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Volume 2011, Article ID 591219,11pages doi:10.1155/2011/591219

Research Article

Multiple Positive Solutions for

m

-Point

Boundary Value Problem on Time Scales

Jie Liu

1, 2

and Hong-Rui Sun

2

1Department of Applied Mathematics, Lanzhou University of Technology, Lanzhou, Gansu, 730050, China

2School of Mathematics and Statistics, Lanzhou University, Lanzhou, Gansu, 730000, China

Correspondence should be addressed to Hong-Rui Sun,[email protected]

Received 29 May 2010; Accepted 6 August 2010

Academic Editor: Feliz Manuel Minh ´os

Copyrightq2011 J. Liu and H.-R. Sun. 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.

The purpose of this article is to establish the existence of multiple positive solutions of the dynamic equation on time scalesφuΔthtft, ut, uΔt 0, t ∈ 0, TT, subject to the multi-point boundary conditionuΔ0 0, uT im−12aiuξi, whereφ : R → Ris an increasing homeomorphism and satisfies the relationφxy φxφyforx, y∈R, which generalizes the usuallyp-Laplacian operator. An example applying the result is also presented. The main tool of this paper is a generalization of Leggett-Williams fixed point theorem, and the interesting points are that the nonlinearityf contains the first-order derivative explicitly and the operatorφis not necessarily odd.

1. Introduction

The study of dynamic equations on time scales goes back to its founder Hilger1, and is a new area of still fairly theoretical exploration in mathematics. On one hand, the time scales approach not only unifies calculus and difference equations, but also solves other problems that have a mix of stop-start and continuous behavior. On the other hand, the time scales calculus has tremendous potential for application in biological, phytoremediation of metals, wound healing, stock market and epidemic models2–6.

LetTbe a time scalean arbitrary nonempty closed subset of the real numbersR. For each intervalIofR, we define IT I∩T. For more details on time scales, one can refer to

1–3,5. In this paper we are concerned with the existence of at least triple positive solutions to the followingm-point boundary value problems on time scales

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uΔ0 0, uT

m−2

i1

aiuξi, 1.2

whereφ:R → Ris an increasing homeomorphism andφxy φxφyforx, y∈R. Multipoint boundary value problem BVP arise in a variety of different areas of applied mathematics and physics, such as the vibrations of a guy wire of a uniform cross section and composed ofNparts of different densities can be set up as a multipoint boundary value problem 7. Small size bridges are often designed with two supported points, which leads to a standard two-point boundary value condition. And large size bridges are sometimes contrived with multipoint supports, which corresponds to a multipoint boundary value condition8. Especially, if we letutdenotes the displacement of the bridge from the unloaded position, and we emphasize the position of the bridge at supporting points near

t0, we can obtain the multipoint boundary condition1.2. The study of multipoint BVPs for linear second-order ordinary differential equations was initiated by Ilin and Moiseev

9, since then many authors studied more general nonlinear multipoint boundary value problems. We refer readers to8,10–14and the references therein.

Recently, when φ is p-Laplacian operator, that is φu |u|p−2up > 1, and the nonlinear term does not depend on the first-order derivative, the existence problems of positive solutions of boundary value problems have attracted much attention, see10,12,15–

22in the continuous case, see15,23–25in the discrete case and11,13,14,26,27in the general time scale setting. From the process of proving main results in the above references, one can notice that the oddness of thep-Laplacian operator is key to the proof. However in this paper the operatorφis not necessary odd, so it improves and generalizes thep-Laplacian operator. One may note this from Example 3.3 in Section 3. In addition, Bai and Ge 16 generalized the Leggett-Williams fixed point theorems by using fixed point index theory. An application of the theorem is given to prove the existence of three positive solutions to the following second-order BVP:

ut ft, ut, ut0, t∈0,1, 1.3

with Dirichlet boundary condition. They also extended the results to four-point BVP in12. When φu |u|p−2u and the nonlinearity f is not involved with the first-order derivative uΔt, in 27, Sun and Li discussed the existence and multiplicity of positive solutions for problems1.1and1.2. The main tools used are fixed point theorems in cones. Thanks to the above-mentioned research articles16,27, in this paper we consider the existence of multiple positive solutions for the more general dynamic equation on time scales

1.1withm-point boundary condition1.2. An example is also given to illustrate the main results. The obtained results are even new for the special cases of difference equations and differential equations, as well as in the general time scale setting. The main result extends and generalizes the corresponding results of Liu18and Webb21 TR, φu u, T

1, m 3, ft, u, v fu, Sun and Li27 φu |u|p−2u, ft, u, v ft, u. We also emphasize that in this paper the nonlinear term f is involved with the first-order delta derivativeuΔt, the operatorφis not necessary odd and have the more generalized form, and the tool is a generalized Leggett-Williams fixed point theorem16.

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final part of this section, we present an example to illustrate the application of the obtained result.

Throughout this paper, the following hypotheses hold:

H10, T ∈ T, 0 < ξ1 < ξ2 < · · · < ξm−2 < ρT, ξi ∈ T, ai ≥ 0 fori 1, . . . , m−2,and

d1−m−2i1 ai >0;

H2η max{t ∈ T : 0 < tT/2}exists and hCld0, TT,0,∞such that 0 < T

0 hs∇s <∞andf:0, TT×0,∞×−∞,∞ → 0,∞is continuous.

2. Preliminaries

In this section, we first present some basic definition, then we define an appropriate Banach space, cone, and integral operator, and finally we list the fixed-point theorem which is needed later.

Definition 2.1. SupposePis a cone in a Banach spaceB. The mapαis said to be a nonnegative continuous concaveconvexfunctional onP provided thatα : P → 0,∞is continuous and

αλx 1−λy≥≤λαx 1−λαy ∀x, y∈P, 0≤λ≤1. 2.1

Let the Banach space B Cld10, TT be endowed with the norm u max{u0,uΔ0}, where

u0t∈max0,T

T

|ut|, uΔ

0t∈sup0,T

T

uΔt, 2.2

and choose the conePBas

PuB:ut≥0 fort∈0, TT, uΔ0 0 anduis concave in0, TT. 2.3

Now we define the operatorA:PBby

Aut

T

t

φ−1

s

0

fτ, uτ, uΔτ∇τΔs

− 1 d

m−2

i1

ai T

ξi

φ−1

s

0

hτfτ, uτ, uΔτ∇τΔs.

2.4

From the definition ofAand the assumptions of H1,H2, we can easily obtain that for eachuP, Aut≥0 fort∈0, TTandAuΔ0 0. From the fact that

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we know thatAuis concave in0, TT. ThusA:PPandAu0is the maximum value of

Aut. In addition, by direct calculation, we get that each fixed point of the operatorAinP

is a positive solution of1.1and1.2. Similar as the proof of Lemma 2.3 in27, it is easy to see thatA:PPis completely continuous.

Supposeαandβare two nonnegative continuous convex functionals satisfying

x ≤L maxαx, βx, xP, 2.6

whereLis a positive constant, and

Ω xP|αx< r, βx< l/∅, r >0, l >0. 2.7

Letr > a > 0,l > 0 be given,α, βnonnegative continuous convex functionals onP

satisfying the relation2.6and2.7, andγa nonnegative continuous concave functional on

P. We define the following convex sets:

Pα, r;β, luP :αu< r, βu< l,

Pα, r;β, luP :αur, βul,

Pα, r;β, l;γ, auP :αu< r, βu< l, γu> a,

Pα, r;β, l;γ, auP :αur, βul, γua.

2.8

In order to prove our main results, the following fixed point theorem is important in our argument.

Lemma 2.2see16. LetBbe Banach space,PBa cone, andr2 ≥d > b > r1 >0, l2 ≥l1 >0. Assume thatαandβare nonnegative continuous convex functionals satisfying2.6and2.7,γis a nonnegative continuous concave functional onPsuch thatγuαufor alluPα, r2;β, l2, and

A:Pα, r2;β, l2 → Pα, r2;β, l2is a completely continuous operator. Suppose

C1{u∈Pα, d;β, l2;γ, b:γu> b}/,γAu> bforuPα, d;β, l2;γ, b;

C2αAu< r1,βAu< l1foruPα, r1;β, l1;

C3γAu> bforuPα, r2;β, l2;γ, bwithαAu> d.

ThenAhas at least three fixed pointsu1, u2, u3∈Pα, r2;β, l2with

u1∈P

α, r1;β, l1

, u2∈

Pα, r2;β, l2;γ, b

|γu> b,

u3∈P

α, r2;β, l2

\Pα, r2;β, l2;γ, b

Pα, r1;β, l1

.

2.9

3. Main Results

In this section, we impose some growth conditions onfwhich allow us to applyLemma 2.2

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1.1and1.2. We note that, from the nonnegativity ofhandf, the solution of1.1and1.2 is nonnegative and concave on0, TT.

First in view of Lemma 2.4 in27, we know that foruP, there isut≥T−t/Tu fort∈0, TT.So we get

utTη T u ≥

1

2u fort

0, ηT. 3.1

Let the nonnegative continuous convex functionals α, β and the nonnegative continuous concave functionalγbe defined on the conePby

αu max

t∈0,TT

|ut|, βu sup

t∈0,TT

uΔt, γu min

t∈0,ηT

ut, uP. 3.2

Then, it is easy to see thatumax{αu, βu}and2.6,2.7hold. Now, for convenience we introduce the following notations. Let

−1

T

0

hτ∇τ

, MTηφ−1

η

0

hτ∇τ

,

N

T

0

φ−1

s

0

hτ∇τ

Δs 1 d

m−2

i1

ai T

ξi

φ−1

s

0

hτ∇τ

Δs.

3.3

Theorem 3.1. Assumeft,0,0/≡0fort∈0, TT. If there are positive numbersr2≥2b > b > r1 >

0, l2≥l1 >0withb/M≤min{r2/N, l2/S}, such that the following conditions are satisfied

ift, u, v≤min{−φ−r2/N,−φ−l2/S}fort, u, v∈0, TT×0, r2×−l2,0;

iift, u, v>−φ−b/Mfort, u, v∈0, ηT×b,2b×−l2,0;

iiift, u, v<min{−φ−r1/N,−φ−l1/S}fort, u, v∈0, TT×0, r1×−l1,0.

then the problem1.1,1.2has at least three positive solutionsu1, u2, u3satisfying

max

t∈0,TT

u1t< r1, sup t∈0,TT

uΔ1t< l1,

b < min

t∈0,ηT

u2t≤ max t∈0,TT

u2t≤r2, sup t∈0,TT

uΔ2t≤l2,

max

t∈0,TT

u3t<2b with min t∈0,ηT

u3t< b, sup t∈0,TT

uΔ3t≤l2.

3.4

Proof. By the definition of operatorAand its properties, it suffices to show that the conditions ofLemma 2.2hold with respect to the operatorA.

We first show that if the conditioniis satisfied, then

A:Pα, r2;β, l2

−→Pα, r2;β, l2

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In fact, ifuPα, r2;β, l2,then

αu max

t∈0,TT

|ut| ≤r2, βu sup t∈0,TT

uΔt≤l2, 3.6

so assumptioniimplies

ft, ut, uΔt≤min

−φ−r2

N

,−φ

l2

S

, t∈0, TT. 3.7

On the other hand, foruP, there isAuP; thenAutis concave in0, TT, andAuΔt≤0 fort∈0, TT, so

αAu max

t∈0,TT

|Aut|Au0

T 0 φ−1 − s 0

fτ, uτ, uΔτ∇τΔs

− 1 d

m−2

i1

ai T ξi φ−1 − s 0

fτ, uτ, uΔτ∇τΔs

r2

N T 0 φ−1 s 0 hτ∇τ

Δs 1 d

m−2

i1

ai T ξi φ−1 s 0 hτ∇τ Δs

r2,

βAu sup

t∈0,TT

AuΔt−AuΔT

−φ−1

T

0

hτfτ, uτ, uΔτ∇τ

l2

−1T 0

hτ∇τ

l2.

3.8

Therefore,3.5holds.

In the same way, ifuPα, r1;β, l1, then conditioniiiimplies

ft, ut, uΔt<min

−φ−r1

N

, φ

l1

S

fort∈0, TT. 3.9

As in the argument above, we can get thatA:Pα, r1;β, l1 → Pα, r1;β, l1.Thus, condition

C2ofLemma 2.2holds.

Next we show that conditionC1inLemma 2.2holds. We chooseut 2bfort ∈ 0, TT.It is easy to see that

uPα,2b;β, l2;γ, b

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and consequently

uPα,2b;β, l2;γ, b

:γu> b/∅. 3.11

Therefore, foruPα,2b;β, l2;γ, b,there are

but≤2b, uΔt≤l2 fort

0, ηT. 3.12

Hence in view of hypothesisii, we have

ft, ut, uΔt>−φ

b M

fort∈0, ηT. 3.13

So by the definition of the functionalγ, we see that

γAu min

0,ηT

Aut Auη

T

η

φ−1

s

0

hτfτ, uτ, uΔτ∇τΔs

− 1 d

m−2

i1

ai T

ξi

φ−1

s

0

fτ, uτ, uΔτ∇τΔs

≥ −

T

η

φ−1

s

0

hτfτ, uτ, uΔτ∇τΔs

≥ −

T

η

φ−1

η

0

hτfτ, uτ, uΔτ∇τΔs

> b M

T

η

φ−1

η

0

hτ∇τΔs b

MMb.

3.14

Therefore, we getγAu > bforuPα,2b;β, l2;γ, b, and conditionC1inLemma 2.2is

fulfilled.

We finally prove thatC3inLemma 2.2holds. In fact, foruPα, r2;β, l2;γ, bwith

αAu>2b,we have

γAu min

0,ηT

Aut AuηTη T t∈max0,TT

|Aut| ≥ 1

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Thus fromLemma 2.2and the assumption thatft,0,0/≡0 on0, TT, the BVP1.1and1.2 has at least three positive solutionsu1, u2, andu3inPα, r2;β, l2with

u1∈P

α, r1;β, l1

, u2 ∈

Pα, r2;β, l2;γ, b

:γu> b,

u3∈P

α, r2;β, l2

\Pα, r2;β, l2;γ, b

Pα, r1;β, l1

.

3.16

The fact that the functionalsαandβonP satisfy an additional relation1/2αu≤γufor

uPimplies that

max

t∈0,TT

u3t<2b. 3.17

The proof is complete.

FromTheorem 3.1, we see that, when assumptions asi,ii, and iiiare imposed appropriately onf, we can establish the existence of an arbitrary odd number of positive solutions of1.1and1.2.

Theorem 3.2. Suppose that there exist constants

0< r1< b1<2b1≤r2 < b2<2b2≤ · · · ≤rn, 0< l1≤l2≤ · · · ≤ln−1, n∈N 3.18

with

bi

M ≤min

ri1

N , li1

S

for1≤in−1 3.19

such that the following conditions hold:

ift, u, v<min{−φ−ri/N,−φ−li/S}fort, u, v∈0, TT×0, ri×−li, li,1≤i

n;

iift, u, v>−φ−bi/Mfort, u, v∈0, ηT×bi,2bi×−li1, li1,1≤in.

Then, BVP1.1and1.2has at least2n−1positive solutions.

Proof. Whenn1,it is immediate from conditionithatA:Pα, r1;β, l1 → Pα, r1;β, l1,

which means that Ahas at least one fixed point u1 ∈ Pα, r1;β, l1 by the Schauder fixed

point theorem. Whenn2,it is clear that the hypothesis ofTheorem 3.1holds. Then we can obtain at least three positive solutionsu1, u2,andu3. Following this way, we finish the proof

by induction. The proof is complete.

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Example 3.3. LetT 0,1∪ {1 1/2N0}, whereN

0 denote nonnegative integer numbers

set. If we chooseT 2,η 1, m 4, a1 a2 1/3, ξ1 1/2, ξ2 3/2, andht 1 and

consider the following BVP on time scaleT:

φuΔt∇ft, ut, uΔt0, t∈0,2T,

uΔ0 0, u2 1 3u 1 2 1 3u 3 2 , 3.20 where φu ⎧ ⎪ ⎨ ⎪ ⎩

u, u≤0;

u2, u >0.

ft, u, v

⎧ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎩ 1 120t 2 3u 3 v 100 3

, t∈0,2T, u∈−∞,3, v∈−∞,∞;

1

120t18

v

100

3

, t∈0,2T, u∈3,∞, v∈−∞,∞,

3.21

obviously the hypothesesH1,H2hold andft,0,0/≡0 on0,2T. By simple calculations, we have

−1

2

0

1∇s

√2, −1

1 0 1∇s 1, N

T 1 d

m−2

i1

aiT−ξi φ−1 T 0 hs∇s

4√2.

3.22 Observe that N T 0 φ−1 s 0 hτ∇τ

Δs 1 d

m−2

i1

ai T ξi φ−1 s 0 ∇τ Δs <

T 1 d

m−2

i1

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If we chooser2180, b2, r11/3,andl278, l110, thenft, u, vsatisfies

ft, u, v≤ 45 √

2

2 min

−φ

r2

N

,−φ

l2

S

<min

−φ−r2

N

,−φ

l2

S

, t, u, v∈0,2T×0,180×−78,78;

ft, u, v>4 b

M fort, u, v∈0,1T×2,4×−78,78,

ft, u, v<

2

24 min

−φ

r1

N

,−φ

l1

S <min −φ

r1

N

,−φ

l1

S

, t, u, v∈0,2T×

0,1

3

×−10,10.

3.24

So all conditions ofTheorem 3.1hold. Thus byTheorem 3.1, the problem3.20has at least three positive solutionsu1, u2, u3such that

max

t∈0,TT u1t<

1

3; t∈sup0,TT

uΔ1t<10,

2< min

t∈0,ηT

u2t≤ max t∈0,TT

u2t≤180; sup t∈0,TT

uΔ2t≤78,

max

t∈0,TT

u3t<4 with min t∈0,ηT

u3t<2, sup t∈0,TT

uΔ3t≤78.

3.25

Acknowledgments

This work was supported by the NNSF of China10801065and NSF of Gansu Province of China0803RJZA096.

References

1 S. Hilger, “Analysis on measure chains-a unified approach to continuous and discrete calculus,” Results in Mathematics, vol. 18, no. 1-2, pp. 18–56, 1990.

2 M. Bohner and A. Peterson, Dynamic Equations on Time Scales: an Introduction with Applications, Birkh¨auser, Boston, Mass, USA, 2001.

3 M. Bohner and A. Peterson,Advances in Dynamic Equations on Time Scales, Birkh¨auser, Boston, Mass, USA, 2003.

4 M. A. Jones, B. Song, and D. M. Thomas, “Controlling wound healing through debridement,” Mathematical and Computer Modelling, vol. 40, no. 9-10, pp. 1057–1064, 2004.

5 V. Lakshmikantham, S. Sivasundaram, and B. Kaymakcalan,Dynamic systems on measure chains, vol. 370 ofMathematics and Its Applications, Kluwer Academic, Boston, Mass, USA, 1996.

6 V. Spedding, “Taming nature’s numbers,”New Scientist, vol. 7, no. 19, pp. 28–32, 2003.

(11)

8 Y. Zou, Q. Hu, and R. Zhang, “On numerical studies of multi-point boundary value problem and its fold bifurcation,”Applied Mathematics and Computation, vol. 185, no. 1, pp. 527–537, 2007.

9 V. A. Ilin and E. I. Moiseev, “Nonlocal boundary value problem of the second kind for a Sturm-CLiouville operator,”Difference Equation, vol. 23, pp. 979–987, 1987.

10 R. P. Agarwal, D. O’Regan, and P. J. Y. Wong,Positive Solutions of Differential, Difference and Integral Equations, Kluwer Academic, Boston, Mass, USA, 1999.

11 D. R. Anderson, R. Avery, and J. Henderson, “Existence of solutions for a one dimensionalp-Laplacian on time-scales,”Journal of Difference Equations and Applications, vol. 10, no. 10, pp. 889–896, 2004. 12 Z. Bai, W. Ge, and Y. Wang, “Multiplicity results for some second-order four-point boundary-value

problems,”Nonlinear Analysis, vol. 60, no. 3, pp. 491–500, 2005.

13 W. T. Li and H. R. Sun, “Positive solutions for second-orderm-point boundary value problems on time scales,”Acta Mathematica Sinica, vol. 22, no. 6, pp. 1797–1804, 2006.

14 Y.-H. Su, W.-T. Li, and H.-R. Sun, “Triple positive pseudo-symmetric solutions of three-point BVPs forp-Laplacian dynamic equations on time scales,”Nonlinear Analysis, vol. 68, no. 6, pp. 1442–1452, 2008.

15 R. I. Avery, C. J. Chyan, and J. Henderson, “Twin solutions of boundary value problems for ordinary differential equations and finite difference equations,”Computers & Mathematics with Applications, vol. 42, no. 3-5, pp. 695–704, 2001.

16 Z. Bai and W. Ge, “Existence of three positive solutions for some second-order boundary value problems,”Computers & Mathematics with Applications, vol. 48, no. 5-6, pp. 699–707, 2004.

17 C. Bereanu and J. Mawhin, “Existence and multiplicity results for some nonlinear problems with singularϕ-Laplacian,”Journal of Differential Equations, vol. 243, no. 2, pp. 536–557, 2007.

18 B. Liu, “Positive solutions of a nonlinear three-point boundary value problem,”Applied Mathematics and Computation, vol. 132, no. 1, pp. 11–28, 2002.

19 H. L ¨u, D. O’Regan, and C. Zhong, “Multiple positive solutions for the one-dimensional singularp -Laplacian,”Applied Mathematics and Computation, vol. 133, no. 2-3, pp. 407–422, 2002.

20 J. Wang, “The existence of positive solutions for the one-dimensionalp-Laplacian,”Proceedings of the American Mathematical Society, vol. 125, no. 8, pp. 2275–2283, 1997.

21 J. R. L. Webb, “Positive solutions of some three point boundary value problems via fixed point index theory,”Nonlinear Analysis, vol. 47, no. 7, pp. 4319–4332, 2001.

22 E. Zeidler,Nonlinear Analysis and Its Applications I: Fixed-Point Theorems, Springer, New York, NY, USA, 1993.

23 Z. He, “Double positive solutions of three-point boundary value problems forp-Laplacian difference equations,”Zeitschrift f ¨ur Analysis und ihre Anwendungen, vol. 24, no. 2, pp. 305–315, 2005.

24 Y. Li and L. Lu, “Existence of positive solutions of p-Laplacian difference equations,” Applied Mathematics Letters, vol. 19, no. 10, pp. 1019–1023, 2006.

25 Y. Liu and W. Ge, “Twin positive solutions of boundary value problems for finite difference equations withp-Laplacian operator,”Journal of Mathematical Analysis and Applications, vol. 278, no. 2, pp. 551– 561, 2003.

26 H.-R. Sun and W.-T. Li, “Existence theory for positive solutions to one-dimensional p-Laplacian boundary value problems on time scales,”Journal of Differential Equations, vol. 240, no. 2, pp. 217– 248, 2007.

References

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