Hindawi Publishing Corporation Advances in Mathematical Physics Volume 2016, Article ID 4619450, 6 pages http://dx.doi.org/10.1155/2016/4619450 Research Article The Effect of Initial State Error for Nonlinear Systems with Delay via Iterative Learning Control Zhang Qunli Department of Mathematics, Heze University, Heze, Shandong 274015, China Correspondence should be addressed to Zhang Qunli; [email protected] Received 6 February 2016; Accepted 23 March 2016 Academic Editor: Ming Mei Copyright © 2016 Zhang Qunli. 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. An iterative learning control problem for nonlinear systems with delays is studied in detail in this paper. By introducing the π-norm and being inspired by retarded Gronwall-like inequality, the novel sufficient conditions for robust convergence of the tracking error, whose initial states are not zero, with time delays are obtained. Finally, simulation example is given to illustrate the effectiveness of the proposed method. 1. Introduction Since iterative learning control is proposed by Arimoto et al. in 1984 (see [1]), this feedforward control approach has become a major research area in recent years. Iterative learning control, which belongs to the intelligent control methodology, is an approach for fully utilizing the previous control information and improving the transient performance of studied systems that is suitable for repetitive movements. Its goal is to achieve full range of tracking tasks on finite interval (see [2β14]). In practice, the control problem of systems with delays has always been an interesting research, since time delay can be often encountered in a wide range, such as aircraft systems, turbojet engines, microwave oscillators, nuclear reactors, and chemical processes. The existence of time delay in a system may degrade the control performance and even at worst may become a source of instability. Stabilization problem of control systems with delay has received much attention for several decades and some research results have been reported in the literature (see [3, 11, 13, 15β23]). However, only a few results are available for nonlinear systems, combining with the iterative learning control items, with time delays [11, 24β 26]. In this paper, under the case that the πth iterative state vector π₯π (π‘) is different from the (π+1)th iterative state vector π₯π+1 (π‘), that is, π₯π+1 (π‘) β π₯π (π‘) =ΜΈ 0, the iterative learning controller of nonlinear time-delayed systems is designed by using π-norm and retarded Gronwall-like inequality. Before ending this section, it is worth pointing out the main contributions of this paper as follows. (1) The iterative learning control problem for nonlinear systems with delays is investigated. That is, we consider the system π₯Μ π (π‘) = π (π‘, π₯π (π‘)) + π (π‘, π₯π (π‘ β π)) + π’π (π‘) , (1) which is different from the mentioned system π₯Μ π (π‘) = π (π‘, π₯π (π‘)) + π’π (π‘) (2) in past literature. (2) Based on retarded Gronwall-like inequality and the convergence of tracking error ππ (π‘) = π¦π (π‘) β π¦π (π‘), the practical output π¦π (π‘) is determinate by the previous iterative learning control information π₯π (π‘), π’π (π‘), ππ,β (π‘). 2. Preliminaries Throughout this paper, the 2-norm for the π-dimensional vector π₯ = (π₯1 , π₯2 , . . . , π₯π )π is defined as βπ₯β = (βππ=1 π₯π2 )1/2 , while the π-norm for a function is defined as β β βπ = supπ‘β[0,π] {πβππ‘ β β β}, where the superscript π represents the transpose and π > 0. πΌ and 0 represent the identity matrix and a zero matrix, respectively. 2 Advances in Mathematical Physics Lemma 1 (see [10, 27]). Consider 3. Main Results π‘ sup (πβππ‘ β« βπ₯ (π)β ππ) β€ 0 π‘β[0,π] 1 βπ₯ (π‘)βπ . π Consider the following system with time delay: (3) Lemma 2 (see [28] retarded Gronwall-like inequality). Consider such an inequality π π’ (π‘) β€ π (π‘) + β β« ππ (π‘) π=1 ππ (π‘0 ) π₯Μ π (π‘) = π (π‘, π₯π (π‘)) + π (π‘, π₯π (π‘ β π)) + π’π (π‘) , π’π+1 (π‘) = π’π (π‘) + πππ (π‘) β ππ,β (π‘) (π₯π+1 (0) β π₯π (0)) , π¦π (π‘) = πΆπ₯π (π‘) + π·π’π (π‘) β ππ,β (π‘) , ππ (π‘, π ) π€π (π’ (π )) ππ , (4) π‘0 β€ π‘ < π‘1 , and suppose that (1) all π€π (π = 1, 2, . . . , π) are continuous and nondecreasing functions on [0, +β) and are positive on (0, +β) such that π€1 β π€2 β β β β β π€π ; (2) π(π‘) is continuously differentiable in π‘ and nonnegative on [π‘0 , π‘1 ), where π‘0 , π‘1 are constants and π‘0 < π‘1 ; (3) all ππ : [π‘0 , π‘1 ) β [π‘0 , π‘1 ) (π = 1, 2, . . . , π) are continuously differentiable and nondecreasing such that ππ (π‘) β€ π‘ on [π‘0 , π‘1 ); (4) all ππ (π‘, π ), π = 1, 2, . . . , π, are continuous and nonnegative functions on [π‘0 , π‘1 ) × [π‘0 , π‘1 ). ππ+1,β (π‘) = ππ,β (π‘) β π·ππ,β (π‘) (π₯π+1 (0) β π₯π (0)) , where π₯π (π‘) β π π , π¦π (π‘) β π π , and π’π (π‘) β π π are the state vector, output vector, and input vector, respectively. π is the number of iterations, π β {1, 2, 3, . . .} and π‘ β [0, π]. π‘ β«0 ππ,β (π)ππ = 1, (π‘ β₯ β), π, πΆ, π· are real constant matrices; ππ (π‘) = π¦π (π‘) β π¦π (π‘), π¦π (π‘) is a reference output. Suppose that there exist the bounded constants ππ > 0 and ππ > 0 such that σ΅©σ΅© σ΅© σ΅© σ΅© σ΅©σ΅©π (π‘, π₯π+1 (π‘)) β π (π‘, π₯π (π‘))σ΅©σ΅©σ΅© β€ ππ σ΅©σ΅©σ΅©π₯π+1 (π‘) β π₯π (π‘)σ΅©σ΅©σ΅© , σ΅©σ΅©σ΅©π (π‘, π₯π+1 (π‘ β π)) β π (π‘, π₯π (π‘ β π))σ΅©σ΅©σ΅© (9) σ΅© σ΅© σ΅© σ΅© β€ ππ σ΅©σ΅©σ΅©π₯π+1 (π‘ β π) β π₯π (π‘ β π)σ΅©σ΅©σ΅© . Theorem 3. For system (8) and a given reference π¦π (π‘), if there exist matrices π, πΆ, π· and functions ππ,β (π‘) and ππ,β (π‘) such that βπΌ β π·πβ β€ π < 1, π Take the notation ππ (π , π 0 ) fl β«π (ππ§/π€π (π§)) for π > 0, where 0 π 0 > 0 is a given constant. It is denoted by ππ (π ) simply when there is no confusion. If π’(π‘) is a continuous and nonnegative function on [π‘0 , π‘) satisfying (4), then π’ (π‘) β€ ππβ1 [ππ (ππ (π‘)) + β« ππ (π‘) max ππ (π, π ) ππ ] , ππ (π‘0 ) π‘0 β€π<π‘ π₯π+1 (π‘) β π₯π (π‘) π‘ = β« (π₯Μ π+1 (π) β π₯Μ π (π)) ππ + π₯π+1 (0) β π₯π (0) where ππ (π‘) is determined recursively by 0 π‘ = β« (π (π, π₯π+1 (π)) β π (π, π₯π (π))) ππ π‘ σ΅¨ σ΅¨ π1 (π‘) fl π (π‘0 ) + β« σ΅¨σ΅¨σ΅¨σ΅¨πσΈ (π )σ΅¨σ΅¨σ΅¨σ΅¨ ππ , π‘ 0 π‘ 0 ππ (π‘) max ππ (π, π ) ππ ] , (6) ππ (π‘0 ) π‘0 β€π<π‘ + β« (π (π, π₯π+1 (π β π)) β π (π, π₯π (π β π))) ππ 0 π‘ + β« (π’π+1 (π) β π’π (π)) ππ + π₯π+1 (0) β π₯π (0) π = 1, 2, . . . , π β 1; 0 π‘ = β« (π (π, π₯π+1 (π)) β π (π, π₯π (π))) ππ π < π‘1 and π is the largest number such that ππ (ππ (π)) + β« ππ (π) max ππ (π, π ) ππ β€ β« ππ (π‘0 ) π‘0 β€π<π +β π 0 0 ππ§ , π€π (π§) π = 1, 2, . . . , π. π‘ + β« (π (π, π₯π+1 (π β π)) β π (π, π₯π (π β π))) ππ (7) (10) where π is a constant, then system (8) with the iterative learning control law can guarantee that βπ¦π (π‘) β π¦π (π‘)β is bounded but π¦π (π‘) cannot track π¦π (π‘) on π‘ β [0, β] and limπββ π¦π (π‘) = π¦π (π‘) on π‘ β [β, π] for arbitrary initial state π₯π (0). Proof. It is easy to know that, for any π‘ β [β, π], (5) π‘0 β€ π‘ β€ π, ππ+1 (π‘) fl ππβ1 [ππ (ππ (π‘)) + β« (8) 0 π‘ + β« πππ (π) ππ 0 Advances in Mathematical Physics 3 π‘ Using Lemma 1 and multiplying both sides of the above inequality (14) by πβππ‘ and taking the π-norm, we have σ΅©σ΅© σ΅© σ΅©σ΅©ππ+1 (π‘)σ΅©σ΅©σ΅©π σ΅© σ΅© β€ βπΌ β π·πβ σ΅©σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅©π β (π₯π+1 (0) β π₯π (0)) (β« ππ,β (π) ππ β 1) 0 π‘ = β« (π (π, π₯π+1 (π)) β π (π, π₯π (π))) ππ 0 π‘ + β« (π (π, π₯π+1 (π β π)) β π (π, π₯π (π β π))) ππ + 0 π‘ + β« πππ (π) ππ. βπΆβ βπβ π(1+ππ /ππ )π σ΅©σ΅© σ΅© σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅©π π = (βπΌ β π·πβ + 0 (11) π‘ σ΅© σ΅© σ΅© σ΅©σ΅© σ΅©σ΅©π₯π+1 (π‘) β π₯π (π‘)σ΅©σ΅©σ΅© β€ ππ β« σ΅©σ΅©σ΅©π₯π+1 (π) β π₯π (π)σ΅©σ΅©σ΅© ππ 0 π‘βπ 0βπ σ΅© σ΅©σ΅© σ΅©σ΅©π₯π+1 (π) β π₯π (π)σ΅©σ΅©σ΅© ππ (12) π‘ σ΅© σ΅© + β« βπβ σ΅©σ΅©σ΅©ππ (π)σ΅©σ΅©σ΅© ππ. 0 0 π‘ In this paper, we use Lemma 2. Taking π‘0 = 0, π1 (π‘) = π‘, π‘ π π2 (π‘) = π‘ β π, π(π‘) = β«0 βπββππ (π)βππ, π1 (π ) = ππ β«1 (ππ§/π§) = π ππ lnπ , and π2 (π ) = ππ β«1 (ππ§/π§) = ππ lnπ , then π1 (π‘) = π‘ β«0 βπββππ (π)βππ and π2 (π‘) = exp[ln(β«0 βπββππ (π)βππ) + π‘ (ππ /ππ )π‘ β«0 (ππ /ππ )ππ] = π π₯π (π‘)β β€ exp[ln(π (1+ππ /ππ )π‘ π π‘ β β« βπββππ (π)βππ. So we have βπ₯π+1 (π‘)β 0 (ππ /ππ )π‘ π‘ π‘ π‘βπ β«0 βπββππ (π)βππ) + β«0βπ ππ] = β β«0 βπββππ (π)βππ: π‘ + β« πππ (π) ππ 0 π‘ β (π₯π+1 (0) β π₯π (0)) (β« ππ,β (π) ππ β 1) , σ΅© σ΅©σ΅© σ΅©σ΅©π₯π+1 (π‘) β π₯π (π‘)σ΅©σ΅©σ΅© π‘βπ + ππ β« 0βπ β πΆπ₯π+1 (π‘) β π·π’π+1 (π‘) + ππ+1,β (π‘) 0 (16) σ΅© σ΅©σ΅© σ΅©σ΅©π₯π+1 (π) β π₯π (π)σ΅©σ΅©σ΅© ππ π‘ σ΅© σ΅© + β« βπβ σ΅©σ΅©σ΅©ππ (π)σ΅©σ΅©σ΅© ππ 0 = ππ (π‘) β πΆ (π₯π+1 (π‘) β π₯π (π‘)) + (ππ+1,β (π‘) β ππ,β (π‘)) 0 π‘ = ππ (π‘) + πΆπ₯π (π‘) + π·π’π (π‘) β ππ,β (π‘) β π· (π’π+1 (π‘) β π’π (π‘)) + β« (π (π, π₯π+1 (π β π)) β π (π, π₯π (π β π))) ππ σ΅© σ΅© β€ ππ β« σ΅©σ΅©σ΅©π₯π+1 (π) β π₯π (π)σ΅©σ΅©σ΅© ππ 0 ππ+1 (π‘) = ππ (π‘) + π¦π (π‘) β π¦π+1 (π‘) (13) σ΅© π‘ σ΅©σ΅© σ΅© σ΅© σ΅© σ΅©σ΅© + σ΅©σ΅©σ΅©π₯π+1 (0) β π₯π (0)σ΅©σ΅©σ΅© σ΅©σ΅©σ΅©β« ππ,β (π) ππ β 1σ΅©σ΅©σ΅© σ΅©σ΅© 0 σ΅©σ΅© π‘ σ΅© σ΅© β€ ππ β« σ΅©σ΅©σ΅©π₯π+1 (π) β π₯π (π)σ΅©σ΅©σ΅© ππ 0 = ππ (π‘) β πΆ (π₯π+1 (π‘) β π₯π (π‘)) β π·πππ (π‘) π‘βπ + π·ππ,β (π‘) (π₯π+1 (0) β π₯π (0)) + ππ β« 0βπ + (ππ+1,β (π‘) β ππ,β (π‘)) σ΅© σ΅©σ΅© σ΅©σ΅©π₯π+1 (π) β π₯π (π)σ΅©σ΅©σ΅© ππ π‘ σ΅© σ΅© + β« βπβ σ΅©σ΅©σ΅©ππ (π)σ΅©σ΅©σ΅© ππ + π, 0 = (πΌ β π·π) ππ (π‘) β πΆ (π₯π+1 (π‘) β π₯π (π‘)) , σ΅© σ΅© σ΅© σ΅©σ΅© σ΅©σ΅©ππ+1 (π‘)σ΅©σ΅©σ΅© β€ βπΌ β π·πβ σ΅©σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅© σ΅© σ΅© + βπΆβ σ΅©σ΅©σ΅©π₯π+1 (π‘) β π₯π (π‘)σ΅©σ΅©σ΅© σ΅© σ΅© β€ βπΌ β π·πβ σ΅©σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅© + βπΆβ π(1+ππ /ππ )π π₯π+1 (π‘) β π₯π (π‘) = β« (π (π, π₯π+1 (π)) β π (π, π₯π (π))) ππ π‘ π‘ βπΆβ βπβ π(1+ππ /ππ )π σ΅©σ΅© σ΅© ) σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅©π . π Thus, condition (10) can guarantee (βπΌ β π·πβ + βπΆββπβπ(1+ππ /ππ )π /π) < 1 by selecting π sufficiently large, so we have limπββ βππ (π‘)βπ = 0 for any π‘ β [β, π]. It follows from the equivalence of norms; we get that limπββ βππ (π‘)β = 0. For any π‘ β [0, β], So we obtain from condition (9) + ππ β« (15) π‘ π‘ where π = supπ‘β[0,β] (βπ₯π+1 (0) β π₯π (0)ββ β«0 ππ,β (π)ππ β 1β). It is easy to know that σ΅©σ΅© σ΅© σ΅©σ΅©π₯π+1 (π‘) β π₯π (π‘)σ΅©σ΅©σ΅© π‘ (17) σ΅© σ΅© β€ π(1+ππ /ππ )π‘ (β« βπβ σ΅©σ΅©σ΅©ππ (π)σ΅©σ΅©σ΅© ππ + π) 0 0 by using Lemma 2. σ΅© σ΅© β β« βπβ σ΅©σ΅©σ΅©ππ (π)σ΅©σ΅©σ΅© ππ. (14) 4 Advances in Mathematical Physics Then σ΅© σ΅©σ΅© σ΅© σ΅© σ΅©σ΅©ππ+1 (π‘)σ΅©σ΅©σ΅© β€ βπΌ β π·πβ σ΅©σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅© σ΅© σ΅© + βπΆβ σ΅©σ΅©σ΅©π₯π+1 (π‘) β π₯π (π‘)σ΅©σ΅©σ΅© σ΅© σ΅© β€ βπΌ β π·πβ σ΅©σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅© (18) π‘ σ΅© σ΅© + βπΆβ π(1+ππ /ππ )π (β« βπβ σ΅©σ΅©σ΅©ππ (π)σ΅©σ΅©σ΅© ππ) 0 + βπΆβ π(1+ππ /ππ )π π. Using Lemma 1 and multiplying both sides of the above inequality by πβππ‘ and taking the π-norm, we have σ΅© σ΅©σ΅© σ΅©σ΅©ππ+1 (π‘)σ΅©σ΅©σ΅©π β€ (βπΌ β π·πβ + βπΆβ βπβ π(1+ππ /ππ )π σ΅©σ΅© σ΅© ) σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅©π + π (19) π σ΅© σ΅© = π σ΅©σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅©π + π, π π σ΅© σ΅© β€ π (σ΅©σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅©π + ). πβ1 πβ1 0 < πΏ1 πΌ < π π’ = ππ (π₯π (π‘) , π’π (π‘)) β€ πΏ2 πΌ, ππ’π (π‘) ππ (π₯π (π‘) , π’π (π‘)) β€ πΏ4 πΌ, 0 < πΏ3 πΌ < π π₯ = ππ₯π (π‘) (23) it is easy to obtain that π (π‘, π₯π+1 (π‘) , π’π+1 (π‘)) β π (π‘, π₯π (π‘) , π’π (π‘)) where π = βπΌ β π·πβ + βπΆββπβπ(1+ππ /ππ )π /π: σ΅©σ΅© σ΅© σ΅©σ΅©ππ+1 (π‘)σ΅©σ΅©σ΅©π + Theorem 5. For system (21) and a given reference π¦π (π‘), if there exist matrices π(π‘), πΆ(π‘), and π·(π‘) and functions ππ,β (π‘) and ππ,β (π‘) such that βπΆ(π‘)ββπ(π‘)β is bounded and βπΌ β π·(π‘)π(π‘)β β€ π < 1, where π is a constant, then system (21) with the iterative learning control law can guarantee that βπ¦π (π‘) β π¦π (π‘)β is bounded but π¦π (π‘) cannot track π¦π (π‘) on π‘ β [0, β] and limπββ π¦π (π‘) = π¦π (π‘) on π‘ β [β, π] for arbitrary initial state π₯π (0). When π¦π (π‘) = π (π‘, π₯π (π‘), π’π (π‘)) β ππ,β (π‘) and π (π‘, π₯π (π‘), π’π (π‘)) satisfies = π π₯ (π) (π₯π+1 (π‘) β π₯π (π‘)) (20) (24) + π π’ (π) (π’π+1 (π‘) β π’π (π‘)) , Imitating the above proof, the result limπββ βππ (π‘)βπ = 0 for any π‘ β [β, π] is obtained by selecting π sufficiently large. So it is true that βππ (π‘)β is bounded on π‘ β [0, β]. where π β [π₯π (π‘)+π(π₯π+1 (π‘)βπ₯π (π‘)), π’π (π‘)+π(π’π+1 (π‘)βπ’π (π‘))], π β (0, 1). Consider the following system: Remark 4. When the number of iterations π β β and [β, π] β [0, π], the tracking error satisfies that βππ (π‘)β β 0 on π‘ β [0, π] for arbitrary initial state π₯π (0). System (8) is π₯Μ π (π‘) = π (π‘, π₯π (π‘)) + π (π‘, π₯π (π‘ β π)) + π’π (π‘) , π’π+1 (π‘) = π’π (π‘) + πππ (π‘) β ππ,β (π‘) (π₯π+1 (0) β π₯π (0)) , π₯Μ π (π‘) = π (π‘, π₯π (π‘)) + π (π‘, π₯π (π‘ β π (π‘))) + π’π (π‘) , π¦π (π‘) = π (π‘, π₯π (π‘) , π’π (π‘)) β ππ,β (π‘) , π’π+1 (π‘) = π’π (π‘) + π (π‘) ππ (π‘) β ππ,β (π‘) (π₯π+1 (0) β π₯π (0)) , (21) π¦π (π‘) = πΆ (π‘) π₯π (π‘) + π· (π‘) π’π (π‘) β ππ,β (π‘) , Μ β€ πΎ < 1. where the delay π(π‘) satisfies 0 < π(π‘) Similar to the proof of Theorem 3, inequality (14) is written as σ΅©σ΅©σ΅©ππ+1 (π‘)σ΅©σ΅©σ΅© β€ βπΌ β π· (π‘) π (π‘)β σ΅©σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅© + βπΆ (π‘)β σ΅© σ΅© σ΅© σ΅© βπΆ (π‘)β βπ (π‘)β π(1+(1βπΎ)ππ /ππ )π σ΅©σ΅© σ΅© ) σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅©π . π Then we have the following. σ΅© σ΅©σ΅© σ΅©σ΅©ππ+1 (π‘)σ΅©σ΅©σ΅©π σ΅© σ΅© (1+π /π )π σ΅© σ΅© σ΅© σ΅©σ΅©π σ΅©σ΅© βπβ π π π σ΅© β€ (σ΅©σ΅©σ΅©πΌ β π π’ πσ΅©σ΅©σ΅© + σ΅© π₯ σ΅© ) σ΅©σ΅©σ΅©ππ (π‘)σ΅©σ΅©σ΅©π . π (26) So we have the following result. π‘ σ΅© σ΅© β βπ (π‘)β π(1+(1βπΎ)ππ /ππ )π β β« σ΅©σ΅©σ΅©ππ (π)σ΅©σ΅©σ΅© ππ, 0 σ΅©σ΅© σ΅© σ΅©σ΅©ππ+1 (π‘)σ΅©σ΅©σ΅©π β€ (βπΌ β π· (π‘) π (π‘)β ππ+1,β (π‘) = ππ,β (π‘) β π π’ ππ,β (π‘) (π₯π+1 (0) β π₯π (0)) . Similar to the proof of Theorem 3, we get ππ+1,β (π‘) = ππ,β (π‘) β π· (π‘) ππ,β (π‘) (π₯π+1 (0) β π₯π (0)) , + (25) (22) Theorem 6. For system (25) and a given reference π¦π (π‘), if conditions (9) are true and there exist matrix π and functions π‘ ππ,β (π‘) and ππ,β (π‘) such that β«0 ππ,β (π)ππ = 1, π‘ > β, βπ π₯ β is bounded, max(βπΌ β πΏ1 πβ, βπΌ β πΏ2 πβ) β€ π < 1, where π is a constant, then system (25) with the iterative learning control law can guarantee that limπββ π¦π (π‘) = π¦π (π‘) is bounded but π¦π (π‘) cannot track π¦π (π‘) on π‘ β [0, β] and limπββ π¦π (π‘) = π¦π (π‘) on π‘ β [β, π] for arbitrary initial state π₯π (0). Advances in Mathematical Physics 5 4. Numerical Example For further illustration, we consider the following system: π₯Μ π (π‘) = 0.8 cos2 (π₯π (π‘)) σ΅¨ σ΅¨ σ΅¨ σ΅¨ β 0.5 (σ΅¨σ΅¨σ΅¨π₯π (π‘ β 1) + 1σ΅¨σ΅¨σ΅¨ β σ΅¨σ΅¨σ΅¨π₯π (π‘ β 1) β 1σ΅¨σ΅¨σ΅¨) + π’π (π‘) , π’π+1 (π‘) = π’π (π‘) + 0.9ππ (π‘) (27) β ππ,β (π‘) (π₯π+1 (0) β π₯π (0)) , π¦π (π‘) = tanh (2π₯π (π‘) + 0.9π’π (π‘)) β ππ,β (π‘) , ππ+1 (π‘) = ππ (π‘) β 0.9ππ,β (π‘) (π₯π+1 (0) β π₯π (0)) , where π = 0.9 and π π { cos ( π‘) , π‘ β [0, 0.5) , 2 × 0.5 (28) ππ,β (π‘) = { 2 × 0.5 0, π‘ β 5] , [0.5, { taking the reference π¦π (π‘) = sin π‘ + 1. From the above numerical example, it can be easily proved that the conditions of Theorem 6 are satisfied. 5. Conclusion In this paper, considering the iterative learning control problem for nonlinear systems with delays, the novel sufficient conditions for robust convergence of the tracking error have been addressed. Competing Interests The author declares that there are no competing interests. 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