Research Article Finite Frequency Filtering for Time-Delayed...

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  • Research ArticleFinite Frequency𝐻

    ∞Filtering for Time-Delayed Singularly

    Perturbed Systems

    Ping Mei,1,2 Jingzhi Fu,1,2 and Yunping Liu1

    1Nanjing University of Information Science and Technology, Nanjing, Jiangsu 210044, China2Jiangsu Collaborative Innovation Center on Atmospheric Environment and Equipment Technology, Nanjing, Jiangsu 210044, China

    Correspondence should be addressed to Ping Mei; pmei njist@sina.com

    Received 18 September 2014; Revised 29 January 2015; Accepted 16 February 2015

    Academic Editor: Thomas Hanne

    Copyright Β© 2015 Ping Mei et al.This is an open access article distributed under the Creative Commons Attribution License, whichpermits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

    This paper investigates the problem of finite frequency (FF) 𝐻∞

    filtering for time-delayed singularly perturbed systems. Ourattention is focused on designing filters guaranteeing asymptotic stability and FF 𝐻

    ∞disturbance attenuation level of the filtering

    error system. By the generalized Kalman-Yakubovich-Popov (KYP) lemma, the existence conditions of FF 𝐻∞filters are obtained

    in terms of solving an optimization problem, which is delay-independent. The main contribution of this paper is that systematicmethods are proposed for designing 𝐻

    ∞filters for delayed singularly perturbed systems.

    1. Introduction

    Several physical processes are on one hand of high order andon the other hand complex, what returns their analysis andespecially their control, with the aim of certain objectives,very delicate. However, knowing that these systems possessvariables evolving in various speeds (temperature, pressure,intensity, voltage. . .), it could be possible to model thesesystems by singularly perturbed technique [1, 2]. They arisein many physical systems such as electrical power systemsand electrical machines (e.g., an asynchronous generator,a DC motor, and electrical converters), electronic systems(e.g., oscillators), mechanical systems (e.g., fighter aircrafts),biological systems (e.g., bacterial-yeast-virus cultures, heart),and also economic systems with various competing sectors.This class of systems has two time scales, namely, β€œfast” andβ€œslow” dynamics. This makes their analysis and control morecomplicated than regular systems. Nevertheless, they havebeen studied extensively [3–5].

    As the dual of control problem, the filtering problemsof dynamic systems are of great theoretical and practicalmeaning in the field of control and signal processing and thefiltering problem has always been a concern in the controltheory [6–8]. The state estimation of singularly perturbedsystems also has attracted considerable attention over the pastdecades and a great number of results have been proposed

    in various schemes, such as Kalman filtering [9, 10] and 𝐻∞

    filtering [11].Like all kinds of systems which can contain a time-

    delay in their dynamic or in their control, the singularlyperturbed systems can also contain a delay, which has beenstudied in many references such as [12–15]. For example,Fridman [12] has considered the effect of small delay onstability of the singularly perturbed systems. In [13, 14], thecontrollability problem of nonstandard singularly perturbedsystems with small state delay and stabilization problem ofnonstandard singularly perturbed systems with small delaysboth in state and control have been studied, respectively.In [15] a composite control law for singularly perturbedbilinear systems via successive Galerkin approximation waspresented. However, there is seldom literature dealing withthe synthesis design for the delayed singularly perturbedsystems, which is the main motivation of this paper.

    With the fundamental theory-generalized KYP lemmaproposed by Iwasaki and Hara [16], the applications usingthe GKYP lemma have been sprung up in recent years [17–23]. Actually, if noise belongs to a finite frequency (FF) range,more accurately, low/middle/high frequency (LF/MF/HF)range, design methods for the entire range will be much con-servative due to overdesign. Consequently, the FF approachhas a wide application range. In future work, we can use thisapproach to Markovain jump systems [24, 25].

    Hindawi Publishing CorporationMathematical Problems in EngineeringVolume 2015, Article ID 456768, 7 pageshttp://dx.doi.org/10.1155/2015/456768

  • 2 Mathematical Problems in Engineering

    Lately, using FF approach to analyze and design controlproblems becomes a new interesting in singularly perturbedsystems [19–21]. In [20] the author has studied the 𝐻

    ∞

    control problem for singularly perturbed systems within thefinite frequency. In [21] the positive control problem forsingularly perturbed systems has been studied based on thegeneralized KYP lemma. The idea is that design in the finitefrequency is critical to singularly perturbed systems sincethe transfer function of singularly perturbed systems has twodifferent frequencies, that is, the high frequency and lowfrequency, which are corresponding to the fast subsystem andthe low subsystem separately. Hence the idea based on thegeneralized KYP lemma actually is constructing the designproblem in separate time scale and also separate frequencyscale. Obviously, it could be seen that the conservativenessis much less than existing results. As far as the author’sknowledge, there is seldom literature referring to the filteringdesign problem within the separate frequencies for delayedsingularly perturbed systems, which is also the main motiva-tion of this paper.

    In this paper we are concerned with FF 𝐻∞

    filtering forsingularly perturbed systems with time-delay. The frequen-cies of the exogenous noises are assumed to reside in a knownrectangular region, which is the most remarkable differenceof our results compared with existing ones. Based on thegeneralized KYP lemma, we first obtained an FF boundedreal lemma in the parameter-independent sense. Filter designmethods will be derived by a simple procedure. The maincontribution of this paper is summarized as follows: thestandard 𝐻

    ∞filtering for singularly perturbed systems has

    been extended to the FF𝐻∞filtering for singularly perturbed

    systemswith time-delay, and systematic filter designmethodshave been proposed.

    The paper is organized as follows. Section 2 gives theproblem formulation and preliminaries used in the next sec-tions. The main results are given in Section 3. An illustrativeexample is given in Section 4. And conclusions are given inthe last section.Notation. For a matrix 𝑋, its transpose is denoted by 𝑋𝑇; 𝑁

    𝑋

    is an arbitrary matrix whose column forms a basis of the nullspace of 𝑋. Sym(𝑋) indicates 𝑋𝑇 + 𝑋. 𝜎max(β‹…) denotes maxi-mum singular value of transfer function. diag{β‹… β‹… β‹… } stands fora block-diagonal matrix.

    2. Problem Formulation and Preliminaries

    The following time-delayed singularly perturbed systems willbe considered in this paper:

    οΏ½Μ‡οΏ½1(𝑑) = 𝐴

    01π‘₯1(𝑑) + 𝐴

    02π‘₯2(𝑑) + 𝐴

    11π‘₯1(𝑑 βˆ’ 𝑑)

    + 𝐴12π‘₯2(𝑑 βˆ’ 𝑑) + 𝐡

    1πœ” (𝑑) ,

    πœ€οΏ½Μ‡οΏ½2(𝑑) = 𝐴

    03π‘₯1(𝑑) + 𝐴

    04π‘₯2(𝑑) + 𝐴

    13π‘₯1(𝑑 βˆ’ 𝑑)

    + 𝐴14π‘₯2(𝑑 βˆ’ 𝑑) + 𝐡

    2πœ” (𝑑) ,

    𝑦 (𝑑) = 𝐢1π‘₯1(𝑑) + 𝐢

    2π‘₯2(𝑑) + 𝐢

    3π‘₯1(𝑑 βˆ’ 𝑑) + 𝐢

    4π‘₯2(𝑑 βˆ’ 𝑑) ,

    𝑍 (𝑑) = 𝐺1π‘₯1(𝑑) + 𝐺

    2π‘₯2(𝑑) + 𝐺

    3π‘₯1(𝑑 βˆ’ 𝑑) + 𝐺

    4π‘₯2(𝑑 βˆ’ 𝑑) ,

    (1)

    where π‘₯1(𝑑) ∈ 𝑅

    𝑛1 is β€œslow” state and π‘₯

    2(𝑑) ∈ 𝑅

    𝑛2 is β€œfast”

    state. Denote 𝑛π‘₯

    = 𝑛1+ 𝑛2; π‘₯(𝑑) = [π‘₯

    1(𝑑)𝑇

    π‘₯2(𝑑)𝑇

    ]𝑇

    ∈ 𝑅𝑛π‘₯

    is the state vector; 𝑦(𝑑) ∈ 𝑅𝑛𝑦 is the measured output signal,𝑧(𝑑) ∈ 𝑅

    𝑛𝑧 is the signal to be estimated, and πœ”(𝑑) ∈ π‘…π‘›πœ” is the

    noise input signal in the 𝐿2[0, +∞) functional space domain.

    Time-delay 𝑑 is known and time-invariantΞ¦(𝑑) is the knowninitial condition in the domain [βˆ’π‘‘, 0]; let 𝐸

    πœ€= [

    𝐼𝑛10

    0 πœ€πΌπ‘›2

    ],𝐴 = [

    𝐴01𝐴02

    𝐴03𝐴04

    ], 𝐴𝑑= [𝐴11𝐴12

    𝐴13𝐴14

    ], 𝐡 = [ 𝐡1𝐡2

    ], 𝐢 = [𝐢1

    𝐢2], 𝐢𝑑=

    [𝐢3

    𝐢4], 𝐺 = [𝐺

    1𝐺2], 𝐺𝑑

    = [𝐺3

    𝐺4], 𝐴𝑖𝑗

    (𝑖 = 0, 1; 𝑗 =

    1, . . . , 4), π΅π‘˜, πΆπ‘˜, πΊπ‘˜, π‘˜ = 1, 2, 𝐢

    𝑙, 𝐺𝑙, 𝑙 = 3, 4, be appropriate

    constant matrices.Then the above system can be regulated as

    πΈπœ€οΏ½Μ‡οΏ½ = 𝐴π‘₯ (𝑑) + 𝐴

    𝑑π‘₯ (𝑑 βˆ’ 𝑑) + π΅πœ” (𝑑) ,

    𝑦 (𝑑) = 𝐢π‘₯ (𝑑) + 𝐢𝑑π‘₯ (𝑑 βˆ’ 𝑑) ,

    𝑧 (𝑑) = 𝐺π‘₯ (𝑑) + 𝐺𝑑π‘₯ (𝑑 βˆ’ 𝑑) ,

    (2)

    π‘₯ (𝑑) = Ξ¦ (𝑑) βˆ€π‘‘ = [βˆ’π‘‘, 0] . (3)

    First, we give the following assumption on noise signal πœ”(𝑑).

    Assumption 1. Noise signal πœ”(𝑑) is only defined in the low,medium, and high frequency domains

    Ξ©

    =Μ‚

    {{{{

    {{{{

    {

    {πœ” ∈ 𝑅 | |πœ”| β‰₯ πœ”β„Ž, πœ”β„Žβ‰₯ 0} (high frequency)

    {πœ” ∈ 𝑅 | πœ”1≀ |πœ”| ≀ πœ”

    2, πœ”1≀ πœ”2} , (media frequency)

    {πœ” ∈ 𝑅 | |πœ”| ≀ πœ”π‘™, πœ”π‘™β‰₯ 0} (low frequency) .

    (4)

    Remark 2. By the generalized KYP lemma in [16] and by anappropriate choice Ξ¦ and Ξ¨, the set 𝑍 can be specialized todefine a certain range of the frequency variable πœ”. For thecontinuous time setting, we have Ξ¦ = [ 0 1

    1 0], 𝑍 = {π‘—πœ” : πœ” ∈

    𝑅}, whereΞ© is defined in (4); in this situation,Ξ¨ can be chosenas

    Ξ¨ =Μ‚

    {{{{{{{{{{{{{{{{{{{{{{{{{{{{{{{

    {{{{{{{{{{{{{{{{{{{{{{{{{{{{{{{

    {

    [

    [

    1 0

    0 πœ”2

    β„Ž

    ]

    ]

    ,

    when πœ” ∈ {πœ” ∈ 𝑅 | |πœ”| β‰₯ πœ”β„Ž, πœ”β„Žβ‰₯ 0}

    (high frequency)

    [

    [

    βˆ’1 π‘—πœ”π‘

    βˆ’π‘—πœ”π‘

    βˆ’πœ”1πœ”2

    ]

    ]

    ,

    when πœ” ∈ {πœ” ∈ 𝑅 | πœ”1≀ |πœ”| ≀ πœ”

    2, πœ”1≀ πœ”2} ,

    (media frequency)

    [

    [

    βˆ’1 0

    0 πœ”2

    𝑙

    ]

    ]

    ,

    when πœ” ∈ {πœ” ∈ 𝑅 | |πœ”| ≀ πœ”π‘™, πœ”π‘™β‰₯ 0}

    (low frequency) ,(5)

    where πœ”π‘:= (πœ”1+ πœ”2)/2.

  • Mathematical Problems in Engineering 3

    Themain objective of this paper is to design the followingfull-order linear filtering:

    �̇�𝐹(𝑑) = 𝐴

    𝐹π‘₯𝐹(𝑑) + 𝐡

    𝐹𝑦 (𝑑) , π‘₯

    𝐹(0) = 0,

    𝑧𝐹(𝑑) = 𝐢

    𝐹π‘₯𝐹(𝑑) + 𝐷

    𝐹𝑦 (𝑑) ,

    (6)

    where π‘₯𝐹(𝑑) ∈ 𝑅

    𝑛π‘₯ is the state vector, 𝑦(𝑑) ∈ 𝑅𝑛𝑦 is the mea-

    sured output signal, 𝑧𝐹(𝑑) ∈ 𝑅

    𝑛𝑧 is the output for the filtering

    systems, and 𝐴𝐹, 𝐡𝐹, 𝐢𝐹, 𝐷𝐹are the filtering matrices to be

    solved. Combine (2) and (6) and let π‘₯(𝑑) = [π‘₯(𝑑)𝑇 π‘₯𝐹(𝑑)𝑇

    ]𝑇;

    the following filtering error system is obtained:

    πΈπœ€

    Μ‡π‘₯ (𝑑) = 𝐴π‘₯ (𝑑) + 𝐴

    𝑑π‘₯ (𝑑 βˆ’ 𝑑) + π΅πœ” (𝑑) ,

    𝑒 (𝑑) = 𝐢π‘₯ (𝑑) + 𝐢𝑑π‘₯ (𝑑 βˆ’ 𝑑) ,

    (7)

    π‘₯ (𝑑) = [Φ𝑇

    (𝑑) , 0]

    𝑇

    βˆ€π‘‘ = [βˆ’π‘‘, 0] , (8)

    where 𝑒(𝑑) = 𝑧(𝑑) βˆ’ 𝑧𝐹(𝑑) is the filtering error and 𝐸

    πœ€=

    [

    𝐼𝑛10 0

    0 πœ€πΌπ‘›20

    0 0 𝐼𝑛π‘₯

    ]; the filtering system matrices are

    𝐴 =[

    [

    [

    𝐴01

    𝐴02

    0

    𝐴03

    𝐴04

    0

    𝐡𝐹𝐢1

    𝐡𝐹𝐢2

    0

    ]

    ]

    ]

    ,

    𝐴𝑑=

    [

    [

    [

    𝐴11

    𝐴12

    0

    𝐴13

    𝐴14

    0

    𝐡𝐹𝐢3

    𝐡𝐹𝐢4

    0

    ]

    ]

    ]

    , 𝐡 =[

    [

    [

    𝐡1

    𝐡2

    0

    ]

    ]

    ]

    ,

    𝐢 = [𝐺1βˆ’ 𝐷𝐹𝐢1

    𝐺2βˆ’ 𝐷𝐹𝐢2

    βˆ’πΆπΉ] ,

    𝐢𝑑= [𝐺3βˆ’ 𝐷𝐹𝐢3

    𝐺4βˆ’ 𝐷𝐹𝐢4

    0] .

    (9)

    The transfer function of the filtering error system in (7) fromπœ” to 𝑧 is given by

    𝐺𝑒(𝑠) = (𝐢 + 𝑒

    βˆ’π‘‘π‘ 

    𝐢𝑑𝐾) (𝐸

    πœ€π‘ πΌ βˆ’ 𝐴 βˆ’ 𝑒

    βˆ’π‘‘π‘ 

    𝐴𝑑𝐾)

    βˆ’1

    𝐡, (10)

    where β€œπ‘ β€ is the Laplace operator.Due to the asymptotic stability of the filtering error

    system (7) depends on system (2), while delayed system (2)does not include input channel for the input signal, so thefollowing assumption is given.

    Assumption 3. Time-delayed singularly perturbed system in(2) is asymptotically stable.

    Now the problems to be solved can be summarized asfollows.

    Problem 4. For the continuous time-delay system in (2), finda full-order linear filtering (6), such that the filtering errorsystem in (7) satisfies the following conditions.

    (1) The filtering error system in (7) is asymptoticallystable.

    (2) Given the appropriate positive real 𝛾, under the zeroinitial condition, the following finite frequency indexis satisfied:

    sup𝜎max [𝐺𝑒 (π‘—πœ”)] < 𝛾, βˆ€πœ” ∈ Ξ©. (11)

    To conclude this section, we give the following technicallemma that plays an instrumental role in deriving our results.

    Lemma 5 ((projection lemma) [26]). Let 𝑋, 𝑍, and Ξ£ begiven. There exists a matrix π‘Œ satisfying

    Sym(π‘‹π‘‡π‘Œπ‘) + Ξ£ < 0 (12)

    if and only if the following projection inequalities are satisfied:

    𝑁𝑇

    𝑋Σ𝑁𝑋

    < 0, 𝑁𝑇

    𝑍Σ𝑁𝑍

    < 0. (13)

    3. Main Results

    3.1. FF 𝐻∞

    Filtering Performance Analysis. To ensure theasymptotic stability and FF specification in (11) for thefiltering error system, we need to resort to the generalizedKYP lemma in [16]. Based on this, the following lemma canbe obtained.

    Lemma 6. (i) Given system in (2) and scalars 𝛾 > 0, πœ€ > 0,𝑑 > 0, the filtering error system in (7) is asymptotically stablefor all πœ” ∈ Ξ© and satisfies the specifications in (11) if there existmatrices 𝑃

    πœ€βˆˆ 𝑅2𝑛π‘₯Γ—2𝑛π‘₯ with the form of (16), 0 < 𝑃

    11∈ 𝑅𝑛1×𝑛1 ,

    0 < 𝑃13

    ∈ 𝑅𝑛2×𝑛2 , 𝑃2

    ∈ 𝑅𝑛π‘₯×𝑛π‘₯ , 𝑃3

    ∈ 𝑅𝑛π‘₯×𝑛π‘₯ , π‘‚πœ€

    ∈ 𝑅2𝑛π‘₯Γ—2𝑛π‘₯

    with the form of (17), 0 < 𝑂11

    ∈ 𝑅𝑛1×𝑛1 , 0 < 𝑂

    13∈ 𝑅𝑛2×𝑛2 ,

    𝑂2∈ 𝑅𝑛π‘₯×𝑛π‘₯ , 𝑂3∈ 𝑅𝑛π‘₯×𝑛π‘₯ such that 𝐸

    πœ€π‘ƒ1πœ€

    > 0, πΈπœ€π‘‚1πœ€

    > 0, andmatrices 0 < 𝑄 ∈ 𝑅2𝑛π‘₯Γ—2𝑛π‘₯ , 𝑅

    1∈ 𝑅𝑛π‘₯×𝑛π‘₯ , and 0 ≀ 𝑅

    2∈ 𝑅𝑛π‘₯×𝑛π‘₯

    that satisfy

    𝐹𝑇

    0Ξ0𝐹0+ 𝐹𝑇

    1Ξ1𝐹1+ 𝐹𝑇

    2(Ξ¦ βŠ— 𝑃

    πœ€+ Ξ¨ βŠ— 𝑄)𝐹

    2< 0, (14)

    𝐹𝑇

    3Ξ2𝐹3+ 𝐹𝑇

    4(Ξ¦ βŠ— 𝑂

    πœ€) 𝐹4< 0, (15)

    where

    π‘ƒπœ€= [

    𝑃1πœ€

    0

    𝑃2

    𝑃3

    ] , 𝑃1πœ€

    = [

    𝑃11

    πœ€π‘ƒπ‘‡

    12

    𝑃12

    𝑃13

    ] , (16)

    π‘‚πœ€= [

    𝑂1πœ€

    0

    𝑂2

    𝑂3

    ] , 𝑂1πœ€

    = [

    𝑂11

    πœ€π‘‚π‘‡

    12

    𝑂12

    𝑂13

    ] , (17)

    𝐹0= [

    𝐢 𝐢𝑑

    0

    0 0 𝐼

    ] , 𝐹1=

    [

    [

    [

    [

    𝐴 𝐴𝑑

    𝐡

    𝐼 0 0

    0 𝐼 0

    ]

    ]

    ]

    ]

    ,

    𝐹2= [

    𝐴 𝐴𝑑

    𝐡

    𝐼 0 0

    ] , 𝐹3=

    [

    [

    [

    [

    𝐴 𝐴𝑑

    𝐼 0

    0 𝐼

    ]

    ]

    ]

    ]

    ,

    𝐹4= [

    𝐴 𝐴𝑑

    𝐼 0

    ] , Ξ0β‰… [

    𝐼 0

    0 βˆ’π›Ύ2

    𝐼

    ] ,

    Ξžπ‘–= diag {0 𝑅

    π‘–βˆ’π‘…π‘–} (𝑖 = 1, 2) .

    (18)

  • 4 Mathematical Problems in Engineering

    (ii) Given 𝑑 > 0, if there exist matrices 𝑃0∈ 𝑅2𝑛π‘₯Γ—2𝑛π‘₯ with

    the form of (16) when πœ€ = 0, 0 < 𝑃11

    ∈ 𝑅𝑛1×𝑛1 , 0 < 𝑃

    13∈

    𝑅𝑛2×𝑛2 , 𝑃2∈ 𝑅𝑛π‘₯×𝑛π‘₯ , 𝑃3∈ 𝑅𝑛π‘₯×𝑛π‘₯ , 𝑂0∈ 𝑅2𝑛π‘₯Γ—2𝑛π‘₯ with the form

    of (17) when πœ€ = 0, 0 < 𝑂11

    ∈ 𝑅𝑛1×𝑛1 , 0 < 𝑂

    13∈ 𝑅𝑛2×𝑛2 ,

    𝑂2∈ 𝑅𝑛π‘₯×𝑛π‘₯ , 𝑂3∈ 𝑅𝑛π‘₯×𝑛π‘₯ , 0 < 𝑄 ∈ 𝑅2𝑛π‘₯Γ—2𝑛π‘₯ , 𝑅

    1∈ 𝑅𝑛π‘₯×𝑛π‘₯ , and

    0 ≀ 𝑅2∈ 𝑅𝑛π‘₯×𝑛π‘₯ such that (14), (15) are feasible for πœ€ = 0 then

    filtering error system (7) is asymptotic stable and satisfies thespecifications in (11) for all small enough πœ€ > 0 and 0 ≀ 𝑑 ≀ 𝑑.

    Proof. (i) Let πœ‰(𝑑) =Μ‚ [π‘₯(𝑑)

    π‘₯(π‘‘βˆ’π‘‘)

    πœ”(𝑑)

    ].Give the following Lyapunov-Krasovskii functional

    𝑉1(𝑑) =Μ‚ 𝑉

    1,1(𝑑) + 𝑉

    1,2(𝑑) , (19)

    where

    𝑉1,1

    (𝑑) = π‘₯𝑇

    (𝑑) πΈπœ€π‘ƒπœ€π‘₯ (𝑑) ,

    𝑉1,2

    (𝑑) = ∫

    𝑑

    π‘‘βˆ’π‘‘

    π‘₯𝑇

    (πœ‚) 𝑅1π‘₯ (πœ‚) π‘‘πœ‚,

    οΏ½Μ‡οΏ½1,1

    =Μ‡

    π‘₯

    𝑇

    πΈπœ€π‘ƒπœ€π‘₯ (𝑑) + π‘₯

    𝑇

    (𝑑) 𝑃𝑇

    πœ€πΈπœ€

    Μ‡π‘₯ (𝑑)

    = (𝐴π‘₯ (𝑑) + 𝐴𝑑𝐾π‘₯ (𝑑 βˆ’ 𝑑) + π΅πœ” (𝑑))

    𝑇

    β‹… π‘ƒπœ€π‘₯ (𝑑) + π‘₯

    𝑇

    (𝑑)

    β‹… 𝑃𝑇

    πœ€(𝐴π‘₯ (𝑑) + 𝐴

    𝑑𝐾π‘₯ (𝑑 βˆ’ 𝑑) + π΅πœ” (𝑑)) ,

    οΏ½Μ‡οΏ½1,2

    = π‘₯𝑇

    (𝑑) 𝑅1π‘₯ (𝑑) βˆ’ π‘₯

    𝑇

    (𝑑 βˆ’ 𝑑) 𝑅1π‘₯ (𝑑 βˆ’ 𝑑) .

    (20)

    Then

    οΏ½Μ‡οΏ½1= οΏ½Μ‡οΏ½1,1

    (𝑑) + οΏ½Μ‡οΏ½1,2

    (𝑑)

    = πœ‰ (𝑑)𝑇

    [𝐹𝑇

    2(Ξ¦ βŠ— 𝑃

    πœ€) 𝐹2+ 𝐹𝑇

    1Ξ1𝐹1] πœ‰ (𝑑) .

    (21)

    Define the following performance index:

    𝐽 = ∫

    ∞

    0

    [𝑒𝑇

    (𝑑) 𝑒 (𝑑) βˆ’ 𝛾2

    πœ”π‘‡

    (𝑑) πœ” (𝑑)] 𝑑𝑑. (22)

    Using the zero initial conditions, we could get

    𝐽 ≀ ∫

    ∞

    0

    [𝑒𝑇

    (𝑑) 𝑒 (𝑑) βˆ’ 𝛾2

    πœ”π‘‡

    (𝑑) πœ” (𝑑)] 𝑑𝑑 + 𝑉1(∞) βˆ’ 𝑉

    1(0)

    = ∫

    ∞

    0

    πœ‰π‘‡

    (𝑑) [𝐹𝑇

    0Ξ0𝐹0+ 𝐹𝑇

    1Ξ1𝐹1+ 𝐹𝑇

    2(Ξ¦ βŠ— 𝑃

    πœ€) 𝐹2] πœ‰ (𝑑) .

    (23)

    LetΘ = 𝐹𝑇0Ξ0𝐹0+𝐹𝑇

    1Ξ1𝐹1+𝐹𝑇

    2(Ξ¦βŠ—π‘ƒ

    πœ€)𝐹2and use the Parseval

    equality to get

    ∫

    ∞

    0

    πœ‰π‘‡

    (𝑑) Ξ˜πœ‰ (𝑑) 𝑑𝑑 =

    1

    2πœ‹

    ∫

    ∞

    βˆ’βˆž

    πœ‰π‘‡

    π‘ Ξ˜πœ‰π‘ π‘‘πœ”. (24)

    Considering frequency πœ” ∈ Ξ© and combining (23) and (24),we know that πœ‰π‘‡

    π‘ Ξ˜πœ‰π‘ < 0 is a sufficient condition of 𝐽 < 0, for

    all πœ” ∈ Ξ©. Additionally, due to Ξ“πœ†πΉ2πœ‰π‘ = 0, we know that πœ‰

    𝑠is

    a zero space of Ξ“πœ†πΉ2.

    By the zero space theory, we know that

    𝑁𝑇

    Ξ“πœ†πΉ2

    Ξ˜π‘Ξ“πœ†πΉ2

    < 0 β‡’ πœ‰π‘‡

    π‘ Ξ˜πœ‰π‘ < 0. (25)

    Then by generalized KYP lemma in [16], the sufficientcondition for 𝑁𝑇

    Ξ“πœ†πΉ2

    Ξ˜π‘Ξ“πœ†πΉ2

    < 0 is existing 𝑃 ∈ 𝑅2𝑛π‘₯Γ—2𝑛π‘₯ , 0 <𝑄 ∈ 𝑅

    2𝑛π‘₯Γ—2𝑛π‘₯ , such that the following inequality is satisfied:

    Θ + 𝐹𝑇

    2(Ξ¦ βŠ— 𝑃 + Ξ¨ βŠ— 𝑄)𝐹

    2< 0. (26)

    By redefining π‘ƒπœ€+ 𝑃 as 𝑃

    πœ€, we obtain inequality (14) that

    completes the first part of (i).As for the asymptotic stability, the Lyapunov-Krasovskii

    functional can be reselected as follows:

    𝑉2(𝑑) =Μ‚ 𝑉

    2,1(𝑑) + 𝑉

    2,2(𝑑) , (27)

    where 𝑉2,1

    (𝑑) = π‘₯𝑇

    (𝑑)πΈπœ€π‘‚πœ€π‘₯(𝑑) and 𝑉

    2,2(𝑑) =

    ∫

    𝑑

    π‘‘βˆ’π‘‘

    π‘₯𝑇

    (πœ‚)𝑅2π‘₯(πœ‚)π‘‘πœ‚.

    Then similar to the proof of the first part of (i), it couldbe shown that inequality (15) can guarantee the asymptoticstability of (7).

    (ii) If (14), (15) are feasible for πœ€ = 0, then they arefeasible for all small enough πœ€ > 0 and thus, due to (i),filtering error system in (7) is asymptotic stable and satisfiesthe specifications in (11) for these values πœ€ > 0. Furthermore,linear matrix inequalities (14), (15) are convex with respect to𝑑; hence they are feasible for some 𝑑; then they are feasiblefor all 0 ≀ 𝑑 ≀ 𝑑.

    Remark 7. Though the essence of the proof of Lemma 6follows from that of Theorem 1 in [6], there are also somedifferences in Lemma 6. First, in Lemma 6, time-delayedsingularly perturbed systems are considered,which are totallydifferent from the regular systems. Since the singularlyperturbed systems have perturbed parameter πœ€, the existenceof πœ€ can lead to the ill-conditioned numerical problems, sohere comes part (ii) of Lemma 6. Furthermore, consideringthe special structure of singularly perturbed systems, notethat, in the proof of part (i), the selected Lyapunov-Krasovskiifunctionals are different from the regular systems.

    To facilitate and reduce the conservatism of the filterdesign using the projection lemma, we present an alternativeof Lemma 6.

    Lemma 8. Given delayed systems in (2) and scalars 𝛾 > 0,𝑑 > 0, filter in (6) exists such that the filtering error system in(7) is asymptotically stable and satisfies the specifications in (11)if there exist matrices 𝑃

    0∈ 𝑅2𝑛π‘₯Γ—2𝑛π‘₯ with the form of (16), 𝑂

    0∈

    𝑅2𝑛π‘₯Γ—2𝑛π‘₯ with the form of (17), 0 < 𝑄 ∈ 𝑅2𝑛π‘₯Γ—2𝑛π‘₯ , 𝑅

    1∈ 𝑅𝑛π‘₯×𝑛π‘₯ ,

    and 0 ≀ 𝑅2∈ 𝑅𝑛π‘₯×𝑛π‘₯ and π‘Œ

    π‘–βˆˆ 𝑅4𝑛π‘₯Γ—2𝑛π‘₯(𝑖 = 1, 2) satisfying

    [

    [

    βˆ’πΌπ‘›π‘§

    [0𝑛𝑧×2𝑛π‘₯

    𝐢 𝐢𝑑

    0]

    βˆ— diag {Ξ1+ Ξ (𝑃

    0) + Ξ (𝑄) , βˆ’π›Ύ

    2

    πΌπ‘›πœ”

    } + Sym(π‘‹π‘‡π‘Œ1𝑍1)

    ]

    ]

    < 0,

    (28)

    Ξ2+ Ξ (𝑂

    0) + Sym(𝑋𝑇

    2π‘Œ2𝑍2) < 0, (29)

  • Mathematical Problems in Engineering 5

    with

    Ξ (𝑃0) = [

    Ξ¦π‘βŠ— 𝑃0

    04𝑛π‘₯×𝑛π‘₯

    0𝑛π‘₯Γ—4𝑛π‘₯

    0𝑛π‘₯×𝑛π‘₯

    ] ,

    Ξ (𝑂0) = [

    Ξ¦π‘βŠ— 𝑂0

    04𝑛π‘₯×𝑛π‘₯

    0𝑛π‘₯Γ—4𝑛π‘₯

    0𝑛π‘₯×𝑛π‘₯

    ] ,

    Ξ (𝑄) = [

    Ξ¨π‘βŠ— 𝑄 0

    4𝑛π‘₯×𝑛π‘₯

    0𝑛π‘₯Γ—4𝑛π‘₯

    0𝑛π‘₯×𝑛π‘₯

    ] ,

    𝑋1= ⌊𝐼4𝑛π‘₯

    04𝑛π‘₯Γ—(𝑛π‘₯+π‘›πœ”)βŒ‹ , 𝑍

    1= [βˆ’πΌ2𝑛π‘₯

    𝐴 𝐴𝑑

    𝐡] ,

    𝑋2= ⌊𝐼4𝑛π‘₯

    04𝑛π‘₯×𝑛π‘₯βŒ‹ , 𝑍

    2= [βˆ’πΌ2𝑛π‘₯

    𝐴 𝐴𝑑] ;

    (30)

    the other notations are defined in (14) and (15).

    Proof. Define𝑀 = [0𝑛π‘₯Γ—2𝑛π‘₯

    𝐢 𝐢𝑑

    0]. By the Schur comple-ment, (28) is equivalent to

    diag {Ξ1+ Ξ (𝑃

    0) + Ξ (𝑄) , βˆ’π›Ύ

    2

    πΌπ‘›πœ”

    }

    + 𝑀𝑇

    𝑀 + Sym (𝑋𝑇1π‘Œ1𝑍1) < 0.

    (31)

    By the definition of matrices 𝑋1and 𝑍

    1, one can choose

    𝑁𝑋1

    = 0 and 𝑁𝑍1

    =[

    [

    𝐴 𝐴𝑑𝐡

    𝐼2𝑛π‘₯0 0

    0 𝐼𝑛π‘₯0

    0 0 πΌπ‘›πœ”

    ]

    ]

    ; thus the first inequality

    in (13) vanishes and then by Lemma 5, (31) is equivalent to

    π‘βˆ—

    𝑍1

    (diag {Ξ1+ Ξ (𝑃

    0) + Ξ (𝑄) , βˆ’π›Ύ

    2

    πΌπ‘›πœ”

    } + π‘€βˆ—

    𝑀)𝑁𝑍1

    < 0.

    (32)

    By calculation, we can obtain (32) is equivalent to (14) whenπœ€ = 0.

    Similarly, by introducing the following null space,

    𝑁𝑋2

    = 0, 𝑁𝑍2

    =

    [

    [

    [

    [

    𝐴 𝐴𝑑

    𝐼2𝑛π‘₯

    0

    0 𝐼𝑛π‘₯

    ]

    ]

    ]

    ]

    . (33)

    Using projection lemma, (29) is equivalent to the followinginequality:

    𝑁𝑇

    𝑍2

    {Ξ2+ Ξ (𝑂

    0) + Sym (𝑋𝑇

    2π‘Œ2𝑍2)}𝑁𝑍2

    < 0. (34)

    By calculation, (34) is equivalent to (15) when πœ€ = 0.Thus, Lemma 8 is equivalent to Lemma 6.

    3.2. Design of FF 𝐻∞

    Filters. Lemma 8 does not give asolution to filter realization explicitly. Based on the result inthe following section we focus on developing methods fordesigning FF 𝐻

    ∞filters. The following result can be derived

    via specifying the structure of the slack matrices π‘Œ1and π‘Œ

    2in

    Lemma 8.Theorem9. Given time-delayed systems in (2) and scalars 𝛾 >0, 𝑑 > 0, filter in (6) exists such that the filtering error systemin (7) is asymptotically stable and satisfies the specifications in(11) if there exist matrices 𝑃

    0∈ 𝑅2𝑛π‘₯Γ—2𝑛π‘₯ with the form of (16),

    𝑂0

    ∈ 𝑅2𝑛π‘₯Γ—2𝑛π‘₯ with the form of (17), 0 < 𝑄 ∈ 𝑅2𝑛π‘₯Γ—2𝑛π‘₯ , 𝑅

    1∈

    𝑅𝑛π‘₯×𝑛π‘₯ , 0 ≀ 𝑅

    2∈ 𝑅𝑛π‘₯×𝑛π‘₯ , Γ𝑖,𝑗

    ∈ 𝑅𝑛π‘₯×𝑛π‘₯(𝑖 = 1, 2, 𝑗 = 1, . . . , 4),

    Ξ“5

    ∈ 𝑅𝑛π‘₯×𝑛π‘₯ , Ξ”1

    ∈ 𝑅𝑛π‘₯×𝑛π‘₯ , Ξ”2

    ∈ 𝑅𝑛π‘₯×𝑛𝑦 , Ξ”3

    ∈ 𝑅𝑛𝑧×𝑛π‘₯ , Ξ”4

    ∈

    𝑅𝑛𝑧×𝑛𝑦 such that the followingmatrices are satisfied for the given

    scalars πœ…π‘–(𝑖 = 1, . . . , 4):

    [

    βˆ’πΌπ‘›π‘§

    Ξ£

    βˆ— diag {Ξ1+ Ξ (𝑃

    0) + Ξ (𝑄) , βˆ’π›Ύ

    2

    πΌπ‘›πœ”

    } + Sym(Ξ›1)

    ]

    < 0,

    Ξ2+ Ξ (𝑂

    0) + Sym(Ξ›

    2) < 0,

    (35)

    where

    Ξ£ =Μ‚ ⌊0𝑛𝑧×2𝑛π‘₯

    𝐺 βˆ’ Ξ”4𝐢 βˆ’Ξ”

    3πΊπ‘‘βˆ’ Ξ”4𝐢𝑑

    0βŒ‹ ,

    Ξ›1=Μ‚

    [

    [

    [

    [

    [

    [

    [

    [

    [

    βˆ’Ξ“1,1

    βˆ’Ξ“5

    Ξ“1,1

    𝐴 + Ξ”2𝐢 Ξ”

    1Ξ“1,1

    𝐴𝑑+ Ξ”2𝐢𝑑

    Ξ“1,1

    𝐡

    βˆ’Ξ“1,2

    βˆ’Ξ“5

    Ξ“1,2

    𝐴 + Ξ”2𝐢 Ξ”

    1Ξ“1,2

    𝐴𝑑+ Ξ”2𝐢𝑑

    Ξ“1,2

    𝐡

    βˆ’Ξ“1,3

    βˆ’πœ…1Ξ“5

    Ξ“1,3

    𝐴 + πœ…1Ξ”2𝐢 πœ…1Ξ”1

    Ξ“1,3

    𝐴𝑑+ πœ…1Ξ”2𝐢𝑑

    Ξ“1,3

    𝐡

    βˆ’Ξ“1,4

    βˆ’πœ…2Ξ“5

    Ξ“1,4

    𝐴 + πœ…2Ξ”2𝐢 πœ…2Ξ”1

    Ξ“1,4

    𝐴𝑑+ πœ…2Ξ”2𝐢𝑑

    Ξ“1,4

    𝐡

    0 0 0 0 0 0

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ,

    Ξ›2=Μ‚

    [

    [

    [

    [

    [

    [

    [

    [

    [

    βˆ’Ξ“2,1

    βˆ’Ξ“5

    Ξ“2,1

    𝐴 + Ξ”2𝐢 Ξ”

    1Ξ“2,1

    𝐴𝑑+ Ξ”2𝐢𝑑

    βˆ’Ξ“2,2

    βˆ’Ξ“5

    Ξ“2,2

    𝐴 + Ξ”2𝐢 Ξ”

    1Ξ“2,2

    𝐴𝑑+ Ξ”2𝐢𝑑

    βˆ’Ξ“2,3

    βˆ’πœ…3Ξ“5

    Ξ“2,3

    𝐴 + πœ…3Ξ”2𝐢 πœ…3Ξ”1

    Ξ“2,3

    𝐴𝑑+ πœ…3Ξ”2𝐢𝑑

    βˆ’Ξ“2,4

    βˆ’πœ…4Ξ“5

    Ξ“2,4

    𝐴 + πœ…4Ξ”2𝐢 πœ…4Ξ”1

    Ξ“2,4

    𝐴𝑑+ πœ…4Ξ”2𝐢𝑑

    0 0 0 0 0

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    .

    (36)

  • 6 Mathematical Problems in Engineering

    Ξžπ‘–, Ξ(𝑃0), Ξ(𝑄), and Ξ(𝑂

    0) are defined in (28) and (29).

    Moreover, if the previous conditions are satisfied, an acceptablestate-space realization of the filter in (6) is given by

    [

    𝐴𝐹

    𝐡𝐹

    𝐢𝐹

    𝐷𝐹

    ] = [

    Ξ“βˆ’1

    50

    0 𝐼

    ] [

    Ξ”1

    Ξ”2

    Ξ”3

    Ξ”4

    ] . (37)

    Proof. First, in order to prove Theorem 9, we just need toprove that (28) and (29) in Lemma 8 can be deduced from(35) inTheorem 9. It is noted that the slack matrix π‘Œ

    2has the

    following form:

    π‘Œ2=

    [

    [

    [

    [

    [

    [

    Ξ“2,1

    Ξ“5

    Ξ“2,2

    Ξ“6

    Ξ“2,3

    Ξ“7

    Ξ“2,4

    Ξ“8

    ]

    ]

    ]

    ]

    ]

    ]

    . (38)

    Here, Ξ“2,𝑖

    (𝑖 = 1, . . . , 4), Γ𝑗(𝑗 = 5, . . . , 8) are complexmatrices

    with dimension 𝑛π‘₯Γ— 𝑛π‘₯. In fact, Ξ“

    6is nonsingular and can be

    implied from (24); then by multiplying π‘Œ2from the left side

    and the right side, respectively, with 𝐼1= diag {𝐼 Ξ“

    5Ξ“βˆ’1

    6𝐼 𝐼}

    and 𝐼2= diag {𝐼 (Ξ“

    5Ξ“βˆ’1

    6)𝑇

    }, we could get

    𝐼1π‘Œ2𝐼2=

    [

    [

    [

    [

    [

    [

    [

    [

    [

    Ξ“2,1

    Ξ“5(Ξ“5Ξ“βˆ’1

    6)

    𝑇

    Ξ“5Ξ“βˆ’1

    6Ξ“2,2

    Ξ“6(Ξ“5Ξ“βˆ’1

    6)

    𝑇

    Ξ“2,3

    Ξ“7(Ξ“5Ξ“βˆ’1

    6)

    𝑇

    Ξ“2,4

    Ξ“8(Ξ“5Ξ“βˆ’1

    6)

    𝑇

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    . (39)

    Without loss of generality, we could restrict Ξ“5≑ Ξ“6.

    On the other hand, to overcome the difficulty of filteringdesign, more work should be done. Next, we will consider Ξ“

    7

    and Ξ“8to be linearly Ξ“

    5-dependent; that is, Ξ“

    7= πœ…3Ξ“5, Ξ“8

    =

    πœ…4Ξ“5, πœ…3and πœ…

    4are scalars, respectively. Similarly, the slack

    matrix π‘Œ1has the same structure restriction; that is,

    π‘Œ1=

    [

    [

    [

    [

    [

    [

    Ξ“1,1

    Ξ“5

    Ξ“1,2

    Ξ“5

    Ξ“1,3

    πœ…1Ξ“5

    Ξ“1,4

    πœ…2Ξ“5

    ]

    ]

    ]

    ]

    ]

    ]

    , π‘Œ2=

    [

    [

    [

    [

    [

    [

    Ξ“2,1

    Ξ“5

    Ξ“2,2

    Ξ“5

    Ξ“2,3

    πœ…3Ξ“5

    Ξ“2,4

    πœ…4Ξ“5

    ]

    ]

    ]

    ]

    ]

    ]

    . (40)

    Define

    [

    Ξ”1

    Ξ”2

    Ξ”3

    Ξ”4

    ] = [

    Ξ“5

    0

    0 𝐼

    ][

    𝐴𝑓

    𝐡𝑓

    𝐢𝑓

    𝐷𝑓

    ] . (41)

    By substituting 𝑋𝑖, 𝑍𝑖in (28) and (29) and π‘Œ

    𝑖of (40) into

    𝑋𝑇

    π‘–π‘Œπ‘–π‘π‘–, one can obtain Ξ›

    𝑖= 𝑋𝑇

    π‘–π‘Œπ‘–π‘π‘–(𝑖 = 1, 2). Moreover,

    by using (41), one can also obtain Ξ£ ≑ 𝑀. The proof iscomplete.

    4. Numerical Example

    In this section, we use an example to illustrate the effective-ness and advantages of the design methods developed in this

    paper. Consider the singularly perturbed system with time-invariant delay in (2) with matrices given by

    𝐴 = [

    βˆ’1 0

    0 βˆ’1

    ] , 𝐴𝑑= [

    βˆ’1 0

    1 βˆ’1

    ] , 𝐡 = [

    βˆ’0.5

    2

    ] ,

    𝐢 = [0 1] , 𝐢𝑑= [1 2] , 𝐺 = [2 1] ,

    𝐺𝑑= [0 0] , πœ€ = 0.1, 𝑑 = 0.1.

    (42)

    Suppose the frequencies πœ”π‘™= 1, πœ”

    β„Ž= 100, we calculate

    the achieved minimum performance π›Ύβˆ— by using Theorem 9in this paper. For brevity, the scalar parameters inTheorem 9are given by πœ…

    1= πœ…2= 5, πœ…3= πœ…4= 1.The obtainedminimum

    performance is π›Ύβˆ— = 0.9976, when 𝑄 = 0; the problembecomes a standard 𝐻

    ∞filtering problem and the minimum

    performance of the nominal 𝐻∞

    filtering is π›Ύβˆ— = 1.4533.And the obtained state-space matrices of𝐻

    ∞filtering are

    [

    𝐴𝐹

    𝐡𝐹

    𝐢𝐹

    𝐷𝐹

    ] =[

    [

    [

    βˆ’1.5861 βˆ’0.0552 0

    βˆ’0.2522 βˆ’1.1106 0

    0 0 0

    ]

    ]

    ]

    . (43)

    5. Conclusions

    This paper has studied the problem of FF 𝐻∞

    filtering fortime-delayed singularly perturbed systems. The frequenciesof the exogenous noise are assumed to reside in a known rect-angular region and the standard 𝐻

    ∞filtering for singularly

    perturbed systems has been extended to the FF𝐻∞case.The

    generalized KYP lemma for singularly perturbed systems hasbeen further developed to derive conditions that are moresuitable for FF 𝐻

    ∞performance synthesis with time-delay.

    Via structural restriction for the slack matrices, systematicmethods have been proposed for the design of the filters thatguarantee the asymptotic stability and FF 𝐻

    ∞disturbance

    attenuation level of the filtering error system.

    Conflict of Interests

    The authors declare that there is no conflict of interestsregarding the publication of this paper.

    Acknowledgments

    This work was supported in part by National Natural Sci-ence Foundation of China under Grants (no. 61304089,no. 51405243), in part by Natural Science Foundation ofJiangsu Province Universities (no. BK20130999), and in partby Natural Science Foundation of Jiangsu Province (no.BK2011826).

    References

    [1] A. Tahar and M. N. Abdelkrim, β€œMultimodel 𝐻∞loop shaping

    control of a DC motor under variable loads,” in Proceedingsof the 8th International Multi-Conference on Systems, Signals &Devices (SSD ’11), pp. 1–6, IEEE, Sousse, Tunisia, March 2011.

  • Mathematical Problems in Engineering 7

    [2] N. Abdelkrim, A. Tellili, and M. N. Abdelkrim, β€œAdditive faulttolerant control applied to delayed singularly perturbed system,”Journal of Software Engineering and Applications, vol. 5, no. 4,pp. 217–224, 2012.

    [3] P.Mei, J. Fu, Y. Gong, and Z. Zhang, β€œGeneralizedH2control for

    fast sampling discrete-time fuzzy singularly perturbed systems,”ICIC Express Letters, vol. 5, no. 4, pp. 1487–1493, 2011.

    [4] W.-H. Chen, G. Yuan, and W. X. Zheng, β€œRobust stabilityof singularly perturbed impulsive systems under nonlinearperturbation,” IEEE Transactions on Automatic Control, vol. 58,no. 1, pp. 168–174, 2013.

    [5] T. Nguyen, W.-C. Su, and Z. Gajic, β€œVariable structure con-trol for singularly perturbed linear continuous systems withmatched disturbances,” IEEE Transactions on Automatic Con-trol, vol. 57, no. 3, pp. 777–783, 2012.

    [6] H. Gao and X. Li, β€œπ»βˆžfiltering for discrete-time state-delayed

    systems with finite frequency specifications,” IEEE Transactionson Automatic Control, vol. 56, no. 12, pp. 2935–2941, 2011.

    [7] P. Shi, E.-K. Boukas, and R. K. Agarwal, β€œKalman filtering forcontinuous-time uncertain systems with Markovian jumpingparameters,” IEEE Transactions on Automatic Control, vol. 44,no. 8, pp. 1592–1597, 1999.

    [8] H. Wang and G.-H. Yang, β€œA finite frequency approach tofilter design for uncertain discrete-time systems,” InternationalJournal of Adaptive Control and Signal Processing, vol. 22, no. 6,pp. 533–550, 2008.

    [9] X. Shen, M. Rao, and Y. Ying, β€œDecomposition method forsolving the gains of Kalman filter in singularly perturbedsystems,” in Proceedings of the American Control Conference, pp.3350–3354, 1992.

    [10] M. D. S. Aliyu and E. K. Boukas, β€œH2filtering for non-

    linear singularly perturbed systems,” IET Control Theory andApplications, vol. 5, no. 17, pp. 2023–2032, 2011.

    [11] X. Shen and L. Deng, β€œDecomposition solution of𝐻∞filter gain

    in singularly perturbed systems,” Signal Processing, vol. 55, no.3, pp. 313–320, 1996.

    [12] E. Fridman, β€œEffects of small delays on stability of singularlyperturbed systems,” Automatica, vol. 38, no. 5, pp. 897–902,2002.

    [13] V. Y. Glizer, β€œControllability of nonstandard singularly per-turbed systems with small state delay,” IEEE Transactions onAutomatic Control, vol. 48, no. 7, pp. 1280–1285, 2003.

    [14] V. Y. Glizer, β€œOn stabilization of nonstandard singularly per-turbed systems with small delays in state and control,” IEEETransactions on Automatic Control, vol. 49, no. 6, pp. 1012–1016,2004.

    [15] Y.-J. Kim, B.-S. Kim, and M.-T. Lim, β€œComposite control forsingularly perturbed bilinear systems via successive Galerkinapproximation,” IEE Proceedings: Control Theory and Applica-tions, vol. 150, no. 5, pp. 483–488, 2003.

    [16] T. Iwasaki and S. Hara, β€œGeneralized KYP lemma: unifiedfrequency domain inequalities with design applications,” IEEETransactions on Automatic Control, vol. 50, no. 1, pp. 41–59,2005.

    [17] T. Iwasaki and S. Hara, β€œFeedback control synthesis of multiplefrequency domain specifications via generalized KYP lemma,”International Journal of Robust and Nonlinear Control, vol. 17,no. 5-6, pp. 415–434, 2007.

    [18] H. G. Hoang, H. D. Tuan, and T. Q. Nguyen, β€œFrequency-selective KYP lemma, IIR filter, and filter bank design,” IEEETransactions on Signal Processing, vol. 57, no. 3, pp. 956–965,2009.

    [19] P.Mei and Y. Zou, β€œFinite frequency positive realness analysis ofsingularly perturbed systems based on generalized KYP lemmaapproach,” Control and Decision, vol. 25, no. 5, pp. 711–714, 2010(Chinese).

    [20] P. Mei, C. Cai, and Y. Zou, β€œA generalized KYP lemma-basedapproach for 𝐻

    ∞control of singularly perturbed systems,”

    Circuits, Systems, and Signal Processing, vol. 28, no. 6, pp. 945–957, 2009.

    [21] Y. Huang, C. Cai, and Y. Zou, β€œFinite frequency positive realcontrol for singularly perturbed systems,” International Journalof Control, Automation and Systems, vol. 9, no. 2, pp. 376–383,2011.

    [22] H. Wang and G.-H. Yang, β€œFault detection observer designfor linear discrete-time systems in finite frequency domain,” inProceedings of the 46th IEEEConference onDecision and Control(CDC ’07), pp. 378–383,NewOrleans, Lo,USA,December 2007.

    [23] C. Du, L. Xie, G. Guo, and J. Nee Teoh, β€œA generalized KYPlemma based approach for disturbance rejection in data storagesystems,” Automatica, vol. 43, no. 12, pp. 2112–2118, 2007.

    [24] P. Balasubramaniam, V. M. Revathi, and J. H. Park, β€œπΏ2βˆ’ 𝐿∞

    filtering for neutral Markovian switching system with mode-dependent time-varying delays and partially unknown transi-tion probabilities,” Applied Mathematics and Computation, vol.219, no. 17, pp. 9524–9542, 2013.

    [25] V. M. Revathi, P. Balasubramaniam, J. H. Park, and T. H. Lee,β€œπ»βˆžfiltering for sample data systems with stochastic sampling

    and Markovian jumping parameters,” Nonlinear Dynamics, vol.78, no. 2, pp. 813–830, 2014.

    [26] P.Gahinet andP.Apkarian, β€œA linearmatrix inequality approachto 𝐻∞

    control,” International Journal of Robust and NonlinearControl, vol. 4, no. 4, pp. 421–448, 1994.

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