Volume 2011, Issue 1 725045
Research Article
Open Access

Global Attractor for the Generalized Dissipative KDV Equation with Nonlinearity

Zai-yun Zhang

Corresponding Author

Zai-yun Zhang

School of Mathematical Science and Computing Technology, Central South University, Changsha 410075, Hunan, China csu.edu.cn

Department of Mathematics and Science, Hunan First Normal University, Feng Lin San Lu 1015, Changsha 410205, Hunan, China csu.edu.cn

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Zhen-hai Liu

Zhen-hai Liu

School of Mathematics and Computer Science, Guangxi University for Nationalities, Nanning 530006, Guangxi, China gxun.cn

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First published: 03 May 2011
Citations: 4
Academic Editor: Marco Squassina

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

In order to study the longtime behavior of a dissipative evolutionary equation, we generally aim to show that the dynamics of the equation is finite dimensional for long time. In fact, one possible way to express this fact is to prove that dynamical systems describing the evolutional equation comprise the existence of the global attractor [1]. The KDV equation without dissipative and forcing was initially derived as a model for one direction water waves of small amplitude in shallow water, and it was later shown to model a number of other physical stems. In recent years, the KDV equations has been always being an important nonlinear model associated with the science of solids, liquids, and gases from different perspectives both mathematics and physics. As for dissipative KDV equation, existence of a global attractor is a significant feature. In [2], Ghidaglia proved that for the dissipative KDV equation
(1.1)
with periodic boundary condition u(x, t) = u(x + L, t), there exists a weak global attractor of finite dimension. Later, there are many contributions to the global attractor of the dissipative KDV equation (see [310]). In [3], Guo and Wu proved the existence of global attractors for the generalized KDV equation
(1.2)
However, few efforts are devoted to the existence of global attractor for generalized dissipative four-order KDV equation with nonlinearity in unbounded domains. In this paper, we consider the existence of global attractor for generalized dissipative four-order KDV equation with nonlinearity as follows:
(1.3)
u(x, 0) = u0, where α, β > 0, (x, t) ∈ Ω × [0, T], and Ω is unbounded domain.

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 [1113]). 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 [1517]). 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 u0H3(Ω), fH1(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)) = (∫Ωu · ∇vdx) and the norm . While in the space H, we consider the scalar product (u, v) = (∫Ωu · vdx) and the norm .

Notice Ei, C, c, ci denote for different positive constants.

First, we assume that fH, and ϕ(u), g(u) satisfy the following conditions:
  • (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.

Secondly, we can rewrite (1.3) as the following equation with the above assumption:
(2.1)
u(x, 0) = u0, where α, β > 0, (x, t) ∈ Ω × [0, T].

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, u0H2, fH1, 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 BH2 in which sense the trajectories are attract to 𝒜, such that

(2.2)
where S(t) is semigroup operator generated by the problem (2.1).

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, u0H, fH, then for the solution u of the problem (2.1), one has the estimates

(3.1)
(3.2)
(3.3)

Proof. Taking the inner product of (2.1) with u, we have

(3.4)
where
(3.5)
here, we apply Young’s inequality and the condition (A4).

Thus, from (3.4), we get

(3.6)
By virtue of Gronwall′s inequality and (3.6), one has (3.1) and which implies (3.2) and (3.3).

Lemma 3.2. In addition to the conditions of Lemma 3.1, one supposes that

(3.7)
then one has the estimate
(3.8)
where
(3.9)

Proof. Taking the inner product of (2.1) with uxx, we have

(3.10)
where
(3.11)

Noticing that

(3.12)

Using Nirberg′s interpolation inequality and the Sobolev embedding theory (see [11]), we have

(3.13)

Due to Lemma 3.1 and conditions of Lemma 3.2, we get that

(3.14)

From (3.10) and above inequalities, we get

(3.15)
Setting Cγ = c8, then we can obtain that
(3.16)
Thus, by Gronwall’s inequality and (3.15), we get that
(3.17)
which implies
(3.18)
Therefore, we prove Lemma 3.2.

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)

    u0H2, fH1,

then for the solution u of the problem of (2.1), one has the following estimate
(3.19)
furthermore,
(3.20)

Proof. Taking the inner product of (2.1) with uxxxx, we have

(3.21)
where
(3.22)
By Young’s inequality and Lemmas 3.1 and 3.2, thus from (3.22), we have
(3.23)
Due to Lemmas 3.1 and 3.2 and (A3), we obtain
(3.24)

Using Young’s inequality, we have

(3.25)
By (3.21), (3.23) and (3.25), we get
(3.26)
that is,
(3.27)
where
(3.28)
By virtue of Gronwall’s inequality, we have
(3.29)
and (3.27) implies
(3.30)
Therefore, we prove Lemma 3.3.

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)

    u0H3, fH2,

then for the solution u of the problem of (2.1), we have the following estimates:
(3.31)
where
(3.32)
furthermore,
(3.33)

Proof. Taking the inner product of (2.1) with uxxxxxx, we have

(3.34)
where
(3.35)
(3.36)

Using Nirberg’s interpolation inequality and Young’s inequality, from (3.36) and Lemmas 3.13.3, we have

(3.37)
Due to the condition (4.3), we get
(3.38)
By direct calculations, it is easy to get that
(3.39)
Due to (3.34)–(3.39), we have
(3.40)
that is,
(3.41)
where
(3.42)
Using Gronwall′s inequality, we deduce that
(3.43)
moreover, (3.41) implies
(3.44)
Therefore, we prove Lemma 3.4.

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)

    u0Hm+1, fHm,

  • (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,

(3.45)
then there exists a unique global solution u for the problem (2.1) such that uL(0, T; Hm(Ω)), and furthermore,the semigroup operator S(t) associated with the problem of (2.1) is continuous and there exists an absorbing set BH2(Ω), where
(3.46)

Proof. Similar to the proof of Lemmas 3.13.4, we have

(3.47)
At the same time, we use the Galerkin method (see [11]) and Lemmas 3.13.4 to prove the existence of global solution for the problem (2.1). So, we omit them here.

Next, we will prove the uniqueness of the global solution.

Assume that u, v are two solutions of the problem (2.1) and w = uv, then we have

(3.48)

Taking the inner product in H of (2.1) with w, we have

(3.49)
where
(3.50)
Due to the condition
(3.51)
and from (3.49), we obtain
(3.52)
that is,
(3.53)
By application of Gronwall′s inequality, we get w = 0.

Finally, we recall some basic results in [11, 23] and by Lemmas 3.13.3, it is easy to prove that there exists an absorbing set

(3.54)
in H2(Ω). But as for the continuity of semigroup S(t), we can apply the following Lemmas 3.6, and 3.7 to prove the result.

Lemma 3.6. Suppose that u0H2, fH1, and ϕ(u), g(u) satisfy (A1)–(A4), there exists constant C > 0, such that

(3.55)

Now, we use the decomposition method to prove the continuity of S(t) for sake of overcoming the difficult of noncompactness.

Set fH1(Ω), , 0 ≤ λL ≤ 1, satisfies
(3.56)
then, for  all  η ∈ (0,1), there exists Lη > 0, such that
(3.57)
Assume that uη is solution of the following equation:
(3.58)
Setting
(3.59)
is a solution of the equation as follows:
(3.60)

Now, we prove the Lemma 3.6.

Proof. We take the scalar product in space H of (3.58) with uη, we get

(3.61)
Due to (A3) and Young’s inequality, we get
(3.62)
From (3.61), we obtain the following inequality:
(3.63)
By Gronwall’s inequality, one has
(3.64)
Hence, there exists C > 0, such that
(3.65)
and implies
(3.66)

We take the scalar product in space H of (3.58) with uηxx and similar to the proof of Lemma 3.2, we have

(3.67)
By application of Gronwall′s inequality, we deduce that
(3.68)
So, there exists C > 0, such that
(3.69)
and implies
(3.70)

We take the scalar product in space H of (3.58) with uηxxxx and similar to the proof of Lemma 3.3, we have

(3.71)
It is easy to prove that
(3.72)

We take the scalar product in space H of (3.58) with uηxxxxxx and similar to the proof of Lemma 3.4, we have

(3.73)
that is,
(3.74)

Hence, by Gronwall’s inequality, we get

(3.75)
At the same time, we have
(3.76)
and we omit them here.

Lemma 3.7. Under the conditions of Lemma 3.6, one has the following estimates

(3.77)
where Ci(η) > 0, (i = 1,2, 3).

Proof. We take the scalar product in space H of (3.60) with x2wη and noticing that

(3.78)
it is easy to get that
(3.79)
By Gronwall’s inequality, we have
(3.80)
From (3.60), we obtain
(3.81)

We take the scalar product in space H of (3.61) with x2wηxx and noticing that

(3.82)

By Young’s inequality and the Sobolev embedding theory (see [11]) and (3.81)-(3.82), we deduce that

(3.83)
Using Gronwall’s inequality, we obtain
(3.84)
The proof of Lemma 3.7 is completed.

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, s1N), 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

(4.1)
there exists an integer A > 0, such that
(4.2)
Let Ω = {x||x| < A|}, then the imbedding is compact. Thus,
(4.3)
is relatively compact in and has a finite -net , k = 1,2, …, m with , and ukB. We claim that is an ε-net of B in .

Indeed, for any uB, , then there exists a such that

(4.4)
Hence,
(4.5)
This completes the lemma.

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) : EE satisfy

(4.6)
where I is the identity operator and E is space H2(Ω). We also assume that
  • (1)

    S(t) is bounded, that is, for each R > 0, there exists a constant C > 0 such that ∥uEC implies ∥S(t)uER, (t ≥ 0),

  • (2)

    there is an bounded absorbing set B0E, that is, for any bounded set BE, there exists a constant T, such that S(t)BB0, for tT,

  • (3)

    S(t) is a continuous operator for t > 0, then S(t) has a compact global attractor

(4.7)
in the space E0, such that
  • (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

(4.8)
for any bounded set BH2(Ω) in which sense the trajectories are attracted to 𝒜 (see[9, 24]), using Kuratowski α-measure in order to overcome the non-compactness of the classical Sobolev embedding.

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 BE, the set ω(B) defined by is called the ω-limit set of B.

Remark 4.4. (1) It is easy to see that ψω(B) if and only if there exists a sequence of element ψnB and a sequence tn, such that

(4.9)

 (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)BB0, for all tt0.

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 tt0,

  • (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 xB  inf yAd(x, y).

Definition 4.7 (see [12], [27].)Kuratowski α-measure of set B is defined by the formula

(4.10)
for every bounded set B of a Banach space X.

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 + ) ≤ α(𝒜) + α(),

(3) α(𝒜) ≤ Max {α(𝒜), α()},

(4) if 𝒜, α(𝒜) ≤ α(),

(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

(4.11)
Taking ε = 1/n, (n = 1,2, …), we can find a sequence {tn}, t1 < t2 < ⋯tn < ⋯, such that
(4.12)
By , we get
(4.13)
First, we prove that 𝒜 = ω(B) is variant. As a matter of fact, if ψS(t)ω(B), then ψ = S(t)ϕ, for some ϕω(B). So, there exists a sequence ϕnB and tn such that S(t)ϕnϕ, that is,
(4.14)
which implies that ψω(B) and S(t)ω(B) ⊂ ω(B).

Conversely, if ψω(B), by (4.9), we can find two sequences ϕnB and tn such that S(tn)ϕnϕ. We need to prove that {S(tnt)ϕn} has a subsequence which converges in E. For any ε > 0, there exists a tε such that

(4.15)
which implies that
(4.16)
Hence, there exists an integer N, such that
(4.17)
Then, it follows that
(4.18)
Notice that contains only a finite number of elements, where N0 is fixed such that tnt ≥ 0, as nN0.

By properties (1)–(4) in Remark 4.8, we have

(4.19)
Let ε → 0, then we get that
(4.20)
This implies that {S(tnt)ϕn} is relatively compact. So, there exists a subsequence and ψE, such that
(4.21)
It is easy to see that ψω(B) and
(4.22)
furthermore, ϕS(t)ω(B).

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

(4.23)
For each n, there exist bnB0, (n = 1,2, …) satisfying
(4.24)
Whereas B is an absorbing set, S(tn)B0 and S(tn)bn belong to B, for n sufficiently large. As in the discussion above, we obtain that S(tn)bn is relatively compact admits at least one cluster point γ,
(4.25)
where t1 follows S(t1)B0B. So, γ𝒜 = ω(B) and this contradicts (4.24). The proof is complete.

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.

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