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Research article

Input-to-state stability for discrete-time switched systems by using Lyapunov functions with relaxed constraints

  • Received: 10 September 2023 Revised: 23 October 2023 Accepted: 06 November 2023 Published: 15 November 2023
  • MSC : 34D05, 37B25, 93C10, 93C55, 93D20

  • In this paper, input-to-state stability (ISS) is investigated for discrete-time time-varying switched systems. For a switched system with a given switching signal, the less conservative assumptions for ISS are obtained by using the defined weak multiple ISS Lyapunov functions (WMISSLFs). The considered switched system may contain some or all subsystems which do not possess ISS. Besides, for an ISS subsystem the introduced Lyapunov function could be increasing along the trajectory of the subsystem without input at some moments. Then for a switched system under any switching signal, the relaxed sufficient constraints for ISS are attained by using the defined weak common ISS Lyapunov functions. For this case, each subsystem of the considered system must be ISS. The proposed function may be increasing along the trajectory of each ISS subsystem of the considered system without input at some instants. The relationship between WMISSLFs for a switched system and the defined weak multiple Lyapunov functions for this switched system without input is set up. Three numerical examples are investigated to display the usefulness of the principal outcomes. According to the main conclusions, an intermittent controller is applied to ensure ISS for a discrete-time disturbed Chua's chaotic system.

    Citation: Huijuan Li. Input-to-state stability for discrete-time switched systems by using Lyapunov functions with relaxed constraints[J]. AIMS Mathematics, 2023, 8(12): 30827-30845. doi: 10.3934/math.20231576

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  • In this paper, input-to-state stability (ISS) is investigated for discrete-time time-varying switched systems. For a switched system with a given switching signal, the less conservative assumptions for ISS are obtained by using the defined weak multiple ISS Lyapunov functions (WMISSLFs). The considered switched system may contain some or all subsystems which do not possess ISS. Besides, for an ISS subsystem the introduced Lyapunov function could be increasing along the trajectory of the subsystem without input at some moments. Then for a switched system under any switching signal, the relaxed sufficient constraints for ISS are attained by using the defined weak common ISS Lyapunov functions. For this case, each subsystem of the considered system must be ISS. The proposed function may be increasing along the trajectory of each ISS subsystem of the considered system without input at some instants. The relationship between WMISSLFs for a switched system and the defined weak multiple Lyapunov functions for this switched system without input is set up. Three numerical examples are investigated to display the usefulness of the principal outcomes. According to the main conclusions, an intermittent controller is applied to ensure ISS for a discrete-time disturbed Chua's chaotic system.



    The concept of input-to-state stability (ISS) for continuous-time dynamic systems was proposed by Sontag in [1]. Many interesting results with respect to ISS for continuous-time dynamic systems were discussed in references such as [2,3,4,5]. The ISS property for a discrete-time dynamic system was studied well in [6]. ISS Lyapunov functions with relaxed constraints for dynamic systems were discussed in [7]. The introduced Lyapunov function could increase at some times for the considered system without input. Since ISS is very useful for the analysis of the stability of dynamic systems, ISS for switched systems has been an interesting and meaningful topic for researchers. In [8], stability for a switched linear system was investigated. Then via multiple Lyapunov functions, the authors showed how to stabilize a switched linear system. By using Lyapunov-like functions with relatively mild requirements, in [9] a discrete-time switched system related to a given switching signal was proved to be asymptotically stable. In [10], a novel average dwelling time approach was designed to attain stability for a switched discrete-time system constituted by some subsystems which are not stable. For an asymptotically stable subsystem, the Lyapunov function must be decreasing along the trajectory of the state. By constructing a bounded function in regard to the average dwell time, the authors of [11] discussed ISS for a switched nonlinear system. The ISS property for switched nonlinear systems was explored in [12,13]. In these papers, it was assumed that each subsystem is ISS. In [14], by constructing a hybrid ISS Lyapunov function, the authors attained ISS for switched systems consisting of some modes which are not stable. In these references, Lyapunov functions must be decreasing along the trajectory of an ISS subsystem without input. In [15], ISS for discrete-time time-invariant switched systems was investigated by utilizing Lyapunov functions with relatively weak conditions. The switched system may have subsystems which are not ISS. In [16], the authors proposed a formula related to the activation time and the average dwell time. Then, the formula was utilized to attain ISS for a continuous-time time-invariant switched system. The considered switched system may have some unstable subsystems. In [17], the authors utilized Lyapunov functions with relaxed conditions to investigate asymptotic stability for impulsive systems. In [18], via the multiple max-separable ISS Lyapunov function, the authors obtained ISS and stabilization state-feedback control was designed for switched nonlinear time-invariant positive systems under deterministic or random switching. In [19], a time-invariant system was stabilized to exponential ISS by designing aperiodic intermittent control. In [20], the authors designed periodic event-triggered control to make sure that nonlinear networked control systems are ISS. In [21], the authors studied how to input-state stabilize semilinear systems by designing aperiodical intermittent event-triggered control. The authors analyzed the ISS of multilayer coupled systems by introducing a periodic event-triggered control with a dynamic term in [22]. ISS was studied in [23] for time-varying nonlinear switched systems with multiple Lyapunov functions under relaxed constraints. The authors of [24] studied ISS for time-varying delayed switched systems. In [25], ISS was investigated for a discrete-time time-invariant switched nonlinear system. In these references, switched systems could have some subsystems which are not ISS. But ISS Lyapunov functions for ISS subsystems were used for the ISS of the considered system. In [26], the ISS for continuous-time time-varying dynamic systems with input was analyzed via Lyapunov functions with less conservative constraints. Inspired by this reference, we are interested in investigating ISS of discrete-time switched systems. Discrete-time switched systems are of interest since they are widely utilized to analyze practical phenomena in many application fields such as chemistry, finance and engineering. It is necessary to point out that in our manuscript non-ISS Lyapunov functions with certain constraints can be used to analyze the ISS of a system which may have non-ISS subsystems.

    In this paper, we are going to investigate relaxed assumptions for the ISS of discrete-time time-varying switched nonlinear systems. For a switched system under a given switching, the less conservative sufficient requirements for ISS are obtained by using the defined WMISSLFs (Theorem 3.1). The key points of our results are listed as follows. Compared with the results of [14,16,24,25], the introduced Lyapunov function along the trajectory of an ISS subsystem without input could increase at some instants. It is necessary to emphasize that we can apply Theorem 3.1 in ISS analysis for switched systems constituted by some or all subsystems which are not ISS. This point of view is demonstrated by Examples 2 and 3 from Section 4. The relationship between WMISSLFs for a switched system and the introduced weak multiple Lyapunov functions (WMLFs) for this switched system without input is described in Theorem 3.2. Proposition 3.1 discusses ISS for discrete-time time-varying switched systems with all ISS subsystems under any switching. The introduced Lyapunov function could increase along the trajectory of the sate at some instants for a system without input. According to Theorem 3.1, an intermittent controller is applied to ensure ISS for a discrete-time disturbed Chua's chaotic system.

    The rest of the manuscript is organized as follows. In Section 2, we present the notations and definitions used in this paper. The problems studied in this paper are described. In Section 3, we attain the main results. For a switched system under a given switching signal, the less conservative sufficient conditions for ISS are proposed through the use of WMISSLFs (Theorem 3.1). For a switched system with any switching signal, the relaxed sufficient constraints for ISS are attained by using the introduced weak common ISS Lyapunov functions (WCISSLFs) (Proposition 3.1). Theorem 3.2 (Proposition 3.2) describes the relationship between WMISSLFs (WCISSLFs) for a switched system and WMLFs (WCLFs) for this switched system without input. The efficacy of the obtained outcomes is displayed by three numerical examples in Section 4. According to Theorem 3.1, in Section 5 intermittent control is applied to ensure ISS for a discrete-time disturbed Chua's chaotic system. Some concluding discussions are presented in Section 6.

    Notations utilized in this paper are listed as follows. R+ is for the set of nonnegative real numbers. Z+ represents the set of nonnegative integers. The n-dimension real Euclidean space is denoted by Rn. The Euclidean norm of xRn is represented by |x|. Given a function u:Z+Rm, we let |u|=supkZ+u(k) denote the supremum norm of the function u(k).

    For a continuous function α:R+R+, if α strictly increases and satisfies that α(0)=0, then we say that α is of class K. A function αK belongs to class K if lims+α(s)=+ holds. A function β(s,t):R+×R+R+ is of class KL if for any fixed tR+, β(s,t) is a K function in the argument s, and for any fixed sR+, limt+β(s,t)=0 is satisfied and β(s,t) is strictly decreasing as the argument t increases.

    In this paper, we are concerned about the following switched system

    x(k+1)=fτ(k)(k,x(k),u(k)),kZ+, (2.1)

    where x(k)Rn is the state of system (2.1) and u(k)Rm is an input. The admissible value function is uU={u:Z+Rm}. The switching signal is determined by the function τ(k):Z+Δ={1,2,,N} (N2). Let 0=k0<k1<<kr< denote the switching time instants.

    For all iΔ and kZ+, it is required that fi(k,0,0)0 holds for all iΔ. The function fi:Z+×Rn×RmRn(iΔ) is supposed to be Lipschitz continuous. Then there exist positive constants Lx and Lu satisfying

    |fi(k,x1,u1)fi(k,x2,u2)|Lx|x1x2|+Lu|u1u2|, (2.2)

    for x1,x2Rn, u1,u2U. The notation xτ(k,x0,u) is for the solution of system (2.1) in regard to an initial condition x0=x(0), a given switching signal τ(k) and an input uU. For convenience, x(k,x0,u) or x(k) will be utilized hereafter instead of xτ(k,x0,u).

    Since we are going to analyze ISS for system (2.1), the definition of ISS is recalled.

    Definition 2.1. System (2.1) is called input-to-state stable (ISS) if there exist functions βKL and γK such that

    |x(k,x0,u)|β(|x0|,k)+γ(|u|),

    for any input uU and any initial condition x0.

    In what follows, we will utilize ISS Lyapunov functions with relaxed constraints to analyze ISS for system (2.1) with some or all non-ISS subsystems under a given switching signal or arbitrary switching signal.

    In this part, for system (2.1) under a given switching signal, the less conservative sufficient constraints for ISS are investigated by using the subsequently defined WMISSLFs. For system (2.1) under any switching signal, the relaxed conditions for ISS are attained by using WCISSLFs introduced in the subsection.

    Theorem 3.1. For system (2.1) under a switching τ(k), if there exist positive constants M,μiR+ and functions Vi:R+×RnR+, α1,α2,ρK, φi:Z+R+ satisfying the following constraints for iΔ, xRn, uUR and kN+,

    α1(|x|)Vi(k,x)α2(|x|), (3.1)
    Vi(k+1,fi(k,x(k),u(k))φi(k)Vi(k,x(k))+ρ(|u(k)|), (3.2)
    Vi(k,x(k))μiVj(k,x(k)),i,jΔ,ij, (3.3)
    0<φi(k)M. (3.4)

    Let μ=maxiΔ{μi} and φ(k)=φτ(k)(k) for kZ+. Furthermore, if we have positive constants KZ+ and 0<ξ<1 (ξR+) that satisfy the constraint

    μχφ(SK)φ(SK+1)φ(SK+K1)ξ,SN+, (3.5)

    where χ denotes the largest number of switching times during the time period [SK,(S+1)K1] (for any SZ+), then system (2.1) is ISS under the given switching signal.

    Proof. Let 0k0<k1<<kr< (rZ+,r>0) denote the switching times. Then for k+1[kr,kr+1) by utilizing the constraints (3.2) and (3.3), we have that

    Vτ(k+1)(k+1,x(k+1))φτ(k)(k)μN[k,k]Vτ(k)(k,x(k))+ρ(|u|)φτ(k)(k)φτ(k)(k1)μN[k1,k]Vτ(k1)(k1,x(k1))+φτ(k)(k)μN[k,k]ρ(|u|)+ρ(|u|)kj=kr1φ(j)μN[kr1,k]Vτ(kr1)(kr1,x(kr1))+k1j=kr1kq=j+1φ(q)μ[j+1,k]ρ(|u|)+ρ(|u|),

    where N[j,k] is for the switching times of τ(k) in [j,k] with jZ+.

    Then utilizing the constraints and the recursive method, we derive that

    Vτ(k+1)(k+1,x(k+1))kj=0φ(j)μN[0,k]Vτ(0)(0,x(0))+k1j=0kq=j+1φ(q)μN[j+1,k]ρ(|u|)+ρ(|u|),

    where N[0,k] denotes the switching times of τ(k) in [0,k].

    We have that

    (S+1)K1j=SKMjSK+1μN[j+1,(S+1)K1]{KMKμχ,M>1,Kμχ,M1.

    Since KMKμχ is bounded, we obtain a positive constant AR+ such that

    A{KMKμχ,M>1,Kμχ,M1.

    It is evident that the equation k=dK+c holds with d,cZ+ and 0c<K. By using the condition (3.5), it is computed that

    Vτ(k+1)(k+1,x(k+1))kj=0φ(j)μN[0,k]Vτ(0)(0,x(0))+ρ(|u|)+k1j=k1(K1)kq=j+1φ(q)μN[j+1,k]Aρ(|u|)+k1(K1)1j=k12(K1)1kq=j+1φ(q)μN[j+1,k+1]Aξρ(|u|)++rj=0kq=j+1φ(q)μN[j+1,k]ξdAρ(|u|)kj=0φ(j)μN[0,k]Vτ(0)(0,x(0))+(A+ξA++ξdA)ρ(|u|)+ρ(|u|)kj=0φ(j)μN[0,k]Vτ(0)(0,x(0))+(1+11ξA)ρ(|u|).

    Based on the constraints (3.2) and (3.5), we attain the following inequalities

    Vτ(k+1)(k+1,x(k+1))kj=lKφ(j)μN[lK,k]lK1j=(l1)Kφ(j)μN[(l1)K,lK1]ξK1j=0φ(j)μN[0,K1]ξVτ(0)(0,x(0))+(1+11ξA)ρ(|u|)Mc+1μχξdVτ(0)(0,x(0))+(1+11ξA)ρ(|u|)Mc+1μχ1ξξkKα2(|x0|)+(1+11ξA)ρ(|u|).

    Now we define the function

    β(s,t)={α11(2μχ1ξξtKα2(s)),M1,s,tR+,α11(2μχMK1ξξtKα2(s)),M>1,s,tR+.

    Because α1,α2K and 0<ξ<1, it is gained that the function α11 is of K. Moreover, for any fixed variable tR+ the above defined function β(s,t) belongs to K which is related to the argument s, and for each fixed s the function β(s,t) is decreasing as the argument tR+ increases and limt+β(s,t)=0 holds. Thus β belongs to KL.

    Using the inequalities given by (3.1), the estimate of the norm of the state is obtained:

    |x(k)|β(|x0|,k)+α11(2(1+11ξA)ρ(|u|)).

    Then based on Definition 2.1, the ISS for system (2.1) is attained.

    Remark 3.1. (1) For system (2.1) with u0, if the constraints of Theorem 3.1 hold, then the asymptotic stability of system (2.1) is derived. This conclusion is similar to Theorem 2 from [27].

    (2) It is clear that the inequality μ1 holds. To make sure that the constraint (3.5) is satisfied, we must require that the inequality φ(SK)φ(SK+1)φ(SK+K1)δ with 0<ξ<1 holds for SN+. We emphasize that it may hold that φ(SK+j)>1 for some jZ+.

    (3) According to the constraints of Theorem 3.1, for a subsystem x(k+1)=fi(k,x(k),u(k)) (some iΔ), since φi(k) may be larger than 1 for all kZ+, this system may not be ISS. However, for system (2.1) with some or all subsystems which are not ISS, Theorem 3.1 can be used to analyze ISS. This point of view is illustrated in Examples 2–3 from Section 4. For an ISS subsystem, Vi may not be an ISS Lyapunov function for this system. This is demonstrated by Example 1 from Section 4.

    (4) Let ΔsΔu=Δ, and ΔsΔu=. In Theorem 3.1, if the constraints (3.2) and (3.4) are replaced by

    Vi(k+1,fi(k,x(k),u(k)))λsVi(k,x(k))+ρ(|u|),iΔs,Vi(k+1,fi(k,x(k),u(k)))λuVi(k,x(k))+ρ(|u|),iΔu,

    where 0λs<1 and λu1. Then in order to ensure that the constraint (3.5) holds, it is necessary to require that we have positive constants r,σaR+ satisfying the following constraints

    σa>lnμ(1r)lnλsrlnλu,r<lnρslnλulnλs,Nτ[k,k+K]Kσa,kN,ku[k,k+K]rK,kN, (3.6)

    where μ=maxiΔ{μi} and ku[k,k+K] denotes the activation time period of the subsystems in Δu in [k,k+K]. Under these constraints, we derive the following:

    μχφ(SK)φ(SK+1)φ(SK+K1)μkσaλkuuλ(1r)ksμkσaλrkuλ(1r)ks=ξ<1.

    Then according to the derivation of Theorem 3.1, we can attain ISS for system (2.1). We have to point out that the above constraints are similar to those of [28, Theorem 2].

    Based on Theorem 3.1, for system (2.1) under a given switching, we introduce the concept of weak multiple input-to-state stability Lyapunov functions for switched system (2.1).

    Definition 3.1. For system (2.1) under a switching signal τ(k), we call {Vi:R+×RnR+,iΔ} a weak multiple input-to-state stability Lyapunov function (WMISSLF) if the conditions (3.1)–(3.3) of Theorem 3.1 on the functions Vis and the assumptions (3.4) and (3.5) imposed on φi,μi(iΔ) hold.

    Remark 3.2. (1) For system (2.1) with u0, {Vi:R+×RnR+,iΔ} from Definition 3.1 is called a weak multiple Lyapunov function (WMLF).

    (2) If the functions fi (iΔ) satisfy

    |fi(k,x(k),u(k))|φi(k)|x(k)|+ρ(|u|),

    where φi(k), ρ satisfy the constraints of Theorem 3.1, then Vi(k,x(k))=Vj(k,x(k))=|x| (i,jΔ, ij) is a WMISSLF for system (2.1). This conclusion indicates that under the above given constraints we may first check if |x| is a WMISSLF for the considered examples in Section 4. It is noteworthy that φiφj may hold for i,jΔ, ij.

    The relationship between WMISSLFs for system (2.1) and WMLFs for system (2.1) without input is described as Theorem 3.2.

    Theorem 3.2. For system (2.1) with u0 and a switching τ(k), if there exist a WMLF {Vi:R+×RnR+,iΔ} and a positive constant L such that |Vi(k,x1)Vi(k,x2)|L|x1x2| for kZ+ and x1, x2Rn, then {Vi:R+×RnR+,iΔ} is a WMISSLF for the switched system (2.1) under the switching signal τ(k).

    Proof. To demonstrate that {Vi:R+×RnR+,iΔ} is a WMISSLF for system (2.1) with the given switching signal τ(k), we have to prove that the inequality (3.2) holds. Based on the assumptions, we have

    Vi(k+1,fi(k,x(k),0))φi(k)Vi(k,x(k)).

    Then we get that

    Vi(k+1,fi(k,x(k),u(k)))Vi(k+1,fi(k,x(k),u(k)))+φi(k)Vi(k,x(k))Vi(k+1,fi(k,x(k),0))φi(k)Vi(k,x(k))+L|fi(k,x(k),u(k))fi(k,x(k),0)|φi(k)Vi(k,x(k))+LLu|u|.

    Hence we attain that the inequality (3.2) is satisfied. Therefore, {Vi:R+×RnR+,iΔ} is a WMISSLF for system (2.1).

    Remark 3.3. Theorem 3.2 shows one way to construct a WMISSLF for system (2.1), i.e., construction of a WMLF with Lipschitz continuity for system (2.1) with u0. The topic with respect to the computation of WMISSLFs for system (2.1) will be investigated in the future.

    For Theorem 3.1, if the equations φi(k)φj(k) and Vi(k,x(k))=Vj(k,x(k)) (ij,i,jΔ) are required, then we have the following proposition.

    Proposition 3.1. For system (2.1), if we have the functions V:R+×RnR+, α1,α2,ρK, φ:Z+R+ and positive constants M,μiR+ satisfying the following constraints for iΔ, xRn, uUR and kN+,

    α1(|x|)V(k,x)α2(|x|), (3.7)
    V(k+1,fi(k,x(k),u(k))φ(k)V(k,x(k))+ρ(|u(k)|), (3.8)
    0<φ(k)M. (3.9)

    Moreover, if the positive constants KZ+ and 0<ξ<1 (ξR+) satisfying the following inequality exist:

    φ(SK)φ(SK+1)φ(SK+K1)ξ,SN+, (3.10)

    then system (2.1) is ISS under any switching signal.

    Proof. The conclusion can be obtained through a similar derivation of Theorem 3.1.

    Remark 3.4. (1) It is worthy to point out that for an ISS subsystem, V from Proposition 3.1 may not be an ISS Lyapunov function, since for some iΔ, φ>1 can hold for some kZ+.

    (2) Compared to Theorem 3.1, the merit of Proposition 3.1 is that it can be used for the ISS analysis of switched system (2.1) in regard to arbitrary switching signal. This point is illustrated via Example 1 in Section 4.

    (3) Under the constraints of Proposition 3.1, for system (2.1) without input (u0), the asymptotic stability is derived.

    Based on Proposition 3.1, we introduce the definition of weak common input-to-state stability Lyapunov functions for switched system (2.1).

    Definition 3.2. For system (2.1), a function V:R+×RnR+ is called a weak common input-to-state stability Lyapunov function (WCISSLF) for system (2.1), if the constraints (3.7) and (3.8) from Proposition 3.1 on the function V and the assumptions (3.9) and (3.10) imposed on φ are satisfied.

    Remark 3.5. We call a WCISSLF V:R+×RnR+ from Definition 3.2 a weak common Lyapunov function(WCLF) for system (2.1) with u0.

    The relationship between the WCISSLFs for system (2.1) and WCLFs for system (2.1) without input is set up via Proposition 3.2.

    Proposition 3.2. If there exist a WCLF V:R+×RnR+ for system (2.1) with u0 and a positive constant L1 such that |V(k,x1)V(k,x2)|L1|x1x2| for kZ+, x1,x2Rn, then V is a WCISSLF for system (2.1).

    Proof. This result is obtained via a derivation similar to that for Theorem 3.2.

    Remark 3.6. Proposition 3.2 provides one way to construct a WCISSLF for system (2.1), i.e., construction of a Lipschitz continuous WCLF for system (2.1) with u0. We will investigate how to compute the WCISSLF for system (2.1) in the future.

    In this part, we are going to analyze ISS for three examples by applying our main results.

    We study a switched system described by

    x(k+1)=fτ(k)(k,x(k),u(k)), (4.1)

    where x(k)R, u(k)R, τ(k)Δ={1,2}, and

    f1(k,x(k),u(k))=6+2k21+4k2+x2(k)x(k)+14sin2(kπ4)u(k),f2(k,x(k),u(k))=(12+sin2(kπ4))x(k)+0.2u(k).

    Now we use Proposition 3.1 to investigate ISS for system (4.1) with an arbitrary switching signal. We check if a WCISSLF candidate V(k,x(k))=|x(k)| satisfies all requirements from Proposition 3.1. By simple calculation, we have the inequalities

    V(k+1,f1(k,x(k),u(k)))6+2k21+4k2|x(k)|+0.2|u(k)|,V(k+1,f2(k,x(k),u(k)))(12+sin2(kπ4))|x(k)|+0.2|u(k)|.

    Define φ:Z+R+ as follows

    φ(k)=max{6+2k21+4k2,(12+sin2(kπ4))}.

    It is clear that φ(k)6 is satisfied and the inequality (3.10) holds with K=37 and ξ=0.9234. Thus

    V(k+1,fi(k,x(k),u(k)))φ(k)V(k,x(k))+0.2|u(k)|,iΔ. (4.2)

    Hence the requirements of Proposition 3.1 hold. Therefore, system (4.1) under an arbitrary switching signal is ISS. Figure 1 shows the ISS for system (4.1) with x0=0.5, u(k)=rand(1) and the following switching signal

    τ(k)={1,k=2s,sZ+,2,k2s,sZ+. (4.3)
    Figure 1.  State of system (4.1) related to the switching signal (4.3), x0=0.5 and u(k)=rand(1).

    Figure 2 displays the asymptotic stability of system (4.1) without input. Example 1 demonstrates how to analyze ISS for switched systems with any switching signal.

    Figure 2.  State of system (4.1) without input, but with x0=0.5 and the switching signal (4.3).

    Remark 4.1. In [25], for an ISS subsystem, the function V is an ISS Lyapunov function. However, it is clear that the function V(k,x) is not an ISS Lyapunov function for each subsystem of system (4.1), since it increases at some times for each subsystem without input.

    We investigate the ISS for a switched system

    x(k+1)=fi(k,x(k),u(k)),i=1,2, (4.4)

    with x=(x1,x2)R2, u=(u1,u2)R2.

    The functions denoted by fi are

    f1(k,x(k),u(k))={(15+sin2(kπ2))x1(k)+u1(k),(15+sin2(kπ2))x2(k)+u2(k).
    f2(k,x(k),u(k))={x1(k)+u1(k),(1+cos2(k))x2(k).

    The switching signals are determined by

    τ(k)={1,k[ks,ks+2),2,k[ks+2,ks+4),

    where k0=0, ks+1=ks+4 and sZ+.

    For the subsystem described by (4.5), it is clear that we cannot get asymptotic stability for system (4.5) without input. Therefore, the subsystem (4.5) is not ISS. Thus system (4.4) is not ISS for any switching signal.

    x(k+1)=f2(k,x(k),u(k)). (4.5)

    Then using Theorem 3.1, we analyze the ISS for system (4.4). We examine if a WMISSLF candidate {V1(k,x)=V2(k,x)=|x|1=|x1|+|x2|} meets the requirements of Theorem 3.1. Here in order to make it easy to calculate, 1-norm ||1 is used. We compute that

    V1(k+1,f1(k,x(k),u(k)))(15+sin2(kπ2))V1(k,x(k))+|u(k)|1,V2(k+1,f2(k,x(k),u(k)))=|x1(k+1)|+|x2(k+1)|2V2(k,x(k))+|u(k)|1.

    Thus we have

    φ1(k)=15+sin2(kπ2),φ2(k)=2.

    Let

    φ(k)={φ1(k)=15+sin2(kπ2),k[ks,ks+2),φ2(k)=2,k[ks+2,ks+4).

    Then it holds that φ(k)2 for kZ+. The constraint (3.5) is satisfied with K=4 and ξ=2425. Therefore, the assumptions of Theorem 3.1 hold. Hence system (4.4) is ISS (see Figure 3). The asymptotic stability of system (4.4) without input is demonstrated by Figure 4.

    Figure 3.  State of system (4.4) given x0=(1,5) and u(k)=(sin2(kπ4),cos2(kπ4)).
    Figure 4.  State of system (4.4) in connection with x0=(1,5) but without input.

    Remark 4.2. It is necessary to point out that the subsystem (4.5) of system (4.4) is not ISS and that V1 increases at some moments for the second subsystem without input. However, via Theorem 3.1, ISS of system (4.4) is attained under the given switching signal.

    We evaluate ISS for the following switched system

    x(k+1)=fτ(k)=(k,x(k),u(k)), (4.6)

    with x(k)R2,u(k)R2 and

    τ(k)={1,k[ks,ks+2),2,k[ks+2,ks+4),

    where k0=0, ks+1=ks+4 and sZ+.

    The functions fi (i=1,2) are described by

    f1(k,x(k),u(k))=3x(k)+u(k),kZ+,f2(k,x(k),u(k))=c(k)x(k)+3u(k),kZ+,withc(k)={5,k[ks,ks+2),sZ+,14,k[ks+2,ks+4),sZ+.

    For the subsystem x(k+1)=fi(k,x(k),u(k)) (i=1,2) with u0, we can not attain asymptotic stability. Hence each subsystem of system (4.6) is not ISS. However, we can analyze the ISS of system (4.6) by utilizing Theorem 3.1. Let {V1(k,x(k))=|x|,V2(k,x(k))=56|x|} be a WMISSLF candidate for system (4.6). Under the given constraints, we have

    V1(k+1,x(k+1))3V(k,x(k))+3|u|, (4.7)
    V1(k+1,x(k+1))c(k)V(k,x(k))+3|u|, (4.8)

    where c(k)={5,k[ks,ks+2),sZ+,14,k[ks+2,ks+4),sZ+.

    Then we obtain that μ=65, M=5 and

    φ(k)={3,k[ks,ks+2),sZ+,14,k[ks+2,ks+4),sZ+.

    We check that the inequality (3.5) holds with K=4, χ=2 and ξ=324400. Thus all constraints of Theorem 3.1 are satisfied. Therefore, under the given switching signal, system (4.6) is ISS. This is shown in Figure 5. Figure 6 displays that system (4.6) without input is asymptotically stable.

    Figure 5.  State of system (4.6) given x0=(1,1) and u(k)=(sin2(kπ4),cos2(kπ4)).
    Figure 6.  State of system (4.6) given x0=(1,1) and u(k)=0.

    Remark 4.3. According to the above analysis, it is clear that subsystems of system (4.6) are not ISS. Hence Example 3 demonstrates that we can use Theorem 3.1 to analyze ISS for switched systems constituted by all subsystems which are not ISS.

    By using Theorem 3.1, in this section we are going to design an intermittent controller to ensure ISS for a discrete-time disturbed Chua's chaotic system described by

    x(k+1)=Ax(k)+G(x(k))+u(k)+w(k), (5.1)

    where A=(α(1+b)+1α01010β1), G(x)=(g(x)00), x=(x1,x2,x3)R3, g(x)=α(ab)(|x1+1||x11|)2 and constants α,β,a<b<0. For system (5.1), the control input is u:RnRn and the external disturbance is w:RnRn.

    The intermittent control is designed as follows:

    u(k)={Hx(k)+(α(ab),0,0),x1<1,¯kik<¯ki+Ti,Hx(k)+(α(ab)x1,0,0),1x11,¯kik<¯ki+Ti,Hx(k)+(α(ab),0,0),x1>1,¯kik<¯ki+Ti,0,¯ki+Tik<¯ki+1,iZ+, (5.2)

    where H is a constant control matrix, ¯ki is the beginning time of the ith intermittent control and 0<Ti¯ki+1¯ki is the ith time period during which the control u is activated. It is required that Ti and ¯ki+1¯ki are bounded and ¯k0=0. Let Tm=miniZ+{Ti} and ¯km=maxiZ+{¯ki+1¯kiTi}. It is clear that the switching times are ¯ki,¯ki+Ti (iZ+). Then we consider system (5.1) with the input control (5.2) as a switched system composed of two subsystems. Then we are going to stabilize system (5.1) to ISS by applying the intermittent controller (5.2) and Theorem 3.1.

    By imposing the controller (5.2) on system (5.1), we will study the system described by

    x(k+1)={Ax(k)+Hx(k)+w(k),¯kik<¯ki+Ti,Ax(k)+G(x(k))+w(k),¯ki+Tik<¯ki+1,iZ+. (5.3)

    Let {V1(k,x)=V2(k,x)=|x(k)|} be a WMISSLF candidate. Then we have

    |x(k+1)|{|A+H||x(k)|+|w|,¯kik<¯ki+Ti,(|A|+α(ba))|x(k)|+|w|,¯ki+Tik<¯ki+1,iZ+.

    According to Theorem 3.1 and Proposition 3.1, the following conclusion can be obtained.

    Proposition 5.1. For system (5.1) with the input control (5.2), if we get a matrix H satisfying

    (|A|+α(ba))¯km|A+H|Tm=ξ<1, (5.4)

    then the constraint (3.5) with K=¯km+Tm from Theorem 3.1 is satisfied. Furthermore, system (5.1) with the input control (5.2) has ISS under the disturbance w.

    In this section, we investigate again system (5.1) with α=9.2156, β=15.9946, a=1.2495, b=0.75735 and the disturbance

    w(k)=2(sin2(k),cos2(k),rand(1)).

    These constraints are the same as those of Example 5.1 of [19].

    Let ¯km=2 and Tm=3. In order to ensure that the condition (5.4) holds, we let

    H=(0.1+α(1+b)1α010.110β0.11).

    It is evident that A+H=(0.10000.10000.1), |A|+α(ba)=23.0258 and (|A|+α(ba))¯km×(0.1)Tm=ξ=0.5302.

    Based on Theorem 3.1, system (5.1) is stabilized to ISS under the intermittent control (5.2) with the above given control matrix H. This is shown in Figure 7. The asymptotic stability of system (5.3) without the disturbance is displayed in Figure 8.

    Figure 7.  Sate of x for system (5.3) with the initial condition x0=(3,1,4), T0=5,¯k1=6,T1=4,¯k2=12,T2=8, ¯k3=20.
    Figure 8.  Sate of x for system (5.3) without the disturbance, but with the initial condition x0=(3,1,4), T0=5,¯k1=6,T1=4,¯k2=12,T2=8, ¯k3=20.

    For system (2.1) under a given switching signal, the less conservative sufficient requirements for ISS were obtained by using the defined WMISSLFs (Theorem 3.1). The key properties of Theorem 3.1 are described as follows. Compared with the results of [14,16,24,25], the considered system can consist of all or some subsystems which are not ISS. Besides, the introduced function for an ISS subsystem could be increasing along the trajectory of the subsystem without input at some moments. Then for system (2.1) under any switching signal, the relaxed sufficient assumptions for ISS were attained by using the introduced WCISSLFs (Proposition 3.1). For this case, each subsystem of system (2.1) should be ISS. The function V from Proposition 3.1 may be increasing along the trajectory of each ISS subsystem of system (2.1) without input at some moments. The relationship between WMISSLFs for system (2.1) and WMLFs for system (2.1) without input was set up in Theorem 3.2. We also discussed the relationship between the WCISSLFs for system (2.1) and WCLFs for system (2.1) without input in Proposition 3.2. The efficacy of the main outcomes was illustrated through the three presented numerical examples. Based on Theorem 3.1 an intermittent controller was designed to ensure ISS for a discrete-time disturbed Chua's chaotic system. Proposition 5.1 describes the constraints which the control matrix H should satisfy. The efficiency of the designed intermittent control was demonstrated through the given simulation results. We will investigate how to construct WMISSLFs (WCISSLFs) for system (2.1) based on WMLFs (WCLFs) for system (2.1) without input in the future.

    The author declares she has not used Artificial Intelligence (AI) tools in the creation of this article.

    This work was supported in part by the National Natural Science Foundation of China [NSFC11701533].

    The author declares no conflicts of interest in this paper.



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