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Electronic Journal of Qualitative Theory of Differential Equations

2005, No. 18, 1-12,http://www.math.u-szeged.hu/ejqtde/

EXISTENCE OF SOLUTIONS TO NONLOCAL AND SINGULAR VARIATIONAL ELLIPTIC INEQUALITY VIA GALERKIN

METHOD

FRANCISCO JULIO S. A. CORR ˆEA & SILVANO B. DE MENEZES

Abstract. In this article, we study the existence of solutions for nonlocal variational elliptic inequality

−M(kuk2)∆uf(x, u)

Making use of the penalized method and Galerkin approximations, we estab-lish existence theorems for both cases whenM is continuous and whenM is discontinuous.

1. Introduction

Let Ω⊂RN be a bounded smooth domain with boundary∂Ω. Let us consider

the Sobolev spacesL2(Ω), H1

0(Ω) whose inner products and norms will be denoted

by (,),|,|,((,)),k,k, respectively. We haveH1

0(Ω)⊂L2(Ω) dense and continuous.

Then the duals (L2(Ω)) (H1

0(Ω))′ also dense and continuous. If we identify

L2(Ω) = (L2(Ω))we have

H1

0(Ω)⊂L

2(Ω)H−1(Ω),

whereH−1(Ω) is the dual ofH1

0(Ω). Throughout this paper, let us represent byK

a closed convex set ofL2(Ω), with 0K, which has the following property:

(H1) There exists a contractionρ:R−→R(e.g., |ρ(λ1)ρ(λ2)|≤ |λ1λ2|)

withρ(0) = 0 such that (PKv)(x) =ρ(v(x)),∀v ∈L2(Ω), wherePK is the

projec-tion operator fromL2(Ω) intoK.

For example, let us considerK={v∈L2(Ω); av(x)b a.e. in}

where−∞ ≤a≤0≤b≤ ∞. We defineρ(λ) as follows

ρ(λ) =   

λ f or a < λ < b

b f or λ≥b (if b is f inite) a f or λ≤a (if a is f inite)

In this paper we study some questions related to the existence of solutions for the nonlocal elliptic variational inequality:

u∈K: (−M(kuk2)∆u, v)(f, v), f or all vK(H1

0(Ω)∩H

2(Ω)) (1.1)

where f ∈ H1

0(Ω) and M : R → R is a function whose behavior will be stated

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problem (1.1), and its nonlinear counterpart, possesses a solution. This inequality has called our attention because the operator

Lu:=M(kuk2)∆u

contains the nonlocal term M(kuk2) which poses some interesting mathematical

questions. Also the operatorL appears in the Kirchhoff equation, which arises in nonlinear vibrations, namely

utt−M

Z

|∇u|2dx∆u=f(x, u) in Ω×(0, T),

u= 0 on∂Ω×(0, T), u(x,0) =u0(x), ut(x,0) =u1(x).

The mathematical aspects of this model were largely investigated. See, for example, Arosio-Spagnolo [2], Hazoya-Yamada [11], Lions [16], Pohozhaev [18]. A survey of the results about the mathematical aspects of Kirchhoff model can be found in Medeiros-Limaco-Menezes [14]. Unilateral problems for nonlinear operators of the Kirchhoff type were initially studied by Kludnev [12], Larkin [13], Medeiros-Milla Miranda [17] among others.

Recently, Alves-Corrˆea [1] focused their attention on problem related with (1.1) in case M(t) ≥ m0 > 0, for all t ≥ 0, where m0 is a constant. Among other

things they studied the aboveM-linear problem (1.1) whereM, besides the strict positivity mentioned before, satisfies the following assumption:

The functionH :RRwith

H(t) =M(t2)t

is monotone andH(R) =R.

In a previous paper, Menezes-Corrˆea [8] proved a similar results by allowingMto attain negative values andM(t)≥m0>0 only fortlarge enough. This is possible

thanks to a device explored by Alves-de Figueiredo [3], who use Galerkin method to attack a non-variational elliptic system. The technique can be conveniently adapted to problems such as (1.1). In this way we improve substantially the existence result on the above problem mainly because our assumptions onM are weakened. Indeed, we may also consider the case in whichM possesses a singularity. The methodology used in our proof consists in transforming, by penalty, the inequality (1.1) into a family of equations depending of a parameterǫ >0 and apply Galerkin’s method. In the application of Galerkin’s methods we use the sharp angle lemma(see Lions [15, p.53]). This paper is organized as follows: Section 2 is devoted to the study of (1.1) in the continuous case. In Section 3 the inequality (1.1) is studied in case M possesses a discontinuity. In Section 4 we analyze another type of variational inequality.

2. The M-linear Problem: Continuous Case

In this section we are concerned with the M-linear problem (1.1) where f ∈

H1

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(M1) There exists a positive numberm0such thatM(t)≥m0, for allt≥0.

We have

Theorem 2.1. Assume that and (M1) and (H1) hold. Then for any choice of

06=f ∈H1

0(Ω) the problem (1.1) admits at least one solution.

The proof of Theorem 2.1 is given by the penalty method. In fact, let us represent byβ the operator from L2(Ω) intoL2(Ω) defined byβ =IP

K, e.g., (βv)(x) =

v(x)−ρ(v(x)) for allv∈L2(Ω).The operatorβis monotone and Lipschitzian. The

next result can be found in Haraux [10] p. 58.

Lemma 2.2. Letg:RRbe a Lipschitzian and increasing function withg(0) =

0. Then(g(u),−∆u)≥0 for allu∈H1

0(Ω)∩H 2(Ω).

We have thatg(s) =s−ρ(s) is under the condition of the Lemma 2.2, then

(β(v),−∆v)≥0f or all v∈H01(Ω)∩H 2

(Ω). (2.1)

The penalized problem associated to the problem (1.1), consists in givenǫ >0, find uǫsolution in Ω of the problem

−M(kuǫk2)∆uǫ+

1

ǫβ(uǫ) =f in Ω, uǫ= 0 on∂Ω,

(2.2)

wheref is given in H1 0(Ω).

The existence of one solution of the penalized problem (2.2) is give by the

Theorem 2.3. Assume that(M1)hold. Then, for any06=f ∈H1

0(Ω)there exists at least oneuǫ∈H01(Ω)∩H2(Ω), solution of the problem (2.2).

Proof. We employ the Galerkin Method by using the sharp angle lemma. Let us consider the Hilbertian basis of spectral objects (ej)j∈Nand (λj)j∈Nfor the operator

−∆ inH1

0(Ω), cf. Brezis [5]. We know that the eigenvectors (ej)j∈Nare orthonormal

complete inL2(Ω) and complete inH1

0(Ω)∩H2(Ω). For eachm∈Nconsider Vm= span{e1, . . . , em},

the subspace ofH1

0(Ω)∩H2(Ω) generated bymeigenvectorse1, e2, ..., em. Ifuǫm ∈

Vm, then

uǫm = m

X

j=1

ξjej with real ξj, 1≤j ≤m.

We will consideruminstead ofuǫm . The approximate problem consists in finding

a solutionum∈Vmof the system of algebraic equations

M(kumk2)((um, ei)) +

1

ǫ(β(uǫ), ei) = (f, ei), i= 1, . . . , m. (2.3) We need to prove that (2.3) has a solutionum∈Vm. To this end, we will consider

the vectorη= (ηi)1≤i≤m ofRmdefined by

ηi =M(kumk2)((um, ei)) +

1

ǫ(β(um), ei)−(f, ei), i= 1, . . . , m.

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Let ξ = (ξi)1≤i≤m be the components of the vector um of Vm. The mapping

P :Rm Rm defined byP ξ =η is continuous. If we prove thathP ξ, ξi ≥0 for

kξkRn=r, with an appropriater, it will follow by the sharp angle lemma that there

exists aξ in the ballBr(0)⊂Rmsuch that P ξ= 0. This implies the existence of

a solution to (2.3). In fact, we have

hP ξ, ξi=

m

X

1

ξiηi=M(kumk)((um, um)) +

1

ǫ(β(um), um)−(f, um).

Using (M1), H¨older and Poincar´e inequalities and observing that (β(um), um)≥0,

we get

hP ξ, ξi ≥m0kumk2−Ckfkkumk

We can consider r large enough that (P ξ, ξ) ≥ 0 for kξkRm = r. Then P ξ = 0

for some ξ ∈ Br(0), which implies that system (2.3) has a solution um ∈ Vm

corresponding to thisξ. Thus, there isum∈Vm,

kumk ≤r, (2.4)

rdoes not depend onmandǫ, such that

M(kumk2)((um, ei)) +

1

ǫ(β(um), ei) = (f, ei), i= 1, . . . , m, which implies that

M(kumk2)((um, ω)) +

1

ǫ(β(um), ω) = (f, ω), for allω∈Vm. (2.5) Because (kumk2) is a bounded real sequence and M is continuous one has

kumk2→˜t0, (2.6)

for some ˜t0≥0, and

um⇀ uinH01(Ω), um→uin L2(Ω), M(kumk2)→M(˜t0), (2.7)

perhaps for a subsequence.

Takek≤m,Vk Vm. Fixk and letm→ ∞in equation (2.5) to obtain

M(˜t0)((u, ω)) +

1

ǫ(β(u), ω) = (f, ω), for allω∈(H

1 0 ∩H

2

)(Ω). (2.8)

Since−∆ej=λjej we takeω=−∆um in (2.8). We obtain

M(te0)(∆um,∆um) +

1

ǫ(β(um),−∆um) = (∇f,∇um) (2.9) By (2.1), we obtain

|∆um|2≤C(|∇f|2+|∇um|2). (2.10)

Sincef ∈H1

0(Ω) and by (2.6), we have that

|∆um|2≤C (2.11)

whereCdoes not depend onmandǫ. By (2.7) and (2.11) and by compact imbed-ding of (H1

0(Ω)∩H2(Ω))⊂H01(Ω) we deduce that

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The continuity ofM and convergence (2.7) and (2.12) permit to pass to the limit in (2.5). We obtain

M(kuk2)((u, v)) +1

ǫ(β(u), v) = (f, v), for allv∈H

1

0(Ω)∩H2(Ω). (2.13)

Thusuǫ is a weak solution of problem (2.2) and the proof of Theorem 2.3 is

com-plete.

Proof. of Theorem 2.1

Let (ǫn)n∈Nbe a sequence of real numbers such that

0< ǫn<1f or all n∈N and lim

n→∞ǫn= 0.

For eachn∈N, we get functionuǫnwhich satisfies Theorem 2.3. Since the estimates

were uniform onǫ and n, we can see that there exists a subsequence ofuǫn, again

calleduǫn, and a functionu∈H01(Ω)∩H2(Ω) such that

uǫm →uin H01(Ω). (2.14)

Considerv in H1

0(Ω)∩H

2(Ω) with vbelongs toK. By (2.5), we have

(−M(kuǫnk2)∆uǫn−f, v) = (−

1 ǫn

β(uǫn), v) (2.15)

and

(−M(kuǫnk2)∆uǫn−f,−uǫn) = (−

1 ǫn

β(uǫn),−uǫn). (2.16)

Follows of (2.15) and (2.16) that

(−M(kuǫnk2)∆uǫn−f, v−uǫn) =

1

ǫ(−β(uǫn), v−uǫn)

= 1

ǫ(β(v)−β(uǫn), v−uǫn)≥0,

(2.17)

becausev∈K and monotonicity ofβ. Hence

(−M(kuǫnk2)∆uǫn−f, v) + (f, uǫn)≥(−M(kuǫnk2)∆uǫn, uǫn), (2.18)

But

(−M(kuǫnk2)∆uǫn, uǫn) =M(kuǫnk2)(∇uǫn,∇uǫn) =

M(kuǫnk2)(∇(uǫn−u),∇(uǫn−u)) +M(kuǫnk2)(∇uǫn,∇u)+

M(kuǫnk2)(∇u,∇(uǫn−u))≥M(kuǫnk2)(∇uǫn,∇u)+

M(kuǫnk2)(∇u,∇(uǫn−u)),

(2.19)

becauseM(kuǫnk2)(∇(uǫn−u),∇(uǫn−u))≥0.Then,

lim inf[−M(kuǫnk2)(∆uǫn, uǫn)]≥ −M(kuk2)(∇u, u). (2.20)

By (2.18) and (2.20), we obtain (1.1).

In order to proveu∈K we observe that from (2.5), withω =uǫm, that

0≤(β(uǫn), uǫn)≤ǫC (2.21)

therefore

(β(uǫn), uǫn) converges to zero. (2.22)

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Letv∈H1

0(Ω) be arbitrarily fixed; then the inequality

(β(uǫn)−β(v), uǫn−v)≥0

yields (β(v), u−v)≤0, hence (β(u−λω)), ω)≤0 with the choice of v=u−λω withλ >0 andω∈H1

0(Ω). By hemicontinuity ofβ we can letλ→0+ and obtain

(β(u), ω)≥0, hence β(u) = 0 by the arbitrariness ofω. Thereforeu∈K.

3. The M-linear Problem: A Discontinuous Case

In this section we concentrate our atention on problem (1.1) whenM possesses a discontinuity. More precisely, we study problem (1.1) with M : R/{θ} → R

continuous such that

(M2) limt→θ+M(t) = limtθ−M(t) = +∞

(M3) lim supt→+∞M(t2)t= +∞.

Theorem 3.1. Assume that (M1)–(M3) and (H1) hold. Then for any choice of

f ∈H1

0(Ω)the problem (1.1)admits at least one solution solution.

The proof of Theorem 3.1 is given as in the proof of Theorem 2.1. We will formulate the penalized problem, associated with the variational inequality (1.1), as follows. Givenǫ >0, find a functionuǫ∈H01(Ω) solution of the problem

−M(kuǫk2)∆uǫ+

1

ǫβ(uǫ) =f in Ω, uǫ= 0 on∂Ω,

(3.1)

wheref is given in H1 0(Ω).

The existence of one solution of the penalized problem (3.1) is given by the

Theorem 3.2. Assume that (M1)−(M3) hold. Then, for any 0 6=f ∈ H1 0(Ω) there exists at least oneuǫ∈L2(Ω), solution of the problem (3.1).

Proof. We first consider the sequence of functionsMn :R→Rgiven by

Mn(t) =

(

n, θ−δ′

n≤t≤θ+δ′′n,

M(t), t≤θ−δ′

n or t≥θ+δn′′,

forn > m0, whereθ−δn′ andθ+δ′′n,δn′,δ′′n>0, are, respectively, the points closest

toθ, at left and at right, so that

M(θ−δ′n) =M(θ+δ ′′ n) =n.

We point out that, in this case,δ′

n, δn′′→0 asn→ ∞.

Taken > m0 and observe that the horizontal linesy=ncross the graph ofM.

Hence Mn is continuous and satisfies (M1), for each n > m0. In view of this, for

eachnlike above, there isun ∈H01(Ω)

T

H2(Ω) satisfying

Mn(kunk2)((un, ω)) +

1

ǫ(β(un), ω) = (f, ω), for allω∈H01(Ω)∩H

2

(Ω).

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Takingω=un in the above equation one has

Mn(kunk2)kunk2+

1

ǫ(β(un), un) = (f, un), and so

Mn(kunk2)kunk ≤ kfk,

since 0 ≤ (β(un), un). Because of (M3) the sequence (kunk) must be bounded.

Hence

un⇀ u inH01(Ω),

un→u inL2(Ω),

kunk2→θ0, for someθ0,

(3.3)

perhaps for subsequences. We note that if (Mn(kunk2) converges its limit is different

of zero. Suppose thatkunk2→θ. Ifkunk2> θ+δn′′orkunk2< θ−δ′n, for infinitely

manyn, we would getMn(kunk2) =M(kunk2), for suchn, and so

M(kunk2)kunk2≤(f, un) ⇒ +∞ ≤(f, u)

which is a contradiction. On the other hand, if there are infinitely manynso that θ−δ′

n≤ kunk2 ≤θ+δ′′n ⇒ Mn(kunk2) =n and sonkunk2 ≤(f, un) ⇒ +∞ ≤

(f, u) and we arrive again in a contradiction.

Consequentlykunk2→θ06=θwhich implies that fornlarge enough

kunk2< θ−δn′ or kunk2> θ+δn′′

and soMn(kunk2) =M(kunk2) which yields

M(kunk2)((un, ω)) +

1

ǫ(β(un), ω) = (f, ω), ∀ω∈H

1

0(Ω)∩H

2(Ω). (3.4)

Taking ω = −∆un in (3.4), using(2.1) and arguments of compactness as in the

proof of theorem 2.1, we obtain that

un→u ∈H01(Ω) (3.5)

The estimates (3.3) and (3.5) are sufficient to pass to the limit in the approximate equation and to obtain

M(kuk2)((u, ω)) +1

ǫ(β(u), ω) = (f, ω), ∀ω∈H

1

0(Ω)∩H

2(Ω). (3.6)

Proof. of Theorem 3.1

As in the proof of Theorem 2.1, let (ǫn)n∈N be a sequence of real numbers such,

that

0< ǫn<1f or all n∈N and lim

n→∞ǫn= 0.

Applying Theorem 3.1, for each n∈ N, we get a function uǫn H01(Ω)H2(Ω)

which satisfies

M(kuǫnk2)((uǫn, ω)) +

1 ǫn

(β(uǫn), ω) = (f, ω), ∀ω∈H01(Ω)∩H

2(Ω). (3.7)

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Since the estimates were uniform onǫ and n, we can see that there exists a sub-sequence of (uǫn), again called (uǫn), and a function u ∈ H01(Ω)∩H2(Ω) such

that

uǫn→uinH01(Ω). (3.8)

We note that kuǫnk does not converges to θ. In fact, we assume by contradiction

thatkuǫnk →θ. By (3.7) and (3.8), withω=uǫn, we get

M(kuǫnk2)kuǫnk ≤C

By hyphotese (M2), lettingn→ ∞, we have a contradiction. Thus M(kuǫnk2)→M(kuk2),

sincekuǫnk → kuk andM is continuous in an neighboard ofkuk 6=θ.

Considerv in H1

0(Ω) withv belonging toK. By (3.7), we have

(−M(kuǫnk2)∆uǫn−f, v) = (−

1

ǫβ(uǫn), v) (3.9) and

(−M(kuǫnk2)∆uǫn−f,−uǫn) = (−

1

ǫβ(uǫn),−uǫn). (3.10) Follows of (3.9) and (3.10) that

(−M(kuǫnk2)∆uǫn−f, v−uǫn) =

1

ǫ(−β(uǫn), v−uǫn)

= 1

ǫ(β(v)−β(uǫn), v−uǫn)≥0,

(3.11)

becausev∈K and monotonicity ofβ. Hence

(−M(kuǫnk2)∆uǫn−f, v) + (f, uǫn)≥(−M(kuǫnk2)∆uǫn, uǫn). (3.12)

As in the proof of Theorem 2.1, letting n → ∞, we obtain that u satisfies the conditions of Theorem 3.2.

4. Another Nonlocal Problem

Next, we make some remarks on a nonlocal problem which is a slight generaliza-tion of one studied by Chipot-Lovat [6] and Chipot-Rodrigues [7]. More precisely, the above authors studied the problem

−a Z

u∆u=f in Ω,

u= 0 on∂Ω,

(4.1)

where Ω ⊂ RN is a bounded domain, N 1, and a : R (0,+) is a given

function. Equation (4.1) is the stationary version of the parabolic problem

ut−a

Z

u(x, t)dx∆u=f in Ω×(0, T),

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Here T is some arbitrary time and u represents, for instance, the density of a population subject to spreading. See [6, 7] for more details. In particular, [6] studies problem (4.1), withf ∈H−1(Ω), and proves the following result.

Proposition 4.1. Let a:R(0,+)be a positive function,f H−1(Ω). Then problem (4.1) has as many solutionsµ as the equation

a(µ)µ=hhf, ϕii,

whereϕis the function(unique) satisfying

−∆ϕ= 1 inΩ, ϕ= 0 on∂Ω.

In the present work, we consider the variational inequality

u∈K: (−a Z

|u|q∆u, ω)(f, ω) f or all vK(H1

0(Ω)∩H

2(Ω)) (4.2)

where K and f are as before and 1 < q <2N/(N−2), N ≥3. When q = 2 we have the well known Carrier model.

Theorem 4.2. If t 7→ a(t) is a decreasing and continuous function, for t ≥ 0,

limt→+∞a(tq)t= +∞andt7→a(tq)t is injective, fort≥0, then, for each06=f ∈

H−1(Ω), problem (4.2) possesses a weak solution.

The proof of Theorem 4.2 is given as in the proof of Theorem 2.1. We will formulate the penalized problem, associated with the variational inequality (4.2), as follows: Givenǫ >0, find a functionuǫ∈H01(Ω) solution of the problem

−a Z

|uǫ|q∆uǫ+

1

ǫβ(uǫ) =f in Ω, uǫ= 0 on∂Ω,

(4.3)

wheref is given in H1 0(Ω).

The existence of one solution of the penalized problem (4.3) is given by the

Theorem 4.3. Under the hypotheses of Theorem 4.2, then for each 0 6= f ∈

H−1(Ω)there exists at least one u

ǫ∈H01(Ω) solution of the problem (4.3). Proof. As in the proof of Theorem 2.1, letP={e1, . . . , em, . . .}be an orthonormal

basis of the Hilbert space H1

0(Ω). For each m∈Nconsider the finite dimensional

Hilbert space

Vm= span{e1, . . . , em},

P :RmRm be the functionP(ξ) = (P1(ξ), . . . , Pm(ξ)), where

Pi(ξ) =a(kukqq)((u, ei)) +

1

ǫ(β(u), ei)− hhf, eiii, i= 1, . . . , m withu=Pmj=1ξjej and the identifications ofRmandVmmentioned before. So

Pi(ξ) =a(kukqq)ξi+

1

ǫ(β(u), ei)− hhf, eiii, i= 1, . . . , m and then

< P(ξ), ξ >=a(kukqq)kuk 2

+1

ǫ((β(u), u))− hhf, uii

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We have to show that there isr >0 so thathP(ξ), ξi ≥0, for allkξkRm =rinVm.

Suppose, on the contrary, that for eachr >0 there isur∈Vm such thatkurk=r

and

hP(ξr), ξri<0, ξr↔ur.

Takingr=n∈Nwe obtain a sequence (un),kunk=n,unVmand

hP(un), uni=a(kunkqq)kunk2+

1

ǫ(β(un), un)− hhf, unii<0 and so

a(kunkqq)kunk< Ckfk, ∀n= 1,2, . . . ,

since(β(un), un) > 0. Because of the continuous immersion H01(Ω) ⊂ Lq(Ω) one

getskukq≤Ckukand the monotonicity ofayieldsa(kukqq)≥a(Ckukq) and so

a(Ckunkq)kunk< Ckfk.

In view of limt→+∞a(tq)t= +∞one has thatkunk ≤C,∀n∈N, which contradicts

kunk=n. So, there isrm>0 such thathF(ξ), ξi ≥0, for all|ξ|=rm. In view of

the sharp angle lemma there isum ∈Vm, kumk ≤ rm such that Pi(um) = 0, i=

1, . . . , m, that is,

a kumkqq

((um, ω)) +

1

ǫ(β(um), ω) =hhf, ωii, ∀ω∈Vm. (4.4) Reasoning as before, by using the facts that t → a(t) is decreasing for t ≥ 0 , limt→+∞a(tq)t= +∞and

R

Ωβ(u)u >0 we conclude thatkumk ≤C,∀m= 1,2. . .

for some constantCthat does not depend onm. Hence,um⇀ uinH01(Ω),um→u

in Lq(Ω), 1 < q < 2N

N−2, and so kumkq → kukq. Taking limits on both sides of

equation (4.4) we conclude that the function uis a solution of problem (4.3).

Remark 4.4. The function

a(t) = 1 t2β+ 1,

whereβ andq are related by 2βq <1, satisfies the assumptions of Theorem 4.2

Proof. of Theorem 4.2

Let (ǫn)n∈Nbe a sequence of real numbers such, that

0< ǫn<1f or all n∈N and lim

n→∞ǫn= 0.

For eachn∈N, we get functionuǫnwhich satisfies Theorem 4.3. Since the estimates

were uniform onǫ and n, we can see that there exists a subsequence ofuǫn, again

calleduǫn, and a functionu∈H01(Ω)∩L

q(Ω), 1q 2N

N−2 such that

uǫn⇀ uin H01(Ω)∩H

2(Ω) (4.5)

uǫn→uinLq(Ω), 1≤q≤

2N

N−2 (4.6)

kuǫnkq → kukq (4.7)

Considerv in H1

(11)

(−a(kuǫnkpq)∆uǫn−f, v−uǫn) = (−

1

ǫβ(uǫn), v−uǫn) = 1

ǫ(β(v)−β(uǫn), v−uǫn)≥0

(4.8)

becausev∈K and monotonicity ofβ.

As in the proof of Theorem 2.1, whenǫn →0 we obtain thatusatisfies the

condi-tions of Theorem 4.2.

References

[1] C. O. Alves & F. J. S. A. Corrˆea,On existence of solutions for a class of problem involving a nonlinear operator, Communications on applied nonlinear analysis, 8(2001), N. 2, 43-56. [2] A. Arosio & S. Spagnolo,Global solution to the Cauchy problem for a nonlinear hyperbolic

equation, Nonlinear Partial Differential Equations and Their Applications, College de France Seminar, Vol. 16, H. Brezis and J. L. Lions edts., Pitman, London, 1984.

[3] C. O. Alves & D. G. de Figueiredo, Nonvariational elliptic systems via Galerkin methods, Function Spaces, Differential Operators and Nonlinear Analysis - The Hans Triebel Anniver-sary Volume, Ed. Birkhauser, Switzerland, 47-57, 2003.

[4] A. Ambrosetti, H. Brezis & G. Cerami,Combined effects of concave and convex nonlinearities in some elliptic problems, J. Funct. Anal. 122(1994), 519-543.

[5] H. BrezisAnalyse Fonctionnelle, Th´eorie et Applications, Masson, Paris (1983).

[6] M. Chipot & B. Lovat,Some remarks on nonlocal elliptic and parabolic problems, Nonlinear Analysis, T.M.A., Vol. 30, No. 7,(1997), 4619-4627.

[7] M. Chipot & J. F. Rodrigues,On a class of nonlocal nonlinear elliptic problems, Mathemat-ical Modelling and NumerMathemat-ical Analysis, Vol. 26, No. 3, 1992, 447-468.

[8] F. J. S. A. Corrˆea & S. B. de Menezes,Existence of solutions to nonlocal and singular elliptic problems via Galerkin Method, Eletronic Journal of Differential Equations, Vol. 2004(2004), No. 19, 2004, 1-10.

[9] J. G. Eisley, Nonlinear vibrations of beams and rectangular plates, Z. Anger. Math. Phys. 15,(1964)167-175.

[10] A. HarauxNonlinear Evolution Equations- Global Behaviour of Solutions, Lectures Notes in Mathematics 841, Springer Verlag, (1981).

[11] A. Hazoya & Y. YamadaOn some nonlinear wave equations II, Global existence and decay of solutions, J. Fac. Sci. (Univ. Tokio) Vol.38, No. 2 (1991) 230-250.

[12] A. N. Kludnev One-side problem connected with a weakly nonlinear parabolic operator, Siberian Math. J. 19 (1978) 412-417.

[13] N. A. LarkinThe unilateral problem for nonlocal quasilinear hyperbolic equation of the theory of elasticity, Doklady Acad. URSS, 274(6) (1984) 341-344 (in Russian).

[14] J. Limaco, L. A. Medeiros & S. B. de Menezes,Vibrations of elastic strings: Mathematical aspects, Part one, Journal of Computational Analysis and Applications, Vol. 4. N. 2,(2002)91-127.

[15] J. L. Lions,Quelques M´ethodes de r´esolution des probl´emes aux limites non lin´eaires, Dunod, Gauthier-Villars, Paris, 1969.

[16] J. L. Lions,On some questions in boundary value problems of Mathematical Physics, Con-temporary Development in Continuum Mechanics and Partial Differential Equations, Edited by G. M. de La Penha and L. A. Medeiros, North-Holland, Amsterdan (1978) 285-346. [17] L. A. Medeiros & M. Milla MirandaLocal solutions for nonlinear unilateral problems, Revue

Romaine de Math. Pures et Appliqu´ees, 31(1986) 371-382.

[18] S. I. Pohozhaev, The Kirchhoff quasilinear hyperbolic equation, Differential Equations, Vol. 21, No. 1 (1985) 101-108 (in Russian)

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(Received December 12, 2004)

Francisco Julio S. A. Corrˆea

Departamento de Matem´atica-CCEN, Universidade Federal do Par´a, 66.075-110 Bel´em Par´a Brazil

E-mail address: [email protected] Silvano D. B. Menezes

Departamento de Matem´atica-CCEN, Universidade Federal do Par´a, 66.075-110 Bel´em Par´a Brazil

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