Volume 2011, Issue 1 419341
Research Article
Open Access

A Multiplicity Result for Quasilinear Problems with Nonlinear Boundary Conditions in Bounded Domains

S. Khademloo

Corresponding Author

S. Khademloo

Department of Mathematics, Faculty of Basic Sciences, Babol Noshirvani University of Technology, 47148-71167 Babol, Iran nit.ac.ir

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First published: 15 December 2011
Citations: 1
Academic Editor: Enrico Obrecht

Abstract

We study the following quasilinear problem with nonlinear boundary condition −Δpuλa(x)u | u|p−2 = b(x)u | u|γ−2, in Ω and (1 − α)|∇u|p−2(∂u/n) + αu | u|p−2 = 0, on Ω, where Ω⊆RN is a connected bounded domain with smooth boundary Ω, the outward unit normal to which is denoted by n. Δp is the p-Laplcian operator defined by Δpu = div (|∇u|p−2u), the functions a and b are sign changing continuous functions in Ω, 1 < p < γ < p*, where p* = Np/(Np) if N > p and otherwise. The properties of the first eigenvalue and the associated eigenvector of the related eigenvalue problem have been studied in (Khademloo, In press). In this paper, it is shown that if , the original problem admits at least one positive solution, while if , for a positive constant λ*, it admits at least two distinct positive solutions. Our approach is variational in character and our results extend those of Afrouzi and Khademloo (2007) in two aspects: the main part of our differential equation is the p-Laplacian, and the boundary condition in this paper also is nonlinear.

1. Introduction and Results

In this paper, we consider the problem
(1.1)
where Ω⊆RN is a connected bounded domain with a smooth boundary Ω, the outward unit normal to which is denoted by n. Δp is the p-Laplcianian operator defined by Δpu = div (|∇u|p−2u). The functions a and b are assumed to be sign changing in Ω. Here, we say a function a(x) changes sign if the measure of the sets {x ∈ Ω; a(x) > 0} and {x ∈ Ω; a(x) < 0} are both positive. λ ≥ 0 is a real parameter and exponent γ is assumed to satisfy the condition 1 < p < γ < p*, where p* = Np/(Np) if N > p and otherwise.

A host of literature exists for this type of problem when p = 2. For the works concerning with problems similar to (1.1) in the case p = 2, we refer to [13] and references therein.

The growing attention in the study of the p-Laplace operator is motivated by the fact that it arises in various applications, for example, non-Newtonian fluids, reaction diffusion problems, flow through porus media, glacial sliding, theory of superconductors, biology, and so forth (see [4, 5] and the references therein).

In this paper, we obtain new existence results by using a variational method based on the properties of eigencurves, that is, properties of the map λμ(α, λ), where μ(α, λ) denotes the principal eigenvalue of the problem
(1.2)
Similar to [6] our method works provided that the eigenvalue problem
(1.3)
has principal eigenvalues and it can be shown that this occurs on an interval [α0, 1] where α0 ≤ 0. Thus, we are able to obtain existence results for problem (1.2) even in the case of nonlinear Neumann boundary conditions where α is small and negative. Our method depends on using eigencurves to produce an equivalent norm on W1,p(Ω); such an equivalent norm is also introduced in [2]. The results that we obtain in this paper are generalization of the previous results obtained by Pohozaev and Veron [7].
It can be shown that μ(α, λ) has the variational characterization:
(1.4)
from whence it follows that
  • (i)

    λ is a principal eigenvalue of (1.2) if and only if μ(α, λ) = 0,

  • (ii)

    αμ(α, λ) is an increasing function,

  • (iii)

    λμ(α, λ) is a concave function with a unique maximum such that μ(α, λ) → − as λ → ± [6].

If α ∈ (0,1], then μ(α, λ) > 0, and so λμ(α, λ) has exactly one negative zero and one positive zero . Thus, and are principal eigenvalues for (1.2).

If α = 0, then μ(0,0) = 0. If a(x) > 0, then μ(0, λ) is decreasing, and if a(x) < 0, then μ(0, λ) is increasing. Assume now that a(x) changes sign in Ω: if ∫Ωa(x)dx < 0, there exists a unique such that μ(0, λ+(0)) = 0 and μ(0, λ) > 0 for . If ∫Ωa(x)dx = 0, then μ(0,0) = 0 and μ(0, λ) < 0 for λ ≠ 0. If ∫Ωa(x)dx > 0, then there exists a unique such that and μ(0, λ) > 0 for .

Suppose now that ∫Ωa(x)dx < 0 and that α is small and negative. Then, since αμ(α, λ) is increasing, it follows that there still exist principal eigenvalues of (2.5), but now both of them are positive.

It can be shown that there exists α0 < 0 such that the above is true for all α ∈ (α0, 0), but for α < α0, μ(α, λ) < 0 for all λ so that principal eigenvalues no longer exist.

Similar considerations show that when ∫Ωa(x)dx > 0, there exists α0 < 0 such that there are principal eigenvalues for α0 < α < 0 but when ∫Ωa(x)dx = 0, there are no principal eigenvalues for α < 0 (see [6]).

It is easy to see that if and exist, μ(α, λ) > 0 for all .

Thus, we assume that the following conditions hold:
  • (𝒜1) α ∈ (0,1)  or  that∫Ωa(x)dx ≠ 0  and  α ∈ (α0, 1],

  • 𝒜2 a(x) ∈ L(Ω),

  • (1) b(x) ∈ L(Ω),

  • (2) b+≢0,

  • (3) ,

where is the positive principal eigenfunction corresponding to .

With these constructions we have the following.

Proposition 1.1. Assume (𝒜1), then for every ,

(1.5)
defines a norm in W1,p(Ω) which is equivalent to the usual norm of W1,p(Ω), that is,
(1.6)

Proof. See [2].

Now we can state our main results.

Theorem 1.2. Assume (𝒜1), (𝒜2), (1), and (2). Then, for every , problem (1.2) admits at least one positive solution uW1,p(Ω)∩L(Ω).

Theorem 1.3. Assume (𝒜1), (𝒜2), (1), (2), and (3). Then, problem (1.2) has at least one positive solution uW1,p(Ω)∩L(Ω) for .

Theorem 1.4. Assume (𝒜1), (𝒜2), (1), (2), and (3). Then, there exists such that problem (1.2) admits at least two distinct positive weak solutions in W1,p(Ω)∩L(Ω), whenever .

When λ = 0 and α = 0, we have the following.

Corollary 1.5. Assume ∫Ωb(x)dx < 0. Then, the problem

(1.7)
has a positive solution.

Throughout this paper, c denotes a positive constant. We will use fibrering method in a similar way to those in [8]. A brief description of the method and the proof of Theorem 1.2 are presented in Section 2. We then study the cases and in Sections 3 and 4.

2. The Case When

In this section, motivated by Pohozaev [8], we will introduce the fibrering map as our framework for the study of problem (1.2).

For a (weak) solution of problem (1.2), we mean a function uX = W1,p(Ω) such that for every vW1,p(Ω), there holds
(2.1)
Now let us define the variational functional corresponding to problem (1.2). We set Iλ : XR as
(2.2)
It is easy to see that IλC1(X, R), and for vX, there holds
(2.3)

Since , we know that critical points of Iλ are weak solutions of the problem (1.2). Thus, to prove our main theorems, it suffices to show that Iλ admits critical point. We will do this in this paper. Our main tool is the theory of the fibrering maps. First, we will introduce this map for Iλ : XR.

Let ϕu(t) = Iλ(tu)  (t > 0). We refer to such maps as fibrering maps. It is clear that if u is a local minimizer of Iλ, then ϕu has a local minimum at t = 1.

Lemma 2.1. Let uX − {0} and t > 0. Then, if and only if .

Proof. The result is an immediate consequence of the fact that

(2.4)

Thus critical points of Iλ correspond to stationary points of the maps ϕu that can be given by
(2.5)
where
(2.6)
Hence,
(2.7)
Thus, if Aλ(u) and B(u) have the same sign, ϕu has exactly one turning point at
(2.8)
provided that B(u) ≠ 0, and if Aλ(u) and B(u) have opposite signs, ϕu has no turning points. Now substituting (2.8) into (2.5), we get
(2.9)

Lemma 2.2. Suppose that u0 is a critical point of Jλ, where Aλ(u0) and B(u0) have the same sign. Then, .

Proof. Let u0X, B(u0) ≠ 0, then

(2.10)
for all vX. This completes the proof.

The following lemma shows that the critical points of the functional Iλ can be found by using the conditional variational problem associated with Iλ.

Lemma 2.3. Suppose that H is a well-defined functional on X and u0 is a minimizer of Jλ on

(2.11)
for some c ≠ 0. Then,.

Proof. If u0 is a local minimizer of Jλ on S, then u0 is a solution of the optimization problem:

(2.12)
where γ(u) = H(u) − c. Hence, by the theory of the Lagrange multipliers, there exists μR such that . Thus,
(2.13)
Note that the functional Jλ is 0-homogeneous and the Gateaux derivative of Jλ at the point vX, B(v) ≠ 0, in direction v, is zero, that is, . It then follows that μ = 0 due to u0S. Hence, the proof is complete.

The following scheme for the investigation of the solvability of (1.2) is based on previous lemmas. First, we will prove the existence of nonzero critical points of Jλ under the constraint given by suitable functional H. This will be an actual critical point of Jλ and it will generate critical point of the Euler functional Iλ which will coincide with the weak solution of problem (1.2).

Proof of Theorem 1.2. Suppose that (𝒜1), (𝒜2), (1), (2) satisfy. It follows from variational characterization of μ(α, λ) that Aλ(u) ≥ 0 for all uX and . Moreover, we have

(2.14)
Hence, for using Lemma 2.3, it is sufficient to consider the case Aλ(u) = c ≠ 0, for example c = 1. In this case, we have
(2.15)
From the necessary condition for the existence of t(u), we have B(u) > 0. It follows that we must consider a critical point with B(u) > 0.

The functional Jλ(u) is nonnegative and so bounded below, hence we can look for positive local minimizer for Jλ(u) on X.

Let us consider variational problem:

(2.16)
Note that for , this set is not empty, and from Lemma 2.3, the solution of this problem is a minimizer of Jλ(u) on X.

Suppose {un} is the maximizing sequence of this problem. It follows from the equivalent property in Proposition 1.1, {un} is bounded and so we may assume that unu0 in X. Since X may be compactly embedded in Lp(Ω), Lγ(Ω), and Lp(Ω), we have unu0 in Lp(Ω), Lγ(Ω) and Lp(Ω). Hence,

(2.17)
Moreover, we have
(2.18)
Here, the weak lower semicontinuity of the equivalent norm was used.

Assume that Aλ(u0) < 1. By using the map:

(2.19)
we have L(1) < 1 and lim tL(t) = and so L(t0) = 1 for some t0 > 1, that is, Aλ(t0u0) = 1. So we derive
(2.20)

which is a contradiction. Hence, Aλ(u0) = 1 and so u0 is a maximizer. As Lemma 2.2, the result would follow by considering u1 = t(u0)u0X. Then, u1 is a weak solution of (1.2) and u1 ≥ 0 in Ω. Now, following the bootstrap argument (used, e.g., in [9]), we prove u1L(Ω). Then, we can apply the Harnack inequality due to Trudinger [5] in order to get u1 > 0 in Ω (cf. [9]).

3. The Case When

Proof of Theorem 1.3. If , It is easy to see that the set {uX; Aλ(u) = 1} is unbounded and we are forced to require an additional assumption (3). In this case, again we are looking for a maximizing of the problem:

(3.1)
Suppose {un} is a maximizing sequence of this problem. First, we investigate the case when {un} is unbounded. Then, we may assume without loss of generality that ∥un∥→. So, we obtain
(3.2)
where vn = un/∥un∥. Thus, we have
(3.3)
Since ∥vn∥ = 1, we may assume that vnv0 in X. Again, since X may be compactly embedded in Lp(Ω), Lγ(Ω) and Lp(Ω), we have
(3.4)
So,
(3.5)
And, therefore, v0≢0. Returning to , we have also
(3.6)
Due to simplicity of , there exists c ≠ 0 such that . Therefore, we have
(3.7)
that implies , which contradicts (3). Therefore, {un} is bounded and so unu0 in X and unu0 in Lp(Ω), Lγ(Ω) and Lp(Ω). Hence, , and so u0 ≠ 0.

Moreover, we obtain . Here, the variational characteristic of and the weak lower semicontinuity of the norm were used. Let us now consider the case . Again, we obtain for some c ≠ 0, and so which contradicts (3).

Now we prove that . Suppose otherwise, then by using L(t) in (2.20), we obtain some t0 > 1 such that . By direct calculation, we get a contradiction like (4.1). This yields that u0 is a nonnegative solution of problem (1.2). Using the same ideas as the proof of Theorem 1.2, we have proved Theorem 1.3.

4. The Case When

As it is proved in [10], we will show that for but close enough to , we have two distinct positive solutions for problem (1.2). The existence of one of them is obtained by using the following lemma.

Lemma 4.1. Under the assumption of Theorem 1.4, there exists a maximizer u1 of the problem:

(4.1)
whenever , for some δ > 0. Moreover, u1XL(Ω) is a positive weak solution of problem (1.2).

Proof. First note that using L(t) in (2.20), it is easy to see that u1 is a maximizer of problem (4.2) if and only if u1 is a maximizer of the problem:

(4.2)
Now suppose that the result is false. Then, there exists a sequence {δk} such that δk → 0 and problem (4.1) has no solution for . For simplicity, we use . Let be a maximizing sequence of this problem, that is,
(4.3)
We prove that if be bounded or unbounded, we arrive at a contradiction and so the lemma is proved.

The first case: is bounded. Thus, in X for some and in Lp(Ω), Lγ(Ω), and Lp(Ω). Hence, and the weak lower semicontinuity of the norm gives . Therefore, is a solution of problem (4.5), which is a contradiction.

The case is unbounded. Then we may assume that . Let . Then, in X for some and in Lp(Ω), Lγ(Ω) and Lp(Ω). This implies that

(4.4)
Therefore, . Furthermore, and so . Thus, we arrive at
(4.5)
which implies
(4.6)
(4.7)
It is a direct consequent of the comactly embedding of X in Lp(Ω), Lγ(Ω) and Lp(Ω). Now, we pass to the limit for k. Then, and since is a bounded sequence, we may assume that in X for some v0X and in Lp(Ω), Lγ(Ω), and Lp(Ω).

It follows from (4.10) that

(4.8)
and from the variational characteristic of and (4.6) that
(4.9)
which contradicts (3).

Hence, for some δ > 0, problem (4.5) has at least one nonnegative solution u1 for any .

In order to find the second positive solution, we consider the minimizing problem:
(4.10)

Note that this set is empty for (because of the variational characterization of ). Hence, this second problem does not have a solution for .

Lemma 4.2. Under the assumption of Theorem 1.4, there exists ɛ > 0 such that for , problem (1.1) has a nonnegative solution u2 satisfying Aλ(u2) < 0.

Proof. First note that using the auxiliary function L(t) = |t|γB(u) and the assumption (3), it is easy to see that for some t1 < 1. Thus, the set {uX; B(u) = −1} is nonempty. Also, for this t1, we have

(4.11)
for .

Again, we assume that the result is not true. Then, there exists ɛk → 0 such that for , problem (1.1) has no solution.

Let be a minimizing sequence of this problem, that is,

Assume that is bounded. Using similar argument as in the proof of Lemma 4.1, we find a solution of problem (1.1) which is a contradiction. Let us assume is bounded. Again, we consider

(4.12)
is bounded, and so in X for some . Thus,.

Letting n, we arrive at . It follows easily that , and so . As might be expected, we arrive at a contradiction with assumption (3), by using similar steps as in the proof of Theorem 1.3. This completes the proof.

Proof of Theorem 1.4. Let η = min {ɛ, δ}, and w1 = t(u1)u1 and w2 = t(u2)u2, where t(ui) is defined by (2.16).

It easy to see that Aλ(w1) > 0 and Aλ(w2) ≤ 0, and so w1w2. Thus, w1 and w2 are two distinct non negative weak solutions to (1.2). Other properties of w1 and w2 follow in the same way as in Section 2.

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