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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Design of PD Observer-Based Fault Estimator Using a Descriptor Approach</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Dušan Krokavec</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Anna Filasová</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Pavol Lišcˇinský</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Vladimír Serbák</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Department of Cybernetics and Artificial Intelligence, Technical University of Košice, Faculty of Electrical Engineering and Informatics</institution>
          ,
          <addr-line>Košice</addr-line>
          ,
          <country country="SK">Slovakia</country>
        </aff>
      </contrib-group>
      <fpage>235</fpage>
      <lpage>240</lpage>
      <abstract>
        <p>A generalized principle of PD faults observer design for continuous-time linear MIMO systems is presented in the paper. The problem addressed is formulated as a descriptor system approach to PD fault observers design, implying the asymptotic convergence both the state observer error as fault estimate error. Presented in the sense of the second Lyapunov method, an associated structure of linear matrix inequalities is outlined to possess the observer asymptotic dynamic properties. The proposed design conditions are verified by simulations in the numerical illustrative example.</p>
      </abstract>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>-</title>
      <p>As is well known, observer design is a hot research field
owing to its particular importance in observer-based control,
residual fault detection and fault estimation [1], where,
especially from the stand point of the active fault tolerant
control (FTC) structures, the problem of simultaneous state and
fault estimation is very eligible. In that sense various
effective methods have been developed to take into account the
faults effect on control structure reconfiguration and fault
detection [16], [22]. The fault detection filters, usually
relying on the use of particular type of state observers, are
mostly used to produce fault residuals in FTC. Because it is
generally not possible in residuals to decouple totally fault
effects from the perturbation influence, different approaches
are used to tackle in part this conflict and to create residuals
that are as a rule zero in the fault free case, maximally
sensitive to faults, as well as robust to disturbances [2], [8]. Since
faults are detected usually by setting a threshold on the
generated residual signal, determination of an actual
threshold is often formulated in adaptive frames [3]. Generalized
method to solve the problem of actuator faults detection and
isolation in over-actuated systems is given in [14], [15].</p>
      <p>To estimate actuator faults for the linear time invariant
systems without external disturbance the principles based
on adaptive observers are frequently used, which make
estimation of actuator faults by integrating the system output
errors [25]. In particular, proportional-derivative (PD)
observers introduce a design freedom giving an opportunity
for generating state and fault estimates with good sensitivity
properties and improving the observer design performance
[6], [18], [19]. Since derivatives of the system outputs can
be exploited in the fault estimator design to achieve faster
fault estimation, a proportional multi-integral derivative
estimators are proposed in [7], [24].</p>
      <p>Although the state observers for linear and nonlinear
systems received considerable attention, the descriptor
design principles have not been studied extensively for
nonsingular systems. Modifying the descriptor observer design
principle [13], the first result giving sufficient design
conditions, but for linear time-delay systems, can be found in [5].
Reflecting the same problems concerning the observers for
descriptor systems, linear matrix inequality (LMI) methods
were presented e.g. in [9] but a hint of this method can be
found in [23], [25]. The extension for a class of nonlinear
systems which can be described by Takagi-Sugeno models
is presented in [12].</p>
      <p>Adapting the approach to the observer-based fault
estimation for descriptor systems as well as its potential extension,
the main issue of this paper is to apply the descriptor
principle in PD fault observer design. Preferring LMI
formulation, the stability condition proofs use standard arguments
in the sense of Lyapunov principle for the design
conditions requiring to solve only LMIs without additional
constraints. This presents a method designing the PD
observation derivative and proportional gain matrices such that the
design is non-singular and ensures that the estimation error
dynamics has asymptotical convergence. From viewpoint
of application, although the descriptor principle is used, it
is not necessary to transform the system parameter into a
descriptor form or to use matrix inversions in design task
formulation. Despite a partly conservative form, the design
conditions can be transformed to LMIs with minimal
number of symmetric LMI variables.</p>
      <p>The paper is organized as follows. Placed after
Introduction, Sec. 2 gives a basic description of the PD fault
observer and Sec. 3 presents design problem formulation in
the descriptor form for a standard Luenberger observer. A
new LMI structure, describing the PD fault observer design
conditions, is theoretically explained in Sec 4. An example
is provided to demonstrate the proposed approach in Sec. 5
and Sec. 6 draws some conclusions.</p>
      <p>Used notations are conventional so that xT , XT
denote transpose of the vector x and matrix X, respectively,
X = XT &gt; 0 means that X is a symmetric positive
definite matrix, kXk∞ designs the H∞ norm of the matrix X,
the symbol In represents the n-th order unit matrix, ρ(X)
and rank(X) indicate the eigenvalue spectrum and rank of
a square matrix X, IR denotes the set of real numbers and
IRn, IRn× r refer to the set of all n-dimensional real vectors
and n × r real matrices, respectively.
2</p>
    </sec>
    <sec id="sec-2">
      <title>The Problem Statement</title>
      <p>The systems under consideration are linear continuous-time
dynamic systems represented in state-space form as
q˙ (t) = Aq(t) + Bu(t) + F f (t) ,</p>
      <p>y(t) = Cq(t) ,
where q(t) ∈ IRn, u(t) ∈ IRr, y(t) ∈ IRm are the vectors
of the state, input and output variables, f (t) ∈ IRp is the
fault vector, A ∈ IRn× n, B ∈ IRn× r, C ∈ IRm× n and
F ∈ IRn× p are real finite values matrices, m, r, p &lt; n and
rank</p>
      <p>A F
C 0
= n + p .</p>
      <p>It is considered that the fault f (t) may occur at an uncertain
time, the size of the fault is unknown but bounded and that
the pair (A, C) is observable.</p>
      <p>Focusing on fault estimation task for slowly-varying
faults, the fault PD observer is considered in the following
form [19]
q˙ e(t) = Aqe(t) + Bu(t) + F f e(t)+
+J (y(t) − ye(t)) + L(y˙ (t) − y˙ e(t)) ,</p>
      <p>ye(t) = Cqe(t) ,
f˙ e(t) = M (y(t) − ye(t)) + N (y˙ (t) − y˙ e(t)) ,
where qe(t) ∈ IRn, ye(t) ∈ IRm, f e(t) ∈ IRp are
estimates of the system states vector, the output variables
vector and the fault vector, respectively, and J , L ∈ IRn× m,
M , N ∈ IRp× m is the set of observer gain matrices is to be
determined.</p>
      <p>To explain and concretize the obtained results, the
following well known lemma of Schur complement property is
suitable.</p>
      <p>
        Lemma 1. [20] Considering the matrices Q = QT , R =
RT and S of appropriate dimensions, where detR 6= 0,
then the following statements are equivalent
(1)
(2)
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
(4)
(
        <xref ref-type="bibr" rid="ref5">5</xref>
        )
(
        <xref ref-type="bibr" rid="ref6">6</xref>
        )
Q
ST
      </p>
      <p>S
−R</p>
      <p>
        &lt; 0 ⇔ Q + SR−1ST &lt; 0, R &gt; 0 (
        <xref ref-type="bibr" rid="ref7">7</xref>
        )
      </p>
      <p>This shows that the above block matrix inequality has a
solution if the implying set of inequalities has a solution.
3</p>
    </sec>
    <sec id="sec-3">
      <title>Descriptor Principle in Luenberger</title>
    </sec>
    <sec id="sec-4">
      <title>Observer Design</title>
      <p>To formulate the proposed PD observer design approach,
the descriptor principle in the observer stability analysis is
presented.</p>
      <p>If the fault-free system (1), (2) is considered, the
Luenberger observer is given as
q˙ e(t) = Aqe(t) + Bu(t) + J (y(t) − ye(t)) ,</p>
      <p>
        ye(t) = Cqe(t) ,
and using (1), (2), (
        <xref ref-type="bibr" rid="ref8">8</xref>
        ), (
        <xref ref-type="bibr" rid="ref9">9</xref>
        ), it yields
      </p>
      <p>e˙(t) = (A − J C)e(t) ,
(A − J C)e(t) − e˙(t) = 0 ,
respectively, where</p>
      <p>eq(t) = q(t) − qe(t) .</p>
      <p>
        Using the descriptor principle, the following lemma
presents the Luenberger observer design conditions in terms of
LMIs for the fault-free system (1), (2).
(
        <xref ref-type="bibr" rid="ref8">8</xref>
        )
(
        <xref ref-type="bibr" rid="ref9">9</xref>
        )
(
        <xref ref-type="bibr" rid="ref10">10</xref>
        )
(
        <xref ref-type="bibr" rid="ref11">11</xref>
        )
(
        <xref ref-type="bibr" rid="ref12">12</xref>
        )
respectively. Introducing the matrix
then, with respect to (
        <xref ref-type="bibr" rid="ref23">23</xref>
        ), it has to be
      </p>
      <p>P ⋄ TA⋄e + A⋄eTP ⋄ &lt; 0 ,
P ⋄ =</p>
      <p>P 1
P 3</p>
      <p>P 2
P 4
In 0
0 0
which gives</p>
      <p>P 1 P 2
P 3 P 4
P 1
0</p>
      <p>P 2
0
=
=</p>
      <p>P 1T
P 2T</p>
      <p>P 3T</p>
      <p>
        P 4T
P 1T
P 2T
Lemma 2. The Luenberger observer (
        <xref ref-type="bibr" rid="ref8">8</xref>
        ), (
        <xref ref-type="bibr" rid="ref9">9</xref>
        ) is stable if for
given positive scalar δ ∈ IR there exist a symmetric positive
definite matrix P 1 ∈ IRn× n a regular matrix P 3 ∈ IRn× n
and a matrix Y ∈ IRn× m such that
      </p>
      <p>Hereafter, ∗ denotes the symmetric item in a symmetric
matrix.</p>
      <p>
        Proof. Denoting the observer system matrix as
#
(
        <xref ref-type="bibr" rid="ref13">13</xref>
        )
e˙(t)
e¨(t) =
e˙(t)
0
=
, A⋄e =
0
Ae
      </p>
      <p>
        In
−In
. (
        <xref ref-type="bibr" rid="ref21">21</xref>
        )
Defining the Lyapunov function of the form
v(e⋄ (t)) = e⋄ T (t)E⋄ TP ⋄ e⋄ (t) &gt; 0 ,
      </p>
      <p>
        E⋄ TP ⋄ = P ⋄ TE⋄ ≥ 0 ,
then the derivative of (
        <xref ref-type="bibr" rid="ref22">22</xref>
        ) becomes
      </p>
      <p>
        v˙ (e⋄ (t)) =
= e˙⋄ T(t)E⋄ TP ⋄ e⋄ (t) + e⋄ T(t)P ⋄ TE⋄ e˙⋄ (t) &lt; 0
and, inserting (
        <xref ref-type="bibr" rid="ref19">19</xref>
        ) in (
        <xref ref-type="bibr" rid="ref24">24</xref>
        ), it yields
v˙ (e⋄ (t)) = e⋄ T (t)(P ⋄ TA⋄e + A⋄eTP ⋄ )e⋄ (t) &lt; 0 , (
        <xref ref-type="bibr" rid="ref25">25</xref>
        )
It is evident that (29) can be satisfied only if
by denoting
P 1 = P 1T &gt; 0,
and, owing to emerged products P 3TAe, P 4TAe in (31), the
restriction on the structure of P 4 can be enunciated as
where δ &gt; 0, δ ∈ IR. Since now
then, with the notation
      </p>
      <p>P 4TAe = δP 3T (A − J C) ,</p>
      <p>P 4 = δP 3 ,</p>
      <p>
        Y = P 3T J ,
(31) implies (
        <xref ref-type="bibr" rid="ref14">14</xref>
        ). This concludes the proof.
      </p>
      <p>Remark 1. It is naturally to point out that the symmetrical
form of Lemma 2, defined for P 1 = P , P 3 = P 3T =
Q, is an equivalent inequality to the enhanced Lyapunov
inequality for Luenberger observer design [11].</p>
      <p>The above results can be generalized to formulate the
descriptor principle in fault PD observer design. The main
reason is to eliminate matrix inverse notations from the design
conditions.
4</p>
    </sec>
    <sec id="sec-5">
      <title>PD Observer Design</title>
      <p>If the observer errors between the system state vector and
the observer state vector as well as between the fault vector
and the vector of its estimate are defined as follows
eq(t) = q(t) − qe(t) ,
ef (t) = f (t) − f e(t) , (36)
then, for slowly-varying faults, it is reasonable to consider
[12]
e˙f (t) = 0 − f˙ e(t) = −M Ceq(t) − N C e˙q(t) .
(37)
Note, since f e(t) can be obtained as integral of f˙ e(t), an
adapting parameter matrix G can be adjust interactively to
set the amplitude of f e(t), i.e., as results it is
f e(t) = G</p>
      <p>f˙ e(τ )dτ .</p>
      <p>
        t
Z
0
To express the time derivative of the system state error eq(t),
the equations (1), (4) together with (2), (
        <xref ref-type="bibr" rid="ref5">5</xref>
        ) can be integrated
as
      </p>
      <p>
        e˙q(t) = Aeeq(t) + F ef (t) − LC e˙q(t) ,
where Ae is given in (
        <xref ref-type="bibr" rid="ref16">16</xref>
        ) and the PD observer system
matrix is
AP De = (In+LC)−1Ae = (In+LC)−1(A−J C) . (40)
Since (37), (39) can be rewritten in the following
composed form
e˙ q(t)
e˙ f (t)
=
−M C
      </p>
      <p>Ae F
0
eq(t)
ef (t) −</p>
      <p>LC 0
N C 0
e˙ q(t)</p>
      <p>,
e˙ f (t)
(41)
(32)
(33)
(34)
(35)
(38)
(39)</p>
      <p>eqT (t) efT (t) ,
A F
0 0
I◦ =
, J ◦ =
0
Ip</p>
      <p>J
M
, L◦ =</p>
      <p>L</p>
      <p>N
, C◦ = [ C</p>
      <p>
        The following solvability theorem is proposed to the
design PD fault observer in the structure proposed in (4)-(
        <xref ref-type="bibr" rid="ref6">6</xref>
        ).
Theorem 1. The PD fault observer (4)-(
        <xref ref-type="bibr" rid="ref6">6</xref>
        ) is stable if for
given positive scalar δ ∈ IR there exist a symmetric
positive definite matrix P 1◦ ∈ IR(n+p)× (n+p), a regular matriz
P 3◦ ∈ IR(n+p)× (n+p) and matrices Y ◦ ∈ IR(n+p)× m, Z◦ ∈
IR(n+p)× m such that
      </p>
      <p>P 1◦ = P 1◦T &gt; 0 ,
A◦TP 3◦ + P 3◦TA◦ − Y ◦C◦ − C◦T Y ◦T</p>
      <p>V 2◦1</p>
      <p>∗
V 2◦2
where
V 2◦1 = P 1◦ − P 3◦ + δP 3◦TA◦ − δY ◦C◦ − C◦TZ◦T , (54)</p>
      <p>V 2◦2 = −δP 3◦ − δP 3◦T − δZ◦C◦ − δC◦TZ◦T .
If the above conditions hold, the set of observer gain
matrices is given by the equations</p>
      <p>J ◦ = (P 3◦T )−1Y ◦,</p>
      <p>L◦ = (P 3◦T )−1Z◦
and the matrices J , L M , N can be separated with respect
to (43).
e◦(t)</p>
      <p>.
e˙◦(t)
(49)
(45)
(46)
(47)
(48)
(50)
(51)
(52)
&lt; 0 ,
(53)
(55)
(56)
Proof. Defining the Lyapunov function of the form
v(e• (t)) = e• T (t)E• TP • e• (t) &gt; 0 ,
then, using the property (58), the time derivative of (57)
along the trajectory of (51) becomes
in analogy with (29) then (58) implies</p>
      <p>P 1◦ = P 1◦T &gt; 0,</p>
      <p>P 2◦ = P 2◦T = 0
and, using (50) and (62), (63) in (61), it yields
" 0</p>
      <p>Ae◦T #
I◦ −De◦T</p>
      <p>P 1◦ 0
P 3◦ P 4◦
+
" P 1◦ P 3◦T #
0</p>
      <p>P 4◦T
0</p>
      <p>
        I◦
= −P 4◦T (I◦ +L◦C◦) − (I◦ +L◦C◦)TP 4◦ = −R•
and comparing (
        <xref ref-type="bibr" rid="ref7">7</xref>
        ) and (65), then, if the inequalities
(52)(53) are satisfied, the Schur complement property (
        <xref ref-type="bibr" rid="ref7">7</xref>
        )
applied to (65) implies that R• is positive definite.
      </p>
      <p>Since P 4◦ is regular, (I◦ + L◦C◦) is also regular and so
AP De given by (40) exists. This concludes the proof.</p>
      <p>
        Since there is no restriction on the structure of P 3 in
Theorem 1, it follows that the problem of checking the existence
of a stable system matrix of PD adaptive fault observer in a
given matrix space may also be formulated with
symmetric matrices P 3 and P 3. This limit case of the LMI
structure design condition, bound to a single symmetric matrix,
is given by the following theorem.
Theorem 2. The PD observer (4)-(
        <xref ref-type="bibr" rid="ref6">6</xref>
        ) is stable if for given
positive scalar δ ∈ IR there exist a symmetric positive
definite matrix Q◦ ∈ IR(n+p)× (n+p) and matrices Y ◦ ∈
IR(n+p)× m, Z◦ ∈ IR(n+p)× m such that
      </p>
      <p>Q◦ = Q◦T &gt; 0 ,
A◦TQ◦ + Q◦A◦ − Y ◦C◦ − C◦T Y ◦T</p>
      <p>Note, the design conditions formulated in Theorem 2 give
potentially more conservative solutions.</p>
    </sec>
    <sec id="sec-6">
      <title>5 Illustrative Example</title>
      <p>The considered system is represented by the model (1), (2)
with the model parameters [10]
(71)
(72)
(73)
(74)
(75)
(76)
(77)
(78)
(80)
 −0.1316</p>
      <p>0.0252
That means the PD observer is stable as well as its "P" part
is stable, too. Moreover, also the descriptor form (45) of the
PD observer is stable, where
ρ (I◦ + L◦C◦)−1(A◦ − J ◦C◦) =</p>
      <p>−1.7763, −2.0966,
−0.6629 ± 0.7872 i, −1.3632 ± 0.4931 i
Comparing with a solution of (52)-(55) for the δ = 0.95, it
is possible to verify that in this case
ρ(Ae) = { −6.8230, −10.3876, −81.5789, −472.0230 } ,
ρ(AP De) = { −0.9562, −0.9774, −7.2561, −9.8300 } ,
ρ (I◦ + L◦C◦)−1(A◦ − J ◦C◦) =
−1.0240, −1.0748, −6.4810, −9.1501</p>
      <p>−0.9650 ± 0.0068 i
which implies in this case a faster dynamics of the descriptor
form of the PD observer but a slower for the PD observer.
Note, the exploitation of δ = 0.75 leads in this case to
unstable "P" part of the PD observer.
,
.
2.5
2</p>
      <p>Although many actuator faults can cause the gain to drift,
in practice the faults lead to an abrupt change in gain [21].
To simulate this phenomena, it was assumed that the fault in
actuators for (1) was given by
f (t) =





</p>
      <p>0,
tsbf−htsa (t − tsa),
fh,</p>
      <p>tsb ≤ tca ,
 − tcbf−htca (t − tcb), tca &lt; tcb ,
 0,
t ≥ tcb ,
t ≤ tsa ,
tsa &lt; tsb ,
where, analyzing the single first actuator fault estimation, it
was set</p>
      <p>fh = 2, tsa = 30s, tsb = 35s, tea = 65s, teb = 70s ,
and for the single second actuator fault these parameters
were
fh = 2, tsa = 100s, tsb = 105s, tea = 135s, teb = 140s .
It is demonstrates that for equal fh in the first and the
second actuator faults it is possible for given B to adjust the
common adapting parameter matrix G in (38) as follows
G =
40.0
5.9
5.9
22.0
.</p>
      <p>The obtained results are illustrated in Fig. 1 where, just in
terms of rendering, all faults responses and their estimates
were combined into a single image, and so the
demonstration can not be seen as a progressive sequence of single
faults in the actuators system. This figure presents the fault
signals, as well as their estimations, reflecting the single first
actuator fault starting at the time instant t = 30s and
applied for 40s and then the fault of the second actuator is
demonstrated beginning in the time instant t = 100s and
lasts for 40s. The presented simulation was carried out in
the system autonomous mode, practically the same results
were obtained for forced regime of the system.</p>
      <p>The adapting parameter G and the tuning parameter δ
were set interactively considering the maximal value of fault
signal amplitude fh and the fault observer dynamics. It can
be seen that the exists very small differences between the
signals reflecting single actuator faults and the observer
approximate ones for slowly warring piecewise constant
actuator faults. The principle can be used directly in the control
structures with the fault compensation [4], but can not be
directly used to localize actuator faults [14].
6</p>
    </sec>
    <sec id="sec-7">
      <title>Concluding Remarks</title>
      <p>Based on the descriptor system approach a new PD fault
observer design method for continuous-time linear systems
and slowly-varying actuator faults is introduced in the paper.
Presented version is derived in terms of optimization over
LMI constraints using standard LMI numerical procedures
to manipulate the fault observer stability and fault
estimation dynamics. Presented in the sense of the second
Lyapunov method expressed through LMI formulation, design
conditions guaranty the asymptotic convergence of the state
as well as fault estimation errors. The numerical simulation
results show good estimation performances.</p>
    </sec>
    <sec id="sec-8">
      <title>Acknowledgments</title>
      <p>The work presented in this paper was supported by VEGA,
the Grant Agency of the Ministry of Education and the
Academy of Science of Slovak Republic, under Grant No.
1/0348/14. This support is very gratefully acknowledged.</p>
    </sec>
  </body>
  <back>
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