Abstract
In this article, we investigate the existence of infinitely many periodic solutions for some nonautonomous second-order differential systems with p(t)-Laplacian. Some multiplicity results are obtained using critical point theory.
2000 Mathematics Subject Classification: 34C37; 58E05; 70H05.
Keywords:
p(t)-Laplacian; Periodic solutions; Critical point theory1. Introduction
Consider the second-order differential system with p(t)-Laplacian
where T > 0, F: [0, T] × ℝN → ℝ, and p(t) ∈ C([0, T], ℝ+) satisfies the following assumptions:
(A) p(0) = p(T) and
Moreover, we suppose that F: [0, T] × ℝN → ℝ satisfies the following assumptions:
(A') F(t, x) is measurable in t for every x ∈ ℝN and continuously differentiable in x for a.e. t ∈ [0, T], and there exist a ∈ C(ℝ+, ℝ+), b ∈ L1(0, T; ℝ+), such that
for all x ∈ ℝN and a.e. t ∈ [0, T].
The operator
In 2003, Fan and Fan [13] studied the ordinary p(t)-Laplacian system and introduced a generalized Orlicz-Sobolev space
The rest of the article is divided as follows: Basic definitions and preliminary results are collected in Second 2. The main results and proofs are given in Section 3. The three examples are presented in Section 4 for illustrating our results.
In this article, we denote by
2. Preliminaries
In this section, we recall some known results in nonsmooth critical point theory,
and the properties of space
Definition 2.1 [14]. Let p(t) satisfies the condition (A), define
with the norm
For
Define
with the norm
In this article, we will use the following equivalent norm on W1, p(t) ([0, T], ℝN), i.e.,
and some lemmas given in the following section have been proven under the norm of
Remark 2.1. If p(t) = p, where p ∈ (1, ∞) is a constant, by the definition of |u|p(t), it is easy to get
The space Lp(t) is a generalized Lebesgue space, and the space W1, p(t) is a generalized Sobolev space. Because most of the following lemmas have appeared in [13,14,17,18], we omit their proofs.
Lemma 2.1 [13]. Lp(t) and W1, p(t) are both Banach spaces with the norms defined above, when p- > 1, they are reflexive.
Lemma 2.2 [14]. (i) The space Lp(t) is a separable, uniform convex Banach space, its conjugate space is Lq(t), for any u ∈ Lp(t) and v ∈ Lq(t), we have
where
(ii) If p1(t) and p2(t) ∈ C([0, T], ℝ+) and p1(t) ≤ p2(t) for any t ∈ [0, T], then
Lemma 2.3 [14]. If we denote
(i) |u|p(t) < 1 (= 1; > 1) ⇔ ρ(u) < 1 (= 1; > 1);
(ii)
(iii) |u|p(t) → 0 ⇔ ρ(u) → 0; |u|p(t) → ∞ ⇔ ρ(u) → ∞.
(iv) For u ≠ 0,
Similar to Lemma 2.3, we have
Lemma 2.4. If we denote
(i) ||u|| < 1 (= 1; > 1) ⇔ I(u) < 1 (= 1; > 1);
(ii)
(iii) ||u|| → 0 ⇔ I(u) → 0; ||u|| → ∞ ⇔ I(u) → ∞.
(iv) For u ≠ 0,
Defnition 2.2 [17].
with the norm
For a constant p ∈ (1, ∞), using another conception of weak derivative which is called T-weak derivative, Mawhin and Willem gave the definition of the space
Definition 2.3 [17]. Let u ∈ L1([0, T], ℝN) and v ∈ L1([0, T], ℝN), if
then v is called a T-weak derivative of u and is denoted by
Definition 2.4 [17]. Define
with the norm
Definition 2.5 [13]. Define
and
Remark 2.2. From Definition 2.4, if
Lemma 2.5 [13].
(i)
(ii)
(iii) If
Lemma 2.6 [17]. Assume that
(i)
(ii) u has its continuous representation, which is still denoted by
(iii)
Since every closed linear subspace of a reflexive Banach space is also reflexive, we have
Lemma 2.7 [13].
Obviously, there are continuous embeddings
Lemma 2.8 [13]. There is a continuous embedding
when p- > 1, the embedding is compact.
Lemma 2.9 [13]. Each of the following two norms is equivalent to the norm in
(i)
(ii)
Lemma 2.10 [13]. If u, un ∈ Lp(t) (n = 1,2,...), then the following statements are equivalent to each other
(i)
(ii)
(iii) un → u in measure in [0, T] and
Lemma 2.11 [14]. The functional J defined by
is continuously differentiable on
and J' is a mapping of (S+), i.e., if un ⇀ u weakly in
then un has a convergent subsequence on
Lemma 2.12 [18]. Since
For k = 1, 2,..., denote
Lemma 2.13 [19]. Let X be a reflexive infinite Banach space, ϕ ∈ C1(X, ℝ) is an even functional with the (C) condition and ϕ(0) = 0. If X = Y ⊕ V with dimY < ∞, and ϕ satisfies
(i) there are constants σ, α > 0 such that
(ii) for any finite-dimensional subspace W of X, there exists positive constants R2(W) such that ϕ(u) ≤ 0 for u ∈ W\Br(0), where Br(0) is an open ball in W of radius r centered at 0. Then ϕ possesses an unbounded sequence of critical values.
Lemma 2.14 [15]. Suppose
(A1) ϕ ∈ C1(X, ℝ) is an even functional, then the subspace Xk, Yk, and Zk are defined by (2.2);
If for every k ∈ ℕ, there exists ρk > rk > 0 such that
(A2)
(A3)
(A4) ϕ satisfies the (PS)c condition for every c > 0.
Then ϕ has an unbounded sequence of critical values.
Lemma 2.15 [16]. Assume (A1) is satisfied, and there is a k0 > 0 so as to for each k ≥ k0, there exist ρk > rk > 0 such that
(A5)
(A6)
(A7)
(A8) ϕ satisfies the
Then ϕ has a sequence of negative critical values converging to 0.
Remark 2.3. ϕ satisfies the
3. Main results and proofs of the theorems
Theorem 3.1. Let F(t, x) satisfies the condition (A'), and suppose the following conditions hold:
(B1) there exist β > p+ and r > 0 such that
for a.e. t ∈ [0, T] and all |x| ≥ r in ℝN;
(B2) there exist positive constants μ > p+ and Q > 0 such that
uniformly for a.e. t ∈ [0, T];
(B3) there exists μ' > p+ and Q' > 0 such that
uniformly for a.e. t ∈ [0, T];
(B4) F(t, x) = F(t, -x) for t ∈ [0, T] and all x in ℝN.
Then system (1.1) has infinite solutions uk in
Remark 3.1. Suppose that F(t, ·) is continuously differentiable in x and p(t) ≡ p, then condition (B1) reduces to the well-known Ambrosetti-Rabinowitz condition (see [19]), which was introduced in the context of semi-linear elliptic problems. This condition implies that F(t, x) grows at a superquadratic rate as |x| → ∞. This kind of technical condition often appears as necessary to use variational methods when we solve super-linear differential equations such as elliptic problems, Dirac equations, Hamiltonian systems, wave equations, and Schrödinger equations.
Theorem 3.2. Assume that F(t, x) satisfies (A'), (B1), (B3), and (B4) and the following assumption:
(B5)
Then system (1.1) has infinite solutions uk in
Theorem 3.3. Assume that F(t, x) satisfies the following assumption:
(B6) F(t, x):= a(t)|x|γ, where a(t) ∈ L∞ (0, T; ℝ+) and 1 < γ < p- is a constant. Then system (1.1) has infinite solutions uk in
The proof of Theorem 3.1 is organized as follows: first, we show the functional ϕ defined by
satisfies the (PS) condition, then we verify for ϕ the conditions in Lemma 2.14 item-by-item, then ϕ has an unbounded sequence of critical values.
Proof of Theorem 3.1. Let
for all
It follows from (3.1) that
where Ω1:= {t ∈ [0, T]; |un(t)| ≤ r}, Ω2:= [0, T] \ Ω1 and C0 is a positive constant.
However, from (3.2), we have
Thus ||un|| is a bounded sequence in
By Lemma 2.8, the sequence {un} has a subsequence, also denoted by {un}, such that
and ||u||∞ ≤ C1||u|| by Lemma 2.8, where C1 is a positive constant.
Therefore, we have
i.e.,
By (3.4) and (3.5), we get 〈J'(u) - J'(un), u - un〉 → 0, i.e.,
so it follows Lemma 2.11 that {un} admits a convergent subsequence.
For any u ∈ Yk, let
and it is easy to verify that ||·||* defined by (3.6) is a norm of Yk. Since all the norms of a finite dimensional normed space are equivalent, so there exists positive constant C2 such that
In view of (B3), there exist two positive constants M1 and C3 such that
for a.e. t ∈ [0, T] and |x| ≥ C3.
It follows (3.7) and (3.8) that
where Ω3:= {t ∈ [0, T]; |u(t)| ≥ C3}, Ω4:= [0, T] \ Ω3 and C4 is a positive constant.
Since μ' > p+, there exist positive constants dk such that
For any u ∈ Zk, let
then we conclude βk → 0 as k → ∞.
In fact, it is obvious that βk ≥ βk + 1 > 0, so βk → β ≥ 0 as k → ∞. For every k ∈ ℕ, there exists uk ∈ Zk such that
As
In fact, for any fm ∈ {fn: n = 1, 2...,}, we have fm(uk) = 0, when k > m, so
for any fm ∈ {fn: n = 1, 2 ...,}, therefore u = 0.
By Lemma 2.8, when uk ⇀ 0 in
In view of (B2), there exist two positive constants M2 and C10 such that
uniformly for a.e. t ∈ [0, T] and |x| ≥ C5.
When ||u|| ≥ 1, we conclude
where Ω5:= {t ∈ [0, T]; |u(t)| ≥ C5}, Ω6:= [0, T] \ Ω5 and C6 is a positive constant.
Choosing rk = 1/βk, it is obvious that
then
i.e., the condition (A3) in Lemma 2.14 is satisfied.
In view of (3.9), let ρk:= max{dk, rk + 1}, then
and this shows the condition of (A2) in Lemma 2.14 is satisfied.
We have proved the functional ϕ satisfies all the conditions of Lemma 2.14, then ϕ has an unbounded sequence of critical values ck = ϕ(uk) by Lemma 2.14, we only need to show ||uk||∞ → ∞ as k → ∞.
In fact, since uk is a critical point of the functional ϕ, we have
Hence, we have
since ck → ∞, we conclude
by (3.14). In fact, if not, going to a subsequence if necessary, we may assume that
for all k ∈ ℕ and some positive constant C7.
Combining (A') and (3.14), we have
which contradicts ck → ∞. This completes the proof of Theorem 3.1.
Proof of Theorem 3.2. To prove {un} has a convergent subsequence in space
Proposition 3.1. Under the condition (B5), there exist two positive constants σ and α such that ϕ(u) ≥ α for all
Proof. In view of condition (B5), there exist two positive constants ε and δ such that
where C1 is the same as in (3.3), and
for a.e. t ∈ [0, T] and |x| ≤ δ.
Let σ:= δ/C1 and ||u|| = σ, since σ < 1, we have
by Lemmas 2.4 and 2.8.
Combining (3.15) and (3.16), we have
so we can choose σ small enough, such that
and this completes the proof of Proposition 3.1.
Proposition 3.2. For any finite dimensional subspace W of
Proof. The proof of Proposition 3.2 is the same as the proof of the condition (A2) in the proof of Theorem 3.1.
We have proved the functional ϕ satisfies all the conditions of Lemma 2.13, ϕ has an unbounded sequence of critical values ck = ϕ(uk) by Lemma 2.13. Arguing as in the proof of Theorem 3.1, system (1.1) has infinite
solutions {uk} in
Proof of Theorem 3.3. First, we show that ϕ satisfies the
However, from (3.17), we have
thus ||un|| is a bounded sequence in
In view of (3.4) and (3.5), we can also conclude
Let us prove ϕ'(u) = 0 below. Taking arbitrarily ωk ∈ Yk, notice when nj ≤ k we have
Going to limit in the right side of above equation reaches
so ϕ'(u) = 0, this shows that ϕ satisfies the
For any finite dimensional subspace
Otherwise, for any positive integer n, there exists un ∈ W \ {0} such that
Set
Since dimW < ∞, it follows from the compactness of the unit sphere of W that there exists a subsequence, denoted also by {vn}, such that {vn} converges to some v0 in W. It is obvious that ||v0|| = 1.
By the equivalence of the norms on the finite dimensional space W, we have vn → v0 in
By (3.20) and Hölder inequality, we have
Thus, there exist ξ1, ξ2 > 0 such that
In fact, if not, we have
for all positive integer n.
It implies that
as n → ∞, where C6 is the same in (3.3). Hence v0 = 0 which contradicts that ||v0|| = 1. Therefore, (3.22) holds. Now let
and
By (3.19) and (3.22), we have
for all positive integer n. Let n be large enough such that
then we have
for all large n, which is a contradiction to (3.21). Therefore, (3.18) holds.
For any u ∈ Zk, let
then we conclude γk → 0 as k → ∞ as in the proof of Theorem 3.1.
Let
so the condition (A7) in Lemma 2.15 is satisfied.
Furthermore, by (3.23), for any u ∈ Zk with ||u|| ≤ ρk, we have
Therefore,
so we have
for ρk, γk → 0, as k → ∞.
For any u ∈ Yk \ {0} with ||u|| ≤ 1,
where ε1 is given in (3.18), and
Choosing
i.e., the condition (A6) in Lemma 2.15 is satisfied. The proof of Theorem 3.3 is complete.
4. Example
In this section, we give three examples to illustrate our results.
Example 4.1. In system (1.1), let
Choose
so it is easy to verify that all the conditions (B1)-(B4) are satisfied. Then by Theorem
3.1, system (1.1) has infinite solutions {uk} in
Example 4.2. In system (1.1), let F(t, x) = |x|8 and
We choose
Example 4.3. In system (1.1), let F(t, x) = a(t)|x|3 where
and
It is easy to verify that all the conditions of Theorem 3.3 are satisfied. Then by
Theorem 3.3, so system (1.1) has infinite solutions {uk} in
Competing interests
The authors declare that they have no competing interests.
Authors' contributions
All the authors typed, read, and approved the final manuscript.
Acknowledgements
The authors thank the anonymous referees for valuable suggestions and comments which led to improve this article. This Project is supported by the National Natural Science Foundation of China (Grant No. 11171351).
References
-
Chen, Y, Levine, S, Rao, M: Variable exponent linear growth functionals in image restoration. SIAM J Appl Math. 66, 1383–1406 (2006). Publisher Full Text
-
Harjulehto, P, Hästö, P, Latvala, V: Minimizers of the variable exponent non-uniformly convex Dirichlet energy. J Math Pure Appl. 89, 174–197 (2008). Publisher Full Text
-
Dai, G: Three solutions for a Neumann-type differential inclusion problem involving the p(x)-Laplacian. Nonlinear Anal. 70, 3755–3760 (2009). Publisher Full Text
-
Dai, G: Infinitely many solutions for a differential inclusion problem in ℝN involving the p(x)-Laplacian. Nonlinear Anal. 71, 1116–1123 (2009). Publisher Full Text
-
Dai, G: Nonsmooth version of Fourtain theorem and its application to a Dirichlet-type differential inclusion problem. Nonlinear Anal. 72, 1454–1461 (2010). Publisher Full Text
-
Diening, L, Hästö, P, Nekvinda, A: Open problems in variable exponent Lebesgue and Sobolev spaces. In: Drábek P, Rákosník J (eds.) pp. 38–58. FSDONA04 Proceedings, Milovy, Czech Republic (2004)
-
Harjulehto, P, Hästö, P: An overview of variable exponent Lebesgue and Sobolev spaces. 85–93 Future Trends in Geometric Function Theory RNC Workshop, Jyväskylä (2003)
-
Samko, S: On a progress in the theory of Lebesgue spaces with variable exponent Maximal and singular operators. Integral Transfor Spec Funct. 16, 461–482 (2005). Publisher Full Text
-
Zhikov, VV: Averaging of functionals of the calculus of variations and elasticity theory. Math USSR Izv. 9, 33–66 (1987)
-
Fan, XL, Zhao, D: The quasi-minimizer of integral functionals with m(x) growth conditions. Nonlinear Anal. 39, 807–816 (2000). Publisher Full Text
-
Fan, XL, Zhao, D: On the space Lp(x) and Wm,p(x). J Math Anal Appl. 263, 424–446 (2001). Publisher Full Text
-
Fan, XL, Zhang, QH: Existence of solutions for p(x)-Laplacian Dirichlet problem. Nonlinear Anal. 52, 1843–1852 (2003). Publisher Full Text
-
Fan, XL, Fan, X: A Knobloch-type result for p(t)-Laplacian systems. J Math Anal Appl. 282, 453–464 (2003). Publisher Full Text
-
Wang, XJ, Yuan, R: Existence of periodic solutions for p(t)-Laplacian systems. Nonlinear Anal. 70, 866–880 (2009). Publisher Full Text
-
Bartsch, T: Infinitely many solutions of a symmetic Dirchlet problem. Nonlinear Anal. 68, 1205–1216 (1993)
-
Bartsch, T, Willem, M: On an elliptic equation with concave and convex nonlinearities. Proc Am Math Soc. 123, 3555–3561 (1995). Publisher Full Text
-
Mawhin, J, Willem, M: Critical Point Theory and Hamiltonian Systems. Springer, Berlin (1989)
-
Fan, XL, Han, XY: Existence and multiplicity of solutions for p(x)-Laplacian equations in ℝN. Nonlinear Anal. 59, 173–188 (2004)
-
Rabinowitz, PH: Minimax methods in critical point theory with applications to differential equations. CBMS Reg Conf Ser in Math, American Mathematical Society, Providence, RI (1986)



