Volume 2011, Issue 1 378389
Research Article
Open Access

Periodic Solutions for Autonomous (q, p)-Laplacian System with Impulsive Effects

Xiaoxia Yang

Xiaoxia Yang

School of Mathematical Sciences and Computing Technology, Central South University, Changsha, Hunan 410083, China csu.edu.cn

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Haibo Chen

Corresponding Author

Haibo Chen

School of Mathematical Sciences and Computing Technology, Central South University, Changsha, Hunan 410083, China csu.edu.cn

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First published: 07 December 2011
Citations: 2
Academic Editor: Yongkun Li

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.

In this paper, we consider the following system:
()
where p > 1,     q > 1, T > 0, ,  tj(j = 1,2, …, l), and sm(m = 1,2, …, k) are the instants where the impulses occur and 0 = t0 < t1 < t2 < ⋯<tl < tl+1 = T,   0 = s0 < s1 < s2 < ⋯<sk < sk+1 = T, Ij : N  (jB), and Km : N  (mC) are continuously differentiable
()
and F : N × N satisfies the following assumption.
  •   (A) F(x) is continuously differentiable in (x1, x2), and there exist a1, a2C(+, +) such that

    ()

for all x = (x1, x2) ∈ N × N.

When p = q = 2, Ij ≡ 0  (jB), Km ≡ 0  (mC), and F(u1, u2) = F1(u1), system (1.1) reduces to the following autonomous second-order Hamiltonian system:
()
There have been lots of results about the existence of periodic solutions for system (1.4) and nonautonomous second order Hamiltonian system
()
(e.g., see [121]). Many solvability conditions have been given, for instance, coercive condition, subquadratic condition, superquadratic condition, convex condition, and so on.
When p = q = 2, ∇Ij≢0  (jB), Km ≡ 0  (mC), and F(u1, u2) = F1(u1), system (1.1) reduces to the following autonomous second-order Hamiltonian system with impulsive effects:
()
Recently, many authors studied the existence of periodic solutions for impulsive differential equations by using variational methods, and lots of interesting results have been obtained. For example, see [2228]. Especially, nonautonomous second-order Hamiltonian system with impulsive effects is considered in [25, 26] by using the least action principle and the saddle point theorem.
When Ij ≡ 0  (jB) and Km ≡ 0  (mC), system (1.1) reduces to the following system:
()
In [29, 30], Paşca and Tang obtained some existence results for system (1.7) by using the least action principle and saddle point theorem. Motivated by [17, 2230], in this paper, we are concerned with system (1.1) and also use the least action principle and saddle point theorem to study the existence of periodic solution. Our results still improve those in [17] even if system (1.1) reduces to system (1.4).
A function G : N is called to be (λ, μ)-quasiconcave if
()
for some λ, μ > 0 and x, yN.

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:

  • (F1) there exist

    ()
    such that
    ()
    where
    ()

  • (F2) F(x) → +,     as    |x| → ,   where    x = (x1, x2),

  • (I1) there exists β such that

    ()

Then, system (1.1) has at least one solution in , where is absolutely continuous,  u(0) = u(T) and.

Furthermore, if Ij ≡ 0  (jB), Km ≡ 0  (mC) and the following condition holds:

  • (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:

  • (A) F1(z) is continuously differentiable in z and there exists a1C(+, +) such that

    ()
    for all zN.

  • (F1) there exists 0 < r < 6/T2 such that

    ()

  • (F2) F1(z) → +,     as    |z| → ,     zN;

  • (I1)   there exists β such that

    ()

Then, system (1.6) has at least one solution in . Furthermore, if Ij ≡ 0  (jB) and the following condition holds:
  • (F3) there exist δ > 0 and a ∈ [0, (3/T2)) such that

    ()
    then system (1.4) has at least two nonzero solutions in .

For the Sobolev space , one has the following sharp estimates (see in [3, Proposition  1.2]):
()
()
By the above two inequalities, we can obtain the following better results than by Corollary 1.2.

Theorem 1.3. Suppose F1 satisfies assumption (A)′, (F2)′, (I1)′ and

  • (F1) there exists 0 < r < 4π2/T2 such that (1.15) holds.

Then, system (1.6) has at least one solution in . Furthermore, if Ij ≡ 0  (jB) and the following condition holds:
  • (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:

  • (F4) F1(z) is (λ, μ)-quasiconcave on N,

  • (F5) F1(z) → − as |z| → +, zN,

  • (I2) there exist dj > 0  (jB) such that

    ()

  • (I3) there exist bj > 0,   cj > 0, γj, αj ∈ [0,   2)(jB) such that

    ()

Then, system (1.6) has at least one solution in .

Remark 1.5. In [17], Yang considered the second-order Hamiltonian system with no impulsive effects, that is, system (1.4). When Ij ≡ 0  (jB), 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

()
Finally, it is remarkable that Theorems 1.3 and 1.4 are also different from those results in [116]. We can find an example satisfying our Theorem 1.3 but not satisfying the results in [121]. For example, let
()
where . We can also find an example satisfying our Theorem 1.4 but not satisfying the results in [121]. For example, let
()
where 12/T2 < r < 4π2/T2.

2. Variational Structure and Some Preliminaries

The norm in is defined by
()
Set
()
Let
()
Obviously, is a reflexive Banach space. It is easy to know that is a subset of and . In this paper, we will use the space W defined by
()
with the norm . It is clear that W is a reflexive Banach space. Let . Then, .

Lemma 2.1 (see [31] or [32].)Each and each can be written as and with

()
Then,
()
()
where
()

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.

Following the idea in [22], one takes and multiplies the two sides of
()
by v1 and integrate from 0 to T, one obtains
()
Note that v1(t) is continuous. So, . Combining , one has
()
Combining with (2.10), one has
()
Similarly, one can get
()
for all . Considering the above equalities, one introduces the following concept of the weak solution for system (1.1).

Definition 2.2. We say that a function is a weak solution of system (1.1) if

()
holds for any .

Define the functional by

()
where ,
()
By assumption (A) and [33], we know that . The continuity of Ij(jB) and Km(mC) implies that . So, , and for all , we have
()
Definition 2.2 shows that the critical points of φ correspond to the weak solutions of system (1.1).

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 = X1X2 with φ(0) = 0, satisfying (PS) condition, and assume that for some ρ > 0,

()
Assume also that φ is bounded below and inf Xφ < 0, then φ has at least two nonzero critical points.

Lemma 2.5 (see [35], Theorem  4.6.)Let X = X1X2, where X is a real Banach space and X1 ≠ {0} and is finite dimensional. Suppose that φC1(X, ) satisfies (PS)-condition and

  • (φ1) there is a constant α and a bounded neighborhood D of 0 in X1 such that φDα,

  • (φ2) there is a constant β > α such that .

Then, φ possesses a critical value cβ. Moreover, c can be characterized as

()
where,
()

3. Proof of Theorems

Lemma 3.1. Under assumption (A), φ is weakly lower semicontinuous on .

Proof. Let

()
Since
()
then ϕ1 is convex. Moreover, by [33], we know that ϕ1 is continuous, and so, it is lower semicontinuous. Thus, it follows from [3, Theorem  1.2] that ϕ1 is weakly lower continuous. By assumption (A), it is easy to verify that ϕ2(u1, u2) is weakly continuous. We omit the details. Let
()
Next, we show that ψ1 and ψ2 are weakly continuous on and , respectively. In fact, if
()
then by in [3, Proposition  1.2], we know that
()
So, there exists M1 > 0 such that ∥u1M1 and ∥u1nM1, for all n. Thus, we have
()
Hence, ψ1 is weakly continuous on . Similarly, we can prove that ψ2 is also weakly continuous on . Thus, we complete the proof.

Proof of Theorem 1.1. It follows from (F1) and (2.7) that

()
()
Hence, by (I1), (3.7), and (3.8), we have
()
Note that for ,
()
and for ,
()
So, (F2) and (3.9) imply that
()
Thus, by Lemma 2.3, we know that φ has at least one critical point which minimizes φ on W.

Furthermore, if Ij(u1(tj)) ≡ 0  (jB) and Km(u2(sm)) ≡ 0  (mC), 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 = N × N 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

()
Since and , (3.13) implies that φ(u1, u2) ≥ 0 for all (u1, u2) ∈ X1 with ∥uWρ. By (F3), it is easy to obtain that φ(u1, u2) ≤ 0, for all (u1, u2) ∈ X2 with ∥uWρ.

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)∥Wρ. Hence, all (u1, u2) ∈ X2 with ∥(u1, u2)  Wρ 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  (mC). It is easy. So, we omit it.

Lemma 3.2. Under the assumptions of Theorem 1.4, the functional φ1 defined by

()
satisfies (PS) condition.

Proof. Suppose that {u1n} is a (PS) sequence for φ1; that is, there exists D1 > 0 such that

()
Hence, for n large enough, we have ∥φ(u1n)∥   ≤ 1. It follows from (F1) , (I2), and (1.18) that
()
for n large enough. By (1.18), we have
()
and (3.16), (3.17), and r < 4π2/T2 imply that there exists D2, D3 > 0 such that
()
It follows from (F4), (3.15), (I3), (1.18), and (3.18) that
()
for all n and (3.19) and (F5) imply that is bounded. Combining (3.18), we know that {u1n} is a bounded sequence. Similar to the argument in [25], it is easy to obtain that φ satisfies (PS) condition.

Proof of Theorem 1.4. From (I3) and (F5), it is easy to see that for x1N,

()
For all , by (1.18), (F1)  and (I3), we have
()
Note that for all , is equivalent to . Then, r1 < 4π2/T2, αj < 2(jB) and (3.21) imply that
()
It follows from (3.20) and (3.22) that φ1 satisfies (φ1) and (φ2) in Lemma 2.5. Combining with Lemma 3.2, Lemma 2.5 shows that φ1 has at least one critical point. Thus, we complete the proof.

4. Examples

Example 4.1. Let q = 4, p = 2, T = π, t1 = 1, and s1 = 2. Consider the following system:

()
where , x1 = (x11, x12, …, x1N), x2 = (x21, x22, …, x2N), , , xN. It is easy to verify that all conditions of Theorem 1.1 hold so that system (4.1) has at least one weak solution. Moreover, if , x2 = (x21, x22, …, x2N), I1(x) = 0 and K1(x) = 0, xN, then system (4.1) has at least two nonzero solutions.

Example 4.2. Let T = 2, t1 = 1. Consider the following autonomous second-order Hamiltonian system with impulsive effects:

()
where ,, . It is easy to verify that all conditions of Theorem 1.3 hold so that system (4.2) has at least one weak solution. Moreover, if and I1(z) = 0, zN, then system (4.2) has at least two nonzero solutions.

Example 4.3. Let T = π, t1 = 2. Consider the following autonomous second-order Hamiltonian system with impulsive effects:

()
where F(z)   = −|z|2,   I1(z)   = 2sin z1, . It is easy to verify that all conditions of Theorem 1.4 hold so that system (4.3) has at least one weak solution.

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