A Multiplicity Result for Quasilinear Problems with Nonlinear Boundary Conditions in Bounded Domains
Abstract
We study the following quasilinear problem with nonlinear boundary condition −Δpu − λa(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−2∇u), the functions a and b are sign changing continuous functions in Ω, 1 < p < γ < p*, where p* = Np/(N − p) 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
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 [1–3] 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).
If α ∈ (0,1], then μ(α, λ) > 0, and so λ → μ(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 α → μ(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 .
-
(𝒜1) α ∈ (0,1) or that∫Ωa(x)dx ≠ 0 and α ∈ (α0, 1],
-
𝒜2 a(x) ∈ L∞(Ω),
-
(ℬ1) b(x) ∈ L∞(Ω),
-
(ℬ2) b+≢0,
-
(ℬ3) ,
where is the positive principal eigenfunction corresponding to .
With these constructions we have the following.
Proposition 1.1. Assume (𝒜1), then for every ,
Proof. See [2].
Now we can state our main results.
Theorem 1.2. Assume (𝒜1), (𝒜2), (ℬ1), and (ℬ2). Then, for every , problem (1.2) admits at least one positive solution u ∈ W1,p(Ω)∩L∞(Ω).
Theorem 1.3. Assume (𝒜1), (𝒜2), (ℬ1), (ℬ2), and (ℬ3). Then, problem (1.2) has at least one positive solution u ∈ W1,p(Ω)∩L∞(Ω) for .
Theorem 1.4. Assume (𝒜1), (𝒜2), (ℬ1), (ℬ2), and (ℬ3). 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
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).
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 : X → R.
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 u ∈ X − {0} and t > 0. Then, if and only if .
Proof. The result is an immediate consequence of the fact that
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 u0 ∈ X, B(u0) ≠ 0, then
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
Proof. If u0 is a local minimizer of Jλ on S, then u0 is a solution of the optimization problem:
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), (ℬ1), (ℬ2) satisfy. It follows from variational characterization of μ(α, λ) that Aλ(u) ≥ 0 for all u ∈ X and . Moreover, we have
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:
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 un⇀u0 in X. Since X may be compactly embedded in Lp(Ω), Lγ(Ω), and Lp(∂Ω), we have un → u0 in Lp(Ω), Lγ(Ω) and Lp(∂Ω). Hence,
Assume that Aλ(u0) < 1. By using the map:
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)u0 ∈ X. 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 u1 ∈ L∞(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 {u ∈ X; Aλ(u) = 1} is unbounded and we are forced to require an additional assumption (ℬ3). In this case, again we are looking for a maximizing of the problem:
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 (ℬ3).
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:
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:
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
It follows from (4.10) that
Hence, for some δ > 0, problem (4.5) has at least one nonnegative solution u1 for any .
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 (ℬ3), it is easy to see that for some t1 < 1. Thus, the set {u ∈ X; B(u) = −1} is nonempty. Also, for this t1, we have
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
Letting n → ∞, we arrive at . It follows easily that , and so . As might be expected, we arrive at a contradiction with assumption (ℬ3), 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 w1≢w2. 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.