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Boundary Value Problems

Volume 2011, Article ID 212980,22pages doi:10.1155/2011/212980

Research Article

Multiple Positive Solutions of a Singular

Emden-Fowler Type Problem for Second-Order

Impulsive Differential Systems

Eun Kyoung Lee and Yong-Hoon Lee

Department of Mathematics, Pusan National University, Busan 609-735, Republic of Korea

Correspondence should be addressed to Yong-Hoon Lee,[email protected]

Received 14 May 2010; Accepted 26 July 2010

Academic Editor: Feliz Manuel Minh ´os

Copyrightq2011 E. K. Lee and Y.-H. Lee. 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.

This paper studies the existence, and multiplicity of positive solutions of a singular boundary value problem for second-order differential systems with impulse effects. By using the upper and lower solutions method and fixed point index arguments, criteria of the multiplicity, existence and nonexistence of positive solutions with respect to parameters given in the system are established.

1. Introduction

In this paper, we consider systems of impulsive differential equations of the form

ut λh1tfut, vt 0, t∈0,1, t /t1,

vt μh2tgut, vt 0, t∈0,1, t /t1,

Δu|tt1Iuut1, Δv|tt1Ivvt1,

Δutt

1 Nuut1, Δv

tt1 Nvvt1,

u0 a≥0, v0 b≥0, u1 c≥0, v1 d≥0,

P

whereλ, μare positive real parameters,Δu|tt1 ut1−ut1, andΔu|tt1 ut1−ut−1.

Throughout this paper, we assumef, g∈ CR2

,Rwithf0,0 0 g0,0andfu, v >

0, gu, v > 0 for all u, v/ 0,0, Iu, IvCR,R satisfyingIu0 0 Iv0, Nu, Nv

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hi may be singular at t 0 and/or 1.Let J 0,1, J 0,1\ {0,1, t1}, P C 0,1 {u |

u : 0,1 → Rbe continuous att /t1,left continuous att t1,and its right-hand limit at

tt1exists}andXP C 0,P C 0,1.ThenP C 0,1andXare Banach spaces with norm

usupt0,1|ut|andu, vuv,respectively. The solution of problemPmeans

u, vXC2J×C2Jwhich satisfiesP.

Recently, several works have been devoted to the study of second-order impulsive differential systems. See, for example 1–6, and references therein. In Particular, E.K. Lee and Y.H. Lee 3studied problemPwhenfandgsatisfyf0,0>0 andg0,0>0.More precisely, let us consider the following assumptions.

D1

1

0s1−shisds <,fori1,2.

D2t1NuuIuu≤ −1−t1Nuuandt1NvvIvv≤ −1−t1Nvv.

D3uIuuandvIvvare nondecreasing.

D4Nu,∞limu→ ∞|Nuu|/u <1 andNv,∞limv→ ∞|Nvv|/v <1.

D5f∞limuv→ ∞fu, v/uv∞andg∞limuv→ ∞gu, v/uv.

D6f and g are nondecreasing on R2, that is,fu1, v1 ≤ fu2, v2 andgu1, v1 ≤

gu2, v2wheneveru1, v1 ≤ u2, v2,where inequality onR2 can be understood

componentwise.

Under the above assumptions, they proved that there exists a continuous curveΓ splitting

R2

\ {0,0} into two disjoint subsetsO1 and O2 such that problem3.20 has at least two

positive solutions forλ, μ∈ O1,at least one positive solution forλ, μ∈Γ,and no solution

forλ, μ∈ O2.

The aim of this paper is to study generalized Emden-Fowler-type problem for P, that is,f andg satisfyf0,0 0 andg0,0 0,respectively. In this case, we obtain two interesting results. First, for Dirichlet boundary condition, that is,abcd0,assuming

D1,D2and

D4Nu,0limu→0|Nuu|/u <1/2 andNv,0 limv→0|Nvv|/v <1/2,

D5f∞∞, g∞∞andf0limuv→0fu, v/uv0, g0limuv→0gu, v/uv0,

we prove that problemPhas at least one positive solution for allλ, μ∈R2\{0,0}.On the other hand, for two-point boundary condition, that is,c > aandd > b,assumingD1∼D6,

we prove that there exists a continuous curveΓ0splittingR2\{0,0}into two disjoint subsets

O0,1andO0,2and there exists a subsetO ⊂ O0,1such that problemPhas at least two positive

solutions forλ, μ ∈ O,at least one positive solution for λ, μ ∈ O0,1 \ O∪Γ0,and no

solution forλ, μ∈ O0,2.

Our technique of proofs is mainly employed by the upper and lower solutions method and several fixed point index theorems.

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2. Preliminary

In this section, we introduce two types of fundamental theorems of upper and lower solutions method for a singular system with no impulse effect and an impulsive system and then introduce several well-known fixed point index theorems. We first give definition s of somewhat general type of upper and lower solutions for the following singular system:

ut Ft, ut, vt 0, t∈0,1,

vt Gt, ut, vt 0, t∈0,1,

u0 A, u1 C, v0 B, v1 D,

H

whereF, G :0,1×R×R → Rare continuous.

Definition 2.1. We say thatαu, αvC0,C 0,1is aG-lower solution ofHifαu, αv

C20,1×C20,1except at finite pointsτ

1, . . . , τnwith 0< τ1< . . . < τn<1 such that

L1at each τi, there exist αu τi, αv τi,αuτi, αvτi such that αu τi− ≤

αuτi, αvτi−≤αvτi,and

L2

αut Ft, αut, αvt≥0,

αvt Gt, αut, αvt≥0, t{ 0,1

τ1, . . . , τn}

,

αu0≤A, αu1≤C,

αv0≤B, αv1≤D.

2.1

We also say that βu, βvC 0,1 ×C 0,1 is a G-upper solution of the problem H if

βu, βvC20,C20,1 except at finite pointsσ1, . . . , σm with 0 < σ1 < · · · < σm < 1

such that

U1at each σi, there exist βuσj, βvσj,βuσj, βvσj such that βuσj− ≥

βu σj, βvσj−≥βvσj,and

U2

βut Ft, βut, βvt

≤0,

βvt Gt, βut, βvt

≤0, t∈ 0,1

{σ1, . . . , σn}

,

βu0≥A, βu1≥C,

βv0≥B, βv1≥D.

2.2

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Lemma 2.2. LetF, G :D → Rbe continuous functions andD⊂0,1×R×R.Assume that there existhF, hGC0,1,Rsuch that

|Ft, u, v| ≤hFt, |Gt, u, v| ≤hGt, 2.3

for allt, u, v∈0,1×R×R,and

1

0

s1−shFsds

1

0

s1−shGsds <. 2.4

Then problemHhas a solution.

Let Dβα {t, u, v | αut, αvtu, vβut, βvt, t ∈ 0,1}. Then the

fundamental theorem of G-upper and G-lower solutions for singular problemHis given as follows.

Theorem 2.3. Letαu, αvand βu, βvbe a G-lower solution and a G-upper solution of problem

H, respectively, such that

a1 αut, αvtβut, βvtfor allt∈ 0,1.

Assume also that there existhF, hGC0,1,Rsuch that

a2|Ft, u, v| ≤hFtand|Gt, u, v| ≤hGtfor allt, u, vDαβ;

a3

1

0s1−shFsds

1

0s1−shGsds <∞;

a4Ft, u, v1 ≤Ft, u, v2,wheneverv1 ≤ v2andGt, u1, vGt, u2, v,wheneveru1 ≤

u2.

Then problemHhas at least one solutionu, vsuch that

αut, αvtut, vt

βut, βvt

,t∈ 0,1. 2.5

Proof. Define a modified function ofFas follows:

Ft, u, v

⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩

Ft, βut, v

uβut

1 u

2 ifu > β

ut,

Ft, u, v ifαutuβut,

Ft, αut, v

uαut

1 u

2 ifu < α

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Ft, u, v ⎧ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎩

Ft, u, βvt

ifv > βvt,

Ft, u, v ifαvtvβvt,

Ft, u, αvt ifv < αvt,

Gt, u, v

⎧ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎩

Gt, βut, v

if u > βut,

Gt, u, v if αutuβut,

Gt, αut, v if u < αut,

2.6

Gt, u, v

⎧ ⎪ ⎪ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎪ ⎪ ⎩

Gt, u, βvt,

vβvt

1 v

2 ifv > β

vt,

Gt, u, v ifαvtvβvt,

Gt, u, αvt

vαvt

1 v

2 ifv < α

vt.

2.7

ThenF, G∗:0,1×R×R → Rare continuous and

|Ft, u, v| ≤mαu, βu

hFt,

|Gt, u, v| ≤mαv, βv

hGt,

2.8

for allt, u, v∈0,1×R×R,wheremα, β αβ1.For the problem

ut Ft, ut, vt 0,

vt Gt, ut, vt 0, t∈0,1

u0 A, u1 C, v0 B, v1 D,

M

Lemma 2.2guarantees the existence of solutions of problemM and thus it is enough to prove that any solutionu, vof problemMsatisfies

αut, αvtut, vt

βut, βvt

,t∈ 0,1. 2.9

Suppose, on the contrary,αu, αv/u, v, so we consider the caseαu /u.Letαuut0

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cases. First, ifαvt0≤vt0,then byαut0> ut0and conditiona4,

0≥αuut0 αut0 Ft0, ut0, vt0

αut0 Ft0, αut0, vt0−

ut0−αut0

1u2t 0

αut0 Ft0, αut0, αvt0− ut0−αut0

1u2t 0

αut0−ut0

1u2t0 >0,

2.10

which is a contradiction. Next, ifαvt0> vt0,then by the definition ofF,

0≥αuut0 αut0 Ft0, ut0, vt0

αut0 Ft0, αut0, αvt0−

ut0−αut0

1u2t 0

>0,

2.11

which is also a contradiction. Ift0τifor somei1, . . . , n,then sinceαuuattains its positive

maximum atτi,

αuu

τi

≥0, αuuτi≤0. 2.12

Ifαuuτi>0,then

0<αuu

τi

αuuτi αu

τi

αuτi. 2.13

This leads a contradiction to the definition ofG-lower solution. Ifαuuτi− 0,then there

existsδ >0 such that for alltτiδ, τi,

αuut>0, αuut≥0, αuut≤0. 2.14

Fortτiδ, τi,ifαvtvt,then byαut> utand conditiona4,

0≥αuut αut Ft, ut, vt

αut Ft, αut, vtutαut

1u2t

αut Ft, αut, αvt

utαut

1u2t

αutut

1u2t >0,

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which is a contradiction. Ifαvt> vt,then by definition ofF,

0≥αuut αut Ft, ut, vt

αut Ft, αut, αvtutαut

1u2t >0,

2.16

which is a contradiction. Ift00 or 1,then

0<αuu0 αu0−A≤0,

0<αuu1 αu1−C≤0,

2.17

which is a contradiction. Similarly, we get contradictions for the caseαv/v.The proof for

u, vβu, βvcan be done by similar fashion.

Now we introduce definition and fundamental theorem of upper and lower solutions for impulsive differential systems of the form

ut Ft, ut, vt 0, t /t1, t∈0,1,

ut Gt, ut, vt 0, t /t1, t∈0,1,

Δu|tt1Iuut1, Δv|tt1Ivvt1, Δutt

1Nuut1, Δv

tt1Nvvt1,

u0 a, v0 b, u1 c, v1 d,

S

whereF, GC0,1×R×R,R,Iu, IvCR,RsatisfyingIu0 0Iv0andNu, Nv

CR,−∞,0.

Definition 2.4. αu, αvXC2J×C2Jis called a lower solution of problemSif

αut Ft, αut, αvt≥0, t /t1,

αvt Gt, αut, αvt≥0, t /t1,

Δαu|tt1Iuαut1, Δαv|tt1 Ivαvt1, Δαutt

1≥Nuαut1, Δα

vtt1 ≥Nvαvt1,

αu0≤a, αv0≤b, αu1≤c, αv1≤d.

2.18

We also define an upper solutionβu, βvXC2J×C2Jifβu, βvsatisfies the reverses

of the above inequalities.

The following existence theorem for upper and lower solutions method is proved in

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Theorem 2.5. Letαu, αvandβu, βvbe lower and upper solutions of problemS, respectively,

satisfyinga1. Moreover, we assumea2∼a4andD3. Then problemShas at least one solution

u, vsuch that

αut, αvtut, vt

βut, βvt

,t∈ 0,1. 2.19

The following theorems are well known cone theoretic fixed point theorems. See Lakshmikantham 8for proofs and details.

Theorem 2.6. LetXbe a Banach space andKa cone inX. Assume thatΩ1andΩ2are bounded open subsets inXwith0 ∈Ω1 andΩ1 ⊂ Ω2. LetT :K ∩Ω2\Ω1 → Kbe a completely continuous such that either

iTuuforu∈ K ∩Ω1andTuuforu∈ K ∩Ω2or

iiTuuforu∈ K ∩Ω1andTuuforu∈ K ∩Ω2.

ThenT has a fixed point inK ∩Ω2\Ω1.

Theorem 2.7. LetX be a Banach space,Ka cone inXand Ωbounded open inX.Let0 ∈ Ωand

T :K ∩Ω → Kbe condensing. Suppose thatTx /νx, for allx∈ K ∩Ωand allν≥1.Then

iT,K ∩Ω,K 1. 2.20

3. Existence

In this section, we prove an existence theorem of positive solutions for problemPwith Dirichlet boundary condition and the existence and nonexistence part of the result for problemPwith two-point boundary condition. Let us consider the following second-order impulsive differential systems.

ut λh1tfut, vt 0, t∈0,1, t /t1,

vt μh2tgut, vt 0, t∈0,1, t /t1,

Δu|tt1Iuut1, Δv|tt1 Ivvt1

Δutt

1Nuut1, Δv

tt1Nvvt1,

u0 a≥0, v0 b≥0, u1 c≥0, v1 d≥0,

P

where λ, μare positive real parameters, f, gCR2

, 0,∞ with f0,0 0, g0,0 0,

and fu, v > 0, gu, v > 0 for all u, v/ 0,0, Iu, IvCR,R satisfying Iu0 0

Iv0, Nu, NvCR,−∞,0,andh1, h2 ∈C0,1,0,∞may be singular att0 and/or

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We first set up an equivalent operator equatio for problemP. Let us define:X

P C 0,1and:XP C 0,1by taking

Aλu, vta catλ

1

0

Kt, sh1sfus, vsdsWut, u,

Bμu, vtb dbtμ

1

0

Kt, sh2sgus, vsdsWvt, v,

3.1

where

Kt, s

⎧ ⎨ ⎩

tIvvt1−1−t1Nvvt1, 0≤tt1,

1−tIvvt1−t1Nvvt1, t1< t≤1.

Wut, ut

⎧ ⎨ ⎩

tIuut1−1−t1Nuut1, 0≤tt1,

1−tIuut1−t1Nuut1, t1< t≤1,

Wvt, ut

⎧ ⎨ ⎩

tIvvt1−1−t1Nvvt1, 0≤tt1,

1−tIvvt1−t1Nvvt1, t1< t≤1.

3.2

Also define

Tλ,μu, v

Aλu, v, Bμu, v

. 3.3

ThenTλ,μ : XX is well defined on X and problemPis equivalent to the fixed-point

equation

Tλ,μu, v u, v inX. 3.4

Mainly due to D1, Tλ,μ is completely continuous see 3 for the proof. Let u0

supt0,t

1|ut|,u1suptt1,1|ut|, S0 t1/4,3t1/4, S1 3t11/4, t13/4,P{u, v

X | u, v≥0},andK{u, v∈ P | mintS0ut vtt1/4u0v0,mintS1ut

vt≥1−t1/4u1v1}.Thenumax{u0,u1}andP,Kare cones inX.By using

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We now prove the existence theorem of positive solutions for Dirichlet boundary value problem

ut λh1tfut, vt 0, t∈0,1, t /t1,

vt μh2tgut, vt 0, t∈0,1t /t1,

Δu|tt1Iuut1, Δv|tt1Ivvt1,

Δutt

1Nuut1, Δv

tt1Nvvt1,

u0 0, v0 0, u1 0, v1 0.

PD

Theorem 3.1. Assume D1,D2,D4, and D5. Then problem PD has at least one positive solution for allλ, μ∈R2

\ {0,0}.

Proof. First, we consider caseλ > 0 andμ > 0.By the factNu,0 < 1/2 andNv,0 < 1/2,we

may choosec1, m1 > 0 such that max{Nu,0, Nv,0} < c1 < 1/2,|Nuu |≤c1uforum1and

|Nvv| ≤ c1vforvm1.Also chooseηλ andημ satisfying 0 < ηλ < 1−2c1/2λ

1

0s1−

sh1sdsand 0< ημ < 1−2c1/2μ

1

0s1−sh2sds.Sincef0 0 andg0 0,there exist

m2, m3>0 such thatfu, vηλuvforuvm2andgu, vημuvforuvm3.

LetΩ1 BM1 {u, vX | u, v< M1}withM1 min{m1, m2, m3}.Then foru, v

K ∩Ω1,we obtain by usingD2

Aλu, vt λ

1

0

Kt, sh1sfus, vsdsWut, u

ληλ

1

0

s1−sh1sus vsds|Nuut1|

ληλ

1

0

s1−sh1sdsc1

u, v

≤1 2u, v,

3.5

for allt∈ 0,1.Similarly, we obtain

Bμu, vt≤ 1

2u, v 3.6

for allt∈ 0,1.Thus

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On the other hand, let us chooseη1andη2such that

1

η2

< μmin

⎧ ⎪ ⎨ ⎪ ⎩ t1

8mintS0

S0

Kt, sh2sds,

1−t1

8 mintS1

S1

Kt, sh2sds

⎫ ⎪ ⎬ ⎪ ⎭. 1 η2

< μmin

⎧ ⎪ ⎨ ⎪ ⎩ t1

8mintS0

S0

Kt, sh2sds,

1−t1

8 mintS1

S1

Kt, sh2sds

⎫ ⎪ ⎬ ⎪ ⎭. 3.8

Also byD5,we may chooseRf and Rg such thatfu, vη1uvforuvRf and

gu, vη2uvfor uvRg.LetΩ2 {u,v ∈ X | u, v < M2},where M2

max{8Rf/t1,8Rf/1−t1,8Rg/t1,8Rg/1−t1, M11}.ThenΩ1⊂Ω2.Letu, v∈ K ∩Ω2,

then we have the following four cases: uv and u u0,uv and u

u1,uvandv v0,anduvandv v1.We consider the first case,

the rest of them can be considered in a similar way. So letuvanduu0; then for

tS0,we have

ut vtutt1

82u0≥

t1

8uv

t1

8u, vRf. 3.9

Thusfut, vtη1ut vtfortS0.SinceWut, u≥0,we get fortS0,

Aλu, vt λ

1

0

Kt, sh1sfus, vsdsWut, u

λ

S0

Kt, sh1sfus, vsds

λη1

S0

Kt, sh1sus vsds

λη1

t1

8

S0

Kt, sh1sds2u02v0

λη1t1

8mintS0

S0

Kt, sh1sdsu, v>u, v.

3.10

Therefore,

Tλ,μu, vAλu, v>u, v, 3.11

and byTheorem 2.6,Tλ,μhas a fixed point inK ∩Ω2\Ω1.

Second, consider caseλ > 0 andμ 0.Takingc1, ηλ, m1,andm2 as above and using

the same computation, we may show

Aλu, v

1

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for allu, v∈ K ∩Ω1,whereΩ1BM1withM1min{m1, m2}.Sinceμ0,

Bμu, vt Wvt, v≤ |Nvvt1| ≤c1u, v ≤ 1

2u, v, 3.13

for allt∈ 0,1.Thus

Tλ,μu, vAλu, vBμu, vu, v, 3.14

for u, v ∈ K ∩Ω1.Now, let us choose η1 andRf as above and letΩ2 {u, vX |

u, v < M2},whereM2 max{8Rf/t1,8Rf/1−t1, M11}.ThenΩ1 ⊂ Ω2 and we can

show by the same computation as above,

Tλ,μu, vAλu, v>u, v, 3.15

foru, v∈ K ∩Ω2and thusTλ,μhas a fixed point inK ∩Ω2\Ω1.

Finally, consider caseλ 0 andμ > 0.Takingc1,ημ, m1,andm3 as the first case, we

may show by similar argument,

Bμu, v

1

2u, v, Aλu, v ≤ 1

2u, v, 3.16

for allu, v∈ K ∩Ω1,whereΩ1BM1withM1min{m1, m3} .Thus

Tλ,μu, vu, v, 3.17

foru, v∈ K ∩Ω1.Now, let us chooseη2andRgas the first case and letΩ2 {u, vX |

u, v < M2},whereM2 max{8Rg/t1,8Rg/1−t1, M11}.ThenΩ1 ⊂ Ω2 and we also

show similarly, as before,

Tλ,μu, vBμu, v>u, v, 3.18

foru, v∈ K ∩Ω2.Therefore,Tλ,μhas a fixed point inK ∩Ω2\Ω1and this completes the

proof.

Now let us consider two point boundary value problems given as follows:

ut λh1tfut, vt 0, t∈0,1, t/t1,

vt μh2tgut, vt 0, t∈0,1, t /t1,

Δu|tt1Iuut1, Δv|tt1Ivvt1,

Δutt

1Nuut1, Δv Δv

tt1 Nvvt1,

u0 a≥0, v0 b≥0, u1 c > a, v1 d > b.

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Lemma 3.2. AssumeD5.LetRbe a compact subset ofR2\ {0,0}.Then there exists a constant

bR >0such that for allλ, μ ∈ Rfor possible positive solutionsu, vof problem3.20atλ, μ,

one hasu, v< bR.

Proof. Suppose on the contrary that there is a sequenceun, vnof positive solutions of3.20

at λn, μnsuch that λn, μn ∈ R for allnand un, vn → ∞.Since0,0/∈ R, there is a

subsequence, say again{λn, μn},such thatαmin{λn}>0 orβ min{μn} >0. First, we

assumeα >0. Fromun, vn → ∞, we knowun0vn0 → ∞orun1vn1 → ∞.

Supposeun0vn0 → ∞. Then by the concavity ofunandvn, we have

unt vnt

t1

4un0vn0, 3.19

fortS0.Let us chooseη1>2π2/t21αh1,whereh1 mintS0h1t. Then byD5, there exists

Rf >0 such that

fu, vη1uvuvRf. 3.20

Sinceun0vn0 > 4/t1Rf for sufficiently largen,3.19impliesunt vnt > Rf for

tS0. Thus fortS0,

funt, vnt> η1unt vntη1unt. 3.21

Hence we have fortS0,

0unt λnh1tfunt, vnt> unt αh1η1unt. 3.22

If we multiply byφt sin2π/t1tt1/4both sides in the above inequality and integrate

onS0, then by the factsφt1/4>0, φ3t1/4<0 and integration by part, we obtain

0>

3t1/4

t1/4

untφtdtαh1η1

3t1/4

t1/4

untφtdt

≥ −

2π t1

23t1/4

t1/4

untφtdtαh1η1

3t1/4

t1/4

untφtdt.

3.23

Thus2π/t12/αh1≥η1which is a contradiction to the choice ofη1.Supposeun1vn1 →

∞, then we also get a contradiction by a similar calculation withη2 > 2π2/1−t12 αh1,

whereh1 mintS1h1t.Finally, the caseβ >0 can also be proved by similar way using the

conditiong.

Lemma 3.3. AssumeD1,D3,and

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If problem 3.20has a positive solution atλ, μ.Then the problem also has a positive solution at

λ, μfor allλ, μλ, μ.

Proof. Letu, vbe a positive solution of problem3.20atλ, μand letλ, μ∈R2

\ {0,0}

withλ, μλ, μ.Thenu, vis an upper solution of3.20atλ, μ.Defineαu, αvby

αut

⎧ ⎪ ⎨ ⎪ ⎩

0, t∈ 0, t1,

c

1−t1

tt1, tt1,1,

αvt

⎧ ⎪ ⎨ ⎪ ⎩

0, t∈ 0, t1,

d

1−t1

tt1, tt1,1.

3.24

Thenαu, αvis a lower solution of problem3.20atλ, μ.By the concavity ofu, v,u, v

αu, αv.Therefore,Theorem 2.5implies that problem3.20has a positive solution atλ, μ.

Lemma 3.4. AssumeD1 ∼ D4and Q.Then there existsλ, μ> 0,0such that problem

3.20has a positive solution for allλ, μλ, μ.

Proof. It is not hard to see that the following problem:

ut h1t 0, t∈0,1, t /t1,

vt h2t 0, t∈0,1, t /t1,

Δu|tt1Iuut1, Δv|tt1Ivvt1,

Δutt

1Nuut1, Δv

tt1Nvvt1,

u0 a≥0, v0 b≥0, u1 c > a, v1 d > b

3.25

has a positive solution so letβu, βvbe a positive solution. LetMf supt0,1fβut, βvt

andMg supt∈0,1gβut, βvt.ThenMf, Mg > 0 and forλ, μ∗ 1/Mf,1/Mg,we

get

βuλh1tf

βut, βvt

h1t

λfβut, βvt

−1≤0,

βvμh2tg

βut, βvt

h2t

μgβut, βvt

−1≤0.

3.26

This shows that βu, βv is an upper solution of 3.20 at λ, μ. On the other hand,

αu, αv given inLemma 3.3is obviously a lower solution andαu, αvβu, βv.Thus by

Theorem 2.5,3.20has a positive solution atλ, μ∗and the proof is done byLemma 3.3.

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Lemma 3.5see9. Consider,D1,D5andQ. For problem

ut λh1tfut, vt 0,

vt μh2tgut, vt 0, t∈0,1,

u0 a≥0, u1 c > a,

v0 b≥0, v1 d > b,

UT

letAT {λ, μ∈R2\ {0,0} |3.27has a positive solution atλ, μ}.ThenAT,is bounded

above.

DefineA {λ, μ∈R2

\ {0,0} |3.20has a positive solution atλ, μ}.ThenA/by

Lemma 3.4andA,is a partially ordered set.

Lemma 3.6. AssumeD1∼D6.ThenA,is bounded above.

Proof. Suppose on the contrary that there exists a sequenceλn, μn∈ Asuch that|λn, μn| →

.Letun, vnbe a positive solution of problem3.20atλn, μn.By conditionD2,we may

choose sequencessn,tnin 0, t1∪t1,1such that ifIuunt1>0,thentnt1,1and

Iuunt1 tnt1Nuunt1 0,

Iuunt1 tt1Nuunt1>0, on t1, tn,

Iuunt1 tt1Nuunt1<0, ontn,1;

3.27

ifIuunt1<0,thentn∈ 0, t1and

Iuunt1 tnt1Nuunt1 0,

Iuunt1 tt1Nuunt1>0, on 0, tn,

Iuunt1 tt1Nuunt1<0, ontn, t1;

3.28

ifIvvnt1>0,thensn∈t1,1and

Ivvnt1 snt1Nvvnt1 0,

Ivvnt1 tt1Nvvnt1>0, on t1, sn,

Ivvnt1 tt1Nvvnt1<0, onsn,1;

3.29

ifIvvnt1<0,thensn∈ 0, t1and

Ivvnt1 snt1Nvvnt1 0,

Ivvnt1 tt1Nvvnt1>0, on 0, sn,

Ivvnt1 tt1Nvvnt1<0, onsn, t1.

(16)

IfIuunt1>0,define

unt

⎧ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎩

unt, on 0, t1,

untIuunt1 tt1Nuunt1, ont1, tn,

unt, on tn,1,

3.31

and ifIuunt1<0, define

unt

⎧ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎩

unt, on 0, tn,

unt Iuunt1 tt1Nuunt1, ontn, t1,

unt, ont1,1.

3.32

Moreover, ifIvvnt1>0, define

vnt

⎧ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎩

vnt, on 0, t1,

vntIvvnt1 tt1Nvvnt1, ont1, sn,

vnt, on sn,1,

3.33

and ifIvvnt1<0, define

vnt

⎧ ⎪ ⎪ ⎪ ⎨ ⎪ ⎪ ⎪ ⎩

vnt, on 0, sn,

vnt Ivvnt1 tt1Nvvnt1, onsn, t1,

vnt, ont1,1.

3.34

Then we can easily see that un,vnC 0,1 × C 0,1 ∩ C20,1 × C20,1 except

t1, tn, sn.Furthermore,unt−1,vnt−1 unt1,vnt1,untn,vntnuntn,vntnand

unsn,vnsnunsn,vnsn.We also seeunt, vntunt,vnton 0,1.Thus by

D6,we get

unt λnh1tfunt,vnt unt λnh1tfunt,vnt

λnh1t

funt,vntfunt, vnt

≤0,

vnt μnh2tgunt,vnt vnt μnh2tgunt,vnt

μnh2t

gunt,vntgunt, vnt

≤0.

3.35

We also getun0 un0 a,un1 un1 c,vn0 vn0 b,andvn1 vn1 d.

Thusun,vnis aG-upper solution of problemUTatλn, μn.IfIuunt1 0 orIvvnt1

0, then we consider un un or vn vn as a G-upper solution. Let αut,αvt c

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byTheorem 2.3, problem 3.27 has a positive solution for all λn, μn. This contradicts to

Lemma 3.5and the proof is done.

Lemma 3.7. AssumeD1∼D6.Then every nonempty chain inAhas a unique supremum inA.

Proof. LetCbe a chain inA. Without loss of generality, we may choose a distinct sequence {λn, μn} ⊂ C such that λn, μnλn1, μn1. By Lemma 3.6, there exists λC, μC such

thatλn, μnλC, μC.If we showλC, μC ∈ A, then the proof is done. Since{λn, μn}

is bounded, Lemma 3.2implies that there is a constantB such that un, vn < B, where

un, vnis a solution corresponding toλn, μn. By the compactness ofTλ,μ,{un, vn}has a

convergent subsequence converging to say,uC, vC. By Lebesgue Convergence theorem, we

see thatuC, vCis a solution of3.20atλC, μC. ThusλC, μC∈ A.

Theorem 3.8. AssumeD1∼D6.Then there exists a continuous curveΓsplittingR2\ {0,0}

into two disjoint subsetsO1 and O2 such that problem PT has at least one positive solution for

λ, μ∈ O1∪Γand no solution forλ, μ∈ O2.

Proof. λ, μ∗ is given inLemma 3.4. We know from Lemma 3.4that 3.20 has a positive solution at0, sfor all 0 < sμ∗. Thus{0, s|s > 0} ∩ Ais a nonempty chain inAand byLemma 3.7, it has unique supremum of the form0, s∗inA. This implies that3.20has a positive solution at0, sfor all 0 < ss∗and no solution at0, sfor alls > s∗. Similarly, there isr∗ ≥ λ∗ such that 3.20has a positive solution atr,0 for all 0 < rr∗ and no solution atr,0for allr > r.DefineL :R → R2by takingLt {r, s|srt}.Then

fort ∈ −r, s∗,Lt∩ Ais a nonempty chain inA.DefineΓtas the unique supremum ofLt∩ A. ThenΓis well defined on −r, s∗and as a consequence ofLemma 3.3, we see thatΓ is continuous on −r, s∗,Γ−rr,0,and Γs∗ 0, s. Therefore, the curve

Γ Γ −r, s∗separatesR2\{0,0}into two disjoint subsetsO1andO2, whereO1is bounded

andO2is unbounded and we get the conclusion of this theorem forΓ,O1,andO2.

4. Multiplicity

In this section, we study existence of the second positive solution for two point boundary value problem3.20with λ, μin certain region of O1 appeared inTheorem 3.8. For the

computation of fixed point index, we need to consider problems of the form

ut λh1tfut, vt 0, t∈0,1, t /t1,

vt μh2tgut, vt 0, t∈0,1, t /t1,

Δu|tt1Iuut1, Δv|tt1Ivvt1,

Δutt

1 Nuut1, Δv

tt1 Nvvt1,

u0 aε, u1 cε,

v0 bε, v1 dε,

PTε

whereε >0, c > a≥0 andd > b≥0.Theorem 3.8implies that there exists a continuous curve

ΓεsplittingR2\ {0,0}into two disjoint subsetsOε,1andOε,2such that the problem4.1has

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and lower solutions argument, we can easily show that if 0< ε < ε,thenOε,1∪Γε⊂ Oε,1∪Γε.

LetO ∪ε>0Oε,1∪Γε,thenO ⊂ O0,1.We state the main theorem for two point boundary

value problem3.20as follows.

Theorem 4.1. AssumeD1∼D6.Then there exists a continuous curveΓ0splittingR2\ {0,0} into two disjoint subsetsO0,1and,O0,2and there exists a subsetO ⊂ O0,1such that problem3.20has at least two positive solutions forλ, μ∈ O,at least one positive solution forλ, μ∈O0,1\ O∪Γ0, and no solution forλ, μ∈ O0,2.

Proof. LetO∪ε>0Oε,1∪Γεand letλ, μ∈ O.It is enough to prove that problem3.20has

the second solution atλ, μ.By the definition ofO,there existsε >0 such thatλ, μ∈ Oε,1∪Γε.

That is4.1has a positive solution atλ, μ.So letuε, vεbe a positive solution of problem

4.1atλ, μand letΩ {u, vX| −ε < ut< uεt,ε < vt< vεtfort∈ 0,1, ut1<

uεt1, vt1 < vεt1}.ThenΩis bounded open inX,0 ∈Ω.Furthermore,Tλ,μ : K ∩Ω →

Kis condensing, since it is completely continuous. We show that Tλ,μu, v/νu, vfor all

u, v∈ K ∩Ωand allν≥1.If it is not true, then there existu, v∈ K ∩Ωandν0≥1 such

thatTλ,μu, v ν0u, v.Thusu, vis a positive solution of the following equation

ν0ut λh1tfut, vt 0, t∈0,1, t /t1,

ν0vt μh2tgut, vt 0, t∈0,1, t /t1,

νu|tt1Iuut1, νv|tt1 Ivvt1,

νutt1Nuut1, νvtt1Nvvt1,

ν0u0 a, ν0v0 b, ν0u1 c, ν0v1 d,

4.1

and we can consider the following two cases. The first case isut0 uεt0orvt0 vεt0

for somet0 ∈0,1. The second case isut1 t1orvt1 vεt1.First, let us consider

caseut0 uεt0for some t0 ∈ 0,1. One may prove similarly for casevt0 vεt0.

If t0 ∈ J,that is, t0/t1,let mt uuεt,then mt ≥ 0 onJ, m0 < 0, m1 < 0,

and mt1 ≤ 0.Thus on one of intervals 0, t1 ort1,1containing t0,maximum principle

impliesm ≡ 0 and this contradicts to the facts of m0 < 0 and m1 < 0.Ift0 t1,then

ut1 uεt1, ututand vtvεton 0,1.Thus by D6and D2, we get the

following contradiction:

ut1

1

ν0

Aλu, vt1

a bat1

ν0

λ ν0

1

0

Kt1, sh1sfus, vsds

t1Iuut1 1−t1Nuut1

ν0

< aε bat1λ

1

0

Kt1, sh1sfuεs, vεsds

t1Iuuεt1 1−t1Nuuεt1

uεt1 ut1.

(19)

Second, let us considerut1 uεt1. Sinceututandvtvεt, we get

ut1 1 ν0

Aλu, v

t1 a bat1 ν0

λ ν0

1

0

Kt1, sh1sfus, vsds

1−t1Iuut1−t1Nuut1

ν0

< aε bat1λ

1

0

Kt1, sh1sfuεs, vεsds

1−t1Iuuεt1−t1Nuuεt1

t1ut1.

4.3

One may show the contradiction similarly for casevt1 vεt1.This contradiction shows

Tλ,μu, v/νu, vfor allu, v∈ K ∩Ωandν≥1.Therefore, byTheorem 2.7, we obtain

iTλ,μ,K ∩Ω,K

1. 4.4

On the other hand, by Lemma 3.6, we know that there is λ1, μ1 such that 3.20has no

positive solution atλ1, μ1.Thus for any open setUinX, we get

iTλ11,K ∩ U,K

0. 4.5

LetRbe a compact rectangle containingλ, μandλ1, μ1.ByLemma 3.2, for allλ, μ∈ R,

there existsbR>0 such that all possible solutionsu, vofPTatλ, μsatisfyu, v< bR

andΩ⊂BbR.Defineh: 0,BbR∩ K → Kby

hτ,u, v Tτλ11−τλ,τμ11−τμu, v. 4.6

Thenh0,u, v Tλ,μu, v, h1,u, v 11u, v, his completely continuous on 0,

K,andhτ,u, v/ u, vfor allτ,u, v∈ 0,∂BbR∩ K.By the property of homotopy invariance and4.5, we have

iTλ,μ, BbR∩ K,K

iTλ11, BbR∩ K,K

0. 4.7

By the additive property and4.4,4.7, we have

i

Tλ,μ,

B

bR

Ω

∩ K,K

−1. 4.8

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5. Applications

In this section, we apply the results in previous sections to study the existence and multiplicity theorems of positive radial solutions for impulsive semilinear elliptic problems.

5.1. On an Annular Domain

Let us consider

Δuλk1|x|fu, v 0,

Δvμk2|x|gu, v 0, inΩl1, l2,|x|/r1,

Δu||x|r1Iu

u||x|r1, Δv||x|r1Iv

u||x|r1,

Δ∂u ∂r

|x|r1 −r

1−n

1 Nu

u||x|r1

m ,

Δ∂v ∂r

|x|r1 −r

1−n

1 Nv

v||x|r1

m ,

ux a≥0, vx b≥0 if|x|l1,

ux c > a, vx d > b if |x|l2,

PA

wheref0,0 0, g0,0 0,Δis the Laplacian ofu,0 < l1 < r1 < l2,andΩl1, l2 {x

Rn| l

1 < |x| < l2} with n > 2. ∂u/∂r denotes the differentiation in the radial direction,

Δu||x|r1 ur1−ur1,Δ∂u/∂r||x|r1 ∂u/∂rr

1−∂u/∂rr1− andm

l2

l1t

1−ndt.

Applying consecutive changes of variables,r |x|, sl2

r t1−ndtandtms/m,we may

transform problem5.1into problem3.20, wheret1 r12−nl12−n/l22−nl21−nandhican

be written as

hit m2 rm1−t2n−1kirm1−t. 5.1

Ifki : l1, l2 → 0,∞are continuous, then hi : 0,1 → 0,∞are also continuous and

satisfiesD1. We may applyTheorem 4.1to obtain the following result.

Corollary 5.1. Assume D2 ∼ D6. Let kiC l1, l2,0,, i 1,2. Then there exists a continuous curveΓ0splittingR2\ {0,0}into two disjoint subsetsO0,1andO0,2 and there exists a subsetO ⊂ O0,1such that problem5.1has at least two positive solutions forλ, μ∈ O,at least one positive solution forλ, μ∈O0,1\ O∪Γ0,and no solution forλ, μ∈ O0,2.

Ifki : l1, l2 → 0,are continuous and singular atr l1 and/or l2,thenhi are also

singular att0and/or1.In this case, we assume

l2

l1

r2−nl12−nl22−nr2−nkirdr <, 5.2

(21)

Corollary 5.2. AssumeD2∼D6.If bothkiCl1, l2,0,satisfy

l2

l1

r2−nl21nl22nr2−nkirdr <. 5.3

Then the conclusion ofCorollary 5.1is valid.

5.2. On an Exterior Domain

Let us consider

Δuλk1|x|fu, v 0,

Δvμk2|x|gu, v 0, |x|> r0, |x|/r1,

Δu||x|r1Iu

u||x|r1, Δv||x|r1 Iv

v||x|r1,

Δ∂u ∂r

|

x|r1

n−2

r0

r1

r0

1−n

Nu

u||x|r1,

Δ∂v ∂r

|

x|r1

n−2

r0

r1

r0

1−n

Nv

v||x|r1,

ux a≥0, vx b≥0, if|x|r0,

uxc > a, vxd > b, as|x| → ∞,

PE

wheref0,0 0, g0,0 0,0 < r0 < r1,andn >2.Assume that bothki : r0,∞ → 0,

are continuous. Applying changes of variables,r|x|andt1−r/r02−n,we may transform

problem5.4into problem3.20, wheret11−r0/r1n−2andhiare written as

hit

r02n−1

n−221−t

−2n−1/n−2k

i

r01−t−1/n−2

. 5.4

We know that hi are singular at t 1 and can easily check that hi satisfyD1if ki satisfy

r0 rkirdr <∞fori1,2.Thus byTheorem 4.1, we obtain the following result.

Corollary 5.3. AssumeD2∼D6.If bothkiC r0,,0,satisfy

r0

rkirdr <, 5.5

(22)

Acknowledgment

This work was supported for two years by Pusan National University Research Grant.

References

1 S. C. Hu and V. Lakshmikantham, “Periodic boundary value problems for second order impulsive differential systems,”Nonlinear Analysis: Theory, Methods & Applications, vol. 13, no. 1, pp. 75–85, 1989. 2 S. G. Hristova and D. D. Ba˘ınov, “Existence of periodic solutions of nonlinear systems of differential equations with impulse effect,”Journal of Mathematical Analysis and Applications, vol. 125, no. 1, pp. 192–202, 1987.

3 E. K. Lee and Y.-H. Lee, “Multiple positive solutions of a singular Gelfand type problem for second-order impulsive differential systems,”Mathematical and Computer Modelling, vol. 40, no. 3-4, pp. 307– 328, 2004.

4 B. Liu and J. Yu, “Existence of solution of m-point boundary value problems of second-order differential systems with impulses,”Applied Mathematics and Computation, vol. 125, no. 2-3, pp. 155– 175, 2002.

5 L. Liu, L. Hu, and Y. Wu, “Positive solutions of two-point boundary value problems for systems of nonlinear second-order singular and impulsive differential equations,”Nonlinear Analysis: Theory, Methods & Applications, vol. 69, no. 11, pp. 3774–3789, 2008.

6 Y. Dong, “Periodic solutions for second order impulsive differential systems,” Nonlinear Analysis: Theory, Methods & Applications, vol. 27, no. 7, pp. 811–820, 1996.

7 Y.-H. Lee, “A multiplicity result of positive radial solutions for a multiparameter elliptic system on an exterior domain,”Nonlinear Analysis: Theory, Methods & Applications, vol. 45, pp. 597–611, 2001. 8 D. J. Guo and V. Lakshmikantham,Nonlinear Problems in Abstract Cones, vol. 5, Academic Press, Boston,

Mass, USA, 1988.

References

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