Hindawi Publishing Corporation Journal of Applied Mathematics Volume 2013, Article ID 401572, 8 pages http://dx.doi.org/10.1155/2013/401572 Research Article Input-to-State Stability of Singularly Perturbed Control Systems with Delays Yongxiang Zhao,1,2 Aiguo Xiao,2 and Li Li1 1 2 School of Mathematics and Statistics, Chongqing Three Gorges University, Wanzhou 404000, China School of Mathematics and Computational Science, Hunan Key Laboratory for Computation and Simulation in Science and Engineering, Xiangtan University, Xiangtan, Hunan 411105, China Correspondence should be addressed to Yongxiang Zhao; zyxlily80@126.com Received 16 December 2012; Revised 9 April 2013; Accepted 14 May 2013 Academic Editor: Kang Liu Copyright © 2013 Yongxiang Zhao et al. 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. We study the input-to-state stability of singularly perturbed control systems with delays. By using the generalized Halanay inequality and Lyapunov functions, we derive the input-to-state stability of some classes of linear and nonlinear singularly perturbed control systems with delays. 1. Introduction The stability properties of control systems are an important research field. The concept of input-to-state stability (ISS) of the control systems was proposed by Sontag [1]. Since then, the ISS of the control systems has been widely studied (cf. [2– 12]), and most of the obtained results are often based on the Lyapunov functions. Singularly perturbed control systems are a special class of control systems which is characterized by small parameters multiplying the highest derivates. Recently, many attentions have been devoted to the study of singularly perturbed systems, in particular, to their stability properties. Saberi and Khalil [13] investigated the asymptotic and exponential stability of nonlinear singularly perturbed systems. They obtained a quadratic-type Lyapunov function as a weighted sum of quadratic-type Lyapunov functions of the reduced and the boundary-layer systems. They used the composite Lyapunov function to estimate the degree of exponential stability and the domain of attraction of stable equilibrium point. Corless and Glielmo [14] obtained some results and properties related to exponential stability of singularly perturbed systems. They pointed out that, if both the reduced and the boundarylayer systems are exponentially stable, then, provided that some further regularity conditions are satisfied, the full-order system is exponentially stable for sufficiently small value π. Liu et al. [15] derived the exponential stability criteria of singularly perturbed systems with time delay. Christofides and Teel [11] obtained a type of total stability for the input-tostate stability property with respect to singular perturbations under the assumptions that the reduced system is ISS and the boundary-layer system is uniformly globally asymptotically stable. Tian [16, 17] discussed the analytic and numerical dissipativity and exponential stability of singularly perturbed delay differential equations. There are some results about the stability of numerical methods for control systems (cf. [18, 19]). The previous studies have mainly focused on the exponential stability of singularly perturbed systems with or without delays and the ISS of singularly perturbed control systems without delay. There are no results about the ISS of delay singulary perturbed control systems. In this paper, we study the ISS of some classes of delay singularly perturbed control systems. By using the generalized Halanay inequality and the Lyapunov functions, we obtain the sufficient conditions under which these delay singularly perturbed control systems are input-to-state stable. 2 Journal of Applied Mathematics where πΊ = supπ‘0 −π≤π≤π‘0 |π€(π)| and πβ > 0 is defined as 2. Preliminary We introduce the following symbols (cf. [8, 11, 15]). (1) β ⋅ β denotes the standard Euclidean norm of a vector, β|π₯π‘ |β = supπ∈[π‘−π,π‘] βπ₯(π)β and βπ΄β = max1≤π≤π (∑ππ=1 πππ2 )1/2 denotes the norm of an π × π matrix π΄ = (πππ ). A matrix π΄(π‘) is bounded means that βπ΄(π‘)β < ∞. (2) π΄π denotes the transpose of the matrix π΄, π π (π΄) denotes the πth eigenvalue of the matrix π΄, and Re π π (π΄) denotes the real part of π π (π΄). (3) The matrix π΄ > 0 means that π΄ is positive-definite. The vector V = (V1 , V2 , . . . , Vπ )π ≥ 0 (> 0) means each component Vπ ≥ 0 (> 0), π = 1, 2, . . . , π. (4) A real π × π matrix π΄ = (πππ ) with πππ ≤ 0 for all π =ΜΈ π is an π-matrix if π΄ is nonsingular and π΄−1 > 0. (5) For any measurable locally essentially bounded function π’ : π ≥0 → π π , βπ’[0,π‘) β = supπ‘≥0 {βπ’(π‘)β}. (6) A function πΎ: π ≥0 → π ≥0 is a π -function if it is continuous, strictly increasing, and πΎ(0) = 0. (7) A function π½: π ≥0 × π ≥0 → π ≥0 is a π π-function if, for each fixed π‘ ≥ 0, the function π½(⋅, π‘) ∈ π , and for each fixed π ≥ 0, the function π½(π , ⋅) is decreasing and π½(π , π‘) → 0 as π‘ → ∞. Lemma 1 (see [20]). Let π΄(π‘) be an π × π matrix whose elements are continuous functions defined on the time interval π½ = [0, ∞) and the following assumptions hold: (i) Re π (π΄ (π‘)) ≤ −π1 < 0, (ii) βπ΄ (π‘)β ≤ π2 , σ΅© σ΅© (iii) σ΅©σ΅©σ΅©σ΅©π΄σΈ (π‘)σ΅©σ΅©σ΅©σ΅© ≤ π2 , ∀π‘ ∈ π½, ∀π‘ ∈ π½, (1) Then there exists a positive-definitive matrix π(π‘) such that the following algebraic Lyapunov equation holds: π΄π (π‘) π (π‘) + π (π‘) π΄ (π‘) = −πΌ, (2) where π1 , π2 are constants, πΌ is the identity matrix, and π(π‘) is bounded. The following generalized Halanay inequality will play a key role in studying the ISS for the system (9). Lemma 2 (generalized Halanay inequality (see [16, 17])). Suppose π€σΈ (π‘) ≤ π (π‘) − πΌ (π‘) π€ (π‘) + π½ (π‘) sup π€ (π) , for π‘ ≥ π‘0 . (3) Here π€(π‘) is a non-negative real-value continuous function, π ≥ 0, π(π‘), πΌ(π‘), and π½(π‘) are continuous with 0 ≤ π(π‘) ≤ π∗ , πΌ(π‘) ≥ πΌ0 > 0, and 0 < π½(π‘) ≤ ππΌ(π‘) for π‘ ≥ π‘0 and 0 ≤ π < 1. Then π€ (π‘) ≤ ∗ β π + πΊπ−π (π‘−π‘0 ) , (1 − π) πΌ0 π‘≥π‘0 (5) Lemma 3. Let π΄(π‘) and π΅(π‘) be π × π matrix-value functions, ](π‘) = (]1 (π‘),]2 (π‘), . . . , ]π (π‘))π , and let Γ(π‘) = (Γ1 (π‘), Γ2 (π‘), . . . , Γπ (π‘))π be vector functions of dimensions π. Assume that (i) π π (π΄(π‘) + π΄π (π‘)) ≤ −π(π‘) < 0 (π = 1, 2, . . . , π), π΅(π‘) is bounded; (ii) −ππ(π‘) + (1 + π)βπ΅(π‘)β + π ≤ 0 with 0 ≤ π < 1; (iii) π(π‘) − βπ΅(π‘)β − 1 ≥ π0∗ > 0; (iv) ]σΈ (π‘) ≤ Γ(π‘) + π΄(π‘)](π‘) + π΅(π‘)supπ‘−π≤π≤π‘ ](π), βΓ(π‘)β ≤ Γ∗ , for π‘ ≥ π‘0 , where supπ‘−π≤π≤π‘ ](π) = (supπ‘−π≤π≤π‘ ]1 (π), supπ‘−π≤π≤π‘ ]2 (π),. . . , supπ‘−π≤π≤π‘ ]π (π))π . Then the following estimate holds β]β ≤ Γ∗ √(1 − π) π0∗ σ΅©σ΅¨ σ΅¨σ΅© ∗ + σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨]π‘0 σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅© π−πΎ (π‘−π‘0 ) , for π‘ ≥ π‘0 , (6) where πΎ∗ is defined as 2πΎ∗ = inf {πΎ (π‘) : πΎ (π‘) − (π (π‘) − βπ΅ (π‘)β − 1) + βπ΅ (π‘)β ππΎ(π‘)π } . (7) Proof. Let π(π‘) = β]β2 = ]π ]. Then π πσΈ (π‘) = ]σΈ ] + ]π ]σΈ ≤ 2]π Γ (π‘) + ]π (π΄(π‘)π + π΄ (π‘)) ] (π‘) + 2]π π΅ (π‘) sup ] (π) ∀π‘ ∈ π½. π‘−π≤π≤π‘ πβ = inf {π (π‘) : π (π‘) − πΌ (π‘) + π½ (π‘) ππ(π‘)π = 0} . π‘ ≥ π‘0 , (4) π‘−π≤π≤π‘ ≤ 2 β] (π‘)β βΓ (π‘)β − π (π‘) β] (π‘)β2 σ΅©σ΅¨ σ΅¨σ΅© + 2 βπ΅ (π‘)β β] (π‘)β σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨]π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© (8) ≤ βΓ (π‘)β2 + β] (π‘)β2 − π (π‘) β] (π‘)β2 σ΅©σ΅¨ σ΅¨σ΅©2 + βπ΅ (π‘)β (β] (π‘)β2 + σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨]π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© ) ≤ βΓ (π‘)β2 − (π (π‘) − βπ΅ (π‘)β − 1) β] (π‘)β2 σ΅©σ΅¨ σ΅¨σ΅©2 + βπ΅ (π‘)β σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨]π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© . Moreover, by the conditions (i)–(iii), the estimate (6) can be derived as a consequence of (3)–(5) and (8). Consider the delay singularly perturbed control systems π₯σΈ (π‘) = π (π‘, π₯ (π‘) , π₯ (π‘ − π) , π¦ (π‘) , π¦ (π‘ − π) , π’ (π‘)) , ππ¦σΈ (π‘) = π (π‘, π₯ (π‘) , π₯ (π‘ − π) , π¦ (π‘) , π’ (π‘)) , π₯ (π‘) = π (π‘) , π¦ (π‘) = π (π‘) , π‘ ≥ 0, 0 < π βͺ 1, π‘ ∈ [−π, 0] , (9) Journal of Applied Mathematics 3 where π‘ ∈ π is the “time,” π₯ ∈ π π and π¦ ∈ π π are the state variables, π’(π‘) ∈ π π is the control input which is locally essentially bounded, π is the singular perturbation parameter, and π is a constant time delay. The sufficiently smooth mapping π : π × π π × π π × π π × π π × π π → π π , π : π ×π π ×π π ×π π ×π π ×π π → π π has bounded derivatives and π(π‘, 0, 0, 0, 0, 0) = π(π‘, 0, 0, 0, 0, 0) = 0. π ∈ π π and π ∈ π π are given vector-functions and the derivative of π exists. Definition 4. The delay singularly perturbed control system (9) is ISS if there exist π π-functions π½1 , π½2 : π ≥0 × π ≥0 → π ≥0 and π -functions πΎ1 , πΎ2 such that, for any initial functions π(π‘), π(π‘) and each essentially bounded input π’(π‘), the solution of (9) satisfy σ΅© σ΅© σ΅© σ΅©σ΅© σ΅©σ΅©π₯ (π‘, π, π, π’, π)σ΅©σ΅©σ΅© ≤ π½1 (π, π‘) + πΎ1 (σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅©) , σ΅© σ΅©σ΅© σ΅© σ΅© σ΅©σ΅©π¦ (π‘, π, π, π’, π)σ΅©σ΅©σ΅© ≤ π½2 (π, π‘) + πΎ2 (σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅©) , From Assumption 5 and Lemma 1, we can easily show that there exist the differentiable positive-definite matrices π1 (π‘) and π2 (π‘) such that π΄π11 (π‘) π1 (π‘) + π1 (π‘) π΄ 11 (π‘) = −πΌπ , (13a) π π΅21 (π‘) π2 (π‘) + π2 (π‘) π΅21 (π‘) = −πΌπ , (13b) where πΌπ , πΌπ are π×π, π×π identity matrices, respectively, [21] shows that Assumption 5 guarantees that Reference, for every π‘ ≥ π‘0 , (13a), (13b) have unique positive-definite solutions π1 (π‘) and π2 (π‘) given by ∞ 0 ∞ (14) π π΅21 (π‘)π π΅21 (π‘)π π2 (π‘) = ∫ π (10) where π₯(π‘, π, π, π’, π), π¦(π‘, π, π, π’, π) are the solutions of (9), π = sup−π≤π‘≤0 βπ(π‘)β + sup−π≤π‘≤0 βπ(π‘)β + sup−π≤π‘≤0 βπσΈ (π‘)β. π π1 (π‘) = ∫ ππ΄ 11 (π‘)π ππ΄ 11 (π‘)π ππ, π 0 ππ, respectively. It follows from the boundness and the positivedefiniteness of π1 (π‘) and π2 (π‘) that there exist positive constants ππ , πΌπ , π½π (π = 1, 2) such that σ΅© σ΅© π1 ≤ σ΅©σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅© ≤ π2 , π = 1, 2, 3. Linear Systems πΌ1 βπ₯β2 ≤ π₯π π1 (π‘) π₯ ≤ π½1 βπ₯β2 , In this section, we are concerned with ISS of the following linear delay singularly perturbed control systems as a special class of (9): σ΅© σ΅©2 σ΅© σ΅©2 πΌ2 σ΅©σ΅©σ΅©π¦σ΅©σ΅©σ΅© ≤ π¦π π2 (π‘) π¦ ≤ π½2 σ΅©σ΅©σ΅©π¦σ΅©σ΅©σ΅© . π₯σΈ = π΄ 11 (π‘) π₯ + π΄ 12 (π‘) π₯π‘ + π΅11 (π‘) π¦ + π΅12 (π‘) π¦π‘ + πΆ1 (π‘) π’ (π‘) , + πΆ2 (π‘) π’ (π‘) , π₯ (π‘) = π (π‘) , σ΅©σ΅¨ σ΅¨σ΅©2 ≤ π1 (π‘) βπ’ (π‘)β2 + π11 (π‘) βπ₯β2 + π12 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π₯π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© σ΅©2 σ΅© σ΅©σ΅¨ σ΅¨ σ΅©2 + π11 (π‘) σ΅©σ΅©σ΅©π¦ − βσ΅©σ΅©σ΅© + π12 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨(π¦ − β)π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© , π‘ ∈ [−π, 0] . Here we let π₯ = π₯(π‘), π¦ = π¦(π‘), π₯π‘ = π₯(π‘ − π), π¦π‘ = π¦(π‘ − π), and π’ = π’(π‘) for simplicity; π΄ 1π (π‘) ∈ π π×π , π΄ 2π (π‘) ∈ π π×π , π΅1π (π‘) ∈ π π×π (π = 1, 2), π΅21 (π‘) ∈ π π×π , πΆ1 (π‘) ∈ π π×π , and πΆ2 (π‘) ∈ π π×π are smooth matrix functions of π‘, and π΅21 (π‘) is nonsingular for every π‘. Now, we introduce some assumptions. Assumption 5. There exist positive constants π1 and π2 such that, for for all π‘ ∈ π½ = [0, +∞), σ΅© σ΅©σ΅© σ΅©σ΅©σ΅©π΄σΈ (π‘)σ΅©σ΅©σ΅© ≤ π , σ΅©σ΅©π΄ 11 (π‘)σ΅©σ΅©σ΅© ≤ π2 , σ΅©σ΅© 11 σ΅©σ΅© 2 σ΅© σ΅© σ΅©σ΅© σ΅©σ΅©π΅σΈ (π‘)σ΅©σ΅©σ΅© ≤ π , Re π (π΅21 (π‘)) ≤ −π1 , σ΅©σ΅©π΅21 (π‘)σ΅©σ΅©σ΅© ≤ π2 , σ΅©σ΅© 21 σ΅©σ΅© 2 σ΅©σ΅© σ΅©σ΅© −1 σ΅©σ΅© σ΅©σ΅© −1 σ΅©σ΅©π΅21 (π‘)σ΅©σ΅© ≤ c2 , σ΅©σ΅©π΅21 (π‘) π΄ 21 (π‘)σ΅©σ΅© ≤ π2 , σ΅© σ΅© σ΅© σ΅© σ΅©σ΅© σ΅© σ΅©σ΅© −1 σ΅©σ΅© −1 σ΅©σ΅©π΅21 (π‘) π΄ 22 (π‘)σ΅©σ΅© ≤ π2 , σ΅©σ΅©π΅21 (π‘) πΆ2 (π‘)σ΅©σ΅©σ΅© ≤ π2 . σ΅© σ΅© σ΅© σ΅© (12) Re π (π΄ 11 (π‘)) ≤ −π1 , + π₯π πσΈ 1 (π‘) π₯ (11) 0 < π βͺ 1, π¦ (π‘) = π (π‘) , Assumption 6. There exist bounded functions πππ (π‘), πππ (π‘), and ππ (π‘) (π, π = 1, 2) such that 2π₯π π1 (π‘) (π΄ 12 (π‘) π₯π‘ + π΅11 (π‘) π¦ + π΅12 (π‘) π¦π‘ + πΆ1 (π‘) π’ (π‘)) π‘ ≥ 0, ππ¦σΈ = π΄ 21 (π‘) π₯ + π΄ 22 (π‘) π₯π‘ + π΅21 (π‘) π¦ (15) π π − 2(π¦ − β) π2 (π‘) βσΈ + (π¦ − β) π2σΈ (π‘) (π¦ − β) σ΅©σ΅¨ σ΅¨σ΅©2 ≤ π2 (π‘) βπ’ (π‘)β2 + π21 (π‘) βπ₯β2 + π22 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π₯π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© σ΅©2 σ΅© σ΅©σ΅¨ σ΅¨ σ΅©2 + π21 (π‘) σ΅©σ΅©σ΅©π¦ − βσ΅©σ΅©σ΅© + π22 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨(π¦ − β)π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© , (16) where −π΅−1 (π‘) { { 21 β = { × [π΄ 21 (π‘) π₯ + π΄ 22 (π‘) π₯π‘ + πΆ2 (π‘) π’ (π‘)] , π‘ ≥ 0 { −1 σΈ π‘ ∈ [−π, 0] . {π (π‘) − ππ΅21 (π‘) π (π‘) , (17) Assumption 7. (1) There exists a positive number π0 such that Μ is an π-matrix; −π΄(π‘) Μ +π΄ Μπ (π‘)) ≤ −π(π‘) < 0 (π = 1, 2); (2) π π (π΄(π‘) Μ (3) −ππ(π‘) + (1 + π)βπ΅(π‘)β + π ≤ 0 with 0 ≤ π < 1; ∗ Μ (4) π(π‘) − βπ΅(π‘)β − 1 ≥ π0 > 0, 4 Journal of Applied Mathematics π 1 π π = (π¦ − β) [π΅21 (π‘) π2 (π‘) + π2 (π‘) π΅21 (π‘)] π where 1 − π11 (π‘) π11 (π‘) π½1 πΌ2 Μ (π‘) = ( π΄ ), 1 − π0 π21 (π‘) π21 (π‘) − πΌ1 π0 π½2 π π12 (π‘) π12 (π‘) πΌ πΌ2 π΅Μ (π‘) = ( 1 ). π22 (π‘) π22 (π‘) πΌ1 πΌ2 π − 2(π¦ − β) (π‘) βσΈ + (π¦ − β) π2σΈ (π‘) (π¦ − β) − (18) Theorem 8. If Assumptions 5–7 hold, then the delay singularly perturbed control system (11) is input-to-state stable for π ∈ (0, π0 ]. Proof. Let π(π‘, π₯) = π₯π π1 (π‘)π₯, π(π‘, π₯, π¦) = (π¦ − β)π π2 (π‘)(π¦ − β). For the derivative of π(π‘, π₯) along the trajectory of (11), we have 1 σ΅©2 σ΅© ≤ − (1 − ππ21 (π‘)) σ΅©σ΅©σ΅©π¦ − βσ΅©σ΅©σ΅© + π21 (π‘) βπ₯β2 π σ΅©σ΅¨ σ΅¨σ΅©2 σ΅©σ΅¨ σ΅¨σ΅©2 + π22 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π₯π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + π22 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨(π¦ − β)π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + π2 (π‘) βπ’β2 . (20) From (1) of Assumption 7, we can derive (1 − π0 π21 (π‘))/ π0 π½2 > 0 and the following inequalities for π ∈ (0, π0 ] and π‘ ≥ 0: πσΈ ≤ − + πσΈ (π‘, π₯) = [π΄ 11 (π‘) π₯ + π΄ 12 (π‘) π₯π‘ + π΅11 (π‘) π¦ π +π΅12 (π‘) π¦π‘ + πΆ1 (π‘) π’] π1 (π‘) π₯ + π₯π π1 (π‘) [π΄ 11 (π‘) π₯ + π΄ 12 (π‘) π₯π‘ πσΈ ≤ π12 (π‘) σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© π12 (π‘) σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© 2 σ΅©σ΅¨π σ΅¨σ΅© + σ΅©σ΅¨π σ΅¨σ΅© + π (π‘) βπ’β , πΌ1 σ΅©σ΅¨ π‘ σ΅¨σ΅© πΌ2 σ΅©σ΅¨ π‘ σ΅¨σ΅© 1 π21 (π‘) 1 − ππ21 (π‘) π (π‘) σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© π− π + 22 σ΅©σ΅¨π σ΅¨σ΅© πΌ1 ππ½2 πΌ1 σ΅©σ΅¨ π‘ σ΅¨σ΅© (21) π (π‘) σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© 2 + 22 σ΅©σ΅¨π σ΅¨σ΅© + π (π‘) βπ’β πΌ2 σ΅©σ΅¨ π‘ σ΅¨σ΅© 2 +π΅11 (π‘) π¦ + π΅12 (π‘) π¦π‘ + πΆ1 (π‘) π’] + π₯π π1σΈ (π‘) π₯ = π₯π (π΄π11 (π‘) π1 (π‘) + π1 (π‘) π΄ 11 (π‘)) π₯ 1 − π11 (π‘) π (π‘) π + 11 π π½1 πΌ2 ≤ + 2π₯π π1 (π‘) [π΄ 12 (π‘) π₯π‘ + π΅11 (π‘) π¦ 1 − π0 π21 (π‘) π21 (π‘) π (π‘) σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© π− π + 22 σ΅©σ΅¨π σ΅¨σ΅© πΌ1 π0 π½2 πΌ1 σ΅©σ΅¨ π‘ σ΅¨σ΅© + +π΅12 (π‘) π¦π‘ + πΆ1 (π‘) π’] π22 (π‘) σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© 2 σ΅©σ΅¨π σ΅¨σ΅© + π (π‘) βπ’β . πΌ2 σ΅©σ΅¨ π‘ σ΅¨σ΅© 2 + π₯π π1σΈ (π‘) π₯ σ΅©σ΅¨ σ΅¨σ΅©2 ≤ − (1 − π11 (π‘)) βπ₯β2 + π12 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π₯π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© σ΅©2 σ΅© σ΅©σ΅¨ σ΅¨σ΅©2 + π11 (π‘) σ΅©σ΅©σ΅©π¦ − βσ΅©σ΅©σ΅© +π12 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨(π¦ − β)π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© +π1 (π‘) βπ’β2 . (19) For the derivative of π(π‘, π₯, π¦) along the trajectory of (11), we have π 1 = [ (π΄ 21 (π‘) π₯ + π΄ 22 (π‘) π₯π‘ + π΅21 (π‘) π¦ + πΆ2 (π‘) π’) − βσΈ ] π π × π2 (π‘) (π¦ − β) + (π¦ − β) π2 (π‘) 1 × [ (π΄ 21 (π‘) π₯ + π΄ 22 (π‘) π₯π‘ + π΅21 (π‘) π¦ + πΆ2 (π‘) π’) − βσΈ ] π + (π¦ − σ΅© σ΅©2 π0∗ σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© −2ππ‘ σ΅¨ σ΅© σ΅¨ σ΅© σ΅© σ΅© σ΅¨ σ΅¨ π ≤ (σ΅©σ΅©σ΅¨σ΅¨ππ‘0 σ΅¨σ΅¨σ΅©σ΅© + σ΅©σ΅©σ΅¨σ΅¨ππ‘0 σ΅¨σ΅¨σ΅©σ΅©) π + , √(1 − π) π0∗ σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© π ≤ (σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨ππ‘0 σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨ππ‘0 σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅©) π−2ππ‘ + πσΈ (π‘, π₯, π¦) π β) π2σΈ It follows from Lemma 3 that there exist positive constants π, π0∗ , and π0∗ such that (π‘) (π¦ − β) σ΅© σ΅©2 π0∗ σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© √(1 − π) π0∗ (22) , where β(π1 (π‘), π2 (π‘))π β ≤ π0∗ and π is defined by σ΅© σ΅© σ΅© σ΅© 4π = inf {π (π‘) : π (π‘) − (π (π‘) − σ΅©σ΅©σ΅©σ΅©π΅Μ (π‘)σ΅©σ΅©σ΅©σ΅© − 1) + σ΅©σ΅©σ΅©σ΅©π΅Μ (π‘)σ΅©σ΅©σ΅©σ΅© ππ(π‘)π } . π‘≥0 (23) Journal of Applied Mathematics 5 By the definition of π(π‘, π₯) and the positive-definiteness of π1 (π‘), we have πΌ1 βπ₯β2 ≤ π σ΅© σ΅©2 π∗ σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© ≤ (σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨ππ‘0 σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨ππ‘0 σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅©) π−2ππ‘ + 0 σ΅© √(1 − π) π0∗ σ΅© σ΅©2 π0∗ σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© σ΅© σ΅©2 π0∗ σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© σ΅©σ΅¨ σ΅¨σ΅©2 σ΅©σ΅¨ σ΅¨σ΅©2 σ΅©σ΅¨ σ΅¨σ΅©2 ≤ (π½1 σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π₯0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + 2π½2 σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π¦0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + π½2 π02 π22 σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨π0σΈ σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅© ) π−2ππ‘ + √(1 − π) π0∗ π₯ (π‘) = π (π‘) , π‘ ∈ [−π, 0] , π¦ (π‘) = π (π‘) , (28) Re π (π΄ (π‘)) ≤ −π1 , βπ΄ (π‘)β ≤ π2 , Re π (π΅ (π‘)) ≤ −π1 , βπ΅ (π‘)β ≤ π2 , = π0∗ /√(1 − π)π0∗ πΌ1 . Moreover, Thus, (25) and the inequality (26) π΄π (π‘) π1 (π‘) + π1 (π‘) π΄ (π‘) = −πΌπ , −1/2 1/2 σ΅©σ΅© σ΅©σ΅© σ΅©σ΅©π¦σ΅©σ΅© ≤ βββ + (πΌ2 ) π σ΅© σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© ≤ 2π2 (πΎ1 (σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨π0σΈ σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅©) π−π(π‘−π) + πΎ2 σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅©) −1/2 σ΅© σ΅© + π2 σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© + (πΌ2 ) π1/2 πΌ1 σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© ) πΎ1 (σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨π0σΈ σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅©) π−π(π‘−π) πΌ2 (30) where πΌπ , πΌπ are π × π, π × π identity matrices, respectively. It follows from the boundness and the positivedefiniteness of π1 (π‘) and π2 (π‘) that there exist positive constants ππ , πΌπ , and π½π (π = 1, 2) such that σ΅© σ΅© π1 ≤ σ΅©σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅© ≤ π2 , imply that π = 1, 2, πΌ1 βπ₯β2 ≤ π₯π π1 (π‘) π₯ ≤ π½1 βπ₯β2 , (31) σ΅© σ΅©2 σ΅© σ΅©2 πΌ2 σ΅©σ΅©σ΅©π¦σ΅©σ΅©σ΅© ≤ π¦π π2 (π‘) π¦ ≤ π½2 σ΅©σ΅©σ΅©π¦σ΅©σ΅©σ΅© . Assumption 10. There exist bounded functions πππ (π‘), πππ (π‘), and ππ (π‘) (π, π = 1, 2) such that 2π₯π π1 (π‘) π (π‘, π₯, π₯π‘ , π¦, π¦π‘ , π’) + π₯π π1σΈ (π‘) π₯ σ΅©σ΅¨ σ΅¨σ΅©2 ≤ π1 (π‘) βπ’β2 + π11 (π‘) βπ₯β2 + π12 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π₯π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© πΌ σ΅© σ΅© + ((2π2 + √ 1 ) πΎ2 + π2 ) σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© πΌ2 σ΅© σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© = πΎ1∗ (σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨π0σΈ σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅©) π−π(π‘−π) + πΎ2∗ σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© , If Assumption 9 holds, then there exist the differentiable positive-definite matrices π1 (π‘) and π2 (π‘) such that π΅π (π‘) π2 (π‘) + π2 (π‘) π΅ (π‘) = −πΌπ , σ΅© σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© βπ₯β ≤ πΎ1 (σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨π0σΈ σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅©) π−ππ‘ + πΎ2 σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© . (25) −1/2 1/2 σ΅© σ΅© σ΅©σ΅© σ΅©σ΅© σ΅©σ΅©π¦σ΅©σ΅© − βββ ≤ σ΅©σ΅©σ΅©(π¦ − β) (π‘)σ΅©σ΅©σ΅© ≤ (πΌ2 ) π σ΅©σ΅© σΈ σ΅©σ΅© σ΅©σ΅©π΄ (π‘)σ΅©σ΅© ≤ π2 , σ΅© σ΅© σ΅©σ΅© σΈ σ΅©σ΅© σ΅©σ΅©π΅ (π‘)σ΅©σ΅© ≤ π2 . σ΅© σ΅© (29) = max{π½1 /πΌ1 , 2π½2 /πΌ1 , π½2 π02 π22 /πΌ1 } and πΎ22 ≤ (2π2 + √ 0 < π βͺ 1, , σ΅© σ΅©2 σ΅©σ΅¨ σ΅¨σ΅©2 σ΅©σ΅¨ σ΅¨σ΅©2 σ΅©σ΅¨ σ΅¨σ΅©2 βπ₯β2 ≤ πΎ12 (σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨π0σΈ σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅© ) π−2ππ‘ +πΎ22 σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© , (24) where πΎ12 ππ¦σΈ = π΅ (π‘) π¦ + π (π‘, π₯, π₯π‘ , π’) , Assumption 9. There exist positive constants π1 , π2 for all π‘ ∈ π½ such that √(1 − π) π0∗ σ΅© σ΅©2 π0∗ σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© π‘ ≥ 0, where π΄(π‘) ∈ π π×π , π΅(π‘) ∈ π π×π , π(π‘, 0, 0, 0, 0, 0) = 0, and π(π‘, 0, 0, 0) = 0. Assume that (28) has a unique equilibrium at the origin and the functions π and π are smooth enough and the derivative of π exists. √(1 − π) π0∗ σ΅©σ΅¨ σ΅¨σ΅©2 σ΅©σ΅¨ σ΅¨σ΅©2 σ΅©σ΅¨ σ΅¨σ΅©2 ≤ (π½1 σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π₯0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + π½2 σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π¦0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + π½2 σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨β0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© ) π−2ππ‘ + In this section, we are concerned with ISS of the following nonlinear delay singularly perturbed control systems as a special class of (9): π₯σΈ = π΄ (π‘) π₯ + π (π‘, π₯, π₯π‘ , π¦, π¦π‘ , π’) , σ΅©σ΅¨ σ΅¨σ΅©2 σ΅©σ΅¨ σ΅¨σ΅©2 ≤ (π½1 σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π₯0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + π½2 σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨(π¦ − β)0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© ) π−2ππ‘ + 4. Nonlinear Systems σ΅©2 σ΅© σ΅©σ΅¨ σ΅¨σ΅©2 + π11 (π‘) σ΅©σ΅©σ΅©π¦ − βσ΅©σ΅©σ΅© + π11 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨(π¦ − β)π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© , π (27) where πΎ1∗ = (2π2 + √πΌ1 /πΌ2 )πΎ1 , πΎ2∗ = (2π2 + √πΌ1 /πΌ2 )πΎ2 + π2 . The proof is complete. π − 2(π¦ − β) π2 (π‘) βσΈ + (π¦ − β) π2σΈ (π‘) (π¦ − β) σ΅©σ΅¨ σ΅¨σ΅©2 ≤ π2 (π‘) βπ’β2 + π21 (π‘) βπ₯β2 + π22 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π₯π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© σ΅©2 σ΅© σ΅©σ΅¨ σ΅¨σ΅©2 + π21 (π‘) σ΅©σ΅©σ΅©π¦ − βσ΅©σ΅©σ΅© + π21 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨(π¦ − β)π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© , (32) 6 Journal of Applied Mathematics For the derivative of π(π‘, π₯, π¦) along the trajectory of (28), we have where −π΅−1 (π‘) π (π‘, π₯, π₯π‘ , π’ (π‘)) , π‘ ≥ 0 β={ π‘ ∈ [−π, 0] . π (π‘) − ππ΅−1 (π‘) πσΈ (π‘) , (33) π 1 = [ (π΅ (π‘) π¦ + π (π‘, π₯, π₯π‘ , π’)) − βσΈ ] π2 (π‘) (π¦ − β) π Assumption 11. (1) There exist a positive number π0 such that Μ is an π-matrix; −π΄(π‘) Μ +π΄ Μπ (π‘)) ≤ −π(π‘) < 0 (π = 1, 2); (2) π π (π΄(π‘) 1 π + (π¦ − β) π2 (π‘) [ (π΅ (π‘) π¦ + π (π‘, π₯, π₯π‘ , π’)) − βσΈ ] π π + (π¦ − β) π2σΈ (π‘) (π¦ − β) π 1 π = (π¦ − β) [π΅π (π‘) π2 (π‘) + π2 (π‘) π΅ (π‘)] (π¦ − β) π Μ (3) −ππ(π‘) + (1 + π)βπ΅(π‘)β + π ≤ 0 with 0 ≤ π < 1; Μ (4) π(π‘) − βπ΅(π‘)β − 1 ≥ π0∗ > 0, π π − 2(π¦ − β) π2 (π‘) βσΈ + (π¦ − β) π2σΈ (π‘) (π¦ − β) 1 σ΅©2 σ΅©σ΅¨ σ΅¨σ΅©2 σ΅© ≤ − (1 − ππ21 (π‘)) σ΅©σ΅©σ΅©π¦ − βσ΅©σ΅©σ΅© + π21 (π‘) βπ₯β2 + π22 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π₯π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© π σ΅©σ΅¨ σ΅¨σ΅©2 + π22 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨(π¦ − β)π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + π2 (π‘) βπ’β2 . (36) where − Μ π΄ (π‘) = ( πσΈ (π‘, π₯, π¦) 1 − π11 (π‘) π11 (π‘) π½1 πΌ2 ), 1 − π0 π21 (π‘) π21 (π‘) − πΌ1 π0 π½2 π12 (π‘) π12 (π‘) πΌ πΌ2 π΅Μ (π‘) = ( 1 ). π22 (π‘) π22 (π‘) πΌ1 πΌ2 (34) From (1) of Assumption 11, we can derive (1 − π0 π21 (π‘))/ π0 π½2 > 0 and the following inequalities for π ∈ (0, π0 ]: πσΈ ≤ − + Theorem 12. If Assumptions 9–11 hold, then the delay singularly perturbed control system (28) is input-to-state stable for π ∈ (0, π0 ]. πσΈ ≤ Proof. Let π(π‘, π₯) = π₯ π1 (π‘)π₯, π(π‘, π₯, π¦) = (π¦ − β) π2 (π‘)(π¦ − β). For the derivative of π(π‘, π₯) along the trajectory of (28), we have πσΈ (π‘, π₯) π12 (π‘) σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© 2 σ΅©σ΅¨π σ΅¨σ΅© + π (π‘) βπ’β , πΌ2 σ΅©σ΅¨ π‘ σ΅¨σ΅© 1 π21 (π‘) 1 − ππ21 (π‘) π (π‘) σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© π− π + 22 σ΅©σ΅¨π σ΅¨σ΅© πΌ1 ππ½2 πΌ1 σ΅©σ΅¨ π‘ σ΅¨σ΅© π (π‘) σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© 2 + 22 σ΅©σ΅¨π σ΅¨σ΅© + π (π‘) βπ’β πΌ2 σ΅©σ΅¨ π‘ σ΅¨σ΅© 2 π π 1 − π11 (π‘) π (π‘) π (π‘) σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© π + 11 π + 12 σ΅©σ΅¨π σ΅¨σ΅© π½1 πΌ2 πΌ1 σ΅©σ΅¨ π‘ σ΅¨σ΅© ≤ (37) 1 − π0 π21 (π‘) π21 (π‘) π (π‘) σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© π− π + 22 σ΅©σ΅¨π σ΅¨σ΅© πΌ1 π0 π½2 πΌ1 σ΅©σ΅¨ π‘ σ΅¨σ΅© + π22 (π‘) σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© 2 σ΅©σ΅¨π σ΅¨σ΅© + π (π‘) βπ’β . πΌ2 σ΅©σ΅¨ π‘ σ΅¨σ΅© 2 π = [π΄ (π‘) π₯ + π (π‘, π₯, π₯π‘ , π¦, π¦π‘ , π’)] π1 (π‘) π₯ π + π₯ π1 (π‘) [π΄ (π‘) π₯ + π (π‘, π₯, π₯π‘ , π¦, π¦π‘ , π’)] + π₯π π1σΈ (π‘) π₯ = π₯π (π΄π (π‘) π1 (π‘) + π1 (π‘) π΄ (π‘)) π₯ + 2π₯π π1 (π‘) π (π‘, π₯, π₯π‘ , π¦, π¦π‘ , π’) + π₯π π1σΈ (π‘) π₯ σ΅©σ΅¨ σ΅¨σ΅©2 ≤ − (1 − π11 (π‘)) βπ₯β2 + π12 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π₯π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© σ΅©2 σ΅© σ΅©σ΅¨ σ΅¨σ΅©2 + π11 (π‘) σ΅©σ΅©σ΅©π¦ − βσ΅©σ΅©σ΅© + π12 (π‘) σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨(π¦ − β)π‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + π1 (π‘) βπ’β2 . (35) It follows from Lemma 3 that there exist positive constants π, π0∗ , and π0∗ such that σ΅© σ΅©2 π∗ σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© π ≤ (σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨ππ‘0 σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨ππ‘0 σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅©) π−2ππ‘ + 0 σ΅© , √(1 − π) π0∗ σ΅© σ΅©2 π∗ σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© π ≤ (σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨ππ‘0 σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨ππ‘0 σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅©) π−2ππ‘ + 0 σ΅© , √(1 − π) π0∗ where β(π1 (π‘), π2 (π‘))π β ≤ π0∗ and π is defined as in (23). (38) Journal of Applied Mathematics 7 By the definitions of π(π‘, π₯), π(π‘, π₯, π¦), the positivedefiniteness of π1 (π‘), π2 (π‘), and the similar proof process to that of Theorem 8, we can obtain σ΅© σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© βπ₯β ≤ πΎ1 (σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨π0σΈ σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅©) π−ππ‘ + πΎ2 σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© , σ΅©σ΅© σ΅©σ΅© σ΅© σ΅© ∗ σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σΈ σ΅¨σ΅© −π(π‘−π) + πΎ2∗ σ΅©σ΅©σ΅©π’[0,π‘) σ΅©σ΅©σ΅© , σ΅©σ΅©π¦σ΅©σ΅© ≤ πΎ1 (σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨σ΅¨π0 σ΅¨σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅©σ΅©) π (39) where πΎ1 √max{π½1 /πΌ1 , 2π½2 /πΌ1 , π½2 π02 π22 /πΌ1 }, πΎ2 = = √ π0∗ /√(1 − π)π0∗ πΌ1 , πΎ1∗ = (2π2 + √πΌ1 /πΌ2 )πΎ1 and πΎ2∗ = (2π2 + √πΌ1 /πΌ2 )πΎ2 + π2 . The proof is complete. Example 2. Consider the following nonlinear delay system as an application of Theorem 12: π₯σΈ (π‘) = −15π₯ (π‘)+5 ln (1+π₯2 (π‘ − π))+sin (π¦ (π‘))+π’ (π‘) , ππ¦σΈ (π‘) = 2π₯ (π‘ − π) − 6π¦ (π‘) . (44) Let π = π₯2 /30, π = (π¦ − β)2 /12, and β = π₯(π‘ − π)/3. Then πσΈ (π‘, π₯) = ≤ πσΈ (π‘, π₯, π¦) = 5. Examples 1 π₯ (−15π₯ + 5 ln (1 + π₯π‘2 ) + sin π¦ + π’) 15 −68 2 16 σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© 1 2 π+ π+ σ΅©σ΅¨π σ΅¨σ΅© + βπ’β , 3 5 3 σ΅©σ΅¨ π‘ σ΅¨σ΅© 30 1 1 (π¦ − β) ( (2π₯π‘ − 6π¦) − βσΈ ) 6 π Example 1. Consider the following linear delay system as an application of Theorem 8: ≤ (− π₯σΈ (π‘) = −5π₯ (π‘) + π¦ (π‘ − π) + π’ (π‘) , + ππ¦σΈ (π‘) = 3π₯ (π‘) − 5π¦ (π‘) . (40) 1 πσΈ (π‘, π₯) = π₯ (−5π₯ + π¦π‘ + π’) 5 37 3 σ΅©σ΅¨ σ΅¨σ΅© σ΅©σ΅¨ σ΅¨σ΅© 1 ≤ − π + σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨ππ‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + σ΅©σ΅©σ΅©σ΅¨σ΅¨σ΅¨ππ‘ σ΅¨σ΅¨σ΅¨σ΅©σ΅©σ΅© + βπ’β2 , 5 5 5 πσΈ (π‘, π₯, π¦) = + Μ (π‘) = ( π΄ (41) 10 114 + )π π 25 9 σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© 3 σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© 3 2 σ΅©σ΅¨π σ΅¨σ΅© σ΅©σ΅¨π σ΅¨σ΅© + βπ’β . 25 σ΅©σ΅¨ π‘ σ΅¨σ΅© 5 σ΅©σ΅¨ π‘ σ΅¨σ΅© 50 (42) Μ (π‘) = ( π΄ 2 5 68 3 0 − 12 67 ) , + π 9 16 0 3 π΅Μ (π‘) = ( 61 1 ) . 9 3 (46) If we require that the constant π0 satisfies −12/π + 67/9 ≤ −68/3; that is, π0 ≤ 108/271, then, we can take π0 = 108/271 such that it is easy to show that the conditions in Assumptions 9–11 will be satisfied for any π ∈ (0, π0 ]. Moreover, by Theorem 12, the system (44) is ISS for π ∈ (0, π0 ]. 6. Conclusion So we obtain the matrices − 1 σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© 1 2 σ΅©σ΅¨π σ΅¨σ΅© + βπ’β . 3 σ΅©σ΅¨ π‘ σ΅¨σ΅© 36 So we obtain the matrices 1 1 3 (π¦ − β) ( (3π₯ − 5π¦) − (−5π₯ + π¦π‘ + π’)) 5 π 5 ≤ 3π + (− 12 67 61 σ΅©σ΅©σ΅¨σ΅¨ σ΅¨σ΅¨σ΅©σ΅© + )π + σ΅©σ΅¨π σ΅¨σ΅© π 9 9 σ΅©σ΅¨ π‘ σ΅¨σ΅© − Let π = π₯2 /10, π = (π¦ − β)2 /10, β = 3π₯(π‘)/5. Then (45) 37 5 3 0 − 10 114 ) , + π 25 3 1 5 π΅Μ (π‘) = ( 9 3 ) . 25 5 (43) If we require that the constant π0 satisfies −10/π0 + 114/25 ≤ −37/5; that is, π0 ≤ 250/299, then, we can take π0 = 250/299 such that it is easy to show that the conditions in Assumptions 5–7 will be satisfied for any π ∈ (0, π0 ]. Moreover, by Theorem 8, the system (40) is ISS for π ∈ (0, π0 ]. In this paper, we have studied the input-to-state stability of two classes of the linear and nonlinear delay singularly perturbed control systems. The generalized Halanay inequality and the Lyapunov function play important roles in obtaining the stability results. The sufficient conditions of input-to-state stability for delay singularly perturbed control systems are given. Acknowledgment This work is supported by projects NSF of China (11126329, 11271311, 11201510), NSF of Hunan Province (09JJ3002), Projects Board of Education of Chongqing City (KJ121110). The authors express their sincere thanks to the referees for their useful comments and suggestions, which led to improvements of the presentation. 8 References [1] E. D. Sontag, “Smooth stabilization implies coprime factorization,” IEEE Transactions on Automatic Control, vol. 34, no. 4, pp. 435–443, 1989. [2] A. R. Teel, L. Moreau, and D. NesΜicΜ, “A unified framework for input-to-state stability in systems with two time scales,” IEEE Transactions on Automatic Control, vol. 48, no. 9, pp. 1526–1544, 2003. [3] D. Kazakos and J. Tsinias, “The input to state stability condition and global stabilization of discrete-time systems,” IEEE Transactions on Automatic Control, vol. 39, no. 10, pp. 2111–2113, 1994. [4] E. D. Sontag, “Further facts about input to state stabilization,” IEElE Transactions on Automatic Control, vol. 35, no. 4, pp. 473– 476, 1990. [5] E. D. Sontag and Y. Wang, “New characterizations of input-tostate stability,” IEEE Transactions on Automatic Control, vol. 41, no. 9, pp. 1283–1294, 1996. [6] E. D. Sontag, “Input-to-state stability: basic concepts and results,” in Nonlinear and Optimal Control Theory, P. Nistri and G. Stefani, Eds., pp. 163–220, Springer, Berlin, Germany, 2007. [7] E. D. Sontag, Mathematical Control Theory Deterministic FiniteDimensional Systems, vol. 6, Springer, New York, NY, USA, 2nd edition, 1998. [8] G.-D. Hu and M. Liu, “Input-to-state stability of Runge-Kutta methods for nonlinear control systems,” Journal of Computational and Applied Mathematics, vol. 205, no. 1, pp. 633–639, 2007. [9] I. Karafyllis and J. Tsinias, “Nonuniform in time input-to-state stability and the small-gain theorem,” IEEE Transactions on Automatic Control, vol. 49, no. 2, pp. 196–216, 2004. [10] N. Yeganefar, P. Pepe, and M. Dambrine, “Input-to-state stability of time-delay systems: a link with exponential stability,” IEEE Transactions on Automatic Control, vol. 53, no. 6, pp. 1526–1531, 2008. [11] P. D. Christofides and A. R. Teel, “Singular perturbations and input-to-state stability,” IEEE Transactions on Automatic Control, vol. 41, no. 11, pp. 1645–1650, 1996. [12] Z. -P. Jing, E. Sontag, and Y. Wang, “Input-to-state stablility for discrete-time nonlinear control systems,” Automatica, vol. 37, pp. 857–869, 1999. [13] A. Saberi and H. Khalil, “Quadratic-type Lyapunov functions for singularly perturbed systems,” IEEE Transactions on Automatic Control, vol. 29, no. 6, pp. 542–550, 1984. [14] M. Corless and L. Glielmo, “On the exponential stability of singularly perturbed systems,” SIAM Journal on Control and Optimization, vol. 30, no. 6, pp. 1338–1360, 1992. [15] X. Liu, X. Shen, and Y. Zhang, “Exponential stability of singularly perturbed systems with time delay,” Applicable Analysis, vol. 82, no. 2, pp. 117–130, 2003. [16] H.-J. Tian, “Dissipativity and exponential stability of π-methods for singularly perturbed delay differential equations with a bounded lag,” Journal of Computational Mathematics, vol. 21, no. 6, pp. 715–726, 2003. [17] H. J. Tian, “The exponential asymptotic stability of singularly perturbed delay differential equations with a bounded lag,” Journal of Mathematical Analysis and Applications, vol. 270, no. 1, pp. 143–149, 2002. [18] Y. X. Yu, “Input-to-state stablility of one-leg methods for nonlinear control systems,” Journal of System Simulation, vol. 20, no. 1, pp. 19–20, 2008. Journal of Applied Mathematics [19] Y. X. Yu and X. Z. Tian, “Input-to-state stablility of muti-step Runge-Kutta methods for nonlinear control systems,” Journal of System Simulation, vol. 6, no. 2, pp. 1573–1574, 2008, vol. 37, pp. 857–869, 2001. [20] P. V. Kokotovic, H. K. Khalil, and J. Orelly, Singular Perturbation Methods in Control: Analysis and Design, Academic Press, London, UK, 1986. [21] X. X. Liao, Theory Methods and Application of Stability, Huazhong University of Science and Technology Press, Wuhan, China, 1999. Advances in Operations Research Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Advances in Decision Sciences Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Mathematical Problems in Engineering Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Journal of Algebra Hindawi Publishing Corporation http://www.hindawi.com Probability and Statistics Volume 2014 The Scientific World Journal Hindawi Publishing Corporation http://www.hindawi.com Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 International Journal of Differential Equations Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Volume 2014 Submit your manuscripts at http://www.hindawi.com International Journal of Advances in Combinatorics Hindawi Publishing Corporation http://www.hindawi.com Mathematical Physics Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Journal of Complex Analysis Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 International Journal of Mathematics and Mathematical Sciences Journal of Hindawi Publishing Corporation http://www.hindawi.com Stochastic Analysis Abstract and Applied Analysis Hindawi Publishing Corporation http://www.hindawi.com Hindawi Publishing Corporation http://www.hindawi.com International Journal of Mathematics Volume 2014 Volume 2014 Discrete Dynamics in Nature and Society Volume 2014 Volume 2014 Journal of Journal of Discrete Mathematics Journal of Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Applied Mathematics Journal of Function Spaces Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Optimization Hindawi Publishing Corporation http://www.hindawi.com Volume 2014 Hindawi Publishing Corporation http://www.hindawi.com Volume 2014