A NNALES DE L ’I. H. P., SECTION C
F RANÇOIS M URAT
Homogenization of renormalized solutions of elliptic equations
Annales de l’I. H. P., section C, tome 8, n
o3-4 (1991), p. 309-332
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Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques
Homogenization of renormalized solutions of elliptic equations
François MURAT
Laboratoire d’Analyse Numerique,
Tour 55-65, Universite Paris VI, 75252 Paris Cedex 05, France
Vol. 8, n° 3-4, 1991, p. 309-332. Analyse non linéaire
ABSTRACT. - We
study
in this paper thestability
of the renormalized nonlinearelliptic equation
where 03A6 : R - [RN is a continuous function which is not assumed to
satisfy
any
growth
condition. The above renormalized formulation differs from the usual weak oneby
the fact that the test functions h(u)
(p(which depend
on the solution
itself)
are used inplace
of the usual test functions cp(Q).
Consider a sequence of renormalized solutions uE relative to a fixed
right-hand
sidef,
to a fixed function d~ and to a sequence of matrices AE which converges in thehomogenization’s
sense toA°.
We prove that asubsequence
of uEweakly
converges inHo (Q)
to a renormalized solution of theequation
relative to and A°.We also consider a sequence of renormalized solutions u~ relative to a
fixed matrix
A,
to a fixed function 03A6 and to a sequence ofright-hand
sides
IE
which.weakly
convergesto 10
in H -1(SZ).
Under aspecial equi- integrability assumption on f
we prove that asubsequence
of uEweakly
Classification A.M.S. : 35 J 60.
Annales de I’Institut Henri Poincaré - Analyse linéaire - 0294-1449
converges in
Hà (Q)
to a renormalized solution of theequation
relativeto
and fO .
Key words : Homogenization, Renormalized solutions, Nonlinear elliptic equations.
RESUME. - Nous etudions dans cet article la stabilite de
1’equation elliptique
non lineaire rcnormalisee!RN est une fonction continue a
laquelle
aucunehypothese
decroissance n’est
imposee.
La formulation renormalisee ci-dessus differe de la formulation faible habituelle par le faitqu’on
y utilise des fonctionstest h
(u)
cp(qui dependent
de la solutionelle-même)
et non seulement les fonctions test habituelles cp(SZ).
Considerons une suite de solutions renormalisées ut relatives a un second membre
fixe f,
a une fonction fixée 03A6 et a une suite de matrices AEqui
converge au sens de
l’homogénéisation
vers A°. Nous demontronsqu’une
sous-suite de ut converge faiblement dans
Hà (S2)
vers une solution renor-malisee de
1’equation
relativeà f, 03A6
et A°.Nous considerons
egalement
une suite de solutions renormalisees u£relatives a une matrice fixee
A,
a une fonction et a une suite de second membresf qui
converge faiblement dans H -1(S2)
versfO.
Sousune
hypothese d’equi-integrabilite speciale
surles f~
nous montronsqu’une
sous-suite de u£ converge faiblement dans
Ho (Q)
vers une solution renor-malisee de
1’equation
relative aA, C
etf °.
To the memory of Ron DiPerna
1. INTRODUCTION
In a
joint
paper[BDGM1]
with LucioBoccardo,
Ildefonso Diaz and DanielaGiachetti,
we have considered the nonlinearelliptic problem
where Q is a bounded open subset of
I~N
withboundary
an(no
smoothnessis assumed on
aS2),
A is a coercive matrix with L~coefficients,
i. e. satisfiesfor some
0153>O;
theright-hand side f is
assumed tosatisfy
and the
nonlinearity -
div(0 (u))
is defined from a function 0 whichonly
satisfies
The main feature of this
problem
is the fact that nogrowth
condition is assumed on ~. In view of( 1. 5)
it is very natural to look for a solution uof
(1.1), (1.2)
whichonly belongs
to and not to a space of moreregular
functions. Therefore there is noground
for the measurable functionO (u)
tobelong
to(L~ (Q))N,
and to be defined in distribu- tional sense.This is the reason
why
we considered in[BDGM 1]
a weaker formulation of(1.1), (1.2):
for which we were able to prove the existence of at least one solution.
We then extended in
[BDGM2]
this existence result to the case where- div
(A grad u)
isreplaced by
aLeray-Lions
operatordefined from into its dual.
Note that each term of
(1.8)
makes sense as a distribution whenever ubelongs
toHo (Q),
since h O and h C’belong
to(C° (R)
n L~((~))N
for any h inC; (!R),
while theright
hand-side of(1.8)
read asEquation (1.8)
is obtainedformally by
apointwise multiplication
of(1.1) by
h(u)
and a convenientrewriting
of the various terms.Equation (1.8)
isactually
ageneralization
of the usual weak formulation ofequation (1.1),
since two different test functions have now to be used:the usual test function in ~
(Q)
and a new one, h(u)
with h EC; (R),
whichdepends
on the solution u itself. This isexactly
the concept of renormalized solution introducedby
Ronald DiPerna and Pierre-Louis Lions in[DL1],
[DL2]
tostudy
the Boltzmannequation.
The present paper consists of two variations on the theme introduced above: Section 2 deals with the
homogenization
of the renormalized equa- tions(1.7), (1.8),
i. e. with the case where a sequence of matrices AE is considered which is bounded in(L °°
N and satisfies( 1.4)
for somefixed a > 0. We prove that if A~
H-converges
to A°(see
the definition of this convergence inAppendix
Abelow),
asubsequence
of the sequence of the solutions of the renormalizedequations (1.8)
relative to AEweakly
converges in
Ho (Q)
to a solution of the renormalizedequation
relativeto A°. The notion of renormalized
equation
is thus robust in the sensethat it is stable under the
H-convergence
of thematrices,
which is the"weakest
possible"
convergence for thecorresponding
operators. It is also worthnoticing
that theproof
that we will present in Section 3 to prove thishomogenization
result of renormalized solutions is closed to theproof
we used in
[BDGMl], [BDGM2]
to obtain the existence of renormalized solutions. This illustrates the robustness of the method.The robustness of both the notion of renormalized solution and of the method of
proof
isemphasized by
thestability
result of renormalized solutions with respect to variations of theright-hand
side which isgiven
in Section 4: consider a sequence of renormalized solutions u£ of
(1.7), (1.8)
relative to the same matrix A and to a sequence ofright-hand
sidesf E
which convergesweakly to fO
in H -1(Q).
Under aspecial assumption
of
equi-integrability
onf
asubsequence
of the sequence uE isproved
toconverge
weakly
in to a solution of the renormalizedequation
relative to the
right
hand-sidef °.
2. STABILITY OF THE RENORMALIZED SOLUTIONS WITH RESPECT TO HOMOGENIZATION
Consider a
given
bounded open subset Q of(~N,
a fixedright-hand
sidef and
a fixednonlinearity 03A6
such thatConsider also a sequence of matrices which
satisfy
forsome a > 0 and
~3 > 0
as well as
for the definition of the
H-convergence (2.5),
see if necessary Definition A.I inAppendix
A below. Note that the matrix A° alsobelongs
to
(L °°
and satisfies(2.3)
and(2.4).
Note also that matrices AEsatisfying (2.4)
are bounded in(L°°
N since thechoice §
= AE(x)
~, in(2.4)
andCauchy
Schwartz’inequality
lead toIn view of the existence result of
[BDGMl],
Theorem1.1,
there existsat least
(*)
one solution uE of the renormalizedequation
relative toAE, f
and cp, i. e. some uE which satisfies
Moreover Theorem 1. 3 of
[BDGM1] asserts
thatThis
equality
can be obtainedformally by taking
h = 1 in(2.8),
thenmultiplying by uE, integrating
par parts, andusing
Stokes’ Theorem whichformally implies
thatnote that
although
this heuristiccomputation
is notlicit,
inparticular
since 1 does not
belong
toC~ (R)
and since there is noground
for~ (uE) grad
uE tobelong
to L1(SZ).
Nevertheless the result(2.9)
can beproved rigourously by using
some convenientapproximation
of h =1,
see[BDGM 1].
From
(2.9)
and the uniform coercivenessassumption (2.3)
we inferTHEOREM 2. 1. - Assume that
(2.1)-(2.5)
hold true and extract(*)
asubsequence
E’ such that[see (2.10)
and use Rellich’s compactnessTheorem]
(*) See the Note added in proof
The weak limit u is a solution
of
the renormalizedequation
relative toA°, , f
and cp, i. e. u
satisfies
Note that the extraction of a
subsequence
in(2.11 )
is due to the factthat we do not know if the solution of the renormalized
equation (2.12) (2.13)
isunique
or not(*).
In order to prove Theorem 2.1 let us introduce the solution zE of the linear
problem
where u is defined
by (2.11 ).
Note that in view ofhypotheses (2.3), (2.4), (2.5)
on At and of the Definition A.I ofH-convergence
we haveThe main step in the
proof
of Theorem 2.1 is thefollowing
THEOREM 2.2. -
Define
One has the strong convergence
for
thesubsequence
E’ extracted(*)
in(2.11 ).
The convergence(2.17)
takesplace
inHo (S2) (and
notonly locally
inS2)
when aSZ issufficiently
smooth. C~
3. PROOF OF THE HOMOGENIZATION RESULT
(THEOREMS
2.2 AND2.1)
The
proof
followsalong
the lines of[BDGM 1 J, [BDGM2],
and is insome sense very closed to the
proofs
used there to obtain the existence ofa renormalized solution of
( 1.7), ( 1. 8).
On the otherhand,
the idea which(*) See the Note added in proof
consists in
introducing
the solution zEequation (2.14)
and inproving
thestrong convergence
(2.17)
hasalready
been used in[B], [BeBM2].
Since Theorem 2.1 appears as a
simple
consequence of Theorem2. 2,
we
begin
with theproof
of thelatest,
which uses non linear(with
respectto
uE)
test functionsclosely
related to those used in[BeBM1] for
thestudy
of another
elliptic equation.
Proof of Theorem 2. 2
For any
positive
real numberk,
denoteby Tk : (~ -~ (~
the "truncation at theheight
k" definedby
and denote
by Sk
the"surplus"
of thistruncation,
definedby
First step. - Since
Sk
is aLipschitz-continuous, piecewise
C1(R)
func-tion such that
Sk (o) = o,
Theorem 3.1 of[BDGM 1] applies
toSk (ui
and(2.7), (2.8),
andyields
this
equality
can be obtainedformally by
an heuristiccomputation
similarto that described above to obtain
(2.9).
Defining E~
as the setwe deduce from
(3.2)
and from the uniform coerciveness(2.3)
of AE thatExtracting (*)
asubsequence
E’ such that(2.11 )
holds true, we thus have for any fixed k > 0(*) See the Note added in proof.
and since
u-Tk(u)
tends to 0 in when k tends toinfinity,
we haveproved
thatSecond
Step. -
Consider in(2.8)
the test functionwhere z£ is defined
by (2.14)
and the truncationsTi
andT~
are definedby
(3.1 ). Since u£ (x) ~ >_ l +~ implies (x) - T~ (z£ (x)) (
>_ i we haveAn alternative to Theorem 1.3 of
[BDGMl] (see
Theorem 4 of[BDGM2]
or Theorem B.I in
Appendix
Bbelow)
then asserts thatwhere
C,+~.
is the(C° (R)
n L~((F~))N
function definedby
Define
F ~
as the setSubstracting
to both hand sides of(3.8)
thequantity
and
noticing
that in view of(2.14)
we obtain
using
the uniform coerciveness(2.3)
of At:Since w~~ tends
weakly
toT~ (u - T~ (u))
in[see (2.11 ), (2.15)]
andsince tends
strongly
to inby Lebesgue’s
domi-nated convergence
Theorem,
we havein order to obtain the latest
equality
we used theidentity
03A9 03B8 (u) grad
u dx = 0 which results from Stokes’ Theorem for anypiecewise- continuous,
bounded function 03B8 : R ~ RN and any u in(see
Lemma 2.1
of [BDGM1]
ifnecessary).
Consider now the
right-hand
side of(3.10).
It isstraightforward
to pass to the limit in the first two terms and to obtainFor the last term we use the bound
(2.6)
and the coerciveness(2.3)
of AEto obtain the estimate
Since the truncations decrease the
Ho (Q)
norm we have in view of(3.7)
and
(2.10)
On the other
hand, using
first the property thatTj (s)
= 1when ~ s ( j
and0
elsewhere,
thenusing
zE - as test function in(2.14)
andpassing
to the limit in E
imply
thatCombining (3.10)-(3.15)
we haveproved
that for any fixed iand j:
Since the truncation
T~
decreases theHà (Q)
norm and since(u)
tends to 0 in
Hà (Q) when j
tends toinfinity,
thisimplies
that for any fixed iand j
Third step. - Consider a fixed measurable set K with K c Q.
[When
00 is
sufficiently smooth,
the choice K=Q becomes licit and this will prove the strong convergence of rf.’ inH5 (Q).]
From now on we willassume that
Since (x) - T J (zE (x)) ( > implies
one has
[see
the definitions(3.9)
and(3.3)
ofF ~
andE~]
Thus
In view of the results
(3.17)
and(3.6)
of two first steps of the presentproof,
the lim sup in E’ of the first and third terms of theright-hand
sideof
(3.19)
are smallwhenever j
andi - j
arelarge. Similarly (3.15) implies
that the lim sup in E of the second term of the
right-hand
side of(3.19)
issmall
when j
islarge.
Theproof
of Theorem 2.2 will thus becomplete
ifwe prove that for any fixed measurable set K with K c Q
(the
choiceK = Q
being
licit if aSZ issufficiently smooth)
we haveSince M" is bounded in L2
(H) [see (2.10)]
one has in view of the definition(3.3)
ofE~
which
implies
that themeasure I
ofE~
is smallindependently
of Ewhen k is
large. Proposition
A.4(which
is a consequence ofMeyers’
regularity theorem)
thenimplies (3.20).
Theorem 2.1 isproved.
DProof of Theorem 2.1
Since uE’ tends to u
weakly
inH5 (Q)
and almosteverywhere
in Q sinceh O and h’ C
belong
to(C° (~)
n L 00( ~))N
we haveh
(M’)
0(zt’)
-- h(u) ~ (u) weakly *
in(L 00 (Q))"
and a. e. in Q(3 22)
h’
(uE’)
C(uE’)
~ h’(M) C (u) weakly *
in(L 00 (S2))N
and a. e. inS2. (3.22)
This allows one to pass to the limit in E’ in distributional sense in the two
last terms of the left-hand side of
(2.8)
for any fixed h inC~ (R).
For what concerns the
right-hand
side we use the formulation(1.9),
i. e.f h (uE’) = -
div(h (uE’) g)
+ h’(uE’)
ggrad (3.23)
in which it is easy to pass to the limit in E’ in distributional sense since h
(uE’)
and h’(u£~)
grespectively
tend to h(u)
and h’(u)
gstrongly
in L2(SZ)
and in
(L2
Passing
to the limit in E’ for any fixed h inC; (R)
in the first two termsof
(2.8)
needs to use Theorem 2.2. For what concerns the first term of(2.8)
we haveindeed h
(uE~)
convergesstrongly
to h(u)
in L2(Q)
while AEgrad
z£ tendsweakly
toA 0 grad u
in(L2 (S~))N by
the definition ofH-convergence (see (2.15)) ;
on the other hand h(u£~)
and At arerespectively
bounded inL °° (SZ)
and in(L °°
N[see (2.6)]
whilegrad
rE~strongly
converges to 0 inby
Theorem 2.2.For what concerns the second term of
(2 . 8)
we haveindeed AE’
grad r~’ grad h (u£’)
tends to 0 in distributional sense since AE’and
grad
h(u£’)
arerespectively
bounded in(L °°
N and in(L2 (Q))N
while
grad rE’ strongly
tends to 0 in(S2))N by
Theorem2.2 ;
the conver-gence in distributional sense of AE’
grad z£’ grad
h(uE’)
to A°grad
ugrad
h(u)
is
easily
obtainedby using
cp h(u£’) [with
cp in D(SZ)]
as test function in(2.14)
and thenpassing
to the limit in E’ with thehelp
of(2.15) [from
another
standpoint
this isjust
anapplication
of thetheory
ofcompensated compactness (see [T2], [M2])
since thedivergence
of AE’grad zE’
is fixedwhile the curl of
grad
h(uE’)
isidentically zero].
In
conclusion,
wepassed
to the limit(in
distributionalsense)
in E’ forany fixed h E
C~ (R)
in each term of(2.8), obtaining
thecorresponding
terms of
(2.13).
Theproof
of Theorem 2.1 is thuscomplete.
D4. STABILITY OF THE RENORMALIZED SOLUTIONS WITH RESPECT TO THE VARIATION
OF THE RIGHT-HAND SIDE
In this Section we fix a matrix A
satisfying (1.3)
and(1.4)
and weconsider a sequence of
right-hand
sidesf satisfying
Let uf. be a solution of the renormalized
equation
associated to A andf,
i. e.
Theorem 1. 3 of
[BDGM 1]
asserts that[see
the comment after(2.9)
above for a formalproof
of thisequality].
In view of
(4.1), (4 . 4) implies
that if is bounded inH© (S~)
andextracting
a
subsequence (*)
we haveDenote
by yE
the solution ofand
by Yk
the numberTHEOREM 4. 1. - Assume that
Then u is a solution
of
the renormalizedequation
relative tofO,
~. e. usatisfies
Hypothesis (4.8)
isnothing
but to assume aspecial equi-integrability
property in
(L2 (S2))~
ongrad yE [actually
thehypothesis
thatgrad yE
isequi-integrable
in(L2 (S~))~ implies (4.8)],
i. e. aspecial
property on theright-hand sides f .
Thishypothesis
is inparticular
satisfied when theright-hand
sides are"equi-integrable
in H - ~(S~)"
and aSZ issmooth,
see Remark 4. 3 below. We do not know if the result of Theorem 4. I still holds true withoutassuming (4. 8).
The
proof
of Theorem 4 .1 issimple when f~ strongly
converges tof0
in
H -1 (SZ):
in such case it is sufficient to followalong
the lines of the(*) See the Note added in proof
proof
of the existence result of[BDGM 1] ] (proofs
of Theorems 1.1 and2.1)
to obtain theresult;
thisproof
isnothing
but theproof
ofTheorems
2 .1, 2 . 2 above,
when AE coincides with A and zE with u.When
only
the weak convergenceof f
and(4. 8)
are isassumed,
themain step in the
proof
of Theorem 4.1 is thefollowing
THEOREM 4 . 2. - Assume that
(4 .1 )-(4 . 8)
hold true. Then one has thefollowing
strong convergencefor
anyfixed
k. 0Proof of Theorem 4.1
Theorem 4.1 is
easily
deduced of Theorem 4. 2. Indeed in view of thedefinition (4 . 6) of yt
one hasand
(4. 3)
can thus be rewritten asIt is then easy to pass to the limit in E’ in distributional sense in each term of
(4.13), using (4 .11 )
for the two last terms and(4 . 5)
for the otherones. Note that we take here
advantage
of the presence of the "cut-off functions"h (ut)
and h’ in the delicate last two terms of(4 .13), using only
the strong convergence of u£~- u - yt’
to 0 "in the areawhere I ut’ I is
bounded
by
k ". DREMARK 4.3. - If
hypothesis (4. 8)
isreplaced by
the strongerhypoth-
esis
one can
actually
prove thatConvergence (4 . 15),
whichimproves (4 .11 ),
iseasily proved by
combin-ing (4.11), (4 . 14)
and the estimateThis latest estimate is obtained
by multiplying (4 . 3) by
inthe first step of the
proof
of Theorem 2. 2 above: one obtainsand one uses the
equi-integrability assumption (4.14)
since the last term/r 1/2
is controlled
by
some constantmultiplied by (|u~|~k I grad y~|2 dx)
.Note also that
hypothesis (4.14) [and
thushypothesis (4. 8)]
is satisfiedwhen aSZ is
sufficiently
smooth in order forMeyers’
Theorem to hold trueand
when f~
is"equi-integrable
in H -1(Q)",
i. e. satisfiesIndeed
denoting by
the(L2
function obtainedby applying
the
(scalar)
truncationTk
to each component ofgE, hypothesis (4.17)
isequivalent
toDecompose gE and y~
as followswhere y~k and yk
are definedby
In view of
(4.18), (4. 20)
we haveOn the other
hand, Meyers’ regularity
result(see
e. g. Theorem A. 5 inAppendix
Abelow)
ensures that for k fixedgrad yk
is bounded in(LP
for some
p > 2
and is thusequi-integrable
in(L2(Q))N. Combining
thesetwo results proves that
(4.17) implies (4.14)
when lQ issufficiently
smooth. D
Proof of Theorem 4. 2 Consider the test function
where
Tk
is the truncation at theheight k
definedby (3 .1 ).
The testfunction wE
belongs
L~(Q)
and satisfiesAn alternative to Theorem 1. 3 of
[BDGM 1] (see
Theorem 4 of[BDGM 2]
or Theorem B. 1 in
Appendix
Bbelow)
asserts that:where is the
(C°
L °" function definedby
From
(4.22)
we deduce thatNote that the first and the last terms of the
right-hand
side of(4.23)
cancel in view of the definition
(4.6)
ofy£.
On the other hand since wt’weakly
tends to inHo {S2)
it is easy to pass to the limit in thesecond,
third and fourth terms of theright-hand
side of(4.23), obtaining
In
(4.24)
the third term is zero since a. e.The second term in zero too, since
defining B)/ by
[note that B)/
is aLipschitz-continuous, piecewise {rC 1 ~~~~N function]
wehave
using
Stokes’ Theorem:Finally
the fifth term of theright
hand-side of(4.23)
is estimatedby
where
Y~
is the number definedby (4.7)
and whereCo
is a constant suchthat
(recall
that the truncation reduces theL~ norm)
Using
the coerciveness of the matrix A in theright-hand
side of(4.23)
we have thus
proved
thatFix now k and define
for j
and mlarge
the
following
inclusion holds true:Since
we have in view of
(4.28),
Since
we deduce from
(4. 29), (4. 27)
and(4. 30)
thatSince the
right
hand-side of(4 . 31 )
tends to zero when k is fixedwhile j
and m tend to
infinity,
Theorem 4. 2 isproved.
DAPPENDIX A
WHAT DO YOU NEED TO KNOW ABOUT H-CONVERGENCE IN ORDER TO READ SECTIONS 2 AND 3
Recall that in the present paper E denotes a sequence of
strictly positive
real numbers which converges to zero.
Define for a
given
bounded open subset Q of !RN(no
smoothness is assumed on and two real numbers aand P satisfying
0 a~i
the setof matrices:
This set is bounded in
(L°°
since any element of ~~(a, [i; Q)
satisfies
[see (2. 6)]
DEFINITION A . .1. - A sequence AE
of
~~(a, (3; Q)
is said toH-converge
to a matrix A°
(a, (3; Q),
and this convergence is denotedby
if
andonly if for
any g in H -1(Q)
the sequenceof
the solutions v£of
satisfies
where v° is the solution
of
The above definition was introduced
by
S.Spagnolo [S] (under
thename of
G-convergence)
in the case ofsymmetric matrices,
andby
L. Tartar
[T 1]
and F. Murat[M 1]
in the nonsymmetric
case. An extensivelitterature on the
topic
in now available: see e. g. the books of A. Bensous- san,J.-L. Lions and G.
Papanicolaou [BeLiP]
and of E. Sanchez-Palencia[Sa]
[which
deal with theimportant
case ofperiodic coefficients,
i. e. the casewhere A£
(x)
= A(x/~)
for someperiodic
matrix A defined on~N],
as wellas the survey paper of V. V.
Zhikov,
S. M.Kozlov,
O. A. Oleinik and K. T.Ngoan [ZKON];
for a summary of the basic results of H-conver- gence, andspecially
for the corrector results(a topic
which will not be discussedhere)
one can consult Section 2 of S.Brahim-Otsmane,
G. A. Francfort and F. Murat
[BrFM].
The above definition A. 1 of
H-convergence
is motivatedby
the follow-ing
compactnessresults,
due to S.Spagnolo [S]
and L. Tartar[T 1] ] (see
also
[M 1]):
THEOREM A. 2. -
Any
sequenceof
~~(a, [i; S2)
has asubsequence
whichH-converges
to an element(a, (3; SZ).
C~We
emphasize
in thisAppendix
the property of"convergence
of theenergy".
THEOREM A. 3. - Consider a
fixed right-hand
sideg E H -1 (SZ)
and asequence A£
of ~~ (a, (3; SZ)
whichH-convergence
to a matrix(a, (3; Q). Defining respectively
v£ and v to be the solutionof (A. 3)
and
(A. 5)
we haveA~
grad
v£grad 03C5~
A°grad v grad v weakly
inL1loc (SZ). (A. 6)
This convergence takes
place
in L1(Q) (and
notonly locally
inQ)
when aSZis
sufficiently
smooth. DThe fact that AE
grad vE grad vE
converges in distributional sense toA°
grad v grad v easily
results from(A. 4)
and fromintegrations by
parts in(A. 3)
and(A. 5)
aftermultiplication by
and cp v, with cp in ~(Q) [from
anotherstandpoint,
this convergence in distributional sense is thesimplest application
of thetheory
ofcompensated
compactness(see [T 2], [M 2])
since thedivergence
of A~grad vE
is fixed while the curl ofgrad 03C5~
isidentically zero].
The fact that the convergence(A. 6)
takesplace
in theweak
topology
ofLtoc (Q) (and
notonly
in distributionalsense)
isactually
an immediate consequence of the
PROPOSITION A. 4. - Let h be
fixed
in H -1(SZ)
and let w bedefined by
When A varies in (03B1,
03B2; Q) (with
0 cxfixed) the family of functions grad w
isuniformly equi-integrable
in(03A9))N,
i. e.for
anyfixed
set Kwith
|grad w|2 dx
is smallindependently of
A in(03B1, 03B2; Q)
and
of
the measurable set E whenever the measure( E is
small. The choiceK = S2 becomes licit when c3~ is
sufficiently
smooth: in such casegrad
w isuniformly equi-integrable
in(~,2 (S2)~~’.
DProposition
A. 4 results from the easy estimatesee (A . 8)
below forthe definition of
w-
here r is definedby
p~- ~
r=1
and from an
important regularity
result due to N. G.Meyers [Me] (see
also
[BeLiP], Chapter l,
Section25);
a local version of this result can be stated as follows.THEOREM A . 5
(N.
G.Meyers). -
For any measurable set K with K ~ 03A9 there exists some numberp > 2
and some constant C(which only depend
onQ, K,
oc and~}
such thatfor
any h inw - ~ ~
F(Q)
and any A in ~~~3; Q)
the solution w
of
belongs
to P(K)
andsatisfies
The choice K = 03A9 becomes licit when aSZ is
sufficiently
smooth. DAPPENDIX B
USING SPECIAL TEST FUNCTIONS IN RENORMALIZED
EQUATIONS
The
following
Theorem is in some sense an alternative to Theorem 1.3 of[BDGM 1] ] (see
also Theorem 4 of[BDGM 2]).
THEOREM B .1. - Assume
that (1.3)-(1. 6)
hold true. Consider a solutionu
of
the renormalizedequation (1 . 7), (1 8j
and afunction w
whichsatisfies
The
following equality
then holds:where is the "truncation at the
height
k "defined by (3 . .1).
[]Note
that 03A6Tk belongs
to is anelement of
(L 00
and each term of(B. 2)
makes sense.Proof of Theorem B. 1
This
proof
is a variation of theproof
of Theorem 1.3 of[BDGM 1].
First step. -
Equation (1.8)
is understood in distributional sense.Consider however a test function w which
belongs
Using
a sequence of functions which converges to w in~o (Q)
and remains bounded in
L°° {~2j,
it can beeasily proved
that if u is asolution
pf
the renormalizedequation (1.7), (1.8),
thenfor any w in
I~,~ (Q)
U L°°(Q)
and any h in Note that each term makes sense in(B. 3).
Second step. - Assume first that further to
hypothesis (B . I),
w alsobelongs
to L 00(Q).
Consider a function H in
~~ ~~~
such thatand
define 1~,~ (s) by
Since w
belongs
toand hn
to we have in view of(B.3)
/* -
It is easy to pass to the limit in each term of
(B. 5)
when n tends toinfinity, mostly using Legesgue’s
dominated convergence Theorem: in the thirdcan
bereplaced [which belongs
to(L °°
in view of
hypothesis (B .1 );
the fourth term is zero whenevern _>_ k,
sincedefining
which
belongs
to(C 1 ((~)
n °°(~))N,
we haveusing
Stokes’ Theorem and thenhypothesis (B .1 )
combined with the fact that(s)
= 0 when(u)grad
w dx = 0.This proves that
tor any w in L 00
(Q) satisfying (B . 1).
Third step. - Consider now the
general
case where wsatisfying (B. 1)
is not assumed to
belong
toL°° (SZ).
The function wm= Tm (w)
obtainedby
the truncation of w to theheight m
is an admissible test function in(B . 6).
It is now easy to pass to the limit with mtending
toinfinity, recovering (B. 2).
DACKNOWLEDGEMENTS
It is a
pleasure
for me to thank Lucio Boccardo and Pierre-Louis Lions for many veryinteresting
and fruitful discussionsconcerning
this workand renormalized solutions in
general.
In a forthcoming joint paper with Pierre-Louis Lions we will prove that the renormalized solution of (1. 7), (1. 8) is unique if (p is assumed to be locally Lipschitz-continuous and if a zero order term with ~, > 0 is added to the left-hand side of (1 . 8). In such a setting
the extraction of a sub-sequence E’ in the statements of Theorems 2 . and 2 . 2 [respectively
in (4.5) and in the statement of Theorem 4 . 2] becomes unnecessary, since this uniqueness
result of the renormalized solution of (2. 7), (2 . 8) [respectively of (4. 9), (4.10)] implies the
convergences for the whole sequence E.
REFERENCES
[BeBM 1] A. BENSOUSSAN, L. BOCCARDO and F. MURAT, On a Nonlinear Partial Differen- tial Equation Having Natural Growth Terms and Unbounded Solution, Ann.
Inst. Henri Poincaré, Analyse non linéaire, Vol. 5, 1988, pp. 347-364.
[BeBM 2] A. BENSOUSSAN, L. BOCCARDO and F. MURAT, H-Convergence for Quasilinear Elliptic Equations with Quadratic Growth, (to appear).
[BeLiP] A. BENSOUSSAN, J.-L. LIONS and G. PAPANICOLAOU, Asymptotic Analysis for
Periodic Structures, North-Holland, Amsterdam, 1978.
[B] L. BOCCARDO, Homogénéisation pour une classe d’équations fortement non linéaires, C. R. Acad. Sci. Paris, T 306, Serie I, 1988, pp. 253-256.
[BDGM 1] L. BOCCARDO, J. I. DIAZ, D. GIACHETTI and F. MURAT, Existence of a Solution for a Weaker Form of a Nonlinear Elliptic Equation, in Recent Advances in Nonlinear Elliptic and Parabolic Problems, Proceedings, Nancy, 1988,
P. BENILAN, M. CHIPOT, L. C. EVANS and M. PIERRE Eds., Pitman Res. Notes in Math., Vol. 208, Longman, Harlow, 1989, pp. 229-246.
[BDGM 2] L. BOCCARDO, J. I. DIAZ, D. GIACHETTI and F. MURAT, Existence and Regularity
of a Renormalized Solution for Some Elliptic Problem Involving Derivatives of Nonlinear Terms, (to appear).
[BrFM] S. BRAHIM-OTSMANE, G. A. FRANCFORT and F. MURAT, Correctors for the
Homogenization of the Wave and Heat Equations, J. Math. pures et appl., (to appear).
[DL 1] R. J. DIPERNA and P.-L. LIONS, On the Cauchy Problem for Boltzmann Equa-
tion : Global Existence and Weak Stability, Annals of Math., Vol. 130, 1989,
pp. 321-366.
[DL2] R. J. DIPERNA and P.-L. LIONS, On the Fokker-Planck-Boltzmann Equation,
Comm. Math. Phys., Vol. 120, 1988, pp. 1-23.
[Me] N. G. MEYERS, An Lp-Estimate for the Gradient of Solutions of Second Order
Elliptic Divergence Equations, Ann. Sc. Norm. Sup. Pisa, Vol. 17, 1963, pp. 183- 206.
[M1] F. MURAT, H-convergence, Séminaire d’analyse fonctionnelle et numérique, Univer- sité d’Alger, 1977-1978, multigraphed.
[M 2] F. MURAT, A Survey on Compensated Compactness, in Contributions to Modern Calculus of Variations, L. CESARI Ed., Pitman Res. Notes in Math., Vol. 148, Longman, Harlow, 1987, pp. 145-183.
[Sa] E. SANCHEZ-PALENCIA, Non Homogeneous Media and Vibration Theory, Lecture
Notes in Phys., Vol. 127, Springer-Verlag, Berlin, 1980.
[S] S. SPAGNOLO, Sulla convergenza di soluzioni di equazioni paraboliche ed ellitiche,
Ann. Sc. Norm. Sup. Pisa, Vol. 22, 1968, pp. 577-597.
[T 1] L. TARTAR, Cours Peccot, Collège de France, 1977.
[T 2] L. TARTAR, Compensated Compactness and Applications to Partial Differential
Equations, in Nonlinear Analysis and Mechanics, Heriot-Watt Symposium
Volume IV, R. J. KNOPS Ed., Res. Notes in Math., Vol. 39, Pitman, London, 1979, pp. 136-212.
[ZKON] V. V. ZHIKOV, S. M. KOZLOV, O. A. OLEINIK and K. T. NGOAN, Averaging and G-Convergence of Differential Operators, Russian Math. Surveys, Vol. 34, 1979,
pp. 39-147.
( Manuscript received November 1989.)