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Journal of Inequalities and Applications Volume 2009, Article ID 191649,12pages doi:10.1155/2009/191649

Research Article

Multiple Solutions for a Class of

p

x

-Laplacian Systems

Yongqiang Fu and Xia Zhang

Department of Mathematics, Harbin Institute of Technology, Harbin 150001, China

Correspondence should be addressed to Xia Zhang,[email protected]

Received 19 November 2008; Accepted 11 February 2009

Recommended by Ondrej Dosly

We study the multiplicity of solutions for a class of Hamiltonian systems with thepx-Laplacian. Under suitable assumptions, we obtain a sequence of solutions associated with a sequence of positive energies going toward infinity.

Copyrightq2009 Y. Fu and X. 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 and Main Results

Since the space Lpx and W1,px were thoroughly studied by Kov´aˇcik and R´akosn´ık 1,

variable exponent Sobolev spaces have been used in the last decades to model various phenomena. In2, R ˚uˇziˇcka presented the mathematical theory for the application of variable exponent spaces in electro-rheological fluids.

In recent years, the differential equations and variational problems withpx-growth conditions have been studied extensively; see for example3–6. In7, De Figueiredo and Ding discussed the multiple solutions for a kind of elliptic systems on a smooth bounded domain. Motivated by their work, we will consider the following sort of px-Laplacian systems with “concave and convex nonlinearity”:

−div∇upx−2∇u|u|px−2uHux, u, v, xΩ,

−div∇vpx−2∇v|v|px−2v−Hvx, u, v, xΩ,

ux vx 0, xΩ,

1.1

whereΩ⊂RNis a bounded domain,pis continuous onΩand satisfies 1< p

−≤pxp <

(2)

of HamiltoniansHsuch that

Hx, u, v |u|

αx

αx |v|βx

βx Fx, u, v, 1.2

where 1< α− ≤αxpx, pxβxpx.Here we denote

psup

x∈Ωpx, px∈infΩpx, 1.3

and denote by px βx the fact that infx∈Ωβxpx > 0.Throughout this paper,

Fx, u, vsatisfies the following conditions:

H1FC1Ω×R2,R.Writingz u, v, Fx,00, Fzx,00;

H2there existpx< q1xpx,1< q2−≤q2x< pxsuch that Fux, u, v,Fvx, u, va0

1|u|q1x−1|v|q2x−1, 1.4

wherea0is positive constant;

H3there existμx, νxC1Ωwithpxμxpx,1< ν

− ≤νxpx,

andR0>0 such that

1

μxFux, u, vu

1

νxFvx, u, vvFx, u, v>0, 1.5

when|u, v| ≥R0.

As8, Lemma 1.1, from assumptionH3, there existb0, b1>0 such that

Fx, u, vb0

|u|μx|v|νxb

1, 1.6

for anyx, u, v∈Ω×R2.We can also get that there existsb

2>0 such that

1

μxFux, u, vu

1

νxFvx, u, vvb2≥Fx, u, v, 1.7

for anyx, u, v∈Ω×R2.In this paper, we will prove the following result.

Theorem 1.1. Assume that hypotheses (H1)–(H3) are fulfilled. IfFx, zis even inz, then problem 1.1has a sequence of solutions{zn}such that

Izn

Ω

∇unpxunpx

px

∇vnpx

vnpx

pxH

x, zn

dx−→ ∞, 1.8

(3)

2. Preliminaries

First we recall some basic properties of variable exponent spaces LpxΩ and variable

exponent Sobolev spaces W1,pxΩ,where Ω RN is a domain. For a deeper treatment

on these spaces, we refer to1,9–11.

Letbe the set of all Lebesgue measurable functionsp:Ω → 1,∞and

|u|pxinf

λ >0 :

Ω

uλpxdx≤1

. 2.1

The variable exponent spaceLpxΩis the class of all functionsusuch that

Ω|ux|pxdx <

∞.Under the assumption thatp < ∞, LpxΩis a Banach space equipped with the norm

2.1.

The variable exponent Sobolev space W1,pxΩ is the class of all functions u

LpxΩsuch that|∇u| ∈LpxΩand it can be equipped with the norm

u1,px|u|px|∇u|px. 2.2

ForuW1,pxΩ,if we define

|||u|||inf

λ >0 :

Ω

|u|px|∇u|px

λpx dx≤1

, 2.3

then|||u|||andu1,pxare equivalent norms onW1,pxΩ.

By W01,pxΩ we denote the subspace ofW1,pxΩ which is the closure ofC0 Ω

with respect to the norm2.2and denote the dual space ofW01,pxΩbyW−1,pxΩ.We

know that ifΩ ⊂ RN is a bounded domain,||u||

1,px and |∇u|px are equivalent norms on

W01,pxΩ.

Under the condition 1< p− ≤ p <∞, W01,pxΩis a separable and reflexive Banach

space, then there exist{en}n1∞ ⊂W01,pxΩand{fm}m∞1⊂W−1,p

x

Ωsuch that

fmen

1 ifnm,

0 ifn /m, W01,pxΩ spanei:i1, . . . , n, . . .

,

W−1,pxΩ spanfj:j 1, . . . , m, . . .

.

2.4

In the following, we will denote thatEE1⊕E2,where

(4)

For any zE, define the norm||z|| ||u, v|| |||u||||||v|||. For anyn ∈ N,set e1

n 0, en, e2

n en,0and

Xnspan

e11, . . . , en1

E2, XnE1⊕spane12, . . . , e2n

, 2.6

denote the complement ofXninEbyXnspan{e2

n1, en22, . . .}.

3. The Proof of Theorem

1.1

Definition 3.1. We say thatz0 u0, v0∈Eis a weak solution of problem1.1, that is,

Ω

∇u0px−2∇u0∇uu0px−2u0u−∇v0px−2∇v0∇v

v0px−2v0vHu

x, u0, v0

uHv

x, u0, v0

vdx0, ∀z∈E.

3.1

In this section, we denote thatVm span{ei :i 1, . . . , m},for anym ∈N, andci is

positive constant, for anyi0,1,2. . . .

Lemma 3.2. AnyPSsequence{zn} ⊂ E, that is,|Izn| ≤ cand Izn → 0,as n → ∞,is bounded.

Proof. Lets > 0 be sufficiently small such thatl1 infx∈Ω1/px −1s/μx > 0, l2

infx∈Ω1s/νx−1/px>0, l3supx∈Ω1/αx−1s/μx>0, l4supx∈Ω1

s/νx− 1/ βx >0.

Let{zn} ⊂Ebe such that|Izn| ≤c and Izn → 0,asn → ∞.We get

Izn

Izn

,

1s μxun,

1s νxvn

Ω 1

px

1s μx

∇unpxunpx

1sun

μx2 ∇un

px−2∇u

n∇μ

1s νx

1

px

∇vnpxvnpx

− 1svn

νx2

∇vnpx−2∇v

n∇ν

1s

μxFu

x, un, vn

un

1s νxFv

x, un, vn

vnF

x, un, vn

1s μx

1

αx

unαx

1s νx

1

βx

vnβx

dx ≥ Ω

l1∇unpxl2∇vnpxsF

x, un, vn

l3unαxl4vnβx

1sun

μx2

∇unpx−2∇u

n∇μ− 1svn

νx2

∇vnpx−2∇v

n∇ν−1sb2

dx.

(5)

Asμx, νxC1Ω,by the Young inequality, we can get that for anyε

1, ε2∈0,1,

1sun

μx2 ∇un

px−2∇u

n∇μ

c0∇unpx−1un

c0

ε1px−1

px ∇un

px ε11−px

px un

px

c0

ε1∇unpxε11−punpx

,

1svn

νx2

∇vnpx−2∇v

n∇ν

c1

ε2∇vnpxε21−pvnpx

.

3.3

Letε1, ε2be sufficiently small such that

c0ε1≤ l1

2 , c1ε2≤

l2

2 , 3.4

then

Izn

Izn

,

1s μxun,

1s νxvn

Ω

l1

2 ∇un

px l2

2 ∇vn

px

sb0unμxb0vnνxb1

l3unαxc0ε11−punpx

l4vnβxc1ε12−pvnpx

−1sb2

dx.

3.5

Note thatαxpxμx, pxβx,by the Young inequality, for anyε3, ε4, ε5∈0,1,

we get

unαx ε3αxunμx

μx

μxαx μx ε

αx/αx−μx 3

ε3unμxε−α3 /μ−α,

unpx ε4px

μx un

μx μxpx

μx ε

px/px−μx 4

ε4unμxε−p4 /μ−p,

vnpx ε5px

βx vn

βx βxpx

βx ε

px/px−βx 5

ε5vnβxε−p5 /β−p.

(6)

Letε3, ε4, ε5 be sufficiently small such thatl3ε3c0ε11−pε4 ≤sb0 andc1ε12−pε5 ≤ l4,then we

get

Izn

Izn

,

1s μxun,

1s νxvn

≥ Ω l1

2 ∇un

px l2

2 ∇vn

px

c2

dx. 3.7

Note that

Izn

,

1s μxun,

1s νxvn

Izn·1s μxun

1s

νxvn

c3I

zn·

1s μxun

px

1s νxvn

px

c4I

zn·

∇unpx∇vnpx

,

3.8

and forn∈Nbeing large enough, we have

c4I

zn≤min

l1 4 , l2 4

. 3.9

It is easy to know that if|∇un|px≥1 and|∇vn|px≥1,

∇un

px

Ω

∇unpx

dx, ∇vnpx

Ω

∇vnpx

dx, 3.10

thus we get

Izn

≥ Ω l1

4 ∇un

px l2

4 ∇vn

px

c2

dx, 3.11

then|∇un|px,|∇vn|pxare bounded. Similarly, if|∇un|px < 1 or|∇vn|px < 1,we can also

get that|∇un|px,|∇vn|pxare bounded. It is immediate to get that{zn}is bounded inE.

Lemma 3.3. AnyPSsequence contains a convergent subsequence.

Proof. Let{zn} ⊂ Ebe aPSsequence. ByLemma 3.2, we obtain that{zn}is bounded inE.

(7)

existszEsuch thatznzweakly inE.Then we can getunuweakly inW01,pxΩ.

Note that

Izn

Iz,unu,0

Ω

∇unpx−2∇un−∇upx−2∇u

unu

unpx−2un− |u|px−2uunu

unαx−2un− |u|αx−2u

unu

Fu

x, un, vn

Fux, u, vunu

dx.

3.12

It is easy to get that

Izn

Iz,unu,0

−→0,

ΩFux, u, v

unu

dx−→0, 3.13

andunuinLpxΩ, unuinLαxΩ,asn → ∞.Then

Ω

unpx−2un− |u|px−2uunu

dx−→0,

Ω

unαx−2un− |u|αx−2u

unu

dx−→0,

3.14

asn → ∞.By conditionH2, we obtain

Ω Fu

x, un, vn

unudx

Ωa0

1unq1x−1vnq2x−1

unudx

a1

unu1unq1x−1

q1x·unuq1x

vnq2x−1 q2x

·unuq2x

.

3.15

It is immediate to get that |unu|1 → 0,||un|q1x−1|q1x,||vn|q2x−1|q2x are bounded and

|unu|q1x → 0,|unu|q2x → 0,then we get

ΩFu

x, un, vn

unu

dx−→0,

Ω

∇unpx−2∇un−∇upx−2∇u

unu

dx−→0,

3.16

asn → ∞.Similar to3,4, Theorem 3.1, we divideΩinto two parts:

(8)

OnΩ1,we have

Ω1

∇un− ∇upx

dx

c5

Ω1

∇unpx−2∇un−∇upx−2∇u∇un− ∇u

px/2

×∇unpx∇upx

2−px/2

dx

c6

∇unpx−2∇un−∇upx−2∇u∇un− ∇u

px/2

2/ px,Ω1

×∇unpx∇upx

2−px/2

2/2−px,Ω1

,

3.18

thenΩ

1|∇un− ∇u|

pxdx 0.OnΩ

2,we have

Ω2

|∇un− ∇u|pxdxc7

Ω2

|∇un|px−2∇un− |∇u|px−2∇u∇un− ∇udx−→0. 3.19

Thus we getΩ|∇un− ∇u|pxdx → 0.Thenunuin W01,pxΩ,asn → ∞.Similarly,

vnvinW01,pxΩ.

Lemma 3.4. There existsRm>0such thatIz≤0for allzXmwith||z|| ≥Rm.

Proof. For anyz u, vXm, uVm,we have

Iz

Ω

∇upx|u|px

px

∇vpx|v|px

pxFx, u, v dx

Ω

∇upx|u|px

p− −

∇vpx|v|px

pb0|u|

μxb

1 dx.

3.20

In the following, we will considerΩ|∇u|px|u|px/pb0|u|μxdx.

iIf|||u||| ≤1.We have

Ω

∇upx|u|px

p− −b0|u|

μx dx 1

p. 3.21

iiIf|||u|||>1.Note thatμ, pCΩ, pxμx.For anyx∈Ω,there existsQx

which is an open subset ofΩsuch that

px sup

(9)

then{Qx}x∈Ωis an open covering ofΩ.AsΩis compact, we can pick a finite subcovering

{Qx}ni1forΩ.Thus there exists a sequence of open set{Ωi}ni1such thatΩ ni1Ωiand

pi sup

x∈Ωipx< μi−

inf

x∈Ωiμx, 3.23

fori1, . . . , n.Denote thatri|||u|||Ωi,then we have

Ω

∇upx|u|px

p− −b0|u|

μx dx

n i1

Ωi

∇upx|u|px

p− −b0|u|

μx dx

ri>1

Ωi

∇upx|u|px

p− −b0|u|

μx dx

ri≤1

Ωi

∇upx|u|px

p− −b0|u|

μx dx

ri>1

|||u|||pi

Ωi

p− −b0kmi|||u||| μi

Ωi pn ,

3.24

where kmi infu∈Vmi,|||u|||Ωi1

Ωi|u|μxdx.As Vm|Ωi is a finite dimensional space, we have

kmi >0,fori1, . . . , n.

We denote bysi the maximum of polynomial tpi/p− −b0kmitμi− on 0,,fori

1, . . . , n.Then there existst0>1 such that

tpi

p− −b0kmit μic

8≤0, 3.25

fort > t0andi1, . . . , n,wherec8 ni1sin/pb1measΩ.

LetRm max{2,2pc8 1/ p−1/p,2nt0}.If ||z|| ≥ Rm,we get |||u||| ≥ Rm/2 or

|||v||| ≥Rm/2.

iIf|||u||| ≥Rm/2,|||u||| ≥nt0 > 1.It is easy to verify that there exists at leasti0such

that|||u|||Ωi

0 ≥t0>1,thus

Iz≤ |||u|||

pi0

Ωi0

p− −b0kmi0|||u||| μi0

(10)

iiIf|||v||| ≥Rm/2,|||v||| ≥pc81/p−1/p.We obtain

Izc8

1

p− −

|||v|||p

p ≤0. 3.27

Now we get the result.

Lemma 3.5. There existrm>0andam → ∞m → ∞such thatIzam,for anyzXm−1⊥ with||z||rm.

Proof. Forz u, vXm−1, v0.By conditionH2, there existsc

9>0 such that Fx, u,0c9|u|q1xc

9. 3.28

Let||z|| ≥1,we get

Iz

Ω

∇upx|u|px

px − |u|αx

αxFx, u,0 dx

Ω

∇upx|u|px

p

|u|αx

α− −c9|u| q1xc

9 dx

Ω

∇upx|u|px

pc10|u|

q1x dxc

11.

3.29

Denote that

θm sup u∈V

m

|||u|||≤1

Ω|u|

q1xdx, 3.30

thus

Iz≥ |||u|||

p

pc10θmu

q1c

11. 3.31

Let

rmmax

1,

p

c10pq1θm

1/q1−p−

,

2

c11pq1

q1−p

1/p

(11)

By5, Lemma 3.3, we get thatθm → 0,asm → ∞,then

Izrmp

q1−p

pq1 −c11

am,

3.33

whenmis sufficiently large and||z||rm.It is easy to get thatam → ∞,asm → ∞.

Lemma 3.6. I is bounded from above on any bounded set ofXm.

Proof. Forz u, vXm.We get

Iz

Ω

∇upx|u|px

pxFx, u, v dx. 3.34

By conditionsH2and H3, we know that if|u, v| ≥ R0, Fx, u, v ≥ 0 and if |u, v| <

R0,|Fx, u, v| ≤c0.Then

Iz

Ω

∇upx|u|px

px c12 dx, 3.35

and it is easy to get the result.

Proof ofTheorem 1.1. By Lemmas3.2–3.6above, and7, Proposition 2.1 and Remark 2.1, we know that the functionalI has a sequence of critical valuesck → ∞,ask → ∞.Now we

complete the proof.

Acknowledgments

This work is supported by Science Research Foundation in Harbin Institute of Technology

HITC200702and The Natural Science Foundation of Heilongjiang ProvinceA2007-04.

References

1 O. Kov´aˇcik and J. R´akosn´ık, “On spacesLpx andWk,px,”Czechoslovak Mathematical Journal, vol. 41116, no. 4, pp. 592–618, 1991.

2 M. R ˚uˇziˇcka,Electrorheological Fluids: Modeling and Mathematical Theory, vol. 1748 ofLecture Notes in Mathematics, Springer, Berlin, Germany, 2000.

3 J. Chabrowski and Y. Fu, “Existence of solutions forpx-Laplacian problems on a bounded domain,” Journal of Mathematical Analysis and Applications, vol. 306, no. 2, pp. 604–618, 2005.

4 J. Chabrowski and Y. Fu, “Corrigendum to: “Existence of solutions forpx-Laplacian problems on a bounded domain”,”Journal of Mathematical Analysis and Applications, vol. 323, no. 2, p. 1483, 2006.

5 X. Fan and X. Han, “Existence and multiplicity of solutions forpx-Laplacian equations inRN,”

Nonlinear Analysis: Theory, Methods & Applications, vol. 59, no. 1-2, pp. 173–188, 2004.

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7 D. G. De Figueiredo and Y. H. Ding, “Strongly indefinite functionals and multiple solutions of elliptic systems,”Transactions of the American Mathematical Society, vol. 355, no. 7, pp. 2973–2989, 2003.

8 P. L. Felmer, “Periodic solutions of “superquadratic” Hamiltonian systems,”Journal of Differential Equations, vol. 102, no. 1, pp. 188–207, 1993.

9 D. E. Edmunds, J. Lang, and A. Nekvinda, “OnLpxnorms,”Proceedings of the Royal Society of London. Series A, vol. 455, no. 1981, pp. 219–225, 1999.

10 D. E. Edmunds and J. R´akosn´ık, “Sobolev embeddings with variable exponent,”Studia Mathematica, vol. 143, no. 3, pp. 267–293, 2000.

References

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