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On Some Elliptic Problems in Unbounded Domains∗

更新时间:2016-07-05

1 Introduction

The goal of this note is to prove existence and uniqueness of solutions for some classes of elliptic problems set in unbounded domains.More precisely ifΩis an unbounded domain in R n,let

be an n × n matrix with entries a ij ∈ L(R n)for i,j=1,···,n,which satisfies the usual ellipticity condition

and

Here “·” denotes the usual Euclidean product in R n,|·|the Euclidean norm,λ and Λ some positive constants.

If f denotes some distribution onΩwe would like to consider for instance problems of the type

where is the boundary ofΩ which is split into two parts where we impose Dirichlet or Neumann boundary conditions,νdenotes the outward unit normal to∂Ωsupposed to be possibly smooth.We refer to[11,13–14]for the classical notation and results on Sobolev spaces.

It is clear thatthen,using the arguments used for for(see(2.7)),leads to

Note that we made the choice of uniformizing the constantΛappearing here and in(1.2).This can be done w.l.o.g.at the expense of choosing this constant bigger.

In a bounded domain f ∈ H−1(Ω)allows to solve(1.3)relatively easily.Unfortunately whenΩ is unbounded many simple functions fail to belong to H−1(Ω)as it is the case for the constant functions(see for instance[4,9]).Thus,in this case,some new techniques have to be developed.

These kinds of problems were attacked by the Russian school in the past decades.For instance one will find in[17],(see also[12,16]),some technique of resolution of(1.3)in the distributional sense in the case,where

with p>1,a(x)≥λ>0 under the boundary conditions below.Our approach is different and allows for instance the case

Suppose that there exists some constant that w.l.o.g.we can denote byλsuch that forℓlarge enough

Let us introduce further notation.Ifωis a bounded,convex open set of R n containing 0 forℓ>0 we denote byΩthe set

Let V denote the closed subspace of H 1(Ω)defined as

Moreover one has for some positive constants C andβindependent ofℓ

Forthe dual of Vand forℓlarge enough there exists a unique usolution to

The hydraulic natural frequency of the EHA system is

where denotes the duality bracket betweenand V.

To see this,one sets

First note that for u∈Vone has

and thus the right-hand side integral in(1.11)is well defined.It is then easy to seethat A defines a monotone operator frominto (see below).Moreover this operator is hemicontinuous and coercive.Indeed to see this last point note that for all u,u0∈Vone has

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for some δsmall enough.Note that for a ≥ 0, the norms

are equivalent in H 1(Ω)(see[2]or Section 3 below).The existence of u follows then from classical results(see[3,15]).

Set

with a≥0.In addition we establish an exponential rate of convergence of the approximate solutions to(1.3)toward u.Note that here we do not assumeΩbounded in one direction and we are not relying on the Poincaré inequality(see[4–8,10]).

We will give in Section 3 below some conditions on a for this to hold.

Then we can prove the following theorem.

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Theorem 1.1 Under the above assumptions suppose that

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for some positive constantσwhich will be chosen later on.Then there exists a unique u such that forℓlarge enough

V could be define for instance as the closure for the H 1(Ω)-norm of the space offunctions vanishing on We will suppose V equipped with the usual norm of H 1(Ω).

Remark 1.1 Note that due to the second equation of(1.18)usolves the first equation of(1.11)in the distributional sense.

2 Proof of Theorem 1.1

We first will need the following lemma.

Lemma 2.1 u is a Cauchy “sequence”.

Proof Wedo not preciseherein what space uis a Cauchy“sequence”—notethatit will be clear later on.We assume thatℓis large enough in such a way that(1.16)holds.Let r ∈ [0,1].We are going to estimate first u− uℓ+r.

Let R be such that

where B(0,R)denotes the Euclidean ball in R n with center 0 and radius R.Set forℓ1≤ ℓ−1,

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where∨stands for the maximum of two numbers and dist denotes the Euclidean distance.Clearly one has

To prove the last claim of(2.2)it is enough to show that ifthenIf not,for some y∈ωone has

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This implies by(2.1)that where z∈ ω.It follows that

by the convexity ofω.This completes the proof of the last claim of(2.2).

Since clearly using the equation of(1.10)forℓand ℓ+r we get

Using(2.2)we obtain

whereThus by(1.4),

Using again(2.2)–(2.3)and(1.16),we derive,thanks to the Young Inequality,

This can be written as

and thus for anyℓ1≤ ℓ−1 we get

where

Let us denote by[]the integer part of a number.Choosing forlarge enough and iterating the inequality above-times we get

passing to the limit inℓwe obtain the two first properties of(1.18).Next,going back to(2.13)written in replacingℓby 2ℓwe get for some other constant C

Sincethis leads to

We would like now to estimate the right-hand side of(2.7).Taking v=uin(1.10)leads to

Thus by(1.16)–(1.17)for some constant C one has

From this it follows that

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where C is independent ofℓ.Going back to(2.7)we obtain

We choose thenσsmall enough such that

to get for

for some constant C independent ofℓ.Recall that the norm in V is just the induced H 1(Ω)-norm.

The estimate above holds for any r∈[0,1].For any t>0 one deduces then by the triangular inequality

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Thus for any we see that uis a Cauchy sequence in H 1(Ωℓ0).This completes the proof of the lemma.

End of the Proof of Theorem 1.1 Let us fix ℓ0.Forℓlarge enough uis a Cauchy sequence in H 1(Ωℓ0)and thus converges toward some u ∈ Vℓ0(see(1.9)).Since by(1.10),

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Letting t→∞it comes

and thus by(2.8)

for some constant C.This completes the proof of(1.8).Passing to the limit in t in(2.13)leads to(1.19).To show now that the solution to(1.18)is unique ifis another solution one has

We make now more precise our assumptions on β —a Carathéodory function— such that for some a∈ L(Ω),a ≥ 0,a 6≡ 0,Λ >0 one has

Using the last property of(1.18)and(2.10)one deduces easily thatThis completes the proof of the theorem.

Remark 2.1 A priori u depends on the choice ofω.However whenσis chosen small enough it leads to the same solution for two differentω.Indeed suppose thatω andωare two bounded open convex subsets of R n containing 0.For some positive constant c1 one has

Suppose now R small enough in such a way that B(0,R)is included inω andω(see(2.1)).Then Theorem 1.1 is true for σ < σ0(ω)where σ0(ω)is some constant depending on ω (see(2.10)).Then choosing

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one gets solutions to(1.18)corresponding to ω,ωrespectively.Let us denote by V(ω)(respectivelythe spaces V(respectivelycorresponding toω.Due to the inclusion above one has

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and thus by(1.18)corresponding toω andωone has

Then sincefor any one deduces as above the inequality(2.19)and the equality of u andfollows.Diff erent choices ofωmight be useful for computing approximate solutions since a cube is more simple to discretise than a ball or an ellipse.Note that if(1.17)is replaced by

for some positive constantγ then the solution u obtained above is independent ofω,the third condition of(2.18)being replaced by

3 Remarks and Applications

If a(x)≥λ>0 or,more precisely,a(x)≥c>0 for a constant c that without loss of generality we can take equal toλ,then clearly it follows that(1.16)holds and thus Theorem 1.1 applies.

Note that in constructing a solution to(1.18)one can possibly consider only the ℓ’s such thatℓ∈ N.Then—this is common practice in numerical analysis—suppose thatΩcan be covered by similar triangles,rectangles,such that on each of them one has

for some constantsµ and ǫ.Then one can show(see[1])that there exists δ= δ(µ,ǫ)such that

One should notice that the third condition in(1.18)is necessary in order to be able to state an existence and uniqueness result in all generality.Indeed suppose for instance thatΩis a domain in R2 containing the strip,

Summing up on the different Q i allows to get(1.16).Such a situation arises for instance in the case of a periodic a.We refer to[4]for details.

It is clear then that(1.16)holds.To convince the reader by a more simple case suppose that on each Q=Q i coveringΩthe function a is the same up perhaps to a rigid motion.Then on each Q i one has for someδ,

Suppose in addition that

i.e.,the principal part of the operator is the usual Laplace operator.Then,since a vanishes on S,it is clear that for any n the function defined by

satisfies

where∂S denotes the boundary of S.Thus adding to a solution to(1.18)a combination of these v n’s would lead to another solution to the first part of(1.18)in such a way that uniqueness is lost—even though(1.16)could be satisfied(see above).Of course for such solutions the third property of(1.18)is not satisfied.We refer the reader to[3]for the connection betweenσand λ1.

Note that the assumption(1.6)can be relaxed at the expense of changingβ(x,u)into β(x,u)−β(x,0)and f into f−β(x,0).

In the case of f=0 Theorem 1.1 provides a Liouville type result,namely,if u is a function satisfying(1.18)with f=0 then u=0.This is clear since f=0 satisfies(1.17)and then the only solution to(1.18)is 0.

Theorem 1.1 could be extended to nonlinear operators when the operator

is replaced by an operator of the type

equipped with the ad hoc structural assumptions.

Acknowledgements The author would like to thank the referee for some constructive remarks which allow him to improve this paper.This work was performed when the author visiting the City University of Hong Kong and the USTC in Hefei.He is very greatful to these institutions for their support.This article was also written during a part time employment at the S.M.Nikolskii Mathematical Institute of RUDN University,6 Miklukho-Maklay St,Moscow,117198.

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[3]Chipot,M.,Elliptic Equations:An Introductory Course,Birkhäuser Advanced Texts,Birkhäuser,Basel,2009.

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[9]Chipot,M.and Yeressian,K.,On some variational inequalities in unbounded domains,Boll.Unione Mat.Ital.,9,2012,243–262.

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[11]Dautray,R.and Lions,J.-L.,Analyse Mathématique et Calcul Numérique Pour les Sciences et les Techniques,1,Masson,Paris,1984.

[12]Diaz,J.I.and Oleinik,O.A.,Nonlinear elliptic boundary-value problems in unbounded domain and the asymptotic behavior of its solution,C.R.Acad.Sci.Paris,315(1),1992,787–792.

[13]Evans,L.C.,Partial Differential Equations,Graduate Studies in Mathematics,19,American Mathematical Society,Providence,1998.

[14]Gilbarg,D.and Trudinger,N.S.,Elliptic Partial Differential Equations of Second Order,Springer-Verlag,Berlin,Heidelberg,New York,2001.

[15]Kinderlehrer,D.and Stampacchia,G.,An Introduction to Variational Inequalities and Their Applications,Academic Press,New York,1980.

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Michel CHIPOT
《Chinese Annals of Mathematics,Series B》2018年第3期文献

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