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Input-to-state stability of nonlinear systems with delayed impulse based on event-triggered impulse control

  • This paper investigates input-to-state stability (ISS) of nonlinear systems with delayed impulse under event-triggered impulse control, where external inputs are different in continuous and impulse dynamics. First, an event-triggered mechanism (ETM) is proposed to avoid Zeno behavior. In order to ensure ISS of the considered system, the relationship among event triggering parameters, impulse intensity, and impulse delay is constructed. Then, as an application, ETM and impulse control gain for a specific kind of nonlinear systems are presented based on linear matrix inequalities (LMI). Finally, two examples confirm the feasibility and usefulness of the proposed strategy.

    Citation: Linni Li, Jin-E Zhang. Input-to-state stability of nonlinear systems with delayed impulse based on event-triggered impulse control[J]. AIMS Mathematics, 2024, 9(10): 26446-26461. doi: 10.3934/math.20241287

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  • This paper investigates input-to-state stability (ISS) of nonlinear systems with delayed impulse under event-triggered impulse control, where external inputs are different in continuous and impulse dynamics. First, an event-triggered mechanism (ETM) is proposed to avoid Zeno behavior. In order to ensure ISS of the considered system, the relationship among event triggering parameters, impulse intensity, and impulse delay is constructed. Then, as an application, ETM and impulse control gain for a specific kind of nonlinear systems are presented based on linear matrix inequalities (LMI). Finally, two examples confirm the feasibility and usefulness of the proposed strategy.



    For systems subject to external disturbances, the requirement to maintain robust dynamic behavior under the influence of exogenous perturbations is particularly important. Therefore, the proposed concept of input-to-state stability [1] proves to be very effective in characterizing the effects of external disturbances on the considered system. Input-to-state stability means that when input is bounded, the state of the system remains bounded. If there is no external disturbance, input-to-state stability indicates that the system is asymptotically stable in the sense of Lyapunov. Based on this thought, input-to-state stability results have been investigated for different types of systems, such as switched systems [2,3], impulsive systems [4,5], and stochastic systems [6,7]. Additionally, it has also been extended to finite time control problems and finite time input-to-state stability [8].

    Impulsive systems are a special class of hybrid systems containing both continuous and discrete dynamics, which are widely used in the fields of communication networks, control technology, and image encryption; see [9,10,11,12]. From the perspective of impulse effect, work on the stability of impulsive systems primarily focuses on two major areas: impulse perturbation and impulse control. Impulse perturbation considers the robustness of the system under unstable impulses. Whereas impulse control [13] considers stabilization of systems containing stable impulses. By using discrete impulse signals as control inputs, satisfactory performance can be obtained, breaking through the limitations of traditional continuous control methods. As a discontinuous control method, impulse control has advantages of low cost, low energy consumption, high efficiency, and the ability to describe sudden change phenomena of systems. Thus, impulse control has attracted a wide range of attention in different fields [14,15,16]. In this literature, impulse controllers adopt a time-triggered mechanism, i.e., signal transmission is independent of system state, but impulse moments are pre-scheduled. However, this may lead to overuse of resources in the process of information transmission, resulting in unnecessary depletion of communication resources. Therefore, in order to better save network resources and overcome the drawbacks of time-triggered control methods, the event-triggered mechanism has been introduced; transmission occurs solely when the mechanism is activated; otherwise, the control signals remain updated. In recent years, there have been extensive research on event-triggered mechanisms; for example, reference [17] developed dynamic event-triggered schemes for uncertain nonlinear strict-feedback systems, and reference [18] proposed event-triggered asymptotic tracking control for multi-input and multi-output nonlinear systems.

    Event-triggered impulse control combines the characteristics of event-triggered and impulse control, so that impulse control only acts on the considered system at the event-triggered instant, and there is no longer any control effect within two adjacent event-triggered intervals. This control mode is characterized by the fact that the control signal is released only when a specific state-dependence criterion is satisfied, thus greatly reducing the resource consumption. In practical application, this control strategy needs to exclude infinite triggering behaviors occurring within a limited time. A typical example is Zeno behavior, i.e., there exist an infinite number of triggering instants that converge to a positive constant [19]. It has been shown in [20] that Zeno behavior can occur in external perturbation or measurement noise, which gives caution when designing event-triggered control. Another circumstance is that trigger intervals tend to 0 as trigger instants tend to infinity. From a practical perspective, a trigger interval should have a minimum lower bound of a normal number. And in recent years, event-triggered impulse control has been applied in various control issues, such as consensus problems of multiagent systems [21], asymptotic stability of impulsive systems [22], synchronization of multiple neural networks [23], etc. It is noted that the results of the literature just mentioned can only be applied to some specific dynamical systems, but the influence of exogenous disturbances has not been considered, leading to certain limitations. Therefore, ISS under event-triggered impulse control has received more and more attention [24,25,26,27,28]. For example, ISS characteristics of nonlinear systems under continuous and discrete event-triggered impulse control were investigated in [25]. Based on event-triggered impulse control strategy, the ISS of nonlinear impulsive systems was developed, and Zeno behavior was excluded in [26,27], but impulse delay was not considered in this literature. In practical applications, time delay is inevitable during transmission of impulses; that is, the transient of impulse depends not only on the current state of the system but also on the historical state of the system. In [28], by designing three levels of event triggering schemes, the influence of event-triggered impulse control with time delay on ISS stabilization was discussed. Although delayed impulse is taken into account, these works ignore interference of external input in discrete dynamics. On the other hand, there is some ISS work on impulse control based on the assumption [29], that is, the ratio coefficient of the Lyapunov function is constant. Recently, reference [30] explores the ISS properties of nonlinear impulse systems under event-triggered impulse control. The Lyapunov rate coefficients considered are all constant, but this may not be achieved in practical applications. Therefore, it is necessary to consider the case where the Lyapunov rate coefficient is time-varying. In [31], ISS results of time-varying nonlinear impulsive systems are obtained, but event-triggered impulse control is not considered, resulting in certain conservatism. ISS criteria obtained from [27] are applicable to the nonlinear rate of the Lyapunov functions, but impulse delay and hybrid inputs are not considered, which makes its application limited. In view of this, when delayed impulse is involved, related work to ensure ISS of nonlinear impulsive systems via event-triggered impulse control needs to be further enriched.

    On the basis of the above motivation, the main work of this paper is to explore the ISS of nonlinear systems with delayed impluse in the framework of event-triggered impulse control. A Lyapunov-based ETM containing forced impulse sequence is proposed to realize ISS of the considered system, and Zeno behavior is ruled out. Subsequently, design criteria of impulse control gain and ETM are derived by solving LMI. The contribution of this paper can be summarized in three points:

    (ⅰ) External inputs of continuous and discrete parts are the same in [27,30,32], leading to certain restrictions. This paper considers hybrid inputs, that is, external inputs can be different for the continuous and impulsive parts, which broadens the existing conclusions.

    (ⅱ) Compared to [25,27], the impulse part of this paper involves time delay, and delay information is incorporated into the dynamic analysis of the considered system to establish relationships among event- triggering parameters, impulse intensity, and impulse delay.

    (ⅲ) ISS criteria in this paper are derived on the premise that the Lyapunov rate coefficient is time-varying, rather than constant, which makes the results relax restrictions in [26,28,30].

    Notations: R+, N+, R are sets of non-negative real numbers, positive integers, and real numbers. Rm is m-dimensional space. PC([e,f];Rm) : [e,f]Rm denotes piecewise continuous function. v0 denotes a given category of local Lipschtiz function. Symbol represents a symmetric block in a symmetric matrix. λmax(ϱ), ϱ1 and ϱT represent the maximum eigenvalue, inverse, and transpose of matrix ϱ, respectively. I>0 denotes a positive definite matrix I. K is said to be a class of continuous strictly increasing function c:R+R+ with c(0)=0. K is a radially unbounded subset of K. A function d:R+×R+R+ is defined to be class KL if d(,t) is a kind of K for every fixed t0, d(,t)0 as t+. AB = max{A,B}.

    Consider the following delayed impulsive systems:

    ˙z(t)=g(z(t),vc(t)), ttr, tt0,z(t)=hr(z(tτ),vd(t)), t=tr, rN+,z(nt0)=ϵn, n[t0τ,t0], (1)

    where z(t)Rm is system state. ϵn is the initial state. τ>0 is constant delay. vc(t), vd(t)Rm are locally bounded exogenous perturbation and impulsive perturbation input. g, h : Rm×RnRm satisfy (0,0)=§(0,0)=0 and some appropriate conditions such that existence and uniqueness of solution of system (1) are guaranteed. Impulse instant {tr}rN+ satisfies 0=t0<t1<<tr< and limr+tr=+. Assume the solution of system (1) is right continuous, that is, z(t+)=z(t).

    Definition 1 ([33]). If there exist functions ξKL and β, Γc, ΓdK, system (1) is ISS if

    β(|z(t)|)<ξ(ϵτ,tt0)+supt0stΓc(|vc(s)|)+Γd(maxt0trt{|vd(trτ)|}), tt0,

    where ϵτ=sup[t0τ,t0]|ϵ|.

    Lemma 1 ([34]). Let continuous functions Δ(t), Θ(t), v1(t), v2(t)pc([t0,+);Rm) for t[tr1,tr), rN+, ΔR+ satisfy

    {D+v1(t)Δ(t)v1(t)+Θ(t),ttr, tt0,v1(tr)Δ(t)v1(tr)+Θ(tr),t=tr,

    and

    {D+v2(t)>Δ(t)v2(t)+Θ(t),ttr, tt0,v2(tr)Δ(t)v2(tr)+Θ(tr),t=tr,

    then v1(t)v2(t) for tt0.

    Lemma 2 ([25]). There exist real matrices T>0, Ψ, Ψ, and constant c>0, and the following inequality holds:

    ΨTΨ+ΨTΨcΨTTΨ+c1ΨTT1Ψ.

    In this section, in the framework of the event-triggered impulse control approach, considering the effect of delayed impulses, some conditions to ensure ISS of system (1) are established and Zeno behavior is eliminated. First, the following ETM is considered:

    tr=min{tr,tr1+r}, rN+,tr=inf{ttr1:V(t,z(t))exp(ırς(ttr1))V(tr1,z(tr1))exp(ˉırˉς(ttr1))ϕ1(vc[tr1,t])0}, (2)

    where ϕ1K, V(t,z(t)) is Lyapunov function depending on solution z(t) of system (1) at time t. Event-triggering parameters ı, ˉı, ς, ˉςR+ and rR+ satisfy

    sr=1ı+,sr=1ˉı+, s+, (3)

    and

    infrN+{r}>0. (4)

    In order to exclude Zeno behavior, we give the following result based on designed ETM (2).

    Theorem 1. If functions Υ(t)PC([t0,+);R), ϕ1K, Vv0 satisfy:

    D+V(t,z(t))Υ(t)V(t,z(t))+ϕ1(|vc(t)|),

    and

    tsΥ(u)duc(ts),s,t0,

    where c0 is constant, then system (1) has no Zeno phenomenon via ETM (2), impulse sequence {tr}rN+ satisfies

    trtr1t=max{ırc+ς,ˉırc+ˉς}. (5)

    Proof. According to the definition of ETM (2), three scenarios will be considered.

    Case 1. Impulse instant tr is made up entirely of forced impulse instant, i.e., tr=tr1+r. Based on trtr1=△r and assumption condition (4), it is possible to know that there is no Zeno behavior.

    Case 2. Forced impulse instant tr1+r and event-triggered impulse instant tr occur simultaneously. First, assume that forced impulse instants are finite and satisfy t1+r<t2+r<<tn+1+r. It clearly holds that impulse instant tr is composed entirely of event-triggered impulse instant tr after the last forced impulse instant tn+1+r, thus tn+1+r=tn+1+r,rN+. By Lemma 1, we derive

    V(t,z(t))v(t)=exp(ttn+rΥ(u)du)V(tn+r,z(tn+r))+ttn+rexp(tsΥ(v)dv)ϕ1(|vc(u)|)du.

    Based on ETM (2), we obtain

    V(tn+r+1,z(tn+r+1))=exp(ın+r+1ς(trtr1))V(tn+r,z(tn+r))+exp(ˉın+r+1ˉς(trtr1))ϕ1(vc[tn+r,tn+r+1])exp(tn+r+1tn+rΥ(u)du)V(tn+r,z(tn+r))+tn+r+1tn+rexp(tn+r+1tn+rΥ(v)dv)ϕ1(|vc(u)|)duexp(c(tn+r+1tn+r))V(tn+r,z(tn+r))+exp(c(tn+r+1tn+r))ϕ1(vc[tn+r,tn+r+1]), (6)

    which yields that

    trtr1ın+r+1c+ς,
    trtr1ˉın+r+1c+ˉς,

    hence

    trtr1max{ın+r+1c+ς,ˉın+r+1c+ˉς},

    then, according to condition (3), we know tn+r+1+ as r+, which means that Zeno behavior is excluded under this circumstance.

    Second, forced impulse instants are infinite. Supposing that under ETM (2) Zeno behavior occurs in system (1), which indicates that there are countless impulse moments in the interval [t0,T], and T represents the accumulated time of impulse instants. Then, impulse instants tend to T, that is, forced impulse instants also tend to T, which is inconsistent with expression (4). Thus, Zeno behavior is also ruled out.

    Case 3. Impulse instant tr consists absolutely of event-triggered impulse instant tr, that is, tr=tr, rN+. Proof is similar to case 2, we find

    V(t,z(t))v(t)=exp(ttr1Υ(u)du)V(tr1,z(tr1))+ttr1exp(tsΥ(v)dv)ϕ1(|vc(u)|)du,

    and

    V(tr,z(tr))=exp(ırς(trtr1))V(tr1,z(tr1))+exp(ˉırˉς(trtr1))ϕ1(vc[tr1,tr])exp(trtr1Υ(u)du)V(tr1,z(tr1))+tr1tr1exp(trtr1Υ(v)dv)ϕ1(|vc(u)|)duexp(c(trtr1))V(tr1,z(tr1))+exp(c(trtr1))ϕ1(vc[tr1,tr]). (7)

    Similarly,

    trtr1ırc+ς,trtr1ˉırc+ˉς,

    then

    trtr1max{ırc+ς,ˉırc+ˉς}.

    We can conclude that there is no Zeno phenomenon. Thus, it is clear from the above that Zeno behaviour does not occur under ETM (2) in either case.

    Remark 1. Zeno behavior implies that an infinite number of continuous trigger instants occur in a finite period of time. ETM (2) consisting of event-triggered impulse instants and forced impulse moments can effectively eliminate Zeno behavior, and it is clear from (4) that there is no upper bound on forced impulse instants in this paper. In addition, condition (5) provides a variable lower bound with respect to parameters ır, c, ς, ¯ır, ˉς on the neighboring event-triggered impulse instants. Whereas literature [28,35,36] gives a uniformly positive lower bound, which suggests that conditions in this paper have less conservatism.

    Remark 2. Due to the existence of the effect of exogenous interference, unlike literature [36], this paper introduces ϕ1(vc[t0,t]) to represent the potential effect of exogenous disturbance, leading to a difference from the proof of [37]. It is worth noting that ϕ1(vc[t0,t]) cannot be replaced by ϕ1(vc(t)). This is because the fact that Theorem 1 effectively rules out Zeno behavior, ϕ1(vc[t0,t]) and ϕ1(vc(t)) are not comparable in size; therefore, it is necessary to show the value of ϕ1 on this interval [t0,t].

    Theorem 2. Let conditions in Theorem 1 hold, and there exist functions α1, α2, ϕ2K,Vv0, constants ır, ˉır, ς, ˉς, r, ϖR+, rN+ satisfying:

    (i) α1(|z|)V(t,z)α2(|z|),

    (ii) V(tr,hr(z(trτ),vd(trτ)))exp(r)V(trτ,z(trτ))+ϕ2(|vd(trτ)|),

    (iii) ır, ˉır, ς, ˉςr, impulse strengths r and impulse instant tr satisfy:

    r+ır+1+ςτ>(ςˉς)(tr+1tr),
    lr=1(ımrmr)+ˉıml+ςmτϖ, l{1,2,,m1}, m2,

    then system (1) is ISS under ETM (2).

    Proof. It can be seen from ETM (2) that

    V(t,z(t))exp(ı1ς(tt0))V(t0,z(t0))+exp(ˉı1ˉς(tt0))ϕ1(vc[t0,t]), t[t0,t1).

    Using condition (ⅱ), for triggering instant t1, we gain

    V(t1,z(t1))=h1(z(t1τ),vd(t1τ))exp(1)V(t1τ,z(t1τ))+ϕ2(|vd(t1τ)|){exp(1+ı1ς(t1τt0))V+exp(1+ˉı1ˉς(t1τt0))ϕ1(vc[t0,t1]) +ϕ2(|vd(t1τ)|), t0t1τt1exp(1)V+ϕ2(|vd(t1τ)|), t1τt0exp(1+ı1ς(t1τt0))V+exp(1+ˉı1ˉς(t1τt0))ϕ1(vc[t0,t1])+ϕ2(|vd(t1τ)|),

    where V=supn[t0τ,t0]V(n,z(n)), and

    V(t,z(t))exp(ı2ς(tt1))V(t1,z(t1))+exp(ˉı2ˉς(tt1))ϕ1(vc[t1,t])exp(1+ı1+ı2ς(tτt0))V+exp(1+ˉı1+ı2ς(tt1)ˉς(t1τt0))ϕ1(vc[t0,t1])+exp(ı2ς(tt1))ϕ2(|vd(t1τ)|)+exp(ˉı2ˉς(tt1))ϕ1(vc[t1,t]), t[t1,t2).

    Similarly, at triggering instant t2,

    V(t2,z(t2))=h2(z(t2τ),vd(t2τ))exp(2)V(t2τ,z(t2τ))+ϕ2(|vd(t2τ)|){exp(12+ı1+ı2ς(t22τt0))V+exp(12+ˉı1+ı2ς(t2τt1) ˉς(t1τt0))ϕ1(vc[t0,t1])+exp(2+ı2ς(t2τt1))ϕ2(|vd(t1τ)|) +exp(2+ˉı2ˉς(t2τt1))ϕ1(vc[t1,t2])+ϕ2(|vd(t2τ)|), t1t2τt2exp(2+ı1ς(t2τt0))V+exp(2+ˉı1ˉς(t2τt0))ϕ1(vc[t0,t1]) +ϕ2(|vd(t2τ)|), t0t2τt1exp(2)V+ϕ2(|vd(t2τ)|), t2τt0exp(12+ı1+ı2ς(t22τt0))V+exp(12+ˉı1+ı2ς(t2τt1)ˉς(t1τt0))ϕ1(vc[t0,t1])+exp(2+ı2ς(t2τt1))ϕ2(|vd(t1τ)|)+exp(2+ˉı2ˉς(t2τt1))ϕ1(vc[t1,t2])+ϕ2(|vd(t2τ)|).

    Analogously,

    V(t,z(t))exp(ı3ς(tt2))V(t2,z(t2))+exp(ˉı3ˉς(tt2))ϕ1(vc[t2,t])exp(12+ı1+ı2+ı3ς(t2τt0))V+exp(12+ˉı1+ı2+ı3ς(tτt1)ˉς(t1τt0))ϕ1(vc[t0,t1])+exp(2+ı2+ı3ς(tτt1))ϕ2(|vd(t1τ)|)+exp(2+ˉı2+ı3ς(tt2)ˉς(t2τt1))ϕ1(vc[t1,t2])+exp(ı3ς(tt2))ϕ2(|vd(t2τ)|)+exp(ˉı3ˉς(tt2))ϕ1(vc[t2,t]), t[t2,t3).

    Repeating the above steps, one can derive that

    V(t,z(t))exp(ık+k1n=1(ınn)ς(t(k1)τ)t0)V+exp(ık+k1n=2(ınn)1+ˉı1ˉς(t1τt0)ς(t(k2)τt1)ϕ1(vc[t0,t1])+exp(ık+k1n=3(ınn)2+ˉı2ˉς(t2τt1)ς(t(k3)τt2)ϕ1(vc[t1,t2])+exp(ık+k1n=2(ınn)ς(t(k2)τt1)ϕ2(|vd(t1τ)|)+exp(ık+k1n=3(ınn)ς(t(k3)τt2)ϕ2(|vd(t2τ)|)++exp(ıkk1+ˉık1ˉς(tk1τtk2)ς(ttk1))ϕ1(vc[tk2,tk1])+exp(ıkς(ttk1))ϕ2(|vd(tk1τ)|)+exp(ˉıkˉς(tktk1)ϕ1(vc[tk1,t])), t(tk1,tk).

    Together with (ⅰ) and (ⅲ), we obtain

    α1(|z(t)|)exp(ϖ+ı)α2(ϵτ)exp(ς(tt0))+exp((ϖ+ı)ˉı)ϕ1(vc[t0,t])+exp(ϖ+ı)ϕ2(maxt0tkt|vd(tkτ)|),t(tk1,tk),

    where ı=supkN+{ık}, ˉı=supkN+{¯ık}, which confirms system (1) is ISS under ETM (2).

    Remark 3. It follows from proof of Theorem 2 that in order to ensure ISS of system (1), it is necessary to introduce forced impulse sequence into ETM (2). In other words, without a forced impulse instant, an event trigger may not occur or occur countless times, so this requires frequent occurrence of stable impulses. The average dwell time is often used to solve this problem in the previous literature, but it causes unnecessary waste. However, forced impulse time in this paper satisfies conditions of ETM (2) and does not necessarily need to occur continuously, reflecting the necessity of its existence.

    Remark 4. The ISS problem of nonlinear systems without delayed impulse based on event-triggered impulse control has been involved in [25,27,32]. When time delay in impulse is taken into account, overdispersion of system causes some trouble in description of delayed impulses. Therefore, the relationship among trigger parameters ır, ˉır, ς, ˉςr, impulse intensity r, and time delay τ is established under condition (iii) of Theorem 2 to overcome the influence of time delay.

    In this section, our presented event-triggered impulse control tactics are applied to nonlinear systems to achieve ISS.

    Considering the following systems with external disturbance:

    ˙z(t)=Λz(t)+Γ(z(t))+Υu(t)+v(t), ttr, tt0, (8)

    where Λ, Γ, ΥRn are given real matrices. u(t)Rm is the locally bounded interference input. satisfies globally Lipschitz with Lipschitz matrix M. The following Dirac control input is considered to stabilize system (8):

    v(t)=r=1Oz(t)δ(ttr), (9)

    where {tr}rN+ is impulse instant. O is the impulsive control gain matrix; in this circumstance, system (8) can be written in the underlying form:

    ˙z(t)=Λz(t)+Γ(z(t))+Υu(t), tt0, ttr,z(t)=(Ξ+O)z(tτ), t=tr, rN+, (10)

    where Ξ is the identity matrix.

    Theorem 3. If positive constants Θ, a1, a2, and matrix Ωn×n, Pn×n>0, diagonal matrix Kn×n>0, real matrix Xn×n satisfy:

    (ΛTΩ+ΩΛ+MTKMΘΩΩΓΩΥK0P)0, (11)
    (exp()ΩΩ+XΩ)0, (12)

    then, ISS is guaranteed for system (10) under impulsive control gain O=Ω1XT and ETM:

    tr=min{tr,tr1+r}, rN+,tr=inf{ttr1:Δ(t)0}, (13)

    with

    Δ(t)=zT(t)Ωz(t)a1zT(tr1)Ωz(tr1)a2λmax(P)u2[tr1,t].

    Proof. Select V(t)=zT(t)Ωz(t). By using the Ito formula, we obtain

    D+V(t)=2zT(t)Ω(Λz(t)+Γ(z(t))+Υu(t))=zT(t)(ΩΛ+ΛΩT)z(t)+2zT(t)ΩΓ(z(t))+2zT(t)ΩΥu(t),

    combined with Lemma 2, we conclude

    2zT(t)ΩΓz(t)=zT(t)ΩΓ(z(t))+T(z(t))ΓTΩz(t)zT(t)ΩΓK1ΓTΩz(t)+zT(t)MTKMz(t),
    2zT(t)ΩΥu(t)=zT(t)ΩΥu(t)+uT(t)ΥTΩz(t)zT(t)ΩΥP1ΥTΩz(t)+uT(t)Pu(t).

    Together with (11) and (12), it can be derived that

    D+V(t)ΘzT(t)Ωz(t)+λmax(P)|u(t)|2,

    and

    exp()Ω+(Ξ+O)TΩ(Ξ+O)0,

    which implies that

    V(z(tr))=zT(tr)Ωz(tr)zT(trτ)(Ξ+O)TΩ(Ξ+O)z(trτ)exp()zT(trτ)Ωz(trτ)=exp()V(z(trτ)).

    Similar to proof of Theorem 2, the ISS of system (10) is shown to hold under ETM (13).

    Remark 5. The ISS criterion given in Theorem 3 is based on the system being affected by delayed impulse and external interference. Moreover, the impulse control gain matrix is determined by the LMI method from the predetermined constants Θ and .

    Example 1. Let us consider underlying system:

    ˙z(t)=1.9sin(t)z(t)+vc(t), ttr, tt0,z(t)=exp(0.11)z(tτ)+vd(t), t=tr, rN+, (14)

    where vc(t) and vd(t) are external inputs for continuous and impulse parts, respectively. We select V(z(t))=z(t), c=10, ı=0.9, ς=0.5, ˉır=0.2, ˉς=0.11, vc(t)=sin(t), vd(t)=1/10cos(t). First, when forced impulse instant is not present, ETM is as follows:

    tr=inf{ttr1:|z(t)|exp(0.90.5(ttr1))V(tr1,z(tr1))+exp(0.20.11(ttr1))ϕ1(vc[tr1,t])}. (15)

    Through simulation (Figure 1), we find that system (14) fails to satisfy ISS under ETM (15). Hence, we will introduce the forced impulse sequence tr=tr1+5, then ETM will be designed as follows:

    tr=min{tr,tr1+5}, rN+,tr=inf{ttr1:|z(t)|exp(0.90.5(ttr1))V(tr1,z(tr1))+exp(0.20.11(ttr1))ϕ1(vc[tr1,t])}. (16)
    Figure 1.  State trajectory of system (14) without forced impulse instant.

    It follows from Theorem 1 that system (14) is ISS under ETM (16), and this is verified in Figure 2.

    Figure 2.  State trajectory of system (14) with forced impulse instant.

    Example 2. Now we consider system (10) with

    Λ=(0.691.10.790.3), Γ=(0.4100.18), Υ=(0.10.40.20.3),

    1(z(t))=2(z(t))=tanh(2z(t)), u(t)=(sin(t),cos(t))T, Figure 3 shows that when the impulse effect is not present, system (10) cannot reach ISS. So we will design ETM to make system (10) achieve ISS. We select a1=1.1052, a2=0.075, Θ=4.765 and =0.31. By using Matlab to solve LMI (11) and (12), then ETM is presented as follows:

    tr=min{tr,tr1+3}, rN+,tr=inf{ttr1:zT(t)Ωz(t)1.1052zT(tr1)Ωz(tr1)0.075λmax(P)u2[tr1,t]}, (17)

    where

    Ω=(22.42114.69964.699625.1256), P=(35.23660035.2366),
    K=(13.70925.44445.444419.7417), X=(31.38965.14815.148129.9487)

    and impulsive control gain

    O=Ω1XT=(1.50180.45560.48581.0782).

    According to Theorem 3, system (10) is ISS; see Figure 4. From the other side, with other parameters fixed, we only change impulsive control gain so that it does not satisfy conditions of Theorem 3, such as ˉO=(1523), as can be seen from Figure 5, system (10) is non-ISS, which shows the feasibility of our proposed event-triggered impulse control method.

    Figure 3.  State trajectory of system (10) without impulse.
    Figure 4.  State trajectory of system (10) under (17).
    Figure 5.  State trajectory of system (10) under (17) with ˉO.

    Remark 6. In Example 1, Figure 1 illustrates that when ETM (2) does not contain forced impulse instant, the system is not ISS. But when a forced impulse instant is introduced into ETM (2), the system reaches ISS (i.e., Figure 2). In other words, forced impulse instant plays a key role in ensuring ISS characteristics. In Example 2, Figure 3 demonstrates that when the impulse effect is not present, system (10) is unstable under external perturbations. Therefore, in order to enable system (10) to achieve ISS, ETM (17) and impulse control gain are designed and verified in Figure 3. Figure 4 shows that when impulse control gain changes, that is, conditions (11) and (12) are not satisfied, the system cannot achieve ISS under ETM (17), which shows the feasibility of our proposed event-triggered impulse control method.

    In this paper, ISS properties of nonlinear delayed impulse systems with hybrid inputs in the framework of event-triggered impulse control are investigated, and related criteria of the considered system are derived based on designed ETM, where Zeno behavior is excluded. Then the theoretical results are applied to nonlinear systems, and some sufficient conditions of ETM and impulse control gain are obtained by LMI. Finally, two simulation examples are given to demonstrate the rationality of theoretical results. However, due to time delay in the impulse part, only constant delay is considered, and the control mechanism in this paper is given in advance, which has limitations in application. Then, if it can be extended to multi-agent systems with actuation delay and a self-triggered impulse control method for group consensus of multi-agent systems with sensing/ actuation delays is considered, this is worth further study.

    Linni Li: writing-original draft; Jin-E Zhang: supervision, writing-review and editing. Both authors have read and approved the final version of the manuscript for publication.

    This work is supported by Hubei Province Education Science Planning (Grant No. 2023GA058) and the Research Project on HBNU Education and Teaching Reform (Grant No. 2023002).

    The authors declare no conflicts of interest.



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