Volume 2016, Issue 1 3149482
Research Article
Open Access

Multiplicity Results for the p(x)-Laplacian Equation with Singular Nonlinearities and Nonlinear Neumann Boundary Condition

K. Saoudi

Corresponding Author

K. Saoudi

College of Sciences at Dammam, University of Dammam, Dammam 31441, Saudi Arabia uod.edu.sa

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M. Kratou

M. Kratou

College of Sciences at Dammam, University of Dammam, Dammam 31441, Saudi Arabia uod.edu.sa

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S. Alsadhan

S. Alsadhan

College of Sciences at Dammam, University of Dammam, Dammam 31441, Saudi Arabia uod.edu.sa

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First published: 07 November 2016
Citations: 4
Academic Editor: Julio D. Rossi

Abstract

We investigate the singular Neumann problem involving the p(x)-Laplace operator: (Pλ){−Δp(x)u+|u|p(x)−2u   = 1/uδ(x) + f(x, u), in  Ω;   u > 0,   in  Ω;   |∇u|p(x)−2u/ν = λuq(x),   on  Ω}, where is a bounded domain with C2 boundary, λ is a positive parameter, and p(x), q(x), δ(x), and f(x, u) are assumed to satisfy assumptions (H0)(H5) in the Introduction. Using some variational techniques, we show the existence of a number Λ ∈ (0, ∞) such that problem (Pλ) has two solutions for λ ∈ (0, Λ), one solution for λ = Λ, and no solutions for λ > Λ.

1. Introduction

The purpose of this paper is to study the existence of multiple solutions for the following inhomogeneous singular Neumann problem involving the p(x)-Laplace operator:
(1)
Here (N ≥ 2) is a bounded domain with C2 boundary; λ is a positive parameter. For any continuous and bounded function a we define a+≔sup⁡a(x) and a≔inf⁡a(x). Associated with problem (Pλ) we have the singular functional given by
(2)
where .

Definition 1. uW1,p(x)(Ω) is called a generalized solution of the equation

(3)
if for all
(4)

Obviously, every weak solution of problem (Pλ) is also a generalized solution of (3).

The operator Δp(x)u≔div⁡(|∇u|p(x)−2u) is called p(x)-Laplace where p is a continuous nonconstant function. This differential operator is a natural generalization of the p-Laplace operator Δpu≔div⁡(|∇u|p−2u), where p > 1 is a real constant. However, the p(x)-Laplace operator possesses more complicated nonlinearity than p-Laplace operator, due to the fact that Δp(x) is not homogeneous. This fact implies some difficulties; for example, we cannot use the Lagrange Multiplier Theorem in many problems involving this operator.

The study of differential and partial differential equations involving variable exponent is a new and an interesting topic. The interest in studying such problems was stimulated by their applications in elastic mechanics, fluid dynamics, electrorheological fluids, image processing, flow in porous media, calculus of variations, nonlinear elasticity theory, heterogeneous porous media models (see Acerbi and Mingione [1], Diening [2]), and so forth. These physical problems were facilitated by the development of Lebesgue and Sobolev spaces with variable exponent.

At this point, we briefly recall related existence and multiplicity results for elliptic equations with Neumann boundary conditions. Neumann type problems are studied in [36] and references therein. The multiplicity result for Neumann problem with Sobolev critical nonlinearity has been studied in [5] where authors considered the problem
(5)
Here , N ≥ 3, and 0 < q < 1 < p ≤ 2N/(N − 2). They proved the existence of such that problem (5) admits at least two solutions for all , one solution when , and no solutions for The problem in two dimensions has been considered in [6] where the authors extended the results obtained by [5].

Results for p(x)-Laplacian problems Neumann boundary conditions are rare (see [7, 8]). In [7], Fan and Deng studied the Neumann problems with p(x)-Laplace operator and the nonlinear potential f(x, u) under appropriate assumptions. By using the subsupersolution method and variation method, the authors get the multiplicity of positive solutions. In [8], Sreenadh and Tiwari extend previous works on nonlinear parametric problems with the p(x)-Laplace operator to the case where the Neumann boundary condition is nonlinear. Precisely, under supplementary hypotheses on p, q, the authors show that there exists a finite number Λ such that the posed problem has two solutions for λ ∈ (0, Λ), one solution for λ = Λ, and no solutions for λ > Λ.

Before stating our main results, we make the following assumptions throughout this paper:
  • (H0)

    , 1 < pp+ < N, and . As usual, p(x) = Np(x)/(Np(x)).

  • (H1)

    0 < q(x) ∈ Cβ(Ω) for some β ∈ (0,1) satisfying 0 ≤ q+ + 1 < p(p/p+).

  • (H2)

    satisfying 0 < δδ+ < 1.

Let be a nondecreasing Carathéodory function satisfying the following:
  • (H3)

    f(x, 0) = 0 and f(x, t)t ≥ 0 for all .

  • (H4)

    There exist C1, C2 > 0 such that, for γ > 0, with p+ − 1 < γ and p+ < a.

    (6)

  • (H5)

    There exist a constant M > 0 and θ > p+ such that

    (7)

  • Next we describe in a more precise way our main results.

Theorem 2. Assume that (H0)–(H5) hold and a(x) ≤ p(x) = Np(x)/(Np(x)) in (6). Then there exists Λ > 0 with the following properties:

  • (1)

    Problem (Pλ) has a solution uλ for every λ ∈ (0, Λ).

  • (2)

    Problem (Pλ) has a solution if λ = Λ.

  • (3)

    Problem (Pλ) does not have any solution if λ > Λ.

Theorem 3. Assume that (H0)–(H5) hold and a(x) < p(x) in (6). Then, problem (Pλ) has at least two distinct solutions uλ(x) and vλ(x) for every λ ∈ (0, Λ).

This paper is organized as follows. In Section 2, we will recall some basic facts about the variable exponent Lebesgue and Sobolev spaces which we will use later. Proofs of our results will be presented in Sections 3 and 5.

2. Generalized Lebesgue-Sobolev Spaces Setting

To deal with the p(x)-Laplacian problem, we need to introduce some functional spaces Lp(·)(Ω), W1,p(·)(Ω), and properties of the p(x)-Laplacian which we will use later. Denote by S(Ω) the set of all measurable real-valued functions defined in Ω. Note that two measurable functions are considered as the same element of S(Ω) when they are equal almost everywhere. Let
(8)
with the norm
(9)
The space (Lp(·)(Ω), |·|p(·)) becomes a Banach space. We call it variable exponent Lebesgue space. Moreover, this space is a separable, reflexive, and uniform convex Banach space; see [9, Theorems 1.6, 1.10, and 1.14].
The variable exponent Sobolev space
(10)
can be equipped with the norm
(11)
Note that is the closure of in W1,p(·)(Ω) under the norm ‖u‖ = |∇u|p(·). The spaces W1,p(·)(Ω) and are separable, reflexive, and uniform convex Banach spaces (see [9, Theorem 2.1]). The inclusion between Lebesgue spaces also generalizes naturally: if 0 < |Ω| < and p1, p2 are variable exponents so that p1(x) ≤ p2(x) almost everywhere in Ω then there exists the continuous embedding .
We denote by Lq(x)(Ω) the conjugate space of Lp(x)(Ω), where 1/q(x) + 1/p(x) = 1. For uLp(x)(Ω) and vLq(x)(Ω), the Hölder type inequality
(12)
holds true.
An important role in manipulating the generalized Lebesgue spaces is played by the modular of the Lp(x)(Ω) space, which is the mapping defined by
(13)
If (un), uLp(x)(Ω) and p+ < , then the following relations hold true.

Lemma 4. Consider the following:

(14)

The following result generalizes the well-known Sobolev embedding theorem.

Theorem 5 (see [10], [11].)Let be an open bounded domain with Lipschitz boundary and assume that with p(x) > 1 for each . If and p(x) ≤ r(x) ≤ p(x) for all , then there exists a continuous embedding W1,p(x)(Ω)↪Lr(x)(Ω). Also, the embedding is compact r(x) < p(x) almost everywhere in , where

(15)

Now, we recall the following boundary trace embedding theorem from [12].

Theorem 6. Let be an open bounded domain with Lipschitz boundary. If qC(Ω) such that

(16)
then W1,p(x)Lq(x)(Ω).

Next we give a comparison principle as follows.

Lemma 7 (see [8], Lemma 3.2.)Let u, vW1,p(·)(Ω) be nonnegative functions satisfying

(17)
Then uv almost everywhere in Ω.

We recall the following strong maximum principle from [13].

Theorem 8. Let , for some 0 < β < 1, satisfy 0≨u, 0≨v and

(18)
with u = v = 0 on Ω, where g, hL(Ω) are such that 0 ≤ g < h pointwise everywhere in Ω. If
(19)
where n is the inward unit normal on Ω, then, the following strong comparison principle holds:
(20)

3. Existence of a Solution

In this section, we show the existence of a local minimum for Eλ in a small neighborhood of the origin in W1,p(x)(Ω). Firstly, let us define
(21)

Lemma 9. There exists λ0 > 0 such that (Pλ) admits a solution for λ < λ0.

Proof. Using (14) and the embeddings in Theorem 5, we estimate Eλ(u) for as follows:

(22)

Hence, noting that 0 < δ+ < 1 and 1 − δ+ < p+ < a, we can choose r0 > 0 small enough, and there exists δ0 > 0 such that

(23)
Moreover, since W1,p(x)(Ω)↪L1−δ(x)(Ω), we have, for λ > 0, small enough,
(24)
Set
(25)
Now, note that, for t → 0+ and uW1,p(x)(Ω), we have
(26)

Since 1 − δ+ < p+ < θ, this implies that Eλ(tu) → − as t. Thus, Now, let be a minimizing sequence for c0. Then for r0 ∈ (0, r). Now by the Ekeland variational principle, there exists a sequence {vj} such that and

(27)
Moreover, using the Brézis-Lieb lemma in [14] combined with the p(x) version of Theorem 2.1 in Boccardo and Murat [15], it follows that ∇vj(x)→∇uλ(x) for almost every xΩ,
(28)
Hence, from (28) and the compact boundary trace embedding in Theorem 5, we get Eλ(vj) ≥ Eλ(uλ) + oj(1). Thus, it follows that Eλ(uλ) = c0 < 0. Hence uλ≢0 and it is a local minimizer of Eλ in W1,p(x)(Ω).

We prove now the existence of positive solution to (Pλ) for 0 < λ < Λ. Precisely, we have the following result.

Lemma 10. Problem (Pλ) possesses a solution uλ for 0 < λ < Λ.

Proof. Fix 0 < λ < λ2 < Λ. λ2 such that there exist solutions to (Pλ) for λ = λ2, say . Note that is a supersolution for (Pλ). It is clear that 0 is not a local minimizer of Eλ on since Eλ(0) = 0 and Eλ(tv) < 0 for t → 0+. Now, we show the existence of a local minimizer of the functional energy. For this, we use the cut-off argument. Define

(29)
Also define the functional by
(30)
where , , and From the dominated convergence and the compact boundary trace embedding in Theorem 5, it is easy to see that is bounded below and is weakly lower semicontinuous in W1,p(x)(Ω). Then, there exists such that achieves its global minimum in W1,p(x)(Ω). Moreover, since is from Lemma A.4, solves the equation
(31)

Now, using the strong maximum principle (see Theorem 8) and since 0 is not a local minimizer of Eλ on By the definition of , and we have

(32)
Again, by the strong comparison principle (see Lemma 7), we conclude that in Ω and on Ω. Hence is a solution to (Pλ). This completes the proof of Lemma 10.

Now, we show the following result.

Lemma 11. There exists at least one positive weak solution for λ = Λ to problem (Pλ).

Proof. Let , λkΛ as k, and be a solution of such that for all xΩ. Now, taking as test function in , we get

(33)
Moreover, as , we have
(34)
It follows that
(35)
Now, from (7) there exists C > 0 such that, for θ > p+ and for all t > 0,
(36)
Moreover, using Theorem 4.2 in [16], we get the existence of the constants C1 > 0, C2 > 0 such that
(37)
where θ1 = maxd(x)≤σ⁡(p(x)/(p(x) − 1 + δ(x))),   θ2 = mind(x)≤σ⁡(p(x)/(p(x) − 1 + δ(x))), and d(x) = dist⁡(x, Ω). On the other hand, we recall the following inequality due to Lieberman [17]. There exists a constant K(Ω) > 0 such that
(38)

Inserting (36), (37), and (38) in (33), we get It follows that is bounded in W1,p(x)(Ω) since for all xΩ. Without loss of generality, in W1,p(x)(Ω) and then by the Sobolev imbedding in Lq(x)(Ω) and for a.e. xΩ. By the L(Ω)-regularity results of [13], the boundedness of implies the boundedness of By the C1,α(Ω)-regularity Theorem 16, the boundedness of implies the boundedness of , where α ∈ (0,1) is a constant. Thus, we have in For every vW1,p(x)(Ω), since is a solution of problem , we have that, for each k,

(39)
Passing to the limit in (39) as k yields
(40)
which shows that uΛ is a solution of (PΛ). Obviously uΛ ≥ 0 and uΛ≢0. Hence uΛ is a positive solution of (PΛ) in W1,p(x)(Ω). This completes the proof of Lemma 11.

Then we prove the following nonexistence result.

Lemma 12. Consider the following:

Λ < .

Proof. Let uλ be a solution of (Pλ). Taking φ ≡ 1 as a test function in the weak formulation of (Pλ), we get

(41)
On the other hand, we have
(42)
Using assumption (H2) we have , and using (6) we have Therefore, from (41) and (42) we get
(43)
Now, since p+ − 1 < γ and −δ+ < γ, by the embedding of Lγ(Ω) into and by the embedding of Lγ(Ω) into we obtain
(44)
Substituting (44) in (43) we get
(45)
Hence, is bounded by a constant independent of λ. Now, taking as a test function in the weak formulation of (Pλ) and using (H2) we get
(46)
Now since
(47)
it follows that Λ is finite. The proof of Lemma 12 is now completed.

Proof of Theorem 2. Theorem 2 follows from Lemmas 10, 11, and 12.

Now, we prove that the solution of problem (Pλ) obtained in Lemma 10 is a local minimum for the functional energy associated to problem (Pλ). Precisely, we have the following result.

Lemma 13. Let uλ be the weak solution of problem (Pλ) obtained in Lemma 10. Then, uλ is a local minimum for .

Proof. Fix 0 < λ1 < λ < λ2 < Λ and let be solutions to (Pλ) for λ = λ1 and λ = λ2, respectively, such that . By Lemma 7,   on Define the following cut-off functions:

(48)
Then the corresponding functional given by
(49)
where , , and (xΩ). Firstly, from Lemma A.4   is Then, it is simple to see that is coercive and bounded below. Let uλ denote the global minimum of on W1,p(x)(Ω) which satisfies the equation
(50)
Therefore, from the regularity results Theorem 16, we conclude that uλ is in for some 0 < α < 1. Now, using (H2) and since f(x, t) is nondecreasing, by the definition of , , and we have
(51)
Again, by the strong comparison principle (see Lemma 7), we conclude that in Ω. Let We claim that β > 0. If not, then there exists xΩ such that and But this contradicts the boundary data as λ1λ2. Therefore, if then in since on the set Hence uλ is a local minimum for This completes the proof of Lemma 13.

4. C1 versus W1,p(x) Local Minimizers of the Energy

The following lemma is crucial in showing multiplicity of solutions. It has been shown in the case p = 2 in [18] for the case of critical growth functionals Eλ: , , N ≥ 3 and later for critical growth functionals , 1 < p < N, , N ≥ 3 in [19]. A key feature of these latter works is the uniform C1,α estimate they obtain for equations like (Pϵ) but involving two p-Laplace operators. Using constraints based on Lp-norms rather than Sobolev norms as in [19], the equations for which uniform estimates are required can be simplified to a standard type involving only one p-Laplace operator. This approach was followed in [20] in the subcritical case, in [21] in the critical case, in [2224], and also in this work to deal with the boundary value problem involving the nonlinear p(x)-Laplacian case. More precisely, we have the following result.

Lemma 14. Suppose that conditions (H0)–(H5) are satisfied. Let satisfying

(52)
be a local minimizer of Eλ in topology. Then, u0 is a local minimum of Eλ in W1,p(x)(Ω) also.

For proving Lemma 14, we will need the following uniform L-estimates for a family of solutions to (Pϵ).

Proposition 15. Let be a family of solutions to (Pϵ), where u0 satisfies (52) and solves (Pλ). Let γ > 1 be such that

(53)
Then,
(54)

The proof of Proposition 15 is a consequence of the results proved in Appendix  A in [13]. Hence, the regularity results of Saoudi and Ghanmi [13] give the following regularity result for weak solutions to problem (Pλ).

Theorem 16. Let uW1,p(x)(Ω)∩L(Ω) be a solution to problem (Pλ). Then, there exists such that any weak solution to problem (Pλ) belongs to for some α ∈ (0,1).

Proof of Lemma 14. Assume that the conclusion of Lemma 14 is not true. We define the following constraint for each ϵ > 0:

(55)
We consider the following constraint minimization problem:
(56)
Firstly, clearly Iϵ > −. Moreover, we note that is a convex set. Using the trace embeddings we see that is also a closed set in W1,p(x)(Ω) which implies that is weakly closed in W1,p(x)(Ω); with the fact that Eλ is weakly low semicontinuous in W1,p(x)(Ω), it follows that for ϵ   ∈ (0,1)  Iϵ is achieved on some ; that is
(57)
Moreover, since and , we may assume that uϵ ≥ 0.

We now consider the following two cases.

(1) Let ρ(uϵ) < ϵ. Then uϵ is also a local minimizer of Eλ in W1,p(x)(Ω). We now show that Eλ admits Gâteaux derivatives on uϵ to derive that uϵ satisfies the Euler-Lagrange equation associated with Eλ. For this, according to Lemma A.2, in the Appendix, we need to prove that such that

(58)
where d(x)≝dist⁡(x, Ω). To prove (58), we argue by contradiction: ∀η > 0 let
(59)
and suppose that Ωη has a nonzero measure.

Let and for 0 < t ≤ 1 set ξ(t) = Eλ(uϵ + tuη). Then, there exists c(t) satisfying c(t) > ηt such that inf⁡((uϵ + tuη)/d(x)) ≥ c(t)  for    t > 0. Then, from Lemma A.4  ξ is differentiable for 0 < t ≤ 1 and . Thus,

(60)
From (H1)(H3), we see that
(61)
for η > 0 small enough.

Now, since sδ(x) + f(x, s) + λsq(x) is nonincreasing for 0 < s small enough uniformly to xΩ (by (H1)(H3)) and from the monotonicity of the operator −Δp(x)u + |u|p(x)−1u, we have that for 0 < η small enough 0 ≤ ξ(1) − ξ(t). Therefore, from Taylor’s expansion and since ρ(uϵ) ≤ ϵ, there exists 0 < γ < 1 such that

(62)
Letting t = γ we have ξ(γ) ≤ ξ(1) < 0. We obtain a contradiction with (62) and then uϵηd(x) for some η > 0 (which depends a priori on ϵ). Since uϵ is a local minimizer of Eλ and Eλ is Gâteaux differentiable in uϵ, we get that is defined and Recalling that is the solution to the pure singular problem given by Theorem 4.2 in [16] and from the weak comparison principle, there exist C1 > 0, C2 > 0 such that
(63)
where θ1 = maxd(x)≤σ⁡(p(x)/(p(x) − 1 + δ(x))), for some η > 0 (independent of ϵ). Since and from the fact that uϵ satisfies (Pλ), we get that is uniformly bounded in W1,p(x)(Ω). Now, using Proposition 15 and Theorem 16, we get
(64)
and as ϵ → 0+
(65)
which contradicts the fact that u0 is a local minimizer in .

Now, we deal with the second case.

(2) ρ(uϵ) = ϵ: we again show that uϵηd(x) in Ω for some η > 0. Taking ,    ξ(t) = Eλ(uϵ + tuη), we obtain as above that     ξ(t) ≤ ξ(1) < 0 for 0 < t < 1 and 0 < η small enough.

Then ξ(t) = Eλ(uϵ + tuη) is decreasing. This implies that Eλ(uϵ) > Eλ(uϵ + tuη) for t > 0 and using (52)

(66)
This yields a contradiction with the fact that uϵ is a global minimizer of Eλ on . In this case, using Lemma A.4 and from the Lagrange multiplier rule we have
(67)

We first show that μϵ ≤ 0. We argue by contradiction. Suppose that μϵ > 0; then there exists φW1,p(x)(Ω) such that

(68)
and then for t small we have
(69)
This contradicts the fact that uϵ is a global minimizer of Eλ in .

We deal now with the two following cases.

Case 1 (infϵ∈(0,1)μϵl > −). In this case, we write (67) in its PDE form as

(70)

In this case, from (57), we have that Hence, we can apply Proposition 15 to conclude that for some constant K > 0 independent of ϵ. Therefore, using Theorem 16 we conclude that for some constant C > 0 independent of ϵ and as ϵ → 0+

(71)
which contradicts the fact that u0 is a local minimizer in .

Now, we deal with the second case.

Case 2 (infϵ∈(0,1)μϵ = −). From above, we can assume that μϵ ≤ −1 for 0 < ϵ small enough. Furthermore, we can find a number M > 0 independent of ϵ > 0 and , such that (1/sδ(x) + f(x, s) + με|s|α(x)−2s) and are negative for all |s| ≥ M. Then, from the weak comparison principle (see Lemma 7 and using (uεM) + as test function) we have that for ϵ > 0 small enough. Now, since u0W1,p(x)(Ω) is a C1 local minimizer, u0 is a weak solution to (Pλ); that is, satisfies ess infKu0 > 0 over every compact set KΩ and

(72)
for all . Therefore, for every function wW1,p(x)(Ω), u0 satisfies
(73)
Similarly,
(74)
Now, substracting the above relations with w = (uϵu0) | uϵu0|β−1, with β > 1, as a test function in (Pϵ), integrate by parts and use the fact that u ↦ −Δp(x)u+|u|p(x)−1u is a monotone operator to obtain
(75)
Using the bounds of uϵ, u0 we get
(76)
where C does not depend on β and ϵ. Now, using Hölder’s inequality and the bounds of uϵ combined with Lemma 4 we obtain
(77)
Therefore
(78)
Thus for any β > 1
(79)
Passing to the limit in (79) β → + we get
(80)
Then, using (80) combined with Proposition 15, the uniform L bounds for in Ω as well as Ω, we get that the right-hand side terms in (Pε) are uniformly bounded in L(Ω) and in L(Ω) from which as in the first case we obtain that uϵ  (0 < ϵ ≤ 1) is bounded in independently of ϵ. Finally, using Ascoli-Arzela Theorem we find a sequence ϵn → 0+ such that
(81)
It follows that, for ϵ > 0 sufficiently small,
(82)
which contradicts the fact that u0 is a local minimizer of Eλ for the topology. The proof of Lemma 14 is now completed.

5. Existence of a Second Weak Solution for 0   <   λ   <   Λ

In this section, we fix λ ∈ (0, Λ) and let 0 < λ1 < λ < λ2 < Λ, and be as in Section 3. Now, we are able to show the existence of a second solution using the generalized Mountain Pass Theorem. Since the functional is not C1, we use the cut-off functional defined in (86). Define the cut-off functions

by
(83)
by
(84)
by
(85)
and define now the corresponding functional given by
(86)
where , and . Firstly, we prove the following lemma on compactness of Palais-Smale sequences.

Lemma 17. The functional satisfies the Palais-Smale condition.

Proof. Let {un} be a (PS) sequence; namely, is bounded and when n. Then,

(87)
Now, we estimate the boundary term from above as follows:
(88)
Hence, taking (88) in (87) and using (H2) combined with (7) we get
(89)
Now, using Lemma 4 and the fact that , we get
(90)
Hence, is bounded. Without loss of generality, we assume that there exists a subsequence of {un} such that unu0. Therefore, using Theorems 5 and 6 we get
(91)
Observe that
(92)
We already know that
(93)
Using (91), we obtain
(94)
This together with the convergence of unu0 in W1,p(x)(Ω) implies that unu0 strongly in W1,p(x)(Ω); that is, satisfies the (PS) condition. The proof of Lemma 17 is now completed.

Proof of Theorem 3. Firstly, note that for any solution u of (50). Hence, as in Section 3 we can conclude that uλ is a local minimum for in W1,p(x)(Ω). By the strong comparison principle and Hopf lemma, we can conclude that any critical point of is also a critical point of Eλ and hence u also solves (Pλ). It is easy to see that and are a subsolution and a supersolution to the problem associated with the functional energy Therefore, using the approach as in Theorem 2, we prove that this problem has a solution such that vλ is a local minimizer of in the C1 topology. Now, by the comparison principle we can see that vλuλ and also vλ solves (Pλ). If vλuλ the conclusion of Theorem 3 holds. That is, we can assume vλuλ and uλ is a strict local minimum of in the W1,p(x)(Ω) topology. Then, from Lemma A.4, the functional and note that as t. Thus, we can apply Lemma 17 combined with the Mountain Pass Theorem to conclude that problem (Pλ) has a solution vλ such that vλuλ. Therefore the proof of Theorem 3 is now completed.

Competing Interests

The authors declare that there is no conflict of interests regarding the publication of this article.

Acknowledgments

This work is supported by the Research Center, Scientific Research Deanship, University of Dammam, KSA, under Award no. 2015078.

    Appendix

    We start with an important technical tool which enables us to estimate the singularity in the Gâteaux derivative of the energy functional defined in (2).

    Lemma A.1. Let 0 < δ < 1. Then there exists a constant Cδ > 0 such that the inequality

    (A.1)
    holds true for all with |a| + |b| > 0.

    An elementary proof of this lemma can be found in Takáč [25, Lemma  A.1, p. 233]. We continue by showing the Gâteaux differentiability of the energy functional Eλ at a point uW1,p(x)(Ω) satisfying in Ω with θ1 = maxdist⁡(x)≤σ⁡(p(x)/(p(x) − 1 + δ(x))) (for details see Theorem 4.2 in [16]).

    Lemma A.2. Let assumptions (H0)–(H5) be satisfied. Assume that u, vW1,p(x)(Ω) and u satisfies in Ω. Then we have

    (A.2)

    Proof. We show the result only for the singular term ; the other two terms are treated in a standard way. So let

    (A.3)
    For we define
    (A.4)
    Consequently,
    (A.5)
    Notice that for almost every xΩ we have u(x) > 0 and
    (A.6)
    Moreover, the integral on the left-hand side (with nonnegative integrand) is dominated by
    (A.7)
    with constants independent of xΩ. Here, we have used the estimate (A.1) from Lemma A.1 above. Finally, we have , by vW1,p(x)(Ω) and Hardy’s inequality. Hence, we are allowed to invoke the Lebesgue dominated convergence theorem in (A.5) from which the lemma follows by letting t → 0.

    Corollary A.3. Let assumptions (H0)–(H5) be satisfied. Then the energy functional is Gâteaux differentiable at every point uW1,p(x)(Ω) that satisfies in Ω. Its Gâteaux derivative at u is given by

    (A.8)
    for vW1,p(x)(Ω).

    We continue by proving the C1-differentiability of the cut-off energy functional defined below.

    Lemma A.4. Let assumptions (H0)–(H5) be satisfied, and wW1,p(x)(Ω) such that in Ω. Setting for xΩ

    (A.9)
    and for uW1,p(x)(Ω)
    (A.10)
    we have that belongs to .

    Proof. As in Lemma A.2, we concentrate on the singular term, the others being standard. Let

    (A.11)
    , and . Proceeding as in Lemma A.2, we obtain that, for all , S(u) has a Gâteaux derivative S(u) given by
    (A.12)
    Let , uku0. Then
    (A.13)
    for all vW1,p(x)(Ω). Again, as in Lemma A.2, we use Hardy’s inequality to deduce that , so that by Lebesgue’s dominated convergence theorem we conclude that the Gâteaux derivative of S is continuous which implies that .

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