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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 fL1(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

fL1(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,

uW01,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

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a(x,u,u)Tk[u−ϕ]dx

f Tk[u−ϕ]dx+

φ(u)Tk[u−ϕ]dx

ϕW01,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)

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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

Mu(x)dx <∞ (2.2)

(resp.,M(u(x)/λ)dx <∞for someλ >0). The spaceLM(Ω) is a Banach space under the norm

uM=inf

λ >0 :

M 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

u(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

M unu 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).

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We say thatunconverges toufor the modular convergence inW1LM(Ω) if for someλ >0

MDαunDαu 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]). Letbe 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) +k1P1Mk2|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)={uLM(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 letuW01LM(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 weaktopologyσ(LM,EM¯).

Lemma 2.3 (see [11]). Lethave the segment property. Then for each vW01LM(Ω), there exists a sequencevn∈Ᏸ(Ω)such thatvn converges tovfor the modular convergence inW01LM(Ω). Furthermore, ifvW01LM(Ω)∩L(Ω)then

vnL(Ω)≤(N+ 1)vL(Ω). (2.9)

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2.6. We introduce the following notation, see [2,15].

Definition 2.4. LetMbe anN-function, and define the following set:

M=

Q:Qis anN-function such thatQ Q

M M, 1

0

QH−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¯ξξ¯>0, (3.2) a(x,t,ξ)ξαM

|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

fL1(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).

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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

uW01LQ(Ω) ∀Q∈ᏭM, Tk(u)∈W01LM(Ω) k >0,

a(x,u,u)Tk[u−ϕ]dx

f Tk[u−ϕ]dx+

φ(u)Tk[u−ϕ]dx

ϕW01LM(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], ϕW01LM(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. Letbe a bounded open subset ofRNwith the segment property. If u∈(W01LM(Ω))Nthendivudx=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,uW1LM(Ω)such thatM(|∇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

µxX:γ(x)=0=0, (3.10)

then for each>0, there existsδ >0such thatAγ(x)dx < δimplies

µ(A). (3.11)

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Theorem3.5. Under assumptions (3.1), (3.2), (3.3), (3.4), and (3.5), withM=

, 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.,uW01,q(Ω), q <p˜=((p−1)N/N−1)). In fact, byTheorem 3.5, we have uW01LQ(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

unW01LM(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≤ξt, 1

h(ξ−t) ift < ξ < t+h, 1 ifξt+h,

ϕ(ξ) ifξ <0.

(3.14)

Using the test functionv=ϕ(un) in (3.13) (v∈W01LM(Ω) byLemma 2.2), we have

ax,un,unϕunundx=

fnϕundx+

φnunϕundx. (3.15) We claim now that

φnunϕundx=0. (3.16) Indeed,

ϕun

=ϕun

un, (3.17)

where

ϕ(ξ)=



 1

h ift <|ξ|< t+h,

0 otherwise, (3.18)

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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

φnunϕundx=

φnun1

{t<|un|<t+h}undx=

θunundx

=

divθ˜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

Mundxf1,Ω. (3.20) Leth→0, then

d dt

{|un|>t}MundxC 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|>tQundx

≤ −µn(t)Q◦H−1 − 1 NC1N/Nµn(t)1−1/N

d dt

{|un|>t}Mundx

.

(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

MH1(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|>tMundx

, (3.24)

then

µn(t)·MH−1 − 1 NC1N/Nµn(t)1−1/N

d dt

|un|>tMundx

NCN1/Nµn(t)1−1/N − 1 NC1/NN µn(t)1−1/N

d dt

|un|>tMundx

, (3.25)

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and also 1 µn(t)

d dt

{|un|>t}Mundx

MH−1 − 1 NCN1/Nµn(t)1−1/N

d dt

{|un|>t}Mundx

(3.26)

which gives M−1

1 µn(t)

d dt

{|un|>t}Mundx

H−1

− 1

NC1N/Nµn(t)1−1/N d dt

{|un|>t}Mundx

.

(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}Qundx

µn(t+h) +µn(t)

{t<|un|<t+h}Mundx

µn(t+h) +µn(t) , (3.28) then

Q−1 1 µn(t)

d dt

{|un|>t}Qundx

M−1 1 µn(t)

d dt

{|un|>t}Mundx

H−1 − 1 NCN1/Nµn(t)1−1/N

d dt

{|un|>t}Mundx

(3.29)

which gives (3.22). By (3.21) and (3.22) and since the function t−→

{|un|>t}Qundx (3.30) is absolutely continuous (see [15]), we have

Qundx=

0d

dt

{|un|>t}Qun

dt

0µn(t)Q◦H−1 C NCN1/Nµn(t)1−1/N

dt

≤ 1 C

C·meas(Ω)

0

QH−1 1 r1−1/N

dr <

(3.31)

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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

ax,un,un

Tk un

dx=

fnTk un

dx+

φn un

Tk un

dx. (3.33) We claim that

φnunTkundx=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,

φnunTkundx=

φnunχ{|un|≤k}undx

=

θun

undx

=

divθ˜undx=0 (byLemma 3.2)

(3.35)

which proves the claim.

On the other hand, (3.33) can be written as

ax,un,un

Tk un

dx=

ax,un,Tk un

Tk un

dx

=

fnTkundx,

(3.36)

which implies, with (3.3), that∇Tk(un) is bounded in (LM(Ω))N, andTk(un) is bounded in (W01LM(Ω))N. Sinceunua.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> Bun> Bum> B, E2=unum> k,

E3=unumk,unB,umB,unB,umB,un−∇umλ,

(3.38)

we have{|∇un−∇um| ≥λ} ⊂E1E2E3.

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Since (un) and (un) are bounded in L1(Ω) (since un is bounded in W01LQ(Ω)), we have

2BµE1

<

E1

un+undx <

un+undx < C. (3.39) Then measE1forBsufficiently large enough, independently ofn,m. Thus we fixBin order to have

measE1. (3.40)

Now we claim that measE3fornandmlarge. LetC1be such thatun1C1 and ∇un1C1. 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¯ξξ¯γ(x)>0, (3.41) for allt∈R,ξ,ξ¯∈RN,|t|,|ξ|,|ξ¯| ≤B,|ξξ¯| ≥λa.e. inΩ. We have

E3

γ(x)dx

E3

ax,un,unax,un,umun−∇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(unum) in (3.13) and integrating onE3, we obtain

E3

ax,un,unax,um,umTkunumdx

=

E3

fnfmTkunumdx

+

E3

φn un

φm um

Tk

unum dx,

(3.43)

with

E3

φn un

φm um

Tk

unum dx

≤2B

E3

φn un

φm umdx

≤2B

E3

φTn un

φun+φun

φum +φum

φTm

umdx.

(3.44)

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Letn0B, then forn,mn0 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,mn0by 2kf1,Ω+ 2B

E3

φunφumdx. (3.45) For a.e.x∈Ωand1>0 there existη(x)≥0 (meas{x∈Ω:η(x)=0}=0) such that|ss| ≤η(x),|s|,|s|,|ξ| ≤Bimplies

a(x,s,ξ)−ax,s1. (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 |ss| ≤ η1(x), |s|,|s| ≤ B implies

φ(s)φs2. (3.47)

Then

E3

γ(x)dx

E3∩{x∈Ω:η(x)<k}

ax,um,umax,un,um

×

un−∇um dx +

E3∩{x∈Ω:η(x)≥k}

ax,um,umax,un,um

×

un−∇umdx + 2kf1,Ω+ 2B

E3∩{x∈Ω:η1(x)<k}

φun

φumdx +

E3∩{x∈Ω:η1(x)≥k}

φunφumdx.

(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)dxC(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)1δ

5, C22δ

5, (3.50)

(13)

andksuch that C(B)

E3∩{x∈Ω:η(x)<k}

1 +d(x)dx < δ

5, 2kf1,Ωδ 5, 2C(B) measx∈Ω:η1(x)< k

5.

(3.51)

ThenE

3γ(x)dx < δandLemma 3.4implies that

measE3<n,mn0. (3.52) This completes the proof of the claim.

Let the lastkbe fixed,una Cauchy sequence in measure, we choosen1such that

measE2n,mn1. (3.53)

Then

measx∈Ω:un−∇umλn,m≥maxn1,n0

(3.54) and∇un→ ∇uin measure, consequently

un−→ ∇u a.e. inΩ. (3.55)

Step 5. LetϕW01LM(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[unϕj] as a test function in (3.13) we obtain

ax,un,un

Tk unϕj

dx

=

fnTkunϕjdx+

φnunTkunϕjdx

(3.57)

which gives, ifn→ ∞, lim inf

n→∞

ax,un,un

Tk unϕj

dx

≥lim inf

n→∞

ax,un,unax,un,ϕjTkunϕjdx

+ lim

n→∞

ax,TkjL∞(Ω)

un ,ϕj

Tk unϕj

dx

ax,u,uax,u,ϕjTkuϕjdx

+

ax,u,ϕj

Tk uϕj

dx,

(3.58)

(14)

where we have used Fatou lemma for the first integral, and for the second the convergences∇Tk[unϕj]→ ∇Tk[u−ϕj] by (3.37) in (LM(Ω))N forσ(LM, EM¯) and a(x,TkjL(Ω)(un),∇ϕj) → a(x,TkjL(Ω)(u),∇ϕj) strongly in (EM¯(Ω))Nby (3.1), which implies that

lim inf

n→∞

ax,un,un

Tk unϕj

dx

ax,u,uTk uϕj

dx. (3.59) Fornk+ (N+ 1)ϕL(),

φn un

Tk unϕj

dx=

φTk+(N+1)ϕL∞(Ω)

un

Tk unϕj

dx

n→∞−→

φTk+(N+1)ϕL(Ω)(u)Tkuϕjdx, (3.60) we have used the convergences∇Tk[unϕj]Tk[uϕj] 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 fnf strongly inL1(Ω) andTk[unϕj]Tk[u−ϕj] weaklyinL(Ω), we have

fnTkunϕjdx−→

f Tkuϕjdx. (3.61) Then

a(x,u,u)Tkuϕjdx

φTk+(N+1)ϕL(Ω)(u)Tkuϕjdx +

f Tk uϕj

dx.

(3.62)

Now, ifj→ ∞in (3.62), we get lim inf

j→∞

a(x,u,u)Tk uϕj

dx

≥lim inf

j→∞

a(x,u,u)ax,u,ϕjTkuϕjdx

+ lim

j→∞

ax,u,ϕjTkuϕjdx

a(x,u,u)a(x,u,ϕ)Tk[u−ϕ]dx

+

a(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,

(15)

which implies that lim inf

j→∞

a(x,u,u)Tkuϕj dx

a(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

φTk+(N+1)ϕL∞()(u)Tk uϕj

dx

j→∞−→

φTk+(N+1)ϕL(Ω)(u)Tk[u−ϕ]dx

=

φ(u)Tk[u−ϕ]dx.

(3.65)

Since fL1(Ω) andTk[u−ϕj]Tk[u−ϕ] weaklyinL(Ω), we have

f Tkuϕjdx−→

f Tk[u−ϕ]dx. (3.66) Then

a(x,u,u)Tk[u−ϕ]dx

φ(u)Tk[u−ϕ]dx+

f 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, the2-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

a(x,u,u)TkuTlu+dx

f Tk uTl

u+dx+

φ(u)Tk uTl

u+dx.

(3.68)

We have

f Tk uTl

u+dx

{u≥l}f Tk

uTl(u)dx. (3.69)

(16)

Indeed,

f TkuTlu+dx=

u≥lf TkuTlu+dx +

0<u<l

f Tk uTl

u+dx +

u≤0f Tk uTl

u+dx.

(3.70)

If 0< u < lthenuTl(u+)=0 and0<u<lf Tk[u−Tl(u+)]dx=0. Ifu≤0 then uTl(u+)=uandu≤0f Tk[u−Tl(u+)]dx ≤0 since f is positive. Ifulthen u+=uandu≥lf Tk[u−Tl(u+)]dx

u≥lf Tk[u−Tl(u)]dx.

On the other hand, we claim that

φ(u)TkuTlu+dx=0. (3.71) Indeed, if 0< u < l, thenuTl(u+)=0, 0<u<lφ(u)Tk[u−Tl(u+)]dx =0. If u≤0, thenuTl(u+)=u,

u≤0φ(u)Tk uTl

u+dx=

−k≤u≤0φ(u)udx

=

φ(u){−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

φ(u){−k≤u≤0}dx=

θ(u)udx

=

divθ(u)˜ dx=0 (byLemma 3.2).

(3.73)

Ifulthenu+=uand

{u≥l}φ(u)Tk uTl

u+dx=

l≤u≤l+k

φ(u)udx

=

φ(u){l≤u≤l+k}dx.

(3.74)

Similarly, we verify that

φ(u){l≤u≤l+k}dx=0. (3.75)

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