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A NNALES DE LA FACULTÉ DES SCIENCES DE T OULOUSE

A NDRÉE D ECARREAU J IN L IANG

J EAN -M ICHEL R AKOTOSON

Trace imbeddings for T -sets and application to Neumann-Dirichlet problems with measures included in the boundary data

Annales de la faculté des sciences de Toulouse 6

e

série, tome 5, n

o

3 (1996), p. 443-470

<http://www.numdam.org/item?id=AFST_1996_6_5_3_443_0>

© Université Paul Sabatier, 1996, tous droits réservés.

L’accès aux archives de la revue « Annales de la faculté des sciences de Toulouse » (http://picard.ups-tlse.fr/~annales/) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions).

Toute utilisation commerciale ou impression systématique est constitu- tive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright.

Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques

http://www.numdam.org/

(2)

- 443 -

Trace imbeddings for T-sets

and application to Neumann2014Dirichlet problems

with

measures

included in the boundary data(*)

ANDRÉE DECARREAU(1),

JIN

LIANG(2)

and JEAN-MICHEL

RAKOTOSON(1)

Annales de la Faculté des Sciences de Toulouse Vol. V, n° 3, 1996

R,ESUIVtE. - Dans cet article, on etudie l’existence de solutions pour

un probleme quasi-linéraire elliptique a donnees mesures y compris sur la frontiere et on montre l’unicité de solutions lorsque ces donnees sont dans L 1.

ABSTRACT. - In this paper, we investigate in the existence and unique-

ness of a quasilinear elliptic problem with measure data included in the free terms both of equation and boundary. We study first some Sobolev- type imbeddings for T-sets and we use the notion of renormalized solution for having uniqueness. .

0. Introduction

Dirichlet

problems

with measures as data have been

widely

studied

recently by

various

authors,

for instance

[BG], [BGV], [BS], [BCP], [GV], [Ral]-[Ra6], [Lia], [LM], [At].

Most of them concern the

homogeneous boundary

Dirichlet condition

except

in

[GV],

where a semilinear

equation

is studied with a measure as a

boundary

condition. In this paper, we will discuss a kind of more

general

mixed

boundary

condition.

~ * ~ Recu le 26 mai 1994

(1) Departement de Mathematiques, Université de Poitiers, 40, avenue du Recteur-

Pineau, F-86000 Poitiers

(France)

(2) Department of mathematics and statistics, University of Edinburgh, King’s build- ing, Edinburgh EH9 3JZ, UK

(United Kingdom)

(3)

More

precisely,

consider the

following problem:

where a is a

Caratheodory

function defined in H x R x

II~~,

H is a smooth

bounded open set B is defined on ~SZ = F =

Fo

U

Fi formally by

Bu = u on

Fo

and Bu = a

~ n

on

I‘1,

~a and ~b

equal

to 0 or

1,

p E

] 1,

cx~

~, s

will be

precised later, n

is the outer normal to

r 1, M(Q) (resp. M(F))

is the set of bounded Radon measures on S2

(resp. F).

We

assume v = 0 on

Fo.

The function â is

required

to

satisfy

the standard

Leray-Lions

assump-

tions :

(A2) for a.e. x ~ 03A9, for all u ~ R, all 03BE ~ RN

where C is a

positive constant,

7

p))

and

(A3) for a.e.

As a

model,

we can condiser

(4)

If Ea =

0,

there is

generally

no solution for

problem (P) ;

for this reason,

we need a

compatibility

condition

involving

the measures p and v, that is + = 0.

The

problem (P)

does not possess solutions in the usual Sobolev spaces:

one can

verify

that fact on the fundamental

equation.

For this reason, as in

[BBGGVP], [RA2]

and

[RA3],

we introduce some

convenient functional sets in which we search weak solutions

(sects

1 and

2).

In the first

time,

we

interpret

in the distribution sense, but as

pointed

out

by

a

counter-example given by

Serrin

[Se],

the weak solution

given

in that

sense is not

unique.

This lack of

uniqueness

is

widely explained

in

[Ra6].

Another notion of weak solution is then useful to ensure the

uniqueness

of

solutions. When the

data p

and v are in

L1,

we can borrow the notion of

renormalized solution of Di Perna-Lions and

adapt

it to our case. As it is

shown in

[Ra6], when

and v are

smooth,

say in

Lp’ (Q),

then this notion of renormalized solution is

completely equivalent

to the notion of classic weak solution.

For

proving

the existence of a weak

solution,

we consider a

family

of

approximating problems, and, by compacity arguments,

we construct a solution u. This function u is also a renormalized solution

(when

and

v are and we prove

uniqueness

result in this case

by comparing

an

arbitrary

renormalized solution w with the solution u mentioned above

(see [Ra6]

for Dirichlet

equations).

An

uniqueness

result is also

given

in

[BBGGVP]

under less

general

conditions than ours and technics are

completely different,

for instance

they

compare

directly

two

arbitrary

solutions.

Recently,

Xu

[X]

borrows the same ideas as in

[BBGGVP], [Ral]

and

[Ra2]

to show the existence of solution for a

multivoque problem.

There is

no

uniqueness

result in this paper and the data are in

L1.

We will

distinguish

in the

proofs

the mixed

problems corresponding

to

the case of > 0 is the N - 1 dimensional Hausdorf

measure of

Fo)

and the Neumann

problems corresponding

to the case of

= 0. We

give

a sense for the traces of the founded weak solution

by using

truncations.

(5)

1. Functional

sets ;

T-sets

Let S2 be a smooth bounded open connected set of

N > 2,

p

E ~

80 = r -

ho U r1, Fo

and

Fi disjoints.

We introduce

the

following

sets:

Here

L~(H) (resp.

and is called T-set

(resp. T-subset).

We note that

C~(H)

G

and,

in the case of =

0,

the

spaces

C~(~)

and are the classical spaces and and the T-set and T-subset are

simply

denoted

by

and

These spaces and sets possess similar

properties

as Sobolev spaces. The first lemma concerns the

derivability

result.

LEMMA 1.1.2014

If v

E exists almost

everywhere and for

For the

proof

see

[Ra3]

or

[At].

(6)

LEMMA 1.2. - C

L~(n).

The

proof

is easy.

The two lemmas below are fundamental:

they

concern trace results

in the

T-spaces

and

provide inequalities

for estimations in section 3 and convergence results in section 4. We introduce four constants defined with PC

]1,~V]:

LEMMA 1.3. - For r E

] 0,

rc

~

and

r’

E

] 0, r~ ~ satisfying r(N

-

1)

=

r’N,

there exists a constant

C, depending only

on S2 and r, such that

for

all

u E n

u(x)

makes sense

for

a. e. x E

F,

and we have with

T =

~p

- =

~p~

-

r~ ~ ~~~

:

Moreover, if u

E and

for

any T E

] 1/p 1 [,

Proof.

- Consider

4Y(t)

=

J) da/ (i

+ Let u E n

(Q),

by

definition

V(u*’)

e c

LP(Q) ,

for all k > 0 we

write,

(7)

We arise this

equality

to the power

p

and

integrate

over

Q,

we

get

Thus we obtain:

by

the usual Sobolev

inequality applied

to

~(u~~,

we deduce:

Since

~(u~) ~

we then have

Similarly, by

the trace

imbedding

theorem on usual Sobolev spaces,

applied

to the function

u~

= we have:

(8)

(C

is

independent

of

l~)

. For x E

F,

=

u ~x) + ~ - ~c ~~) ~’ : thus,

it has

a limit

in -oo , -~-oo ~,

when k go to

infinity;

we denote this limit

by By

Fatou’s lemma and

Lebesgue

dominated convergence, when

letting k

go to

infinity,

we obtain the

inequality (1).

For the last

inequality,

let u E with the condition

From usual Sobolev

imbedding theorem, applied

to

~(u~),

we can obtain:

(C

is

independent

of

k)

and

noticing

that

thus

arguing

as for the

inequality (1)

and

using

the above

inequality,

we

derive the

inequality (2) . ~

Remark. - The existence of a trace function can also be derived

by showing

that u is

p-quasicontinuous

in Q.

LEMMA 1.4. For all q E

~ 1 , N/(N - 1) ~,

there exists r E

~ 0 , rc[,

,

there exists a constant C such that

for

all u E

(9)

Proof.

- Choose t =

q(p

-

1 )

and b > 0 small

enough,

then

with r =

t(1

+

8)/(p - t)

re. 0

The

proof

is the same as in

[Ra3].

.

2. Weak solutions and renormalized solutions.

Main results

For p E

] 1, oo [

we set

(N - 1)(p - 1)/(N - p)

if 1 p N.

We want to solve the

following problem:

find u in an

appropriate

T-set

satisfying:

B is defined on F =

Fo

U

Fi formally by

Bu = u on

Fo,

Bu = a ’

~ n

+

u on = 0 on

Fo,

~~

and Eb equal

to 0 or

1, s

sc.

The above

problem

has to be understood in a

precise

sense, this is

why

we introduce a few definitions

(see below).

The first one is available for

general

measure and the second one is true for

integrable

function. We will

see that one can

get

an

uniqueness

result for renormalized solution.

(10)

DEFINITION 2.1. - We will say u is a weak solution

of

the

problem (P) if

u E and

for

any v E there holds:

DEFINITION 2.2.- lel p E and v E we will say that

u e

fl%§"

is a renormalized solution

if: for

any v e

Wj§"(Q)

n

L°(Q), for

T E

W1,~compact(R),

there holds:

The main results in this paper are stated in Theorem 1 below and Theorems 2 and 3 in section 7: Theorem 1 concerns an existence result and the others concern

uniqueness

results.

THEOREM 1.2014

Let

E

M(n)

and v E

M(F). If p

E

] 1, N]

and

s E

~ 0 , [ if p N,

under the

assumptions

to

~A3~,

there exists

at least a weak solution u

of problem (P). (HN-1(03930)

= 0 in the case

Ea = Eb =

0,

and v = 0 on

I‘o if

>

0~.

Futhermore, if

u E and v E this weak solution is a

renormalized solution.

The

proof

will be divided in two cases

according

to the values of ~~ and

6~: The first one is the case

when Ea

or Eb = 0 which will include three subcases

(that

is Ea = Eb =

1,

~~ = 1 - Eb =

1,

Ea =

1 - Eb

=

0).

But since

the discussions of them are

similar, we just

consider the case

And the other case that we will discuss is Ea = Eb = 0.

The first

step

consists in

considerating

an

approximating problem.

We

will make some uniform a

priori

estimates

compatible

to the structure of

T-set that we consider.

Using

some

compactness

results similar to those

produced

in

[Ral]-[Ra3],

we pass to the limit.

(11)

3. An

Approximating problem

of

problem

in the case Ea = t b = 1 We will consider an

approximating problem

of

problem (P)

in the

following

manner.

Let n E E n = 0 on

Fo satisfying:

for

any 03A6

E

(set

of continuous

functions)

and for all n,

With the

assumptions

of Theorem

1,

there exists a weak solution r~, E of

problem (Pn )

below and the

proof

can be found in

[LL].

Uniform estimates for the sequence u,n

(i)

We prove first that the sequence un lies in a bounded subset of and a bounded subset of

We take v = > 0 in

(6)

where

after

dropping

the

positive

terms in the first member and

letting

r~ -~

0,

we obtain:

(12)

(ii)

Let T E we shall prove that the sequence

D(T(un))

lies

in a bounded subset of

LP(Q) oo):

for

this,

we take

v* - dO’ in

(6)

and we obtain

(because II v* II L~ (~~

where C is

independent

of n.

Thus

T(un)

remains in a bounded set of

(iii)

Now take

as a test function in

(6),

we obtain:

where C is

independent

of nand k.

(iv)

We

apply

Lemma 1.3 to un and we have for any r and

r’ verifying 0~r~,

(using

the

previous

estimate and

noticing

that pT >

1),

where C is

independent

of n.

Nloreover, using

Lemma 1.4 and the above estimate

for q

E

~ 1 , ~~~~ - 1) ~ ~

where C is

independent

of n.

(13)

4. The limit process.

Existence of a weak solution in the case Ea = ~.b = 1 Let us choose =

arctan(t)

E Set wn =

remains in a bounded set of

By (ii)

in section

3,

and the usual

compactness

on Sobolev

Spaces

there exists a

subsequence

still denoted wn which verifies:

We introduce u =

tan(w),

then we have

For T E the sequence

T(un)

lies in a bounded subset of

thus we have

T (u)

E From the

previous

estimates on un , we see

that u

belongs

to

We can use v =

S",(un -

E as a test function in

(6),

where

to

obtain,

as in

[Ra2]-[Ra3],

and then

We want to show the

following

result on the trace of u on F: u exists a.e.

on r and un ~ u on F when n ~ oo.

For any

integer k

>

0,

we have

u~

E

uniformly

with

respect

to n.

So

un -~ u~,

in

weakly.

Thus

by

trace lemma - 0

{as n -~ oo).

Then there exists

Ek

such that = 0 and

exists on

F B Ek. Now,

for any x E

I‘ ~ E~,

exists for all

l~,

then

(14)

letting k

= oo as in Lemma

1.3,

we have that has a limit a.e. on r denoted

by u( x) E ~ -oo , +00].

To show that

u(x)

is

finite,

we remark that

with C

independent on n and k,

so that

C,

and

consequently

+00.

Futhermore,

we have

We

decompose

F in three subsets: F = U

r!3n

U with

and,

E

]0, s [,

we consider

dHN_1:

and

(15)

and we have

proved

that

The estimates

(7), (8)

and

(9)

show that there exist r and

~~, p-1

r ~~,

s

r’ r~

= sc so that u E Du e

L’’ (SZ),

u E and

then with Vitali’s lemma we deduce from the

previous pointwise

convergence

that ,

We

finally

can pass to the limit in

(6)

and obtain that u is a weak solution of

problem (P). 0

5. An

approximating problem

in the case éa = 0

In this section =

0,

we consider the

problem (P)

when

éa = 0 under the

supplementary following compatibility

condition:

We define the sequences

and 1/n

as in section

3,

but

and vn

must

satisfy

an additional condition:

We will

distinguish

the cases p >

2N/(N

+

2)

and

p 2N/(N

+

2).

(16)

First case, p > +

2)

We consider the

approximating problem

below.

Find un E

verifying f

un d.r =

0,

and for all v E

There is a solution u~, E n for this

problem (see [LL]

for

the existence and

[RT]

for

L~-estimates).

We have for un the

following

estimates obtained with the same test functions as in section

3,

that is:

where is

independent

of n;

with C

independent

of n.

But we cannot use Lemma 1.3 for un ; we introduce another function un

by noticing that,

for all T 1 there exists

cn

such that

We fix

Note that

and Lemma 1.3 can be

applied

to Un with r =

(1 - T)Np/(N - p) (> 1).

.

Exactly:

with C

independent

of n

(choose v

= in

( 10) ) .

So

~

C with C

independent

of n and then

03A9 |un (’’

dx C.

(17)

Using

Lemma 1.4 for un we have the

following inequality

with

with C

independent

of n.

We introduce u as in section 4. We can

apply

Vitali’s lemma when n -~ o0

(note

that r >

cr)

to prove that un,

a(x,

u,

Du)

and that u is a

weak solution of

problem (P).

Second case,

p 2N/(N

+

2)

We assume here that â does no

depend explicitely

on un; we note

â(x, Dun)

and we consider the

following problem,

after

fixing

a real

Find un E

verifying f~

d.r =

0,

and for all v E

There exists a solution u~ E

verifying (10bis):

for

proving

this we

apply

the

Leray-Lions

theorem

[LL]

and L°°-estimates results

[RT] ;

we find a function wn E n such that

~’~

wn d.r =

0,

and for

all v E

As in the first case, there exists

cn

such that

~’~

+

c~)

dx = 0. .

So,

un = wn +

c~

verifies

( lobis),

and we derive the estimates below:

where is

independent

of n;

(18)

with C

independent

of n;

with C

independent

of n.

We conclude as in the first case and find a weak solution u for the

problem (P). 0

6. End of the

proof

of Theorem 1

u is also a renormalized solution when ~c and v are in

L 1.

Here p

and v are

respectively

in and We use the sequences un defined in sections 3 and 5 and u the

corresponding

weak solution.

We

give

additional

properties

to prove

(5)

for v E n and

T ~ W1,~compact(R).

LEMMA 6.1.2014 The sequences un introduced in

(6)

and

(10) verify:

Proof.

- Case ~a = ~b = l. First we take v =

un +1 -

as a test

function in

(6)

and we obtain:

(19)

and

consequently, using

the

properties

of the sequence un and Fatous’s

lemma,

Then let m tend to

infinity, using

the dominated convergence theorem

we

get (11).

Case 6;a = 0. For the sequence defined in section

5, taking

v = as a test function in

(10)

or

(lObis),

we obtain:

and for m -~ oo we

get (11).

~

COROLLARY OF LEMMA 6.1. - Let

hm

be the continuous

function

de-

fined

on II~

by:

then

for

any v E n

for

any T E

(20)

Proof

with

hypothesis (A2);

futhermore

I T(u)vI

is bounded with

M,

the

support

of T is

compact,

ao is in

L~~ (SZ),

then

(21)

where C is

independent of n,

We conclude with Lemma 6.1. D

We now prove that u is a renormalized solution of

problem (P).

. First we consider the case Ea = 1. For v C n T C

and m e N ,

we take

hm(um)T(u)v

as a test function in

(6) :

First,

when n -~ o0

The five terms in the second member have a limit and then:

(22)

Secondly,

when m -~ o0

For m,

large enough (say supp T

C

[-m,

m

]),

we can write

The

corollary

of Lemma 6.1 and the dominated convergence theorem

permit

to conclude that u verifies

(5).

. In the case of ~o = Eb = 0 and u~ Is the sequence defined in section

5,

the

proof

is similar.

7.

Uniqueness

result

We have seen that there exists at least one function u G

being

a renormalized solution in the sense of definition 2.2.

Futhermore,

this

solution is a limit of a smooth sequence i~

being

a classical solution of an

approximate problem.

We want to show some

uniqueness result ;

we

begin by

a

"simple"

case.

THEOREM 2.- Assume that

(x,~,03BE)

is

independent of ~ (we

note

(x,03BE)),

then there exists a

unique

renormalized solution w G up to

a constant

if ~a

= Eb = 0

verifying for

e n

for

any

T ~

Proof.

- It remains to show the

uniqueness

of the

solution;

let us call w

an

arbitrary

solution of the

preceding problem;

we

keep

the notation u for the

particular

solution

being

a limit of sequence un

(that

we found

before).

The aim is to show that w = u.

(23)

Let and consider as in section

6;

the function

can be used as a test function in

(6)

or

( 10)

or

(10bis),

that is

But we have also

(5)

for u = w with T =

hm

and v =

that is

Let us make the difference between the two last

equations;

we

get:

(24)

The third ans fourth terms of the left hand-side are

non-negative;

when

dropping

those

terms,

we

get:

. In a first

time, letting

m go to

infinity (n

and k

being fixed),

we have the

two

inequalities:

and,

with the fact w E it comes:

.

Now, k being fixed,

we let n -~ oo; Fatous’s lemma and the

monotony

of a

(condition A3)

lead to:

.

Finally,

we let k --~ oo and we

have, using Beppo

Levi

theorem,

(25)

Consequently

Dw =

Du,

then

Dwk

=

Duk

for that is and

uk

differ from a constant

Ck ;

these constants are

uniformly

bounded because

u~

and

w~

are in a bounded subset of so a

subsequence

of

(Ck)

converges to a constant

C,

and we conclude w = u + C.

We prove that C = 0 if ~

~

0: if

0,

without

dropping

the

positive

terms in

(12)

and

using

Fatou’s

lemma,

we deduce:

and,

when k --~ oo,

for the same reason, and then- C = 0. D

Now consider the

general

case for

a,

that is r~,

~) depends

of r~, for

problem (P)

with ~a = ~b = 1.

If a satisfies the

supplementary

condition:

(A4)

for a.e. x E

Q,

for

all /

for all r~1 and r~2

in -h , -i-h ~

C I~B:

~T1~ ~) - ~12~ ~)I C

+

where

C(h)

is a constant

depending only

of

h,

and

bo

E

L~~ (S~),

then we have an

uniqueness

result for the mixed

problem.

THEOREM 3. - Assume a

satis fies

the

hypothesis

to

(Al~~.

There

exists a

unique

renormalized solution E

verifying for

any v E

for

any T E "

(26)

Proof.

- As in the

proof

of Theorem 2 we call w an

abritrary

solution

of

(13)

and compare w and u

(the

solution founded in section

4).

We

introduce, for q

e

] 0 , 1 [ the

function

F~

defined from R to R

by:

Then, for m ~ N, k ~ N, ~ ~ ]0,1[,

we take v =

as a test function in

(6);

we have also

(13)

with T =

hm

and v =

we take the difference between the two

corresponding equations

and we obtain:

We consider

separately

all these terms

(four

in the first left hand-side and two in the

right hand-side)

and let

successively m -~ oo, r~ -.~ 0, n ~ oo,

The fourth term of the left hand-side of

(14)

is

non-negative;

we

drop

it.

The two terms in the second member are

respectively

bounded

by

The first term is

decomposed

in two

parts, using

(27)

we use the

hypothesis (A2)

and

(A4)

on

â,

it comes

which is less than

where C =

hy-

pothesis (A4)

is uded with h = 1~ +

Now,

let m go to

infinity (r~, n , k fixed) ;

we

get

the

following

convergences:

has a limit which is

non-negative (A3),

,. _

(28)

In a second

step,

r~ --~ oo:

In a third

step

n -~ oo and

finally k

-~ oo,

We can conclude that

(z,c~ - u)+

= 0.

By

an

analogous

manner we prove that

(u - w)+

=

0,

and the Theorem 3 is

proved. D

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