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Research article

H-infinity bipartite consensus of multi-agent systems with external disturbance and probabilistic actuator faults in signed networks

  • Received: 28 August 2021 Accepted: 25 October 2021 Published: 05 November 2021
  • MSC : 93C57, 93C65

  • The H-infinity bipartite consensus problem is addressed for a class of linear multi-agent systems with external disturbance, where the positive and negative links are allowed in communication topology. A novel event-triggered communication scheme is presented to save limited network resources, which dependents on information from neighboring agents at event-triggered instants, the given event-triggered condition is detected only at discrete sampling times, thus Zeno behavior can be excluded, two types of event-triggered matrices have been introduced in our event-triggered communication scheme, which can further reduce the sampled-data transmission compared with some existed results. Considering the probabilistic actuator faults, the reliable controller is designed based on sampled-data, then a new distribution-based fault model is constructed by using coordinate transform. Some H-infinity bipartite consensus criteria can be derived by the Lyapunov stability theory and algebraic graph theory, at the same time, the feedback matrices and event-triggered matrices can be obtained by solving some linear matrix inequalities. Finally, a numerical example is employed to show the validity and advantage of the proposed transmission scheme.

    Citation: Hongjie Li. H-infinity bipartite consensus of multi-agent systems with external disturbance and probabilistic actuator faults in signed networks[J]. AIMS Mathematics, 2022, 7(2): 2019-2043. doi: 10.3934/math.2022116

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  • The H-infinity bipartite consensus problem is addressed for a class of linear multi-agent systems with external disturbance, where the positive and negative links are allowed in communication topology. A novel event-triggered communication scheme is presented to save limited network resources, which dependents on information from neighboring agents at event-triggered instants, the given event-triggered condition is detected only at discrete sampling times, thus Zeno behavior can be excluded, two types of event-triggered matrices have been introduced in our event-triggered communication scheme, which can further reduce the sampled-data transmission compared with some existed results. Considering the probabilistic actuator faults, the reliable controller is designed based on sampled-data, then a new distribution-based fault model is constructed by using coordinate transform. Some H-infinity bipartite consensus criteria can be derived by the Lyapunov stability theory and algebraic graph theory, at the same time, the feedback matrices and event-triggered matrices can be obtained by solving some linear matrix inequalities. Finally, a numerical example is employed to show the validity and advantage of the proposed transmission scheme.



    Recently, the distributed consensus control for multi-agent systems has received compelling attentions owing to its potential applications [1,2,3]. The main objective is to design distributed control protocol such that all agents can achieve an agreement. Generally speaking, the consensus problems can be divided into three types, leader-following consensus problem, which means a leader is designated and all the followers track the leader. Containment control is a consensus-like tracking problem with multiple leaders, the control target is to let the followers states finally converge to the convex hull spanned by the leaders. Leaderless consensus problem means all the agents can eventually converge to the weighted average value of all the agents. For the above three consensus problems, many fruitful results have been obtained for linear, nonlinear or stochastic multi-agent systems [4,5,6,7,8,9,10], and so on.

    It is noted that most of the existing results are focused on multi-agent systems with cooperative communication links, that is the elements of adjacency matrix are non-negative, however, the adjacency matrix with antagonistic links is very common in practical application to describe the competitive relationship among the agents [11,12]. Therefore, more and more attention has been paid to the signed networks with negative and positive elements [13,14,15,16,17,18,19] and the references therein. In [11], the concept of bipartite consensus is introduced for multi-agent systems with structurally balanced graph, all agents will reach a final state with opposite sign. The authors [13] have extended the concept of bipartite consensus to interval bipartite consensus, some interval bipartite consensus results are derived for structurally unbalanced networks. In [14], the distributed bipartite tracking consensus problem has studied for a class of linear multi-agent systems with a dynamic leader, where the leader's control inputs are allowed to be nonzero and unknown to each follower. In [15], a novel concept of node-to-node bipartite consensus is proposed, where the communication channels of the followers are assumed to be structurally balanced. For signed directed graphs, the reference [16] has designed two types of state feedback and dynamic output feedback control laws to achieve bipartite consensus, respectively. In [17], a pinning scheme is proposed for a class of coupled nonlinear systems with antagonistic interactions and switching topologies. Additionally, similar to bipartite consensus problem, the reverse group consensus is firstly studied in the cooperation-competition network [18], the results show that the couple group consensus can be achieved if the mirror graph is strongly connected, as an extension, the distributed stabilization problem is considered for multiple heterogeneous agents in the uncertain strong-weak completion network with exogenous disturbances [19].

    In practical multi-agent systems, each agent is equipped with micro-processor, it can collect information from neighboring agents, therefore, it is desired to implement actuating the controller updates on a digital platform [20], the scheduling can be done in a time-triggered scheme and an event-triggered scheme, where time-triggered scheme with a fixed sampling period, which should be selected to guarantee a desired performance under worst conditions, this kind of triggered method will lead to send many unnecessary sampling data to neighboring agents. Considering the limited network resources, the event-triggered scheme is an effective method to improve the resources utilization while ensuring a satisfactory performance [21,22]. Event-triggered bipartite leader-following consensus problems have been studied in [23,24,25,26], event-triggering condition is allowed to be intermittently examined at its own sampling instants in [23], a novel distributed protocol based on independent sampling period is presented. In [24], a novel event-triggered function is designed, where the continuous communication can be avoided and the Zeno-behavior can be excluded. In [25], the distributed static bipartite event-triggered controller and the fully distributed adaptive bipartite event-triggered controller are designed respectively, where the communication in both controller updating and triggered condition monitoring is intermittent, thus the communication resources can be greatly saved. In [26], by using pinning control strategies, a novel event-triggered controller is designed to achieve bipartite consensus. The refereances [27,28] discuss fully distributed bipartite output consensus of heterogeneous multi-agent systems, the fully distributed bipartite compensator and dynamic event-triggered mechanism are proposed in [27], where the proposed compensator is independent of any global information of the network topology. The reference [28] discusses the distributed bipartite finite-time event-triggered output consensus for heterogeneous linear multi-agent systems under directed signed communication topology, where a novel distributed bipartite compensator with intermittent communication mechanism is proposed in finite time. In [29], distributed event-triggered control strategy is proposed to guarantee the semi-global bipartite consensus. The reference [30] presents an even-triggered control framework to achieve bipartite consensus for networked Euler-Lagrange systems with external disturbance. In [31], event-triggered bipartite consensus is addressed under DoS attacks. Bipartite consensus of multi-agent systems with switching communication topologies is addressed in [32], where event-triggered conditions are piecewise functions depending on the variable couplings and topologies. However, the above schemes still exist some room for improvement. Inspired by [33,34,35], the next transmission instant is determined by tk+1h=tkh+min{eT(jkh)Φe(jkh)>δxT(tkh)Φx(tkh)}, where Φ is a symmetric positive definite matrix, which can be replaced by tk+1h=tkh+min{eT(jkh)Φ1e(jkh)>δxT(tkh)Φ2x(tkh)}, where Φ1 and Φ2 are two symmetric positive definite matrices, some comparisons are given in Section 4, it can be seen that our event-triggered scheme can lead to larger sampling period. The lower bound event interval is the sampling period h, which is strictly larger than zero, therefore, Zeno behavior is excluded in our proposed scheme.

    Furthermore, it is well known that actuators often suffer from faults inevitably in practical applications, which may degrade the performance of even cause instability [36,37]. In response to requirements for the reliability of multi-agent systems, some considerable works have been done on designing control schemes to accommodate actuator faults [38,39,40,41,42]. The leader-following consensus problem for multi-agent systems with actuator faults [38,39], actuator faults are time-varying[38], for two cases of the leader without control input and the leaders unknown bounded input, the distributed event-triggered fault-tolerant protocol is proposed to reach leader-following consensus. For a class of multi-agent systems against actuator faults and some perturbed factors as state-dependent uncertainties in [39], the distributed controllers is constructed to ensure leader-following consensus based on adaptive updates. In [40,41,42], the adaptive techniques are adopted to achieve the consensus of multi-agent systems with actuator faults. By the sliding mode control method, the reference [40] investigates the consensus tracking problem of second-order nonlinear multi-agent systems with disturbance. In [41], for a class of high-order nonlinear systems with intermittent actuator faults, a novel distributed adaptive controller is proposed to solve the output consensus tracking problem. In [42], for the actuator faults of partial loss of effectiveness fault and biased fault, a neural network-based adaptive consensus protocol is developed based on the Lyapunov analysis. In addition, the disturbance is inevitable and may degrade the performance in practical applications, H-infinity bipartite consensus problem is studied of nonlinear multi-agent systems with bounded disturbances in [43], where an performance criterion from bounded disturbances to the consensus error has been provided. In [44], the bipartite consensus controller is designed for cooperation-competition multi-agent systems with round-robin protocols such that the predetermined H-infinity bipartite consensus is satisfied over a given finite horizon. But in the above references, the event-triggered scheme and probabilistic actuator faults have not considered, to the best of the author's knowledge, no result has been reported for H-infinity bipartite consensus of multi-agent systems with event-triggered scheme and probabilistic actuator faults in signed networks, which motivates the present study.

    Motivated by the aforementioned discussion, this paper is devoted to investigate H-infinity bipartite consensus for a class of linear multi-agent systems with external disturbance in signed networks. The main contributions can be summarized as follows: (1) A novel concept of H-infinity bipartite consensus is introduced to quantify against the exogenous disturbance. (2) The proposed event-triggered scheme can ensure the desired performance while further reducing the frequency of data transmission, Zeno behavior is excluded owing to the lower bound of inter event interval is the sampling period. (3) The generalized random variables are introduced to describe probabilistic actuator failures, which represent the case of complete measurement failure, partial failure and complete normal of the actuator, but also including the case of the measured value of the actuator bigger than the real value.

    The remainder of this paper is organized as follows: In Section 2, some preliminaries are introduced. In Section 3, main results are presented for H-infinity bipartite consensus. A numerical simulation is provided to verify the theoretical results in Section 4. Some conclusions and future works are provided in Section 5.

    Notation Rn denotes the n-dimensional Euclidean space and Rn×m is a set of real n×m matrices. Notation . is the Euclidean norms of vector and matrix. If A is positive definite (or semi-definite), denote A>0 (or A0). Suppose that matrix MRn×n is a real symmetric matrix, λmax(M) and λmin(M) denote the maximum and minimum eigenvalues of matrix M, respectively. The notation means the Kronecker product. diag{} stands for a block-diagonal matrix. The superscript 1n(0n) indicates the n-dimensional column vector with each entry being 1(0). sgn() is the standard sign function. E() stands the mathematical expectation of random variable.

    The communication topology can be described as a signed graph g=(v,ε,A), where v=(v1,v2,,vN) denotes a set of vertices, εv×v is a set of edges, A=(aij)N×N denotes a weighted adjacency matrix representing the communication topology, where the entry aij of the matrix A can be allowed to negative and positive, aij>0 indicating node i and node j are cooperative relationship, if aij<0 indicating node i and node j are competitive relationship, otherwise, aij=0 means node i and node j have no information communication. The Laplacian matrix of the signed graph g can be defined as L=(lij)N×N, where lii=k=1,ki|aik|, and lij=aij (ij). A signed graph g is called structurally balance if the node set v can be divided into two sub-networks V1 and V2, which satisfy V1V2=v and V1V2=Φ, aij0 holds for any i,jVp, p{1,2} and aij<0 holds for all iVq, jVr, where qr, otherwise, the signed graph g is called structurally unbalance.

    Consider a group of N identical agents with general linear dynamics, in which the dynamics of agent i is described as follow:

    ˙xi(t)=Axi(t)+Bui(t)+Dwi(t)(i=1,2,,N), (2.1)

    where xi(t)Rn, ui(t)Rn and wi(t)Rq represent the system state, control input and external disturbance of the ith agent, respectively. ARn×n, BRn×m and DRn×q are some known constant matrices with compatible dimensions.

    In what follows, some key lemmas are summarized, which play the important roles to derive the main results.

    Lemma 1. [11] Suppose that signed network g is structurally balance, if and only if there is a gauge transformation W such that WTAW=ˉA has all nonnegative entries, where a gauge transformation is a change of orthant order by W=diag{w1,w2,,wN} with wi{1,1}, A=(aij)N×N and ˉA=(|aij|)N×N are the adjacency matrices of the signed and unsigned networks, respectively. In addition, W provides a partition, that is V1={vi|wi=1} and V2={vi|wi=1}.

    Lemma 2. [45] If x(t):(a,b)Rn is absolutely continuous function satisfying x(a)=0 and MRn×n is a positive definite matrix, then the following wirtinger's inequality holds:

    baxT(s)Mx(s)ds4(ba)2π2ba˙xT(s)M˙x(s)ds. (2.2)

    Lemma 3. [46] It is assumed that there exists a positive definite matrix MRn×n and a vector function x(t):(a,b)Rn, the following integrations are well defined, then

    (ba)baxT(s)Mx(s)ds[bax(s)ds]TM[bax(s)ds]. (2.3)

    Lemma 4. [47] For any two real vector functions y1(t)Rn and y2(t)Rn, a positive definite matrix RRn×n and any matrix SRn×n, then

    1αyT1(t)Ry1(t)+11αyT2(t)Ry2(t)yT(t)[RSTSR]y(t), (2.4)

    where y(t)=[y1(t)y2(t)], [RSTSR]>0 and 0<α<1.

    Lemma 5. [48] The following linear matrix inequality

    S=[S11S12S21S22]>0,

    where S11=ST11, S12=ST21, S22=ST22 are some constant matrices with appropriate dimensions, the following matrix inequalities hold:

    (i)S11>0,S22S21S111S12>0,(ii)S22>0,S11S12S122S21>0.

    For reducing the communication burden among the agents, and considering the unreliable channel from control to actuator, the sampled control algorithm is designed as follow:

    ui(t)=cΞKNj=1|aij|[xi(tkh)sgn(aij)xj(tkh)](i=1,2,,N;t[tkh,tk+1h);kZ+), (2.5)

    where c>0 is the coupling strength, Ξ=diag{Ξ1,Ξ2,,Ξm} with Ξi being m unrelated random variables, taking on the interval [0,θ] with θ1. KRm×n is the feedback matrix to be designed. tkh (k=0,1,2,) is the release times, t0h=0, {t0,t1,}{0,1,2,}, the data will be updated until next event-triggered instant t=tk+1h.

    Remark 1. Inspired by some related literatures [49,50], the random variable Ξ is used to describe the actuator fault. For the case of Ξ=0, it means complete failure of the ith actuator. For Ξ(0,1), it means partial failure of the ith actuator. For the case of Ξ=1, it means the ith actuator is in good working condition. For Ξ>1, it means the data distortion with the measurement of the ith actuator.

    Assumption 1. Supposed that mathematical expectation of Ξi (i=1,2,,m) is αi, the variance of Ξi is δ2i, denoted as E(Ξi)=αi and D(Ξi)=δ2i, respectively.

    Substituting (2.5) into (2.1), one has

    ˙xi(t)=Axi(t)cBΞKNj=1|aij|[xi(tkh)sgn(aij)xj(tkh)]+Dwi(t). (2.6)

    Based on the definition of Laplacian matrix, Eq (2.6) can be rewritten as

    ˙xi(t)=Axi(t)cBΞKNj=1lijxj(tkh)+Dwi(t). (2.7)

    Considering limited bandwidth of the communication network, to further reduce the data transmission among the agents, the event-triggered communication scheme is proposed for system (2.1), which is utilized to determine whether or not the current sampled data should be transmitted to neighboring agents. Supposed that the latest transmitted data is x(tkh), then for i=2,3,,N, the next transmission instant tk+1h can be determined by

    tkh+min{lh|[ei(tkh+lh)ei(tkh)]TΦ(1)i[ei(tkh+lh)ei(tkh)]>σieTi(tkh+lh)Φ(2)iei(tkh+lh)}, (2.8)

    where the error ei(t)=wixi(t)w1x1(t), Φ(1)i and Φ(2)i are some positive definite event-triggered matrices to be designed, σi>0 is event-triggered parameter, tk+1htkh denotes the release period which corresponds to the sampling period given by the event-triggered scheme.

    Remark 2. Noted that the sampled state x(tkh) satisfying the inequality (2.8) will be sent to the neighbour agents, some of the sampled states that violate (2.8) will not be transmitted. Obviously, the communication burden of the network is reduced, the corresponding transmission energy can also be saved.

    Remark 3. The above event-triggered communication scheme (2.8) includes the following special cases: (i) if Φ(1)i=Φ(2)i=Φi (i=2,3,,N), the scheme shrinks to a discrete event-triggered transmission scheme. (ii) if σi=0, one has tk+1h=tkh+h, then transmission scheme shrinks to a periodic transmission scheme. (iii) if Φ(1)i=Φ(2)i=In (i=2,3,,N), transmission scheme becomes a discrete absolute error-based transmission scheme. Hence the proposed event-triggered communication scheme includes some existing schemes. The framework of the event-triggered communication can be found in Figure 1.

    Figure 1.  The framework of event-triggered communication between agent i and j.

    Remark 4. The proposed transmission scheme (2.8) is different from a continuous absolute error-based needed to monitor the continuous measurement, where only the sampled-data is used, the lower bound event interval is the sampling period h, which is strictly larger than zero, therefore, Zeno behavior is excluded in our proposed scheme.

    Let ˉxi(t)=wixi(t) (i=1,2,,N), here wi=1 (iV1) and wi=1 (iV2), it follows from (2.7) that

    ˙ˉxi(t)=Aˉxi(t)cBΞKNj=1ˉlijˉxj(tkh)+wiDwi(t), (2.9)

    where ˉL=(ˉlij)N×N is the Laplacian matrix of unsigned graph with zero-row-sum, ˉlii=k=1,ki|aik|, ˉlij=wilijwj=|aij| (ij).

    In views of (2.9) and ei(t)=ˉxi(t)ˉx1(t) (i=2,3,,N), one has

    ˙ei(t)=Aei(t)cBΞKNj=2(ˉlijˉl1j)ej(tkh)+wiDwi(t)w1Dw1(t). (2.10)

    Inspired by [34,35], the interval [tkh,tk+1h) can be expressed as the union of several subintervals as follow:

    [tkh,tk+1h)=tk+11l=0[tkh+lh,tkh+lh+h). (2.11)

    Define τ(t)=t(tkh+lh), for t[tkh+lh,tkh+lh+h), it can be derived that 0τ(t)<h, let ˉei(tkh+lh)=ei(tkh+lh)ei(tkh) (i=2,3,,N), we have

    ei(tkh)=ei(tτ(t))ˉei(tkh+lh). (2.12)

    Applying (2.12) into (2.10), one has

    ˙ei(t)=Aei(t)cBΞKNj=2(ˉlijˉl1j)[ej(tτ(t))ˉej(tkh+lh)]+wiDwi(t)w1Dw1(t). (2.13)

    Rewrite (2.13) in compact matrix form, we can get

    ˙e(t)=(IN1A)e(t)c(ˆLBΞK)e(tτ(t))+c(ˆLBΞK)ˉe(tkh+lh)+(ˉWD)w(t)(1N1w1D)w1(t), (2.14)

    where

    e(t)=[eT2(t),eT3(t),,eTN(t)]T,ˉW=diag{w2,w3,,wN},w(t)=[wT2(t),wT3(t),,wTN(t)]T,ˆL=(ˆlpq)R(N1)×(N1),ˆlpq=ˉl(p+1)×(q+1)ˉl1×(q+1)(p,q=1,2,,N1),1N1=[1,1,,1N1]T.

    Definition 1. For signed networks g, H-infinity bipartite consensus can be achieved for coupled linear system (2.1), if for given a weighting positive-definite matrix SRn×n, a performance index γ>0 and the initial disagreement vector e(0), its solution satisfies

    E{0eT(t)e(t)dt}γE{0ˉwT(t)ˉw(t)dt+eT(0)(IN1S)e(0)}. (2.15)

    Definition 2. For given function V:CbF0([τM,0],Rn)×S, its infinitesimal operator L is defined as

    LV(t)=limΔ0+E(V(xt+Δ)|xt)V(xt)Δ. (2.16)

    In this section, H-infinity bipartite leaderless consensus problem is investigated under event-triggered scheme, supposed that the topology is directed signed graph and structurally balance.

    Let ˉΞ=diag{α1,α2,,αm}=mi=1αiCi, here Ci=diag{0,0,,0i1,1,0,,0mi}, then system (2.14) can be formulated as follow:

    ˙e(t)=(IN1A)e(t)c(ˆLBˉΞK)e(tτ(t))+c(ˆLBˉΞK)ˉe(tkh+lh)c[ˆLB(ΞˉΞ)K]×e(tτ(t))+c[ˆLB(ΞˉΞ)K]ˉe(tkh+lh)+(ˉWD)w(t)(1N1w1D)w1(t). (3.1)

    Combining (2.8) and (2.12), for t[tkh,tk+1h), the event-triggered scheme can be rewritten as

    [ei(tkh+lh)ei(tkh)]TΦ(1)i[ei(tkh+lh)ei(tkh)]<σieTi(tτ(t))Φ(2)iei(tτ(t)). (3.2)

    From the above analysis, it can be known from (3.2) that the current sampled data ei(tkh+lh) will not be sent, which will be employed in the following consensus analysis.

    By using Kronecher product, it can be derived from (3.2) that

    ˉeT(tkh+lh)Φ(1)ˉe(tkh+lh)<eT(tτ(t))(σIn)Φ(2)e(tτ(t)), (3.3)

    where

    Φ(1)=diag{Φ(1)2,Φ(1)3,,Φ(1)N},Φ(2)=diag{Φ(2)2,Φ(2)3,,Φ(2)N},σ=diag{σ2,σ3,,σN}.

    Theorem 1. Suppose that signed network is directed and structurally balance, for given sampled period h>0, triggered parameters σi>0 (i=2,3,,N), coupled strength c>0, feedback matrix KRn×n, and a disturbance attenuation γ>0, H-infinity bipartite consensus can be achieved in system (2.1) under the control algorithm (2.5) and event-triggered scheme (2.8), if there exist some n×n positive definite matrices P>0, Q>0, R>0, Ω>0, Φ(1)>0, Φ(2)>0, and matrix URn×n, such that the following matrix inequalities hold:

    Σ=[ΓhA(IN1R)1hA0(IN1Ω)1hcB00˜RhcB000˜Ω]<0, (3.4)
    [RUR]>0, (3.5)

    where

    Γ=[Γ11Γ21Γ22Γ31Γ32Γ33Γ4100Φ(1)Γ51000π24(IN1Ω)Γ61000012γI(N1)qΓ710000012γIq],Γ11=IN1ATP+IN1QIN1Rπ24(IN1Ω)+12ITN1P,Γ21=c(ˆLTKTΞTBT)(IN1P)+ITN1(RU),Γ22=IN1(U+UT2R)+(σIn)Φ(2),Γ31=IN1U,Γ32=IN1(RU),Γ33=IN1(Q+R),Γ41=c(ˆLTKTΞTBT)(IN1P),Γ51=π24(IN1Ω),Γ61=(ˉWTDT)(IN1P),Γ71=(1TN1DTw1)(IN1P),A=[IN1Ac(ˆLBˉΞK)0c(ˆLBˉΞK)0ˉWD1N1w1D],B=[0δ1(ˆLBC1K)0δ1(ˆLBC1K)0000δ2(ˆLBC2K)0δ2(ˆLBC2K)0000δm(ˆLBCmK)0δm(ˆLBCmK)000],˜R=diag{(IN1R)1,(IN1R)1,,(IN1R)1m},˜Ω=diag{(IN1Ω)1,(IN1Ω)1,,(IN1Ω)1m}.

    Proof. Construct the following Lyapunov function candidate

    V(t)=4i=1Vi(t), (3.6)

    where

    V1(t)=eT(t)(IN1P)e(t),V2(t)=ttheT(s)(IN1Q)e(s)ds,V3(t)=htthts˙eT(v)(IN1R)˙e(v)dvds,V4(t)=h2ttkh+lh˙eT(s)(IN1Ω)˙e(s)dsπ24ttkh+lh[e(s)e(tkh+lh)]T(IN1Ω)[e(s)e(tkh+lh)]ds,

    where P,Q,R,ΩRn×n>0.

    Next, some necessary explanations are given to show the Lyapunov function V4(t) is valid. By using the Wirtinger's inequality in Lemma 2, one has

    h2ttkh+lh˙eT(s)(IN1Ω)˙e(s)ds=h2ttkh+lh[˙e(s)˙e(tkh+lh)]T(IN1Ω)[˙e(s)˙e(tkh+lh)]dsh2π24[t(tkh+lh)]2ttkh+lh[e(s)e(tkh+lh)]T(IN1Ω)[e(s)e(tkh+lh)]dsπ24ttkh+lh[e(s)e(tkh+lh)]T(IN1Ω)[e(s)e(tkh+lh)]ds. (3.7)

    It can be easily derived that V4(t)0 from (3.7), thus the Lyapunov function V4(t) is valid.

    For convenient description, Eq (3.1) can be rewritten as the following concise form:

    ˙e(t)=A1ξ1(t)+A2ξ2(t), (3.8)

    where

    A1=[IN1AcˆLBˉΞKcˆLBˉΞKˉWD1N1w1D],A2=[cˆLB(ΞˉΞ)KcˆLB(ΞˉΞ)K],ξT1(t)=[eT(t)eT(tτ(t))ˉeT(tkh+lh)wT(t)wT1(t)],ξT2(t)=[eT(tτ(t))eT(tkh+lh)].

    By using the fact E{ΞˉΞ}=0, and infinitesimal operator (2.16) in Definition 2, taking the derivative of Vi(t) (i=1,2,3,4) along the trajectories (3.8), one gets

    E{LV1(t)}=E{2eT(t)(IN1P)(A1ξ1(t)+A2ξ2(t))}=E{2eT(t)(IN1P)A1ξ1(t)}, (3.9)
    E{LV2(t)}=E{eT(t)(IN1Q)e(t)eT(th)(IN1Q)e(th)}, (3.10)
    E{LV3(t)}=E{h2˙eT(t)(IN1R)˙e(t)htth˙eT(s)(IN1R)˙e(s)ds}, (3.11)
    E{LV4(t)}=E{h2˙eT(t)(IN1Ω)˙e(t)π24[e(t)e(tkh+lh)]T(IN1Ω)[e(t)e(tkh+lh)]}. (3.12)

    For any τ(t)[0,h), it follows from Jensen's inequality in Lemma 3 and the reciprocally convex approach in Lemma 4 that

    E{htth˙eT(s)(IN1R)˙e(s)ds}=E{httτ(t)˙eT(s)(IN1R)˙e(s)dshtτ(t)th˙eT(s)(IN1R)˙e(s)ds}E{hτ(t)[e(t)e(tτ(t))]T(IN1R)[e(t)e(tτ(t))]htτ(t)[e(tτ(t))e(th)]T(IN1R)[e(tτ(t))e(th)]}E{[e(t)e(tτ(t))e(tτ(t))e(th)]T(IN1[RUTUR])[e(t)e(tτ(t))e(tτ(t))e(th)]}=E{[e(t)e(tτ(t))e(th)]T(IN1[RUTRUTR+U2RUUTUTRUURR])[e(t)e(tτ(t))e(th)]}. (3.13)

    It can be derived from (3.12) that

    E{π24[e(t)e(tkh+lh)]T(IN1Ω)[e(t)e(tkh+lh)]}=E{π24[e(t)e(tkh+lh)]T(IN1[ΩΩΩΩ])[e(t)e(tkh+lh)]}. (3.14)

    Recalling (3.8), (3.11) and (3.12), we can obtain

    E{h2˙eT(t)[IN1(R+Ω)]˙e(t)}=E{h2[A1ξ1(t)+A2ξ2(t)]T[IN1(R+Ω)][A1ξ1(t)+A2ξ2(t)]}=E{h2ξT1(t)AT1[IN1(R+Ω)]A1ξ1(t)+h2ξT2(t)AT2[IN1(R+Ω)]A2ξ2(t)}=E{h2ξT1(t)AT1[IN1(R+Ω)]A1ξ1(t)}+h2c2E{mj=1δ2jeT(tτ(t))(ˆLTKTCTjBT)[IN1(R+Ω)](ˆLBCjK)e(tτ(t))}2h2c2E{mj=1δ2jeT(tτ(t))(ˆLTKTCTjBT)[IN1(R+Ω)](ˆLBCjK)ˉe(tkh+lh)}+h2c2E{mj=1δ2jˉeT(tkh+lh)(ˆLTKTCTjBT)[IN1(R+Ω)](ˆLBCjK)ˉe(tkh+lh)}, (3.15)

    where Cj=diag{0,0,,0j1,1,0,,0mj}.

    Combing Eqs (3.9–3.15), one gets

    E{LV(t)}E{ˉξT(t)Γˉξ(t)+h2ξT1(t)AT1[IN1(R+Ω)]A1ξ1(t)+h2c2mj=1δ2jeT(tτ(t))(ˆLTKTCTjBT)[IN1(R+Ω)](ˆLBCjK)e(tτ(t))2h2c2mj=1δ2jeT(tτ(t))(ˆLTKTCTjBT)[IN1(R+Ω)](ˆLBCjK)ˉe(tkh+lh)+h2c2mj=1δ2jˉeT(tkh+lh)(ˆLTKTCTjBT)[IN1(R+Ω)](ˆLBCjK)ˉe(tkh+lh)ˉeT(tkh+lh)Φ(1)ˉe(tkh+lh)+eT(tτ(t))(σIn)Φ(2)e(tτ(t))+12eT(t)(IN1P)e(t)12γˉwT(t)ˉw(t)12eT(t)(IN1P)e(t)+12γˉwT(t)ˉw(t)}, (3.16)

    where

    ˉξT(t)=[eT(t)eT(tτ(t))eT(th)ˉeT(tkh+lh)eT(tkh+lh)wT(t)wT1(t)],ˉwT(t)=[wT1(t)wT2(t)wTn(t)],Γ=[Γ11Γ21Γ22Γ31Γ32Γ33Γ4100Φ(1)Γ51000π24(IN1Ω)Γ61000012γIN1Γ710000012γ],

    and the other elements can be found in Theorem 1.

    By using Schur complement in Lemma 5 to (3.4), we can obtain (3.16), then

    E{LV(t)}E{12eT(t)(IN1P)e(t)+12γˉwT(t)ˉw(t)}. (3.17)

    Next, integrating both sides of Eq (3.17) from 0 to , one has

    E{0eT(t)e(t)dt}<γE{0ˉwT(t)ˉw(t)dt+V(0)}, (3.18)

    where γ=2λmin(P), which indicates H-infinity bipartite consensus is achieved by using Definition 1. This completes the proof.

    Notice that if σi=0 (i=2,3,,N), then event-triggered scheme reduces to time-triggered scheme, from Theorem 1, we can obtain H-infinity bipartite consensus under sampled-data control.

    Corollary 1. Suppose that signed network is directed and structurally balance, for given sampled period h>0, coupled strength c>0, feedback matrix KRn×n, and a disturbance attenuation γ>0, H-infinity bipartite consensus can be achieved in system (2.1) under the control algorithm (2.5), if there exist some n×n positive definite matrices P>0, Q>0, R>0, Ω>0 and matrix URn×n, such that the following matrix inequalities hold:

    ˉΣ=[ˉΓhˉA(IN1R)1hˉA0(IN1Ω)1hcˉB00˜RhcˉB000˜Ω]<0, (3.19)
    [RUR]>0, (3.20)

    where

    ˉΓ=[Γ11ˉΓ21Γ22Γ31Γ32Γ33Γ4100π24(IN1Ω)Γ5100012γI(N1)qΓ61000012γIq],Γ11=IN1ATP+IN1QIN1Rπ24(IN1Ω)+12ITN1P,ˉΓ21=c(ˆLTKTΞTBT)(IN1P)+ITN1(RU),Γ22=IN1(U+UT2R),Γ31=IN1U,Γ32=IN1(RU),Γ33=IN1(Q+R),Γ41=π24(IN1Ω),Γ51=(ˉWTDT)(IN1P),Γ61=(1TN1DTw1)(IN1P),˜R=diag{(IN1R)1,(IN1R)1,,(IN1R)1m},˜Ω=diag{(IN1Ω)1,(IN1Ω)1,,(IN1Ω)1m},ˉA=[IN1Ac(ˆLBˉΞK)00WD1N1w1D],ˉB=[0δ1(ˆLBC1K)00000δ2(ˆLBC2K)00000δm(ˆLBCmK)0000].

    Remark 5. When σi0+, it can be concluded that (3.3) can not be satisfied, the data of each sampling time will be transmitted to the neighbor agents, that is, event-triggered scheme reduces to time-triggered scheme, thus bipartite leaderless consensus can be derived based on the sampled control algorithm.

    In the following, we will design the reliable protocol to achieve H-infinity bipartite consensus for multi-agent system (2.1) with probabilistic actuator faults.

    Theorem 2. Suppose that signed network is directed and structurally balance, for given sampled period h>0, triggered parameters σi>0 (i=2,3,,N), coupled strength c>0, any a positive scalar ε>0, and a disturbance attenuation γ>0, H-infinity bipartite consensus can be achieved in system (2.1) under the control algorithm (2.5) and event-triggered scheme (3.3), if there exist some positive definite matrices X>0, ˆQ>0, ˆR>0, ˆΩ>0, ˆΦ(1)=diag{XˆΦ(1)2X,XˆΦ(1)3X,,XˆΦ(1)NX}>0, ˆΦ(2)=diag{XˆΦ(2)2X,XˆΦ(2)3X,,XˆΦ(2)NX}>0, and matrix ˆURn×n, YRm×n, such that the following linear matrix inequalities hold:

    ˆΣ:[ˆΓhˆA2ε(IN1X)+ε2(IN1ˆR)hˆA02ε(IN1X)+ε2(IN1ˆΩ)hcˆB00ˇRhcˆB000ˇΩ]<0, (3.21)
    [ˆRˆUˆR]>0, (3.22)

    where

    ˆB=[0δ1(ˆLBC1)(IN1Y)0δ1(ˆLBC1)(IN1Y)0000δ2(ˆLBC2)(IN1Y)0δ2(ˆLBC2)(IN1Y)0000δm(ˆLBCm)(IN1Y)0δm(ˆLBCm)(IN1Y)000],ˆΓ=[ˆΓ11ˆΓ21ˆΓ22ˆΓ31ˆΓ32ˆΓ33ˆΓ4100ˆΦ1π24(IN1ˆΩ)000π24(IN1ˆΩ)WTDT000012γI(N1)q1TN1DTw10000012γIq],ˆΓ11=IN1AT+IN1ˆQIN1ˆRπ24(IN1ˆΩ)+12(IN1X),ˆΓ21=c(IN1YT)(ˆLTˉΞTBT)+IN1(ˆRˆU),ˆΓ22=IN1(ˆU+ˆUT2ˆR)+(σIn)ˆΦ2,ˆΓ31=IN1ˆU,ˆΓ32=IN1(ˆRˆU),ˆΓ33=IN1(ˆR+ˆQ),ˆΓ41=c(IN1YT)(ˆLTˉΞTBT),ˇR=diag{2ε(IN1X)+ε2(IN1ˆR),,2ε(IN1X)+ε2(IN1ˆR)m},ˇΩ=diag{2ε(IN1X)+ε2(IN1ˆΩ),,2ε(IN1X)+ε2(IN1ˆΩ)m},ˆA=[IN1AXc(ˆLBˉΞ)(IN1Y)0c(ˆLBˉΞ)(IN1Y)0ˉWD1N1w1D],

    then the feedback matrix K=YX1.

    Proof. Denote X=P1, ˆQ=XQX, ˆR=XRX, ˆΩ=XΩX, ˆU=XUX, ˆΦ(1)=diag{XˆΦ(1)2X,XˆΦ(1)3X,,XˆΦ(1)NX}, ˆΦ(2)=diag{XˆΦ(2)2X,XˆΦ(2)3X,,XˆΦ(2)NX} and Y=KX, then pre-multiplying and post-multiplying Eq (3.4) with

    X=diag{IN1X,IN1X,IN1X,IN1X,IN1X5,I,I,,I2m+2}. (3.23)

    Due to the fact

    [IN1ˆRε1(IN1X)]T(IN1ˆR)[IN1ˆRε1(IN1X)]0, (3.24)

    it can be derived from (3.23) that

    (IN1X)T(IN1ˆR)1(IN1X)2ε(IN1X)+ε2(IN1ˆR), (3.25)

    then

    (IN1R)1=(IN1X)T[(IN1X)(IN1R)(IN1X)]1(IN1X)=(IN1X)T(IN1ˆR)1(IN1X)2ε(IN1X)+ε2(IN1ˆR). (3.26)

    Similar to Eq (3.25), we have

    (IN1Ω)12ε(IN1X)+ε2(IN1ˆΩ). (3.27)

    Replace the term ˜R=diag{(IN1R)1,(IN1R)1,,(IN1R)1m} by the following matrix

    ˇR=diag{2ε(IN1X)+ε2(IN1ˆR),,2ε(IN1X)+ε2(IN1ˆR)m}. (3.28)

    Replace the term ˜Ω=diag{(IN1Ω)1,(IN1Ω)1,,(IN1Ω)1m} by the following matrix

    ˇΩ=diag{2ε(IN1X)+ε2(IN1ˆΩ),,2ε(IN1X)+ε2(IN1ˆΩ)m}. (3.29)

    Combining (3.22–3.28), then Eqs (3.21) and (3.22) can be obtained. This completes the proof.

    Corollary 2. Suppose that signed network is directed and structurally balance, for given sampled period h>0, coupled strength c>0, any a positive scalar ε>0, and a disturbance attenuation γ>0, H-infinity bipartite consensus can be achieved in system (2.1) under the control algorithm (2.5), if there exist some positive definite matrices X>0, ˆQ>0, ˆR>0, ˆΩ>0, and matrix ˆURn×n, YRm×n, such that the following linear matrix inequalities hold:

    ˘Σ:[˘Γh˘A2ε(IN1X)+ε2(IN1ˆR)h˘A02ε(IN1X)+ε2(IN1ˆΩ)hc˘B00ˇRhc˘B000ˇΩ]<0, (3.30)
    [ˆRˆUˆR]>0, (3.31)

    where

    then the feedback matrix K=YX1.

    Consider the following linear multi-agent systems consisting of seven agents

    ˙xi(t)=Axi(t)+Bui(t)+Dwi(t)(i=1,2,,7), (4.1)

    where

    xi(t)=[xi1(t)xi2(t)xi3(t)],A=[0.55981.3018011100.01350.0297],B=[0.44220.17613.54467.59225.52004.4900],D=[0.0010.0010.002],wi(t)=0.001sin(5t).

    The network topology is structurally balance in Figure 2, which can be divided into two sub-networks V1={1,2,3,4} and V2={5,6,7}, the agents are cooperative relationship in V1 or V2, the agents are competitive relationship between V1 and V2, by using Lemma 1, we can obtain the gauge transformation W=diag{1,1,1,1,1,1,1}, then we have w1=1 and ˉW=diag{1,1,1,1,1,1}.

    Figure 2.  Illustration for the communication topology.

    Case 1: Event-triggered matrices Φ(1)Φ(2)

    Let the coupling strength c=1, the sampling period h=0.01, event-triggered parameter σi=0.01 (i=2,3,,7), H-infinity performance index γ=0.001, the positive scale ε=0.01, the mathematical expectation ˉΞ=diag{0.5,0.1}, and the variance δ1=0.1, δ2=0.2, by using Theorem 2, the related matrices can be obtained, which means bipartite leaderless consensus can be achieved, the event-triggered matrices Φ(1)i and Φ(2)i (i=2,3,,7) is given as follows:

    Φ(1)2=[1.43300.01580.00260.01581.44510.00610.00260.00611.4659],Φ(2)2=[1.46150.01550.00710.01551.45020.00670.00710.00671.4731],Φ(1)3=[1.35970.03140.00450.03141.38840.01160.00450.01161.4278],Φ(2)3=[1.29260.02030.00880.02031.30320.00800.00880.00801.2745],Φ(1)4=[1.35930.03070.00450.03071.38720.01120.00450.01121.4245],Φ(2)4=[1.29250.02040.00880.02041.30300.00810.00880.00811.2741],Φ(1)5=[1.37770.05910.00830.05911.43280.02240.00830.02241.5105],Φ(2)5=[1.29580.01740.00700.01741.30530.00810.00700.00811.2777],Φ(1)6=[1.36120.03380.00480.03381.39250.01280.00480.01281.4365],Φ(2)6=[1.29340.01910.00860.01911.30500.00750.00860.00751.2790],Φ(1)7=[1.35960.03110.00450.03111.38800.01150.00450.01151.4265],Φ(2)7=[1.29250.02040.00890.02041.30300.00810.00890.00811.2740],

    then the feedback gain can be obtained

    K=[0.02090.03590.07560.12910.16490.1996], (4.2)

    taking t[0,20), the simulation results show that only 38 sampled data are sent out, which take 1.9% of the sampled signals. It can be computed that the average sampling period is 0.5263 by our proposed event-triggered scheme. The release instants and release intervals are illustrated in Figure 3. The curve of xij(t) (i=1,2,,7,j=1,2,3) are presented in Figure 4, it can be seen H-infinity bipartite consensus is achieved. In order to show the benefits of our proposed triggered scheme than [34,35], some comparisons are given in Table 1, it can be seen that our event-triggered scheme can lead to larger sampling period h.

    Figure 3.  The release instants and release intervals under the event-triggered scheme for event-triggered matrices Φ(1)Φ(2).
    Figure 4.  The trajectories of the state xij(t)(i=1,2,,7;j=1,2,3) for H bipartite consensus for event-triggered matrices Φ(1)Φ(2).
    Table 1.  The upper bound of sampling period h for bipartite leaderless consensus (i=2,3,,7).
    Trigger scheme Trigger matrix Coupling strength Trigger parameter Upper bound of h
    Our scheme Φ(1)iΦ(2)i c=1 σi=0.01 h=0.8292
    [34,35] Φ(1)i=Φ(2)i c=1 σi=0.01 h=0.8281

     | Show Table
    DownLoad: CSV

    Case 2: Event-triggered matrices Φ(1)=Φ(2)

    Suppose that the dynamics of linear multi-agent systems and the related parameters are the same with Case 1. By using Theorem 2, the event-triggered matrix Φi (i=2,3,,7) can be obtained as follows:

    Φ2=[1.32770.00870.00170.00871.35030.00270.00170.00271.3580],Φ3=[1.33500.02020.00020.02021.36880.00710.00020.00711.3920],Φ4=[1.33460.01950.00030.01951.36760.00660.00030.00661.3887],Φ5=[1.35400.04870.00430.04871.41320.01730.00430.01731.4737],Φ6=[1.33690.02310.00010.02311.37370.00850.00010.00851.4027],Φ7=[1.33480.01990.00020.01991.36830.00690.00020.00691.3906],

    then the feedback gain can be obtained

    K=[0.02060.03550.01460.12750.16280.1970]. (4.3)

    Taking t[0,20), the simulation results show that only 106 sampled data are sent out, which take 5.3% of the sampled signals. Moreover, it can be computed that our event-triggered scheme can obtain a average sampling period of 0.1887, the release instants and release intervals are illustrated in Figure 5. The curve of xij(t) (i=1,2,,7;j=1,2,3) are presented in Figure 6, which can be seen H bipartite consensus is achieved.

    Figure 5.  The release instants and release intervals under the event-triggered scheme for event-triggered matrices Φ(1)=Φ(2).
    Figure 6.  The trajectories of the state xij(t)(i=1,2,,6;j=1,2,3) for H bipartite consensus for event-triggered matrices Φ(1)=Φ(2).

    Remark 6. It can be shown from Case 1 that the sampled times are 38 for the event-triggered matrices Φ(1)Φ(2), for Case 2, the sampled times are 106 for the event-triggered matrices Φ(1)=Φ(2), obviously, our event-triggered scheme can further reduce the sampled data transmission. From the perspective of average sampling period, in Case 1, the average sampling period is 0.4444, and the average sampling period is 0.1887 in Case 2, which can be seen from Figures 3 and 5, that is, our results are less conservative.

    In this paper, a novel event-triggered communication scheme has been proposed to study H-infinity bipartite consensus with external disturbance in the signed networks. Compared with some existing event-triggered results, the proposed event-triggered communication scheme has the advantage to achieve a better performance while saving the limited network resources. A more generalized random variable is introduced to describe probabilistic actuator failure. Some H-infinity bipartite consensus criteria can be derived, the feedback matrices and event-triggered matrices can be obtained by solving some linear matrix inequalities. Notice that the above results are based on the given event-triggered parameters, it would be interesting to further investigate adaptive event-triggered communication scheme, where the triggered parameters can be adjusted with respect to the dynamic errors. The related results can also be extended to the cases of nonlinear multi-agent systems and stochastic multi-agent systems and so on.

    The author declares no conflict of interest in this paper.



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