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doi:10.1155/2009/123565

Research Article

Existence of Solutions for Nonlinear

Four-Point

p

-Laplacian Boundary Value

Problems on Time Scales

S. Gulsan Topal, O. Batit Ozen, and Erbil Cetin

Department of Mathematics, Ege University, Bornova, 35100 Izmir, Turkey

Correspondence should be addressed to S. Gulsan Topal,f.serap.topal@ege.edu.tr

Received 16 March 2009; Accepted 20 July 2009

Recommended by Alberto Cabada

We are concerned with proving the existence of positive solutions of a nonlinear second-order four-point boundary value problem with ap-Laplacian operator on time scales. The proofs are based on the fixed point theorems concerning cones in a Banach space. Existence result forp-Laplacian boundary value problem is also given by the monotone method.

Copyrightq2009 S. Gulsan Topal 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.

1. Introduction

LetTbe any time scale such that0,1be subset ofT. The concept of dynamic equations on time scales can build bridges between differential and difference equations. This concept not only gives us unified approach to study the boundary value problems on discrete intervals with uniform step size and real intervals but also gives an extended approach to study on discrete case with non uniform step size or combination of real and discrete intervals. Some basic definitions and theorems on time scales can be found in1,2.

In this paper, we study the existence of positive solutions for the following nonlinear four-point boundary value problem with ap-Laplacian operator:

φp

xΔ∇t htft, xt 0, t∈0,1, 1.1

αφp

0 −Ψφp

xΔξ 0, γφpxσ1 δφpxΔ

η 0, 1.2

whereφpsis an operator, that is,φps |s|p−2sforp >1,φp−1s φqs,where 1/p

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H1the functionf∈ C0,1×0,,0,∞,

H2the function h ∈ CldT,0,∞ and does not vanish identically on any closed subinterval ofρ0, σ1and 0<ρσ01htt <∞,

H3 Ψ : R → R is continuous and satisfies that there exist B2 ≥ B1 > 0 such that

B1s≤ΨsB2s,fors∈0,∞.

In recent years, the existence of positive solutions for nonlinear boundary value problems withp-Laplacians has received wide attention, since it has led to several important mathematical and physical applications3,4. In particular, forp 2 orφps sis linear,

the existence of positive solutions for nonlinear singular boundary value problems has been obtained5,6.p-Laplacian problems with two-, three-, andm-point boundary conditions for ordinary differential equations and difference equations have been studied in7–9and the references therein. Recently, there is much attention paid to question of positive solutions of boundary value problems for second-order dynamic equations on time scales, see10–13. In particular, we would like to mention some results of Agarwal and O’Regan14, Chyan and Henderson5, Song and Weng15, Sun and Li16, and Liu17, which motivate us to consider thep-Laplacian boundary value problem on time scales.

The aim of this paper is to establish some simple criterions for the existence of positive solutions of thep-Laplacian BVP1.1-1.2. This paper is organized as follows. InSection 2 we first present the solution and some properties of the solution of the linearp-Laplacian BVP corresponding to1.1-1.2. Consequently we define the Banach space, cone and the integral operator to prove the existence of the solution of1.1-1.2. InSection 3, we state the fixed point theorems in order to prove the main results and we get the existence of at least one and two positive solutions for nonlinearp-Laplacian BVP1.1-1.2. Finally, using the monotone method, we prove the existence of solutions forp-Laplacian BVP inSection 4.

2. Preliminaries and Lemmas

In this section, we will give several fixed point theorems to prove existence of positive solutions of nonlinearp-Laplacian BVP1.1-1.2. Also, to state the main results in this paper, we employ the following lemmas. These lemmas are based on the linear dynamic equation:

φp

xΔ∇t yt 0. 2.1

Lemma 2.1. Suppose condition (H2) holds, then there exists a constantθρ01−ρ0/2

that satisfies

0<

σ1θ

θ

htt <. 2.2

Furthermore, the function

At

t

θ

φq

t

s

huu Δs

σ1−θ

t

φq

s

t

huu

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is a positive continuous function, therefore,Athas a minimum onθ, σ1−θ, hence one supposes that there existsL >0such thatAtLfortθ, σ1−θ.

Proof. It is easily seen thatAtis continuous onθ, σ1−θ. Let

A1t t

θ

φq

t

s

huu Δs, A2t σ1θ

t

φq

s

t

huu

Δs. 2.4

Then, from conditionH2, we have that the functionA1tis strictly monoton nondecreasing

on θ, σ1 −θ and A1θ 0, the function A2t is strictly monoton nonincreasing on θ, σ1−θandA2σ1−θ 0, which impliesL mintθ,σ1−θAt>0.

Throughout this paper, letE C0,1, thenEis a Banach space with the normx

supt0,1|xt|. Let

K {xE:xt≥0, xtconcave function on0,1}. 2.5

Lemma 2.2. LetxtKandθbe as inLemma 2.1, then

xtθ

σ1−ρ0x,tθ, σ1−θ. 2.6

Proof. Supposeτ inf{ςρ0, σ1 : suptρ01xt }.We have three different cases.

iτρ0, θ. It follows from the concavity of xt that each point on the chard betweenτ, xτandσ1, xσ1is below the graph ofxt, thus

xt 1−

σ1−τ tτ, tθ, σ1−θ, 2.7

then

xt≥ min

tθ,σ1−θ

1− σ1−τ tτ

1−

σ1−τ σ1−θτ σ1−θτ

σ1−τ 1

θ

σ1−τxτ

θ

σ1−ρ0xτ,

2.8

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iiτθ, σ1−θ. Iftθ, τ, similarly, we have

xt x

ρ0

τρ0 tτ

x

ρ0

τρ0 θτ

θρ0

τρ0

τθ τρ0x

ρ0

θρ0

σ1−ρ0

θ

σ1−ρ0xτ.

2.9

Iftτ, σ1−θ, similarly, we have

xt 1− σ1−τ tτ

≥ min

tθ,σ1−θ

1− σ1−τ tτ

θ σ1−τxτ

σ1−τθ

σ1−τ 1

θ

σ1−ρ0xτ,

2.10

this meansxtθ/σ1−ρ0xfortθ, σ1−θ. iiiτσ1−θ, σ1. Similarly we have

xt x

ρ0

τρ0 tτ, tθ, σ1−θ, 2.11

then

xt≥ min

tθ,σ1−θ

x

ρ0

τρ0 tτ

θρ0

τρ0

τθ τρ0x

ρ0

θ

σ1−ρ0xτ,

2.12

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know

whereτis a solution of the following equation

V1t V2t, t

(6)

Integrating2.1onτ, t,we get

Using the second boundary condition and the formula2.18fort η, we have

1 φq

Lemma 2.4. Suppose that the conditions inLemma 2.3hold. Then there exists a constantAsuch that

the solutionxtofp-Laplacian BVP2.1-1.2satisfies

max

tρ01|xt| ≤Atρmax01

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(8)

Now, we define a mappingT :KEgiven by

Lemma 2.5. Suppose that the conditions (H1)–(H3) hold.T:KKis completely continuous.

Proof. SupposePKis a bounded set. LetM > 0 be such thatxM,xP. For any

By the Arzela-Ascoli theorem, we can easily see that T is completely continuous operator.

For convenience, we set

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In order to follow the main results of this paper easily, now we state the fixed point theorems which we applied to prove Theorems3.1–3.4.

Theorem 2.6see18 Krasnoselskii fixed point theorem. LetEbe a Banach space, and let

KEbe a cone. AssumeΩ1andΩ2are open, bounded subsets ofEwith0∈Ω1, Ω1 ⊂Ω2, and let

A:K∩Ω2\Ω1

−→K 2.31

be a completely continuous operator such that either

iAuuforuKΩ1, AuuforuKΩ2; iiAuuforuKΩ1, AuuforuKΩ2

hold. ThenAhas a fixed point inK∩Ω2\Ω1.

Theorem 2.7see19 Schauder fixed point theorem. LetEbe a Banach space, and letA :

EEbe a completely continuous operator. AssumeKEis a bounded, closed, and convex set. If

AKK, thenAhas a fixed point inK.

Theorem 2.8see20 Avery-Henderson fixed point theorem. LetPbe a cone in a real Banach

spaceE. Set

Pφ, r u∈ P:φu< r. 2.32

Ifμandφare increasing, nonnegative, continuous functionals onP, letθbe a nonnegative continuous functional onPwithθ0 0such that for some positive constantsrandM,

φuθuμu, uMφu 2.33

for allu∈ Pφ, r. Suppose that there exist positive numbersp < q < rsuch thatθλuλθufor all0≤λ≤1anduPθ, q.

IfA:Pφ, r → Pis a completely continuous operator satisfying iφAu> rfor alluPφ, r,

iiθAu< qfor alluPθ, q,

iiiPμ, q/andμAu> pfor alluPμ, p,

thenAhas at least two fixed pointsu1andu2such that

p < μu1 withθu1< q, q < θu2 withφu2< r. 2.34

3. Main Results

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Theorem 3.1. Assume that (H1)–(H3) are satisfied. In addition, suppose thatfsatisfies

A1ft, xφpmk1forθk11−ρ0≤xk1, A2ft, xφpMk2for0≤xk2,

wheremR1,andM∈0, R2. Then thep-Laplacian BVP1.1-1.2has a positive solution

xtsuch thatk1≤ xk2.

Proof. Without loss of generality, we supposek1< k2. For anyxK, byLemma 2.2, we have

xtθ

σ1−ρ0x,tθ, σ1−θ. 3.1

We define two open subsetsΩ1 andΩ2ofEsuch thatΩ1 {xK :x < k1}and Ω2 {xK:x< k2}.

ForxΩ1, by3.1, we have

k1 xxtθ

σ1−ρ0x

θ

σ1−ρ0k1, tθ, σ1−θ. 3.2

Fortθ, σ1−θ, ifA1holds, we will discuss it from three perspectives.

iIfτθ, σ1−θ, thus forxΩ1, byA1andLemma 2.1, we have

2Tx 2Txτ

τ

ρ0

φq

τ

s

hrfr, xrr

Δs

σ1

τ

φq

s

τ

hrfr, xrr

Δs

mk1 τ

θ

φq

τ

s

hrr

Δsmk1 σ1θ

τ

φq

s

τ

hrr

Δs

mk1mk1LR1k1L 2k1 2x.

3.3

iiIfτσ1−θ, σ1, thus forxΩ1, byA1andLemma 2.1, we have

Tx Txτ

τ

ρ0φq

τ

s

hrfr, xrr

Δs

mk1 σ1−θ

θ

φq

σ1−θ

s

hrr Δs

mk11−θmk1L≥2k1 > k1 x.

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iiiIfτρ0, θ, thus forxΩ1, byA1andLemma 2.1, we have

Existence of at least one positive solution is also proved using Schauder fixed point theoremTheorem 2.7. Then we have the following result.

Theorem 3.2. Assume that (H1)–(H3) are satisfied. IfRsatisfies

Q

R2 ≤R,

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whereQsatisfies

φpQ≥max xR

ft, xt fort0,1, 3.8

then thep-Laplacian BVP1.1-1.2has at least one positive solution.

Proof. LetKR : {xK:xR}. Note thatKRis closed, bounded, and convex subset ofE

to which the Schauder fixed point theorem is applicable. DefineT :KREas in2.27for

tρ0, σ1. It can be shown thatT :KREis continuous. Claim thatT :KRKR. Let

xKR. By using the similar methods used in the proof ofTheorem 3.1, we have

Tx Txτ

φq

1

αΨ

τ

ξ

hrfr, xrr

τ

ρ0φq

τ

s

hrfr, xrr

Δs

φq

B2

α

σ1

ρ0hrfr, xrr

σ1

ρ0φq

σ1

ρ0hrfr, xrr Δs

Q

φq

B2

α

σ1−ρ0

φq σ1

ρ0hrr

Q 1 R2 ≤R,

3.9

which impliesTxKR. The compactness of the operatorT : KRKR follows from the

Arzela-Ascoli theorem. HenceT has a fixed point inKR.

Corollary 3.3. Iffis continuous and bounded on0,1×R, then thep-Laplacian BVP1.1-1.2

has a positive solution.

Now we will give the sufficient conditions to have at least two positive solutions for

p-Laplacian BVP1.1-1.2. Set

Pt: φq

t

θ

hrr φq

σ1−θ

t

hrr , tθ, σ1−θ. 3.10

The functionPtis positive and continuous onθ, σ1−θ. Therefore,Pthas a minimum onθ, σ1−θ. Hence we suppose there existsN >0 such thatPtN.

Also, we define the nonnegative, increasing continuous functionsΥ,Φ,andΓby

Υx 1

2 1−θ,

Φx max

tρ0σ1−θ,σ1xt,

Γx max

tρ01xt.

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We observe here that, for everyxKx ≤ Φx ≤ Γx and fromLemma 2.2,x

σ1−ρ0Υx. Also, for 0≤λ≤1,Φλx λΦx.

Theorem 3.4. Assume that (H1)–(H3) are satisfied. Suppose that there exist positive numbersa <

b < csuch that the function f satisfies the following conditions: ift, xφpmaforx∈0, a,

iift, xφpMbforx∈01−ρ0/θb,

iiift, xφp2/θncforxθ/σ1−ρ0c,σ1−ρ0/θc,

for positive constantsmR1,,M∈0, R2,andn∈0, N. Then thep-Laplacian BVP1.1 1.2has at least two positive solutionsx1, x2such that

a < max

tρ01x1t with tρ0max∪σ1−θ,σ1x1t< b,

b < max

tρ0σ1−θ,σ1x2t with

1

2x2θ x2σ1−θ< c.

3.12

Proof. Define the cone as in 2.5. From Lemmas 2.2and 2.3 and the conditionsH1and H2, we can obtainTKK. Also fromLemma 2.5, we see thatT :KKis completely continuous.

We now show that the conditions ofTheorem 2.8are satisfied.

To fulfill propertyiofTheorem 2.8, we choosex, c, thusΥx 1/2 1−θ c. Recalling thatxσ1−ρ0Υx σ1−ρ0/θc, we have

θ

σ1−ρ0xxt

σ1−ρ0

θ c. 3.13

Then assumptioniiiimpliesft, x> φp2/θncfortθ, σ1−θ. We have three

different cases.

aIfτσ1−θ, σ1, we have

ΥTx 1

2Txθ Txσ1−θ

Txθ φq

1

αΨ

τ

ξ

hrfr, xrr

θ

ρ0

φq

τ

s

hrfr, xrr

Δs

θ

ρ0

φq

τ

s

hrfr, xrr

Δs

θ

ρ0

φq

σ1−θ

θ

hrfr, xrr Δs

θ

ρ0

φq

σ1−θ

θ

hrφp

2

θnc

r Δs 2 θncφq

σ1−θ

θ

hrr θρ0

≥ 2

θncPθθ

2

NcPθ≥2c.

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(15)

Theniiyieldsft, xφpMbfortρ0, σ1.

So conditioniiofTheorem 2.8holds.

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bIfτθ, σ1−θ, we have

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4. Monotone Method

In this section, we will prove the existence of solution ofp-Laplacian BVP1.1-1.2by using upper and lower solution method. We define the set

D:

x:φp

xΔ∇ is continuous on0,1

. 4.1

Definition 4.1. A real-valued functionutDonρ0, σ1is a lower solution for1.1 1.2if

φp

uΔ∇t htft, ut>0, t∈0,1,

αφp

0 −Ψφp

uΔξ ≤0, γφpuσ1 δφpuΔ

η≤0.

4.2

Similarly, a real-valued functionvtDonρ0, σ1is an upper solution for1.1 1.2if

φp

vΔ∇t htft, vt<0, t∈0,1,

αφp

0 −Ψφp

vΔξ ≥0, γφpvσ1 δφpvΔ

η≥0.

4.3

We will prove when the lower and the upper solutions are given in the well order, that is,uv, thep-Laplacian BVP1.1-1.2admits a solution lying between both functions.

Theorem 4.2. Assume that (H1)–(H3) are satisfied anduandvare, respectively, lower and upper

solutions for thep-Laplacian BVP1.1-1.2such thatuvonρ0, σ1. Then thep-Laplacian BVP1.1-1.2has a solutionxtut, vtonρ0, σ1.

Proof. Consider thep-Laplacian BVP:

φp

xΔ∇t htFt, xt 0, t∈0,1,

αφp

0 −Ψφp

xΔξ 0, γφpxσ1 δφpxΔ

η 0,

4.4

where

Ft, xt

⎧ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎩

ft, vt, xt> vt,

ft, xt, utxtvt,

ft, ut, xt< ut,

4.5

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Clearly, the functionF is bounded fort ∈ 0,1 and satisfies conditionH1. Thus byTheorem 3.2, there exists a solutionxtof thep-Laplacian BVP4.4. We first show that

xtvtonρ0, σ1. Setzt xtvt. Ifxtvtonρ0, σ1is not true, then there exists at0 ∈ρ0, σ1such thatzt0 maxtρ01{xtvt} >0 has a positive

maximum. Consequently, we know thatzΔt0 ≤ 0 and there existst1 ∈ ρ0, t0such that

zΔt ≥ 0 ont1, t0. On the other hand by the continuity ofztatt0,we know there exists

t2∈ρ0, t0such thatzt>0 ont2, t0.Lett max{t1, t2}, then we havezΔt≥0 ont, t0.

Thus we get

zΔt≥0 ⇒φp

xΔtφp

vΔt,

zΔt0≤0 ⇒φp

xΔt0

φp

vΔt0

.

4.6

Therefore,

0≥φp

xΔt0

φp

vΔt0

φp

xΔtφp

vΔt

t0

t

φp

xΔ−φp

vΔ∇tt

t0

t

φp

xΔ∇tφp

vΔ∇t

t

>

t0

t

htft, vt htft, vtt 0,

4.7

which is a contradiction and thust0cannot be an element ofρ0, σ1.

Ift0 ρ0, from the boundary conditions, we have

αφp

0≤B2φp

xΔξφp

α1−qxρ0φ p

B1−2 qxΔξ,

αφp

0≥B1φp

vΔξφp

α1−qvρ0≥φp

B1−1 qvΔξ.

4.8

Thus we get

α1−qxρ0≤B21−qxΔξ, α1−qvρ0≥B11−qvΔξ. 4.9

From this inequalities, we have

α1−qx0≤B21−qxΔξB11−qvΔξB11−qxvΔξ,

α1−qzρ0≤B1−1 qzΔξ≤0,

4.10

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Ift0 σ1, from the boundary conditions, we have

γφpxσ1 −δφp

xΔηφp

γ1−qxσ1

φp

δ1−qxΔη φp

δ1−qxΔη,

γφpvσ1≥ −δφp

vΔηφp

γ1−qvσ1

≥ −φp

δ1−qvΔη φp

δ1−qvΔη.

4.11

Thus we get

γ1−qxσ1 δ1−qxΔη, γ1−qvσ1≥ −δ1−qvΔη. 4.12

From this inequalities, we have

γ1−qx1≤ −δ1−qxvΔη,

γ1−qzσ1≤ −δ1−qzΔη≤0,

4.13

which is a contradiction. Thus we havextvtonρ0, σ1.

Similarly, we can getutxtonρ0, σ1. Thusxtis a solution ofp-Laplacian BVP1.1-1.2which lies betweenuandv.

References

1 M. Bohner and A. Peterson, Dynamic Equations on Time Scales, An Introduction with Application, Birkh¨auser, Boston, Mass, USA, 2001.

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

3 C. Bandle and M. K. Kwong, “Semilinear elliptic problems in annular domains,”Journal of Applied Mathematics and Physics, vol. 40, no. 2, pp. 245–257, 1989.

4 H. Wang, “On the existence of positive solutions for semilinear elliptic equations in the annulus,” Journal of Differential Equations, vol. 109, no. 1, pp. 1–7, 1994.

5 C. J. Chyan and J. Henderson, “Twin solutions of boundary value problems for differential equations on measure chains,”Journal of Computational and Applied Mathematics, vol. 141, no. 1-2, pp. 123–131, 2002.

6 J. A. Gatica, V. Oliker, and P. Waltman, “Singular nonlinear boundary value problems for second-order ordinary differential equations,”Journal of Differential Equations, vol. 79, no. 1, pp. 62–78, 1989. 7 R. Avery and J. Henderson, “Existence of three positive pseudo-symmetric solutions for a one

dimensionalp-Laplacian,”Journal of Mathematical Analysis and Applications, vol. 42, pp. 593–601, 2001. 8 A. Cabada, “Extremal solutions for the differenceφ-Laplacian problem with nonlinear functional boundary conditions,”Computers & Mathematics with Applications, vol. 42, no. 3-5, pp. 593–601, 2001. 9 X. M. He, “The existence of positive solutions ofp-Laplacian equation,”Acta Mathematica Sinica, vol.

46, no. 4, pp. 805–810, 2003.

10 D. R. Anderson, “Solutions to second-order three-point problems on time scales,”Journal of Difference Equations and Applications, vol. 8, no. 8, pp. 673–688, 2002.

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12 E. Akin, “Boundary value problems for a differential equation on a measure chain,”Panamerican Mathematical Journal, vol. 10, no. 3, pp. 17–30, 2000.

13 E. R. Kaufmann, “Positive solutions of a three-point boundary-value problem on a time scale,” Electronic Journal of Differential Equations, no. 82, pp. 1–11, 2003.

14 R. P. Agarwal and D. O’Regan, “Triple solutions to boundary value problems on time scales,”Applied Mathematics Letters, vol. 13, no. 4, pp. 7–11, 2000.

15 C. Song and P. Weng, “Multiple positive solutions forp-Laplacian functional dynamic equations on time scales,”Nonlinear Analysis: Theory, Methods & Applications, vol. 68, no. 1, pp. 208–215, 2008. 16 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.

17 B. Liu, “Positive solutions of three-point boundary value problems for the one-dimensional p-Laplacian with infinitely many singularities,”Applied Mathematics Letters, vol. 17, no. 6, pp. 655–661, 2004.

18 D. J. Guo and V. Lakshmikantham,Nonlinear Problems in Abstract Cones, vol. 5 ofNotes and Reports in Mathematics in Science and Engineering, Academic Press, Boston, Mass, USA, 1988.

19 M. A. Krasnosel’skii, Positive Solutions of Operator Equations, P. Noordhoff, Groningen, The Netherlands, 1964.

References

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