The Long-Time Behavior of 2D Nonautonomous g-Navier-Stokes Equations with Weak Dampness and Time Delay
Abstract
In this paper, we discuss the long-time behavior of g-Navier-Stokes equations with weak dampnesss and time delay. The uniformly attracting sets of processes are obtained. On the basis of the method with asymptotic compactness, the existence of the uniform attractor for the equation is proved with the restriction of the forcing term belonging to translational compacted function space.
1. Introduction
The understanding of the behavior with dynamical systems was one of the most important problems of modern mathematical physics (see [1–17]). In the last decades, g-Navier-Stokes equations have received increasing attention due to their importance in the fluid motion. In [2–4], the existence of weak solution and strong solution for the 2D g-Navier-Stokes equation on some bounded domain was studied. The Hausdorff and fractal dimension of the global attractor about the 2D g-Navier-Stokes equation for the periodic and Dirichlet boundary conditions and the global attractor of the 2D g-Navier-Stokes equation on some unbounded domains were researched in [5]. In [6–10], the finite dimensional global attractor and the pullback attractor for g-Navier-Stokes equation were studied. Moreover, Anh et al. studied long-time behavior for 2D nonautonomous g-Navier-Stokes equations and the stability of solutions to stochastic 2D g-Navier-Stokes equation with finite delays in [11, 12]; Quyee researched the stationary solutions to 2D g-Navier-Stokes equation and pullback attractor for 2D g-Navier-Stokes equation with infinite delays in [13]. Recently, the random attractors for the 2D stochastic g-Navier-Stokes equation were researched in [14]. From these researches, we can see that the attractor of 2D g-Navier-Stokes equation is still important. We would like to use the theory of uniform attractors to study it. So, the present research is necessary and has a theoretical basis.
This paper is organized as follows. In Section 2, we first introduce some notations and preliminary results for the g-Navier-Stokes equation. In Section 3, we prove existence of the uniform attractor of 2D g-Navier-Stokes equation with weak dampness and time delay on the bounded domains.
2. Preliminaries
Let with the inner products (u, v) = ∫Ωu · νgdx and the norms |·| = (·,·)1/2, u, v ∈ L2(g). Let , which is endowed with the inner products and the norms ‖·‖ = ((·,·))1/2, where
Let D(Ω) be the space of function with the compact support contained in Ω, and let ℵ = {v ∈ (D(Ω))2:∇ · gv = 0 on Ω}; the closure of ℵ in L2(g) is Hg; the closure of ℵ in is Vg. Hg has the inner product and norm of L2(g), And Vg has the inner product and norm of .
We define a g-Laplacian operator as follows: −Δgu = −(1/g)(∇·g∇)u = −Δu − (1/g)∇g · ∇u.
From [2], we can define a g-orthogonal projection Pg : L2(g)⟶Hg and a g-Stokes operator Agu = −Pg((1/g)(∇·(g∇u))).
Let T > τ, . For every t ∈ (τ, T), we define ut(s) = u(t + s), s ∈ (−h, 0). For convenience, we denote .
- (I)
is measureable,
- (II)
∀t ∈ R, h(t, 0) = 0,
- (III)
∃Lg > 0, such that , there is
- (IV)
∃m0 ≥ 0, Cg > 0, ∀m ∈ [0, m0], τ ≤ t, u, v ∈ C0([τ − r, t]; Hg), such that
Definition 1. Let and satisfy the hypotheses (I)-(IV). For every τ ∈ R, a function u ∈ L2(τ, T; Vg)∩L∞(τ, T; Hg), ∀T > τ is called a weak solution of problem (1) if it fulfils
We can obtain the following theorem by the standard Faedo-Galerkin methods, where we let T > τ > 0. Other cases can be similarly proved.
Theorem 2. Let satisfies the assumptions (I)-(IV), there exists a unique solution
Proof. We apply the Faedo-Galerkin methods. Since Vg is separable and ℵ is dense in Vg, there exists a sequence , which forms a complete orthonormal system in Hg and a basic for Vg. Let m be a positive integer, for each m, we define an approximate solution um of (6) as , which satisfies
We can write the differential equations in the usual form
Let ϕim(0) be the ith component of u0m. The nonlinear ordinary differential system (18) has a maximal solution defined on some interval [0, tm]. If tm < T, then |um(t)|⟶∞ as t⟶tm. The following we will prove tm = T. We need several estimates to do.
We multiply (16) by ϕjm(t) and add these equations for j = 1, ⋯, m to obtain
Then, we have
so that
Let , then
By the Gronwall inequality, we have
Hence,
Then,
We intergrate (26) from 0 to T; we have
So, the um remains in a bounded set of L2(0, T; Vg).
Let denotes the function from R into Vg, which is equal to um on [0, T] and to 0 on the complement of this interval. The Fourier transform of is denoted by . Then, we will show that there exist a positive constant C and γ such that
Since the um remains in a bounded set of L2(0, T; Vg), the remains in a bounded set of Hγ(R; Vg, Hg). Since has two discontinuities at 0 and T, the distribute derivative of is given by
We obtain
So, fm(t) belongs to a bounded set in the space . For ∀m, we have Since um(0)| and |um(T)| are bounded, from (31), we obtain
Let γ < (1/4), we have
Since um ∈ L2(0, T; Vg), by the Parseval equality and by the Schwarz inequality and the Parseval equality, we obtain
So, um ∈ Hγ(R; Vg, Hg), and um remains in a bounded set of L∞(0, T; Hg), L2(0, T; Vg) and Hγ(R; Vg, Hg). There exists an element u ∈ L2(0, T; Vg)∩L∞(0, T; Hg) and a subsequence such that in L2(0, T; Vg) weakly and in L∞(0, T; Vg) weak-star as m′⟶∞. For any , we have strongly in .
For any support of wj, we have strongly in . Let ψ be a continuously differentiable function on [0, T] with ψ(T) = 0, we multiply (16) by ψ(t), then integrate by parts,
We have
Finally, we prove that u satisfies (7). We multiply (6) by ψ and integrate
We compare (39) with (40) to obtain (u(0) − u0, v)ψ(0) = 0. Let ψ(0) = 1, then we have (u(0) − u0, v) = 0, ∀v ∈ Vg. So, u(0) = u0.
Now, we will prove the solution of (6) and (7) is unique. We let u1 and u2 be the solutions of (9) and u = u1 − u2. We have
We take the scalar product of (41) with u(t), then
Therefore,
Then,
We have
Hence, |u(t)|2 = 0, ∀t ∈ [0, T]. So, u1 = u2.
From [15], we can define a family of two parametric maps {Uf(t, τ)} = {Uf(t, τ) | t ≥ τ, τ ∈ R} in Hg,
Here, is called the time symbol of the system. We have the following concepts and conclusions from [15].
Definition 3. For the given time symbol , a family of two-parametric maps {U(t, τ)} with t ≥ τ ≥ 0 is called a process in Hg, if
Now, we define translation operator in . .
We have
Denote Σ = {T(h)f(x, s) = f(x, s + h), ∀h ∈ R}, where T(·) is the positive invariant semigroups acting on Σ and satifying T(h)Σ ⊂ Σ, ∀h ≥ 0 and
Let be a constant, obviously
Let E be the Banach space; we use to denote the set of all bounded sets on E and consider a family of processes {Uf(t, τ)} with f ∈ Σ, the parameter f is called the symbols of the process family {Uf(t, τ)}, Σ is called the symbol space, and we assume that Σ is a complete metric space.
Definition 4. A family of processes {Uf(t, τ)}, f ∈ Σ is called uniformly bounded (w.r.t.f ∈ Σ), if any , both
Definition 5. A set B0 ⊂ E is said to be uniformly absorbing for the family of processes {Uf(t, τ)}, f ∈ Σ}, if for any τ ∈ R and each , there exists t0 = t0(τ, B) ≥ τ, such that for all t ≥ t0,
Definition 6. A set P ⊂ E is said uniformly atttracting set of {Uf(t, τ)}, f ∈ Σ}, if for any τ ∈ R, there is
A family of processes {Uf(t, τ)}, f ∈ Σ} is said to uniformly compact, if there exists a compacted uniformly absorbed set in {Uf(t, τ)}, f ∈ Σ}. A family of processes {Uf(t, τ)}, f ∈ Σ} is said to uniformly asymptotic compact, if there exists a compacted uniformly atttracting set in {Uf(t, τ)}, f ∈ Σ}.
Definition 7. A closed set is said to be the uniform attractor of the family of processes {Uf(t, τ)}, f ∈ Σ}, if
- (1)
is uniformly attractive
- (2)
is included in any uniformly attracting set of {Uf(t, τ)}, f ∈ Σ}, that is
Theorem 8. Let {fγ(θ): γ ∈ Γ} ⊂ C = C([−r, 0]; X) be equicontinuous and for any ∀θ ∈ [−r, 0], {fγ(θ): γ ∈ Γ} is quasicompact in X, then {fγ(θ): γ ∈ Γ} is relatively compact in C([−r, 0]; X).
Lemma 9 (Uniform Gronwall lemma). Let g, h, y be local integrable function on (t0, ∞), y′ is also local integrable on (t0, ∞), and y′(t) ≤ g(t)y(t) + h(t), ∀t ≥ t0., where r, a1, a2, a3 is positive constant. Then,
3. The Existence of Uniform Attractor for 2D g-Navier-Stokes Equations in Bounded Domain
The following we use to represent the translation compact function class.
Lemma 10. Let for any τ ≤ t, , assume that (I)-(IV) hold, then there exist bounded absorbing sets of process family {Uf(t, τ): t ≥ τ} in .
Proof. Since is bounded, then there exists , such that
For any , we define u(·) = u(·; τ, (u0, ϕ)), then taking the inner product of (9) with u(t), we have
Let , then
Integrating both sides from τ to t, then
Then,
Let s − τ = θ, then
Taking m ∈ (0, m0), such that m + σ + Cg − 2νλ1β < 1, then , so
Let t ≥ τ + h, ∀θ ∈ [−h, 0], then
Then,
Let , we will prove the existence of the uniformly absorbing bounded set in . First, we must prove the boundedness of .
Lemma 11. Given that , then there exist and constant , such that
Proof. Taking the inner product of (9) with u(t),
Then,
Integrating on both sides in [t, t + 1], we have
Then,
When , that is , we have
Lemma 12. For any τ ≤ t, . Assume that (I)-(IV) hold, then there exists uniformly bounded absorbing set of process family {Uf(t, τ): t ≥ τ} in .
Proof. Let , taking the inner product of (9) with Agu, we obtain
Then,
Applying Lemma 9,
Let u(·) = u(·; t − s, (u0, ϕ)), so . Then,
From [16], we have the following definition.
Definition 13. Let E be Banach space, if ∀ε > 0, there exists η > 0, such that
Then, is called normal function.
We will take the sets of all normal function classes in as . From [17], we can see that is the true subspace of . Therefore, the translation compact function must be a normal function.
Theorem 14. Suppose that nonlinear term h satisfies (I)-(III), f is translation compact function in , then process family {Uf(·, ·) | f ∈ Σ} exist uniform attractor , and .
Proof. Since B2 is bounded set in and uniform absorbed set of {Uf(·, ·) | f ∈ Σ}. For each τ ∈ R, we take a set
Let θ2 > θ1, and denote u(·) = u(·; τ, j(ϕ), f) as u(·), then
We estimate the items on the right end of the above formula, let θ1⟶θ2,
Since
When , and θ2 > θ1, then
Let
Then,
So,
And When θ1⟶θ2, ∀ϕ ∈ B2, f ∈ Σ, we have
Then, B3 is equicontinuous, and B3 is relatively compact in , so is compacted uniformly absorbing set of {Uf(·, ·) | f ∈ Σ} in , Let , since and the embedding mapping is continuous, so is compact in ; is also compacted uniformly absorbing set of {Uf(·, ·) | f ∈ Σ} in . Then, process family {Uf(·, ·) | f ∈ Σ} exists uniform attractor
Conflicts of Interest
This work does not have any conflicts of interest.
Acknowledgments
The author would like to thank the referees for the helpful suggestions. This work is supported by the Projects of Natural Science Basic Research Plan in Shaanxi Province of China (no. 2018JM1042).
Open Research
Data Availability
The (data type) data used to support the findings of this study are available from the corresponding author upon request.