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Existence of the uniform attractors for a non-autonomous modified Swift-Hohenberg equation
Advances in Difference Equations volume 2015, Article number: 153 (2015)
Abstract
The paper is concerned with the non-autonomous modified Swift-Hohenberg equation \(u_{t}+{\triangle }^{2}u+2{\triangle }u+au+b|\nabla u|^{2}+u^{3}=g(x,t)\). It is shown that a uniform attractor exists in \(H_{0}^{2}\) when the external force only satisfies the translation bounded condition instead of translation compactness. In order to overcome the difficulty caused by the critical nonlinearity terms \(u^{3}\) and the parameter b belonging to the real set \(\mathbb{R}\), we take advantage of the Gagliardo-Nirenberg inequality several times.
1 Introduction
The Swift-Hohenberg type equations arise in the study of convective hydrodynamics, plasma confinement in toroidal devices, viscous film flow, and bifurcating solutions of the Navier-Stokes equations; see [1]. The long-time behavior, bifurcation, and the pattern selections of the solution for this equation have been investigated in [2–4].
We are concerned with the following non-autonomous modified Swift-Hohenberg equation:
where \(\mathbb{R}_{\tau}=[\tau,+\infty)\), Ω is an open connected bounded domain in \(\mathbb{R}^{2}\) with a smooth boundary ∂Ω, a and b are arbitrary constants, \(u_{t}=\frac{\partial u}{\partial t}\), and g is an external forcing term with \(g(x,t)\in L_{\mathrm{C}^{*}}^{2}(\mathbb{R};X)\). If \(b=0\) and \(g\equiv0\), then (1.1) is the usual Swift-Hohenberg equation. The system (1.1)-(1.3) with \(g\equiv0\) was proposed by the authors in [5] as a pattern formation system with two unbounded spatial directions that is near the onset to instability. Polat studied the existence of global attractors for the problem (1.1) when \(g\equiv0\) in [6] and Song et al. improved the result by showing that the system possesses a global attractor in \(H^{k}\) spaces in [7]. Recently, the authors established the existence of pullback attractors for (1.1)-(1.3) in [8]. To the best of our knowledge, the existence of the uniform attractors for a non-autonomous modified Swift-Hohenberg equation has not yet been considered; it is presently our concern.
In the last two decades, the dynamical systems and their attractors have been extensively studied, please refer to [9–13] and references therein. As we know, the most general methods dealing with the non-autonomous dynamical systems were presented by Chepyzhov and Vishik in their work in [14], and these methods make the general theory of autonomous systems applicable, but it is unsatisfactory that it can only be used in handling the problems with translation compact symbols. In 2005, in [15], the authors presented a new notation and obtained their abstract results by means of the methods introduced in [10] to deal with 2D Navier-Stokes equations with a normal external force in \(L_{\mathrm{loc}}^{2}(\mathbb{R},L^{2})\) which is translation bounded but not translation compact. In the sequel, in [16], a new class of time-dependent external forces in \(L_{\mathrm{C}^{*}}^{2}(\mathbb{R},X)\) was presented, where \(L_{\mathrm{C}^{*}}^{2}(\mathbb{R},X)\) denotes the set of all functions satisfying condition (\(\mathrm{C}^{*}\)) (see below Definition 2.4) and the functions in \(L_{\mathrm{C}^{*}}^{2}(\mathbb{R},X)\) are translation bounded but not translation compact in \(L_{\mathrm{loc}}^{2}(\mathbb{R},L^{2})\). Moreover, the authors proved the existence of uniform attractors for the weakly damped non-autonomous hyperbolic equations. Motivated by [15, 16], in the present paper, we illustrate the existence of uniform attractors for a non-autonomous modified Swift-Hohenberg equation (1.1)-(1.3) using the techniques in [15, 16].
This paper is organized as follows: in Section 2, we give some basic definitions and abstract results concerning the uniform attractors for non-autonomous dynamical systems. In Section 3, we will show the uniformly bounded absorbing set and uniform attractors in \(H_{0}^{2}\).
2 Non-autonomous systems and their attractors
In this subsection, we iterate some basic definitions and abstract results concerning the uniform attractors for non-autonomous dynamical systems in [15, 16], which are important to get our main results.
With the usual notation, we denote \(H=L^{2}(\Omega)\), and endow H with the standard scalar product and norm \((\cdot,\cdot)\), \(\|\cdot\|\). For simplicity, we denote \(V=H_{0}^{2}(\Omega)\) with norm \(\|u\| _{H_{0}^{2}(\Omega)}=\|\triangle u\|\), and write \(\|\cdot\|_{m,p}\) and \(\|\cdot\|_{p}\) as the norm of \(W^{m,p}(\Omega)\) and \(L^{p}(\Omega)\), respectively.
We let an operator \(A=\triangle^{2}\) and λ be the first eigenvalues of A; by the Poincaré inequality, we have
Let E be a Banach space, and let a two-parameter family of mappings \(\{U(t,\tau)\}=\{U(t,\tau)|t\geq\tau, \tau\in\mathbb{R}\}\) act on E:
Definition 2.1
Let Σ be a parameter set. \(\{ U_{\sigma}(t,\tau)| t\geq\tau, \tau\in\mathbb{R}\}\), \(\sigma\in\Sigma\) is said to be a family of processes in Banach space E, if for each \(\sigma\in\Sigma\), \(\{U_{\sigma}(t,\tau)\}\) is a process, that is, the two-parameter family of mappings \(\{U_{\sigma}(t,\tau)\}\) from E to E satisfy
where Σ is called the symbol space and \(\sigma\in\Sigma\) is the symbol.
A set \(B_{0}\subset E\) is said to be uniformly (w.r.t. \(\sigma\in\Sigma \)) absorbing set for the family of processes \(\{U_{\sigma}(t,\tau)\}\), \(\sigma\in\Sigma\), if for any \(\tau\in\mathbb{R}\) and \(B\in\mathcal {B}(E)\), there exists \(t_{0}=t_{0}(\tau,B)\geq\tau\) such that \(\bigcup_{\sigma \in\Sigma}U_{\sigma}(t,\tau)B\subset B_{0}\) for all \(t\geq t_{0}\). A set \(Y\subset E\) is said to be uniformly (w.r.t. \(\sigma\in\Sigma\)) attracting for the family of processes \(\{U_{\sigma}(t,\tau)\}\), \(\sigma \in\Sigma\), if for any fixed \(\tau\in\mathbb{R}\) and every \(B\in\mathcal{B}(E)\),
where \(\mathcal{B}(E)\) is the set of all bounded subset of E.
Assumption I
Let \(\{T(h)|h\geq0\}\) be a family of operators acting on Σ and satisfy:
-
(i)
\(T(h)\Sigma=\Sigma\), \(\forall h\in\mathbb{R^{+}}\);
-
(ii)
translation identity:
$$ U_{\sigma}(t+h,\tau+h)=U_{T(h)\sigma}(t,\tau),\quad \forall \sigma\in \Sigma ,t\geq\tau,\tau\in\mathbb{R},h\geq0. $$(2.5)
Definition 2.2
A family of processes \(\{U_{\sigma}(t,\tau )\}\), \(\sigma\in\Sigma\) is said to be satisfying uniformly (w.r.t. \(\sigma\in\Sigma\)) condition (C) if for any fixed \(\tau\in\mathbb{R}\), \(B\in\mathcal{B}(E)\), and \(\varepsilon>0\), there exist a \(t_{0}=t_{0}(\tau,B,\varepsilon)\geq\tau\) and a finite dimensional subspace \(E_{m}\) of E such that
-
(i)
\(P_{m}(\bigcup_{\sigma\in\Sigma}\bigcup_{t\geq t_{0}}U_{\sigma}(t,\tau)B)\) is bounded;
-
(ii)
\(\|(I-P_{m})(\bigcup_{\sigma\in\Sigma}\bigcup_{t\geq t_{0}}U_{\sigma}(t,\tau )x)\|_{E}\leq\varepsilon\), \(\forall x\in B\),
where \(\operatorname{dim}E_{m}=m\) and \(P_{m}:E\rightarrow E_{m}\) is a bounded projector.
Theorem 2.3
Let Σ be a complete metric space, and Assumption I holds. Then a family of processes \(\{U_{\sigma}(t,\tau)\} \), \(\sigma\in\Sigma\), possess the compact uniform (w.r.t. \(\sigma\in \Sigma\)) attractor \(\mathcal{A}_{\Sigma}\) in E satisfying
if it:
-
(i)
has a bounded uniformly (w.r.t. \(\sigma\in\Sigma\)) absorbing set \(B_{0}\);
-
(ii)
satisfies uniformly (w.r.t. \(\sigma\in\Sigma\)) condition (C).
Moreover, if E is a uniformly convex Banach space, then the converse is true.
Remark 1
Theorem 2.3 is true without any continuous assumption on \(\{U_{\sigma}(t,\tau)\}\), \(\sigma\in\Sigma\), and \(\{T(t)\} _{t\geq0}\).
Definition 2.4
Let X be a Hilbert space. A function \(g\in L_{\mathrm{loc}}^{2}(\mathbb{R};X)\) is said to satisfy condition (\(\mathrm {C}^{*}\)) if for any \(\varepsilon>0\), there exists a finite dimensional subspace \(X_{1}\) of X such that
where \(P_{m}:X\rightarrow X_{1}\) is the canonical projector.
Denote by \(L_{\mathrm{C}^{*}}^{2}(\mathbb{R};X)\) the set of all functions satisfying condition (\(\mathrm{C}^{*}\)).
Lemma 2.5
If \(h\in L_{\mathrm{C}^{*}}^{2}(\mathbb{R};X)\), then for any \(\varepsilon>0\) and \(\tau\in\mathbb{R}\), we have
where \(P_{m}\) is the same as in Definition 2.4 and α is a positive constant.
Lemma 2.6
[9, 14] (Gagliardo-Nirenberg inequality)
Let Ω be an open, bounded domain of the Lipschitz class in \(\mathbb {R}^{n}\). Assume that \(1\leq p\leq\infty\), \(1\leq q\leq\infty\), \(r\geq1\), \(0<\theta\leq1\), and that
Then the following inequality holds:
3 Uniformly (w.r.t. \(\sigma\in\Sigma\)) absorbing set and uniform (w.r.t. \(\sigma\in\Sigma\)) attractor in V
For the existence of the solutions for (1.1)-(1.3), since the time-dependent term introduces no essential complications, we directly give the following results of the existence and uniqueness of solution without proof. In fact, the proof is based on the Faedo-Galerkin approximation approaches; see [9] for the details.
Theorem 3.1
If g and \(u_{\tau}\) are given satisfying \(g\in L_{\mathrm{loc}}^{2}(\mathbb{R};H)\), \(u_{\tau}\in V\), then (1.1)-(1.3) have a unique solution
We now give a fixed external force \(g_{0}\) in \(L_{b}^{2}(\mathbb{R};X)\) and define the symbol space \(\mathcal{H}(g_{0})\) for (1.1)-(1.3). Let a fixed symbol \(\sigma_{0}(s)=g_{0}(s)=g_{0}(\cdot,s)\) satisfy condition (\(\mathrm {C}^{*}\)) in \(L_{\mathrm{loc}}^{2}(\mathbb{R};X)\). That is, the family of translations \(\{g_{0}(s+h),h\in\mathbb{R}\}\) form a function set satisfying condition (\(\mathrm{C}^{*}\)). Therefore
where \([\ ]\) denotes the closure of a set in a topological space \(L_{\mathrm{loc}}^{2,w}(\mathbb{R};X)\).
Thus, for any \(g(x,t)\in\mathcal{H}(g_{0})\), the problem (1.1)-(1.3) with g instead of \(g_{0}\) possesses a corresponding process \(\{ U_{g}(t,\tau)\}\) acting on V.
Proposition 3.2
If X is a reflexive separable, then
-
(1)
for all \(g_{1}\in\mathcal{H}(\phi)\), \(\|g_{1}\|_{L_{b}^{2}(\mathbb{R};X)}^{2}\leq \|g\|_{L_{b}^{2}(\mathbb{R};X)}^{2}\);
-
(2)
the translation group \(\{T(t)\}\) is weakly continuous on \(\mathcal {H}(g)\);
-
(3)
\(T(t)\mathcal{H}(g)=\mathcal{H}(g)\) for all \(t\in\mathbb{R}\).
Therefore, the family of processes \(\{U_{g}(t,\tau)\}\), \(g\in\mathcal {H}(g_{0})\), \(U_{g}(t,\tau):E\rightarrow E\), \(t\geq\tau\), \(\tau\in\mathbb{R}\) are defined. Furthermore, the translation semigroup \(\{T(h)|h\in\mathbb{R^{+}}\}\) satisfies \(\forall h\in\mathbb{R^{+}}\), \(T(h)\mathcal{H}(g_{0})=\mathcal{H}(g_{0})\), and the following translation identity holds:
For (1.1)-(1.3), we give a fixed external force \(g_{0}\in L_{\mathrm{C}^{*}}^{2}(\mathbb{R};H)\) and \(\mathcal{H}(\sigma_{0})=\mathcal{H}(g_{0})=[g_{0}(x,s+h)|h\in\mathbb {R}]_{L_{\mathrm{loc}}^{2,w}(\mathbb{R};H)}\).
For convenience, hereafter we denote by c an arbitrary positive constant, which may be different from line to line and even in the same line.
3.1 A priori estimates
Theorem 3.3
If \(g_{0}\in L_{b}^{2}(\mathbb{R};H)\), \(u_{\tau}\in V\), then the family of processes \(\{U_{g}(t,\tau)\}\), \(g\in\mathcal {H}(h_{0})\) corresponding to the problem (1.1)-(1.3) has a bounded uniformly (w.r.t. \(g\in\mathcal{H}(h_{0})\)) absorbing set \(B_{0}\) in V.
Proof
The proof of this results follows from the following two steps.
Step 1: Taking the scalar products in H of (1.1) with u, we find
and the Hölder and Poincaré inequalities give
We use the Gagliardo-Nirenberg inequality with \(k=1\), \(n=p=r=m=q=2\), \(\theta =\frac{1}{2}\) and get
Similarly, by the Hölder inequality, the Gagliardo-Nirenberg inequality with \(k=1\), \(n=m=q=2\), \(p=r=4\), \(0<\theta<\frac{1}{2}\), and the Young inequality, it follows that
Substituting (3.3), (3.4) into (3.2), we see that
Since \(3<\frac{3-2\theta}{1-\theta}<4\) (\(0<\theta<\frac{1}{2}\)), there exists \(M>0\) such that
Thus we arrive at
Again in line with the Poincaré inequality, we obtain
From Proposition 3.2, recall that
and set \(\delta=\frac{\lambda}{2}\), then by the Gronwall lemma,
Now, multiplying (3.10) by \(e^{\delta t}\) and integrating it over \((\tau ,t)\), we get
Analogously, multiplying (3.7) by \(e^{\delta t}\) and integrating it over \((\tau,t)\) and together with (3.11), we derive that
Step 2: Multiplying (1.1) by \(\triangle^{2}u\) in H we get
Using the Hölder and Young inequalities, we get
The Gagliardo-Nirenberg inequality with \(k=1\), \(p=4\), \(n=m=q=r=2\), \(\theta =\frac{1}{4}\) yields
The Gagliardo-Nirenberg inequality with \(k=0\), \(p=6\), \(n=m=q=r=2\), \(\theta =\frac{1}{6}\) gives
Substituting these estimates into (3.14), and combining with the Poincaré inequalities, we obtain
Multiplying this by \((t-\tau)e^{\delta t}\) and integrating it over \((\tau, t)\), we derive that
and hence
Now, we estimate the terms on the right-hand side of (3.15):
By (3.12), we get
By (3.10) and the Hölder inequalities for the sum, we have
noting that we used the fact \(e^{-2\delta(s-\tau)}\leq1\) for \(s\in[\tau , t]\) in the last inequality.
In addition,
Collecting all inequalities (3.15)-(3.19),
Choosing \((1+\frac{1}{t-\tau} )(1+\delta(t-\tau))e^{-\delta (t-\tau)}\|u_{\tau}\|^{2}+(t-\tau)e^{-\delta(t-\tau)}(\|u_{\tau}\|^{6}+\| u_{\tau}\|^{10}) + (1+\frac{1}{t-\tau} )(1+\|g_{0}\|_{L_{b}^{2}}^{2})\leq (M+\frac{\| g_{0}\|_{L_{b}^{2}}^{2}}{2\delta} )^{3}+ (M+\frac{\|g_{0}\| _{L_{b}^{2}}^{2}}{2\delta} )^{5}\) for \(t>\tau\), we deduce that there exists a time \(t_{0}=t_{0}(\delta, \|g_{0}\|_{L_{b}^{2}}^{2}, \|u_{\tau}\|)>\tau\) such that \(B_{0}=\{u:\|\triangle u(t)\|^{2}\leq\rho^{2}\}\), where \(\rho^{2}=c [ (M+\frac{\|g_{0}\|_{L_{b}^{2}}^{2}}{2\delta} )^{3}+ (M+\frac{\|g_{0}\|_{L_{b}^{2}}^{2}}{2\delta} )^{5} ]\), for \(t\geq t_{0}\), i.e., \(B_{0}\) is the uniformly (w.r.t. \(\sigma\in\Sigma\)) absorbing ball for the process \(\{U_{\sigma}(t,\tau)\}\) in V. □
3.2 Uniform attractor in V
Now we prove the existence of compact uniform (w.r.t. \(h\in\mathcal {H}(g_{0})\)) attractor for the problem (1.1)-(1.3) with the external forces \(g_{0}\in L_{\mathrm{C}^{*}}^{2}(\mathbb{R};H)\) in V.
Theorem 3.4
If \(g_{0}(x,t)\in L_{\mathrm{C}^{*}}^{2}(\mathbb{R};H)\), then the family of processes \(\{U_{g}(t,\tau)\}\), \(g\in\mathcal{H}(g_{0})\) corresponding to the problem (1.1)-(1.3) possess a compact uniform (w.r.t. \(g\in\mathcal{H}(g_{0})\)) attractor \(\mathcal {A}_{\mathcal{H}(g_{0})}\) in V satisfying
where \(B_{0}\) is the uniformly (w.r.t. \(h\in\mathcal{H}(g_{0})\)) absorbing set in V.
Proof
By Theorem 2.3, we need only to verify that the family of processes \(\{U_{g}(t,\tau)\}\), \(g\in\mathcal{H}(g_{0})\), satisfy uniformly (w.r.t. \(g\in\mathcal{H}(g_{0})\)) condition (C).
Since \(A^{-1}\) is a continuous compact operator in H, by the classical spectral theorem, there exists a sequence \(\{\lambda_{j}\} _{j=1}^{\infty}\) with
and a family of elements \(\{\omega_{j}\}_{j=1}^{\infty}\) of V which are orthonormal in H with
Let \(H_{m}=\operatorname{span}\{\omega_{1},\omega_{2},\ldots,\omega_{m}\}\), and \(P_{m}:H\rightarrow H_{m}\) be an orthogonal projector. For any \(u\in V\), we write
Taking the scalar product of (1.1) with \(\triangle ^{2}u_{2}\) in H and using the Young inequality, similar to the estimates (3.14), we get
where \(M_{1}=c(\rho^{2}+\rho^{4}+\rho^{6})\). Thus, we see that
By the Gronwall lemma,
Since \(g\in L_{\mathrm{C}^{*}}^{2}(\mathbb{R};H)\), by Lemma 2.5, for any \(\varepsilon >0\), there exists an m large enough such that
Let \(t_{1}=\tau+\frac{1}{\lambda_{m}}\ln\frac{3\rho^{2}}{\varepsilon}\). Then we conclude that
Obviously, we can choose \(\varepsilon>0\) such that
Therefore, combining with (3.24)-(3.27) leads to
which indicates that the family of processes \(\{U_{g}(t,\tau)\}\), \(g\in \mathcal{H}(g_{0})\), satisfies uniformly (w.r.t. \(g\in\mathcal{H}(g_{0})\)) condition (C) in V. The proof is completed. □
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Acknowledgements
This work was supported by the NSFC (11361053, 11101334) and the NSF of Gansu Province (145RJZA112, 145RJZA232).
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Xu, L., Ma, Q. Existence of the uniform attractors for a non-autonomous modified Swift-Hohenberg equation. Adv Differ Equ 2015, 153 (2015). https://doi.org/10.1186/s13662-015-0492-9
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DOI: https://doi.org/10.1186/s13662-015-0492-9