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Volume 2008, Article ID 257680,19pages doi:10.1155/2008/257680

Research Article

Twin Positive Solutions of a Nonlinear

m -Point Boundary Value Problem for Third-Order p -Laplacian Dynamic Equations on Time Scales

Wei Han1and Guang Zhang2

1Department of Mathematics, North University of China, Taiyuan 030051, China

2Department of Mathematics, School of Science, Tianjin University of Commerce, Tianjin 300134, China

Correspondence should be addressed to Wei Han,qd [email protected] Received 20 April 2008; Accepted 20 June 2008

Recommended by Binggen Zhang

Several existence theorems of twin positive solutions are established for a nonlinear m-point boundary value problem of third-order p-Laplacian dynamic equations on time scales by using a fixed point theorem. We present two theorems and four corollaries which generalize the results of related literature. As an application, an example to demonstrate our results is given. The obtained conditions are different from some known results.

Copyrightq2008 W. Han and G. Zhang. 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

A time scaleT is a nonempty closed subset ofR. We make the blanket assumption that 0 andT are points inT. By an interval0, T, we always mean the intersection of the real interval0, T with the given time scale, that is,0, T∩T.

In this paper, we will be concerned with the existence of positive solutions of the p- Laplacian dynamic equations on time scales:

φpuΔ∇atft, ut 0, t∈0, T, 1.1

φpuΔ∇0 m−2

i1

aiφpuΔ∇ξi, uΔ0 0, uT m−2

i1

bii, 1.2

whereφpsisp-Laplacian operator; that is,φps |s|p−2s, p >1, φ−1p φq, 1/p1/q1, 0<

ξ1<· · ·< ξm−2< ρT, and

H1ai, bi∈0,∞, i1,2, . . . ,satisfy 0<m−2

i1 ai<1 andm−2

i1 bi<1;

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H2atCld0, T ,0,∞and there existst0∈ξm−2, Tsuch thatat0>0;

H3fC0, T ×0,∞,0,∞.

We point out that theΔ-derivative and the∇-derivative in1.2and theCldspace inH2are defined inSection 2.

Recently, there has been much attention paid to the existence of positive solutions for third-order nonlinear boundary value problems of differential equations. For example, see 1–10 and the listed references. Anderson2 considered the following third-order nonlinear problem:

xt ft, xt, t1tt3,

xt1 xt2 0, γxt3 δxt3 0. 1.3

He used the Krasnoselskii and the Leggett and Williams fixed-point theorems to prove the existence of solutions to the nonlinear problem1.3. Li6 considered the existence of single and multiple positive solutions to the nonlinear singular third-order two-point boundary value problem:

ut λatfut 0, 0< t <1,

u0 u0 u1 0. 1.4

Under various assumptions onaandf, they established intervals of the parameterλwhich yield the existence of at least two and infinitely many positive solutions of the boundary value problem by using Krasnoselski’s fixed-point theorem of cone expansion-compression type. Liu et al.7 discussed the existence of at least one or two nondecreasing positive solutions for the following singular nonlinear third-order differential equations:

xt λαtft, xt 0, a < t < b,

xa xa xb 0. 1.5

Green’s function and the fixed-point theorem of cone expansion-compression type are utilized in their paper. In8 , Sun considered the following nonlinear singular third-order three-point boundary value problem:

ut−λatFt, ut 0, 0< t <1,

u0 uη u1 0. 1.6

He obtained various results on the existence of single and multiple positive solutions to the boundary value problem1.6by using a fixed-point theorem of cone expansion-compression type due to Krasnosel’skii. In10 , Zhou and Ma studied the existence and iteration of positive solutions for the following third-order generalized right-focal boundary value problem with p-Laplacian operator:

φput qtft, ut, 0≤t≤1, u0 m

i1αii, uη 0, u1 n

i1βiuθi. 1.7

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They established a corresponding iterative scheme for1.7by using the monotone iterative technique.

On the other hand, the existence of positive solutions for third-order nonlinear boundary value problems of difference equations is also extensively studied by a number of authorssee 1,3,5,9 and the listed references. The present work is motivated by a recent paper4 . In 4 , Henderson and Yin considered the existence of solutions for a third-order boundary value problem on a time-scale equation of the form

uΔ3ft, u, uΔ, uΔΔ, tT, 1.8 which is uniform for the third-order difference equation and the third-order differential equation.

2. Preliminaries and lemmas

For convenience, we list the following definitions which can be found in4,11–15 .

Definition 2.1. Let T be a time scale. Fort < supT and r > infT, define the forward jump operatorσand the backward jump operatorρ, respectively, by

σt inf{τ∈T|τ > t} ∈T,

ρr sup{τ∈T|τ < r} ∈T 2.1

for allt, rT. Ifσt > t,tis said to be right-scattered, and ifρr < r, r is said to be left- scattered; ifσt t,tis said to be right-dense, and ifρr r, r is said to be left-dense. If T has a right-scattered minimumm, defineTk T− {m}; otherwise setTk T. If T has a left-scattered maximumM, defineTkT− {M}; otherwise setTkT.

Definition 2.2. Forf : T→RandtTk, the delta derivative off at the pointtis defined to be the numberfΔt provided that it exists, with the property that for each >0 there is a neighborhoodUoftsuch that

|fσt−fsfΔtσt−s| ≤|σts| 2.2 for allsU.

Forf:T→RandtTk, the nabla derivative offattis denoted byft provided that it exists, with the property that for each >0 there is a neighborhoodUoftsuch that

|fρt−fs−ftρt−s| ≤|ρts| 2.3 for allsU.

Definition 2.3. A functionfis left-dense continuousi.e.,ld-continuousiff is continuous at each left-dense point inT, and its right-sided limit exists at each right-dense point in T.

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Definition 2.4. IfφΔt ft, then one defines the delta integral by b

a

ftΔtφbφa. 2.4

IfFt ft, then one defines the nabla integral by b

a

ft∇tFbFa. 2.5

To prove the main results in this paper, we will employ several lemmas. These lemmas are based on the linear BVP

φpuΔ∇ht 0, t∈0, T, 2.6 φpuΔ∇0 m−2

i1

aiφpuΔ∇ξi, uΔ0 0, uT m−2

i1

bii. 2.7

Lemma 2.5. Ifm−2

i1 ai/1 andm−2

i1 bi/1, then forhCld0, T the BVP2.6-2.7has the unique solution

ut

t

0

t−q

s 0

hτ∇τA

∇sC, 2.8

where

Am−2

i1 ai

ξi

0∇τ

1−m−2

i1 ai

,

C T

0T−qs

0hτ∇τA∇sm−2

i1 bi

ξi

0ξiqs

0hτ∇τA∇s

1−m−2

i1 bi

.

2.9

Proof. iLetube a solution, then we will show that2.8holds. By taking the nabla integral of problem2.6on0, t, we have

φpuΔ∇t − t

0

hτ∇τA 2.10

then

uΔ∇t φq

t

0

hτ∇τA

−φq

t

0

∇τ−A

. 2.11

By taking the nabla integral of2.11on0, t, we can get uΔt −

t

0

φq

s

0

hτ∇τA

∇sB. 2.12

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By taking the delta integral of2.12on0, t, we can get

ut

t

0

t−q

s

0

hτ∇τA

∇sBtC. 2.13

Similarly, lett0 on2.10, then we haveφpuΔ∇0 A; lettξion2.10, then we have

φpuΔ∇ξiξi

0

hτ∇τA. 2.14

Lett0 on2.12, then we have

uΔ0 B. 2.15

LettT on2.13, then we have

uT

T

0

T−q

s 0

∇τ−A

∇sBTC. 2.16

Similarly, letion2.13, then we have

iξi

0

ξiq

s 0

hτ∇τA

∇siC. 2.17

By the boundary condition2.7, we can get

B0, 2.18

Am−2

i1ai

ξi

0

hτ∇τA

. 2.19

Solving2.19, we get

Am−2

i1 ai

ξi

0hτ∇τ

1−m−2

i1 ai

. 2.20

By the boundary condition2.7, we can obtain

T

0

T−q

s

0

hτ∇τA

∇sCm−2

i1

bi

ξi

0

ξiq

s

0

hτ∇τA

∇sC . 2.21

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Substituting2.20in the above expression, one has

C T

0T−qs

0hτ∇τA∇sm−2

i1 bi

ξi

0ξiqs

0hτ∇τA∇s

1−m−2

i1 bi

. 2.22

iiWe show that the functionugiven in2.8is a solution.

Letube as in2.8. By12, Theorem 2.10iii and taking the delta derivative of2.8, we have

uΔt − t

0

φq

s

0

hτ∇τA

∇s; 2.23

moreover, we get

uΔ∇t −φq

t

0

hτ∇τA

,

φpuΔ∇t

0

∇τ−A

.

2.24

Taking the nabla derivative of this expression yields φpuΔ∇ −ht. Also, routine calculation verifies thatusatisfies the boundary value conditions in2.7so thatugiven in 2.8is a solution of2.6and2.7. The proof is complete.

Lemma 2.6. AssumeH1holds. ForhCld0, T andh0, the unique solutionuof2.6and2.7 satisfies

ut0 for t∈0, T . 2.25

Proof. Let

ϕ0s φq

s 0

hτ∇τA

. 2.26

Since

s

0

hτ∇τA

s

0

hτ∇τ

m−2

i1 ai

ξi

0∇τ

1−m−2

i1 ai

≥0, 2.27

thenϕ0s≥0.

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According toLemma 2.5, we get

u0 C

T

0T−0s∇s−m−2

i1 bi

ξi

0ξi0s∇s 1−m−2

i1 bi

T

0T−0s∇s−m−2

i1 bi

ξi

0T−0s∇s 1−m−2

i1 bi

T

0T−0s∇s−m−2

i1 biT

0T−0s∇s−T

ξiT−0s∇s 1−m−2

i1 bi

T

0

T−0s∇s m−2

i1 bi

T

ξiT−0s∇s 1−m−2

i1 bi

≥0,

uT

T

0

T−0s∇sC

T

0

T−0s∇s T

0T−0s∇s−m−2

i1 bi

ξi

0ξi0s∇s 1−m−2

i1 bi

≥ − T

0

T−0s∇s T

0T−0s∇s−m−2

i1 bi

ξi

0T−0s∇s 1−m−2

i1 bi

m−2

i1 bi

T

ξiT−0s∇s 1−m−2

i1 bi

≥0.

2.28

Ift∈0, T, we have

ut

t

0

t−0s∇s 1 1−m−2

i1 bi

T

0

T−0s∇s−m−2

i1

bi

ξi

0

ξi0s∇s

≥ − T

0

T−0s∇s 1 1−m−2

i1 bi

T

0

T−0s∇s−m−2

i1

bi

ξi

0

T−0s∇s

1 1−m−2

i1 bi

1−m−2

i1

bi

T

0

T−sϕ0s∇s T

0

T−sϕ0s∇s−m−2

i1

bi

ξi

0

T−sϕ0s∇s

1 1−m−2

i1 bi m−2

i1

bi

T

ξi

T−0s∇s≥0.

2.29 Sout≥0, t∈0, T .

Lemma 2.7. AssumeH1holds. IfhCld0, T andh0, then the unique solutionuof 2.6and 2.7satisfies

t∈0,T inf utγu, 2.30

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where

γ m−2

i1 biT−ξi Tm−2

i1 biξi

, u max

t∈0,T |ut|. 2.31

Proof. It is easy to check thatuΔt −t

0ϕ0s∇s≤0; this implies that uu0, min

t∈0,T ut uT. 2.32

It is easy to see that uΔt2uΔt1for any t1, t2 ∈ 0, T with t1t2. Hence,uΔt is a decreasing function on0, T . This means that the graph ofutis concave down on0, T.

For eachi∈ {1,2, . . . , m−2}, we have

uTu0

T−0 ≥ uTi

Tξi , 2.33

that is,

TuξiξiuT≥T−ξiu0, 2.34

so that

T

m−2

i1

biim−2

i1

biξiuTm−2

i1

biT−ξiu0. 2.35

With the boundary conditionuT m−2

i1 bii, we have uT

m−2

i1 biT−ξi Tm−2

i1 biξi

u0. 2.36

This completes the proof.

Let the norm onCld0, T be the maximum norm. Then, theCld0, T is a Banach space.

It is easy to see that BVP1.1-1.2has a solutionuutif and only ifuis a fixed point of the operator

Aut − t

0

t−q

s 0

fτ, uτ∇τ−A

∇sC, 2.37 where

Am−2

i1 ai

ξi

0aτfτ, uτ∇τ 1−m−2

i1 ai

,

C T

0T−sφqs

0aτfτ, uτ∇τA∇s− m−2

i1 bi

ξi

0ξiqs

0aτfτ, uτ∇τA∇s 1−m−2

i1 bi

. 2.38 Denote

K

u|uCld0, T , ut≥0, inf

t∈0,T utγu

, 2.39

whereγ is the same as inLemma 2.7. It is obvious thatKis a cone inCld0, T . ByLemma 2.7, AKK. So by applying Arzela-Ascoli theorem on time scales16 , we can obtain thatAK is relatively compact. In view of Lebesgue’s dominated convergence theorem on time scales 13 , it is easy to prove thatAis continuous. Hence,A:K→Kis completely continuous.

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Lemma 2.8. A:K→Kis completely continuous.

Proof. First, we show thatAmaps bounded set into bounded set.

Assumec >0 is a constant anduKc{u∈K:u ≤c}. Note that the continuity off guarantees that there isc>0 such thatft, utφpcfort∈0, T . So

Au max

t∈0,T |Aut| ≤C

T

0T−qs

0aτfτ, uτ∇τ−A∇s 1−m−2

i1 bi

cT

0T−qs

0∇τm−2

i1 ai

ξi

0aτ∇τ/1m−2

i1 ai∇s 1−m−2

i1 bi

.

2.40

That is,AKcis uniformly bounded.

In addition, notice that for anyt1, t2∈0, T , we have

|Aut1Aut2|

t1

0

t2−t1φq

s

0

aτfτ, uτ∇τA

∇s t2

t1

t2−sφq

s

0

fτ, uτ∇τ−A

∇s

c|t1t2| T

0

φq

s

0

∇τ m−2

i1 ai

ξi

0aτ∇τ

1−m−2

i1 ai

∇s Tmax

s∈0,T φq

s 0

∇τ m−2

i1 ai

ξi

0aτ∇τ

1−m−2

i1 ai

.

2.41

So, by applying Arzela-Ascoli theorem on time scales16 , we obtain thatAKc is relatively compact.

Finally, we prove that A : Kc→K is continuous. Suppose that {un}n1Kc and unt converges toutuniformly on 0, T .Hence, {Aunt}n1 is uniformly bounded and equicontinuous on0, T . The Arzela-Ascoli theorem on time scales 16 tells us that there exists uniformly convergent subsequence in{Aunt}n1.Let{Aunmt}m1be a subsequence which converges tovtuniformly on0, T .In addition,

0≤Aunt≤cT

0T−qs

0∇τm−2

i1 ai

ξi

0aτ∇τ/1m−2

i1 ai∇s 1−m−2

i1 bi

. 2.42

Observe the expression of{Aunmt},and then lettingm→∞,we obtain

vt

t

0

t−q

s

0

aτfτ, uτ∇τ−A

∇sC, 2.43

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where

Am−2

i1 ai

ξi

0aτfτ, uτ∇τ 1−m−2

i1 ai

,

C 1

1−m−2

i1 bi

T 0

T−q

s 0

fτ, uτ∇τ−A

∇s

m−2

i1

bi

ξi

0

ξiq

s 0

aτfτ, uτ∇τ−A

∇s .

2.44

Here, we have used the Lebesgue dominated convergence theorem on time scales13 . From the definition ofA, we know thatvt Auton0, T .This shows that each subsequence of{Aunt}n1uniformly converges toAut.Therefore, the sequence{Aunt}n1uniformly converges toAut.This means thatAis continuous atuKc. So,Ais continuous onKc

sinceuis arbitrary. Thus,Ais completely continuous. This proof is complete.

Lemma 2.9. Let

ϕs φq

s 0

aτfτ, uτ∇τ−A

. 2.45

Forξi i1, . . . , m−2, ξi

0

ξisϕs∇sξi

T T

0

T−sϕs∇s. 2.46

Proof. Since s

0

aτfτ, uτ∇τA s

0

fτ, uτ∇τ m−2

i1 ai

ξi

0aτfτ, uτ∇τ 1−m−2

i1 ai

≥0,

2.47

thenϕs≥0. For all t∈0, T , we have t

0t−sϕs∇s t

tt

0ϕs∇st

0t−sϕs∇s

tρt ≥0. 2.48

In fact, letψt tt

0ϕs∇st

0t−sϕs∇s; taking the nabla derivative of this expression, we have

ψt t

0

ϕs∇stϕtt

0

ϕs∇stϕt≥0. 2.49

Hence,ψtis a nondecreasing function on0, T . That is,

ψt≥0. 2.50

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For all t∈0, T ,

t

0t−sϕs∇s

t

T

0T−sϕs∇s

T . 2.51

By2.51, forξi i1, . . . , m−2, we have ξi

0

ξisϕs∇sξi

T T

0

T−sϕs∇s. 2.52

Lemma 2.10see17 . LetEbe a Banach space, and letKEbe a cone. AssumeΩ1,Ω2are open bounded subsets ofEwith 0∈Ω1,Ω1⊂Ω2,and let

F:K∩Ω21→Kbe a completely continuous operator such that iFu ≤ u, u∈K∂Ω1,andFu ≥ u, u∈K∂Ω2, or iiFu ≥ u, u∈K∂Ω1, andFu ≤ u, u∈K∂Ω2. Then,Fhas a fixed point inK∩Ω21.

Now, we introduce the following notations. Let A0

1 1−m−2

i1 bi

T

0

T−q

s

0

aτ∇τ

m−2

i1 ai

ξi

0aτ∇τ

1−m−2

i1 ai

∇s −1

,

B0

Tm−2

i1 bim−2

i1 biξi

T1m−2

i1 bi T

0

T−q

s 0

aτ∇τ

m−2

i1 ai

ξi

0∇τ

1−m−2

i1 ai

∇s −1

.

2.53

Forl >0, Ωl{u∈K:u< l}, and∂Ωl{u∈K:ul},

αl sup{Au: u∂Ωl}, βl inf{Au: u∂Ωl}, 2.54 byLemma 2.6, whereαandβare well defined.

3. Main results

Theorem 3.1. AssumeH1,H2, andH3hold, and assume that the following conditions hold:

A1piC0,∞,0,∞, i1,2, and

l→0lim p1l

lp−1 < Ap−10 , lim

l→∞

p2l

lp−1 < Ap−10 ; 3.1

A2kiL10, T ,0,∞, i1,2;

A3there exist 0< c1c2and 0λ2< p−1< λ1such that

ft, lp1l k1tlλ1, t, l∈0, T ×0, c1 ,

ft, lp2l k2tlλ2, t, l∈0, T ×c2,∞; 3.2

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A4there existsb >0 such that

min{ft, l:t, l∈0, T ×γb, b } ≥bB0p−1. 3.3

Then, problem1.1-1.2has at least two positive solutionsu1, u2satisfying 0<u1< b <u2. Theorem 3.2. AssumeH1,H2, andH3hold, and assume that the following conditions hold:

B1piC0,∞,0,∞, i3,4, and

l→0lim p3l

lp−1 >

B0

γ p−1

, lim

l→∞

p4l lp−1 >

B0

γ p−1

; 3.4

B2kiL10, T ,0,∞, i3,4;

B3there exist 0< c3c4and 0λ4< p−1< λ3such that

ft, lp3l−k3tlλ3, t, l∈0, T ×0, c3 ,

ft, lp4l−k4tlλ4, t, l∈0, T ×c4,∞; 3.5

B4there existsa >0 such that

max{ft, l:t, l∈0, T ×0, a } ≤aA0p−1. 3.6

Then, problem1.1-1.2has at least two positive solutionsu3, u4satisfying 0<u3< a <u4. Proof ofTheorem 3.1. Let

1

2min

Ap−10 −lim

l→0

p1l

lp−1 , Ap−10 −lim

l→∞

p2l

lp−1 , 3.7

then there exist 0< a1c1andc2a2<∞such that

p1l≤Ap−10lp−1, 0≤la1,

p2l≤Ap−10lp−1, a2l≤∞. 3.8

If 0≤la1, u∂Ωl, then 0≤utl, 0≤tT. By conditionA3, we have ft, utp1ut k1tuλ1t

≤Ap−10up−1t k1tuλ1t

≤Ap−10up−1k1tuλ1 Ap−10lp−1k1tlλ1

3.9

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so thats

0

aτfτ, uτ∇τA

s

0

fτ, uτ∇τ m−2

i1 ai

ξi

0aτfτ, uτ∇τ 1−m−2

i1 ai

s

0

Ap−10lp−1k1τlλ1 ∇τ m−2

i1 ai

ξi

0Ap−10lp−1k1τlλ1 ∇τ 1−m−2

i1 ai

. 3.10 Therefore,

Au ≤C 1 1−m−2

i1 bi

T

0

T−sϕs∇sm−2

i1bi

ξi

0

ξisϕs∇s

≤ 1

1−m−2

i1 bi

T

0

T−sϕs∇s

≤ 1

1−m−2

i1 bi

× T

0

T−q

s

0

aτAp−10lp−1k1τlλ1 ∇τ

m−2

i1 ai

ξi

0Ap−10lp−1k1τlλ1 ∇τ 1−m−2

i1 ai

∇s.

3.11

It follows that αl

l ≤ 1

1−m−2

i1 bi

× T

0

T−q

s 0

aτAp−10k1τlλ1−p1 ∇τ

m−2

i1 ai

ξi

0Ap−10k1τlλ1−p1 ∇τ 1−m−2

i1 ai

∇s.

3.12

Noticingλ1p1>0, we have liml→0

αl

l ≤ 1

1−m−2

i1 bi

T

0

T−q

s

0

aτAp−10∇τ m−2

i1 ai

ξi

0aτAp−10∇τ 1−m−2

i1 ai

∇s

Ap−101/p−1 1−m−2

i1 bi

T

0

T−q

s 0

aτ∇τ

m−2

i1 ai

ξi

0∇τ

1−m−2

i1 ai

∇s

Ap−101/p−1A−10 1−A−p−10 1/p−1<1.

3.13 Therefore, there exist 0< a1< a1such thatαa1< a1. It implies thatAu<u, u∈∂Ωa1.

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Ifa2l <∞andu∂Ωl, then 0≤utl. Similar to the above argument, noticing thatλ2p1 <0, we can get liml→∞αl/l<1. Therefore, there exist 0< a2 < a2such that αa2< a2. It implies thatAu<u, u∈∂Ωa2.

On the other hand, sincef :0, T ×0,∞→0,∞is continuous, by conditionA4, there exista1< b1< b < b2< a2such that

min{ft, l:t, l∈0, T ×γbi, bi } ≥biB0p−1, i1,2. 3.14 Ifu∂Ωb1, thenγb1utb1, 0≤tT. ApplyingLemma 2.9, it follows that

Aumax

0≤t≤T|Aut|

≥ − T

0

T−sϕs∇s 1

1−m−2

i1 bi

T

0

T−sϕs∇sm−2

i1

bi

ξi

0

ξisϕs∇s

m−2

i1 bi

1−m−2

i1 bi

T

0

T−sϕs∇sm−2

i1 bi

ξi

0ξisϕs∇s 1−m−2

i1 bi

m−2

i1 bi

1−m−2

i1 bi

T

0

T−sϕs∇s

m−2

i1 biξi

T1m−2

i1 bi T

0

T−sϕs∇s

Tm−2

i1 bim−2

i1 biξi

T1m−2

i1 bi T

0

T−sϕs∇s

Tm−2

i1 bim−2

i1 biξi

T1m−2

i1 bi T

0

T−q

s 0

aτb1B0p−1∇τ m−2

i1 ai

ξi

0aτb1B0p−1∇τ 1−m−2

i1 ai

∇s Tm−2

i1 bim−2

i1 biξi

T1m−2

i1 bi b1B0

T

0

T−q

s 0

aτ∇τ

m−2

i1 ai

ξi

0aτ∇τ

1−m−2

i1 ai

∇s b1B0B0−1b1u.

3.15

In the same way, we can prove that ifu∂Ωb2, thenAu ≥ u.

Now, we consider the operatorAonΩb1a1andΩa2b2, respectively. ByLemma 2.10, we assert that the operatorAhas two fixed pointsu1, u2K such thata1 ≤ u1b1 and b2≤ u2a2. Therefore,ui, i1,2, are positive solutions of problem1.1-1.2.

Proof ofTheorem 3.2. Let

1

2min

l→0lim p3l

lp−1B0

γ p−1

, lim

l→∞

p4l lp−1

B0

γ p−1

, 3.16

(15)

then there exist 0< b3c3andc4b4<∞such that

p3l≥ B0

γ p−1

lp−1, 0≤lb3,

p4l≥ B0

γ p−1

lp−1, b4l≤∞.

3.17

If 0≤lb3, u∂Ωl, thenγlutl, 0≤tT. ByLemma 2.9and conditionB3, we have Aumax

0≤t≤T|Aut|

Tm−2

i1 bim−2

i1 biξi

T1m−2

i1 bi T

0

T−sϕs∇s

Tm−2

i1 bim−2

i1 biξi

T1m−2

i1 bi

× T

0

T−q

s 0

aτp3uτ−k3τuλ3 ∇τ

m−2

i1 ai

ξi

0aτp3uτ−k3τuλ3 ∇τ 1−m−2

i1 ai

∇s

Tm−2

i1 bim−2

i1 biξi

T1m−2

i1 bi

× T

0

T−q

s 0

B0

γ p−1

γlp−1k3τlλ3 ∇τ

m−2

i1 ai

ξi

0aτB0p−1γlp−1k3τlλ3 ∇τ 1−m−2

i1 ai

∇s.

3.18

It follows that βl

lTm−2

i1 bim−2

i1 biξi

T1−m−2

i1 bi

× T

0

T−q

s 0

aτB0p−1γp−1k3τlλ3−p1 ∇τ

m−2

i1 ai

ξi

0Bp−10 γp−1k3τlλ3−p1 ∇τ 1−m−2

i1 ai

∇s.

3.19

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Noticingλ3p1>0, we get

l→0lim βl

lTm−2

i1 bim−2

i1 biξi

T1−m−2

i1 bi

× T

0

T−q

s

0

aτBp−10 γp−1∇τ m−2

i1 ai

ξi

0Bp−10 γp−1∇τ 1−m−2

i1 ai

∇s

B0p−1γp−11/p−1B−10 1γp−1B−p−10 1/p−1>1.

3.20 Therefore, there existsb3with 0 < b3 < asuch thatβb3> b3. It implies thatAu> ufor u∂Ωb3.

Ifb4γl < ∞andu∂Ωl, thenb4γlutl, 0 ≤ tT. Similar to the above argument, noticing thatλ4p1<0, we can get liml→∞βl/l>1.

Therefore, there existb4with 0< b4<∞such thatβb4> b4. It implies thatAu>u foru∂Ωb4.

By conditionB4, we can see that there existb3< a3< a < a4< b4such that

max{ft, l:t, l∈0, T ×0, ai } ≤aiA0p−1, i3,4. 3.21 Ifu∂Ωa3, then 0≤uta3, 0≤tT, andft, ut≤a3A0p−1. It follows that

Au ≤ 1 1−m−2

i1 bi

T

0

T−sϕs∇s

≤ 1

1−m−2

i1 bi

a3A0

T

0

T−q

s

0

aτ∇τ

m−2

i1 ai

ξi

0∇τ

1−m−2

i1 ai

∇s a3u.

3.22

Similarly, ifu∂Ωa4, thenAu ≤ u.

Now, we study the operatorAonΩa3b3andΩb4a4, respectively. ByLemma 2.10, we assert that the operatorAhas two fixed pointsu3, u4K such thatb3 ≤ u3a3 and a4≤ u4b4. Therefore,ui, i3,4, are positive solutions of problem1.1-1.2.

4. Further discussion

If the conditions of Theorems3.1 and3.2 are weakened, we will get the existence of single positive solution of problem1.1-1.2.

Corollary 4.1. AssumeH1,H2, andH3hold, and assume that the following conditions hold:

C1p1C0,∞,0,∞, and liml→0p1l/lp−1< Ap−10 ; C2k1L10, T ,0,∞;

参照

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