• 검색 결과가 없습니다.

The Nehari manifold approach for Dirichlet problem involving the $p(x)$-Laplacian equation

N/A
N/A
Protected

Academic year: 2022

Share "The Nehari manifold approach for Dirichlet problem involving the $p(x)$-Laplacian equation"

Copied!
16
0
0

로드 중.... (전체 텍스트 보기)

전체 글

(1)

J. Korean Math. Soc. 47 (2010), No. 4, pp. 845–860 DOI 10.4134/JKMS.2010.47.4.845

THE NEHARI MANIFOLD APPROACH FOR DIRICHLET PROBLEM INVOLVING THE p(x)-LAPLACIAN EQUATION

Rabil A. Mashiyev, Sezai Ogras, Zehra Yucedag, and Mustafa Avci

Abstract. In this paper, using the Nehari manifold approach and some variational techniques, we discuss the multiplicity of positive solutions for the p(x)-Laplacian problems with non-negative weight functions and prove that an elliptic equation has at least two positive solutions.

1. Introduction

In this paper, we study the multiplicity of positive solutions for the following elliptic equation

(E λ )

½ −∆ p(x) u(x) = λa(x) |u| q(x)−2 u + b(x) |u| h(x)−2 u in Ω

u(x) = 0 on ∂Ω,

where the following conditions are satisfied:

Ω is a bounded domain with smooth boundary in R N , N ≥ 2, q, p, h ∈ C(Ω) such that 1 < q(x) < p(x) < h(x) < p (x) (p (x) = N −p(x) N p(x) if N > p(x), p (x) = ∞ if N ≤ p(x)), 1 < p :=ess inf

x∈Ω p(x) ≤ p(x) ≤ p + := ess sup

x∈Ω p(x) <

∞, 1 < q ≤ q + < p ≤ p + < h ≤ h + , λ > 0 ∈ R and a, b ∈ C ¡ Ω ¢

are non-negative weight functions with compact support in Ω.

Over the last decade, the variable exponent Lebesgue spaces L p(x) and the corresponding Sobolev space W 1,p(x) have been a subject of active research area (we refer to [8, 11, 12, 18, 19] for the fundamental properties of these spaces).

These investigations are stimulated mainly by the development of the studies of problems in Elasticity, Electrorheological fluids, Image Processing, Flow in Porous Media, Calculus of Variations, Differential Equations with p(x)-growth (see Acerbi and Mingione [1], Diening [7], Buhrii and Mashiyev [5], Halsey [15], Mih˘ailescu and R˘adulescu [21], R˚ uˇziˇcka [24], Zhikov [28]). Among these problems, the study of p (x)-Laplacian problems via variational methods is an

Received October 7, 2008; Revised November 4, 2008.

2000 Mathematics Subject Classification. 35B38, 35D05, 35J60, 35J70, 58E05.

Key words and phrases. variable exponent Lebesgue-Sobolev spaces, p(x)-Laplacian, vari- ational methods, Nehari manifold, multiple positive solutions.

This Research Project was supported by DUAPK-2008-59-74, Dicle University, Turkey.

c

°2010 The Korean Mathematical Society

845

(2)

interesting topic. A lot of researchers have devoted their works to this area (see Chabrowski and Fu [6], Fan [10], Fan and Zhang [13, 14], Mih˘ailescu [21], Mih˘ailescu and R˘adulescu [22], Harjulehto, H¨ast¨o, Koskenoja and S. Varonen [16], H¨ast¨o [17], Ogras, Mashiyev, Avci and Yucedag [23]). We refer to the p (x)-Laplace operator ∆ p(x) u := div ³

|∇u| p(x)−2 ∇u ´

, where p is a continuous non-constant function. This differential operator is a natural generalization of the p-Laplace operator ∆ p u := div

³

|∇u| p−2 ∇u

´

, where p > 1 is a real con- stant. However, the p (x)-Laplace operator possesses more complicated nonlin- earity than p-Laplace operator, due to the fact that ∆ p(x) is not homogeneous.

This fact implies some difficulties; for example, we can not use the Lagrange Multiplier Theorem in many problems involving this operator.

In recent years, the similar problems of the form (E λ ) have been studied by many authors using various methods. In [20] for the case p (x) > 1 and 1 < q < infp < sup p < h < min

n

N, N −p N.p

o

and a (x) ≡ a, b (x) ≡ b > 0, using Ekeland’s variational principle and the mountain-pass lemma Mih˘ailescu proved that, if a and b small enough then there are two distinct solutions for the problem; in [22] under the assumptions 1 < min x∈Ω q (x) <

min x∈Ω p (x) < max x∈Ω q (x), where p (x) , q (x) are continuous on Ω, h (x) = 0, a (x) ≡ 1, b (x) = 0, Mih˘ailescu and R˘adulescu showed that there exists λ such that any λ ∈ (0, λ ) is an eigenvalue for the problem by using Eke- land’s variational principle and the mountain-pass lemma; in [14] for the case p (x) = q (x) > 1, h (x) = 0, where p (x) is continuous on Ω, and a (x) ≡ 1, b (x) = 0, Fan, Zhang, and Zhao obtained that, Λ = Λ p(x) , the set of eigen- values, is a nonempty infinite set such that sup Λ = +∞. In addition, they present some sufficient conditions for inf Λ = 0 and for inf Λ > 0, respec- tively; in [4] under the conditions p (x) = 2, q (x) = 2 and 1 < h < N +2 N −2 , where h is constant, and a (x) , b (x) : Ω ⊂ R N → R are smooth functions which may change sign in Ω, Brown and Zhang used the relationship be- tween the Nehari manifold and fibrering maps to show how existence and non- existence results for positive solutions of the equation are linked to properties of the Nehari manifold; in [2] Afrouzi, Mahdavi, and Naghizadeh dealt with the similar problem for the case p (x) = q (x) = p, h (x) = h, 1 < h < p, a (x) = 1 and b (x) : Ω ⊂ R N → R is a smooth function which may change sign and they discussed the existence and multiplicity of non-negative so- lutions of the problem from a variational viewpoint by making use of the Nehari manifold. Under the conditions p (x) = p, q (x) = q, h (x) = h, 1 < q < p < h < p ³

p = N −p N p if N > p, p = ∞ if N ≤ p ´

and the weight

functions a (x) ≡ b (x) ≡ 1, the authors Ambrosetti-Brezis-Cerami [3] have in-

vestigated equation (E λ ). They found that there exists λ 0 such that equation

(E λ ) admits at least two positive solutions for λ ∈ (0, λ 0 ) , has a positive solu-

tion for λ = λ 0 and no positive solution exists for λ > λ 0 , and also in [26] under

(3)

the same assumptions and with sign-changing weight functions a (x) and b (x), Wu gave a variational proof of the existence of at least two positive solutions of equation (E λ ) for p ∈ (1, p ), using Palais-Smale and decomposition of the Nehari manifold.

In this paper, we have generalized the articles of Ambrosetti-Brezis-Cerami [3] and Wu [26] , to the p (x)-Laplacian by using the Nehari manifold under the similar conditions. We shall discuss the multiplicity of positive solutions for the problem (E λ ) and prove the existence of at least two positive solutions.

If we consider all above mentioned papers use of the Nehari manifold ap- proach for the case p (x)-growth condition makes our study quite different and very interesting.

2. Notations and preliminaries

We will discuss our problem (E λ ) in the variable exponent Sobolev space W 0 1,p(x) (Ω), so we need some theories and basic properties on spaces L p(x) (Ω) and W 1,p(x) (Ω) .

Write

L + (Ω) = ©

p ∈ L (Ω) : p > 1 ª .

Let’s define by U (Ω) the set of all measurable real functions defined on Ω.

For any p ∈ L + (Ω), we denote the variable exponent Lebesgue space by

L p(x) (Ω) =

 

u ∈ U (Ω) : Z

|u (x)| p(x) dx < ∞

 

, which is equipped with the norm, so-called Luxemburg norm [11, 12, 18]

|u| p(x) = inf

 

δ > 0 : Z

¯ ¯

¯ ¯ u (x) δ

¯ ¯

¯ ¯

p(x)

dx ≤ 1

 

 and

³

L p(x) (Ω) , | · | p(x)

´

becomes a Banach space, we call it as variable expo- nent Lebesgue space.

Let c is a measurable real-valued function and c(x) > 0 for x ∈ Ω. Then the weighted variable exponent Lebesgue space L p(x) c(x) (Ω) is defined by

L p(x) c(x) (Ω) =

 

u ∈ U (Ω) : Z

c(x) |u (x)| p(x) dx < ∞; c(x) > 0

 

 which is equipped with the norm

|u| (p(x),c(x)) = inf

 

δ > 0 : Z

c(x)

¯ ¯

¯ ¯ u (x) δ

¯ ¯

¯ ¯

p(x)

dx ≤ 1

 

.

(4)

Proposition 2.1 ([11, 18]). The conjugate space of L p(x) (Ω) is L p

0

(x) (Ω) , where p

0

1 (x) + p(x) 1 = 1. For any u ∈ L p(x) (Ω) and v ∈ L p

0

(x) (Ω), we have

¯ ¯

¯ ¯

¯ ¯ Z

uvdx

¯ ¯

¯ ¯

¯ ¯ µ 1

p + 1 (p 0 )

|u| p(x) |v| p

0

(x) ≤ 2 |u| p(x) |v| p

0

(x) .

Proposition 2.2 ([11, 18]). Denote ρ (u) = R

|u (x)| p(x) dx, ∀u ∈ L p(x) Ω, then we have

i) |u| p(x) < 1 (= 1; > 1) ⇔ ρ (u) < 1 (= 1; > 1) , ii) |u| p(x) > 1 =⇒ |u| p p(x)

≤ ρ (u) ≤ |u| p p(x)

+

, iii) |u| p(x) < 1 =⇒ |u| p p(x)

+

≤ ρ (u) ≤ |u| p p(x)

.

Proposition 2.3 ([11, 18]). If u, u n ∈ L p(x) (Ω) , n = 1, 2, . . . , then the follow- ing statements are equivalent to each other:

(1) lim

n→∞ |u n − u| p(x) = 0;

(2) lim

n→∞ ρ(u n − u) = 0;

(3) u n → u in measure in Ω and lim

n→∞ ρ(u n ) = ρ(u).

Define the variable exponent Sobolev space W 1,p(x) (Ω) by W 1,p(x) (Ω) = {u ∈ L p(x) (Ω) ; |∇u| ∈ L p(x) (Ω)}

and it can be equipped with the norm

kuk = |u| p(x) + |∇u| p(x) , ∀u ∈ W 1,p(x) (Ω) .

The space W 0 1,p(x) (Ω) is denoted by the closure of C 0 (Ω) in W 1,p(x) (Ω). We will use kuk = |∇u| p(x) for u ∈ W 0 1,p(x) (Ω) in the following discussions.

Proposition 2.4 ([11, 18]). If p > 1 and p + < ∞, then the spaces L p(x) (Ω), L p(x) c(x) (Ω), W 1,p(x) (Ω) and W 0 1,p(x) (Ω) are separable and reflexive Banach spaces.

Given two Banach spaces X and Y the symbol X ,→ Y means that X is continuously embedded in Y and also the symbol X ,→,→ Y means that there is a compact embedding of X in Y .

Proposition 2.5 ([11, 18]). (i) Assume that the boundary of Ω possesses the cone property and p ∈ C(Ω). If q ∈ C(Ω) and 1 ≤ q (x) < p (x) for any x ∈ Ω, then W 1,p(x) (Ω) ,→,→ L q(x) (Ω).

(ii) If p, q ∈ C(Ω) and p (x) ≤ q (x) ≤ p (x) for any x ∈ Ω, then W 1,p(x) (Ω) ,→ L q(x) (Ω) and also there is a constant c > 0 such that

|u| q(x) ≤ c kuk ∀ u ∈ W 0 1,p(x) (Ω) .

(5)

Proposition 2.6 ([8]). Let p(x) and q(x) be measurable functions such that p(x) ∈ L (Ω) and 1 ≤ p(x)q(x) ≤ ∞ for a.e. x ∈ Ω. Let u ∈ L q(x) (Ω), u 6= 0.

Then

|u| p(x)q(x) ≤ 1 =⇒ |u| p p(x)q(x)

+

¯ ¯

¯|u| p(x)

¯ ¯

¯ q(x) ≤ |u| p p(x)q(x)

|u| p(x)q(x) ≥ 1 =⇒ |u| p p(x)q(x)

¯ ¯

¯|u| p(x)

¯ ¯

¯ q(x) ≤ |u| p p(x)q(x)

+

. In particular, if p(x) = p is constant, then

||u| p | q(x) = |u| p pq(x) .

Theorem 2.7. Assume that the boundary of Ω possesses the cone property and p ∈ C ¡

Ω ¢

. Suppose that b ∈ L β(x) (Ω), b (x) > 0 for x ∈ Ω, β ∈ C ¡ Ω ¢

and β > 1, β 0 ≤ β 0 (x) ≤ β + 0 ³

1 β(x) + β 1

0

(x) = 1 ´

. If h ∈ C ¡ Ω ¢

and (2.1) 1 < h (x) < β(x) − 1

β(x) p (x) , ∀x ∈ Ω or

1 < β(x) < N p(x)

N p(x) − h(x) (N − p(x)) ,

then the embedding from W 1,p(x) (Ω) to L h(x) b(x) (Ω) is compact. Moreover, there is a constant c 5 > 0 such that the inequality

(2.2)

Z

b (x) |u| h(x) dx ≤ c 5

³

kuk h

+ kuk h

+

´

holds.

Proof. We must remark that our proof of the embedding W 1,p(x) (Ω) ,→,→

L h(x) b(x) (Ω) is similar to Fan [10] . Let u ∈ W 1,p(x) (Ω) and set r (x) = β(x)−1 β(x) h (x)

= β 0 (x) h (x). Then (2.1) implies r (x) < p (x). Hence, by Proposition 2.5 we have the embedding W 1,p(x) (Ω) ,→,→ L r(x) (Ω). So, for u ∈ W 1,p(x) (Ω), we have |u| h(x) ∈ L β

0

(x) (Ω). By Proposition 2.1,

Z

b (x) |u| h(x) dx ≤ c 1 |b| β(x)

¯ ¯

¯|u| h(x)

¯ ¯

¯ β

0

(x) < ∞.

This implies that W 1,p(x) (Ω) ⊂ L h(x) b(x) (Ω). Now let {u n } ⊂ W 1,p(x) (Ω) and u n * 0 (weakly) in W 1,p(x) (Ω).

Then, we have

u n → 0 (strongly) in L r(x) (Ω) . So, it follows that

¯ ¯

¯|u n | h(x)

¯ ¯

¯ β

0

(x) → 0. Thus, we have Z

b (x) |u n | h(x) dx ≤ c 1 |b| β(x)

¯ ¯

¯|u n | h(x)

¯ ¯

¯ β

0

(x) → 0,

(6)

which implies |u n | (h(x),b(x)) → 0. Hence, we have the embedding W 1,p(x) (Ω) ,→,→

L h(x) b(x) (Ω).

Now let’s show the inequality (2.2) holds. By the above inequity we know

that Z

b (x) |u| h(x) dx ≤ c 1 |b| β(x)

¯ ¯

¯|u| h(x)

¯ ¯

¯ β

0

(x) < ∞.

Since h ≤ h (x) ≤ h + and |u| h(x) ≤ |u| h

+ |u| h

+

it follows that Z

b (x) |u| h(x) dx ≤ Z

b (x) |u| h

dx + Z

b (x) |u| h

+

dx.

Moreover, by Propositions 2.1, 2.2, 2.5, 2.6 and the condition p(x) < h β 0 (x) ≤ h + β 0 (x) < p (x), we have

(2.3) Z

b (x) |u| h

dx ≤ c 2 |b| β(x)

¯ ¯

¯|u| h

¯ ¯

¯ β

0

(x) = c 2 |b| β(x) |u| h h

β

0

(x) ≤ c 3 kuk h

. Similarly, we can obtain

(2.4)

Z

b (x) |u| h

+

dx ≤ c 4 kuk h

+

.

As a result, from (2.3) and (2.4) it follows that Z

b (x) |u| h(x) dx ≤ c 5

³

kuk h

+ kuk h

+

´ .

The proof is complete. ¤

Theorem 2.8. Assume that the boundary of Ω possesses the cone property and p ∈ C ¡

Ω ¢

. Suppose that a ∈ L α(x) (Ω), a (x) > 0 for x ∈ Ω, α ∈ C ¡ Ω ¢ and α > 1, α 0 ≤ α 0 (x) ≤ α + 0

³ 1 α(x) + α 1

0

(x) = 1

´

. If q ∈ C ¡ Ω ¢

, p (x) <

α(x)

α(x)−1 q (x) and

(2.5) 1 < q (x) < α(x) − 1

α(x) p (x) , ∀x ∈ Ω

or N p(x)

N p(x) − q(x) (N − p(x)) < α(x) < p(x)

p(x) − q(x) with,

then the embedding from W 1,p(x) (Ω) to L q(x) a(x) (Ω) is compact. Moreover, there is a constant c 7 > 0 such that the inequality

(2.6)

Z

a (x) |u| q(x) dx ≤ c 7

³

kuk q

+ kuk q

+

´

holds.

(7)

Proof. Let u ∈ W 1,p(x) (Ω). Set m (x) = α(x)−1 α(x) q (x) = α 0 (x) q (x). Then (2.5) implies m (x) < p (x). Hence, by Proposition 2.5 there is the embedding W 1,p(x) (Ω) ,→,→ L m(x) (Ω). For u ∈ W 1,p(x) (Ω) we have |u| q(x) ∈ L α

0

(x) (Ω).

By Proposition 2.1, Z

a (x) |u| q(x) dx ≤ c 6 |a| α(x)

¯ ¯

¯|u| q(x)

¯ ¯

¯ α

0

(x) < ∞.

This implies that W 1,p(x) (Ω) ⊂ L q(x) a(x) (Ω). Now let {u n } ⊂ W 1,p(x) (Ω) and u n * 0 in W 1,p(x) (Ω).

Then, we have

u n → 0 in L m(x) (Ω) . So, it follows that

¯ ¯

¯|u n | q(x)

¯ ¯

¯ α

0

(x) → 0. Thus, we have Z

a (x) |u| q(x) dx ≤ c 6 |a| α(x)

¯ ¯

¯|u| q(x)

¯ ¯

¯ α

0

(x) → 0,

which implies |u n | (q(x),a(x)) → 0. Hence, we have the embedding W 1,p(x) (Ω) ,→,→

L q(x) a(x) (Ω).

Now, let’s show that the inequality (2.6) holds. By the above inequality we know that Z

a (x) |u| q(x) dx ≤ c 6 |a| α(x)

¯ ¯

¯|u| q(x)

¯ ¯

¯ α

0

(x) < ∞.

Considering the condition p(x) < q α 0 (x) ≤ q + α 0 (x) < p (x) and applying the similar steps as we did in proof of Theorem 2.7, we have

Z

a (x) |u| q(x) dx ≤ c 7 ³

kuk q

+ kuk q

+

´ .

The proof is complete. ¤

Proposition 2.9. Assume that the conditions of Theorem 2.7 and Theorem 2.8 hold, respectively. Let u ∈ W 1,p(x) (Ω), then there are positive constants c 8 , c 9 , c 10 , c 11 > 0 such that the following inequalities hold

i) Z

b (x) |u| h(x) dx ≤ (

c 8 kuk h

+

if kuk > 1 c 9 kuk h

if kuk < 1

ii) Z

a (x) |u| q(x) dx ≤ (

c 10 kuk q

+

if kuk > 1

c 11 kuk q

if kuk < 1.

(8)

Proof. It follows immediately from the conclusions of Theorem 2.7 and Theo-

rem 2.8, respectively. ¤

3. The main results

Let J ∈ C 1 (X, R) be the Euler functional associated with an elliptic problem on Banach space X. If J is bounded below and has a minimizer on X, then this minimizer is a critical point of J. Hence, it is a solution of the corresponding elliptic problem. However, in many problems J is not bounded below on the whole space X, but is bounded below on an appropriate subset of X, and minimizer on this set (if it exists) may give rise to solutions of the corresponding elliptic problem. A good candidate for an appropriate subset of X is the Nehari manifold.

If we consider our problem (E λ ), then, the corresponding Euler functional is defined by

J λ (u) = Z

1

p(x) |∇u| p(x) dx − λ Z

1

q(x) a (x) |u| q(x) dx − Z

1

h (x) b (x) |u| h(x) dx.

Then, by Theorems 2.7, 2.8, and Proposition 2.2, we have

J λ (u) ≥ 1 p +

Z

|∇u| p(x) dx − λ q

Z

a (x) |u| q(x) dx − 1 h

Z

b (x) |u| h(x) dx,

1

p + kuk p

λ q c 7

³

kuk q

+ kuk q

+

´

1 h c 5

³

kuk h

+ kuk h

+

´ .

Since q + < p ≤ p + < h ≤ h + , this shows J λ is not bounded below on whole W 0 1,p(x) (Ω). However, we shall show it is bounded on the Nehari manifold M λ (Ω) which is given by

M λ (Ω) = n

u ∈ W 0 1,p(x) (Ω)\ {0} : hJ λ 0 (u), ui = 0 o

,

where h., .i denotes the usual duality between W 0 1,p(x) (Ω) and W −1,p

0

(x) (Ω). It is clear that all critical points of J λ must lie on M λ (Ω) and local minimizers on M λ (Ω) are usually critical points of J λ .

Thus, u ∈ M λ (Ω) if and only if (3.1)

I λ (u) := hJ λ 0 (u), ui = Z

|∇u| p(x) dx − λ Z

a (x) |u| q(x) dx − Z

b (x) |u| h(x) dx

= 0.

(9)

Then for u ∈ M λ (Ω), we have hI λ 0 (u), ui =

Z

p (x) |∇u| p(x) dx − λ Z

q (x) a (x) |u| q(x) dx

Z

h (x) b (x) |u| h(x) dx

¡

p + − q ¢ λ

Z

a (x) |u| q(x) dx + ¡

p + − h ¢ Z

b (x) |u| h(x) dx.

Now, we split M λ (Ω) into three parts:

M λ + = {u ∈ M λ (Ω) : hI λ 0 (u), ui > 0} , M λ = {u ∈ M λ (Ω) : hI λ 0 (u), ui < 0} , M λ 0 = {u ∈ M λ (Ω) : hI λ 0 (u), ui = 0} .

Theorem 3.1. Suppose that u 0 is a local maximum or minimum for J λ on M λ (Ω) . If u 0 ∈ M / λ 0 (Ω), then u 0 is a critical point of J λ .

Proof. The proof of Theorem 3.1 can be obtained directly from the following

lemmas (particularly Lemma 3.3). ¤

Lemma 3.2. The energy functional J λ is coercive and bounded below on M λ (Ω).

Proof. Let u ∈ M λ (Ω) and kuk > 1. Then using (3.1), Propositions 2.2 and 2.9, we have

J λ (u) = Z

1

p(x) |∇u| p(x) dx − λ Z

1

q(x) a (x) |u| q(x) dx − Z

1

h (x) b (x) |u| h(x) dx

1 p +

Z

|∇u| p(x) dx − λ q

Z

a (x) |u| q(x) dx

1 h

 Z

|∇u| p(x) dx − λ Z

a (x) |u| q(x) dx

µ 1

p + 1 h

¶ Z

|∇u| p(x) dx + λ µ 1

h 1 q

¶ Z

a(x) |u| q(x) dx

µ h − p + h p +

kuk p

− c 10 λ

µ h − q h q

kuk q

+

.

Since, p > q + so, J λ (u) → ∞ as kuk → ∞. This implies J λ is coercive

and bounded below on M λ (Ω) . ¤

Lemma 3.3. There exists λ 1 > 0 such that for 0 < λ < λ 1 we have M λ 0 (Ω) =

∅.

(10)

Proof. Suppose otherwise, that is, M λ 0 (Ω) 6= ∅ for all λ ∈ R r {0} . Let u ∈ M λ 0 (Ω) such that kuk > 1. Then using (3.1), (2.4) and definition of M λ 0 (Ω), we have

0 = hI λ / (u) , ui

= Z

p (x) |∇u| p(x) dx − λ Z

q (x) a (x) |u| q(x) dx − Z

h (x) b (x) |u| h(x) dx

≥ p Z

|∇u| p(x) dx − q +

 Z

|∇u| p(x) dx − Z

b (x) |u| h(x) dx

− h + Z

b (x) |u| h(x) dx

¡

p − q + ¢ Z

|∇u| p(x) dx + ¡

q + − h + ¢ Z

b(x) |u| h(x) dx.

By Proposition 2.9, 0 ≥ ¡

p − q + ¢

kuk p

+ c 8

¡ q + − h + ¢ kuk h

+

,

(3.2) kuk ≥ c 12

µ p − q + h + − q +

1

h+−p−

. Similarly,

0 = hI λ 0 (u) , ui

≤ p + Z

|∇u| p(x) dx − λq Z

a (x) |u| q(x) dx − h Z

b (x) |u| h(x) dx

≤ p + Z

|∇u| p(x) dx − λq Z

a (x) |u| q(x) dx

− h

 Z

|∇u| p(x) dx − λ Z

a (x) |u| q(x) dx

 .

By Proposition 2.9, 0 ≤ ¡

p + − h ¢

kuk p

+ λc 10

¡ h − q ¢ kuk q

+

,

(3.3) kuk ≤ c 13

µ

λ h − q h − p +

1

p−−q+

.

(11)

If λ is sufficiently small (e.g. λ =

³ h

−p

+

h

−q

´ ³ p

−q

+

h

+

−q

+

´

p−−q+

h+−p−

), then from (3.2) and (3.3) we get kuk < 1 which contradicts with our assumption. Hence, we

conclude M λ 0 (Ω) = ∅. ¤

By Lemma 3.3, for 0 < λ < λ 1 , we can write M λ (Ω) = M λ + (Ω) ∪ M λ (Ω).

Therefore, we can let α + λ = inf

u∈M

λ+

(Ω) J λ (u) and α λ = inf

u∈M

λ

(Ω) J λ (u).

Lemma 3.4. If 0 < λ < λ 1 , then for all u ∈ M λ + (Ω), J λ (u) < 0.

Proof. Let u ∈ M λ + (Ω). By definition of J λ (u), we can write (3.4) J λ (u) ≤ 1

p Z

|∇u| p(x) dx− λ q +

Z

a(x) |u| q(x) dx− 1 h +

Z

b (x) |u| h(x) dx.

Since u ∈ M λ + (Ω), we have (3.5) p +

Z

|∇u| p(x) dx − λq Z

a(x) |u| q(x) dx − h Z

b(x) |u| h(x) dx > 0.

Now, if we multiply (3.1) by (−q ) and add with (3.5), we get (3.6)

Z

b(x) |u| h(x) dx < p + − q h − q

Z

|∇u| p(x) dx.

Moreover, using (3.1) together with (3.4) (3.7) J λ (u) ≤

µ 1 p 1

q +

¶ Z

|∇u| p(x) dx + µ 1

q + 1 h +

¶ Z

b(x) |u| h(x) dx,

and applying (3.6) in (3.7), it follows

J λ (u) < − (p − q + ) (h + − p )

h + p q + kuk p

< 0.

Hence, we have α + λ = inf

u∈M

λ+

(Ω) J λ (u) < 0. ¤

Theorem 3.5. If 0 < λ < λ 1 , there exists a minimizer of J λ on M λ + (Ω).

Proof. Since J λ is bounded below on M λ (Ω) and so on M λ + (Ω). Then, there exits a minimizing sequence {u + n } ⊆ M λ + (Ω) such that

n→∞ lim J λ (u + n ) = inf

u∈M

λ+

(Ω) J λ (u) = α + λ < 0.

Since J λ is coercive, u + n is bounded in W 0 1,p(x) (Ω). Thus, we may assume that, without loss of generality, u + n * u + 0 in W 0 1,p(x) (Ω) and by the compact embeddings we have

u + n → u + 0 in L q(x) a(x) (Ω) ,

(12)

and

u + n → u + 0 in L h(x) b(x) (Ω) .

Now, we shall prove u + n → u + 0 in W 0 1,p(x) (Ω). Otherwise, suppose u + n 9 u + 0 in W 0 1,p(x) (Ω). Then

Z

¯ ¯∇u + 0 ¯

¯ p(x) dx < lim

n→∞ inf Z

¯ ¯∇u + n ¯

¯ p(x) dx.

Moreover, by the compact embeddings we have Z

a(x) ¯

¯u + 0 ¯

¯ q(x) dx = lim

n→∞ inf Z

a(x) ¯

¯u + n ¯

¯ q(x) dx, Z

b(x) ¯

¯u + 0 ¯

¯ h(x) dx = lim

n→∞ inf Z

b(x) ¯

¯u + n ¯

¯ h(x) dx.

Using the fact that hJ λ 0 (u + n ), u + n i = 0 and Theorem 2.8, we can write the followings

J λ (u + n ) ≥ µ 1

p + 1 h

¶ Z

¯ ¯∇u + n ¯

¯ p(x) dx+λ µ 1

h 1 q

¶Z

a(x) ¯

¯u + n ¯

¯ q(x) dx,

n→∞ lim J λ (u + n ) ≥ µ 1

p + 1 h

n→∞ lim Z

¯ ¯∇u + n ¯

¯ p(x) dx

+ λ µ 1

h 1 q

n→∞ lim Z

a(x) ¯

¯u + n ¯ ¯ q(x) dx,

α + λ = inf

u∈M

λ+

J λ (u)

>

µ 1 p + 1

h

¶ °

°u + 0 °

° p

+ c 7 λ µ 1

h 1 q

¶ ³° °u + 0 °

° q

+ °

°u + 0 °

° q

+

´ , since p > q + , for °

°u + 0 °

° > 1, we have α + λ = inf

u∈M

λ+

J λ (u) > 0.

However, in Lemma 3.4 it was showed that for any u ∈ M λ + (Ω), J λ (u) < 0.

So, this is a contradiction. Hence, u + n → u + 0 in W 0 1,p(x) (Ω) and J λ (u + 0 ) = lim

n→∞ J λ (u + n ) = inf

u∈M

λ+

(Ω) J λ (u).

Thus, u + 0 is a minimizer for J λ on M λ + (Ω) . ¤

Lemma 3.6. If 0 < λ < λ 1 , then for all u ∈ M λ (Ω), J λ (u) > 0.

(13)

Proof. Let u ∈ M λ (Ω). By definition of J λ (u) and (3.1), we have J λ (u) ≥ 1

p + Z

|∇u| p(x) dx − λ q

Z

a(x) |u| q(x) dx − 1 h

Z

b (x) |u| h(x) dx,

and Z

b (x) |u| h(x) dx = Z

|∇u| p(x) dx − λ Z

a (x) |u| q(x) dx.

Using the two expressions above, it follows J λ (u) ≥ 1

p + Z

|∇u| p(x) dx − λ q

Z

a(x) |u| q(x) dx

1 h

 Z

|∇u| p(x) dx − λ Z

a (x) |u| q(x) dx

µ 1

p + 1 h

¶ Z

|∇u| p(x) dx + λ µ 1

h 1 q

¶ Z

a(x) |u| q(x) dx.

By Propositions 2.2, 2.9, and the condition p > q + , it follows J λ (u) ≥

µ 1 p + 1

h

kuk p

+ c 10 λ µ 1

h 1 q

kuk q+

µ h − p +

p + h + c 10 λ q − h q h

kuk p

.

So, if we choose λ < q

( h

−p

+

)

c

10

p

+

(h

−q

) , we get J λ (u) > 0. Moreover, if we consider the facts M λ (Ω) = M λ + (Ω)∪M λ (Ω) (see Lemma 3.3), M λ + (Ω)∩M λ (Ω) = ∅,

and Lemma 3.4, we must have u ∈ M λ (Ω) . ¤

Theorem 3.7. If 0 < λ < λ 1 , there exists a minimizer of J λ on M λ (Ω).

Proof. Since J λ is bounded below on M λ (Ω) and so on M λ (Ω), then there exits a minimizing sequence {u n } ⊆ M λ (Ω) such that

n→∞ lim J λ (u n ) = inf

u∈M

λ

(Ω) J λ (u) = α λ > 0.

Since J λ is coercive, u n is bounded in W 0 1,p(x) (Ω). Thus, we may assume that, without loss of generality, u n * u 0 in W 0 1,p(x) (Ω) and by the compact embeddings we have

u n → u 0 in L q(x) a(x) (Ω) , and

u n → u 0 in L h(x) b(x) (Ω) .

(14)

Moreover, if u 0 ∈ M λ (Ω), then there is a constant t > 0 such that tu 0

∈ M λ (Ω) and J λ (u 0 ) ≥ J λ (tu 0 ). Indeed, since I λ 0 (u) =

Z

p (x) |∇u| p(x) dx − λ Z

q (x) a (x) |u| q(x) dx − Z

h (x) b (x) |u| h(x) dx,

then, I λ 0 (tu 0 ) =

Z

p (x) ¯

¯∇tu

0

¯

¯

p(x)

dx − λ Z

q (x) a (x) ¯

¯tu

0

¯

¯

q(x)

dx − Z

h (x) b (x) ¯

¯tu

0

¯

¯

h(x)

dx

t

p+

p

+

Z

¯ ¯∇u

0

¯

¯

p(x)

dx − λt

q

q

Z

a (x) ¯

¯u

0

¯

¯

q(x)

dx − t

h

h

Z

b (x) ¯

¯u

0

¯

¯

h(x)

dx .

Since q < p + < h , and by the assumptions on a and b, it follows I λ 0 (tu 0 ) < 0.

Hence, by the definition of M λ (Ω), tu 0 ∈ M λ (Ω).

Now, we shall show u n → u 0 in W 0 1,p(x) (Ω). Otherwise, suppose u n 9 u 0 in W 0 1,p(x) (Ω). Then using the fact that

Z

¯ ¯∇u 0 ¯

¯ p(x) dx < lim

n→∞ inf Z

¯ ¯∇u n ¯

¯ p(x) dx,

we have, J λ (tu 0 ) ≤ t p

+

p Z

¯ ¯∇u 0 ¯ ¯ p(x) dx − λ t q

q + Z

a(x) ¯

¯u 0 ¯ ¯ q(x) dx − t h

h + Z

b(x) ¯

¯u 0 ¯ ¯ h(x) dx

< lim

n→∞

 t

p

+

p

Z

¯ ¯∇u

n

¯ ¯

p(x)

dx − λ t

q

q

+

Z

a(x) ¯

¯u

n

¯ ¯

q(x)

dx − t

h

h

+

Z

b(x) ¯

¯u

n

¯ ¯

h(x)

dx

≤ lim

n→∞ J λ (tu n ) ≤ lim

n→∞ J λ (u n ) = inf

u∈M

λ

(Ω) J λ (u) = α λ . This implies that J λ (tu 0 ) < inf

u∈M

λ

(Ω) J λ (u) = α λ , which is a contradiction.

Hence, u n → u 0 in W 0 1,p(x) (Ω) and so J λ (u 0 ) = lim

n→∞ J λ (u n ) = inf

u∈M

λ

(Ω) J λ (u).

Thus, u 0 is a minimizer for J λ on M λ (Ω). ¤ Corollary 3.8. By Theorems 3.5 and 3.7, we conclude that there exists u + 0 M λ + (Ω) and u 0 ∈ M λ (Ω) such that J λ (u + 0 ) = inf

u∈M

λ+

(Ω) J λ (u) and J λ (u 0 ) = inf

u∈M

λ

(Ω) J λ (u). Moreover, since J λ (u ± 0 ) = J λ (|u ± 0 |) and ¯

¯u ± 0 ¯

¯ ∈ M λ ± (Ω), we

may assume u ± 0 ≥ 0. By Theorem 3.1, u ± 0 are critical points of J λ on W 0 1,p(x) (Ω)

and hence are weak solutions (and so by standard regularity results classical

(15)

solutions) of (E λ ). Finally, by the Harnack inequality due to [25, 27], we ob- tain that u ± 0 are positive solutions of (E λ ).

References

[1] E. Acerbi and G. Mingione, Regularity results for stationary electro-rheological fluids, Arch. Ration. Mech. Anal. 164 (2002), no. 3, 213–259.

[2] G. A. Afrouzi, S. Mahdavi, and Z. Naghizadeh, The Nehari manifold for p-Laplacian equation with Dirichlet boundary condition, Nonlinear Anal. Model. Control 12 (2007), no. 2, 143–155.

[3] A. Ambrosetti, H. Brezis and G. Cerami, Combined effects of concave and convex non- linearities in some elliptic problems, J. Funct. Anal. 122 (1994), no. 2, 519–543.

[4] K. J. Brown and Y. Zhang, The Nehari manifold for a semilinear elliptic equation with a sign-changing weight function, J. Differential Equations 193 (2003), no. 2, 481–499.

[5] O. M. Buhrii and R. A. Mashiyev, Uniqueness of solutions of the parabolic variation inequality with variable exponent of nonlinearity, Nonlinear Anal. 10 (2009), 2325–2331.

[6] J. Chabrowski and Y. Fu, Existence of solutions for p(x)-Laplacian problems on a bounded domain, J. Math. Anal. Appl. 306 (2005), no. 2, 604–618.

[7] L. Diening, Theoretical and Numerical Results for Electrorheological Fluids, Ph. D.

thesis, University of Frieburg, Germany, 2002.

[8] D. Edmunds and J. Rakosnik, Sobolev embeddings with variable exponent, Studia Math.

143 (2000), no. 3, 267–293.

[9] A. El Hamidi, Existence results to elliptic systems with nonstandard growth conditions, J. Math. Anal. Appl. 300 (2004), no. 1, 30–42.

[10] X. L. Fan, Solutions for p(x)-Laplacian Dirichlet problems with singular coefficients, J.

Math. Anal. Appl. 312 (2005), no. 2, 464–477.

[11] X. L. Fan, J. S. Shen, and D. Zhao, Sobolev embedding theorems for spaces W

k,p(x)

(Ω), J. Math. Anal. Appl. 262 (2001), no. 2, 749–760.

[12] X. L. Fan and D. Zhao, On the spaces L

p(x)

(Ω) and W

m,p(x)

(Ω), J. Math. Anal. Appl.

263 (2001), no. 2, 424–446.

[13] X. L. Fan and Q. H. Zhang, Existence of solutions for p(x)-Laplacian Dirichlet problem, Nonlinear Anal. 52 (2003), no. 8, 1843–1852.

[14] X. L. Fan, Q. Zhang, and D. Zhao, Eigenvalues of p(x)-Laplacian Dirichlet problem, J.

Math. Anal. Appl. 302 (2005), no. 2, 306–317.

[15] T. C. Halsey, Electrorheological fluids, Science 258 (1992), 761–766.

[16] P. Harjulehto, P. H¨ ast¨ o, M. Koskenoja, and S. Varonen, The Dirichlet energy integral and variable exponent Sobolev spaces with zero boundary values, Potential Anal. 25 (2006), no. 3, 205–222.

[17] P. H¨ ast¨ o, The p(x)-Laplacian and applications, J. Anal. 15 (2007), 53–62.

[18] O. Kov˘ aˇcik and J. R˘ akosnik, On spaces L

p(x)

and W

k,p(x)

, Czechoslovak Math. J.

41(116) (1991), no. 4, 592–618.

[19] R. A. Mashiyev, Some properties of variable Sobolev capacity, Taiwanese J. Math. 12 (2008), no. 3, 671–678.

[20] M. Mih˘ ailescu, Existence and multiplicity of solutions for an elliptic equation with p(x)- growth conditions, Glasg. Math. J. 48 (2006), no. 3, 411–418.

[21] M. Mih˘ ailescu and V. R˘ adulescu, A multiplicity result for a nonlinear degenerate prob- lem arising in the theory of electrorheological fluids, Proc. R. Soc. Lond. Ser. A Math.

Phys. Eng. Sci. 462 (2006), no. 2073, 2625–2641.

[22] , On a nonhomogeneous quasilinear eigenvalue problem in Sobolev spaces with

variable exponent, Proc. Amer. Math. Soc. 135 (2007), no. 9, 2929–2937.

(16)

[23] S. Ogras, R. A. Mashiyev, M. Avci, and Z. Yucedag, Existence of solutions for a class of elliptic systems in R

N

involving the (p(x), q(x))-Laplacian, J. Inequal. Appl. 2008 (2008), Art. Id 612938, 16 pp.

[24] M. R˚ uˇziˇcka, Electrorheological Fluids: modeling and mathematical theory, Springer Lec- ture Notes in Math. Vol. 1748, Springer Verlag, Berlin, Heidelberg, New York, 2000.

[25] N. S. Trudinger, On Harnack type inequalities and their application to quasilinear el- liptic equations, Comm. Pure Appl. Math. 20 (1967), 721–747.

[26] T. F. Wu, Multiplicity of positive solution of p-Laplacian problems with sign-changing weight functions, Int. J. Math. Anal. (Ruse) 1 (2007), no. 9-12, 557–563.

[27] X. Zhang and X. Liu, The local boundedness and Harnack inequality of p(x)-Laplace equation, J. Math. Anal. Appl. 332 (2007), no. 1, 209–218.

[28] V. V. Zhikov, Averaging of functionals of the calculus of variations and elasticity theory, (russian) Izv. Akad. Nauk SSSR Ser. Mat. 50 (1986), no. 4, 675–710, 877.

Rabil A. Mashiyev

Department of Mathematics Faculty of Science and Arts Dicle University

21280-Diyarbakir, Turkey

E-mail address: [email protected] Sezai Ogras

Department of Mathematics Faculty of Science and Arts Dicle University

21280-Diyarbakir, Turkey

E-mail address: [email protected] Zehra Yucedag

Department of Mathematics Faculty of Science and Arts Dicle University

21280-Diyarbakir, Turkey E-mail address: [email protected] Mustafa Avci

Department of Mathematics Faculty of Science and Arts Dicle University

21280-Diyarbakir, Turkey

E-mail address: [email protected]

참조

관련 문서

In this paper, we investigate a long-time behavior of global solutions to the initial boundary problem of nonlinear dispersive-dissipative wave equation with time-dependent

웹 표준을 지원하는 플랫폼에서 큰 수정없이 실행 가능함 패키징을 통해 다양한 기기를 위한 앱을 작성할 수 있음 네이티브 앱과

with the experimental C versus t data. If the fit is unsatisfactory, another rate equation is guessed and tested. Integral method is especially useful for fitting simple

The index is calculated with the latest 5-year auction data of 400 selected Classic, Modern, and Contemporary Chinese painting artists from major auction houses..

The intent of the Strategy is to design, foster and build synergies for activities and investments in geospatial information management in the United Nations

The key issue is whether HTS can be defined as the 6th generation of violent extremism. That is, whether it will first safely settle as a locally embedded group

Where possible, replace Amazon EC2 workloads with AWS managed services that either don’t require you to make any capacity decisions (such as ELB, Amazon CloudFront, Amazon

1 John Owen, Justification by Faith Alone, in The Works of John Owen, ed. John Bolt, trans. Scott Clark, &#34;Do This and Live: Christ's Active Obedience as the