Weak solutions for some quasilinear elliptic equations by the sub-supersolution method

Similar documents
ON THE EXISTENCE OF A MAXIMAL WEAK SOLUTION FOR A SEMILINEAR ELLIPTIC EQUATION E.N. DANCER G. SWEERS

EXISTENCE AND UNIQUENESS OF POSITIVE SOLUTION OF A LOGISTIC EQUATION WITH NONLINEAR GRADIENT TERM

EXISTENCE OF STRONG SOLUTIONS OF FULLY NONLINEAR ELLIPTIC EQUATIONS

On the role playedby the Fuck spectrum in the determination of critical groups in elliptic problems where the asymptotic limits may not exist

Some non-local population models with non-linear diffusion

SYMMETRY OF POSITIVE SOLUTIONS OF SOME NONLINEAR EQUATIONS. M. Grossi S. Kesavan F. Pacella M. Ramaswamy. 1. Introduction

ON TRIVIAL GRADIENT YOUNG MEASURES BAISHENG YAN Abstract. We give a condition on a closed set K of real nm matrices which ensures that any W 1 p -grad

Discrete Halanay-type inequalities and applications

A Computational Approach to Study a Logistic Equation

Non-homogeneous semilinear elliptic equations involving critical Sobolev exponent

Local mountain-pass for a class of elliptic problems in R N involving critical growth

Elliptic Partial Differential Equations of Second Order

SEMILINEAR ELLIPTIC EQUATIONS WITH DEPENDENCE ON THE GRADIENT

A TWO PARAMETERS AMBROSETTI PRODI PROBLEM*

Seong Joo Kang. Let u be a smooth enough solution to a quasilinear hyperbolic mixed problem:

NONLINEAR FREDHOLM ALTERNATIVE FOR THE p-laplacian UNDER NONHOMOGENEOUS NEUMANN BOUNDARY CONDITION

EXISTENCE OF SOLUTIONS OF THE DIRICHLET PROBLEM FOR AN INFINITE SYSTEM OF NONLINEAR DIFFERENTIAL-FUNCTIONAL EQUATIONS OF ELLIPTIC TYPE

Bifurcation from the rst eigenvalue of some nonlinear elliptic operators in Banach spaces

Existence of Multiple Positive Solutions of Quasilinear Elliptic Problems in R N

Sébastien Chaumont a a Institut Élie Cartan, Université Henri Poincaré Nancy I, B. P. 239, Vandoeuvre-lès-Nancy Cedex, France. 1.

SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS. Massimo Grosi Filomena Pacella S. L. Yadava. 1. Introduction

p-laplacian problems with critical Sobolev exponents

Existence and Multiplicity of Solutions for a Class of Semilinear Elliptic Equations 1

Nonlinear Analysis 72 (2010) Contents lists available at ScienceDirect. Nonlinear Analysis. journal homepage:

GRAND SOBOLEV SPACES AND THEIR APPLICATIONS TO VARIATIONAL PROBLEMS

Multiple positive solutions for a class of quasilinear elliptic boundary-value problems

Spurious Chaotic Solutions of Dierential. Equations. Sigitas Keras. September Department of Applied Mathematics and Theoretical Physics

A GENERALIZATION OF THE FLAT CONE CONDITION FOR REGULARITY OF SOLUTIONS OF ELLIPTIC EQUATIONS

SHARP BOUNDARY TRACE INEQUALITIES. 1. Introduction

Regularity and nonexistence results for anisotropic quasilinear elliptic equations in convex domains

and finally, any second order divergence form elliptic operator

NONTRIVIAL SOLUTIONS TO INTEGRAL AND DIFFERENTIAL EQUATIONS

Exact multiplicity of boundary blow-up solutions for a bistable problem

A Product Property of Sobolev Spaces with Application to Elliptic Estimates

On non negative solutions of some quasilinear elliptic inequalities

2 A Model, Harmonic Map, Problem

HeadMedia Interaction in Magnetic Recording

Nonlinear resonance: a comparison between Landesman-Lazer and Ahmad-Lazer-Paul conditions

THE HARDY LITTLEWOOD MAXIMAL FUNCTION OF A SOBOLEV FUNCTION. Juha Kinnunen. 1 f(y) dy, B(x, r) B(x,r)

ON SOME ELLIPTIC PROBLEMS IN UNBOUNDED DOMAINS

ON QUALITATIVE PROPERTIES OF SOLUTIONS OF QUASILINEAR ELLIPTIC EQUATIONS WITH STRONG DEPENDENCE ON THE GRADIENT

2 The second case, in which Problem (P 1 ) reduces to the \one-phase" problem (P 2 ) 8 >< >: u t = u xx + uu x t > 0, x < (t) ; u((t); t) = q t > 0 ;

Nonlinear aspects of Calderón-Zygmund theory

Nonvariational problems with critical growth

EXISTENCE AND REGULARITY OF WEAK SOLUTIONS FOR SINGULAR ELLIPTIC PROBLEMS. 1. Introduction In this article we study the quasilinear elliptic problem

MIXED BOUNDARY-VALUE PROBLEMS FOR QUANTUM HYDRODYNAMIC MODELS WITH SEMICONDUCTORS IN THERMAL EQUILIBRIUM

ATTRACTORS FOR SEMILINEAR PARABOLIC PROBLEMS WITH DIRICHLET BOUNDARY CONDITIONS IN VARYING DOMAINS. Emerson A. M. de Abreu Alexandre N.

Gradient Schemes for an Obstacle Problem

WITH REPULSIVE SINGULAR FORCES MEIRONG ZHANG. (Communicated by Hal L. Smith) of repulsive type in the sense that G(u)! +1 as u! 0.

Nonlinear elliptic systems with exponential nonlinearities

Nonresonance for one-dimensional p-laplacian with regular restoring

COINCIDENCE SETS IN THE OBSTACLE PROBLEM FOR THE p-harmonic OPERATOR

A NOTE ON THE EXISTENCE OF TWO NONTRIVIAL SOLUTIONS OF A RESONANCE PROBLEM

On a weighted total variation minimization problem

EXISTENCE OF SOLUTIONS FOR CROSS CRITICAL EXPONENTIAL N-LAPLACIAN SYSTEMS

AN ASYMPTOTIC MEAN VALUE CHARACTERIZATION FOR p-harmonic FUNCTIONS. To the memory of our friend and colleague Fuensanta Andreu

Homogenization and error estimates of free boundary velocities in periodic media

Existence and uniqueness of solutions for a diffusion model of host parasite dynamics

Localization phenomena in degenerate logistic equation

LECTURE 15 + C+F. = A 11 x 1x1 +2A 12 x 1x2 + A 22 x 2x2 + B 1 x 1 + B 2 x 2. xi y 2 = ~y 2 (x 1 ;x 2 ) x 2 = ~x 2 (y 1 ;y 2 1

AMBROSETTI-PRODI PROBLEM WITH DEGENERATE POTENTIAL AND NEUMANN BOUNDARY CONDITION

Exact multiplicity results for a p-laplacian problem with concave convex concave nonlinearities

2 BAISHENG YAN When L =,it is easily seen that the set K = coincides with the set of conformal matrices, that is, K = = fr j 0 R 2 SO(n)g: Weakly L-qu

Minimization problems on the Hardy-Sobolev inequality

Global unbounded solutions of the Fujita equation in the intermediate range

On the spectrum of a nontypical eigenvalue problem

Exponential Energy Decay for the Kadomtsev-Petviashvili (KP-II) equation

MULTIPLE SOLUTIONS FOR AN INDEFINITE KIRCHHOFF-TYPE EQUATION WITH SIGN-CHANGING POTENTIAL

COMBINED EFFECTS FOR A STATIONARY PROBLEM WITH INDEFINITE NONLINEARITIES AND LACK OF COMPACTNESS

AN ASYMPTOTIC MEAN VALUE CHARACTERIZATION FOR p-harmonic FUNCTIONS

Explosive Solution of the Nonlinear Equation of a Parabolic Type

WALTER LITTMAN BO LIU kind of problem is related to the deformation of a membrane with strings attached to several sides of the polygon. In other word

MINIMAL GRAPHS PART I: EXISTENCE OF LIPSCHITZ WEAK SOLUTIONS TO THE DIRICHLET PROBLEM WITH C 2 BOUNDARY DATA

MULTIPLE SOLUTIONS FOR THE p-laplace EQUATION WITH NONLINEAR BOUNDARY CONDITIONS

Some lecture notes for Math 6050E: PDEs, Fall 2016

New Lyapunov Krasovskii functionals for stability of linear retarded and neutral type systems

arxiv: v1 [math.ap] 7 May 2009

EXISTENCE OF SOLUTIONS FOR A RESONANT PROBLEM UNDER LANDESMAN-LAZER CONDITIONS

MULTIPLE SOLUTIONS FOR CRITICAL ELLIPTIC PROBLEMS WITH FRACTIONAL LAPLACIAN

A Semilinear Elliptic Problem with Neumann Condition on the Boundary

A REMARK ON MINIMAL NODAL SOLUTIONS OF AN ELLIPTIC PROBLEM IN A BALL. Olaf Torné. 1. Introduction

Asymptotic Behavior of Infinity Harmonic Functions Near an Isolated Singularity

Pseudo-monotonicity and degenerate elliptic operators of second order

Initial value problems for singular and nonsmooth second order differential inclusions

COMPARISON PRINCIPLES FOR CONSTRAINED SUBHARMONICS PH.D. COURSE - SPRING 2019 UNIVERSITÀ DI MILANO

Constrained Leja points and the numerical solution of the constrained energy problem

ANALYTIC SMOOTHING EFFECT FOR NONLI TitleSCHRÖDINGER EQUATION IN TWO SPACE DIMENSIONS. Citation Osaka Journal of Mathematics.

t x 0.25

This method is introduced by the author in [4] in the case of the single obstacle problem (zero-obstacle). In that case it is enough to consider the v

ON THE GLOBAL EXISTENCE OF A CROSS-DIFFUSION SYSTEM. Yuan Lou. Wei-Ming Ni. Yaping Wu

Asymptotic behavior of infinity harmonic functions near an isolated singularity

THE FORM SUM AND THE FRIEDRICHS EXTENSION OF SCHRÖDINGER-TYPE OPERATORS ON RIEMANNIAN MANIFOLDS

Second Order Elliptic PDE

ON NONHOMOGENEOUS BIHARMONIC EQUATIONS INVOLVING CRITICAL SOBOLEV EXPONENT

Universal inequalities for eigenvalues. of elliptic operators in divergence. form on domains in complete. noncompact Riemannian manifolds

MAXIMIZATION AND MINIMIZATION PROBLEMS RELATED TO A p-laplacian EQUATION ON A MULTIPLY CONNECTED DOMAIN. N. Amiri and M.

arxiv: v3 [math.ap] 1 Sep 2017

DETERMINATION OF THE BLOW-UP RATE FOR THE SEMILINEAR WAVE EQUATION

SUB-SUPERSOLUTIONS IN A VARIATIONAL INEQUALITY RELATED TO A SANDPILE PROBLEM

Mathematica Bohemica

Transcription:

Nonlinear Analysis 4 (000) 995 100 www.elsevier.nl/locate/na Weak solutions for some quasilinear elliptic equations by the sub-supersolution method Manuel Delgado, Antonio Suarez Departamento de Ecuaciones Diferenciales y Analisis Numerico, C/Tara s/n, Universidad de Sevilla, 4101-Sevilla, Spain Received 6 March 1998; accepted 11 September 1998 Keywords: Quasilinear elliptic equation; Sub-supersolutions; Leray Schauder theorem; Gagliardo Nirenberg inequalities 1. Introduction Let be a bounded and regular domain in R N ;N, with a smooth boundary @. In this paper we study the solvability of the quasi-linear elliptic boundary value problem Lu = f(x; u; Du) in ; (1) u =0 on @ by the sub-supersolution method, where Du is the gradient of u and f : R R N R is a Caratheodory function satisfying f(x; s; ) g(x; s)+k with k R + 0 ;G(x):=sup s r g(x; s) Lp () for all r 0 and a positive constant with some restrictions that will be detailed below. In (1), L is an elliptic second-order operator of the form Lu := N i;j=1 @ @x i ( a ij (x) @u ) + @x j N i=1 b i (x) @u @x i and the precise assumptions on a ij and b i will also be explained below. Corresponding author. E-mail addresses: delgado@numer.us.es (M. Delgado), suarez@numer.us.es (A. Suarez) 036-546X/00/$ - see front matter? 000 Elsevier Science Ltd. All rights reserved. PII: S036-546X(99)00151-0

996 M. Delgado, A. Suarez / Nonlinear Analysis 4 (000) 995 100 The existence of a solution to a problem of this kind has been considered by several authors. Amann [] proved the existence of a minimal and a maximal classical solution (notions which appear already in papers of Satô [13], Mlak [1] and Akô [1]) for (1), assuming that a classical sub-supersolution couple exists. When p N, Amann and Crandall [3] proved a similar result in W ;p (), again with the help of a sub-supersolution couple for (1), with a more direct proof. Almost simultaneously, using the Leray Schauder xed point theorem, Kazdan and Kramer demonstrated in [9] that a classical solution exists. Here, the proof is considerably easier than in previous papers but the important information concerning the existence of minimal and maximal solutions is lost (see also [11], where the results are generalized including the case of some nonlinear boundary conditions). Several years later, Dancer and Sweers [5] remarked that, under the assumption of existence of a sub-supersolution couple in W 1; (), there exists a minimal and a maximal solution that belong to W 1; (). To this end, a nonconstructive argument which uses Zorn s lemma was employed by the authors. Moreover, Hess [8] proved the existence of a solution u W 1; () for (1), and so by a bootstrap argument u W ;m () where m = min{=; p}. In all these papers, the growth of the gradient in the nonlinear term is at most quadratic, i.e.. This is a reasonable assumption, in accordance with a well known result of Serrin [14] which states, roughly speaking, that if f grows faster than quadratically in Du and is smooth, there are smooth data for which (1) possesses no solution. More recently, several authors have used the Leray Schauder s theorem without any assumption concerning the existence of a sub-supersolution couple. Thus, Xavier [15] has deduced the existence of a solution in W ;p () in the case in which L is Laplace s operator and p N. It has been shown in [16] that the condition p N can be relaxed. In both papers, some conditions on the growth of f in terms of the rst eigenvalue 1 of Laplace s operator are imposed. In this paper, we will prove that, when p N, there exists at least one weak solution to (1) in W ;p (). We will use the sub-supersolution method for a general elliptic operator L.. The main result We consider problem (1), where N ( @ Lu := a ij (x) @u ) N + b i (x) @u : @x i @x j @x i i; j=1 i=1 We assume a ij W 1; (); a ij = a ji ;b i W 1; 0 () and div(b) 0, with b =(b 1 ;:::; b N ); we also assume there exists a positive constant such that N a ij (x) i j ; R N ; x : i; j=1 In (1), f : R R N R is a Caratheodory function, i.e. measurable in x and continuous in (s; ) R R N. In addition, we suppose that f satises f(x; s; ) g(x; s)+k ; ()

M. Delgado, A. Suarez / Nonlinear Analysis 4 (000) 995 100 997 where k; R + 0 ;gis also a Caratheodory function and satisfy: (H1) For all r 0, sup g( ;s) L p (); s r (H) (a) If N =, then 1 p and (b) If N 3, then N N + p N or p +1 : and p +1 N N p N p N and p +1 : (3) Denition 1. A couple {u 0 ;u 0 }, where the functions u 0 and u 0 belong to W ;p () L (), is a sub-supersolution couple for (1) (in W ;p ()) if: (1) u 0 0 u 0 on @, () u 0 u 0 in, (3) Lu 0 f(x; u 0 ;Du 0 ) 0 Lu 0 f(x; u 0 ;Du 0 ). Remark 1. Notice that the last inequalities have a meaning a.e. in. Indeed; whenever v W ;p () L (); we have f( ;v;dv) L q () for some q 1; since f(x; v; Dv) g(x; v) + k Dv a:e: in : In this paper, the main result is the following: Theorem 1. Assume 1 p if N = and N=(N +) p N if N 3. Also; assume (H1) and (H). If there exists a sub-supersolution couple for (1) in W ;p (); then (1) possesses at least one solution in W ;p (). Proof From (H), we know that p = Np=(N p). We also know that the interval [p; p ) is nonempty. For any q [p; p ), one has W ;p (), W 1;q () with a compact imbedding. Fixed q 0 [p; p ), let T : W 1;q0 () W 1;q0 () L () be the truncation operator associated to the sub-supersolution couple {u 0 ;u 0 } u 0 (x) if u 0 (x) u(x); Tu(x)= u(x) if u 0 (x) u(x) u 0 (x); u 0 (x) if u(x) u 0 (x): Observe that Tu(x) max{ u 0 (x) ; u 0 (x) } = m a:e: in ; whence Tu L () for any u W 1;q0 ().

998 M. Delgado, A. Suarez / Nonlinear Analysis 4 (000) 995 100 On the other hand, if u W 1;q0 () then Tu W 1;q0 (). Indeed, Tu(x)= u(x)+u0 (x)+u 0 (x) u(x) u 0 (x) 4 + u(x)+u0 (x) u 0 (x) u(x) u 0 (x) 4 and, by Corollary A:6. in [10] for example, it follows that Tu W 1;q0 (). Let us introduce U 0 =u 0 +K and U 0 =u 0 K, where K is a positive constant chosen in order to have U 0 1 and U 0 1: (4) Observe that TU 0 = u 0 and TU 0 = u 0. Dene now a(x) = max{ LU 0 (x); LU 0 (x); 1}: Then a L p () and a 1. For each 0 t 1, let us consider the boundary value problem Lu +(1 t)a(x)u = tf(x; Tu; D(Tu)) in ; u =0 on @: (5) Then, {U 0 ;U 0 } is a sub-supersolution couple for (5). Indeed, LU 0 +(1 t)a(x)u 0 LU 0 +(1 t)a(x) LU 0 (1 t)lu 0 = tlu 0 tf(x; u 0 ;Du 0 )=tf(x; TU 0 ;D(TU 0 )): Similarly, we can prove that U 0 is a sub-solution of (5). Furthermore, if u W ;p () is a solution of (5) for some t [0; 1], then U 0 u U 0 : (6) Indeed, let us just check that u U 0. Let us set w = u U 0. Then w W ;p () and we want to prove that w + = 0, where w + (x) = max{0;w(x)}. We know that Lu +(1 t)a(x)u = tf(x; Tu; D(Tu)) LU 0 +(1 t)a(x)u 0 tf(x; TU 0 ;D(TU 0 )) = tf(x; u 0 ;Du 0 ): Subtracting, we nd Lw +(1 t)a(x)w t[f(x; Tu; D(Tu)) f(x; u 0 ;Du 0 )]: (7) Multiplying this inequality by w + and integrating over, we obtain: (Lw)w + +(1 t) a(x)(w + ) t [f(x; Tu; D(Tu)) f(x; u 0 ;Du 0 )]w + t (g(x; Tu)+g(x; u 0 ))w + + k ( D(Tu) + Du 0 )w + : (8)

M. Delgado, A. Suarez / Nonlinear Analysis 4 (000) 995 100 999 Since w + =0 on @, one has (Lw)w + Dw + 1 div(b)(w + ) : (9) Here, we have used that p, i.e. that p N=(N + ). Observe that every integral in (8) is well posed. Certainly, g( ;Tu)+g( ;u 0 ) L p () by (H1), while w + L p () with p = p=(p 1) (this follows in a standard manner from Sobolev s imbedding and (H)). On the other hand, from the fact that D(Tu) L p (), we have D(Tu) + Du 0 L p = (): But denoting by s the conjugate of p =, we also have w + L s () (here, we use that (Np N +p)=(n p), which is also implied by (H)). Let us introduce A = {x :u(x) U 0 (x)}; B = {x :u(x) U 0 (x)}: We can write the last two integrals in (8) as the sum of integrals over A and B. Since w + =0 in A and Tu = Tu 0 = u 0 in B, we nd from (8) and (9) that w + = 0. The proof that U 0 u is similar. Let us introduce the mapping S :[0; 1] W 1;q0 () W 1;q0 (), where S(t; u)=v and v is the solution of Lv +(1 t)a(x)v = tf(x; Tu; D(Tu)) in ; v =0 on @: From the assumptions (H1) and (H), it follows that f( ; Tu; D(Tu)) L p () for any u W 1;q0 (). According to the L p theory of elliptic equations (see [7,9]), S(t; u) W ;p () for all t [0; 1] and for all u W 1;q0 (). Furthermore, from the Sobolev s imbedding theorem, it is not dicult to prove that S is continuous and compact. Let us show that u 1;q0 C; (10) whenever u W 1;q0 () and satises S(t; u) =u for some t [0; 1]. Then, from the Leray Schauder s xed point theorem (see for example [7], Theorem 11:6) we will be able to arm there exists u W 1;q0 () such that S(1;u)=u, i.e. satisfying Lu = f(x; Tu; D(Tu)) in ; (11) u =0 on @: Since this u belongs to W 1;q0 (), we will have f( ; Tu; D(Tu)) L p () and u W ;p (). Arguing as we did in the proof of (6), we will also have u 0 u u 0 ; whence Tu = u, that is to say u solves (1).

1000 M. Delgado, A. Suarez / Nonlinear Analysis 4 (000) 995 100 Hence, the proof of Theorem 1 will be achieved if we are able to establish (10). First, we observe that u 1;q0 C u ;p C( a p u + g( ;Tu) p + D(Tu) p ): Thus, one also has u ;p C( a p u + g( ;Tu) p + D(Tu) p ): (1) We know that u W ;p () L r (); r 1. From the Gagliardo Nirenberg inequalities (see [6], Theorem 10:1), we have Du p C u ;p u r 1 (13) with Nr pr pn = (Nr pr pn ) ( [1=; 1]): (14) This gives u ;p C(1 + g( ;Tu) p + u ;p u r (1 ) ): (15) Notice, from (6) that u r C where C is independent of t and r 1. From (H), we see that r can be chosen such that r(n p) pn and r 1; thus [1=; 1] r p + r N N p : (16) On the other hand, we have 1 N +r N + r : (17) Thus, for any and r satisfying r +r 1 r; r(n p) pn and N p + r N + r ; (18) we have 1 and, consequently, (10). We can consider the functions h 1 and h, with h 1 (r) r p + r ; h (r) N +r N + r : They both are increasing and satisfy lim h i(r)=: r + Moreover, h 1 (1) h (1) and their graphs only intersect when r(n p)=pn and, at this value, h i (r)=n=(n p). Thus, if p N and for any with =(p +1) N=(N p), we can nd one value of r which satises (18). If p N, the functions can only intersect at a nonpositive value, so that for any [=(p +1); ) we can nd a value for r which satises (18). In the case p = N the functions never intersect, so we have the same conclusion as the case p N. The proof is thus nished.

M. Delgado, A. Suarez / Nonlinear Analysis 4 (000) 995 100 1001 Remark. Notice that our solution satises u W ;p () and also u L () (remember (6)). Remark 3. We can use a similar argument when p=n. We have W ;p (), W 1;q () for any q [1; ), so every integral of (8) is well posed. We can dene S :[0; 1] W 1;q () W 1;q () for any q [1; ) and we need u 1;q C with C being a constant independent of t and u. From the Sobolev imbedding theorem, we have again u 1;q C u ;p : The Gagliardo Nirenberg inequalities can be also applied. In this situation, we obtain the restrictions N +1 : Moreover, the solution belongs to W 1;q () for any q [1; ). Remark 4. In the case N=(N +) p N=, we obtain in Theorem 1 that the upper bound is N=(N p). This function is increasing in p, so its inmum is achieved for p =N=(N + ). For this value, N=(N p)=(n +)=N which is just the bound in [15,16]. Remark 5. As we say in the Introduction, in [9] the author proved that there exists a solution u W ;m () for (1) where m = min{=; p}, and so, if =p u W ;p (). However, if =p then u belongs to W ;= (), W 1;q () where q = N N : If (N +)=N then q, so following [8] it cannot go further to obtain more regularity of the solution. In particular, it cannot prove the solution belongs to W ;p () by this way. 3. An example In this section, we analyze a simple (academic) example to which Theorem 1 can be applied. Let us consider the particular case N = 3, and the quasilinear problem u = n(x)+u( m(x)u)+(b(x) u) in ; (19) u =0 on @; where R; 3 and (H) m L (); n L (); b (L ()) 3 ; n 0; m m 0 0: In the context of population dynamics, any positive solution of (19) can be viewed as a steady-state population density. The coecient m = m(x) is associated to the limiting

100 M. Delgado, A. Suarez / Nonlinear Analysis 4 (000) 995 100 eect of crowding in the population, while the transport eect and the inuence of the surronding media are responsible for the presence of b=b(x) and n=n(x), respectively. With these assumptions, it is easy to prove that {u 0 ;u 0 } = {0;K} is a sub-supersolution couple for (19), provided K 0 is suciently large. So, we can deduce from theorem 1 that there exists a positive solution of (19). When p N, the existence of a sub-supersolution couple for (1) is ensured by others conditions that can be found in [15,4] Acknowledgements The authors would like to ackowledge support under grant DGICYT PB95-14. They also thank the referee for helpful suggestions. References [1] K. Akô, On the Dirichlet problem for quasi-linear elliptic dierential equations of the second order, J. Math. Soc. Japan 13 (1961) 45 6. [] H. Amann, Existence and multiplicity theorems for semi-linear elliptic boundary value problems, Math. Z. 150 (1976) 81 95. [3] H. Amann, M. Crandall, On some existence theorems for semilinear equations, Indiana Univ. Math. J. 7 (1978) 779 790. [4] N.P. Cac, Some remarks on a quasilinear elliptic boundary value problem, Nonlinear Anal. 8 (1984) 697 709. [5] E.N. Dancer, G. Sweers, On the existence of a maximal weak solution for a semilinear elliptic equation, Di. Int. Equa. (1989) 533 540. [6] A. Friedman, Partial Dierential Equations, Holt Rinehart and Winston. New York, 1969. [7] D. Gilbarg, N.S. Trudinger, Elliptic Partial Dierential Equations of Second Order, Springer, Berlin, 1977. [8] P. Hess, On a second-order nonlinear elliptic boundary value problem, Nonlinear Anal, in: L. Cesari, R. Kannan, H. Weinberger (Eds.), A Collection of Papers in Honor of E. Rothe, Academic Press, New York (1978), pp. 99 107. [9] J. Kazdan, R. Kramer, Invariant criteria for existence of solutions to second-order quasilinear elliptic equations, Commun. Pure Appl. Math. 31 (1978) 619 645. [10] D. Kinderlehrer, G. Stampacchia, An Introduction to Varitional Inequalities and Their Applications, Academic Press, New York 1980. [11] J. Mawhin, K. Schmitt, Upper and lower solutions and semilinear second order elliptic equations with non-linear boundary conditions, Proc. Roy. Soc. Edinburgh 97A (1984) 199 07. [1] W. Mlak, Parabolic dierential inequalities and Chaplighin s method, Ann. Polon. Math. 8 (1960) 139 15. [13] T. Satô T, Sur l equation aux derivees partielles z = f(x; y; z; p; q), Composition Math. 1 (1954) 157 177. [14] J. Serrin, The problem of Dirichlet for quasilinear elliptic dierential equations with many independent variables, Phil. Trans. Roy. Soc. London 64 (1969) 413 496. [15] J.B.M. Xavier, Some existence theorems for equations of the form u = f(x; u; Du), Nonlinear Anal. 15 (1990) 59 67. [16] Z. Yan, A note on the solvability in W ;p () for the equation u = f(x; u; Du), Nonlinear Anal. 4 (1995) 1413 1416.