Hindawi Publishing Corporation Abstract and Applied Analysis Volume 2013, Article ID 494067, 7 pages http://dx.doi.org/10.1155/2013/494067 Research Article The Asymptotic Behavior for a Class of Impulsive Delay Differential Equations Zhichun Yang Department of Mathematics, Chongqing Normal University, Chongqing 400047, China Correspondence should be addressed to Zhichun Yang; zhichy@yahoo.com.cn Received 27 January 2013; Accepted 21 March 2013 Academic Editor: Chuangxia Huang Copyright © 2013 Zhichun Yang. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. This paper is concerned with asymptotical behavior for a class of impulsive delay differential equations. The new criteria for determining attracting sets and attracting basin of the impulsive system are obtained by developing the properties of quasi-invariant sets. Examples and numerical simulations are given to illustrate the effectiveness of our results. In addition, we show that the impulsive effects may play a key role to these asymptotical properties even though the solutions of corresponding nonimpulsive systems are unbounded. 1. Introduction Impulsive delay differential equations have attracted increasing interests since time delays and impulsive effects commonly exist in many fields such as population dynamics, automatic control, drug administration, and communication networks [1–4]. In past two decades, its asymptotical behaviors such as stability and attractivity of the equilibrium point or periodical solutions have been deeply studied for impulsive functional differential equations (see, [5–18]). However, under impulsive perturbation, the solutions may not be attracted to an equilibrium point or periodical trajectory but to some bounded region. In this case, it is interesting to investigate the attracting set and attracting basin, that is, the region attracting the solutions and the range in which initial values vary when remaining the attractivity for impulsive delay differential equations. In [19], Xu and Yang first give the method to estimate global attracting set and invariant set for impulsive delayed systems by developing delayed differential inequalities. The techniques are further developed to study global attractivity for some complex impulsive systems such as impulsive neutral differential equations [20, 21] and impulsive stochastic systems [22]. But the techniques and methods given in the existing publications are invalid for determining locally attracting set and attracting basin for impulsive delay differential equations. In this paper, our objective is to mainly discuss the asymptotical behavior on (locally) attracting set and its attracting basin for a class of impulsive delay differential equations. Based on the quasi-invariant properties, we estimate the existence range of attracting set and attracting basin of the impulsive delay systems by solving algebraic equations and employing differential inequality technique. Examples are given to illustrate the effectiveness of our method and show that the asymptotic behavior of the impulsive systems may be different from one of the corresponding continuous systems. 2. Preliminaries Let π be the set of all positive integers, π π the space of πdimensional real column vectors, and π π×π the set of π × π real matrices. For π΄, π΅ ∈ π π×π or π΄, π΅ ∈ π π , π΄ ≥ π΅(π΄ ≤ π΅, π΄ > π΅, π΄ < π΅) means that each pair of corresponding elements of π΄ and π΅ satisfies the inequality “≥(≤, >, <).” π +π = {π₯ ∈ π π | π₯ ≥ 0}, πΈ = (1, 1, . . . , 1)π ∈ π π , and πΌ denotes an π × π unit matrix. Let π > 0 and π‘0 < π‘1 < π‘2 < ⋅ ⋅ ⋅ be the fixed points with limπ → ∞ π‘π = ∞ (called impulsive moments). πΆ[π, π] denotes the space of continuous mappings from Δ the topological space π to the topological space π. Let πΆ = πΆ[[−π, 0], π π ] especially. 2 Abstract and Applied Analysis Δ Morever, PC = {π : [−π, 0] → π π | π(π‘+ ) = π(π‘) for π‘ ∈ [−π, 0), π(π‘− ) exists for π‘ ∈ (−π, 0], π(π‘− ) = π(π‘) for all but at most a finite number of points π‘ ∈ (−π, 0]}. PC is a space of piecewise right-hand continuous functions which is a nature extension of the phrase space πΆ. Δ We define PC[[π‘0 , ∞), π π ] = {π : [π‘0 , ∞) → π π | π(π‘) is continuous at π‘ =ΜΈ π‘π , π(π‘π+ ) and π(π‘π− ) exist, π(π‘π ) = π(π‘π+ ), for π ∈ π}. For π₯ ∈ π π , π΄ ∈ π π×π , π ∈ πΆ or π ∈ PC, we define σ΅¨ σ΅¨π σ΅¨ σ΅¨ σ΅¨ σ΅¨ [π₯]+ = (σ΅¨σ΅¨σ΅¨π₯1 σ΅¨σ΅¨σ΅¨ , σ΅¨σ΅¨σ΅¨π₯2 σ΅¨σ΅¨σ΅¨ , . . . , σ΅¨σ΅¨σ΅¨π₯π σ΅¨σ΅¨σ΅¨) , σ΅¨ σ΅¨ [π΄]+ = (σ΅¨σ΅¨σ΅¨σ΅¨πππ σ΅¨σ΅¨σ΅¨σ΅¨)π×π , + σ΅© σ΅© σ΅© σ΅© σ΅© σ΅© [π]π = (σ΅©σ΅©σ΅©π1 σ΅©σ΅©σ΅©π , σ΅©σ΅©σ΅©π2 σ΅©σ΅©σ΅©π , . . . , σ΅©σ΅©σ΅©ππ σ΅©σ΅©σ΅©π ) , (1) where β ππ βπ = supπ ∈[−π,0] β ππ (π ) β and β ⋅ β is an norm in π π . In this paper, we will consider a impulsive delay differential equations: π₯Μ (π‘) = π΄π₯ (π‘) + π (π‘, π₯π‘ ) , π‘ =ΜΈ π‘π , π‘ ≥ π‘0 , Δπ₯ = π΅π₯ (π‘π− ) + πΌπ (π‘π− , π₯ (π‘π− )) , π ∈ π, (2) Μ denotes the right-hand derivative of π₯(π‘), Δπ₯ = where π₯(π‘) π₯(π‘π+ ) − π₯(π‘π− ), π₯(π‘π ) = π₯(π‘π+ ), π΄ = diag{π1 ,π2 , . . . , ππ }, π΅ = diag{π1 , π2 , . . . , ππ }, π ∈ πΆ[[π‘π−1 , π‘π ) × PC, π π ], and the limit lim(π‘,π) → (π‘π− ,π) π(π‘, π) = π(π‘π− , π) exists, πΌπ ∈ πΆ[[π‘0 , ∞) × π π , π π ], and π₯π‘ ∈ PC is defined by π₯π‘ (π ) = π₯(π‘ + π ), π ∈ [−π, 0]. A function π₯(π‘) : [π‘0 − π, ∞) → π π is called to be a solution of (2) through (π‘0 , π), if π₯(π‘) ∈ PC[[π‘0 , ∞), π π ] as π‘ ≥ π‘0 , and satisfies (2) with the initial condition π₯ (π‘0 + π ) = π (π ) , π ∈ [−π, 0] , π ∈ PC. (3) Throughout the paper, we always assume that for any π ∈ PC, system (2) has at least one solution through (π‘0 , π), denoted by π₯(π‘, π‘0 , π) or π₯π‘ (π‘0 , π) (simply π₯(π‘) and π₯π‘ if no confusion should occur), where π₯π‘ (π‘0 , π) = π₯(π‘ + π , π‘0 , π) ∈ PC, π ∈ [−π, 0]. In this paper, we need the following definitions involving attracting set, attracting basin, the quasi-invariant set of impulsive systems, and monotonous vector functions. Definition 1. The set π ⊂ PC is called to be an attracting set of (2), and π· ⊂ PC is called an attraction basin of π, if for any initial value π ∈ π·, the solution π₯π‘ (π‘0 , π) converges to π as π‘ → +∞. That is, Definition 3. Let Ω ⊂ π π . The vector function πΉ(π₯) : Ω → π π is called to be monotonically nondecreasing in Ω, if for any π₯σΈ , π₯σΈ σΈ ∈ Ω, π₯σΈ ≤ π₯σΈ σΈ implies πΉ(π₯σΈ ) ≤ πΉ(π₯σΈ σΈ ). 3. Main Results In this paper, we always make the following assumptions. (π»1 ) There exist nonnegative constants π, σ° such that 0 < π ≤ π‘π − π‘π−1 ≤ σ°, for π ∈ π. (π»2 ) [π(π‘, π)]+ ≤ π([π]+π ) for π‘ ≥ π‘0 and π ∈ PC, where the vector function π(⋅) : π +π → π +π is continuous and monotonically nondecreasing in π +π . (π»3 ) [πΌπ (π‘, π₯)]+ ≤ π([π₯]+ ), for π‘ ≥ π‘0 , π ∈ π and π₯ ∈ π π , where the vector function π(⋅) : π +π → π +π is continuous and monotonically nondecreasing in π +π . To obtain attractivity, we first give the quasi-invariant properties of (2). Theorem 4. Assume that in addition to (π»1 )–(π»3 ), there is a vector π§∗ ≥ 0 such that −1 π (ππ§∗ ) + π[πΌ − π−ππ ] π (ππ§∗ ) − ππ§∗ < 0, (5) where π = diag{π€1 , . . . , π€π }, π = diag{π1 , . . . , ππ }, π€π > 0, ππ ≥ 1, π = 1, 2, . . . , π, are defined by σ΅¨ σ΅¨ ln σ΅¨σ΅¨σ΅¨1 + ππ σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ { { − , if 0 < σ΅¨σ΅¨σ΅¨1 + ππ σ΅¨σ΅¨σ΅¨ < 1, −π { π { σ° π€π = { { σ΅¨σ΅¨ σ΅¨σ΅¨ { {−π − ln σ΅¨σ΅¨1 + ππ σ΅¨σ΅¨ , if σ΅¨σ΅¨1 + π σ΅¨σ΅¨ ≥ 1, π π σ΅¨σ΅¨ σ΅¨σ΅¨ (6) { π 1 σ΅¨ σ΅¨ { σ΅¨σ΅¨ σ΅¨ , if 0 < σ΅¨σ΅¨σ΅¨1 + ππ σ΅¨σ΅¨σ΅¨ < 1, ππ = { σ΅¨σ΅¨1 + ππ σ΅¨σ΅¨σ΅¨ σ΅¨ σ΅¨ if σ΅¨σ΅¨σ΅¨1 + ππ σ΅¨σ΅¨σ΅¨ ≥ 1. {1, Then, the set π· = {π ∈ PC | [π]+π ≤ π§∗ } is a positive quasiinvariant set of (2). When π = πΌ especially, π· is a positive invariant set of (2). Proof. Let π₯(π‘) = π₯(π‘, π‘0 , π) be a solution of (2) through (π‘0 , π). It is easily verified that the following formula for the variation of parameters is valid: π‘ π₯ (π‘) = πΎ (π‘, π‘0 ) π (0) + ∫ πΎ (π‘, π ) π (π , π₯π ) ππ π‘0 + ∑ πΎ (π‘, π‘π ) πΌπ (π‘π− , π₯ (π‘π− )) , π‘0 <π‘π ≤π‘ (7) π‘ ≥ π‘0 , (4) where πΎ(π‘, π ) is the Cauchy matrix of linear impulsive system where dist(π, π) = inf π∈π dist(π, π), dist(π, π) = supπ ∈[−π,0] βπ(π ) − π(π )β, for π ∈ PC. π‘ =ΜΈ π‘π , { {π¦Μ (π‘) = π΄π¦ (π‘) , (8) { { + − Δπ¦ (π‘ ) = π΅π¦ (π‘ ) , π ∈ π. π π { According to the representation of the Cauchy matrix (see page 74 [2]), dist (π₯π‘ (π‘0 , π) , π) σ³¨→ 0, aπ π‘ σ³¨→ +∞, Definition 2. The set π· ⊂ PC is called to be a positive quasiinvariant set of (2), if there is a positive diagonal matrix πΏ = diag{ππ } such that for any initial value π ∈ π·, the solutions π₯π‘ (π‘0 , π) satisfy πΏπ₯π‘ (π‘0 , π) ∈ π·, for π‘ ≥ π‘0 . When πΏ = πΌ(identity matrix) especially, the set π· is called positively invariant. πΎ (π‘, π ) = ππ΄(π‘−π ) ∏ (πΌ + π΅) , π <π‘π ≤π‘ π‘ ≥ π ≥ π‘0 . (9) Abstract and Applied Analysis 3 Since 0 < π ≤ π‘π − π‘π−1 ≤ σ°, for π ∈ π, we obtain the following estimate: σ΅¨ σ΅¨ ∏ σ΅¨σ΅¨σ΅¨1 + ππ σ΅¨σ΅¨σ΅¨ + [π₯ (π‘∗ )] ≤ π−π(π‘ π <π‘π ≤π‘ 1 σ΅¨σ΅¨ σ΅¨ σ΅¨ σ΅¨ (ln|1+ππ |/σ°)(π‘−π ) = σ΅¨σ΅¨ , if 0 < σ΅¨σ΅¨σ΅¨1 + ππ σ΅¨σ΅¨σ΅¨ < 1, σ΅¨1 + ππ σ΅¨σ΅¨σ΅¨ { σ΅¨π { {σ΅¨ σ΅¨σ΅¨1 + ππ σ΅¨σ΅¨σ΅¨ ≤{ { {σ΅¨ σ΅¨(π‘−π )/π σ΅¨ σ΅¨ = π(ln|1+ππ |/π)(π‘−π ) , if σ΅¨σ΅¨σ΅¨1 + ππ σ΅¨σ΅¨σ΅¨ ≥ 1. {σ΅¨σ΅¨σ΅¨1 + ππ σ΅¨σ΅¨σ΅¨ (10) ((π‘−π )/σ°)−1 + −π(π‘−π ) [πΎ (π‘, π )] ≤ ππ , π‘ ≥ π ≥ π‘0 . (11) −π(π‘−π‘0 ) [π₯ (π‘)] ≤ ππ π‘ + [π]π + π∫ π π‘0 π‘ ≥ π‘0 . π‘0 <π‘π ≤π‘ −π(π‘−π‘π ) ≤ ∑ π π‘0 <π‘π ≤π‘ ∗ −π‘π ) ≤π‘∗ −π‘0 ) −π‘0 ) π (ππ§) ππ§ + π (πΌ − π−π(π‘ ∗ −π‘0 ) ∗ −π‘0 ) ) π−1 π (ππ§) −1 ) [πΌ − π−ππ ] π (ππ§) ππ−1 −ππ [πΌ − π −1 −π(π‘π −π‘π−1 ) [πΌ − π = ππ§. (18) −ππ −1 ] [πΌ − π −1 < ππ−1 [ππ§ − π (ππ§) − π[πΌ − π−ππ ] π (ππ§)] + π−1 ππ (ππ§) + π[πΌ − π−ππ ] π (ππ§) Since π‘π − π‘π−1 ≥ π > 0 and π = diag{π€1 , . . . , π€π } > 0, we have = ∑ π ∗ ∗ π (ππ§) ππ + π−1 ππ (ππ§) + π[πΌ − π−ππ ] π (ππ§) (12) π‘0 <π‘π ≤π‘ ∑ π −π ) −1 + π ([π₯π ]π ) ππ + −π(π‘−π‘π ) π‘0 <π‘π = π−π(π‘ ∗ π‘0 + π ∑ π−π(π‘ < π−π(π‘ π‘∗ + π[π]π + π ∫ π−π(π‘ −1 −π(π‘−π ) + π ∑ π−π(π‘−π‘π ) π ([π₯ (π‘π− )] ) , −π(π‘−π‘π ) −π‘0 ) × [ππ§ − π (ππ§) − π[πΌ − π−ππ ] π (ππ§)] By (7) and (11) and the assumptions (π»2 ) and (π»3 ), then + ∗ + π (πΌ − π−π(π‘ In terms of the definition of π and π, π‘0 <π‘π ≤π‘ By using (12), (13), (14), (17), π > 0, and the monotonicity of π(⋅), π(⋅), we can get ] This contradicts (16), and so (15) holds. Letting π → 0, from (15), we have for any π ∈ π· (i.e., [π]+π ≤ π§∗ ), −ππ −1 ] [πΌ − π ] + [π₯ (π‘, π‘0 , π)] ≤ ππ§∗ , + that is, [π−1 π₯ (π‘, π‘0 , π)] ≤ π§∗ , π‘ ≥ π‘0 . (19) −ππ −1 = ∑ [π−π(π‘−π‘π ) − π−π(π‘−π‘π−1 ) ] [πΌ − π π‘0 <π‘π ≤π‘ ] −1 ≤ [πΌ − π−π(π‘−π‘0 ) ] [πΌ − π−ππ ] . (13) From the strict inequality (5), there is an enough small number π > 0 such that −ππ −1 π (ππ§) + π[πΌ − π Based on the obtained quasi-invariant set, we have the following Theorem 5. Let −1 ] π (ππ§) − ππ§ < 0, (14) Δ Therefore, the set π· = {π ∈ PC | [π]+π ≤ π§∗ } is a positive quasi-invariant set of (2). When π = πΌ especially, π· is a positive invariant set of (2). The proof is complete. Δ (π§) = π (π§) + π[πΌ − π−ππ ] π (π§) − π−1 ππ§, π§ = π§∗ + ππΈ > 0. Assume that all conditions in Theorem 4 hold. Define In the following, we will prove that [π]+π < π§ implies + [π₯ (π‘)]+ = [π₯ (π‘, π‘0 , π)] < ππ§, π‘ ≥ π‘0 . Ω1 = {π§ ∈ π +π | Δ (ππ§) < 0} , (15) Ω2 = {π§ ∈ π +π | Δ (π§) < 0} , Otherwise, from the piecewise continuity of π₯(π‘), there must be an integer π and π‘∗ > π‘0 such that Ω3 = {π§ ∈ π +π | Δ (π§) ≥ 0} , σ΅¨σ΅¨ ∗ σ΅¨ σ΅¨σ΅¨π₯π (π‘ )σ΅¨σ΅¨σ΅¨ ≥ ππ π§π , + [π₯ (π‘)] ≤ ππ§, (16) ∗ π‘0 ≤ π‘ < π‘ . π§ ∈ π +π . (20) (17) Ω∗1 = β {π§ ∈ π§∗ ∈Ω1 π +π ∗ | π§ ≤ π§ }, Ω∗2 = β {π§ ∈ π +π | π§ ≤ π§∗ } . π§∗ ∈Ω2 (21) 4 Abstract and Applied Analysis Then, π = {π ∈ PC | [π]+π ∈ Ω∗2 ∩ Ω3 } is an attracting set of (2) and π· = {π ∈ PC | [π]+π ∈ Ω∗1 } is the attracting basin of π. Proof. From (5) and the definitions of the above sets, then π§∗ ∈ Ω1 , ππ§∗ ∈ Ω2 , 0 ∈ Ω∗1 , 0 ∈ Ω∗2 , 0 ∈ Ω3 . Obviously, Ω1 , Ω2 , Ω∗1 , Ω∗2 , Ω3 and Ω∗2 ∩ Ω3 are nonempty, and so the definitions of the sets of π and π· are valid. For any π ∈ π·, there is a π§∗ ∈ Ω1 satisfying [π]+π ≤ π§∗ . According to Theorem 4, we obtain + + ∗ [π₯ (π‘)] = [π₯ (π‘, π‘0 , π)] ≤ ππ§ ∈ Ω2 , ∀π‘ ≥ π‘0 . (22) π‘ +∫ π‘−π2 π−π(π‘−π ) ππ (ππΈ + π) ππ + π ∑ π−π(π‘−π‘π ) π (ππ§∗ ) π‘0 <π‘π ≤π1 + π ∑ π−π(π‘−π‘π ) π (ππΈ + π) π1 <π‘π ≤π‘ ≤ π−π(π‘−π‘0 ) ππ§∗ + πππ (ππ§∗ ) + (πΌ − π−ππ2 ) π−1 ππ (ππΈ + π) + πππ (ππ§∗ ) −1 + π (πΌ − π−π(π‘−π1 ) ) [πΌ − π−ππ ] π (ππΈ + π) ≤ π−π(π‘−π‘0 ) ππ§∗ + ππ [π (ππ§∗ ) + π (ππ§∗ )] That is, −1 Δ + π = lim sup [π₯ (π‘)] ∈ π‘→∞ + π−1 ππ (ππΈ + π) + π[πΌ − π−ππ ] π (ππΈ + π) . Ω∗2 . (23) (26) This implies that Then, for any given π > 0, there is a π1 > π‘0 such that + [π₯ (π‘)] ≤ ππΈ + π, π = lim sup[π₯ (π‘)]+ ≤ ππ [π (ππ§∗ ) + π (ππ§∗ )] π‘ → +∞ (27) −1 π‘ ≥ π1 . (24) + π−1 ππ (ππΈ + π) + π[πΌ − π−ππ ] π (ππΈ + π) . Letting π → 0+ , then In light of π = diag{π€π } > 0, for the above π > 0 and π1 , we can find an enough large π2 > 0 such that −1 π ≤ π−1 ππ (π) + π[πΌ − π−ππ ] π (π) . (28) That is, Δ(π) ≥ 0 and π ∈ Ω3 . Thus, π ∈ Ω∗2 ∩ Ω3 . ∞ ∫ π−ππ ππ ≤ ππΌ, π2 −π(π‘−π‘π ) ∑ π ≤ ππΌ, π‘0 <π‘π ≤π1 (25) π‘ > π2 . Using (12), (13), (22), (24), and (25), we have for π‘ ≥ π+π1 +π2 , + ∑ ππ π‘0 <π‘π ≤π‘ + π ([π₯ (π‘π− )] ) + π‘−π2 π‘0 π‘ +∫ π‘−π2 Corollary 6. Assume that (π»1 )–(π»3 ) hold with π = (πππ )π×π ≥ 0, π = (πππ )π×π ≥ 0, + } π−π(π‘−π ) ππ ([π₯π ]π ) ππ } { + + { ∑ + ∑ } ππ−π(π‘−π‘π ) π ([π₯ (π‘π− )] ) {π‘0 <π‘π ≤π1 π1 <π‘π ≤π‘} ∞ ≤ π−π(π‘−π‘0 ) ππ§∗ + ∫ π−ππ ππ (ππ§∗ ) ππ π2 + π ([π]π ) = π[π]π + π, π π = (π1 , . . . , ππ ) ≥ 0, π ([π₯]+ ) = π[π₯]+ + ], ≤ π−π(π‘−π‘0 ) π[π]π + {∫ From the above theorems, we can obtain sufficient conditions ensuring global attractivity and stability in the following corollaries. + π‘0 −π(π‘−π‘π ) From the definition of π and π, dist (π₯π‘ (π‘0 , π), π) → 0 as π‘ → +∞. The proof is complete. + π‘ + [π₯ (π‘)]+ ≤ π−π(π‘−π‘0 ) π[π]π + ∫ π−π(π‘−π ) ππ ([π₯π ]π ) ππ (29) (30) π ] = (]1 , . . . , ]π ) ≥ 0. If the spectral radius π (Λ) < 1, −1 where Λ = π−1 ππ + π[πΌ − π−ππ] π, (31) Δ then π· = {π ∈ PC | [π]+π ≤ π = (πΌ − Λ)−1 π−1 (π + π[πΌ − π−ππ]−1 ])} is a positive quasi-invariant set of (2), and π = {π ∈ PC | [π]+π ≤ (πΌ − Λ)−1 π−1 π(π + π[πΌ − π−ππ]−1 ])} is a global attracting set of (2). Abstract and Applied Analysis 5 Proof. Since π(π§) = ππ§ + π and π(π§) = ππ§ + ], we directly calculate −1 Δ (π§) = π−1 π (Λ − πΌ) π§ + π + π[πΌ − π−ππ] ], (32) −1 Δ (ππ§) = π (Λ − πΌ) π§ + π + π[πΌ − π−ππ] ]. Without loss of generality, we assume that π, ] > 0. Since π(Λ) < 1, (πΌ − Λ)−1 exists and (πΌ − Λ)−1 ≥ 0 (see [23]), and so π > 0. For any π > 0, we take π§∗ = (1 + π )π > 0 in Theorem 4 and verify the condition (5): −1 Δ (ππ§∗ ) = −π (π + π[πΌ − π−ππ] ]) < 0. (33) According to Theorem 4, when π → 0, we deduce that π· is a positive quasi-invariant set of (2). Furthermore, by (33), (1 + π ) π ∈ Ω1 , (1 + π ) ππ ∈ Ω2 . (34) From the arbitrariness of π , we obtain Ω∗1 = Ω∗2 = π +π . Moreover, Ω3 = {π§ ∈ π +π | Δ (π§) ≥ 0} −1 According to Theorems 4 and 5, we have π = σ° = 0.15, π΄ = 0.2, π΅ = −0.6, π = 2.5, π β 5.9086, π(π§) = 0.2π§2 + 0.1, π(π§) = 0.1π§2 + 0.1, Δ(π§) β 1.2052π§2 − 2.3634π§ + 1.1052, and so Ω1 = {π§ ∈ π + | Δ (ππ§) < 0} = (0.3079, 0.4765) , Ω∗1 = [0, 0.4765] , Ω2 = {π§ ∈ π + | Δ (π§) < 0} = (0.7698, 1.1913) , Ω∗2 = [0, 1.1913] , Ω3 = {π§ ∈ π + | Δ (π§) ≥ 0} = [0, 0.7698] ∪ [1.1913, +∞) , Ω∗2 ∩ Ω3 = [0, 0.7698] . (37) Thus, π = {π ∈ PC | [π]+π ≤ 0.7698} is an attracting set of (36), and π· = {π ∈ PC | [π]+π ≤ 0.4765} is an attracting basin of π. However, solutions of the corresponding continuous system (i.e., Δπ₯ = 0 in (36)) may be unbounded. Taking the initial condition π(π ) = 0.2, π ∈ [−1, 0], Figure 1 shows the different asymptotic behavior between the solution of (36) with no impulse and one with impulses. = {π§ ∈ π +π | π−1 π (Λ − πΌ) π§ + π + π[πΌ − π−ππ] ] ≥ 0} −1 = {π§ ∈ π +π | (πΌ − Λ) π§ ≤ π−1 π (π + π[πΌ − π−ππ] ])} Example 9. Consider a 2-dimensional impulsive delay system π₯Μ 1 (π‘) = π₯1 (π‘) + 0.5 sin (π₯1 (π‘ − 1)) − 0.4π₯2 (π‘ − 1) − 0.5, ⊂ {π§ ∈ π +π | π§ ≤ (πΌ − Λ)−1 π−1 π π‘ ≥ 0, π₯Μ 2 (π‘) = −4π₯2 (π‘) − 0.5π₯1 (π‘ − 1) + 0.4 cos (π₯2 (π‘ − 1)) + 0.5, −1 × (π + π[πΌ − π−ππ] ])} . π‘ =ΜΈ π‘π , (35) It follows from Theorem 5 that πσΈ = {π ∈ PC | [π]+π ∈ Ω3 } is a global attracting set of (2) and π is also a global attracting set due to πσΈ ⊂ π. The proof is complete. Δπ₯1 = −0.5π₯1 (π‘π− ) + 0.1 cos (π₯1 (π‘π− )) + 0.5 sin (ππ‘π ) , Corollary 7. Assume that all conditions in Corollary 6 hold with π = ] = 0. Then, the zero solution π₯(π‘) = 0 of (2) is globally asymptotically stable. Δπ₯2 = 0.1π₯2 (π‘π− ) + 0.2 sin (π₯2 (π‘π− )) − 0.5 cos (ππ‘π ) , 4. Illustrative Examples The following illustrative examples will demonstrate the effectiveness of our results and also show the different asymptotical behaviors between the impulsive system and the corresponding continuous system. Example 8. Consider a scalar nonlinear impulsive delay system π₯Μ (π‘) = 0.2π₯ (π‘) + 0.2π₯2 (π‘ − 1) + 0.1, π‘ =ΜΈ π‘π , π ∈ π, π‘ ≥ π‘0 = 0, Δπ₯ = −0.6π₯ (π‘π− ) + 0.1π₯2 (π‘π− ) + 0.1 sin (ππ‘π ) , π‘π = π‘π−1 + 0.15. (36) π‘π = 0.1π, π ∈ π. (38) According to Corollary 6, we have π = σ° = 0.1, π΄ = diag{1, −4}, π΅ = diag{−0.5, 0.1}, π = diag{2, 1}, π = diag{5.9315, 3.0469}, π(π§) = ππ§ + π, π(π§) = ππ§ + ], Λ = π−1 ππ + π[πΌ − π−ππ]−1 π, where π=( 0.5 0.4 ), 0.5 0.4 0.5 π = ] = ( ), 0.5 π=( 0.1 0 ), 0 0.2 0.6156 0.1349 Λ=( ), 0.1641 0.8928 (39) and so π(Λ) = 0.9575 < 1. Therefore, π· = {π ∈ PC | [π]+π ≤ (1.7105, 2.5228)π } is a positive quasi-invariant set of (38), and π = {π ∈ PC | [π]+π ≤ (1.8637, 2.8720)π } is a global attracting set of (38). Figure 2 shows the asymptotic properties of solutions of (38) under the different initial conditions. 6 Abstract and Applied Analysis 10 π₯(π‘) 0.3 0.2 π₯(π‘) ×103 15 5 0 −5 0.1 0 −0.1 2 0 4 6 8 12 10 −0.2 0 2 4 6 8 10 12 14 16 Time π‘ Time π‘ (a) (b) Figure 1: The trajectory of (36) with: (a) no impulse (i.e., Δπ₯ = 0) and (b) impulses. Global attracting set 4 3 2 π¦2 1 0 −1 −2 −3 −4 −5 0 π¦1 5 Figure 2: Global attracting set of (38). Acknowledgments This work is supported partially by the National Natural Science Foundation of China under Grant nos. 10971240, 61263020, and 61004042, the Key Project of Chinese Education Ministry under Grant no. 212138, the Natural Science Foundation of Chongqing under Grant CQ CSTC 2011BB0117, and the Foundation of Science and Technology project of Chongqing Education Commission under Grant KJ120630. References [1] A. M. Somoilenko and N. A. Perslyuk, Differential Equations With Impulse Effect, Visca Skala, Kiev, Ukraine, 1987. [2] V. 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