Startseite Pullback and uniform exponential attractors for non-autonomous Oregonator systems
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Pullback and uniform exponential attractors for non-autonomous Oregonator systems

  • Na Liu EMAIL logo und Yang-Yang Yu
Veröffentlicht/Copyright: 15. Oktober 2024

Abstract

We consider the long-time global dynamics of non-autonomous Oregonator systems. This system is a coupled system of three reaction-diffusion equations, that arises from the Belousov-Zhabotinskii reaction. We first present some sufficient conditions for the existence of pullback and uniform exponential attractors for non-autonomous dynamical system. Then, we apply abstract results to prove the existence of a pullback exponential attractor for Oregonator systems affected by time-dependent forces and a uniform exponential attractor for Oregonator systems driven by quasi-periodic external forces.

MSC 2010: 37B55; 37C70; 37L25

1 Introduction

The Belousov-Zhabotinskii reaction is a family of chemical reactions, which exhibits oscillatory phenomena. During these reactions, transition-metal ions catalyze the oxidation of various, usually organic, reductants by bromic acid in the acidic water solution. The reaction can generate up to several thousand oscillatory cycles in a closed system, which was first discovered by Belousov and Zhabotinskii. The Belousov-Zhabotinskii reaction-type system has been the object of extensive study [17]. The original mathematical model consists of ten chemical reactions with seven intermediates. Later, Field and Noyes [1] proposed a modified model of three variable equations, called Oregonator systems.

For Oregonator systems, Pao [5] considered the asymptotic behavior of time-dependent solutions. Ruan and Pao provided some qualitative analysis (including the existence of a bounded global time-dependent solution, the stability and instability of the zero solution, and the existence and nonexistence of a positive steady-state solution) for Oregonator systems in [6]. Recently, You [8] proved the existence and properties of a global attractor for the solution semiflow of Oregonator systems by a rescaling and grouping estimation method. Moreover, the existence of an exponential attractor for this Oregonator semiflow is also obtained.

There is an extensive literature on global attractors, uniform attractors, pullback attractors for autonomous or non-autonomous dynamical systems. We do not attempt to give an exhaustive list of references. The general theory for autonomous dynamical system may be found in [916]. For non-autonomous dynamical system, we refer the reader to [1720]. However, these attractors present some defaults, especially for practical purposes. Indeed, they may attract the trajectories at a relatively slow speed. It is very difficult, if not impossible, to express the convergence rate in terms of the physical parameters of the model. Furthermore, these attractors may be sensitive to perturbations. In order to overcome these defaults, appropriate alternative is the exponential attractor introduced by Eden et al. [21], which contains the global attractor and attracts each bounded subset of the phase space at a uniform exponential rate. In recent years much attention was paid to pullback and uniform exponential attractors for non-autonomous dynamical system [2224]. It should be mentioned that in [25], Hammami et al. demonstrated how recent existence results for pullback exponential attractors can be applied to non-autonomous delay differential equations with time-varying delays. In addition, explicit estimates for the fractal dimension of the attractors have also been derived. It is also worth mentioning that in [26], an upper bound for the fractal dimension of uniform attractors in Banach spaces was obtained. The main technique used was based on a compact embedding of some auxiliary Banach spaces into the phase space and a corresponding smoothing effect between these spaces.

Now, let us return to the Oregonator systems. As far as we know, there have been very few results on pullback and uniform exponential attractors. This is in fact the chief motivation of the present study. Considering the importance of the class of systems, a natural question arises:

“Do the Oregonator systems have pullback and uniform exponential attractors?”

The main objective of this article is to give an affirmative answer. We will consider the existence of uniform exponential attractors for Oregonator systems affected by time-dependent forces

(1.1) u t = d 1 Δ u + a 1 u + b 1 v α u 2 β 1 u v + p 1 ( x , t ) , x Ω , t > τ , v t = d 2 Δ v b 2 v + c 2 w β 2 u v + p 2 ( x , t ) , x Ω , t > τ , w t = d 3 Δ w + a 3 u c 3 w + p 3 ( x , t ) , x Ω , t > τ

and the existence of pullback exponential attractors for Oregonator systems driven by quasi-periodic external forces

(1.2) u t = d 1 Δ u + a 1 u + b 1 v α u 2 β 1 u v + h 1 ( x ) g 1 ( σ ˜ ( t ) ) , x Ω , t > τ , v t = d 2 Δ v b 2 v + c 2 w β 2 u v + h 2 ( x ) g 2 ( σ ˜ ( t ) ) , x Ω , t > τ , w t = d 3 Δ w + a 3 u c 3 w + h 3 ( x ) g 3 ( σ ˜ ( t ) ) , x Ω , t > τ ,

where τ R and Ω is a bounded domain of R n ( n 3 ) with a smooth boundary Ω . The diffusive coefficients d 1 , d 2 , d 3 and the reaction rate parameters a 1 , a 3 , b 1 , b 2 , c 2 , c 3 , α , β 1 , β 2 are positive constants. The external forces p i L loc 2 ( R ; L 2 ( Ω ) ) , i = 1 , 2 , 3 , are translation bounded, i.e., p i L b 2 2 = p i L b 2 ( R ; L 2 ( Ω ) ) 2 = sup t R t t + 1 Ω p i 2 ( x , s ) d x d s . The functions h i L 2 ( Ω ) , i = 1 , 2 , 3 . Let T m be the m -dimensional torus

T m = { σ = ( σ 1 , σ 2 , , σ m ) : σ j [ π , π ] , j = 1 , 2 , , m }

with the identification

( σ 1 , , σ j 1 , π , σ j + 1 , , σ m ) ( σ 1 , , σ j 1 , π , σ j + 1 , , σ m ) , j = 1 , 2 , , m

and the topology and metric induced by the topology and metric on R m . Hence, the norm in T m is given by

σ T m = j = 1 m σ j 2 1 2 , σ = ( σ 1 , , σ m ) T m .

Let x = ( x 1 , x 2 , , x m ) R m be a fixed vector such that x 1 , x 2 , , x m are rationally independent, i.e., if there exist integers k 1 , , k m such that j = 1 m k j x j = 0 , then k j = 0 for j = 1 , 2 , , m . Define

σ ˜ ( t ) = ( x t + σ ) mod ( T m ) , σ T m .

Let g i : T m R ( i = 1 , 2 , 3 ) satisfy the following conditions

(1.3) g i ( 0 T m ) = 0 , g i ( σ ˜ 1 ( t ) ) g i ( σ ˜ 2 ( t ) ) l i σ 1 σ 2 T m , σ 1 , σ 2 T m .

With (1.1) and (1.2), we associate the homogeneous Dirichlet boundary conditions

(1.4) u ( x , t ) = 0 , v ( x , t ) = 0 , w ( x , t ) = 0 , x Ω , t > τ

and the initial conditions

(1.5) u ( x , τ ) = u τ ( x ) , v ( x , τ ) = v τ ( x ) , w ( x , τ ) = w τ ( x ) , x Ω .

We introduce some notations to be used throughout. Let H = [ L 2 ( Ω ) ] 3 and E = [ H 0 1 ( Ω ) ] 3 . The symbols and ( , ) denote the norm and the inner product in H or any component space L 2 ( Ω ) , respectively. We denote the duality product between H 0 1 ( Ω ) and H 1 ( Ω ) by , H 1 . By the Poincar e ́ inequality and (1.4), there is a constant k > 0 such that

(1.6) ϕ 2 k ϕ 2 , ϕ H 0 1 ( Ω ) .

We also define the linear operator on H by

(1.7) B = d 1 Δ 0 0 0 d 2 Δ 0 0 0 d 3 Δ , D ( B ) = [ H 2 ( Ω ) H 0 1 ( Ω ) ] 3 .

This article continues with the abstract theory of pullback and uniform exponential attractors for non-autonomous dynamical system in Section 2. The existence of a pullback exponential attractor for Oregonator systems affected by time-dependent forces and a uniform exponential attractor for Oregonator systems driven by quasi-periodic external forces are given in Sections 3 and 4, respectively.

2 Pullback and uniform exponential attractors

In this section, we recall several basic definitions on non-autonomous dynamical system that we will need in the sequel and introduce some theory of pullback and uniform exponential attractors for non-autonomous dynamical system.

First, we briefly state some basic concepts (see, e.g., [18,19] and references therein).

Let X be a Banach space with norm X . Denote by dist X ( , ) the Hausdorff semi-distance on X between B 1 and B 2 , i.e.,

dist X ( B 1 , B 2 ) = sup x B 1 inf y B 2 x y X .

Definition 2.1

A two-parameter family of mappings U ( t , τ ) is said to be a continuous process in X if

  1. U ( t , s ) U ( s , τ ) = U ( t , τ ) , t s τ , τ R ;

  2. U ( τ , τ ) = I d X , τ R ;

  3. U ( t , τ ) : X X is continuous for any t τ .

Definition 2.2

A family of subsets D = { D ( t ) } t R of X is said to be pullback absorbing with respect to the process U ( , ) if for every t R and all bounded set B X , there exists T = T ( t , B ) > 0 such that

U ( t , t τ ) B D ( t )

for all τ T .

Definition 2.3

Let D = { D ( t ) } t R be a family of subsets of X . A process U ( , ) is said to be pullback D -asymptotically compact in X if for any t R , any sequence τ n and x n D ( t τ n ) , the sequence { U ( t , t τ n ) x n } is relatively compact in X .

Definition 2.4

A family of compact subsets K = { K ( t ) } t R of X is said to be a pullback attractor if it satisfies the following:

  1. K is invariant, i.e., U ( t , τ ) K ( τ ) = K ( t ) for all t τ ;

  2. K is pullback attracting, i.e., for all bounded sets B X ,

    lim τ dist X ( U ( t , t τ ) B , K ( t ) ) = 0 .

Definition 2.5

A family of subsets { A ( t ) } t R of X is called a pullback exponential attractor for the continuous process U ( t , τ ) if

  1. A ( t ) ( t R ) is a compact subset of X and its fractal dimension is finite and uniformly bounded on t , i.e., sup t R dim f A ( t ) < ;

  2. it is positively invariant, i.e., U ( t , τ ) A ( τ ) A ( t ) for all t τ ;

  3. there exist an exponent α > 0 and two functions Q , T : R + R + such that for any bounded set B X ,

    dist X ( U ( t , τ ) B , A ( t ) ) Q ( B X ) e α ( t τ ) , τ R , τ + T ( B X ) t ,

    where B X = sup ω B ω X .

Below, we provide an existing result on the sufficient conditions for the existence of pullback exponential attractors. This can be seen in [24,27,28].

Proposition 2.1

Let U ( t , τ ) be a continuous process in X. Assume that there exists a family of bounded subsets { Y ( t ) } t R of X satisfying:

  1. the diameter Y ( t ) X of Y ( t ) is uniformly bounded, i.e., sup t R Y ( t ) X R < ;

  2. it is positively invariant, i.e., U ( t , τ ) Y ( τ ) Y ( t ) for all t τ ;

  3. it is absorbing in the sense that for any bounded set B X and τ R , there exists T B , τ 0 such that

    U ( t , τ ) B Y ( t ) , τ + T B , τ t < ;

  4. there exist t * > 0 and L = L ( t * ) > 0 such that for any τ R , t [ 0 , t * ] and φ τ , ψ τ Y ( τ ) ,

    U ( t + τ , τ ) φ τ U ( τ + t , τ ) ψ τ L φ τ ψ τ ;

  5. there exist a constant γ ( 0 , 1 2 ) and a N-dimensional subspace X N ( N N ) of X such that the bounded projection P N : X X N satisfies that for every τ R and φ τ , ψ τ Y ( τ ) ,

    ( I P N ) ( U ( τ + t * , τ ) φ τ U ( τ + t * , τ ) ψ τ ) γ φ τ ψ τ ,

    where γ , N depend on t * but not on τ ;

  6. for any given τ R ,

    lim t τ sup ψ τ Y ( τ ) U ( t , τ ) ψ τ ψ τ = 0 .

Then, { U ( t , τ ) } t τ R possesses a pullback exponential attractor { A ( t ) } t R satisfying that for any t R ,
  1. A ( t ) Y ( t ) ¯ is compact;

  2. dim f ( A ( t ) ) ln N θ ln a θ , where a θ = 2 ( γ + θ L ) with 0 < θ < 1 2 γ 2 L and N θ is the minimal number of closed balls of X with radius θ covering the closed unit ball of X N , B N ( 0 , 1 ) = { ψ X N : ψ 1 } ;

  3. U ( t , τ ) A ( τ ) A ( t ) for all t τ ;

  4. for any bounded set B X ,

    dist X ( U ( t , τ ) B , A ( t ) ) L Re T B , τ ln a θ t * a θ 2 e ln a θ t * ( t τ ) , < τ + T B , τ t < ;

  5. lim s t dist X ( A ( s ) , A ( t ) ) = 0 .

For s R , we define

T ( s ) σ = ( x t + σ ) mod ( T m ) , σ T m ,

where x is defined in Section 1, then { T ( s ) } s R is a translation group on T m with

σ ˜ ( t ) = T ( t ) σ , σ T m , T ( s ) T m = T m , s R .

For τ R , let { U σ ( t , τ ) } σ T m , t τ be a family of continuous processes on X , that is, for any σ T m , { U σ ( t , τ ) } ( t τ ) is a continuous process on X . Denote by the closed bounded subset of X such that

U σ ( t , τ ) , σ T m , t τ , τ R .

Definition 2.6

A set X is called a uniform exponential attractor for the family of processes { U σ ( t , τ ) } σ T m , t τ on X if

  1. is a compact set;

  2. has a finite fractal dimension, i.e., dim f < ;

  3. there exist two positive constants a 1 and a 2 such that

    sup σ T m dist X ( U σ ( t , τ ) , ) a 1 e a 2 ( t τ ) .

The following proposition gives the sufficient conditions for the existence of uniform exponential attractors. This can be seen in [29].

Proposition 2.2

Let { U σ ( t , τ ) } σ T m , t τ R be a family of continuous processes on X. Assume that

  1. { U σ ( t , τ ) } σ T m , t τ R and { T ( s ) } s R satisfy

    (2.1) U σ ( t + s , τ + s ) = U T ( s ) σ ( t , τ ) , s R , t τ , τ R ;

  2. there exists a bounded set 0 X such that for any σ T m , τ R ,

    U σ ( t , τ ) 0 0 , t τ ;

  3. there exist t * > 0 , L = L ( t * ) > 0 and a N-dimensional subspace X N of X such that for any ψ 1 , ψ 2 0 , σ 1 , σ 2 T m ,

    U σ 1 ( t , 0 ) ψ 1 U σ 2 ( t , 0 ) ψ 2 L ( ψ 1 ψ 2 2 + σ 1 σ 2 T m 2 ) 1 2 , t [ 0 , t * ] , ( I P N ) U σ 1 ( t * , 0 ) ψ 1 U σ 2 ( t * , 0 ) ψ 2 1 8 2 ( ψ 1 ψ 2 2 + σ 1 σ 2 T m 2 ) 1 2 ,

where P N : X X N is a orthogonal projection operator. Then, { U σ ( t , τ ) } σ T m , t τ R possesses a uniform exponential attractor on 0 ¯ with dim f ( ) K 0 ( m + N ) ln L 2 + 1 , where K 0 is a positive constant.

3 Existence of pullback exponential attractor for system (1.1)

The main goal of the present section is to prove the existence of a pullback exponential attractor for Oregonator systems affected by time-dependent forces.

We consider the abstract equivalent form of (1.1) as

(3.1) ψ t = B ψ + f ( ψ ) + p ( x , t ) , x Ω , t τ , ψ τ ( x ) = col ( u τ ( x ) , v τ ( x ) , w τ ( x ) ) , x Ω ,

where

f ( ψ ) = a 1 u + b 1 v α u 2 β 1 u v b 2 v + c 2 w β 2 u v a 3 u c 3 w , ψ = col ( u , v , w ) E

and p ( x , t ) = col ( p 1 ( x , t ) , p 2 ( x , t ) , p 3 ( x , t ) ) . Moreover, it is easy to verify that the nonlinearity f is locally Lipschitz continuous from E to H .

The following well-posedness result follows from [8, Lemma 3.1].

Lemma 3.1

Let p i L loc 2 ( R ; L 2 ( Ω ) ) , i = 1 , 2 , 3 . Then, for any ( u τ , v τ , w τ ) H and T τ , there exists a unique weak solution of (3.1) which satisfies

( u , v , w ) C ( [ τ , T ] ; H ) L 2 ( τ , T ; E )

and for any θ i H 0 1 ( Ω ) , i = 1 , 2 , 3 and a.s. t τ ,

u ( t ) , θ 1 H 1 + d 1 ( u ( t ) , θ 1 ) = ( a 1 u ( t ) + b 1 v ( t ) α u 2 ( t ) β 1 u ( t ) v ( t ) , θ 1 ) + ( p 1 ( t ) , θ 1 ) , v ( t ) , θ 2 H 1 + d 2 ( v ( t ) , θ 2 ) = ( b 2 v ( t ) + c 2 w ( t ) β 2 u ( t ) v ( t ) , θ 2 ) + ( p 2 ( t ) , θ 2 ) , w ( t ) , θ 3 H 1 + d 3 ( w ( t ) , θ 3 ) = ( a 3 u ( t ) c 3 w ( t ) , θ 3 ) + ( p 3 ( t ) , θ 3 ) .

Moreover, the weak solution continuously depends on the initial data in H.

Define the solution operator U ( t , τ ) on H by

U ( t , τ ) ( u τ , v τ , w τ ) = Φ ( t , τ ; Φ τ ) ,

where Φ ( t , τ ; Φ τ ) = ( u ( t , τ ; u τ ) , v ( t , τ ; v τ ) , w ( t , τ ; w τ ) ) . Then U ( t , τ ) forms a continuous process on H .

Next, we consider the existence of a uniformly bounded absorbing set of the continuous process U ( t , τ ) . Our main result states as

Theorem 3.1

There exists a uniformly bounded closed absorbing set B 0 = B ( 0 , r 0 ) = { ϕ H : ϕ r 0 } ( r 0 is independent of t and τ ) such that for any τ R and any bounded set B X , there is a function T : R + R + such that U ( t + τ , τ ) B B 0 for all t T ( B ) , where B = sup ϕ B ϕ .

Proof

Let w ˜ = c 2 b 2 w . Clearly, system (1.1) becomes

u t = d 1 Δ u + a 1 u + b 1 v α u 2 β 1 u v + p 1 ( x , t ) , ( 3.2 ) v t = d 2 Δ v b 2 v + b 2 w ˜ β 2 u v + p 2 ( x , t ) , ( 3.3 ) b 2 c 2 w ˜ t = d 3 b 2 c 2 Δ w ˜ + a 3 u c 3 b 2 c 2 w ˜ + p 3 ( x , t ) . ( 3.4 )

Taking the inner-products ( ( 3.2 ) , u ) , ( ( 3.3 ) , v ) , ( 3.4 ) , c 2 w ˜ c 3 and summing them up, by Young’s inequality, we obtain

1 2 d d t u 2 + v 2 + b 2 c 2 w ˜ 2 + d 1 u 2 + d 2 v 2 + b 2 d 3 c 3 w ˜ 2 = Ω a 1 u 2 + b 1 u v + a 3 c 2 c 3 u w ˜ d x Ω ( α u 3 + β 1 u 2 v + β 2 u v 2 ) d x b 2 Ω ( v 2 + w ˜ 2 ) d x + b 2 Ω w ˜ v d x + Ω p 1 u + p 2 v + c 2 c 3 p 3 w ˜ d x Ω a 1 u 2 + b 1 2 b 2 u 2 + b 2 4 v 2 + a 3 2 c 2 2 c 3 2 b 2 u 2 + b 2 4 w ˜ 2 d x Ω α u 3 d x b 2 Ω ( v 2 + w ˜ 2 ) d x + b 2 Ω 1 2 w ˜ 2 + 1 2 v 2 d x + Ω 1 2 u 2 + 1 2 p 1 2 + b 2 4 v 2 + 1 b 2 p 2 2 + b 2 4 w ˜ 2 + c 2 2 c 3 2 b 2 p 3 2 d x .

Let M 1 = a 1 + b 1 2 b 2 + a 3 2 c 2 2 c 3 2 b 2 + 1 2 and M 2 = max { 1 2 , 1 b 2 , c 2 2 c 3 2 b 2 } . We obtain

1 2 d d t u 2 + v 2 + b 2 c 2 w ˜ 2 + d 1 u 2 + d 2 v 2 + b 2 d 3 c 3 w ˜ 2 M 1 u 2 α Ω u 3 d x + M 2 ( p 1 ( t ) 2 + p 2 ( t ) 2 + p 3 ( t ) 2 ) α 3 Ω u 3 d x + M 1 3 3 α 2 Ω + M 2 ( p 1 ( t ) 2 + p 2 ( t ) 2 + p 3 ( t ) 2 ) .

Therefore, by (1.6) and letting

d 0 = min { d 1 , d 2 , d 3 } , M 3 = 2 M 1 3 3 α 2 Ω ,

one has

(3.5) d d t u 2 + v 2 + b 2 c 3 w ˜ 2 + 2 k d 0 u 2 + v 2 + b 2 c 3 w ˜ 2 M 3 + 2 M 2 ( p 1 ( t ) 2 + p 2 ( t ) 2 + p 3 ( t ) 2 ) .

Integrating (3.5) from τ to t + τ gives

u ( t + τ ) 2 + v ( t + τ ) 2 + b 2 c 2 w ˜ ( t + τ ) 2 e 2 k d 0 t ( u ( τ ) 2 + v ( τ ) 2 + b 2 c 2 w ˜ ( τ ) 2 ) + τ t + τ e 2 k d 0 ( t + τ s ) ( M 3 + 2 M 2 ( p 1 ( s ) 2 + p 2 ( s ) 2 + p 3 ( s ) 2 ) ) d s e 2 k d 0 t ( u ( τ ) 2 + v ( τ ) 2 + b 2 c 2 w ˜ ( τ ) 2 ) + i = 0 + t + τ i 1 t + τ i e 2 k d 0 ( t + τ s ) ( M 3 + 2 M 2 ( p 1 ( s ) 2 + p 2 ( s ) 2 + p 3 ( s ) 2 ) ) d s e 2 k d 0 t ( u ( τ ) 2 + v ( τ ) 2 + b 2 c 2 w ˜ ( τ ) 2 ) + i = 0 + e 2 k d 0 i 2 k d 0 ( M 3 + 2 M 2 ( p 1 L b 2 2 + p 2 L b 2 2 + p 3 L b 2 2 ) ) e 2 k d 0 t ( u ( τ ) 2 + v ( τ ) 2 + b 2 c 2 w ˜ ( τ ) 2 ) + e 2 k d 0 2 k d 0 ( e 2 k d 0 1 ) ( M 3 + 2 M 2 ( p 1 L b 2 2 + p 2 L b 2 2 + p 3 L b 2 2 ) ) .

Let M 4 = min 1 , c 2 2 b 2 c 3 and M 5 = max 1 , c 2 2 b 2 c 3 . We then obtain

u ( t + τ ) 2 + v ( t + τ ) 2 + w ( t + τ ) 2 M 5 M 4 e 2 k d 0 t ( u ( τ ) 2 + v ( τ ) 2 + w ( τ ) 2 ) + e 2 k d 0 2 k d 0 M 4 ( e 2 k d 0 1 ) ( M 3 + 2 M 2 ( p 1 L b 2 2 + p 2 L b 2 2 + p 3 L b 2 2 ) ) .

Hence, for any τ R and any bounded set B H ,

Φ ( t + τ , τ ; Φ τ ) 2 M 5 M 4 e 2 k d 0 t sup Φ τ B Φ τ 2 + 1 2 r 0 2 ,

where r 0 2 = e 2 k d 0 k d 0 M 4 ( e 2 k d 0 1 ) ( M 3 + 2 M 2 ( p 1 L b 2 2 + p 2 L b 2 2 + p 3 L b 2 2 ) ) is independent of t and τ . Since

lim t + e 2 k d 0 t sup Φ τ B Φ τ 2 = 0

uniformly for any τ R and any bounded set B H , there exists a function T ( B ) = 1 2 k d 0 ln ( 2 M 5 B 2 r 0 2 M 4 ) such that for any τ R and any bounded subset B H , U ( t + τ , τ ) B B 0 for all t T ( B ) . Hence, B 0 = { ϕ H : ϕ r 0 } is a uniformly bounded closed absorbing set of the continuous process U ( t , τ ) .□

Theorem 3.2

There exists a closed ball B 1 = { ϕ E : ϕ E r 1 } ( r 1 is independent of t and τ ) such that for any τ R , U ( t + τ , τ ) B 0 B 1 for all t T ( B 0 ) + 1 .

Proof

Taking the inner-product ((3.2), Δ u ), ((3.3), Δ v ), ((3.4), c 2 c 3 Δ w ˜ ) and summing them up, by Young’s inequality, we obtain

1 2 d d t u 2 + v 2 + b 2 c 3 w ˜ 2 + d 1 Δ u 2 + d 2 Δ v 2 + d 3 b 2 c 3 Δ w ˜ 2 Ω ( a 1 u + b 1 v + β 1 u v ) ( Δ u ) d x 2 α Ω u u 2 d x + Ω p 1 ( Δ u ) d x b 2 Ω ( v 2 w ˜ v ) d x + β 2 Ω u v ( Δ v ) d x + Ω p 2 ( Δ v ) d x c 2 a 3 c 3 Ω u Δ w ˜ d x b 2 Ω w ˜ 2 d x + c 2 c 3 Ω p 3 ( Δ w ˜ ) d x d 1 4 Δ u 2 + a 1 2 d 1 u 2 + d 1 4 Δ u 2 + b 1 2 d 1 v 2 + d 1 4 Δ u 2 + β 1 2 d 1 Ω u 2 v 2 d x + d 1 8 Δ u 2 + 2 d 1 p 1 ( t ) 2 b 2 Ω ( v 2 w ˜ v ) d x + d 2 4 Δ v 2 + β 2 2 d 2 Ω u 2 v 2 d x + d 2 4 Δ v 2 + 1 d 2 p 2 ( t ) 2 + c 2 a 3 c 3 b 2 d 3 4 c 2 a 3 Δ w ˜ 2 + c 2 a 3 b 2 d 3 u 2 + c 2 c 3 b 2 d 3 4 c 2 Δ w ˜ 2 + c 2 b 2 d 3 p 3 ( t ) 2 b 2 Ω w ˜ 2 d x = 7 d 1 8 Δ u 2 + 1 d 1 ( a 1 2 u 2 + b 1 2 v 2 ) b 2 Ω ( v 2 w ˜ v + w ˜ 2 ) d x + d 2 2 Δ v 2 + β 1 2 d 1 + β 2 2 d 2 Ω u 2 v 2 d x + b 2 d 3 2 c 3 Δ w ˜ 2 + c 2 2 a 3 2 b 2 d 3 c 3 u 2 + 1 d 1 p 1 ( t ) 2 + 1 d 2 p 2 ( t ) 2 + c 2 2 c 3 b 2 d 3 p 3 ( t ) 2 .

Note that

w ˜ 2 = c 2 b 2 2 w 2 , Δ w ˜ 2 = c 2 b 2 2 Δ w 2 , b 2 Ω ( v 2 w ˜ v + w ˜ 2 ) d x 0 .

Let

M 6 = min d 1 8 , d 2 2 , d 3 2 , M 7 = max a 1 2 d 1 + c 2 2 a 3 2 b 2 d 3 c 3 , b 1 2 d 1 , M 8 = max 1 d 1 , 1 d 2 , c 2 2 c 3 d 3 b 2 .

Then, we have

(3.6) d d t u 2 + v 2 + c 2 2 b 2 c 3 w 2 + 2 k M 6 Δ u 2 + Δ v 2 + c 2 2 b 2 c 3 Δ w 2 2 M 7 ( u 2 + v 2 ) + β 1 2 d 1 + β 2 2 d 2 ( u L 4 4 + v L 4 4 ) + 2 M 8 ( p 1 ( t ) 2 + p 2 ( t ) 2 + p 3 ( t ) 2 ) .

From Theorem 3.1, it follows that for any τ R and Φ τ B 0 ,

u ( t + τ ) 2 + v ( t + τ ) 2 r 0 2 , t T ( B 0 ) .

Note also that we have taken ϕ as the norm of H 0 1 ( Ω ) and there exists ν > 0 associated with the Sobolev imbedding inequality

(3.7) ϕ L 4 ν ϕ , ϕ H 0 1 ( Ω ) .

Then, for t T ( B 0 ) + τ , one has

d d t u 2 + v 2 + c 2 2 b 2 c 3 w 2 2 M 7 r 0 2 + β 1 2 d 1 + β 2 2 d 2 ν 4 ( u 4 + v 4 ) + 2 M 8 ( p 1 ( t ) 2 + p 2 ( t ) 2 + p 3 ( t ) 2 ) 2 M 7 r 0 2 + β 1 2 d 1 + β 2 2 d 2 ν 4 ( u 4 + v 4 + c 2 4 b 2 2 c 3 2 w 4 ) + 2 M 8 ( p 1 ( t ) 2 + p 2 ( t ) 2 + p 3 ( t ) 2 ) ν 4 β 1 2 d 1 + β 2 2 d 2 u 2 + v 2 + c 2 2 b 2 c 3 w 2 u 2 + v 2 + c 2 2 b 2 c 3 w 2 + 2 M 7 r 0 2 + 2 M 8 ( p 1 ( t ) 2 + p 2 ( t ) 2 + p 3 ( t ) 2 ) ,

which can be written as

(3.8) d d t y ρ y + h ,

where

y ( t ) = u 2 + v 2 + c 2 2 b 2 c 3 w 2 , ρ ( t ) = ν 4 β 1 2 d 1 + β 2 2 d 2 y ( t ) , h ( t ) = 2 M 7 r 0 2 + + 2 M 8 ( p 1 L b 2 2 + p 2 L b 2 2 + p 3 L b 2 2 ) .

From (3.5), it follows that

(3.9) t t + 1 y ( s ) d s M 3 + 2 M 2 ( p 1 L b 2 2 + p 2 L b 2 2 + p 3 L b 2 2 ) + M 5 r 0 2 2 k d 0 = M 9 .

Then, we can apply the uniform Gronwall inequality to (3.8) and use (3.9) to obtain

u ( t + τ ) 2 + v ( t + τ ) 2 + w ( t + τ ) 2 ( M 9 + 2 M 7 r 0 2 + 2 M 8 ( p 1 L b 2 2 + p 2 L b 2 2 + p 3 L b 2 2 ) ) e M 9 ν 4 β 1 2 d 1 + β 2 2 d 2 M 4 r 1 2

for t T ( B 0 ) + 1 . Hence, for any τ R , U ( t + τ , τ ) B 0 B 1 for all t T ( B 0 ) + 1 .□

Thanks to Theorems 3.1, 3.2, and [19, VIII. Theorem 1.2], we have the following result.

Theorem 3.3

The continuous process U ( t , τ ) has a pullback attractor K = { K ( t ) } t R satisfying that

  1. K ( t ) is compact for all t R ;

  2. K is invariant, i.e., U ( t , τ ) K ( τ ) = K ( t ) for all t τ ;

  3. K is pullback attracting, i.e., for any bounded set B H and t R ,

    lim τ dist H ( U ( t , τ ) B , K ( t ) ) = 0 .

Let A = Δ , with domain D ( A ) = H 2 ( Ω ) H 0 1 ( Ω ) , a linear self-adjoint positive unbounded operator with compact inverse on L 2 ( Ω ) . The operator A possesses the complete orthonormal system of eigenvectors { e j } j = 1 in L 2 ( Ω ) , which corresponds to eigenvalues λ j such that

(3.10) A e j = λ j e j , 0 λ 1 λ 2 λ 3 λ j , λ j as j .

Write, for N N ,

L N 2 ( Ω ) = span { e j : 1 j N } , L N 2 ( Ω ) = span ¯ { e j : j N + 1 } .

Then, [ L N 2 ( Ω ) ] 3 is a 3 N -dimensional subspace of H . Denote by P N the orthogonal projection from H to [ L N 2 ( Ω ) ] 3 . Let Q N = I P N . For ϕ E and Q N ϕ = ϕ N q [ L N 2 ( Ω ) ] 3 ,

(3.11) λ N + 1 ϕ N q 2 ϕ N q 2 .

For any t R , let us define

Y ( t ) = s 2 T ( B 0 ) + 1 U ( t , t s ) B 0 .

Thanks to Theorems 3.1, 3.2, and the continuity of U ( t , τ ) , we obtain

(3.12) U ( t , s ) Y ( s ) Y ( t ) B 0 B 1 E , t s , U ( t , s ) Y ( s ) ¯ Y ( t ) ¯ H , t s .

Lemma 3.2

The continuous process U ( t , τ ) has the following properties.

  1. There exists a continuous function L : R + R + such that for any τ R and t 0 ,

    U ( t + τ , τ ) φ τ U ( t + τ , τ ) ψ τ L ( t ) φ τ ψ τ , φ τ , ψ τ Y ( τ ) .

  2. There exist constants T * > 0 , ε ( 0 , 1 2 ) , and a 3 N 0 -dimensional subspace X N 0 ( N 0 N ) of X such that the bounded projection P N 0 : H [ L N 0 2 ( Ω ) ] 3 satisfies that for every τ R and φ τ , ψ τ Y ( τ ) ,

    ( I P N 0 ) ( U ( τ + T * , τ ) φ τ U ( τ + T * , τ ) ψ τ ) ε φ τ ψ τ ,

    where ε , N 0 depend on T * but not on τ .

  3. For every fixed τ R ,

    lim t τ sup ψ τ Y ( τ ) U ( t , τ ) ψ τ ψ τ = 0 .

Proof

For any τ R and φ τ , ψ τ Y ( τ ) , we define

φ ( t ) = U ( t , τ ) φ τ = ( u 1 ( t ) , v 1 ( t ) , w 1 ( t ) ) , ψ ( t ) = U ( t , τ ) ψ τ = ( u 2 ( t ) , v 2 ( t ) , w 2 ( t ) ) .

From (3.12), it follows that

(3.13) φ ( t ) r 0 , ψ ( t ) r 0 , φ ( t ) r 1 , ψ ( t ) r 1 , t τ .

Let ϕ ( t ) = φ ( t ) ψ ( t ) = ( ξ ( t ) , η ( t ) , ζ ( t ) ) . Then

φ , ψ , ϕ C ( [ τ , ) ; H ) L l o c 2 ( ( τ , ) ; E )

and ϕ satisfies that for any θ i H 0 1 ( Ω ) , i = 1 , 2 , 3 and a.s. t τ ,

(3.14) ξ , θ 1 H 1 + d 1 ( ξ , θ 1 ) = ( a 1 ξ + b 1 η α ( u 1 2 u 2 2 ) β 1 ( u 1 v 1 u 2 v 2 ) , θ 1 ) , η , θ 2 H 1 + d 2 ( η , θ 2 ) = ( b 2 η + c 2 ζ β 2 ( u 1 v 1 u 2 v 2 ) , θ 2 ) , ζ , θ 3 H 1 + d 3 ( ζ , θ 3 ) = ( a 3 ξ c 3 ζ , θ 3 ) .

Taking θ 1 = ξ , θ 2 = η , θ 3 = ζ , we have

1 2 d d t ϕ 2 + d 1 ξ 2 + d 2 η 2 + d 3 ζ 2 = a 1 ξ 2 + b 2 η 2 c 3 ζ 2 + Ω ( b 1 η ξ + c 2 ζ η + a 3 ξ ζ ) d x α Ω ( u 1 2 u 2 2 ) ξ d x + β 1 Ω ( u 1 v 1 u 2 v 2 ) ξ d x β 2 Ω ( u 1 v 1 u 2 v 2 ) η d x .

By the Hölder inequality, one has

(3.15) Ω ( b 1 η ξ + c 2 ζ η + a 3 ξ ζ ) d x b 1 + c 2 2 η 2 + b 1 + a 3 2 ξ 2 + a 3 + c 2 2 ζ 2

and

(3.16) α Ω ( u 1 2 u 2 2 ) ξ d x = α Ω ( u 1 + u 2 ) ξ 2 d x 0 .

From (3.7) and (3.13), it follows that

(3.17) β 1 Ω ( u 1 v 1 u 2 v 2 ) ξ d x = β 1 Ω ( u 1 v 1 u 2 v 1 + u 2 v 1 u 2 v 2 ) ξ d x = β 1 Ω ( ξ 2 v 1 + u 2 η ξ ) d x = Ω d 1 4 ν 4 r 1 2 ξ 2 v 1 2 + β 1 2 ν 4 r 1 2 d 1 ξ 2 + d 1 4 ν 4 r 1 2 ξ 2 u 2 2 + β 1 2 ν 4 r 1 2 d 1 η 2 d x d 1 4 ν 4 r 1 2 ξ L 4 2 ( v 1 L 4 2 + u 2 L 4 2 ) + β 1 2 ν 4 r 1 2 d 1 ( ξ 2 + η 2 ) d 1 4 r 1 2 ξ 2 ( v 1 2 + u 2 2 ) + β 1 2 ν 4 r 1 2 d 1 ( ξ 2 + η 2 ) d 1 2 ξ 2 + β 1 2 ν 4 r 1 2 d 1 ( ξ 2 + η 2 )

and

(3.18) β 2 Ω ( u 1 v 1 u 2 v 2 ) η d x β 2 Ω ξ v 1 η d x Ω d 1 4 ν 4 r 1 2 ξ 2 v 1 2 + β 2 2 ν 4 r 1 2 d 1 η 2 d x d 1 4 ν 4 r 1 2 ξ L 4 2 v 1 L 4 2 + β 2 2 ν 4 r 1 2 d 1 η 2 d 1 4 r 1 2 ξ 2 v 1 2 + β 2 2 ν 4 r 1 2 d 1 η 2 d 1 4 ξ 2 + β 2 2 ν 4 r 1 2 d 1 η 2 .

Let

M 8 = max a 1 + b 1 + a 3 2 + β 1 2 ν 4 r 1 2 d 1 , b 1 + c 2 2 + b 2 + ( β 1 2 + β 2 2 ) ν 4 r 1 2 d 1 , a 3 + c 2 2 .

We then obtain

1 2 d d t ϕ 2 M 8 ϕ 2 .

An application of the Gronwall inequality yields that

(3.19) ϕ ( t + τ ) 2 e M 8 t ϕ τ 2 , t 0 .

This implies that

φ ( t + τ ) ψ ( t + τ ) L ( t ) φ τ ψ τ , t 0 ,

where L ( t ) = e M 8 t 2 . We thus obtain conclusion (1).

Let θ 1 = ξ N q , θ 2 = η N q , θ 3 = ζ N q . From (3.14), it follows that

1 2 d d t ϕ N q 2 + d 1 ξ N q 2 + d 2 η N q 2 + d 3 ζ N q 2 = a 1 ξ N q 2 + b 2 η N q 2 c 3 ζ N q 2 + Ω ( b 1 η ξ N q + c 2 ζ η N q + a 3 ξ ζ N q ) d x α Ω ( u 1 2 u 2 2 ) ξ N q d x + β 1 Ω ( u 1 v 1 u 2 v 2 ) ξ N q d x β 2 Ω ( u 1 v 1 u 2 v 2 ) η N q d x .

Applying the Hölder inequality, we obtain

(3.20) Ω ( b 1 η ξ N q + c 2 ζ η N q + a 3 ξ ζ N q ) d x b 1 + c 2 2 η N q 2 + b 1 + a 3 2 ξ N q 2 + a 3 + c 2 2 ζ N q 2

and

(3.21) α Ω ( u 1 2 u 2 2 ) ξ N q d x 0 .

Using (3.7), (3.13), and the Hölder inequality, one has

(3.22) β 1 Ω ( u 1 v 1 u 2 v 2 ) ξ N q d x = β 1 Ω ( ξ v 1 ξ N q + u 2 η ξ N q ) d x β 1 ξ v 1 L 4 ξ N q L 4 + β 1 u 2 L 4 η ξ N q L 4 β 1 ν 2 ξ v 1 ξ N q + β 1 ν 2 u 2 η ξ N q d 1 2 ξ N q 2 + β 1 2 ν 4 r 1 2 d 1 ( ξ 2 + η 2 )

and

(3.23) β 2 Ω ( u 1 v 1 u 2 v 2 ) η N q d x = β 2 Ω ( ξ v 1 η N q + u 2 η η N q ) d x β 2 Ω ξ v 1 η N q d x β 2 ξ v 1 L 4 η N q L 4 β 2 ν 2 ξ v 1 η N q d 2 2 η N q 2 + β 2 2 ν 4 r 1 2 2 d 2 ξ 2 .

Put

M 9 = min { d 1 , d 2 , 2 d 3 } , M 10 = 2 max a 1 + b 1 + a 3 2 + β 1 2 ν 4 r 1 2 d 1 + β 2 2 ν 4 r 1 2 2 d 2 , b 1 + c 2 2 + b 2 + β 1 2 ν 4 r 1 2 d 1 , a 3 + c 2 2 .

From (3.11) and (3.19), it follows that

d d t ϕ N q 2 + M 9 λ N + 1 ϕ N q 2 M 10 e M 8 ( t τ ) ϕ τ 2 .

This yields, using the Gronwall inequality, that

ϕ N q ( t + τ ) 2 e M 9 λ N + 1 t + M 10 t t + τ e M 9 λ N + 1 ( t + τ s ) + M 8 ( s τ ) d s ϕ τ 2 e M 9 λ N + 1 t + M 10 e M 8 t M 9 λ N + 1 + M 8 ϕ τ 2 .

We obtain, due to (3.10), that there exist T * > 0 and

N 0 = min N N : e M 9 λ N + 1 T * + M 10 e M 8 T * M 9 λ N + 1 + M 8 < 1 4

such that

ε = e M 9 λ N 0 + 1 T * + M 10 e M 8 T * M 9 λ N 0 + 1 + M 8 < 1 2 .

This implies that conclusion (2) holds.

Let τ R and ψ τ Y τ . Put

M 11 = 2 M 7 r 0 2 + β 1 2 d 1 + β 2 2 d 2 r 1 4 .

From (3.6), we have

d d t u 2 + v 2 + c 2 2 b 2 c 3 w 2 + 2 k M 6 Δ u 2 + Δ v 2 + c 2 2 b 2 c 3 Δ w 2 M 11 + 2 M 8 ( p 1 ( t ) 2 + p 2 ( t ) 2 + p 3 ( t ) 2 ) .

Then, integrating the above inequality on [ τ , t ] ( t [ τ , τ + 1 ] ) enables us to find

(3.24) 2 k M 6 τ t Δ u ( s ) 2 + Δ v ( s ) 2 + c 2 2 b 2 c 3 Δ w ( s ) 2 d s M 11 + u ( τ ) 2 + v ( τ ) 2 + c 2 2 b 2 c 3 w ( τ ) 2 + 2 M 8 τ t ( p 1 ( s ) 2 + p 2 ( s ) 2 + p 3 ( s ) 2 ) d s M 11 + 1 + c 2 2 b 2 c 3 r 1 2 + 2 M 8 ( p 1 L b 2 2 + p 2 L b 2 2 + p 3 L b 2 2 ) .

Integrating (3.1) on [ τ , t ] ( t [ τ , τ + 1 ] ) , we obtain

ψ ( t ) ψ ( τ ) = τ t ( B ψ ( s ) + f ( ψ ( s ) ) + p ( x , s ) ) d s .

Let

M 12 = M 11 + 1 + c 2 2 b 2 c 3 r 1 2 + 2 M 8 ( p 1 L b 2 2 + p 2 L b 2 2 + p 3 L b 2 2 ) , M 13 = M 12 2 k M 6 min 1 , c 2 2 b 2 c 3 , M 14 = ( d 1 + d 2 + d 3 ) M 13 1 2 .

Due to (3.24), one can obtain

ψ ( t ) ψ ( τ ) τ t B ψ ( s ) d s + τ t f ( ψ ( s ) ) + p ( x , s ) d s τ t ( d 1 Δ u + d 2 Δ v + d 3 Δ w ) d s + τ t f ( ψ ( s ) ) + p ( x , s ) d s ( t τ ) 1 2 τ t d 1 2 Δ u ( s ) 2 d s 1 2 + ( t τ ) 1 2 τ t d 2 2 Δ v ( s ) 2 d s 1 2 + ( t τ ) 1 2 τ t d 3 2 Δ w ( s ) 2 d s 1 2 + τ t f ( ψ ( s ) ) + p ( x , s ) d s M 14 ( t τ ) 1 2 + τ t f ( ψ ( s ) ) + p ( x , s ) d s .

Then, for any given τ R ,

lim t τ sup ψ τ Y ( τ ) U ( t , τ ) ψ τ ψ τ = 0 .

Thanks to Lemmas 3.1, 3.2, Proposition 2.1, and Theorems 3.13.3, we have the following result.

Theorem 3.4

The continuous process U ( t , τ ) has a pullback exponential attractor { A ( t ) } t R satisfying that

  1. for any τ R , K ( τ ) A ( τ ) Y ( τ ) ¯ B 0 ;

  2. sup τ R dim f ( A ( τ ) ) ln N 0 θ * ln a θ * , where a θ * = 2 ( ε + θ L ( T * ) ) with 0 < θ < 1 2 ε 4 L ( T * ) and N 0 θ * = ( 2 N 0 2 θ + 1 ) 2 N 0 is the minimal number of closed balls of H with radius θ covering the closed unit ball of [ L N 0 2 ( Ω ) ] 3 , B N 0 ( 0 , 1 ) = { ψ [ L N 0 2 ( Ω ) ] 3 : ψ 1 } centered at origin 0;

  3. for every bounded subset B of H,

    dist H ( U ( τ , τ t ) B , A ( τ ) ) 2 L ( T * ) r 0 ( a θ * ) 2 e l n a θ * T * ( t T ( B ) T ( B 0 ) 1 )

    for all t > T ( B ) + T ( B 0 ) + 1 ;

  4. lim s t dist H ( A ( s ) , A ( t ) ) = 0 .

4 Existence of the uniform exponential attractor for system (1.2)

This section is concerned with the existence of a uniform exponential attractor for Oregonator systems driven by quasi-periodic external forces.

We consider the abstract equivalent form of (1.2) as

(4.1) ψ t = B ψ + f ( ψ ) + g ( x , σ , t ) , x Ω , t τ , ψ τ ( x ) = col ( u τ ( x ) , v τ ( x ) , w τ ( x ) ) , x Ω ,

where g ( x , σ , t ) = col ( h 1 ( x ) g 1 ( σ ˜ ( t ) ) , h 2 ( x ) g 2 ( σ ˜ ( t ) ) , h 3 ( x ) g 3 ( σ ˜ ( t ) ) ) and ψ , f ( ψ ) is given in Section 3.

Lemma 4.1

For σ T m , τ R and ψ τ = ( u τ , v τ , w τ ) H , there exists a unique global weak solution ψ = ( u , v , w ) C ( [ τ , ) ; H ) L 2 ( τ , ; E ) of (4.1). Moreover, it generates a family of continuous processes { U σ ( t , τ ) } σ T m , t τ R on H by

U σ ( t , τ ) : ψ τ ψ ( t ) , σ T m , t τ , τ R ,

which satisfies the translation identity (2.1).

Proof

By conducting a priori estimates on the Galerkin approximate solutions of the initial value problem of (4.1) and by the Lions-Magenes type of weak and weak * convergence argument, we obtain immediately

ψ C ( [ τ , T max ) ; H ) L 2 ( τ , T max ; E ) .

We next show that T max = .

Let w ˜ = c 2 b 2 w . System (1.2) becomes

u t = d 1 Δ u + a 1 u + b 1 v α u 2 β 1 u v + h 1 ( x ) g 1 ( σ ˜ ( t ) ) , ( 4.2 ) v t = d 2 Δ v b 2 v + b 2 w ˜ β 2 u v + h 2 ( x ) g 2 ( σ ˜ ( t ) ) , ( 4.3 ) b 2 c 2 w ˜ t = d 3 b 2 c 2 Δ w ˜ + a 3 u c 3 b 2 c 2 w ˜ + h 3 ( x ) g 3 ( σ ˜ ( t ) ) . ( 4.4 )

Taking the inner-products ( ( 4.2 ) , u ) , ( ( 4.3 ) , v ) , ( 4.4 ) , c 2 w ˜ c 3 and summing them up, by Young’s inequality we obtain

1 2 d d t u 2 + v 2 + b 2 c 2 w ˜ 2 + d 1 u 2 + d 2 v 2 + b 2 d 3 c 3 w ˜ 2 = Ω a 1 u 2 + b 1 u v + a 3 c 2 c 3 u w ˜ d x Ω ( α u 3 + β 1 u 2 v + β 2 u v 2 ) d x b 2 Ω ( v 2 + w ˜ 2 ) d x + b 2 Ω w ˜ v d x + Ω h 1 ( x ) g 1 ( σ ˜ ( t ) ) u + h 2 ( x ) g 2 ( σ ˜ ( t ) ) v + c 2 c 3 h 3 ( x ) g 3 ( σ ˜ ( t ) ) w ˜ d x .

Then, performing an argument similar to that in Theorem 3.1, we obtain

(4.5) u ( t + τ ) 2 + v ( t + τ ) 2 + w ( t + τ ) 2 M 5 M 4 e 2 k d 0 t ( u ( τ ) 2 + v ( τ ) 2 + w ( τ ) 2 ) + M 15 M 4 ,

which implies that T max = . Moreover, it is easy to verify that U σ ( t , τ ) ψ τ is continuous with respect to the initial data ψ τ . Hence, it generates a family of continuous processes { U σ ( t , τ ) } σ T m , t τ R on H . The translation identity follows directly from the uniqueness of the solution of (4.1).□

Lemma 4.2

The family of processes { U σ ( t , τ ) } σ T m , t τ R possesses a uniform closed bounded absorbing ball 1 = B ( 0 , R 0 ) H center at 0 with radius R 0 = 2 M 15 M 4 (independent of σ T m and τ R ) such that for any bounded set H , there exists T , 1 > 0 (depending on and 1 only) satisfying U σ ( t + τ , τ ) 1 for all t T , 1 and any σ T m . In particular, there exists T 1 > 0 such that U σ ( t + τ , τ ) 1 1 for all t T 1 and any σ T m .

Proof

This is a direct consequence of (4.5).□

Lemma 4.3

There exists a closed ball 2 = { ϕ E : ϕ E R 1 } E ( R 1 is independent of τ and R ) such that for any τ R , σ T m ,

U σ ( t + τ , τ ) 1 2 , t T 1 + 1 .

Proof

Performing a similar argument with that in Theorem 3.2, we obtain that for any σ T m , τ R , ψ τ 1 ,

u ( t + τ ) 2 + v ( t + τ ) 2 + w ( t + τ ) 2 R 1 2 , t T 1 + 1 ,

where

R 1 2 = ( M 9 + 2 M 7 R 0 2 + 2 M 8 ( m l 1 2 π 2 h 1 + m l 2 2 π 2 h 2 + m l 3 2 π 2 h 3 ) ) e M 9 ν 4 β 1 2 d 1 + β 2 2 d 2 M 4 .

Hence, for any τ R , σ T m ,

U σ ( t + τ , τ ) 1 2 , t T 1 + 1 .

Theorem 4.1

Let 3 = σ T m t 2 T 1 + 1 U σ ( t , 0 ) 1 1 2 . Then the family of processes { U σ ( t , τ ) } σ T m , t τ R possesses a uniform attractor U 3 ¯ .

Proof

This is a direct consequence of Lemmas 4.2, 4.3, and [19, Theorem 4.3.1].□

For ψ ( j 0 ) 3 , j = 1 , 2 , σ T m and t 0 , let

ψ ( j ) ( t ) = U σ j ( t , 0 ) ψ ( j 0 ) = ( u ( j ) ( t ) , v ( j ) ( t ) , w ( j ) ( t ) )

be the solutions of (4.1). Set Ψ ( t ) = ψ ( 1 ) ( t ) ψ ( 2 ) ( t ) = U σ 1 ( t , 0 ) ψ ( 10 ) U σ 2 ( t , 0 ) ψ ( 20 ) = ( ξ ( t ) , η ( t ) , ζ ( t ) ) . Then, for any θ i H 0 1 ( Ω ) , i = 1 , 2 , 3 and a.s. t τ ,

ξ , θ 1 H 1 + d 1 ( ξ , θ 1 ) = ( a 1 ξ + b 1 η α ( u 1 2 u 2 2 ) β 1 ( u 1 v 1 u 2 v 2 ) , θ 1 ) + ( g 1 * ( t ) , θ 1 ) , η , θ 2 H 1 + d 2 ( η , θ 2 ) = ( b 2 η + c 2 ζ β 2 ( u 1 v 1 u 2 v 2 ) , θ 2 ) + ( g 2 * ( t ) , θ 2 ) , ζ , θ 3 H 1 + d 3 ( ζ , θ 3 ) = ( a 3 ξ c 3 ζ , θ 3 ) + ( g 3 * ( t ) , θ 3 ) ,

where ( g i * ( t ) , θ i ) = ( h i g i ( σ ˜ 1 ( t ) ) h i g i ( σ ˜ 2 ( t ) ) , θ i ) , i = 1 , 2 , 3 .

We next show that the family of processes { U σ ( t , τ ) } σ T m , t τ R has the following result.

Lemma 4.4

Let

M 16 = max a 1 + b 1 + a 3 2 + β 1 2 ν 4 R 1 2 d 1 , b 1 + c 2 2 + b 2 + ( β 1 2 + β 2 2 ) ν 4 R 1 2 d 1 , a 3 + c 2 2 , M 17 = 2 M 16 + 2 + 2 ( l 1 2 h 1 2 + l 2 2 h 2 2 + l 3 2 h 3 2 ) .

Then, one has

  1. U σ 1 ( t , σ ) ψ ( 10 ) U σ 2 ( t , σ ) ψ ( 20 ) 2 e M 17 t 2 ( ψ ( 10 ) ψ ( 20 ) 2 + σ 1 σ 2 T m 2 ) , t 0 ;

  2. there exist T 1 > 0 and N 1 N such that

    Q N 1 ( U σ 1 ( T 1 , σ ) ψ ( 10 ) U σ 2 ( T 1 , σ ) ψ ( 20 ) ) 2 1 128 ( ψ ( 10 ) ψ ( 20 ) 2 + σ 1 σ 2 T m 2 ) ,

    where Q N 1 is defined in Section3.

Proof

Let θ 1 = ξ , θ 2 = η , θ 3 = ζ . A simple calculation shows that

1 2 d d t Ψ 2 + d 1 ξ 2 + d 2 η 2 + d 3 ζ 2 = a 1 ξ 2 + b 2 η 2 c 3 ζ 2 + Ω ( b 1 η ξ + c 2 ζ η + a 3 ξ ζ ) d x α Ω ( u 1 2 u 2 2 ) ξ d x + β 1 Ω ( u 1 v 1 u 2 v 2 ) ξ d x β 2 Ω ( u 1 v 1 u 2 v 2 ) η d x + Ω g 1 * ( t ) ξ d x + Ω g 2 * ( t ) η d x + Ω g 3 * ( t ) ζ d x .

Using (1.3), one has

(4.6) Ω g 1 * ( t ) ξ d x + Ω g 2 * ( t ) η d x + Ω g 3 * ( t ) ζ d x ( l 1 2 h 1 2 + l 2 2 h 2 2 + l 3 2 h 3 2 ) σ 1 σ 2 T m 2 + Ψ 2 .

This together with (3.15)–(3.18) yields that

d d t Ψ 2 M 17 ( Ψ 2 + σ 1 σ 2 T m 2 ) .

Note that σ 1 σ 2 T m 2 is independent of t . Hence, we obtain

d d t ( Ψ 2 + σ 1 σ 2 T m 2 ) M 17 ( Ψ 2 + σ 1 σ 2 T m 2 ) .

Applying the Gronwall inequality, we have

Ψ ( t ) 2 + σ 1 σ 2 T m 2 e M 17 t ( Ψ ( 0 ) 2 + σ 1 σ 2 T m 2 ) , t 0 .

Hence, conclusion (1) holds.

Take θ 1 = ξ N q , θ 2 = η N q , θ 3 = ζ N q . It follows that

1 2 d d t Ψ N q 2 + d 1 ξ N q 2 + d 2 η N q 2 + d 3 ζ N q 2 = a 1 ξ N q 2 + b 2 η N q 2 c 3 ζ N q 2 + Ω ( b 1 η ξ N q + c 2 ζ η N q + a 3 ξ ζ N q ) d x α Ω ( u 1 2 u 2 2 ) ξ N q d x + β 1 Ω ( u 1 v 1 u 2 v 2 ) ξ N q d x β 2 Ω ( u 1 v 1 u 2 v 2 ) η N q d x + Ω g 1 * ( t ) ξ N q d x + Ω g 2 * ( t ) η N q d x + Ω g 3 * ( t ) ζ N q d x .

Using (1.3), one has

Ω g 1 * ( t ) ξ N q d x + Ω g 2 * ( t ) η N q d x + Ω g 3 * ( t ) ζ N q d x ( l 1 2 h 1 2 + l 2 2 h 2 2 + l 3 2 h 3 2 ) σ 1 σ 2 T m 2 + Ψ 2 .

Let

M 18 = 2 max a 1 + b 1 + a 3 2 + β 1 2 ν 4 R 1 2 d 1 + β 2 2 ν 4 R 1 2 2 d 2 , b 1 + c 2 2 + b 2 + β 1 2 ν 4 R 1 2 d 1 , a 3 + c 2 2 + 1 , M 19 = l 1 2 h 1 2 + l 2 2 h 2 2 + l 3 2 h 3 2 .

From (3.20)–(3.23), it follows that

d d t Ψ N q 2 + M 9 λ N + 1 Ψ N q 2 M 18 e M 17 t ( Ψ ( 0 ) 2 + σ 1 σ 2 T m 2 ) + M 19 σ 1 σ 2 T m 2 .

Integrating the above inequality on ( 0 , t ) enables us to find

Ψ N q ( t ) 2 e M 9 λ N + 1 t + M 18 e M 17 t M 9 λ N + 1 + M 17 + M 19 M 9 λ N + 1 ( Ψ ( 0 ) 2 + σ 1 σ 2 T m 2 ) .

Thanks to (3.10), we obtain that there exist T 1 > 0 and

N 1 = min N N : e M 9 λ N + 1 T 1 + M 18 e M 17 T 1 M 9 λ N + 1 + M 17 + M 19 M 9 λ N + 1 1 128 ,

such that

Q N 1 ( U σ 1 ( T 1 , σ ) ψ ( 10 ) U σ 2 ( T 1 , σ ) ψ ( 20 ) ) 2 1 128 ( ψ ( 10 ) ψ ( 20 ) 2 + σ 1 σ 2 T m 2 ) .

From Proposition 2.2, Theorem 4.1 and Lemma 4.4, we obtain the following result.

Theorem 4.2

The family of processes { U σ ( t , τ ) } σ T m , t τ R possesses a uniform exponential attractor on 3 ¯ such that

  1. is a compact set;

  2. U ;

  3. has a finite fractal dimension, i.e.,

    dim f ( ) K 0 ( m + 2 N 1 ) ln e M 17 T 1 + 1 + 1 ,

    where K 0 is a positive constant and T 1 , N 1 are given in Lemma 4.4;

  4. there exist two positive constants a 1 and a 2 such that

    sup σ T m dist H ( U σ ( t , τ ) 3 , ) a 1 e a 2 ( t τ ) .

Acknowledgements

The authors would like to thank the referees for their valuable suggestions. And the authors are greatly indebted to all those who made suggestions for improvements to this article.

  1. Funding information: The research leading to the results of this article has received funding from the scientific research start funds for Shandong Technology and Business University advanced talents introduction (No. 306538).

  2. Author contributions: Na Liu wrote and proofread the manuscript. Yang-Yang Yu was mainly responsible for the language correction and technical verification of this manuscript.

  3. Conflict of interest: The authors state no conflict of interest.

References

[1] R. J. Field and R. M. Noyes, Oscillations in chemical systems, IV: Limit cycle behavior in a model of a real chemical reaction, J. Chem. Phys. 60 (1974), no. 5, 1877–1884. 10.1063/1.1681288Suche in Google Scholar

[2] R. J. Field and M. Burger, Oscillations and Traveling Eaves in Chemical Systems, Wiley-Interscience, New York, 1985. Suche in Google Scholar

[3] R. G. Gibbs, Traveling waves in the Belousov-Zhabotinskii reaction, SIAM J. Appl. Math. 38 (1980), no. 3, 422–444. 10.1137/0138035Suche in Google Scholar

[4] S. P. Hastings and J. D. Murray, The existence of oscillatory solutions in the Field-Noyes model for the Belousov-Zhabotinskii reaction, SIAM J. Appl. Math. 28 (1975), no. 3, 678–688. 10.1137/0128057Suche in Google Scholar

[5] C. V. Pao, Asymptotic behavior of solutions for the Belousov-Zhabotinskii reaction diffusion system, J. Partial Differ. Equ. 1 (1988), no. 1, 61–66. Suche in Google Scholar

[6] W. H. Ruan and C. V. Pao, Asymptotic behavior and positive solutions of a chemical reaction diffusion system, J. Math. Anal. Appl. 169 (1992), no. 1, 157–178. 10.1016/0022-247X(92)90109-QSuche in Google Scholar

[7] J. J. Tyson and P. C. Fife, Target patterns in a realistic model of the Belousov-Zhabotinskii reaction, J. Chem. Phys. 73 (1980), no. 5, 2224–2237. 10.1063/1.440418Suche in Google Scholar

[8] Y. C. You, Global dynamics of the oregonator system, Math. Methods Appl. Sci. 35 (2012), no. 4, 398–416. 10.1002/mma.1591Suche in Google Scholar

[9] A. V. Babin and M. I. Vishik, Attractors of Evolution Equations, North-Holland, Amsterdam, 1992. Suche in Google Scholar

[10] J. K. Hale, Asymptotic Behavior of Dissipative Systems, American Mathematical Society, Providence, RI, 1988. Suche in Google Scholar

[11] X. Y. Han, P. E. Kloeden, and S. Sonner, Discretisation of global attractors for lattice dynamical systems, J. Dynam. Differential Equations 32 (2020), no. 3, 1457–1474. 10.1007/s10884-019-09770-1Suche in Google Scholar

[12] M. D. Korzec, P. Nayar, and P. Rybka, Global attractors of sixth order PDEs describing the faceting of growing surfaces, J. Dynam. Differential Equations 28 (2016), no. 1, 49–67. 10.1007/s10884-015-9510-6Suche in Google Scholar

[13] A. C. Nimi and D. Moukoko, Global attractor and exponential attractor for a parabolic system of Cahn-Hilliard with a proliferation term, AIMS Math. 5 (2020), no. 2, 1383–1399. 10.3934/math.2020095Suche in Google Scholar

[14] J. C. Robinson, Infinite-dimensional Dynamical Systems. An Introduction to Dissipative Parabolic PDEs and the Theory of Global Attractors, Cambridge University Press, Cambridge, 2001. Suche in Google Scholar

[15] G. R. Sell and Y. You, Dynamics of Evolutionary Equations, Springer, New York, 2002. 10.1007/978-1-4757-5037-9Suche in Google Scholar

[16] R. Temam, Infinite-dimensional Dynamical Systems in Mechanics and Physics, 2nd edition, Springer-Verlag, New York, 1997. 10.1007/978-1-4612-0645-3Suche in Google Scholar

[17] M. C. Bortolan and J. M. Uzal, Pullback attractors to impulsive evolution processes: applications to differential equations and tube conditions, Discrete Contin. Dyn. Syst. 40 (2020), no. 5, 2791–2826. 10.3934/dcds.2020150Suche in Google Scholar

[18] A. N. Carvalho, J. A. Langa, and J. C. Robinson, Attractors for Infinite-dimensional Non-autonomous Dynamical Systems, Applied Mathematical Sciences, Springer, New York, 2013. 10.1007/978-1-4614-4581-4Suche in Google Scholar

[19] V. V. Chepyzhov and M. I. Vishik, Attractors for Equations of Mathematical Physics, American Mathematical Society Colloquium Publications, vol. 49, American Mathematical Society, Providence, RI, 2002. 10.1090/coll/049Suche in Google Scholar

[20] S. Netchaoui, M. A. Hammami, and T. Caraballo, Pullback exponential attractors for differential equations with delay, Discrete Contin. Dyn. Syst. Ser. S. 14 (2021), no. 4, 1345–1358. 10.3934/dcdss.2020367Suche in Google Scholar

[21] A. Eden, C. Foias, B. Nicolaenko, and R. Temam, Exponential Attractors for Dissipative Evolution Equations, John Wiley and Sons, Chichester, 1994. Suche in Google Scholar

[22] A. Y. Abdallah, Uniform exponential attractors for first order non-autonomous lattice dynamical systems, J. Differential Equations 251 (2011), no. 6, 1489–1504. 10.1016/j.jde.2011.05.030Suche in Google Scholar

[23] J. A. Langa, A. Miranville, and J. Real, Pullback exponential attractors, Discrete Contin. Dyn. Syst. 26 (2010), no. 4, 1329–1357. 10.3934/dcds.2010.26.1329Suche in Google Scholar

[24] S. F. Zhou and X. Y. Han, Pullback exponential attractors for non-autonomous lattice systems, J. Dynam. Differential Equations 24 (2012), no. 3, 601–631. 10.1007/s10884-012-9260-7Suche in Google Scholar

[25] M. A. Hammami, L. Mchiri, S. Netchaoui, and S. Sonner, Pullback exponential attractors for differential equations with variable delays, Discrete Contin. Dyn. Syst. Ser. B 25 (2020), no. 1, 301–319. 10.3934/dcdsb.2019183Suche in Google Scholar

[26] H. Cui, A. N. Carvalho, A. C. Cunha, and J. A. Langa, Smoothing and finite-dimensionality of uniform attractors in Banach spaces, J. Differential Equations 285 (2021), no. 4, 383–428. 10.1016/j.jde.2021.03.013Suche in Google Scholar

[27] R. Czaja and M. Efendiev, Pullback exponential attractors for nonautonomous equations, II: Applications to reaction-diffusion systems, J. Math. Anal. Appl. 381 (2011), no. 2, 766–780. 10.1016/j.jmaa.2011.03.052Suche in Google Scholar

[28] R. Czaja and M. Efendiev, Pullback exponential attractors for nonautonomous equations Part I: Semilinear parabolic problems, J. Math. Anal. Appl. 381 (2011), no. 2, 748–765. 10.1016/j.jmaa.2011.03.053Suche in Google Scholar

[29] S. F. Zhou and X. Y. Han, Uniform exponential attractors for non-autonomous KGS and Zakharov lattice systems with quasiperiodic external forces, Nonlinear Anal. 78 (2013), 141–155. 10.1016/j.na.2012.10.001Suche in Google Scholar

Received: 2023-12-11
Revised: 2024-09-11
Accepted: 2024-09-11
Published Online: 2024-10-15

© 2024 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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