NONLINEAR PROBLEMS IN ORLICZ SPACES
A. BENKIRANE AND J. BENNOUNA Received 20 October 2001
We study in the framework of Orlicz Sobolev spacesW01LM(Ω), the existence of entropic solutions to the nonlinear elliptic problems:−diva(x,u,∇u) + divφ(u)
=f inΩ, for the case where the second member of the equation f ∈L1(Ω), and φ∈(C0(R))N.
1. Introduction
Let Ωbe a bounded open subset ofRN and let A(u)=−diva(x,u,∇u) be a Leray-Lions operator defined onW01,p(Ω), 1< p <∞.
We consider the nonlinear elliptic problem
−diva(x,u,∇u)=f−divφ(u) inΩ,
u=0 on∂Ω, (1.1)
where
f ∈L1(Ω), φ∈
C0(R)N. (1.2)
Note that no growth hypothesis is assumed on the function φ, which implies that the term divφ(u) may be meaningless, even as a distribution. The notion of entropy solution, used in [8], allows us to give a meaning to a possible solution of (1.1).
In fact Boccardo proved in [8], forpsuch that 2−1/N < p < N, the existence and regularity of an entropy solutionuof problem (1.1), that is,
u∈W01,q(Ω), q <p˜=(p−1)N N−1 , Tk(u)∈W01,p(Ω), ∀k >0,
Copyright©2002 Hindawi Publishing Corporation Abstract and Applied Analysis 7:2 (2002) 85–102 2000 Mathematics Subject Classification: 35J60 URL:http://dx.doi.org/10.1155/S1085337502000751
Ωa(x,u,∇u)∇Tk[u−ϕ]dx≤
Ωf Tk[u−ϕ]dx+
Ωφ(u)∇Tk[u−ϕ]dx
∀ϕ∈W01,p(Ω)∩L∞(Ω), (1.3) where
Tk(s)=s if|s| ≤k Tk(s)=k s
|s| if|s|> k. (1.4) For the caseφ=0 and f is a bounded measure, B´enilan et al. proved in [3] the existence and uniqueness of entropy solutions.
We mention as a parallel development, the work of Lions and Murat [14]
who consider similar problems in the context of the renormalized solutions in- troduced by Diperna and Lions [10] for the study of the Boltzmann equations.
They can prove existence and uniqueness of renormalized solution.
The functional setting in these works is that of the usual Sobolev spaceW1,p. Accordingly, the functionais supposed to satisfy polynomial growth conditions with respect touand its derivatives∇u. When trying to generalize the growth condition ona, one is led to replaceW1,pby a Sobolev spaceW1LM built from an Orlicz spaceLM instead ofLp. Here theN-functionM which definesLM is related to the actual growth of the functiona.
It is our purpose, in this paper, to prove the existence of entropy solution for problem (1.1) in the setting of the Orlicz Sobolev spaceW01LM(Ω). Our result, Theorem 3.5, generalizes [8, Theorem 2.1] and gives in particular a refinement of his result (seeRemark 3.6).
For some existence results for strongly nonlinear elliptic equations in Orlicz spaces [4,5,6].
2. Preliminaries
2.1. LetM:R+→R+be anN-function, that is,Mis continuous, convex, with M(t)>0 fort >0,M(t)/t→0 ast→0 andM(t)/t→ ∞ast→ ∞.
Equivalently, M admits the representation M(t) = t
0a(τ)dτ, where a : R+→R+is nondecreasing, right continuous, witha(0)=0,a(t)>0 fort >0 anda(t)→ ∞ast→ ∞.
In the following, we assume, for convenience, that allN-functions are twice continuously differentiable, see Benkirane and Gossez [7].
TheN-function ¯M conjugate to M is defined by ¯M(t)=t
0a(τ)dτ, where¯ a¯:R+→R+is given by ¯a(t)=sup{s:a(s)≤t}, see [1,13].
TheN-functionMis said to satisfy the∆2-condition (resp., near infinity) if for somekand for everyt≥0,
M(2t)≤kM(t) resp., fort≥somet0
. (2.1)
Let M and P be twoN-functions. The notationP M means thatP grows essentially less rapidly thanM, that is, for each>0,P(t)/M(t)→0 ast→ ∞. This is the case if and only if limt→∞M−1(t)/P−1(t)=0. We will extend allN- functions into even functions on allR.
2.2. LetΩbe an open subset ofRN. The Orlicz classKM(Ω) (resp., the Orlicz spaceLM(Ω)) is defined as the set of (equivalence classes of) real-valued mea- surable functionsuonΩsuch that
ΩMu(x)dx <∞ (2.2)
(resp.,ΩM(u(x)/λ)dx <∞for someλ >0). The spaceLM(Ω) is a Banach space under the norm
uM=inf
λ >0 :
ΩM u(x)
λ
dx≤1
(2.3) and KM(Ω) is a convex subset ofLM(Ω). The closure in LM(Ω) of the set of bounded measurable functions with compact support in ¯Ωis denoted byEM(Ω).
The equalityEM(Ω)=LM(Ω) holds if and only ifMsatisfies the∆2condition, for alltor fortlarge according to whetherΩhas infinity measure or not.
The dual ofEM(Ω) can be identified withLM¯(Ω) by means of the pairing
Ωu(x)v(x)dx, and the dual norm onLM¯(Ω) is equivalent to · M¯. We say that unconverges toufor the modular convergence inLM(Ω) if for someλ >0
ΩM un−u λ
dx−→0 asn−→ ∞. (2.4)
IfMsatisfies the∆2-condition, then the modular convergence coincide with the norm convergence.
2.3. The Orlicz Sobolev spaceW1LM(Ω) (resp.,W1EM(Ω)) is the space of all functionsusuch thatuand its distributional derivatives up to order one lie in LM(Ω) (resp.,EM(Ω)). It is a Banach space under the norm
u1,M=
|α|≤1
DαuM. (2.5)
Thus,W1LM(Ω) andW1EM(Ω) can be identified with subspaces of the product ofN+ 1 copies ofLM(Ω). Denoting this product byLM, we will use the weak topologiesσ(LM,EM¯) andσ(LM,LM¯).
The spaceW01EM(Ω) is defined as the norm closure ofᏰ(Ω) inW1EM(Ω) and the spaceW01LM(Ω) as theσ(LM,EM¯) closure ofᏰ(Ω) inW1LM(Ω).
We say thatunconverges toufor the modular convergence inW1LM(Ω) if for someλ >0
ΩMDαun−Dαu λ
dx−→0 ∀|α| ≤1. (2.6) This implies the convergenceσ(LM,LM¯).
2.4. LetW−1LM¯(Ω) (resp.,W−1EM¯(Ω)) denote the space of distributions onΩ which can be written as sums of derivatives of order≤1 of functions inLM¯(Ω) (resp.,EM¯(Ω)). It is a Banach space under the usual quotient norm.
If the open setΩhas the segment property, then the spaceᏰ(Ω) is dense inW01LM(Ω) for the modular convergence and thus for the topologyσ(LM, LM¯). Consequently, the action of a distribution inW−1LM¯(Ω) on an element ofW01LM(Ω) is well defined.
2.5. We recall the following lemmas.
Lemma2.1 (see [5]). LetΩbe an open subset ofRNwith finite measure. LetM,P, andQbeN-functions such thatQ P, and letf :Ω×R→RNbe a Carath´eodory function such that
f(x,s)≤c(x) +k1P−1Mk2|s|
a.e.x∈Ω,∀s∈R, (2.7) wherek1,k2∈R+,c(x)∈EQ(Ω). LetNf be the Nemytskii operator defined from P(EM(Ω),1/k2)={u∈LM(Ω) :d(u,EM(Ω))<1/k2}to(EQ(Ω))NbyNf(u)(x)=
f(x,u(x)). ThenNf is strongly continuous.
Lemma2.2 (see [5]). LetF :R→Rbe uniformly Lipschitzian, with F(0)=0.
LetM be anN-function and letu∈W01LM(Ω)(resp.,W01EM(Ω)). ThenF(u)∈ W01LM(Ω)(resp.,W01EM(Ω)). Moreover, if the setDof discontinuity points ofFis finite, then
∂
∂xiF(u)=
F(u)∂u
∂xi a.e. inx∈Ω:u(x)∈D, 0 a.e. inx∈Ω:u(x)∈D.
(2.8)
ThenF :W01LM(Ω)→W01LM(Ω)is sequentially continuous with respect to the weak∗topologyσ(LM,EM¯).
Lemma 2.3 (see [11]). Let Ω have the segment property. Then for each v ∈ W01LM(Ω), there exists a sequencevn∈Ᏸ(Ω)such thatvn converges tovfor the modular convergence inW01LM(Ω). Furthermore, ifv∈W01LM(Ω)∩L∞(Ω)then
vnL∞(Ω)≤(N+ 1)vL∞(Ω). (2.9)
2.6. We introduce the following notation, see [2,15].
Definition 2.4. LetMbe anN-function, and define the following set:
ᏭM=
Q:Qis anN-function such thatQ Q ≤
M M, 1
0
Q◦H−1 1
r1−1/N
dr <∞whereH(r)=M(r) r
.
(2.10)
Remark 2.5. LetM(t)=tpandQ(t)=tq, then the conditionQ∈ᏭM is equiva- lent to the following conditions:
(i) 2−1/N < p < N
(ii)q <p˜=(p−1)N/(N−1), see (1).
Remark 2.6. We can give some examples ofN-functionsMfor which the setᏭM
is not empty. Here, theN-functionsMare defined only at infinity.
(1) ForM(t)=t2logtandQ(t)=tlogt, we haveH(t)=tlogtandH−1(t)= t(logt)−1at infinity, see [13]. Then theN-functionQbelongs toᏭM.
(2) ForM(t)=t2log2tat infinity andQ(t)=tlog2t, we haveH(t)=tlog2t andH−1(t)=t(logt)−2 at infinity, see [13]. Then theN-functionQbelongs to ᏭM.
3. Definition and existence of entropy solutions
LetΩbe a bounded open subset ofRN with the segment property. LetM,Pbe twoN-functions such thatP M.
Let A :D(A) ⊂ W01LM(Ω) →W−1LM¯(Ω) be a mapping (not defined ev- erywhere) given by A(u)=−diva(x,u,∇u) where a:Ω×R×RN → RN is a Carath´eodory function satisfying for a.e.x∈Ωand allt∈R,ξ,ξ¯withξ=ξ¯,
a(x,t,ξ)≤d(x) +k1P¯−1Mk2|t|
+k3M¯−1Mk4|ξ|
, (3.1)
a(x,t,ξ)−ax,t,ξ¯ξ−ξ¯>0, (3.2) a(x,t,ξ)ξ≥αM
|ξ| λ
, (3.3)
whered(x)∈EM¯(Ω),d≥0,α,λ∈R∗+,k1,k2,k3,k4∈R+. Consider the nonlinear elliptic problem (1.1) where
f ∈L1(Ω) (3.4)
andφ=(φ1,...,φN) satisfies
φ∈
C0(R)N. (3.5)
As in [8], we define the following notion of an entropy solution, which gives a meaning to a possible solution of (1.1).
Definition 3.1. Assume that (3.1), (3.2), (3.3), (3.4), and (3.5) hold true and ᏭM=∅. A functionuis an entropy solution of problem (1.1) if
u∈W01LQ(Ω) ∀Q∈ᏭM, Tk(u)∈W01LM(Ω) ∀k >0,
Ωa(x,u,∇u)∇Tk[u−ϕ]dx≤
Ωf Tk[u−ϕ]dx+
Ωφ(u)∇Tk[u−ϕ]dx
∀ϕ∈W01LM(Ω)∩L∞(Ω).
(3.6)
We cannot use the solutionuas a test function in (1.1), becauseudoes not belong toW01LM(Ω). An important role is played byTk(u) and the test functions Tk[u−ϕ], ϕ∈W01LM(Ω)∩L∞(Ω) (3.7) because both belong toW01LM(Ω).
InTheorem 3.5, we prove the existence of solution of problem (1.1), in the framework of entropy solutions.
Lemma3.2. LetΩbe a bounded open subset ofRNwith the segment property. If u∈(W01LM(Ω))NthenΩdivudx=0.
Proof ofLemma 3.2. It is sufficient to use an approximation ofu.
We recall the following lemma (see [15, Lemma 2]).
Lemma3.3. LetMbe anN-function,u∈W1LM(Ω)such thatΩM(|∇u|)dx <∞, then
−µ(t)≥NC1N/Nµ1−1/N(t)
×C
−1 NC1N/Nµ1−1/N(t)
d dt
{|u|>t}M|∇u| dx
∀t >0, (3.8) whereCis the function defined as
C(t)= 1
supr≥0,H(r)≤t, H(r)=M(r)
r . (3.9)
The functionCNis the measure of the unit ball ofRN, andµ(t)=meas{|u|> t}. Lemma3.4. Let(X,τ,µ)be a measurable set such thatµ(X)<∞. Letγbe a mea- surable functionγ:X→[0,∞)such that
µx∈X:γ(x)=0=0, (3.10)
then for each>0, there existsδ >0such thatAγ(x)dx < δimplies
µ(A)≤. (3.11)
Theorem3.5. Under assumptions (3.1), (3.2), (3.3), (3.4), and (3.5), withᏭM=
∅, there exists an entropy solutionuof problem (1.1) (in the sense ofDefinition 3.1).
Remark 3.6. In the caseM(t)=tp,Theorem 3.5gives a refinement of the regular- ity result (1) (i.e.,u∈W01,q(Ω), q <p˜=((p−1)N/N−1)). In fact, byTheorem 3.5, we have u∈ W01LQ(Ω) for eachQ∈ ᏭM (for example for Q(t) =tp˜/logα(e+ t),α >1).
Proof ofTheorem 3.5
Step 1. Define, for eachn >0, the approximations
φn(s)=φTn(s), fn(s)=Tnf(s). (3.12) Consider the nonlinear elliptic problem
un∈W01LM(Ω), −divax,un,∇un=fn−divφnun inΩ. (3.13) From Gossez and Mustonen [12, Proposition 1, Remark 2], problem (3.13) has at least one solution.
Step 2. We will prove that (un) is bounded inW01LQ(Ω) for eachQ∈ᏭM. Letϕ be the truncation defined, for eacht,h >0, by
ϕ(ξ)=
0 if 0≤ξ≤t, 1
h(ξ−t) ift < ξ < t+h, 1 ifξ≥t+h,
−ϕ(−ξ) ifξ <0.
(3.14)
Using the test functionv=ϕ(un) in (3.13) (v∈W01LM(Ω) byLemma 2.2), we have
Ωax,un,∇unϕun∇undx=
Ωfnϕundx+
Ωφnun∇ϕundx. (3.15) We claim now that
Ωφnun∇ϕundx=0. (3.16) Indeed,
∇ϕun
=ϕun
∇un, (3.17)
where
ϕ(ξ)=
1
h ift <|ξ|< t+h,
0 otherwise, (3.18)
defineθ(s)=φn(s)(1/h)χ{t<|s|<t+h}, and ˜θ(s)=s
0θ(τ)dτ, we have byLemma 2.2, θ(u˜ n)∈(W01LM(Ω))N, which implies
Ωφnun∇ϕundx=
Ωφnun1
hχ{t<|un|<t+h}∇undx=
Ωθun∇undx
=
Ωdivθ˜undx=0 (seeLemma 3.2).
(3.19) This proves (3.16). By (3.3) and (3.15), we have (where we can suppose without loss of generality thatλ=1, since one can takeun=un/λ)
α h
t<|un|<t+h
M∇undx≤ f1,Ω. (3.20) Leth→0, then
−d dt
{|un|>t}M∇undx≤C withC=f1,Ω
α . (3.21)
We prove the following inequality, which allows us to obtain the boundedness of (un) inW01LQ(Ω),
− d dt
|un|>tQ∇undx
≤ −µn(t)Q◦H−1 − 1 NC1N/Nµn(t)1−1/N
d dt
{|un|>t}M∇undx
.
(3.22)
Indeed, let C(s) =1/H−1(s), where H(r) =M(r)/r andH−1(s)=sup{r ≥ 0, H(r)≤s}. Then
C(s)= s
M◦H−1(s). (3.23)
ByLemma 3.3we have, withµn(t)=meas{|un|> t},
−µn(t)≥NCN1/Nµn(t)1−1/N
×C − 1
NCN1/Nµn(t)1−1/N d dt
|un|>tM∇undx
, (3.24)
then
−µn(t)·M◦H−1 − 1 NC1N/Nµn(t)1−1/N
d dt
|un|>tM∇undx
≥NCN1/Nµn(t)1−1/N − 1 NC1/NN µn(t)1−1/N
d dt
|un|>tM∇undx
, (3.25)
and also 1 µn(t)
d dt
{|un|>t}M∇undx
≤M◦H−1 − 1 NCN1/Nµn(t)1−1/N
d dt
{|un|>t}M∇undx
(3.26)
which gives M−1
1 µn(t)
d dt
{|un|>t}M∇undx
≤H−1
− 1
NC1N/Nµn(t)1−1/N d dt
{|un|>t}M∇undx
.
(3.27)
LetQ ∈ᏭM and let D(s)=M(Q−1(s)),D is then convex, and the Jensen’s inequality gives
D {t<|un|<t+h}Q∇undx
−µn(t+h) +µn(t)
≤
{t<|un|<t+h}M∇undx
−µn(t+h) +µn(t) , (3.28) then
Q−1 1 µn(t)
d dt
{|un|>t}Q∇undx
≤M−1 1 µn(t)
d dt
{|un|>t}M∇undx
≤H−1 − 1 NCN1/Nµn(t)1−1/N
d dt
{|un|>t}M∇undx
(3.29)
which gives (3.22). By (3.21) and (3.22) and since the function t−→
{|un|>t}Q∇undx (3.30) is absolutely continuous (see [15]), we have
ΩQ∇undx= ∞
0 −d
dt
{|un|>t}Q∇un
dt
≤ ∞
0 −µn(t)Q◦H−1 C NCN1/Nµn(t)1−1/N
dt
≤ 1 C
C·meas(Ω)
0
Q◦H−1 1 r1−1/N
dr <∞
(3.31)
which implies that (∇un) is bounded in LQ(Ω) for eachQ∈ ᏭM. Then unis bounded inW01LQ(Ω) for eachQ∈ᏭM. Passing to a subsequence if necessary, we can assume that
unu weakly inW01LQ(Ω) forσLQ,EQ¯, a.e. inΩ. (3.32) Step 3. We prove thatTk(un)Tk(u) weakly inW01LM(Ω) for allk >0. Using the test functionTk(un) in (3.13), we obtain
Ωax,un,∇un
∇Tk un
dx=
ΩfnTk un
dx+
Ωφn un
∇Tk un
dx. (3.33) We claim that
Ωφnun∇Tkundx=0. (3.34) Indeed,∇Tk(un)=∇unχ{|un|≤k}, defineθ(t)=φn(t)χ{|t|≤k}, and ˜θ(t)=t
0θ(τ)dτ, we have byLemma 2.2, ˜θ(un)∈(W01LM(Ω))N,
Ωφnun∇Tkundx=
Ωφnunχ{|un|≤k}∇undx
=
Ωθun
∇undx
=
Ωdivθ˜undx=0 (byLemma 3.2)
(3.35)
which proves the claim.
On the other hand, (3.33) can be written as
Ωax,un,∇un
∇Tk un
dx=
Ωax,un,∇Tk un
∇Tk un
dx
=
ΩfnTkundx,
(3.36)
which implies, with (3.3), that∇Tk(un) is bounded in (LM(Ω))N, andTk(un) is bounded in (W01LM(Ω))N. Sinceun→ua.e. inΩthenTk(un)→Tk(u) a.e. inΩ.
Then
TkunTk(u) weakly inW01LM(Ω) forσLM,EM¯
. (3.37) Step 4. We will prove that∇un→ ∇ua.e. inΩ. Letλ >0,>0. ForB >1,k >0, we consider as in [9] forn,m∈N,
E1=∇un> B∪∇um> B∪un> B∪um> B, E2=un−um> k,
E3=un−um≤k,un≤B,um≤B,∇un≤B, ∇um≤B,∇un−∇um≥λ,
(3.38)
we have{|∇un−∇um| ≥λ} ⊂E1∪E2∪E3.
Since (un) and (∇un) are bounded in L1(Ω) (since un is bounded in W01LQ(Ω)), we have
2BµE1
<
E1
∇un+undx <
Ω
∇un+undx < C. (3.39) Then measE1 ≤forBsufficiently large enough, independently ofn,m. Thus we fixBin order to have
measE1≤. (3.40)
Now we claim that measE3≤fornandmlarge. LetC1be such thatun1≤ C1 and ∇un1 ≤C1. As in [9], the assumption (3.2) gives the existence of a measurable functionγ(x) such that
measx∈Ω:γ(x)=0=0,
a(x,t,ξ)−ax,t,ξ¯ξ−ξ¯≥γ(x)>0, (3.41) for allt∈R,ξ,ξ¯∈RN,|t|,|ξ|,|ξ¯| ≤B,|ξ−ξ¯| ≥λa.e. inΩ. We have
E3
γ(x)dx≤
E3
ax,un,∇un−ax,un,∇um∇un−∇umdx
≤
E3
ax,um,∇um
−ax,un,∇um
∇un−∇um dx +
E3
ax,un,∇un
−ax,um,∇um
∇un−∇um dx.
(3.42)
Using the test functionTk(un−um) in (3.13) and integrating onE3, we obtain
E3
ax,un,∇un−ax,um,∇um∇Tkun−umdx
=
E3
fn−fmTkun−umdx
+
E3
φn un
−φm um
∇Tk
un−um dx,
(3.43)
with
E3
φn un
−φm um
∇Tk
un−um dx
≤2B
E3
φn un
−φm umdx
≤2B
E3
φTn un
−φun+φun
−φum +φum
−φTm
umdx.
(3.44)
Letn0≥B, then forn,m ≥n0 we haveTn(un)=un andTm(um)=um on E3, which implies that the first and the third integral of the last inequality vanish.
The second integral of (3.42) is bounded forn,m≥n0by 2kf1,Ω+ 2B
E3
φun−φumdx. (3.45) For a.e.x∈Ωand1>0 there existη(x)≥0 (meas{x∈Ω:η(x)=0}=0) such that|s−s| ≤η(x),|s|,|s|,|ξ| ≤Bimplies
a(x,s,ξ)−ax,s,ξ≤1. (3.46) We use now the continuity ofφ, to obtain for a.e.x∈ Ωand 2 >0, η1(x)≥ 0 (meas{x ∈ Ω : η1(x) = 0} = 0) such that |s−s| ≤ η1(x), |s|,|s| ≤ B implies
φ(s)−φs≤2. (3.47)
Then
E3
γ(x)dx≤
E3∩{x∈Ω:η(x)<k}
ax,um,∇um−ax,un,∇um
×
∇un−∇um dx +
E3∩{x∈Ω:η(x)≥k}
ax,um,∇um−ax,un,∇um
×
∇un−∇umdx + 2kf1,Ω+ 2B
E3∩{x∈Ω:η1(x)<k}
φun
−φumdx +
E3∩{x∈Ω:η1(x)≥k}
φun−φumdx.
(3.48)
By using for the first integral the definition ofE3 and condition (3.1), for the second integral the definition ofE3and (3.46), for the fourth integral the defini- tion ofE3and|φ(un)| ≤C(B) (since|un| ≤Bandφcontinuous), and for the last integral the definition ofE3and (3.47), we obtain
E3
γ(x)dx≤C(B)
E3∩{x∈Ω:η(x)<k}
1 +d(x)dx+ 2C1(B)1
+ 2kf1,Ω+ 2C(B) measx∈Ω:η1(x)< k+C22.
(3.49)
We have meas{x∈Ω:η(x)< k} →0 whenk→0, and meas{x∈Ω:η1(x)<
k} →0 whenk→0. Let>0 and letδbe the real, inLemma 3.4, corresponding to, we choose1,2such that
2C1(B)1≤δ
5, C22≤δ
5, (3.50)
andksuch that C(B)
E3∩{x∈Ω:η(x)<k}
1 +d(x)dx < δ
5, 2kf1,Ω≤δ 5, 2C(B) measx∈Ω:η1(x)< k<δ
5.
(3.51)
ThenE
3γ(x)dx < δandLemma 3.4implies that
measE3< ∀n,m≥n0. (3.52) This completes the proof of the claim.
Let the lastkbe fixed,una Cauchy sequence in measure, we choosen1such that
measE2≤ ∀n,m≥n1. (3.53)
Then
measx∈Ω:∇un−∇um≥λ≤ ∀n,m≥maxn1,n0
(3.54) and∇un→ ∇uin measure, consequently
∇un−→ ∇u a.e. inΩ. (3.55)
Step 5. Letϕ∈W01LM(Ω)∩L∞(Ω). From Lemma 2.3, there exists a sequence (ϕj) ∈ Ᏸ(Ω) such that ϕj converges to ϕ for the modular convergence in W01LM(Ω) with
ϕjL∞(Ω)≤(N+ 1)ϕL∞(Ω). (3.56) UsingTk[un−ϕj] as a test function in (3.13) we obtain
Ωax,un,∇un
∇Tk un−ϕj
dx
=
ΩfnTkun−ϕjdx+
Ωφnun∇Tkun−ϕjdx
(3.57)
which gives, ifn→ ∞, lim inf
n→∞
Ωax,un,∇un
∇Tk un−ϕj
dx
≥lim inf
n→∞
Ω
ax,un,∇un−ax,un,∇ϕj∇Tkun−ϕjdx
+ lim
n→∞
Ωax,Tk+ϕjL∞(Ω)
un ,∇ϕj
∇Tk un−ϕj
dx
≥
Ω
ax,u,∇u−ax,u,∇ϕj∇Tku−ϕjdx
+
Ωax,u,∇ϕj
∇Tk u−ϕj
dx,
(3.58)
where we have used Fatou lemma for the first integral, and for the second the convergences∇Tk[un−ϕj]→ ∇Tk[u−ϕj] by (3.37) in (LM(Ω))N forσ(LM, EM¯) and a(x,Tk+ϕjL∞(Ω)(un),∇ϕj) → a(x,Tk+ϕjL∞(Ω)(u),∇ϕj) strongly in (EM¯(Ω))Nby (3.1), which implies that
lim inf
n→∞
Ωax,un,∇un
∇Tk un−ϕj
dx≥
Ωax,u,∇u∇Tk u−ϕj
dx. (3.59) Forn≥k+ (N+ 1)ϕL∞(Ω),
Ωφn un
∇Tk un−ϕj
dx=
ΩφTk+(N+1)ϕL∞(Ω)
un
∇Tk un−ϕj
dx
n→∞−→
ΩφTk+(N+1)ϕL∞(Ω)(u)∇Tku−ϕjdx, (3.60) we have used the convergences∇Tk[un−ϕj]∇Tk[u−ϕj] by (3.37) in (LM(Ω))N andφ(Tk+(N+1)ϕL∞(Ω)(un))→φ(Tk+(N+1)ϕL∞(Ω)(u)) strongly in (EM¯(Ω))Nsince φis continuous. On the other hand, since fn→f strongly inL1(Ω) andTk[un− ϕj]Tk[u−ϕj] weakly∗inL∞(Ω), we have
ΩfnTkun−ϕjdx−→
Ωf Tku−ϕjdx. (3.61) Then
Ωa(x,u,∇u)∇Tku−ϕjdx≥
ΩφTk+(N+1)ϕL∞(Ω)(u)∇Tku−ϕjdx +
Ωf Tk u−ϕj
dx.
(3.62)
Now, ifj→ ∞in (3.62), we get lim inf
j→∞
Ωa(x,u,∇u)∇Tk u−ϕj
dx
≥lim inf
j→∞
Ω
a(x,u,∇u)−ax,u,∇ϕj∇Tku−ϕjdx
+ lim
j→∞
Ωax,u,∇ϕj∇Tku−ϕjdx
≥
Ω
a(x,u,∇u)−a(x,u,∇ϕ)∇Tk[u−ϕ]dx
+
Ωa(x,u,∇ϕ)∇Tk[u−ϕ]dx,
(3.63)
where we have used Fatou lemma for the first integral, and for the second the convergences∇Tk[u−ϕj]∇Tk[u−ϕ] in (LM(Ω))N for the modular conver- gence anda(x,u,∇ϕj)→a(x,u,∇ϕ) in (LM¯(Ω))Nfor the modular convergence,
which implies that lim inf
j→∞
Ωa(x,u,∇u)∇Tku−ϕj dx≥
Ωa(x,u,∇u)∇Tk[u−ϕ]dx. (3.64) On the other hand, since∇Tk[u−ϕj]→ ∇Tk[u−ϕ] in (LM(Ω))Nfor the mod- ular convergence, then weakly forσ(LM,LM¯) andφ(Tk+(N+1)ϕL∞(Ω)(u))∈ (LM¯(Ω))Nwe have
ΩφTk+(N+1)ϕL∞(Ω)(u)∇Tk u−ϕj
dx
j→∞−→
ΩφTk+(N+1)ϕL∞(Ω)(u)∇Tk[u−ϕ]dx
=
Ωφ(u)∇Tk[u−ϕ]dx.
(3.65)
Since f ∈L1(Ω) andTk[u−ϕj]Tk[u−ϕ] weakly∗inL∞(Ω), we have
Ωf Tku−ϕjdx−→
Ωf Tk[u−ϕ]dx. (3.66) Then
Ωa(x,u,∇u)∇Tk[u−ϕ]dx≥
Ωφ(u)∇Tk[u−ϕ]dx+
Ωf Tk[u−ϕ]dx (3.67)
anduis an entropy solution of problem (1.1).
Theorem3.7. Suppose, inTheorem 3.5, that theN-functionMsatisfies, further- more, the∆2-condition and f ≥0, then the entropy solutionuof problem (1.1) satisfiesu≥0.
Proof ofTheorem 3.7. Usingϕ=Tl(u+) as test function in the definition of en- tropy solution, we obtain
Ωa(x,u,∇u)∇Tku−Tlu+dx
≤
Ωf Tk u−Tl
u+dx+
Ωφ(u)∇Tk u−Tl
u+dx.
(3.68)
We have
Ωf Tk u−Tl
u+dx≤
{u≥l}f Tk
u−Tl(u)dx. (3.69)
Indeed,
Ωf Tku−Tlu+dx=
u≥lf Tku−Tlu+dx +
0<u<l
f Tk u−Tl
u+dx +
u≤0f Tk u−Tl
u+dx.
(3.70)
If 0< u < lthenu−Tl(u+)=0 and0<u<lf Tk[u−Tl(u+)]dx=0. Ifu≤0 then u−Tl(u+)=uandu≤0f Tk[u−Tl(u+)]dx ≤0 since f is positive. Ifu≥lthen u+=uandu≥lf Tk[u−Tl(u+)]dx≤
u≥lf Tk[u−Tl(u)]dx.
On the other hand, we claim that
Ωφ(u)∇Tku−Tlu+dx=0. (3.71) Indeed, if 0< u < l, thenu−Tl(u+)=0, 0<u<lφ(u)∇Tk[u−Tl(u+)]dx =0. If u≤0, thenu−Tl(u+)=u,
u≤0φ(u)∇Tk u−Tl
u+dx=
−k≤u≤0φ(u)∇udx
=
Ωφ(u)∇uχ{−k≤u≤0}dx.
(3.72)
We verify that the third integral of the last inequality vanishes. For this, de- fineθ(t)=φ(t)χ{−k≤t≤0}, and ˜θ(t)=t
0θ(τ)dτ we have, byLemma 2.2, ˜θ(u)∈ (W01LM(Ω))Nwhich implies
Ωφ(u)∇uχ{−k≤u≤0}dx=
Ωθ(u)∇udx
=
Ωdivθ(u)˜ dx=0 (byLemma 3.2).
(3.73)
Ifu≥lthenu+=uand
{u≥l}φ(u)∇Tk u−Tl
u+dx=
l≤u≤l+k
φ(u)∇udx
=
Ωφ(u)∇uχ{l≤u≤l+k}dx.
(3.74)
Similarly, we verify that
Ωφ(u)∇uχ{l≤u≤l+k}dx=0. (3.75)