Global Attractor for the Generalized Dissipative KDV Equation with Nonlinearity
Abstract
We discuss global attractor for the generalized dissipative KDV equation with nonlinearity under the initial condition u(x, 0) = u0(x). We prove existence of a global attractor in space H2(Ω), by using decomposition method with cut-off function and Kuratowski α-measure in order to overcome the noncompactness of the classical Sobolev embedding.
1. Introduction
As we all know, the solutions to the dissipative equation can be described by a semigroup of solution operators. When the equation is defined in a bounded domain, if the semigroup is asymptotically compact, then the classical theory of semiflow yields the existence of a compact global attractor (see [11–13]). But, when the equation is defined in a unbounded domain, which causes more difficulties when we prove the existence of attractors. Because, in this case, the Sobolev embedding is not compact. Hence, we cannot obtain a compact global attractor using classical theory.
Fortunately, as far as we concerned, there are several methods which can be used to show the existence of attractors in the standard Sobolev spaces even the equations are defined in unbounded domains. One method is to show that the weak asymptotic compactness is equivalent to the strong asymptotic compactness by an energy method (see [9, 10, 14]). A second method is to decompose the solution operator into a compact part and asymptotically small part (see [15–17]). A third method is to prove that the solutions uniformly small for large space and time variables by a cut-off function (see [18, 19]) or by a weight function (see [20]).
Generally speaking, the energy method proposed by Ball depends on the weak continuity of relevant energy functions (see [21, 22]). However, for (1.3) in unbounded domains, it seems that the energy method is not easy to use. Consequently, in this paper, we will show the idea to obtain the existence of global attractor in unbounded domains by showing the solutions are uniformly small for large space by a cut-off function or weight function, and at the same time, we apply decomposition method and Kuratowski α-measure to prove our result in order to overcome the noncompactness of the classical Sobolev embedding.
This paper is organized as follows.
In Section 2, firstly, we recall some basic notations; secondly, we make precise assumptions on the nonlinearity g(u) and ϕ(u); finally, we state our main result of the global attractor for (1.3).
In Section 3, we show the existence of a absorbing set in H2(Ω).
In Section 4, we prove the existence of global attractor.
2. Preliminaries and Main Result
We consider the generalized dissipative four-order KDV equation (1.3), where Ω ⊂ Rn is unbounded domain and the initial data u0 ∈ H3(Ω), f ∈ H1(Ω), g(u) is nonlinearity.
Throughout the paper, we use the notation H = L2(Ω), Hs = Hs,2(Ω) with the scalar product and norms given, respectively, by (·, ·), |·|, and ((·, ·)), ∥·∥. In the space H2, we consider the scalar product ((u, v)) = (∫Ω∇u · ∇v dx) and the norm . While in the space H, we consider the scalar product (u, v) = (∫Ωu · v dx) and the norm .
Notice Ei, C, c, ci denote for different positive constants.
- (A1):
ϕ(u) ∈ C3, |ϕ(u)| ≤ A|u|5−σ, (A > 0, 0 < σ ≤ 4),
- (A2):
|ϕ′′(u)| ≤ A|u|3−σ, |ϕ′′(u)| ≤ A|u|2−σ,
- (A3):
g(u) ∈ C2, g(u) = g1(u) + g2(u), where g1(u) = γu, g2(u) = K|u|5(K > 0, γ > 0),
- (A4):
g(0) = 0, |g′(u)| ≤ C.
Finally, we state our main result is the following theorem.
Theorem 2.1. Let the generalized dissipative of four-order KDV equation with nonlinearity given by (2.1). Assume that ϕ(u), g(u) satisfy conditions (A1)–(A4) and, moreover, u0 ∈ H2, f ∈ H1, then for α, β, γ > 0, there exists a global attractor 𝒜 of the problem (2.1), that is, there is a bounded absorbing set B ∈ H2 in which sense the trajectories are attract to 𝒜, such that
3. Existence of Absorbing Set in Space H2(Ω)
In this section, we will show the existence of an absorbing set in space H2(Ω) by obtaining uniformly in time estimates. In order to do this, we start with the following lemmas.
Lemma 3.1. Assume that g(u) satisfied (A4), furthermore, u0 ∈ H, f ∈ H, then for the solution u of the problem (2.1), one has the estimates
Proof. Taking the inner product of (2.1) with u, we have
Thus, from (3.4), we get
Lemma 3.2. In addition to the conditions of Lemma 3.1, one supposes that
Proof. Taking the inner product of (2.1) with uxx, we have
Noticing that
Using Nirberg′s interpolation inequality and the Sobolev embedding theory (see [11]), we have
Due to Lemma 3.1 and conditions of Lemma 3.2, we get that
From (3.10) and above inequalities, we get
Lemma 3.3. Suppose that ϕ(u), g(u) satisfy (A2), (A3) and, moreover, the following conditions hold true:
- (1)
ϕ(u) ∈ C3, g(u) ∈ C2,
- (2)
u0 ∈ H2, f ∈ H1,
Proof. Taking the inner product of (2.1) with uxxxx, we have
Using Young’s inequality, we have
Lemma 3.4. Suppose that ϕ(u), g(u) satisfy (A2), (A3) and, moreover, the following conditions hold true:
- (1)
ϕ(u) ∈ C3, g(u) ∈ C2,
- (2)
u0 ∈ H3, f ∈ H2,
Proof. Taking the inner product of (2.1) with uxxxxxx, we have
Using Nirberg’s interpolation inequality and Young’s inequality, from (3.36) and Lemmas 3.1–3.3, we have
In a similar way as above, we can get the uniformly estimates of ∥uxxxx∥, ∥ut∥ and we omit them here.
Next, we will show the existence of global solution for the problem (2.1) as follows.
Lemma 3.5. Suppose that the following conditions hold true:
- (1)
u0 ∈ Hm+1, f ∈ Hm,
- (2)
ϕ(u) ∈ Cm+1, ∥ϕ(u)∥ ≤ A|u|5−σ, (σ, A > 0),
- (3)
g(u) ∈ Cm, |g2(u)| ≤ K|u|5,
- (4)
g(u) satisfies (A3), (A4) and g(u) is Lipschitz continuous, that is,
Proof. Similar to the proof of Lemmas 3.1–3.4, we have
Next, we will prove the uniqueness of the global solution.
Assume that u, v are two solutions of the problem (2.1) and w = u − v, then we have
Taking the inner product in H of (2.1) with w, we have
Finally, we recall some basic results in [11, 23] and by Lemmas 3.1–3.3, it is easy to prove that there exists an absorbing set
Lemma 3.6. Suppose that u0 ∈ H2, f ∈ H1, and ϕ(u), g(u) satisfy (A1)–(A4), there exists constant C > 0, such that
Now, we use the decomposition method to prove the continuity of S(t) for sake of overcoming the difficult of noncompactness.
Now, we prove the Lemma 3.6.
Proof. We take the scalar product in space H of (3.58) with uη, we get
We take the scalar product in space H of (3.58) with uηxx and similar to the proof of Lemma 3.2, we have
We take the scalar product in space H of (3.58) with uηxxxx and similar to the proof of Lemma 3.3, we have
We take the scalar product in space H of (3.58) with uηxxxxxx and similar to the proof of Lemma 3.4, we have
Hence, by Gronwall’s inequality, we get
Lemma 3.7. Under the conditions of Lemma 3.6, one has the following estimates
Proof. We take the scalar product in space H of (3.60) with x2wη and noticing that
We take the scalar product in space H of (3.61) with x2wηxx and noticing that
By Young’s inequality and the Sobolev embedding theory (see [11]) and (3.81)-(3.82), we deduce that
Using Lemmas 3.6 and 3.7, we can prove that S(t) is continuous.
4. Existence of Global Attractor in Space H2(Ω)
In this section, we prove that the semigroup operator S(t) associated with the problem (2.1) possesses a global attractor in space H2(Ω).
In order to prove our result, we need the following results.
Lemma 4.1 (see [23].)Assume that s > s1, (s, s1 ∈ N), then the following embedding into is compact.
Proof. Let be a bounded set. It suffices to prove that B has a finite ε-net for any ε > 0. First, since
Indeed, for any u ∈ B, , then there exists a such that
Lemma 4.2 (see [7], [11].)Let E be Banach space and {S(t), t ≥ 0} a set of semigroup operators, that is, S(t) : E → E satisfy
- (1)
S(t) is bounded, that is, for each R > 0, there exists a constant C > 0 such that ∥u∥E ≤ C implies ∥S(t)u∥E ≤ R, (t ≥ 0),
- (2)
there is an bounded absorbing set B0 ⊂ E, that is, for any bounded set B ⊂ E, there exists a constant T, such that S(t)B ⊂ B0, for t ≥ T,
- (3)
S(t) is a continuous operator for t > 0, then S(t) has a compact global attractor
- (1)
S(t)𝒜 = 𝒜, t ≥ 0,
- (2)
dist (S(t)B,𝒜)E → 0 as t → +∞, and dist (S(t)B,𝒜)E denotes the Hausdorff semidistance defined as
Firstly, we need the following definitions.
Definition 4.3 (see [11], [25].)Let {S(t)} t≥0 be a semigroup in complete metric space E. For any subset B ⊂ E, the set ω(B) defined by is called the ω-limit set of B.
Remark 4.4. (1) It is easy to see that ψ ∈ ω(B) if and only if there exists a sequence of element ψn ∈ B and a sequence tn → ∞, such that
(2) If ω(B) is ω-limit compact set, then, for every bounded subset B of E and for any ε > 0, there exists a t0 > 0, such that .
Definition 4.5 (see [11], [26].)Let {S(t)}t≥0 be a semigroup in complete metric space E. A subset B0 of E is called an absorbing set in E if, for any bounded subset B of E, there exists some t0 ≥ 0, such that S(t)B ⊂ B0, for all t ≥ t0.
Definition 4.6 (see [11], [26].)Let {S(t)}t≥0 be a semigroup in complete metric space E. A subset 𝒜 of E is called global attractor for the semigroup if 𝒜 is compact and enjoys the following properties:
- (1)
𝒜 is a invariant set, that is, S(t)𝒜 = 𝒜, for any t ≥ t0,
- (2)
𝒜 attract all bounded set of E, that is, for any bounded subset B of E, dist (S(t)B, 𝒜) → 0, as t → ∞, where dist (B, A) is Hausdorff semidistance of two set B and A in space E: dist (B, A) = sup x∈B inf y∈A d(x, y).
Definition 4.7 (see [12], [27].)Kuratowski α-measure of set B is defined by the formula
Secondly, due to Definition 4.6, it is easy to see that Kuratowski α-measure of set B has the following properties.
Remark 4.8. (1) If 𝒜 is compact set, then α(𝒜) = 0;
(2) α(𝒜 + ℬ) ≤ α(𝒜) + α(ℬ),
(3) α(𝒜 ∪ ℬ) ≤ Max {α(𝒜), α(ℬ)},
(4) if 𝒜 ≤ ℬ, α(𝒜) ≤ α(ℬ),
(5) .
Thirdly, we prove Theorem 2.1.
Proof. Using the result of [11], we have S(t) is ω-limit compact and B is bounded, for any ε > 0, there exists t ≥ 0 such that
Conversely, if ψ ∈ ω(B), by (4.9), we can find two sequences ϕn ∈ B and tn → ∞ such that S(tn)ϕn → ϕ. We need to prove that {S(tn − t)ϕn} has a subsequence which converges in E. For any ε > 0, there exists a tε such that
By properties (1)–(4) in Remark 4.8, we have
Next, by virtue of Lemma 4.2 and the result of [11, 12], we prove that 𝒜 = ω(B) is an global attractor in E and attracts all bounded subsets of E.
Otherwise, then there exists a bounded subset B0 of E such that dist (S(t)B0, 𝒜) does not tend to 0 as t → ∞. Thus, there exists a δ > 0 and a sequence tn → ∞ such that
Acknowledgments
The authors are highly grateful for the anonymous referee’s careful reading and comments on this paper. The Z.-Y. Zhang would like to thank Professor Dr. Zhen-hai Liu, who is his Ph. D supervisor, for his valuable attention to our paper. This work was supported by the Graduate Degree Thesis Innovation Foundation of Central South University Grant no. CX2010B115 (China), the Doctoral Dissertation Innovation Project of Central South University Grant no. 2010ybfz016 (China), the NNSF of China Grant no. 10971019, and the Foundation (2010) of Guangxi Education Department.