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Research Article Finite Frequency โˆž Filtering for Time-Delayed Singularly Perturbed Systems Ping Mei, 1,2 Jingzhi Fu, 1,2 and Yunping Liu 1 1 Nanjing University of Information Science and Technology, Nanjing, Jiangsu 210044, China 2 Jiangsu Collaborative Innovation Center on Atmospheric Environment and Equipment Technology, Nanjing, Jiangsu 210044, China Correspondence should be addressed to Ping Mei; pmei [email protected] Received 18 September 2014; Revised 29 January 2015; Accepted 16 February 2015 Academic Editor: omas Hanne Copyright ยฉ 2015 Ping Mei et al. is 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. is paper investigates the problem of ๏ฌnite frequency (FF) โˆž ๏ฌltering for time-delayed singularly perturbed systems. Our attention is focused on designing ๏ฌlters guaranteeing asymptotic stability and FF โˆž disturbance attenuation level of the ๏ฌltering error system. By the generalized Kalman-Yakubovich-Popov (KYP) lemma, the existence conditions of FF โˆž ๏ฌlters are obtained in terms of solving an optimization problem, which is delay-independent. e main contribution of this paper is that systematic methods are proposed for designing โˆž ๏ฌlters for delayed singularly perturbed systems. 1. Introduction Several physical processes are on one hand of high order and on the other hand complex, what returns their analysis and especially their control, with the aim of certain objectives, very delicate. However, knowing that these systems possess variables evolving in various speeds (temperature, pressure, intensity, voltage...), it could be possible to model these systems by singularly perturbed technique [1, 2]. ey arise in many physical systems such as electrical power systems and electrical machines (e.g., an asynchronous generator, a DC motor, and electrical converters), electronic systems (e.g., oscillators), mechanical systems (e.g., ๏ฌghter aircra๏ฌ…s), biological systems (e.g., bacterial-yeast-virus cultures, heart), and also economic systems with various competing sectors. is class of systems has two time scales, namely, โ€œfastโ€ and โ€œslowโ€ dynamics. is makes their analysis and control more complicated than regular systems. Nevertheless, they have been studied extensively [3โ€“5]. As the dual of control problem, the ๏ฌltering problems of dynamic systems are of great theoretical and practical meaning in the ๏ฌeld of control and signal processing and the ๏ฌltering problem has always been a concern in the control theory [6โ€“8]. e state estimation of singularly perturbed systems also has attracted considerable attention over the past decades and a great number of results have been proposed in various schemes, such as Kalman ๏ฌltering [9, 10] and โˆž ๏ฌltering [11]. Like all kinds of systems which can contain a time- delay in their dynamic or in their control, the singularly perturbed systems can also contain a delay, which has been studied in many references such as [12โ€“15]. For example, Fridman [12] has considered the e๏ฌ€ect of small delay on stability of the singularly perturbed systems. In [13, 14], the controllability problem of nonstandard singularly perturbed systems with small state delay and stabilization problem of nonstandard singularly perturbed systems with small delays both in state and control have been studied, respectively. In [15] a composite control law for singularly perturbed bilinear systems via successive Galerkin approximation was presented. However, there is seldom literature dealing with the synthesis design for the delayed singularly perturbed systems, which is the main motivation of this paper. With the fundamental theory-generalized KYP lemma proposed by Iwasaki and Hara [16], the applications using the GKYP lemma have been sprung up in recent years [17โ€“ 23]. Actually, if noise belongs to a ๏ฌnite 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 approach has a wide application range. In future work, we can use this approach to Markovain jump systems [24, 25]. Hindawi Publishing Corporation Mathematical Problems in Engineering Volume 2015, Article ID 456768, 7 pages http://dx.doi.org/10.1155/2015/456768

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  • Research ArticleFinite Frequency๐ป

    โˆžFiltering 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 [email protected]

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

    Academic Editor: Thomas Hanne

    Copyright ยฉ 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) ๐ปโˆž

    filtering for time-delayed singularly perturbed systems. Ourattention is focused on designing filters guaranteeing asymptotic stability and FF ๐ป

    โˆždisturbance attenuation level of the filtering

    error system. By the generalized Kalman-Yakubovich-Popov (KYP) lemma, the existence conditions of FF ๐ปโˆžfilters 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 ๐ป

    โˆžfilters 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, โ€œfastโ€ andโ€œslowโ€ dynamics. This makes their analysis and control morecomplicated than regular systems. Nevertheless, they havebeen studied extensively [3โ€“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 [6โ€“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 ๐ปโˆž

    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 [12โ€“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 [17โ€“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 [19โ€“21]. In [20] the author has studied the ๐ป

    โˆž

    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 authorโ€™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 ๐ปโˆž

    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 ๐ป

    โˆžfiltering for singularly perturbed systems has

    been extended to the FF๐ปโˆžfiltering 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 ๐‘‹, its transpose is denoted by ๐‘‹๐‘‡; ๐‘

    ๐‘‹

    is an arbitrary matrix whose column forms a basis of the nullspace of ๐‘‹. Sym(๐‘‹) indicates ๐‘‹๐‘‡ + ๐‘‹. ๐œŽmax(โ‹…) denotes maxi-mum singular value of transfer function. diag{โ‹… โ‹… โ‹… } stands fora block-diagonal matrix.

    2. Problem Formulation and Preliminaries

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

    ๏ฟฝฬ‡๏ฟฝ1(๐‘ก) = ๐ด

    01๐‘ฅ1(๐‘ก) + ๐ด

    02๐‘ฅ2(๐‘ก) + ๐ด

    11๐‘ฅ1(๐‘ก โˆ’ ๐‘‘)

    + ๐ด12๐‘ฅ2(๐‘ก โˆ’ ๐‘‘) + ๐ต

    1๐œ” (๐‘ก) ,

    ๐œ€๏ฟฝฬ‡๏ฟฝ2(๐‘ก) = ๐ด

    03๐‘ฅ1(๐‘ก) + ๐ด

    04๐‘ฅ2(๐‘ก) + ๐ด

    13๐‘ฅ1(๐‘ก โˆ’ ๐‘‘)

    + ๐ด14๐‘ฅ2(๐‘ก โˆ’ ๐‘‘) + ๐ต

    2๐œ” (๐‘ก) ,

    ๐‘ฆ (๐‘ก) = ๐ถ1๐‘ฅ1(๐‘ก) + ๐ถ

    2๐‘ฅ2(๐‘ก) + ๐ถ

    3๐‘ฅ1(๐‘ก โˆ’ ๐‘‘) + ๐ถ

    4๐‘ฅ2(๐‘ก โˆ’ ๐‘‘) ,

    ๐‘ (๐‘ก) = ๐บ1๐‘ฅ1(๐‘ก) + ๐บ

    2๐‘ฅ2(๐‘ก) + ๐บ

    3๐‘ฅ1(๐‘ก โˆ’ ๐‘‘) + ๐บ

    4๐‘ฅ2(๐‘ก โˆ’ ๐‘‘) ,

    (1)

    where ๐‘ฅ1(๐‘ก) โˆˆ ๐‘…

    ๐‘›1 is โ€œslowโ€ state and ๐‘ฅ

    2(๐‘ก) โˆˆ ๐‘…

    ๐‘›2 is โ€œfastโ€

    state. Denote ๐‘›๐‘ฅ

    = ๐‘›1+ ๐‘›2; ๐‘ฅ(๐‘ก) = [๐‘ฅ

    1(๐‘ก)๐‘‡

    ๐‘ฅ2(๐‘ก)๐‘‡

    ]๐‘‡

    โˆˆ ๐‘…๐‘›๐‘ฅ

    is the state vector; ๐‘ฆ(๐‘ก) โˆˆ ๐‘…๐‘›๐‘ฆ is the measured output signal,๐‘ง(๐‘ก) โˆˆ ๐‘…

    ๐‘›๐‘ง is the signal to be estimated, and ๐œ”(๐‘ก) โˆˆ ๐‘…๐‘›๐œ” is the

    noise input signal in the ๐ฟ2[0, +โˆž) functional space domain.

    Time-delay ๐‘‘ is known and time-invariantฮฆ(๐‘ก) is the knowninitial condition in the domain [โˆ’๐‘‘, 0]; let ๐ธ

    ๐œ€= [

    ๐ผ๐‘›10

    0 ๐œ€๐ผ๐‘›2

    ],๐ด = [

    ๐ด01๐ด02

    ๐ด03๐ด04

    ], ๐ด๐‘‘= [๐ด11๐ด12

    ๐ด13๐ด14

    ], ๐ต = [ ๐ต1๐ต2

    ], ๐ถ = [๐ถ1

    ๐ถ2], ๐ถ๐‘‘=

    [๐ถ3

    ๐ถ4], ๐บ = [๐บ

    1๐บ2], ๐บ๐‘‘

    = [๐บ3

    ๐บ4], ๐ด๐‘–๐‘—

    (๐‘– = 0, 1; ๐‘— =

    1, . . . , 4), ๐ต๐‘˜, ๐ถ๐‘˜, ๐บ๐‘˜, ๐‘˜ = 1, 2, ๐ถ

    ๐‘™, ๐บ๐‘™, ๐‘™ = 3, 4, be appropriate

    constant matrices.Then the above system can be regulated as

    ๐ธ๐œ€๏ฟฝฬ‡๏ฟฝ = ๐ด๐‘ฅ (๐‘ก) + ๐ด

    ๐‘‘๐‘ฅ (๐‘ก โˆ’ ๐‘‘) + ๐ต๐œ” (๐‘ก) ,

    ๐‘ฆ (๐‘ก) = ๐ถ๐‘ฅ (๐‘ก) + ๐ถ๐‘‘๐‘ฅ (๐‘ก โˆ’ ๐‘‘) ,

    ๐‘ง (๐‘ก) = ๐บ๐‘ฅ (๐‘ก) + ๐บ๐‘‘๐‘ฅ (๐‘ก โˆ’ ๐‘‘) ,

    (2)

    ๐‘ฅ (๐‘ก) = ฮฆ (๐‘ก) โˆ€๐‘ก = [โˆ’๐‘‘, 0] . (3)

    First, we give the following assumption on noise signal ๐œ”(๐‘ก).

    Assumption 1. Noise signal ๐œ”(๐‘ก) is only defined in the low,medium, and high frequency domains

    ฮฉ

    =ฬ‚

    {{{{

    {{{{

    {

    {๐œ” โˆˆ ๐‘… | |๐œ”| โ‰ฅ ๐œ”โ„Ž, ๐œ”โ„Žโ‰ฅ 0} (high frequency)

    {๐œ” โˆˆ ๐‘… | ๐œ”1โ‰ค |๐œ”| โ‰ค ๐œ”

    2, ๐œ”1โ‰ค ๐œ”2} , (media frequency)

    {๐œ” โˆˆ ๐‘… | |๐œ”| โ‰ค ๐œ”๐‘™, ๐œ”๐‘™โ‰ฅ 0} (low frequency) .

    (4)

    Remark 2. By the generalized KYP lemma in [16] and by anappropriate choice ฮฆ and ฮจ, the set ๐‘ can be specialized todefine a certain range of the frequency variable ๐œ”. For thecontinuous time setting, we have ฮฆ = [ 0 1

    1 0], ๐‘ = {๐‘—๐œ” : ๐œ” โˆˆ

    ๐‘…}, whereฮฉ is defined in (4); in this situation,ฮจ can be chosenas

    ฮจ =ฬ‚

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

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

    {

    [

    [

    1 0

    0 ๐œ”2

    โ„Ž

    ]

    ]

    ,

    when ๐œ” โˆˆ {๐œ” โˆˆ ๐‘… | |๐œ”| โ‰ฅ ๐œ”โ„Ž, ๐œ”โ„Žโ‰ฅ 0}

    (high frequency)

    [

    [

    โˆ’1 ๐‘—๐œ”๐‘

    โˆ’๐‘—๐œ”๐‘

    โˆ’๐œ”1๐œ”2

    ]

    ]

    ,

    when ๐œ” โˆˆ {๐œ” โˆˆ ๐‘… | ๐œ”1โ‰ค |๐œ”| โ‰ค ๐œ”

    2, ๐œ”1โ‰ค ๐œ”2} ,

    (media frequency)

    [

    [

    โˆ’1 0

    0 ๐œ”2

    ๐‘™

    ]

    ]

    ,

    when ๐œ” โˆˆ {๐œ” โˆˆ ๐‘… | |๐œ”| โ‰ค ๐œ”๐‘™, ๐œ”๐‘™โ‰ฅ 0}

    (low frequency) ,(5)

    where ๐œ”๐‘:= (๐œ”1+ ๐œ”2)/2.

  • Mathematical Problems in Engineering 3

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

    ๏ฟฝฬ‡๏ฟฝ๐น(๐‘ก) = ๐ด

    ๐น๐‘ฅ๐น(๐‘ก) + ๐ต

    ๐น๐‘ฆ (๐‘ก) , ๐‘ฅ

    ๐น(0) = 0,

    ๐‘ง๐น(๐‘ก) = ๐ถ

    ๐น๐‘ฅ๐น(๐‘ก) + ๐ท

    ๐น๐‘ฆ (๐‘ก) ,

    (6)

    where ๐‘ฅ๐น(๐‘ก) โˆˆ ๐‘…

    ๐‘›๐‘ฅ is the state vector, ๐‘ฆ(๐‘ก) โˆˆ ๐‘…๐‘›๐‘ฆ is the mea-

    sured output signal, ๐‘ง๐น(๐‘ก) โˆˆ ๐‘…

    ๐‘›๐‘ง is the output for the filtering

    systems, and ๐ด๐น, ๐ต๐น, ๐ถ๐น, ๐ท๐นare the filtering matrices to be

    solved. Combine (2) and (6) and let ๐‘ฅ(๐‘ก) = [๐‘ฅ(๐‘ก)๐‘‡ ๐‘ฅ๐น(๐‘ก)๐‘‡

    ]๐‘‡;

    the following filtering error system is obtained:

    ๐ธ๐œ€

    ฬ‡๐‘ฅ (๐‘ก) = ๐ด๐‘ฅ (๐‘ก) + ๐ด

    ๐‘‘๐‘ฅ (๐‘ก โˆ’ ๐‘‘) + ๐ต๐œ” (๐‘ก) ,

    ๐‘’ (๐‘ก) = ๐ถ๐‘ฅ (๐‘ก) + ๐ถ๐‘‘๐‘ฅ (๐‘ก โˆ’ ๐‘‘) ,

    (7)

    ๐‘ฅ (๐‘ก) = [ฮฆ๐‘‡

    (๐‘ก) , 0]

    ๐‘‡

    โˆ€๐‘ก = [โˆ’๐‘‘, 0] , (8)

    where ๐‘’(๐‘ก) = ๐‘ง(๐‘ก) โˆ’ ๐‘ง๐น(๐‘ก) is the filtering error and ๐ธ

    ๐œ€=

    [

    ๐ผ๐‘›10 0

    0 ๐œ€๐ผ๐‘›20

    0 0 ๐ผ๐‘›๐‘ฅ

    ]; the filtering system matrices are

    ๐ด =[

    [

    [

    ๐ด01

    ๐ด02

    0

    ๐ด03

    ๐ด04

    0

    ๐ต๐น๐ถ1

    ๐ต๐น๐ถ2

    0

    ]

    ]

    ]

    ,

    ๐ด๐‘‘=

    [

    [

    [

    ๐ด11

    ๐ด12

    0

    ๐ด13

    ๐ด14

    0

    ๐ต๐น๐ถ3

    ๐ต๐น๐ถ4

    0

    ]

    ]

    ]

    , ๐ต =[

    [

    [

    ๐ต1

    ๐ต2

    0

    ]

    ]

    ]

    ,

    ๐ถ = [๐บ1โˆ’ ๐ท๐น๐ถ1

    ๐บ2โˆ’ ๐ท๐น๐ถ2

    โˆ’๐ถ๐น] ,

    ๐ถ๐‘‘= [๐บ3โˆ’ ๐ท๐น๐ถ3

    ๐บ4โˆ’ ๐ท๐น๐ถ4

    0] .

    (9)

    The transfer function of the filtering error system in (7) from๐œ” to ๐‘ง is given by

    ๐บ๐‘’(๐‘ ) = (๐ถ + ๐‘’

    โˆ’๐‘‘๐‘ 

    ๐ถ๐‘‘๐พ) (๐ธ

    ๐œ€๐‘ ๐ผ โˆ’ ๐ด โˆ’ ๐‘’

    โˆ’๐‘‘๐‘ 

    ๐ด๐‘‘๐พ)

    โˆ’1

    ๐ต, (10)

    where โ€œ๐‘ โ€ 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 ๐›พ, under the zeroinitial condition, the following finite frequency indexis satisfied:

    sup๐œŽmax [๐บ๐‘’ (๐‘—๐œ”)] < ๐›พ, โˆ€๐œ” โˆˆ ฮฉ. (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 ๐‘‹, ๐‘, and ฮฃ begiven. There exists a matrix ๐‘Œ satisfying

    Sym(๐‘‹๐‘‡๐‘Œ๐‘) + ฮฃ < 0 (12)

    if and only if the following projection inequalities are satisfied:

    ๐‘๐‘‡

    ๐‘‹ฮฃ๐‘๐‘‹

    < 0, ๐‘๐‘‡

    ๐‘ฮฃ๐‘๐‘

    < 0. (13)

    3. Main Results

    3.1. FF ๐ปโˆž

    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 ๐›พ > 0, ๐œ€ > 0,๐‘‘ > 0, the filtering error system in (7) is asymptotically stablefor all ๐œ” โˆˆ ฮฉ and satisfies the specifications in (11) if there existmatrices ๐‘ƒ

    ๐œ€โˆˆ ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ with the form of (16), 0 < ๐‘ƒ

    11โˆˆ ๐‘…๐‘›1ร—๐‘›1 ,

    0 < ๐‘ƒ13

    โˆˆ ๐‘…๐‘›2ร—๐‘›2 , ๐‘ƒ2

    โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , ๐‘ƒ3

    โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , ๐‘‚๐œ€

    โˆˆ ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ

    with the form of (17), 0 < ๐‘‚11

    โˆˆ ๐‘…๐‘›1ร—๐‘›1 , 0 < ๐‘‚

    13โˆˆ ๐‘…๐‘›2ร—๐‘›2 ,

    ๐‘‚2โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , ๐‘‚3โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ such that ๐ธ

    ๐œ€๐‘ƒ1๐œ€

    > 0, ๐ธ๐œ€๐‘‚1๐œ€

    > 0, andmatrices 0 < ๐‘„ โˆˆ ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ , ๐‘…

    1โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , and 0 โ‰ค ๐‘…

    2โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ

    that satisfy

    ๐น๐‘‡

    0ฮž0๐น0+ ๐น๐‘‡

    1ฮž1๐น1+ ๐น๐‘‡

    2(ฮฆ โŠ— ๐‘ƒ

    ๐œ€+ ฮจ โŠ— ๐‘„)๐น

    2< 0, (14)

    ๐น๐‘‡

    3ฮž2๐น3+ ๐น๐‘‡

    4(ฮฆ โŠ— ๐‘‚

    ๐œ€) ๐น4< 0, (15)

    where

    ๐‘ƒ๐œ€= [

    ๐‘ƒ1๐œ€

    0

    ๐‘ƒ2

    ๐‘ƒ3

    ] , ๐‘ƒ1๐œ€

    = [

    ๐‘ƒ11

    ๐œ€๐‘ƒ๐‘‡

    12

    ๐‘ƒ12

    ๐‘ƒ13

    ] , (16)

    ๐‘‚๐œ€= [

    ๐‘‚1๐œ€

    0

    ๐‘‚2

    ๐‘‚3

    ] , ๐‘‚1๐œ€

    = [

    ๐‘‚11

    ๐œ€๐‘‚๐‘‡

    12

    ๐‘‚12

    ๐‘‚13

    ] , (17)

    ๐น0= [

    ๐ถ ๐ถ๐‘‘

    0

    0 0 ๐ผ

    ] , ๐น1=

    [

    [

    [

    [

    ๐ด ๐ด๐‘‘

    ๐ต

    ๐ผ 0 0

    0 ๐ผ 0

    ]

    ]

    ]

    ]

    ,

    ๐น2= [

    ๐ด ๐ด๐‘‘

    ๐ต

    ๐ผ 0 0

    ] , ๐น3=

    [

    [

    [

    [

    ๐ด ๐ด๐‘‘

    ๐ผ 0

    0 ๐ผ

    ]

    ]

    ]

    ]

    ,

    ๐น4= [

    ๐ด ๐ด๐‘‘

    ๐ผ 0

    ] , ฮž0โ‰… [

    ๐ผ 0

    0 โˆ’๐›พ2

    ๐ผ

    ] ,

    ฮž๐‘–= diag {0 ๐‘…

    ๐‘–โˆ’๐‘…๐‘–} (๐‘– = 1, 2) .

    (18)

  • 4 Mathematical Problems in Engineering

    (ii) Given ๐‘‘ > 0, if there exist matrices ๐‘ƒ0โˆˆ ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ with

    the form of (16) when ๐œ€ = 0, 0 < ๐‘ƒ11

    โˆˆ ๐‘…๐‘›1ร—๐‘›1 , 0 < ๐‘ƒ

    13โˆˆ

    ๐‘…๐‘›2ร—๐‘›2 , ๐‘ƒ2โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , ๐‘ƒ3โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , ๐‘‚0โˆˆ ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ with the form

    of (17) when ๐œ€ = 0, 0 < ๐‘‚11

    โˆˆ ๐‘…๐‘›1ร—๐‘›1 , 0 < ๐‘‚

    13โˆˆ ๐‘…๐‘›2ร—๐‘›2 ,

    ๐‘‚2โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , ๐‘‚3โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , 0 < ๐‘„ โˆˆ ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ , ๐‘…

    1โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , and

    0 โ‰ค ๐‘…2โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ such that (14), (15) are feasible for ๐œ€ = 0 then

    filtering error system (7) is asymptotic stable and satisfies thespecifications in (11) for all small enough ๐œ€ > 0 and 0 โ‰ค ๐‘‘ โ‰ค ๐‘‘.

    Proof. (i) Let ๐œ‰(๐‘ก) =ฬ‚ [๐‘ฅ(๐‘ก)

    ๐‘ฅ(๐‘กโˆ’๐‘‘)

    ๐œ”(๐‘ก)

    ].Give the following Lyapunov-Krasovskii functional

    ๐‘‰1(๐‘ก) =ฬ‚ ๐‘‰

    1,1(๐‘ก) + ๐‘‰

    1,2(๐‘ก) , (19)

    where

    ๐‘‰1,1

    (๐‘ก) = ๐‘ฅ๐‘‡

    (๐‘ก) ๐ธ๐œ€๐‘ƒ๐œ€๐‘ฅ (๐‘ก) ,

    ๐‘‰1,2

    (๐‘ก) = โˆซ

    ๐‘ก

    ๐‘กโˆ’๐‘‘

    ๐‘ฅ๐‘‡

    (๐œ‚) ๐‘…1๐‘ฅ (๐œ‚) ๐‘‘๐œ‚,

    ๏ฟฝฬ‡๏ฟฝ1,1

    =ฬ‡

    ๐‘ฅ

    ๐‘‡

    ๐ธ๐œ€๐‘ƒ๐œ€๐‘ฅ (๐‘ก) + ๐‘ฅ

    ๐‘‡

    (๐‘ก) ๐‘ƒ๐‘‡

    ๐œ€๐ธ๐œ€

    ฬ‡๐‘ฅ (๐‘ก)

    = (๐ด๐‘ฅ (๐‘ก) + ๐ด๐‘‘๐พ๐‘ฅ (๐‘ก โˆ’ ๐‘‘) + ๐ต๐œ” (๐‘ก))

    ๐‘‡

    โ‹… ๐‘ƒ๐œ€๐‘ฅ (๐‘ก) + ๐‘ฅ

    ๐‘‡

    (๐‘ก)

    โ‹… ๐‘ƒ๐‘‡

    ๐œ€(๐ด๐‘ฅ (๐‘ก) + ๐ด

    ๐‘‘๐พ๐‘ฅ (๐‘ก โˆ’ ๐‘‘) + ๐ต๐œ” (๐‘ก)) ,

    ๏ฟฝฬ‡๏ฟฝ1,2

    = ๐‘ฅ๐‘‡

    (๐‘ก) ๐‘…1๐‘ฅ (๐‘ก) โˆ’ ๐‘ฅ

    ๐‘‡

    (๐‘ก โˆ’ ๐‘‘) ๐‘…1๐‘ฅ (๐‘ก โˆ’ ๐‘‘) .

    (20)

    Then

    ๏ฟฝฬ‡๏ฟฝ1= ๏ฟฝฬ‡๏ฟฝ1,1

    (๐‘ก) + ๏ฟฝฬ‡๏ฟฝ1,2

    (๐‘ก)

    = ๐œ‰ (๐‘ก)๐‘‡

    [๐น๐‘‡

    2(ฮฆ โŠ— ๐‘ƒ

    ๐œ€) ๐น2+ ๐น๐‘‡

    1ฮž1๐น1] ๐œ‰ (๐‘ก) .

    (21)

    Define the following performance index:

    ๐ฝ = โˆซ

    โˆž

    0

    [๐‘’๐‘‡

    (๐‘ก) ๐‘’ (๐‘ก) โˆ’ ๐›พ2

    ๐œ”๐‘‡

    (๐‘ก) ๐œ” (๐‘ก)] ๐‘‘๐‘ก. (22)

    Using the zero initial conditions, we could get

    ๐ฝ โ‰ค โˆซ

    โˆž

    0

    [๐‘’๐‘‡

    (๐‘ก) ๐‘’ (๐‘ก) โˆ’ ๐›พ2

    ๐œ”๐‘‡

    (๐‘ก) ๐œ” (๐‘ก)] ๐‘‘๐‘ก + ๐‘‰1(โˆž) โˆ’ ๐‘‰

    1(0)

    = โˆซ

    โˆž

    0

    ๐œ‰๐‘‡

    (๐‘ก) [๐น๐‘‡

    0ฮž0๐น0+ ๐น๐‘‡

    1ฮž1๐น1+ ๐น๐‘‡

    2(ฮฆ โŠ— ๐‘ƒ

    ๐œ€) ๐น2] ๐œ‰ (๐‘ก) .

    (23)

    Letฮ˜ = ๐น๐‘‡0ฮž0๐น0+๐น๐‘‡

    1ฮž1๐น1+๐น๐‘‡

    2(ฮฆโŠ—๐‘ƒ

    ๐œ€)๐น2and use the Parseval

    equality to get

    โˆซ

    โˆž

    0

    ๐œ‰๐‘‡

    (๐‘ก) ฮ˜๐œ‰ (๐‘ก) ๐‘‘๐‘ก =

    1

    2๐œ‹

    โˆซ

    โˆž

    โˆ’โˆž

    ๐œ‰๐‘‡

    ๐‘ ฮ˜๐œ‰๐‘ ๐‘‘๐œ”. (24)

    Considering frequency ๐œ” โˆˆ ฮฉ and combining (23) and (24),we know that ๐œ‰๐‘‡

    ๐‘ ฮ˜๐œ‰๐‘ < 0 is a sufficient condition of ๐ฝ < 0, for

    all ๐œ” โˆˆ ฮฉ. Additionally, due to ฮ“๐œ†๐น2๐œ‰๐‘ = 0, we know that ๐œ‰

    ๐‘ is

    a zero space of ฮ“๐œ†๐น2.

    By the zero space theory, we know that

    ๐‘๐‘‡

    ฮ“๐œ†๐น2

    ฮ˜๐‘ฮ“๐œ†๐น2

    < 0 โ‡’ ๐œ‰๐‘‡

    ๐‘ ฮ˜๐œ‰๐‘ < 0. (25)

    Then by generalized KYP lemma in [16], the sufficientcondition for ๐‘๐‘‡

    ฮ“๐œ†๐น2

    ฮ˜๐‘ฮ“๐œ†๐น2

    < 0 is existing ๐‘ƒ โˆˆ ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ , 0 <๐‘„ โˆˆ ๐‘…

    2๐‘›๐‘ฅร—2๐‘›๐‘ฅ , such that the following inequality is satisfied:

    ฮ˜ + ๐น๐‘‡

    2(ฮฆ โŠ— ๐‘ƒ + ฮจ โŠ— ๐‘„)๐น

    2< 0. (26)

    By redefining ๐‘ƒ๐œ€+ ๐‘ƒ as ๐‘ƒ

    ๐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:

    ๐‘‰2(๐‘ก) =ฬ‚ ๐‘‰

    2,1(๐‘ก) + ๐‘‰

    2,2(๐‘ก) , (27)

    where ๐‘‰2,1

    (๐‘ก) = ๐‘ฅ๐‘‡

    (๐‘ก)๐ธ๐œ€๐‘‚๐œ€๐‘ฅ(๐‘ก) and ๐‘‰

    2,2(๐‘ก) =

    โˆซ

    ๐‘ก

    ๐‘กโˆ’๐‘‘

    ๐‘ฅ๐‘‡

    (๐œ‚)๐‘…2๐‘ฅ(๐œ‚)๐‘‘๐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 ๐œ€ = 0, then they arefeasible for all small enough ๐œ€ > 0 and thus, due to (i),filtering error system in (7) is asymptotic stable and satisfiesthe specifications in (11) for these values ๐œ€ > 0. Furthermore,linear matrix inequalities (14), (15) are convex with respect to๐‘‘; hence they are feasible for some ๐‘‘; then they are feasiblefor all 0 โ‰ค ๐‘‘ โ‰ค ๐‘‘.

    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 ๐œ€, the existenceof ๐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 ๐›พ > 0,๐‘‘ > 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 ๐‘ƒ

    0โˆˆ ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ with the form of (16), ๐‘‚

    0โˆˆ

    ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ with the form of (17), 0 < ๐‘„ โˆˆ ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ , ๐‘…

    1โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ ,

    and 0 โ‰ค ๐‘…2โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ and ๐‘Œ

    ๐‘–โˆˆ ๐‘…4๐‘›๐‘ฅร—2๐‘›๐‘ฅ(๐‘– = 1, 2) satisfying

    [

    [

    โˆ’๐ผ๐‘›๐‘ง

    [0๐‘›๐‘งร—2๐‘›๐‘ฅ

    ๐ถ ๐ถ๐‘‘

    0]

    โˆ— diag {ฮž1+ ฮž (๐‘ƒ

    0) + ฮž (๐‘„) , โˆ’๐›พ

    2

    ๐ผ๐‘›๐œ”

    } + Sym(๐‘‹๐‘‡๐‘Œ1๐‘1)

    ]

    ]

    < 0,

    (28)

    ฮž2+ ฮž (๐‘‚

    0) + Sym(๐‘‹๐‘‡

    2๐‘Œ2๐‘2) < 0, (29)

  • Mathematical Problems in Engineering 5

    with

    ฮž (๐‘ƒ0) = [

    ฮฆ๐‘โŠ— ๐‘ƒ0

    04๐‘›๐‘ฅร—๐‘›๐‘ฅ

    0๐‘›๐‘ฅร—4๐‘›๐‘ฅ

    0๐‘›๐‘ฅร—๐‘›๐‘ฅ

    ] ,

    ฮž (๐‘‚0) = [

    ฮฆ๐‘โŠ— ๐‘‚0

    04๐‘›๐‘ฅร—๐‘›๐‘ฅ

    0๐‘›๐‘ฅร—4๐‘›๐‘ฅ

    0๐‘›๐‘ฅร—๐‘›๐‘ฅ

    ] ,

    ฮž (๐‘„) = [

    ฮจ๐‘โŠ— ๐‘„ 0

    4๐‘›๐‘ฅร—๐‘›๐‘ฅ

    0๐‘›๐‘ฅร—4๐‘›๐‘ฅ

    0๐‘›๐‘ฅร—๐‘›๐‘ฅ

    ] ,

    ๐‘‹1= โŒŠ๐ผ4๐‘›๐‘ฅ

    04๐‘›๐‘ฅร—(๐‘›๐‘ฅ+๐‘›๐œ”)โŒ‹ , ๐‘

    1= [โˆ’๐ผ2๐‘›๐‘ฅ

    ๐ด ๐ด๐‘‘

    ๐ต] ,

    ๐‘‹2= โŒŠ๐ผ4๐‘›๐‘ฅ

    04๐‘›๐‘ฅร—๐‘›๐‘ฅโŒ‹ , ๐‘

    2= [โˆ’๐ผ2๐‘›๐‘ฅ

    ๐ด ๐ด๐‘‘] ;

    (30)

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

    Proof. Define๐‘€ = [0๐‘›๐‘ฅร—2๐‘›๐‘ฅ

    ๐ถ ๐ถ๐‘‘

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

    diag {ฮž1+ ฮž (๐‘ƒ

    0) + ฮž (๐‘„) , โˆ’๐›พ

    2

    ๐ผ๐‘›๐œ”

    }

    + ๐‘€๐‘‡

    ๐‘€ + Sym (๐‘‹๐‘‡1๐‘Œ1๐‘1) < 0.

    (31)

    By the definition of matrices ๐‘‹1and ๐‘

    1, one can choose

    ๐‘๐‘‹1

    = 0 and ๐‘๐‘1

    =[

    [

    ๐ด ๐ด๐‘‘๐ต

    ๐ผ2๐‘›๐‘ฅ0 0

    0 ๐ผ๐‘›๐‘ฅ0

    0 0 ๐ผ๐‘›๐œ”

    ]

    ]

    ; thus the first inequality

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

    ๐‘โˆ—

    ๐‘1

    (diag {ฮž1+ ฮž (๐‘ƒ

    0) + ฮž (๐‘„) , โˆ’๐›พ

    2

    ๐ผ๐‘›๐œ”

    } + ๐‘€โˆ—

    ๐‘€)๐‘๐‘1

    < 0.

    (32)

    By calculation, we can obtain (32) is equivalent to (14) when๐œ€ = 0.

    Similarly, by introducing the following null space,

    ๐‘๐‘‹2

    = 0, ๐‘๐‘2

    =

    [

    [

    [

    [

    ๐ด ๐ด๐‘‘

    ๐ผ2๐‘›๐‘ฅ

    0

    0 ๐ผ๐‘›๐‘ฅ

    ]

    ]

    ]

    ]

    . (33)

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

    ๐‘๐‘‡

    ๐‘2

    {ฮž2+ ฮž (๐‘‚

    0) + Sym (๐‘‹๐‘‡

    2๐‘Œ2๐‘2)}๐‘๐‘2

    < 0. (34)

    By calculation, (34) is equivalent to (15) when ๐œ€ = 0.Thus, Lemma 8 is equivalent to Lemma 6.

    3.2. Design of FF ๐ปโˆž

    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 ๐ป

    โˆžfilters. The following result can be derived

    via specifying the structure of the slack matrices ๐‘Œ1and ๐‘Œ

    2in

    Lemma 8.Theorem9. Given time-delayed systems in (2) and scalars ๐›พ >0, ๐‘‘ > 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 ๐‘ƒ

    0โˆˆ ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ with the form of (16),

    ๐‘‚0

    โˆˆ ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ with the form of (17), 0 < ๐‘„ โˆˆ ๐‘…2๐‘›๐‘ฅร—2๐‘›๐‘ฅ , ๐‘…

    1โˆˆ

    ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , 0 โ‰ค ๐‘…

    2โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , ฮ“๐‘–,๐‘—

    โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ(๐‘– = 1, 2, ๐‘— = 1, . . . , 4),

    ฮ“5

    โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , ฮ”1

    โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฅ , ฮ”2

    โˆˆ ๐‘…๐‘›๐‘ฅร—๐‘›๐‘ฆ , ฮ”3

    โˆˆ ๐‘…๐‘›๐‘งร—๐‘›๐‘ฅ , ฮ”4

    โˆˆ

    ๐‘…๐‘›๐‘งร—๐‘›๐‘ฆ such that the followingmatrices are satisfied for the given

    scalars ๐œ…๐‘–(๐‘– = 1, . . . , 4):

    [

    โˆ’๐ผ๐‘›๐‘ง

    ฮฃ

    โˆ— diag {ฮž1+ ฮž (๐‘ƒ

    0) + ฮž (๐‘„) , โˆ’๐›พ

    2

    ๐ผ๐‘›๐œ”

    } + Sym(ฮ›1)

    ]

    < 0,

    ฮž2+ ฮž (๐‘‚

    0) + Sym(ฮ›

    2) < 0,

    (35)

    where

    ฮฃ =ฬ‚ โŒŠ0๐‘›๐‘งร—2๐‘›๐‘ฅ

    ๐บ โˆ’ ฮ”4๐ถ โˆ’ฮ”

    3๐บ๐‘‘โˆ’ ฮ”4๐ถ๐‘‘

    0โŒ‹ ,

    ฮ›1=ฬ‚

    [

    [

    [

    [

    [

    [

    [

    [

    [

    โˆ’ฮ“1,1

    โˆ’ฮ“5

    ฮ“1,1

    ๐ด + ฮ”2๐ถ ฮ”

    1ฮ“1,1

    ๐ด๐‘‘+ ฮ”2๐ถ๐‘‘

    ฮ“1,1

    ๐ต

    โˆ’ฮ“1,2

    โˆ’ฮ“5

    ฮ“1,2

    ๐ด + ฮ”2๐ถ ฮ”

    1ฮ“1,2

    ๐ด๐‘‘+ ฮ”2๐ถ๐‘‘

    ฮ“1,2

    ๐ต

    โˆ’ฮ“1,3

    โˆ’๐œ…1ฮ“5

    ฮ“1,3

    ๐ด + ๐œ…1ฮ”2๐ถ ๐œ…1ฮ”1

    ฮ“1,3

    ๐ด๐‘‘+ ๐œ…1ฮ”2๐ถ๐‘‘

    ฮ“1,3

    ๐ต

    โˆ’ฮ“1,4

    โˆ’๐œ…2ฮ“5

    ฮ“1,4

    ๐ด + ๐œ…2ฮ”2๐ถ ๐œ…2ฮ”1

    ฮ“1,4

    ๐ด๐‘‘+ ๐œ…2ฮ”2๐ถ๐‘‘

    ฮ“1,4

    ๐ต

    0 0 0 0 0 0

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ,

    ฮ›2=ฬ‚

    [

    [

    [

    [

    [

    [

    [

    [

    [

    โˆ’ฮ“2,1

    โˆ’ฮ“5

    ฮ“2,1

    ๐ด + ฮ”2๐ถ ฮ”

    1ฮ“2,1

    ๐ด๐‘‘+ ฮ”2๐ถ๐‘‘

    โˆ’ฮ“2,2

    โˆ’ฮ“5

    ฮ“2,2

    ๐ด + ฮ”2๐ถ ฮ”

    1ฮ“2,2

    ๐ด๐‘‘+ ฮ”2๐ถ๐‘‘

    โˆ’ฮ“2,3

    โˆ’๐œ…3ฮ“5

    ฮ“2,3

    ๐ด + ๐œ…3ฮ”2๐ถ ๐œ…3ฮ”1

    ฮ“2,3

    ๐ด๐‘‘+ ๐œ…3ฮ”2๐ถ๐‘‘

    โˆ’ฮ“2,4

    โˆ’๐œ…4ฮ“5

    ฮ“2,4

    ๐ด + ๐œ…4ฮ”2๐ถ ๐œ…4ฮ”1

    ฮ“2,4

    ๐ด๐‘‘+ ๐œ…4ฮ”2๐ถ๐‘‘

    0 0 0 0 0

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    .

    (36)

  • 6 Mathematical Problems in Engineering

    ฮž๐‘–, ฮž(๐‘ƒ0), ฮž(๐‘„), and ฮž(๐‘‚

    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

    [

    ๐ด๐น

    ๐ต๐น

    ๐ถ๐น

    ๐ท๐น

    ] = [

    ฮ“โˆ’1

    50

    0 ๐ผ

    ] [

    ฮ”1

    ฮ”2

    ฮ”3

    ฮ”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 ๐‘Œ

    2has the

    following form:

    ๐‘Œ2=

    [

    [

    [

    [

    [

    [

    ฮ“2,1

    ฮ“5

    ฮ“2,2

    ฮ“6

    ฮ“2,3

    ฮ“7

    ฮ“2,4

    ฮ“8

    ]

    ]

    ]

    ]

    ]

    ]

    . (38)

    Here, ฮ“2,๐‘–

    (๐‘– = 1, . . . , 4), ฮ“๐‘—(๐‘— = 5, . . . , 8) are complexmatrices

    with dimension ๐‘›๐‘ฅร— ๐‘›๐‘ฅ. In fact, ฮ“

    6is nonsingular and can be

    implied from (24); then by multiplying ๐‘Œ2from the left side

    and the right side, respectively, with ๐ผ1= diag {๐ผ ฮ“

    5ฮ“โˆ’1

    6๐ผ ๐ผ}

    and ๐ผ2= diag {๐ผ (ฮ“

    5ฮ“โˆ’1

    6)๐‘‡

    }, we could get

    ๐ผ1๐‘Œ2๐ผ2=

    [

    [

    [

    [

    [

    [

    [

    [

    [

    ฮ“2,1

    ฮ“5(ฮ“5ฮ“โˆ’1

    6)

    ๐‘‡

    ฮ“5ฮ“โˆ’1

    6ฮ“2,2

    ฮ“6(ฮ“5ฮ“โˆ’1

    6)

    ๐‘‡

    ฮ“2,3

    ฮ“7(ฮ“5ฮ“โˆ’1

    6)

    ๐‘‡

    ฮ“2,4

    ฮ“8(ฮ“5ฮ“โˆ’1

    6)

    ๐‘‡

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    ]

    . (39)

    Without loss of generality, we could restrict ฮ“5โ‰ก ฮ“6.

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

    7

    and ฮ“8to be linearly ฮ“

    5-dependent; that is, ฮ“

    7= ๐œ…3ฮ“5, ฮ“8

    =

    ๐œ…4ฮ“5, ๐œ…3and ๐œ…

    4are scalars, respectively. Similarly, the slack

    matrix ๐‘Œ1has the same structure restriction; that is,

    ๐‘Œ1=

    [

    [

    [

    [

    [

    [

    ฮ“1,1

    ฮ“5

    ฮ“1,2

    ฮ“5

    ฮ“1,3

    ๐œ…1ฮ“5

    ฮ“1,4

    ๐œ…2ฮ“5

    ]

    ]

    ]

    ]

    ]

    ]

    , ๐‘Œ2=

    [

    [

    [

    [

    [

    [

    ฮ“2,1

    ฮ“5

    ฮ“2,2

    ฮ“5

    ฮ“2,3

    ๐œ…3ฮ“5

    ฮ“2,4

    ๐œ…4ฮ“5

    ]

    ]

    ]

    ]

    ]

    ]

    . (40)

    Define

    [

    ฮ”1

    ฮ”2

    ฮ”3

    ฮ”4

    ] = [

    ฮ“5

    0

    0 ๐ผ

    ][

    ๐ด๐‘“

    ๐ต๐‘“

    ๐ถ๐‘“

    ๐ท๐‘“

    ] . (41)

    By substituting ๐‘‹๐‘–, ๐‘๐‘–in (28) and (29) and ๐‘Œ

    ๐‘–of (40) into

    ๐‘‹๐‘‡

    ๐‘–๐‘Œ๐‘–๐‘๐‘–, one can obtain ฮ›

    ๐‘–= ๐‘‹๐‘‡

    ๐‘–๐‘Œ๐‘–๐‘๐‘–(๐‘– = 1, 2). Moreover,

    by using (41), one can also obtain ฮฃ โ‰ก ๐‘€. 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

    ๐ด = [

    โˆ’1 0

    0 โˆ’1

    ] , ๐ด๐‘‘= [

    โˆ’1 0

    1 โˆ’1

    ] , ๐ต = [

    โˆ’0.5

    2

    ] ,

    ๐ถ = [0 1] , ๐ถ๐‘‘= [1 2] , ๐บ = [2 1] ,

    ๐บ๐‘‘= [0 0] , ๐œ€ = 0.1, ๐‘‘ = 0.1.

    (42)

    Suppose the frequencies ๐œ”๐‘™= 1, ๐œ”

    โ„Ž= 100, we calculate

    the achieved minimum performance ๐›พโˆ— by using Theorem 9in this paper. For brevity, the scalar parameters inTheorem 9are given by ๐œ…

    1= ๐œ…2= 5, ๐œ…3= ๐œ…4= 1.The obtainedminimum

    performance is ๐›พโˆ— = 0.9976, when ๐‘„ = 0; the problembecomes a standard ๐ป

    โˆžfiltering problem and the minimum

    performance of the nominal ๐ปโˆž

    filtering is ๐›พโˆ— = 1.4533.And the obtained state-space matrices of๐ป

    โˆžfiltering are

    [

    ๐ด๐น

    ๐ต๐น

    ๐ถ๐น

    ๐ท๐น

    ] =[

    [

    [

    โˆ’1.5861 โˆ’0.0552 0

    โˆ’0.2522 โˆ’1.1106 0

    0 0 0

    ]

    ]

    ]

    . (43)

    5. Conclusions

    This paper has studied the problem of FF ๐ปโˆž

    filtering fortime-delayed singularly perturbed systems. The frequenciesof the exogenous noise are assumed to reside in a known rect-angular region and the standard ๐ป

    โˆžfiltering for singularly

    perturbed systems has been extended to the FF๐ปโˆžcase.The

    generalized KYP lemma for singularly perturbed systems hasbeen further developed to derive conditions that are moresuitable for FF ๐ป

    โˆžperformance 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 ๐ป

    โˆždisturbance

    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).

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