Hindawi Publishing Corporation Abstract and Applied Analysis Volume 2013, Article ID 791296, 7 pages http://dx.doi.org/10.1155/2013/791296 Research Article Resilient πΏ 2-πΏ ∞ Filtering of Uncertain Markovian Jumping Systems within the Finite-Time Interval Shuping He College of Electrical Engineering and Automation, Anhui University, Hefei 230601, China Correspondence should be addressed to Shuping He; henyhappy@yahoo.com.cn Received 16 November 2012; Revised 10 March 2013; Accepted 17 March 2013 Academic Editor: Gani Stamov Copyright © 2013 Shuping He. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. This paper studies the resilient πΏ 2 -πΏ ∞ filtering problem for a class of uncertain Markovian jumping systems within the finite-time interval. The objective is to design such a resilient filter that the finite-time πΏ 2 -πΏ ∞ gain from the unknown input to an estimation error is minimized or guaranteed to be less than or equal to a prescribed value. Based on the selected Lyapunov-Krasovskii functional, sufficient conditions are obtained for the existence of the desired resilient πΏ 2 -πΏ ∞ filter which also guarantees the stochastic finite-time boundedness of the filtering error dynamic systems. In terms of linear matrix inequalities (LMIs) techniques, the sufficient condition on the existence of finite-time resilient πΏ 2 -πΏ ∞ filter is presented and proved. The filter matrices can be solved directly by using the existing LMIs optimization techniques. A numerical example is given at last to illustrate the effectiveness of the proposed approach. 1. Introduction More recently, the finite-time stability and control problems have received great attention in the literature; see [1–6]. Compared with the Lyapunov stable dynamical systems, a finite-time stable dynamical system does not require the steady-state behavior of control dynamics over an infinitetime interval and the asymptotic pattern of system trajectories. The main attention may be related to the transient characteristics of the dynamical systems over a fixed finitetime interval, for instance, keeping the acceptable values in a prescribed bound in the presence of saturations. However, more details are related to the stability and control problems of various dynamic systems, and very few reports in the literature consider the filtering problems. Since the Kalman filtering theory [7] has been introduced in the early 1960s, the filtering problem has been extensively investigated. In the filtering scheme, its objective is to estimate the unavailable state variables (or a linear combination of the states) of a given system. During the past decades, many filtering schemes have been developed, such as Kalman filtering [8], π»∞ filtering [9], reduced-order π»∞ filtering [10], and πΏ 2 -πΏ ∞ filtering [11]. Then, extension of this effort to the problem of resilient Kalman filtering with respect to estimator gain perturbations was considered in [12]. And the resilient π»∞ filtering [13] was also raised. Among the filtering schemes, the resilient πΏ 2 -πΏ ∞ filtering was not considered. In practical engineering applications, the peak values of filtering error should always be considered. Compared with the π»∞ filtering scheme, the external disturbances are both assumed to be energy bounded; but πΏ 2 -πΏ ∞ filtering setting requires the mapping from the external disturbances to the filtering error is minimized or no larger than some prescribed level in terms of the πΏ 2 -πΏ ∞ performance norm. In this paper, we have studied the resilient finite-time πΏ 2 -πΏ ∞ filtering problem for uncertain Markouvian Jumping Systems (MJSs). Firstly, the augmented filtering error dynamic system is constructed based on the state estimated filter with resilient filtering parameters. Secondly, a sufficient condition is established on the existence of the robust finitetime filter such that the filtering error dynamic MJSs are finite-time bounded and satisfy a prescribed level of πΏ 2 πΏ ∞ disturbance attenuation with the finite-time interval. And the design criterion is presented by means of LMIs techniques. Subsequently, the robust finite-time πΏ 2 -πΏ ∞ filter matrices can be solved directly by using the existing LMIs optimization algorithms. In order to illustrate the proposed result, a numerical example is given at last. 2 Abstract and Applied Analysis Let us introduce some notations. The symbols Rπ and stand for an π-dimensional Euclidean space and the set R of all π × π real matrices, respectively, π΄π and π΄−1 denote the matrix transpose and matrix inverse, diag{π΄ π΅} represents the block-diagonal matrix of π΄ and π΅, πmax (π΄) and πmin (π΄), respectively, denote the maximal and minimal eigenvalues of a real matrix π΄, β ∗ β denotes the Euclidean norm of vectors, E{∗} denotes the mathematics statistical expectation of the stochastic process or vector, π > 0 stands for a positive-definite matrix, πΌ is the unit matrix with appropriate dimensions, 0 is the zero matrix with appropriate dimensions, and ∗ means the symmetric terms in a symmetric matrix. π×π 2. Problem Formulation Given a probability space (Ω, πΉ, ππ ) where Ω is the sample space, πΉ is the algebra of events, and ππ is the probability measure defined on πΉ. Let us consider a class of linear uncertain MJSs defined in the probability space (Ω, πΉ, ππ ) and described by the following differential equations: π₯Μ (π‘) = [π΄ (ππ‘ ) + Δπ΄ (ππ‘ )] π₯ (π‘) + π΅ (ππ‘ ) π€ (π‘) , (1) π§ (π‘) = πΈ (ππ‘ ) π₯ (π‘) , ππ‘ = π0 , π‘ = 0, where π₯(π‘) ∈ Rπ is the state, π¦(π‘) ∈ Rπ is the measured output, π€(π‘) ∈ πΏπ2 [0 + ∞) is the unknown input, π§(π‘) ∈ Rπ is the controlled output, and π₯0 and π0 are, respectively, the initial states and mode. π΄(ππ‘ ), π΅(ππ‘ ), πΆ(ππ‘ ), π·(ππ‘ ), and πΈ(ππ‘ ) are known mode-dependent constant matrices with appropriate dimensions. The jump parameter ππ‘ represents a continuoustime discrete-state Markov stochastic process taking values on a finite set M = {1, 2, . . . , π} with transition rate matrix Π = {πππ }, π, π ∈ M, and has the following transition probability from mode π at time π‘ to mode π at time π‘ + Δπ‘ as πππ Δπ‘ + π (Δπ‘) , πππ = ππ {ππ‘+Δπ‘ = π | ππ‘ = π} = { 1 + πππ Δπ‘ + π (Δπ‘) , π =ΜΈ π, π = π, (2) where Δπ‘ > 0 and limΔπ‘ → 0 (π(Δπ‘)/Δπ‘) → 0. In this relation, πππ ≥ 0 is the transition probability rates from mode π at time π‘ to mode π (π =ΜΈ π) at time π‘ + Δπ‘, and π ∑ πππ = −πππ for π, π ∈ M, π =ΜΈ π. (3) π=1,π =ΜΈ π For presentation convenience, we denote π΄(ππ‘ ), π΅(ππ‘ ), πΆ(ππ‘ ), π·(ππ‘ ), πΈ(ππ‘ ), Δπ΄(ππ‘ ), and ΔπΆ(ππ‘ ) as π΄ π , π΅π , πΆπ , π·π , πΈπ , Δπ΄ π , and ΔπΆπ , respectively. And the matrices with the symbol Δ(∗) are considered as the uncertain matrices satisfying the following conditions: [ π Δπ΄ π ] = [ 1π ] Γπ (π‘) π1π , ΔπΆπ π2π Remark 1. It is always impossible to obtain the exact mathematical model of practical dynamics due to the complexity process, the environmental noises, and the difficulties of measuring various and uncertain parameters, and so forth; thus, the model of practical dynamics to be controlled almost contains some types of uncertainties. In general, the uncertainties Δ(∗) in (1) satisfying the restraining conditions (4) and Γππ (π‘)Γπ (π‘) ≤ πΌ are said to be admissible. The unknown mode-dependent matrix Γπ (π‘) can also be allowed to be state dependent; that is, Γπ (π‘) = Γπ (π‘, π₯(π‘)), as long as βΓπ (π‘, π₯(π‘))β ≤ 1 is satisfied. We now consider the following resilient filter: ΜΜ (π‘) = (π΄ ππ + Δπ΄ ππ ) π₯ Μ (π‘) + π΅ππ π¦ (π‘) , π₯ Μ (π‘) , π§Μ (π‘) = (πΆππ + ΔπΆππ ) π₯ π¦ (π‘) = [πΆ (ππ‘ ) + ΔπΆ (ππ‘ )] π₯ (π‘) + π· (ππ‘ ) π€ (π‘) , π₯ (π‘) = π₯0 , where π1π , π2π , and π1π are known mode-dependent matrices with appropriate dimensions, and Γπ (π‘) is the time-varying unknown matrix function with Lebesgue norm measurable elements satisfying Γππ (π‘)Γπ (π‘) ≤ πΌ. (4) Μ (π‘) = π₯ Μ0, π₯ ππ‘ = π0 , (5) π‘ = 0, Μ (π‘) ∈ Rπ is the filter state, π§Μ(π‘) ∈ Rπ is the filer output, where π₯ Μ 0 is the initial estimation states, and the mode-dependent π₯ matrices π΄ ππ , π΅ππ , and πΆππ are unknown filter parameters to be designed for each value π ∈ M. Δπ΄ ππ and ΔπΆππ are uncertain filter parameter matrices satisfying the following conditions: [ Δπ΄ ππ π ] = [ 3π ] Γππ (π‘) π2π , ΔπΆππ π4π (6) where π3π , π4π , π2π , and Γππ (π‘) are defined similarly as (4). The objective of this paper is to design the resilient πΏ 2 -πΏ ∞ filter of uncertain MJSs in (1) and obtain an estimate Μz(π‘) of the signal π§(π‘) such that the defined guaranteed performance criteria are minimized in an πΏ 2 -πΏ ∞ estimation error sense. Μ (π‘) and π(π‘) = π§(π‘) − π§Μ(π‘), such that the Define π(π‘) = π₯(π‘) − π₯ filtering error dynamic MJSs are given by πΜ (π‘) = (π΄ ππ + Δπ΄ ππ ) π (π‘) + [π΄ π + Δπ΄ π − (π΄ ππ + Δπ΄ ππ ) − π΅ππ (πΆπ + ΔπΆπ )] π₯ (π‘) + (π΅π − π΅ππ π·π ) π€ (π‘) , π (π‘) = (πΆππ + ΔπΆππ ) π (π‘) + [πΈπ − (πΆππ + ΔπΆππ )] π₯ (π‘) . (7) Let π(π‘) = [ π₯(π‘) π(π‘) ], and we have πΜ (π‘) = π΄π π (π‘) + π΅π π€ (π‘) , π (π‘) = πΆπ π (π‘) , (8) Abstract and Applied Analysis 3 Lemma 5 (see [14]). Let π, π, and π be real matrices with appropriate dimensions. Then, for all time-varying unknown matrix function πΉ(π‘) satisfying πΉπ (π‘)πΉ(π‘) ≤ πΌ, the following relation holds: where 0 π΄ π + Δπ΄ π π΄π = [π΄ + Δπ΄ − (π΄ + Δπ΄ ) − π΅ (πΆ + ΔπΆ ) π΄ + Δπ΄ ] , π π ππ ππ ππ π π ππ ππ π΅π π΅π = [ ], π΅π − π΅ππ π·π πΆπ = [πΈπ − (πΆππ + ΔπΆππ ) π + ππΉ (π‘) π + ππ πΉπ (π‘) ππ > 0, if and only if there exists a positive scalar πΌ > 0, such that πΆππ + ΔπΆππ ] . (9) The external disturbance π€(π‘) is varying and satisfies the constraint condition with respect to the finite-time interval [0 π] as follows: π ∫ π€π (π‘) π€ (π‘) ππ‘ ≤ π, (10) 0 Definition 2. Given a time-constant π > 0, the filtering error dynamic MJSs (8) (setting π€(π‘) = 0) are said to be stochastically finite-time stable (FTS) with respect to Μ π ), if (π1 π2 π π Μ π π (0)} ≤ π1 σ³¨⇒ E {π (π‘) π Μ π π (π‘)} < π2 , E {π (0) π π π Μ π = diag[π π where π1 > 0, π2 > 0, π weight coefficient matrix. Theorem 6. For given π > 0, π > 0, π1 > 0, and Μ π > 0, the filtering error dynamic MJSs (8) are stochastically π Μ π π) and have a πΏ 2 -πΏ ∞ FTB with respect to (π1 π2 π π performance level πΎ > 0, if there exist positive constants, πΎ > 0, π2 > 0, and mode-dependent symmetric positive-definite Μ π , such that matrices π πππ π1 ππΜ + (16) π (1 − π−ππ ) < π2 ππΜ , π (17) Proof. Let the mode at time π‘ be π; that is, ππ‘ = π ∈ M. Take the stochastic Lyapunov-Krasovskii functional π(π(π‘), ππ‘ , π‘ > 0) : Rπ × M × R+ → R+ as π½ = βπ (π‘)βππΈ∞ − πΎβπ€ (π‘)βπ2 < 0, supπ‘∈[0 π Μ π, πΆπ πΆπ < πΎ2 π (15) π π ] > 0, and π π is the Definition 4. For the filtering error dynamic MJSs (8), if there exist filter parameters π΄ ππ , π΅ππ , and πΆππ , as well as a positive scalar πΎ, such that the filtering error dynamic MJSs (8) are stochastically FTB and under the zero-valued initial condition, the system output error satisfies the following cost function inequality for π > 0 with attenuation πΎ > 0 and for all admissible π€(π‘) with the constraint condition (10): = Μ Μ Μ π π΅π ] Μ π π΄π + π΄π π Μ π [π π π + ∑ πππ ππ − πππ π=1 [ ] < 0, πΜ −ππ π΅π ππ −π πΌ] [ Μ ππ Μ −1/2 , π Μ = maxπ∈M πmax (π Μ −1/2 π Μ π ), and π Μ = Μπ = π where π π π π π Μ π ). minπ∈M πmin (π Definition 3. Given a time-constant π > 0, the filtering error dynamic MJSs (8) are stochastically finite-time bounded Μ π π), wherein π1 > 0, (FTB) with respect to (π1 π2 π π Μ π2 > 0, π π > 0, if condition (10) holds. π (14) (11) π‘ ∈ [0 π] , βπ(π‘)βππΈ∞ π + πΌ−1 πππ πΌπππ < 0. π where π is a positive scalar. where (13) π] E[βπ(π‘)β], (12) βπ€(π‘)βπ2 = √∫ π€π (π‘)π€(π‘) ππ‘. 0 Then, the resilient filter (5) is called the stochastic finitetime πΏ 2 -πΏ ∞ filter of the uncertain dynamic MJSs (1) with πΎdisturbance attenuation. 3. Main Results In this section, we will study the robust stochastic finite-time resilient filtering problem for the filtering error dynamic MJSs (8) in an πΏ 2 -πΏ ∞ estimation error sense. Before proceeding with the study, the following lemma is needed. Μ π π (π‘) . π (π (π‘) , π) = ππ (π‘) π (18) Then, we introduce a weak infinitesimal generator I[∗] (see [15, 16]), acting on π(π(π‘), π), for all π ∈ M, which is defined as 1 Iπ (π (π‘) , π) = lim [E {π (π (π‘ + Δπ‘) , ππ‘+Δπ‘ , π‘ +Δπ‘) | Δπ‘ → 0 Δπ‘ π (π‘) , ππ‘ = π} − π (π (π‘) , π, π‘)] . (19) The time derivative of π(π(π‘), π) along the trajectories of the filtering error dynamic MJSs (8) is given by π Μ π πΜ (π‘) + ππ (π‘) ∑πππ π Μ π π (π‘) Iπ (π (π‘) , π) = 2ππ (π‘) π π=1 π Μ π π΄π + π΄π π Μ Μ = ππ (π‘) (π π π + ∑ πππ ππ ) π (π‘) (20) π=1 Μ π π΅π π€ (π‘) . + 2ππ (π‘) π Considering the πΏ 2 -πΏ ∞ filtering performance for the dynamic filtering error system (8), we introduce the following cost function by Definition 4 with π‘ ≥ 0: π½ (π‘) = E [Iπ (π (π‘) , π)] − πE [π (π (π‘) , π)] − π−ππ π€π (π‘) π€ (π‘) . (21) 4 Abstract and Applied Analysis It follows from relation (16) that π½(π‘) < 0; that is, E [Iπ (π (π‘) , π)] < πE [π (π (π‘) , π)] + π−ππ π€π (π‘) π€ (π‘) . (22) Then, multiplying the previous inequality by π−ππ‘ , we have −ππ‘ E {I [π −π(π+π‘) π (π (π‘) , π)]} < π π π€ (π‘) π€ (π‘) . (23) Therefore, the cost function inequality (10) can be guaranteed, which implies π½ = βπ(π‘)βππΈ∞ − πΎβπ€(π‘)βπ2 < 0. Μ ππ Μ −1/2 , π Μ = maxπ∈M πmax (π Μπ = π Μ −1/2 π Μ π ), Denote that π π π π Μ π ). From equality (24), we have and π Μ = minπ∈M πmin (π π π‘ Μ π π (π‘)} = E {π (π (π‘) , π)} < ∫ π−ππ π€π (π ) π€ (π ) ππ E {ππ (π‘) π 0 ππ‘ + π E {π(π (0) , π0 )} < πππ‘ E {π(π (0) , π0 )} Integrating the above inequality from 0 to π, we have π‘ π−ππ E {π (π (π) , π)} − E {π (π (0) , π0 )} −ππ <π π −ππ ∫ π 0 π π€ (π ) π€ (π ) ππ . + π ∫ π−ππ ππ < πππ‘ π1 ππΜ 0 (24) Considering π(π(0), π0 ) ≥ 0, as well as the zero initial condition; that is, π(0) = 0, for π‘ > 0, then it follows that π E {π (π (π) , π)} < ∫ π−ππ π€π (π ) π€ (π ) ππ . 0 Μ π π (π)} = E {π (π (π) , π)} < ∫ π−ππ π€π (π ) π€ (π ) ππ . E {π (π) π E {π (π) π (π)} = E {π π π (π) πΆπ πΆπ π (π)} Μ π π (π)} < πΎ2 E {ππ (π) π = πΎ2 E {π (π (π) , π)} (27) π < πΎ2 ∫ π−ππ π€π (π ) π€ (π ) ππ 0 π < πΎ2 ∫ π€π (π ) π€ (π ) ππ . 0 Since the previous inequality is always true for any π > 0, the following relation: π sup E [βπ (π‘)β] < πΎ√ ∫ π€π (π ) π€ (π ) ππ . (28) 0 π‘∈[0 π] On the other hand, it results from the stochastic Lyapunov-Krasovskii functional that Μ π π (π‘)} ≥ π Μ E {ππ (π‘) π Μ π π (π‘)} . E {ππ (π‘) π π π βπ (π‘)βππΈ∞ = πΎ∑ππ { sup E [βπ (π‘)β]} π‘∈[0 π] π π < πΎ∑ππ √ ∫ π€π (π ) π€ (π ) ππ . 0 π=1 π = πΎ√ ∫ π€π (π ) π€ (π ) ππ = πΎβπ€ (π‘)βπ2 . 0 (29) (31) Then, we can get Μ π π (π‘)} < E {ππ (π‘) π πππ π1 ππΜ + (π/π) (1 − π−ππ ) ππΜ . (32) Μ π π(π‘)} < It implies that for all π‘ ∈ [0 π], we have E{ππ (π‘)π π2 by condition (17). This completes the proof. Theorem 7. For given π > 0, π > 0, π1 > 0, and π π > 0, the filtering error dynamic MJSs (8) are stochastically FTB with respect to (π1 π2 π π π π) with π π ∈ Rπ×π > 0 and have a prescribed πΏ 2 -πΏ ∞ performance level πΎ > 0, if there exist a set of mode-dependent symmetric positive-definite matrices ππ , a set of mode-dependent matrices ππ , ππ , and a positive scalar π1 and mode-dependent sequences πΌπ , π½π , π π , satisfying the following matrix inequalities for all π ∈ M: Λ 1π [Λ [ 2π [ [∗ [ [∗ [∗ ∗ ππ π΅π ππ π1π 0 Λ 3π ππ π΅π − ππ π·π ππ π1π − ππ π2π ππ π3π ] ] ] ∗ −π−ππ πΌ 0 0 ] < 0, (33) ] ∗ ∗ −πΌπ πΌ 0 ] ∗ ∗ ∗ −π½π πΌ ] −ππ It is easy to get the following result: π=1 π (1 − π−ππ ) . π (26) By (15) and within the finite-time interval [0 π], we can also get π + (30) π 0 π (1 − π−ππ‘ ) ≤ πππ π1 ππΜ π (25) Then, it can be verified from the defined LyapunovKrasovskii functional that π + [ [ 0 [ [ [ [∗ [ [ [ ∗ [ 0 π −πΈππ + πΆππ −ππ π −πΆππ ∗ −πΎ2 πΌ + π π π4π π4ππ ∗ ∗ π2ππ ] −π2ππ ] ] ] ] < 0, 0 ] ] ] ] −π π πΌ ] π π < ππ < π1 π π , πππ π1 π1 + π (1 − π−ππ ) < π2 , π (34) (35) (36) Abstract and Applied Analysis 5 π where Λ 1π = ππ π΄ π + π΄ππ ππ + ∑π π=1 πππ ππ − πππ + πΌπ π1π π1π + π π π½π π2π π2π , Λ 2π = ππ π΄ π − ππ − ππ πΆπ − π½π π2π π2π , Λ 2π = ππ + π πππ + ∑π π=1 πππ ππ − πππ + π½π π2π π2π . Moreover, the suitable filter parameters can be given as π΄ ππ = ππ−1 ππ , π΅ππ = ππ−1 ππ , πΆππ = πΆππ . Μ π = diag{ππ , ππ }. Then, we can Proof. For convenience, we set π get the following relations according to matrix inequalities (15) and (16): (37) Ππ + ΔΠ1π + ΔΠ2π < 0, (38) Σπ + ΔΣπ < 0, (39) where π π ∗ ππ π΅π [ππ π΄ π + π΄ π ππ + ∑ πππ ππ − πππ ] [ ] π=1 [ ] π ], Ππ = [ π [ ππ΄ − ππ΄ − ππ΅ πΆ ππ π΄ ππ + π΄ ππ ππ + ∑πππ ππ − πππ ππ π΅π − ππ π΅ππ π·π ] π π π ππ π ππ π [ ] [ ] π=1 −ππ ∗ ∗ −π πΌ ] [ π −ππ 0 −πΈππ + πΆππ ] [ π ] [ 0 −ππ −πΆππ ], [ Σπ = [ ] ] [ ∗ ∗ −πΎ2 πΌ ] [ ππ Δπ΄ π + Δπ΄ππ ππ ∗ 0 ] [ [ππ Δπ΄ π − ππ π΅ππ ΔπΆπ 0 0] ], ΔΠ1π = [ ] [ ] [ ∗ ∗ 0 ] [ (40) 0 ∗ 0 [ ] π ΔΠ2π = [−ππ Δπ΄ ππ ππ Δπ΄ ππ + Δπ΄ ππ ππ 0] , ∗ 0] [ ∗ π 0 0 ΔπΆππ [ π] ] [ 0 0 −ΔπΆππ ]. [ ΔΣπ = [ ] ] [ ∗ ∗ 0 ] [ Referring to Lemma 5, ΔΠ1π and ΔΠ2π can be presented as the following form: ΔΠ1π = πΏ 1π Γπ (π‘) πΏ 2π + πΏπ2π Γππ (π‘) πΏπ1π < πΌπ−1 πΏ 1π πΏπ1π +πΌπ πΏπ2π πΏ 2π , π ΔΠ2π = πΏ 3π Γππ (π‘) πΏ 4π + πΏπ4π Γππ (π‘) πΏπ3π < π½π−1 πΏ 3π πΏπ3π +π½π πΏπ4π πΏ 4π , π π ΔΣπ = πΏ 5π Γππ (π‘) πΏ 6π + πΏπ6π Γππ (π‘) πΏπ5π < π π πΏ 5π πΏπ5π +π−1 π πΏ 6π πΏ 6π , (41) where πΏ 1π = col[ππ π1π ππ π1π − ππ π΅ππ π2π 0], πΏ 2π = [π1π 0 0], πΏ 3π = col[0 ππ π3π 0], πΏ 4π = = [−π2π π2π 0], πΏ 5π = col[0 0 π4π ], and πΏ 6π [π2π − π2π 0]. Then, inequalities (15) and (16) are equivalent to LMIs (38) and (39) by letting ππ = ππ π΄ ππ and ππ = ππ π΅ππ . Μ π = diag[π π On the other hand, we set π (35) implies that Μ π) , 1 < ππΜ = min πmin (π π∈M π π ], and LMI Μ π ) < π1 . (42) ππΜ = max πmax (π π∈M Then, recalling condition (17), we can get LMI (36). This completes the proof. To obtain an optimal finite-time πΏ 2 -πΏ ∞ filtering performance against unknown inputs, uncertainties, and model errors, the attenuation lever πΎ2 can be reduced to the minimum possible value such that LMIs (33)–(36) are satisfied. The optimization problem can be described as follows: min ππ ,ππ ,ππ ,πΆππ ,π·ππ ,πΌπ ,π½π ,π π ,π π (43) 2 s. t. LMIs (33) – (36) with π = πΎ . 6 Abstract and Applied Analysis 0.2 40 0.1 35 0 System state π₯2 (π‘) 45 π2 30 25 20 15 −0.2 −0.3 −0.4 10 5 −0.1 0 1 2 3 4 5 π1 6 7 8 9 −0.5 10 0 0.5 1 1.5 2 2.5 3 3.5 4 3.5 4 π‘ (s) Real state π₯2 (π‘) Estimated state π₯2 (π‘) Figure 1: The optimal minimal upper bound π2 with different initial π1 . 0.08 0.06 Output error π(π‘) System state π₯1 (π‘) Figure 3: System response with state π₯2 (π‘). 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0 −0.1 0 0.5 1 1.5 2 π‘ (s) 2.5 3 3.5 4 0.04 0.02 0 −0.02 −0.04 −0.06 0 0.5 1 1.5 2 2.5 3 π‘ (s) Real state π₯1 (π‘) Estimated state π₯1 (π‘) Figure 4: System response with output error π(π‘). Figure 2: System response with state π₯1 (π‘). Mode 2: Remark 8. In Theorems 6 and 7, if π2 is a variable to be solved, then (17) and (36) can be always satisfied as long as π2 is sufficiently large. For these, we can also fix πΎ and look for the optimal admissible π1 or π2 guaranteeing the stochastic finite-time boundedness of desired filtering error dynamic properties. Example 9. Consider a class of MJSs with two operation modes described as follows. Mode 1: −2 1 ], −1 −1 π·1 = 0.1, π21 = −0.1, π΅1 = [ −0.2 ], 0.1 πΈ1 = [0.1 0.2] , 0.1 π31 = [ ], −0.1 π11 = [0.2 0.1] , 0 3 ], −1 −2 π·2 = −0.2, π22 = 0.2, 4. Numeral Examples π΄1 = [ π΄2 = [ πΆ1 = [1 0.5] , 0 π11 = [ ] , 0.2 π41 = 0.2, π21 = [0.1 −0.2] ; (44) π΅2 = [ 0.1 ], −0.2 πΈ2 = [0.2 −0.1] , π32 = [ π12 = [−0.1 0.1] , 0.1 ], 0.2 πΆ2 = [1 1] , π12 = [ −0.1 ], 0.1 π42 = −0.2, π22 = [0.1 0.1] . (45) The mode switching is governed by a Markov chain that has the following transition rate matrix: −0.3 0.3 Π=[ ]. 0.5 −0.5 (46) In this paper, we choose the initial values for π = 2, π = 4, π = 0.25, and π π = πΌ2 . Then, we fix πΎ = 0.8 and look for the optimal admissible π2 with different π1 which can guarantee the stochastic finite-time boundedness of desired filtering error dynamic properties. Figure 1 gives the optimal minimal admissible π2 with different initial upper bound π1 . Abstract and Applied Analysis 7 For π1 = 1, we solve LMIs (33)–(36) by Theorem 7 and the optimization algorithm (43) and get the following optimal resilient finite-time πΏ 2 -πΏ ∞ filter: π΄ π1 = [ −7.7193 −3.3359 ], −6.9662 −6.6546 3.0189 π΅π1 = [ ], 6.7316 π΄ π2 π΅π2 = [ πΆπ1 = [0.05 0.1] ; −1.3004 0.3608 =[ ], −3.0043 −9.2166 1.1415 ], 2.0586 (47) πΆπ2 = [0.1 −0.05] . And then, we can also get the attenuation lever as πΎ = 0.0777 and the relevant upper bound π2 = 592.45. To show the effectiveness of the designed optimal resilient finite-time πΏ 2 -πΏ ∞ filter, we assume that the unknown inputs are unknown white noise with noise power 0.05 over a finitetime interval π‘ ∈ [0 4]. For the selected initial conditions 0.5 ] and π = 2, the simulation results of the π₯(0) = [ −0.5 0 jumping modes and the response of system states are shown in Figures 2, 3, and 4. It is clear from the simulation figures that the estimated states can track the real states smoothly. 5. Conclusion The resilient finite-time πΏ 2 -πΏ ∞ filtering problems for a class of stochastic MJSs with uncertain parameters have been studied. By using the Lyapunov-Krasovskii functional approach and LMIs optimization techniques, a sufficient condition is derived such that the filtering dynamic error MJSs are finite-time bounded and satisfy a prescribed level of πΏ 2 -πΏ ∞ disturbance attenuation in a finite time-interval. The robust resilient filter gains can be solved directly by using the existing LMIs. Simulation results illustrate the effectiveness of the proposed a pproach. Acknowledgments This work was supported in part by the National Natural Science Foundation of China (Grant no. 61203051), the Joint Specialized Research Fund for the Doctoral Program of Higher Education (Grant no. 20123401120010), and the Key Program of Natural Science Foundation of Education Department of Anhui Province (Grant no. KJ2012A014). References [1] P. Dorato, “Short time stability in linear time-varying systems,” in Proceedings of the IRE international Convention Record, pp. 83–87, 1961. [2] F. Amato, R. Ambrosino, C. Cosentino, and G. De Tommasi, “Input-output finite time stabilization of linear systems,” Automatica, vol. 46, no. 9, pp. 1558–1562, 2010. [3] Y. Zhang, C. Liu, and X. Mu, “Robust finite-time stabilization of uncertain singular Markovian jump systems,” Applied Mathematical Modelling, vol. 36, no. 10, pp. 5109–5121, 2012. [4] J. Zhou, S. Xu, and H. Shen, “Finite-time robust stochastic stability of uncertain stochastic delayed reaction—diffusion genetic regulatory networks,” Neurocomputing, vol. 74, no. 17, pp. 2790–2796, 2011. [5] S. He and F. Liu, “Finite-time π»∞ control of nonlinear jump systems with time-delays via dynamic observer-based state feedback,” IEEE Transactions on Fuzzy Systems, vol. 20, no. 4, pp. 605–614, 2012. [6] H. Liu, Y. Shen, and X. Zhao, “Delay-dependent observer-based π»∞ finite-time control for switched systems with time-varying delay,” Nonlinear Analysis: Hybrid Systems, vol. 6, no. 3, pp. 885– 898, 2012. [7] R. E. Kalman, “A new approach to linear filtering and prediction problems,” Journal of Basic Engineering D, vol. 82, pp. 35–45, 1960. [8] P. Shi, E.-K. Boukas, and R. K. Agarwal, “Kalman filtering for continuous-time uncertain systems with Markovian jumping parameters,” Institute of Electrical and Electronics Engineers, vol. 44, no. 8, pp. 1592–1597, 1999. [9] Y. He, G. P. Liu, D. Rees, and M. Wu, “π»∞ filtering for discretetime systems with time-varying delay,” Signal Processing, vol. 89, no. 3, pp. 275–282, 2009. [10] S. Xu and J. Lam, “Reduced-order π»∞ filtering for singular systems,” Systems & Control Letters, vol. 56, no. 1, pp. 48–57, 2007. [11] H. Zhang, A. S. Mehr, and Y. Shi, “Improved robust energy-topeak filtering for uncertain linear systems,” Signal Processing, vol. 90, no. 9, pp. 2667–2675, 2010. [12] G.-H. Yang and J. L. Wang, “Robust nonfragile Kalman filtering for uncertain linear systems with estimator gain uncertainty,” Institute of Electrical and Electronics Engineers, vol. 46, no. 2, pp. 343–348, 2001. [13] M. S. Mahmoud, “Resilient linear filtering of uncertain systems,” Automatica, vol. 40, no. 10, pp. 1797–1802, 2004. [14] Y. Y. Wang, L. Xie, and C. E. de Souza, “Robust control of a class of uncertain nonlinear systems,” Systems & Control Letters, vol. 19, no. 2, pp. 139–149, 1992. [15] X. Feng, K. A. Loparo, Y. Ji, and H. J. Chizeck, “Stochastic stability properties of jump linear systems,” Institute of Electrical and Electronics Engineers, vol. 37, no. 1, pp. 38–53, 1992. [16] X. Mao, “Stability of stochastic differential equations with Markovian switching,” Stochastic Processes and their Applications, vol. 79, no. 1, pp. 45–67, 1999. 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