).

Clearlyφ satisfies property (A1)(i) andψ satisfies property (A2)(iii) thus the hy- pothesis (K1) of Theorem 3.6 is satisfied, and therefore A has a fixed point in

2−Ω1.

Example 4.2. To compare our results with those in [3, Example 3.1], where the authors use the Riemann-Liouville fractional derivative of order 3/2 ∈ (1,2], we take α= 1,β = 1/2,r= 11/1000, R= 9/25, andf(s, x) = 1 + (1/4) sins+x2 in Theorem 4.1 to get the following. One can check that 0<4r < R, andf satisfies the following conditions:

(i)

f(s, x)≤ 15 4 R= 27

20 for alls∈[0,1] and all x∈[0,9/25], (ii)

f(s, x)≥ 960r 33√

3−17 = 264 25(33√

3−17) for alls∈[1/4,3/4] and for allx∈[r,4r].

Thus by Theorem 4.1 the 32-order conjugate boundary value problem

−D0.5x0(t) = 1 + 1

4sint+x(t)2, x(0) =x(1) = 0 has at least one positive solutionxsuch that

11

1000 ≤ min

t∈[1/4,3/4]x(t) and max

t∈[0,1]x(t)≤ 9 25.

In [3, Example 3.1], the result is the existence of a positive solutionx such that 1

14 ≤ max

t∈[0,1]x(t)≤1, with no information on the minimum value of the function.

(9)

References

[1] D. R. Anderson, R.I. Avery; Fixed point theorem of cone expansion and compression of functional type,J. Difference Equations Appl.8(2002), pp. 1073–1083.

[2] R. I. Avery, J. Henderson, D. O’Regan; Functional compression-expansion fixed point theo- rem,Electron. J. Differential Equations2008(2008), No. 22, pp. 1-12.

[3] Zhanbing Bai, Haishen L¨u; Positive solutions for boundary value problem of nonlinear frac- tional differential equation,J. Math. Anal. Appl.311Issue 2 (2005) 495–505.

[4] Bashir Ahmad, J. J. Nieto; Existence results for a coupled system of nonlinear fractional dif- ferential equations with three-point boundary conditions,Computers Math. Appl,58(2009) 1838–1843.

[5] Alberto Cabada, Guotao Wang; Positive solutions of nonlinear fractional differential equa- tions with integral boundary value conditions, J. Math. Anal. Appl. 389 Issue 1 (2012) 403–411.

[6] Guoqing Chai, Songlin Hu; Existence of positive solutions for a fractional high-order three- point boundary value problem,Advances in Difference Equations 20142014:90.

[7] Yanli Chen, Yongxiang Li; The existence of positive solutions for boundary value problem of nonlinear fractional differential equations,Abst. Appl. Anal.2014(2014), Article ID 681513, 7 pages.

[8] Shengping Chen, Yuji Liu; Solvability of boundary value problems for fractional order elastic beam equations,Advances in Difference Equations20142014:204.

[9] P. W. Eloe, J. T. Neugebauer; Existence and comparison of smallest eigenvalues for a frac- tional boundary-value problem,Electron. J. Differential Equations2014(2014), No. 43, pp.

1–10.

[10] U. Katugampola; A new fractional derivative with classical properties,J. American Math.

Soc., arXiv:1410.6535v2.

[11] M. Abu Hammad, R. Khalil; Abel’s formula and Wronskian for conformable fractional dif- ferential equations,International J. Differential Equations Appl.,13No. 3 (2014) 177–183.

[12] Xiaoling Han, Hongliang Gao; Existence of positive solutions for eigenvalue problem of non- linear fractional differential equations,Advances in Difference Equations20122012:66.

[13] J. Henderson, H. B. Thompson; Multiple symmetric positive solutions for a second order boundary value problem,Proc. Amer. Math. Soc.,128Number 8 (2000) 2373–2379.

[14] R. Khalil, M. Al Horani, A. Yousef, M. Sababheh; A new definition of fractional derivative, J. Computational Appl. Math.,264(2014) 65–70.

[15] Xiaoyou Liu, Yiliang Liu; Fractional differential equations with fractional non-separated boundary conditions,Electron. J. Differential Equations2013(2013), No. 25, pp. 1–13.

[16] N. I. Mahmudov, S. Unul, Existence of solutions of α (2,3] order fractional three-point boundary value problems with integral conditions,Abst. Appl. Anal.2014(2014), Article ID 198632, 12 pages.

[17] J. Sun, G. Zhang; A generalization of the cone expansion and compression fixed point theorem and applications,Nonlinear Anal.67(2007), 579-586.

[18] Yongping Sun, Xiaoping Zhang; Existence and nonexistence of positive solutions for fractional-order two-point boundary value problems,Advances in Difference Equations2014 2014:53.

[19] J. Wu, X. Zhang; Eigenvalue problem of nonlinear semipositone higher order fractional dif- ferential equations,Abst. Appl. Anal.2012(2012), Art. ID 740760, 14 pp.

[20] X. Zhang, L. Liu, B. Wiwatanapataphee, Y. Wu; Positive solutions of eigenvalue problems for a class of fractional differential equations with derivatives,Abst. Appl. Anal.2012(2012), Art. ID 512127, 16 pp.

[21] Xiangbing Zhou, Wenquan Wu; Uniqueness and asymptotic behavior of positive solutions for a fractional-order integral boundary-value problem,Electron. J. Differential Equations2013 (2013), No. 37, pp. 1–10.

(10)

Addendum posted on February 4, 2016

In response to a question from a reader, we clarify that “conformable fractional derivative” means “at α= 1 only”; i.e. asαapproaches 1, we recover the full de- rivative. It obvious that asαapproaches 0, we do not recover the identity operator.

End of addendum

Douglas R. Anderson

Department of Mathematics, Concordia College, Moorhead, MN 56562, USA E-mail address:[email protected]

Richard I. Avery

College of Arts and Sciences, Dakota State University, Madison, SD 57042, USA E-mail address:[email protected]

参照

関連したドキュメント

As a consequence of our convergence reult Theorem 2, we are able to extend the description of the excursion measure of the process reflected at its minimum (see Proposition 15, p.

By virtue of the upper and lower solutions method, as well as the Schauder fixed point theorem, the existence of positive solutions to a class of q-fractional difference boundary

Recently, the (n, p) boundary value problems have been given extensive at- tention to the existence of positive solutions, for some excellent results, we refer to R.P.. Wong

Trofimchuk, Existence of a solution of a three-point boundary value problem and the spectral radius of a related linear operator, Nonlinear Anal.. Moiseev, Nonlocal boundary

Zhu; A priori estimates, existence and non-existence of positive solutions of generalized mean curvature equations, Nonlinear.. Deng, Existence of Multiple Solutions to

We make use of a generalization of the fixed point theorem of compression and expansion of functional type to obtain the existence of positive

For example, the vibrations of a guy wire of uniform cross-section and composed of N parts of different densi- ties can be set up as a multi-point boundary-value problem,many

This paper investigates the existence and uniqueness of C[0, 1] pos- itive solutions for a second order integral boundary value problem.. We mainly use the method of lower and