Periodic Solutions for Autonomous (q, p)-Laplacian System with Impulsive Effects
Abstract
By using the variational method, some existence theorems are obtained for periodic solutions of autonomous (q, p)-Laplacian system with impulsive effects.
1. Introduction
Let B = {1,2, …, l}, C = {1,2, …, k}, l, k ∈ ℕ.
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(A) F(x) is continuously differentiable in (x1, x2), and there exist a1, a2 ∈ C(ℝ+, ℝ+) such that
()
for all x = (x1, x2) ∈ ℝN × ℝN.
Next, we state our main results.
Theorem 1.1. Let q′ and p′ be such that 1/q + 1/q′ = 1 and 1/p + 1/p′ = 1. Suppose F satisfies assumption (A) and the following conditions:
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(F1) there exist
()such that()where()
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(F2) F(x) → +∞, as |x| → ∞, where x = (x1, x2),
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(I1) there exists β ∈ ℝ such that
()
Furthermore, if Ij ≡ 0 (j ∈ B), Km ≡ 0 (m ∈ C) and the following condition holds:
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(F3) there exist δ > 0, and such that
()then system (1.7) has at least two nonzero solutions in .
When p = q = 2, F(x1, x2) = F1(x1), by Theorem 1.1, it is easy to get the following corollary.
Corollary 1.2. Suppose F1 satisfies the following conditions:
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(A)′ F1(z) is continuously differentiable in z and there exists a1 ∈ C(ℝ+, ℝ+) such that
()for all z ∈ ℝN. -
(F1)′ there exists 0 < r < 6/T2 such that
() -
(F2)′ F1(z) → +∞, as |z| → ∞, z ∈ ℝN;
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(I1)′ there exists β ∈ ℝ such that
()
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(F3)′ there exist δ > 0 and a ∈ [0, (3/T2)) such that
()then system (1.4) has at least two nonzero solutions in .
Theorem 1.3. Suppose F1 satisfies assumption (A)′, (F2)′, (I1)′ and
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(F1)′′ there exists 0 < r < 4π2/T2 such that (1.15) holds.
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(F3)′′ there exist δ > 0 and a ∈ [0, (2π2)/T2) such that
()then system (1.4) has at least two nonzero solutions in .
Moreover, for system (1.6), we have the following additional result.
Theorem 1.4. Suppose F1 satisfies assumption (A)′, (F1)′ ′ and the following conditions:
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(F4) F1(z) is (λ, μ)-quasiconcave on ℝN,
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(F5) F1(z) → −∞ as |z| → +∞, z ∈ ℝN,
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(I2) there exist dj > 0 (j ∈ B) such that
() -
(I3) there exist bj > 0, cj > 0, γj ∈ ℝ, αj ∈ [0, 2)(j ∈ B) such that
()
Remark 1.5. In [17], Yang considered the second-order Hamiltonian system with no impulsive effects, that is, system (1.4). When Ij ≡ 0 (j ∈ B), our Theorems 1.3 and 1.4 still improve those results in [17]. To be precise, the restriction of r is relaxed, and some unnecessary conditions in [17] are deleted. In [17], the restriction of r is 0 < r < T/12, which is not right. In fact, from his proof, it is easy to see that it should be 0 < r < 12/T2. Obviously, our restriction 0 < r < 4π2/T2 is better. Moreover, in our Theorem 1.4, we delete such conditions (of in [17, Theorem 1]): ∇F1(0) = 0, and there exist positive constants M, N such that
2. Variational Structure and Some Preliminaries
Note that if , then u is absolutely continuous. However, we cannot guarantee that is also continuous. Hence, it is possible that , which results in impulsive effects.
Definition 2.2. We say that a function is a weak solution of system (1.1) if
Define the functional by
We will use the following lemma to seek the critical point of φ.
Lemma 2.3 (see [3], Theorem 1.1.)If φ is weakly lower semicontinuous on a reflexive Banach space X and has a bounded minimizing sequence, then φ has a minimum on X.
Lemma 2.4 (see [34].)Let φ be a C1 function on X = X1 ⊕ X2 with φ(0) = 0, satisfying (PS) condition, and assume that for some ρ > 0,
Lemma 2.5 (see [35], Theorem 4.6.)Let X = X1 ⊕ X2, where X is a real Banach space and X1 ≠ {0} and is finite dimensional. Suppose that φ ∈ C1(X, ℝ) satisfies (PS)-condition and
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(φ1) there is a constant α and a bounded neighborhood D of 0 in X1 such that φ∣∂D ≤ α,
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(φ2) there is a constant β > α such that .
Then, φ possesses a critical value c ≥ β. Moreover, c can be characterized as
3. Proof of Theorems
Lemma 3.1. Under assumption (A), φ is weakly lower semicontinuous on .
Proof. Let
Proof of Theorem 1.1. It follows from (F1) and (2.7) that
Furthermore, if Ij(u1(tj)) ≡ 0 (j ∈ B) and Km(u2(sm)) ≡ 0 (m ∈ C), then system (1.1) reduces to (1.7). When (F3) also holds, we will use Lemma 2.4 to obtain more critical points of φ. Let X = W, X2 = ℝN × ℝN and .
By (3.9), we know that φ(u1, u2) → +∞ as ∥(u1, u2)∥W → ∞. So, φ satisfies (PS) condition and is bounded below. Take ρ = δ/c1, where c1 is a positive constant such that and for all (u1, u2) ∈ W. It follows from (F3) and Lemma 2.1 that
If inf {φ(u1, u2) : (u1, u2) ∈ W} = 0, then from above, we have φ(u1, u2) = 0 for all (u1, u2) ∈ X2 with ∥(u1, u2)∥W ≤ ρ. Hence, all (u1, u2) ∈ X2 with ∥(u1, u2) ∥W ≤ ρ are minimal points of φ, which implies that φ has infinitely many critical points. If inf {φ(u1, u2) : (u1, u2) ∈ W} < 0, then by Lemma 2.4, φ has at least two nonzero critical points. Hence, system (1.7) has at least two nontrivial solutions in W. We complete our proof.
Proof of Theorem 1.3. We only need to use (1.18) and (1.19) to replace (2.6) and (2.7) in the proof Theorem 1.1 with p = q = 2, F(t, u1, u2) = F1(u1) and Km(u2) ≡ 0 (m ∈ C). It is easy. So, we omit it.
Lemma 3.2. Under the assumptions of Theorem 1.4, the functional φ1 defined by
Proof. Suppose that {u1n} is a (PS) sequence for φ1; that is, there exists D1 > 0 such that
Proof of Theorem 1.4. From (I3) and (F5), it is easy to see that for x1 ∈ ℝN,
4. Examples
Example 4.1. Let q = 4, p = 2, T = π, t1 = 1, and s1 = 2. Consider the following system:
Example 4.2. Let T = 2, t1 = 1. Consider the following autonomous second-order Hamiltonian system with impulsive effects: