Robust Decentralized Controller Design for Descriptor-type
Systems with Distributed Time Delay
ALTU ˘
G˙
IFTAR
Department of Electrical and Electronics Engineering
Eskis¸ehir Technical University
26555 Eskis¸ehir, TURKEY
Abstract: - Robust decentralized controller design is considered for linear time-invariant large-scale
descriptor-type systems with distributed time delay which are composed of overlapping subsystems. A
robustness bound, that accounts for the interactions among the subsystems and for modeling uncertainties both
in the subsystem models and the interactions, is derived using overlapping decompositions and expansions. A
robust decentralized controller design approach using this bound is then proposed. Once the robustness bound
is derived, the proposed approach is decoupled for each subsystem and, for each subsystem, it is based on
a local nominal model, which is also derived using overlapping decompositions and expansions. Satisfying
a simple condition, involving the derived robustness bound, however, guarantees the robust stability of the
overall actual closed-loop system.
Key-Words: - Robust controller design, Decentralized control, Time-delay systems, Descriptor-type systems,
Distributed time delay, Large-scale systems, Overlapping decompositions
Received: April 12, 2023. Revised: February 7, 2024. Accepted: March 19, 2024. Published: April 18, 2024.
1 Introduction
Many practical systems, especially large-scale sys-
tems [1] may be subject to time delays [2]. Such
systems, which are typically named as time-delay
systems [3], can be described by delay-differential
equations [4]. For some time-delay systems, such as
telerobotic systems [5], however, delay-differential
equations must be coupled with delay-algebraic
equations to describe the dynamics of the system.
Such systems are known as descriptor-type time-
delay systems. Descriptor-type time-delay systems
impose a challenge since their response may be
discontinuous and even impulsive [6].
Time delays in a system may be pointwise or
distributed [7]. Distributed time delay may appear
in many application areas, such as neural networks
[8], biology [9], traffic flow [10], logistics [11], and
combustion control [12].
There are many examples of large-scale systems,
such as interconnected power systems [13], freeway
traffic regulation systems [14], intelligent vehicle-
highway systems [15], and data-communication net-
works [16], which consist of subsystems with over-
lapping dynamics. To analyze and design controllers
for such systems, the approach of overlapping de-
compositions was first introduced in [17]. Although,
initially, this approach was introduced for linear
time-invariant (LTI) delay-free systems, since then it
has also been extended to time-delay systems with
both pointwise and distributed time delays [18], [19],
[20], [21].
In general, it is not possible to obtain an ex-
act model of any practical system. Therefore, any
designed controller for a practical system must be
robust against modeling uncertainties [22]. To en-
sure such a robustness, a robustness bound, which
accounts for modeling uncertainties in centralized
descriptor-type time-delay systems were considered
in [23]. In the case of large-scale systems, however,
it may be necessary or practical to ignore the inter-
actions among subsystems during controller design
[24]. In this case, besides modeling uncertainties,
the designed controllers must also be robust against
the neglected interactions. Therefore, in the present
work, we consider large-scale LTI descriptor-type
distributed-time-delay systems consisting of subsys-
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tems which dynamically overlap and extend the
robustness bound also to account for the neglected
interactions between the subsystems and any model-
ing uncertainties in the interactions. We then propose
a robust decentralized controller design approach
using this bound. Once the robustness bound is
derived, the proposed approach is decoupled for
each subsystem and, for each subsystem, it is based
on a local nominal model, which is also derived
using overlapping decompositions and expansions.
Satisfying a simple condition, involving the derived
robustness bound, however, guarantees the robust
stability of the overall actual closed-loop system.
Throughout the paper, Rand Crespectively
denote the sets of real and complex numbers. For
sC,Re(s)denotes the real part of s. For positive
integers kand l,Rkand Rk×ldenote the spaces of,
respectively, k-dimensional real vectors and k×l-
dimensional real matrices. Ikdenotes the k×k-
dimensional identity matrix and Idenotes the iden-
tity matrix of appropriate dimensions. 0may denote
either the scalar zero, a zero matrix, or a matrix
function which is identically zero. det(·),rank(·),
¯σ(·), and σ(·)respectively denote determinant, the
rank, the maximum singular value, and the minimum
singular value of the indicated matrix. bdiag(···)
denotes a block diagonal matrix with the indicated
matrices on the main diagonal. For a matrix function
M(·) : [τ, 0] Rk×l,kMk:= R0
τ¯σ(M(θ)) .
Finally, jdenotes the imaginary unit (i.e., j:=
1).
2 Problem Statement
In this work, as mentioned in the introduction, we
consider descriptor-type large-scale LTI distributed-
time-delay systems, which are composed of overlap-
ping subsystems. In practice, such subsystems may
overlap in many different ways. For simplicity of
presentation, however, in here we consider the case
of only two subsystems which are interconnected
through another dynamic subsystem, which form the
overlapping part. Such a system can compactly be
described as:
E˙x(t) = A0x(t)
+Z0
τ
(A(θ)x(t+θ) + B(θ)u(t+θ)) (1)
y(t) = Z0
τ
C(θ)x(t+θ) (2)
where τ > 0is the maximum time-delay in the
system and tis the time variable. The state, the input,
and the output vectors are decomposed as:
x=
x1
xc
x2
, u =u1
u2, y =y1
y2,(3)
where xiRni,uiRpi, and yiRqiare, re-
spectively, the state, the input, and the output vectors
of the ith subsystem (i= 1,2), and xcRncis the
state vector of the overlapping part. The matrices
ERn×n,A0Rn×n, and the matrix functions
A(·) : [τ, 0] Rn×n,B(·) : [τ, 0] Rn×p, and
C(·):[τ, 0] Rq×n(where n:= n1+nc+n2,
p:= p1+p2, and q:= q1+q2) are also decomposed
as:
E=
E10 0
0Ec0
0 0 E2
, A0=
A0
10 0
0A0
c0
0 0 A0
2
,
A(·) =
A1(·)A1c(·) 0
Ac1(·)Ac(·)Ac2(·)
0A2c(·)A2(·)
,
B(·) =
B1(·) 0
0 0
0B2(·)
,
and
C(·) = C1(·) 0 0
0 0 C2(·),
where the partitionings are compatible with those
in (3). All the submatrix functions shown above are
assumed to be bounded, except that they are allowed
to include Dirac-delta terms, δ(θ+h),h[0, τ],
except that A(0) is assumed to be bounded (i.e.,
each submatrix function of A(θ)can include a term
δ(θ+h),h(0, τ], but not δ(θ)). Inclusion of these
terms allow representation of pointwise time delays,
together with distributed time delay. Furthermore, it
is assumed that the submatrix functions of A(·)and
B(·)are subject to uncertainties. Thus, representing
any one of these submatrix functions by M(·), we
assume that M(·) = Mn
(·) + Mu
(·), where Mn
(·)
is the known nominal part and Mu
(·)is the unknown
uncertain part. The uncertain parts, however, are
assumed to be bounded as follows:
kAu
1k α1,kAu
1ck α1c,kAu
c1k αc1,
kAu
ck αc,kAu
c2k αc2,kAu
2ck α2c,
kAu
2k α2,kBu
1k β1,kBu
2k β2,
(4)
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where αs and βs are known non-negative bounds.
Since the input-output uncertainties can in general be
represented either at the input or at the output, here
we assume that all such uncertainties are represented
at the input, hence there are no uncertainties in C(·).
It is also assumed that rank(E) = ¯nn,
where stands for 1,c, or 2, with ¯n< n, for at
least one of 1,c, or 2. This assumption means that
rank(E)< n, which means that the system (1)–
(2) is a descriptor-type system [6]. It is, however,
asuumed that:
Assumption 1: If ¯n< n, then rank(LA0
R) =
n¯n, where LRn¯n×nand R
Rn×n¯nare such that the rows of Lspan the
left null space of Eand the columns of Rspan
the right null space of E.
The above assumption implies that there exists
a unique solution to (1), for any suitable initial
condition, x(t+θ),θ[τ, 0] [4].
The characteristic function of the system (1) is
given by
ψ(s) := det(sE A(s)) ,(5)
where
A(s) := A0+Z0
τ
A(θ)e . (6)
The modes of the system (1) are the roots of ψ(s) =
0. It is known that the system (1) has infinitely many
modes, in general [25]. However, under Assumption
1, it has only finitely many modes with real part
greater than
νf:= sup{Re(s)|det( ¯
A(s)) = 0},(7)
where ¯
A(s) := LA(s)R, where A(s)is as given in
(6),
L:= bdiag(L1,Lc,L2)(8)
and
R:= bdiag(R1,Rc,R2),(9)
where Land Rare as in Assumption 1, if ¯n<
n, and they are missing in (8) and (9), otherwise
[26].
It is known that (1)–(2) can not be stabilized
by a finite-dimensional proper LTI controller unless
νf<0[27]. Thus, since our aim is to stabilize (1)–
(2) for all uncertainties satisfying (4), we make the
following assumption:
Assumption 2: νf<0for any uncertainties satis-
fying (4).
This assumption implies that the system (1) has
only finitely many unstable modes. A mode is called
as an unstable mode if it has a non-negative real part.
Our aim is to design decentralized (possibly time-
delay) LTI controllers:
Ui(s) = Ki(s)Yi(s), i = 1,2,(10)
where Ui(s)and Yi(s)are the Laplace transforms
of, respectively, ui(t)and yi(t), and Ki(s)is the
transfer function matrix (TFM) of the ith controller.
These controllers are to be designed such that
each local nominal closed-loop system is stable,
a local performance criteria is satisfied for each
local nominal closed-loop system, and
the actual overall closed-loop system is ro-
bustly stable for all uncertainties that satisfy the
bounds (4).
Furthermore, the design of each decentralized con-
troller is to be based on a local nominal model,
which is to be derived next.
3 Local Nominal Models
In order to obtain a local nominal model, we expand
[21] the above overlappingly decomposed system by
using the transformation
T=
In10 0
0Inc0
0Inc0
0 0 In2
.(11)
The expanded system is described as:
ˆ
E˙
ˆx(t) = ˆ
A0ˆx(t)
+Z0
τˆ
A(θ)ˆx(t+θ) + ˆ
B(θ)ˆu(t+θ) (12)
ˆy(t) = Z0
τ
ˆ
C(θ)ˆx(t+θ) (13)
where
ˆ
E:= bdiag( ˆ
E1,ˆ
E2),
where
ˆ
E1:= bdiag (E1, Ec),ˆ
E2:= bdiag (Ec, E2),
ˆ
A0:= bdiag( ˆ
A0
1,ˆ
A0
2),
where
ˆ
A0
1:= bdiag A0
1, A0
c,ˆ
A0
2:= bdiag A0
c, A0
2,
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ˆ
A(θ) := ˆ
A1(θ)ˆ
A12(θ)
ˆ
A21(θ)ˆ
A2(θ),
where
ˆ
A1(θ) := A1(θ)A1c(θ)
Ac1(θ)Ac(θ),
ˆ
A12(θ) := 0 0
0Ac2(θ),
ˆ
A21(θ) := Ac1(θ) 0
0 0 ,
and
ˆ
A2(θ) := Ac(θ)Ac2(θ)
A2c(θ)A2(θ),
ˆ
B(θ) := bdiag ˆ
B1(θ),ˆ
B2(θ),
where
ˆ
B1(θ) := B1(θ)
0,ˆ
B2(θ) := 0
B2(θ),
and
ˆ
C(θ) := bdiag ˆ
C1(θ),ˆ
C2(θ),
where,
ˆ
C1(θ) := C1(θ) 0 ,
and
ˆ
C2(θ) := 0C2(θ).
Note that relations ˆ
ET =T E,ˆ
A0T=T A0,
ˆ
A(θ)T=T A(θ),ˆ
B(θ) = T B(θ), and ˆ
C(θ)T=
C(θ)are satisfied. This implies that the expanded
system (12)–(13) is an extension of the original sys-
tem (1)–(2) [21]. Thus, the expanded system includes
the original system, and hence the two systems have
the same input-output map [20].
We note that, because of the block diagonal
structure of ˆ
Eand of ˆ
A0, Assumption 1 implies
that a unique solution to (12), for any suitable initial
condition, ˆx(t+θ),θ[τ, 0], is guaranteed. Here,
we also make the following assumption:
Assumption 3:
sup nRe(s)|det ¯
ˆ
A(s)= 0o<0,(14)
for any uncertainties satisfying (4), where ¯
ˆ
A(s) :=
ˆ
Lˆ
A(s)ˆ
R, where
ˆ
A(s) := ˆ
A0+Z0
τ
ˆ
A(θ)e , (15)
ˆ
L:= bdiag(L1,Lc,Lc,L2),(16)
and
ˆ
R:= bdiag(R1,Rc,Rc,R2),(17)
where Land Rare as in Assumption 1, if ¯n<
n, and they are missing in (16) and (17), otherwise.
We note that, since the expanded system includes the
original system, Assumption 3, in particular, implies
Assumption 2. Thus, under this assumption, both the
expanded system and the original system have only
finitely many unstable modes.
We note that the expanded system (12)–(13) is
composed of two disjoint subsystems with only
weak interactions (through ˆ
A12(·)and ˆ
A21(·)). Thus,
alocal model can be obtained by ignoring these
interactions as:
ˆ
Ei˙
ˆxi(t) = ˆ
A0
iˆxi(t) + Z0
τˆ
Ai(θ)ˆxi(t+θ)
+ˆ
Bi(θ)ˆui(t+θ) (18)
ˆyi(t) = Z0
τ
ˆ
Ci(θ)ˆxi(t+θ) (19)
for i= 1,2. A local nominal model, for i= 1,2,
can then be obtained by taking the nominal part of
(18)–(19):
ˆ
Ei˙
ˆxi(t) = ˆ
A0
iˆxi(t) + Z0
τˆ
An
i(θ)ˆxi(t+θ)
+ˆ
Bn
i(θ)ˆui(t+θ) (20)
ˆyi(t) = Z0
τ
ˆ
Ci(θ)ˆxi(t+θ) (21)
where
ˆ
An
1(θ) := An
1(θ)An
1c(θ)
An
c1(θ)An
c(θ),
ˆ
An
2(θ) := An
c(θ)An
c2(θ)
An
2c(θ)An
2(θ),
ˆ
Bn
1(θ) := Bn
1(θ)
0,
and
ˆ
Bn
2(θ) := 0
Bn
2(θ).
Our final two assumptions are as follows:
Assumption 4: For i= 1,2,
sup nRe(s)|det ¯
ˆ
An
i(s)= 0o<0,(22)
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where ¯
ˆ
An
i(s) := ˆ
Liˆ
An
i(s)ˆ
Ri, where
ˆ
An
i(s) := ˆ
A0
i+Z0
τ
ˆ
An
i(θ)e , (23)
ˆ
L1:= bdiag(L1,Lc),ˆ
L2:= bdiag(Lc,L2),(24)
and
ˆ
R1:= bdiag(R1,Rc),ˆ
R2:= bdiag(Rc,R2),(25)
where Land Rare as in Assumption 3.
Assumption 5: ˆm=m1+m2, where ˆmdenotes the
number of unstable modes of the expanded system
(12)–(13) (which is finite by Assumption 3) and mi
(i= 1,2) denotes the number of unstable modes of
the ith local nominal model (20)–(21) (which is also
finite by Assumption 4).
4 A Robustness Bound
In this section, we derive a robustness bound, to
account for the
uncertainties in the subsystem models,
neglected interactions between the subsystem
models, and
uncertainties in the interactions between the
subsystem models.
For this, from (20)–(21), we obtain the TFM of the
ith local nominal model (i= 1,2) as:
Γn
i(s) = ˆ
Ci(s)sˆ
Eiˆ
An
i(s)1ˆ
Bn
i(s)(26)
where ˆ
Ci(s) := R0
τˆ
Ci(θ)e,ˆ
An
i(s)is defined in
(23), and ˆ
Bn
i(s) := R0
τˆ
Bn
i(θ)e. The TFM for
the overall design model is then given as
Γn(s) = bdiag n
1(s),Γn
2(s)) .(27)
On the other hand, since the expanded system
(12)–(13) includes the original system (1)–(2), the
TFM, Γ(s), of the actual original system is equal to
the TFM, ˆ
Γ(s), of the expanded system:
Γ(s) = ˆ
Γ(s) = ˆ
C(s)sˆ
Eˆ
A(s)1ˆ
B(s)(28)
where ˆ
C(s) := R0
τˆ
C(θ)e,ˆ
A(s)is defined in
(15), and ˆ
B(s) := R0
τˆ
B(θ)e.
Now, let ∆(s)be such that:
Γ(s) = Γn(s) (I+ ∆(s)) .(29)
Then, we can use a frequency-dependent upper
bound on the norm of ∆(jω)as a robustness bound.
Such a bound can be obtained as follows:
Lemma 1: Suppose that δd(ω)>0,ωR. Then
¯σ(∆(jω)) δ(ω) := δn(ω)
δd(ω),ωR,(30)
where
δd(ω) := σ(H(jω)) max δ1
d(ω), δ2
d(ω)
max nδ1,2
d(ω), δ2,1
d(ω)o,(31)
where
H(s) := ˆ
Bn
1(s)H12(s)
H21(s)ˆ
Bn
2(s),(32)
where
H12(s) := 0 0
0R0
τAn
c2(θ)e G2(s)
and
H21(s) := R0
τAn
c1(θ)e 0
0 0 G1(s)
where, for i= 1,2,
Gi(s) := sˆ
Eiˆ
An
i(s)1ˆ
Bn
i(s),
and
δ1
d(ω) := ˆα1g1(ω), δ1,2
d(ω) := αc2g2(ω),
δ2
d(ω) := ˆα2g2(ω), δ2,1
d(ω) := αc1g1(ω),
where, for i= 1,2,gi(ω) := ¯σ(Gi(jω)) and ˆαi:=
max(αi, αc) + max(αci, αic), and
δn(ω) := max δ1
n(ω), δ2
n(ω)
+ max δ1,2
n(ω), δ2,1
n(ω),(33)
where
δ1
n(ω) := β1+ ˆα1g1(ω), δ2
n(ω) := β2+ ˆα2g2(ω),
δ1,2
n(ω) := ¯σ(H12(jω)) + αc2g2(ω),
and
δ2,1
n(ω) := ¯σ(H21(jω)) + αc1g1(ω).
Proof: ∆(s)in (29) can be chosen to satisfy
sˆ
Eˆ
A(s)1ˆ
B(s)
=sˆ
Eˆ
An(s)1ˆ
Bn(s) (I+ ∆(s)) ,(34)
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where ˆ
An(s) := bdiag ˆ
An
1(s),ˆ
An
2(s)and
ˆ
Bn(s) := bdiag ˆ
Bn
1(s),ˆ
Bn
2(s). By premultiplying
both sides of (34) by (sˆ
Eˆ
A(s)) and rearranging
terms, we obtain N(s) = D(s)∆(s), where
D(s) := sˆ
Eˆ
A(s)G(s)
and
N(s) := ˆ
B(s)D(s),
where G(s) := bdiag (G1(s), G2(s)). The result
then follows by noting that ¯σ(N(jω)) δn(ω)and
σ(D(jω)) δd(ω).
Remark: The bound (30) is not defined if δd(ω)
0, i.e., if σ(H(jω)) max{δ1
d(ω), δ2
d(ω)}+
max{δ1,2
d(ω), δ2,1
d(ω)}, for some ωR. However,
note that the matrix H(jω)contains the nominal
input terms ˆ
Bn
i(jω)on the diagonal blocks (which
typically have large norm for any ω) and inter-
action terms (which typically have smaller norm)
on the off-diagonal blocks. Furthermore, the terms
δ
d(ω)contain bounds on the uncertainties (which are
typically small). Therefore, typically, σ(H(jω)) >
max{δ1
d(ω), δ2
d(ω)}+ max{δ1,2
d(ω), δ2,1
d(ω)}, and
hence δd(ω)>0.
5 Controller Design
We now consider the problem of designing de-
centralized controllers (10) so that the following
requirements are satisfied:
(i) each local nominal closed-loop system, (20)–
(21) under the local controller Ki(s), is stable,
(ii) a local performance criteria (if any) is satisfied
for each local nominal closed-loop system, and
(iii) the actual overall closed-loop system, (1)–(2)
under the overall decentralized controller (10) is
robustly stable for all uncertainties that satisfy
(4).
Requirements (i) and (ii) are local requirements
which can be satisfied independently for each chan-
nel. To satisfy requirement (iii), we propose to
design the ith controller (i= 1,2), Ki(s), to satisfy
¯σ(Tn
i(jω)) <1
δ(ω),ωR,(35)
where Tn
i(s) := Γn
i(s)Ki(s) [I+ Γn
i(s)Ki(s)]1is
the complementary sensitivity matrix for the ith
local nominal closed-loop system and δ(ω)is given
by (30). The following theorem shows that when
requirement (i) is satisfied for each local nominal
closed-loop system, satisfying (35) guarantees robust
stability of the actual overall closed-loop system.
Theorem 1: Suppose that Assumptions 1, 3, 4, and
5 hold. Also suppose that each local nominal closed-
loop system is stable and that (35) is satisfied. Then,
the actual overall closed-loop system is robustly
stable for all uncertainties that satisfy (4).
Proof: Assumption 1 is needed for the validity of
the model (1)–(2). This also implies the validity of
the models (12)–(13), (18)–(19), and (20)–(21). The
block diagonal structure (27) of the overall design
model, together with Assumption 4, implies that
there are no modes of the overall design model
approaching the imaginary axis from left and that
the number of unstable modes of the overall design
model is finite. Assumption 3, on the other hand,
implies that there are no modes of the expanded
open-loop system approaching the imaginary axis
from left and that the number of unstable modes
of the expanded open-loop system is finite. The
complementary sensitivity matrix for the overall
closed-loop design model is
Tn(s)=Γn(s)K(s) [I+ Γn(s)K(s)]1
= bdiag (Tn
1(s), T n
2(s)) (36)
where K(s) := bdiag (K1(s), K2(s)) is the TFM
for the overall controller. Due to the block diagonal
structure of the overall closed-loop design model,
stability of the local nominal closed-loop systems
implies the stability of the overall closed-loop design
model. The block diagonal structure of the overall
design model, on the other hand, implies that the
number of unstable modes of the overall design
model is equal to the sum of the number of the
unstable modes of the local nominal models. Then,
by Assumption 5, the number of the unstable modes
of the expanded system (12)–(13) is equal to the
number of unstable modes of the overall design
model. Furthermore, by (36),
¯σ(Tn(jω)) = max
i∈{1,2}{¯σ(Tn
i(jω))}.
Thus, when (35) is satisfied, by (30), we have
¯σ(Tn(jω)) <1
¯σ(∆(jω)) ,ωR.(37)
This, however, implies that the actual expanded
closed-loop system is robustly stable [22]. However,
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since the actual expanded system includes the actual
original system, this implies the robust stability of
the actual original closed-loop system [20].
Note that, once the robustness bound (30) is ob-
tained, (35) is in fact a local requirement. This means
that each local controller Ki(s)can be designed
independently of others based on the local nominal
model (20)–(21). For this, any centralized controller
design approach developed for descriptor-type LTI
time-delay systems (e.g., [28], [29]) can be used.
6 Conclusions
Robust decentralized controller design has been con-
sidered for large-scale LTI descriptor-type systems
with distributed time delay which are composed
of overlapping subsystems. Using overlapping de-
compositions and expansions, a frequency dependent
robustness bound, (30), has been derived. A robust
decentralized controller design approach using this
bound has then been proposed. Once the robustness
bound is derived, the proposed approach is decou-
pled for each subsystem and, for each subsystem, it
is based on a local nominal model. Satisfying a sim-
ple condition, (35), however, guarantees the robust
stability of the overall actual closed-loop system.
Since the derived bound is frequency dependent,
the approach is, in general, less conservative than
an approach in which a constant bound is used.
Furthermore, it also allows frequency shaping [30].
Although, for simplicity of presentation, we have
considered only the case of two overlapping subsys-
tems, the proposed approach can be extended to such
cases as Nsubsystems with a common overlapping
part or a string of Noverlapping subsystems.
References
[1] L. Bakule, “Decentralized control: An overview, Annual
Reviews in Control, vol. 32, pp. 87–98, 2008.
[2] S.-I. Niculescu, Delay Effects on Stability: A Robust Con-
trol Approach, Lecture Notes in Control and Information
Sciences, No. 269. London: Springer-Verlag, 2001.
[3] J.-P. Richard, “Time-delay systems: an overview of some
recent advances and open problems, Automatica, vol. 39,
pp. 1667–1694, 2003.
[4] J. K. Hale and S. M. Verduyn Lunel, Introduction to
Functional Differential Equations. New York: Springer-
Verlag, 1993.
[5] N. Mollet, ed., Remote and Telerobotics. InTech, 2010.
[6] G.-R. Duan, Analysis and Design of Descriptor Linear
Systems. New York: Springer, 2010.
[7] K. L. Cooke and Z. Grossman, “Discrete delay, distributed
delay and stability switches, Journal of Mathematical
Analysis and Applications, vol. 86, pp. 592–627, 1982.
[8] B. Rahman, K. B. Blyuss, and Y. N. Kyrychko, “Dynam-
ics of neural systems with discrete and distributed time
delays, SIAM Journal on Applied Dynamical Systems,
vol. 14, pp. 2069–2095, 2015.
[9] H. ¨
Ozbay, C. Bonnet, and J. Clairambault, “Stability anal-
ysis of systems with distributed delays and application to
hematopoietic cell maturation dynamics, in Proceedings
of the IEEE Conference on Decision and Control, (Cancun,
Mexico), pp. 2050–2055, Dec. 2008.
[10] W. Michiels, C.-I. Mor˘
arescu, and S.-I. Niculescu, “Con-
sensus problems with distributed delays, with application
to traffic flow models, SIAM Journal on Control and
Optimization, vol. 48, pp. 77–101, 2009.
[11] L. Berezansky and E. Braverman, “Oscillation properties
of a logistic equation with distributed delay, Nonlinear
Analysis: Real World Applications, vol. 4, pp. 1–19, 2003.
[12] L. Xie, E. Fridman, and U. Shaked, “Robust Hcontrol of
distributed delay systems with application to combustion
control, IEEE Transactions on Automatic Control, vol. 46,
pp. 1930–1935, 2001.
[13] D. D. ˇ
Siljak, Large–Scale Dynamic Systems: Stability and
Structure. New York: North–Holland, 1978.
[14] L. Isaksen and H. J. Payne, “Suboptimal control of linear
systems by augmentation with application to freeway traf-
fic regulation, IEEE Transactions on Automatic Control,
vol. AC–18, pp. 210–219, 1973.
[15] S. S. Stankovi´
c, M. J. Stanojevi´
c, and D. D. ˇ
Siljak, “De-
centralized overlapping control of a platoon of vehicles,
IEEE Transactions on Control Systems Technology, vol. 8,
pp. 816–832, 2000.
[16] J. S. Meditch and J. C. Mandojana, A decentralized
algorithm for optimal routing in data–communication net-
works, Large Scale Systems, vol. 1, pp. 149–158, 1980.
[17] M. Ikeda and D. D. ˇ
Siljak, “Overlapping decompositions,
expansions, and contractions of dynamic systems, Large
Scale Systems, vol. 1, pp. 29–38, 1980.
[18] L. Bakule and J. M. Rossell, “Overlapping controllers
for uncertain delay continuous-time systems, Kybernetika,
vol. 44, pp. 17–34, 2008.
[19] A. Momeni and A. G. Aghdam, “Overlapping control
systems with delayed communication channels: stability
analysis and controller design, in Proceedings of the
American Control Conference, (St. Louis, MO, U.S.A.),
pp. 4235–4241, June 2009.
[20] A. ˙
Iftar, “Inclusion, restriction, and overlapping decompo-
sitions of neutral systems with distributed time-delay, in
Proceedings of the 14th IFAC Symposium on Large Scale
Complex Systems, IFAC-PapersOnLine, 49-4, (Riverside,
CA, USA), pp. 73–78, May 2016.
[21] A. ˙
Iftar, “Overlapping decentralized controller design
for descriptor-type systems with distributed time-delay,
WSEAS Transactions on Circuits and Systems, vol. 20,
pp. 257–263, 2021.
[22] K. Zhou, J. C. Doyle, and K. Glover, Robust and Optimal
Control. Englewood Cliffs: Prentice Hall, 1996.
[23] A. ˙
Iftar, “Robust controller design for descriptor-type time-
delay systems, WSEAS Transactions on Systems, vol. 20,
pp. 289–294, 2021.
[24] D. D. ˇ
Siljak, Decentralized Control of Complex Systems.
San Diego: Academic Press, Inc., 1991.
WSEAS TRANSACTIONS on SYSTEMS and CONTROL
DOI: 10.37394/23203.2024.19.12
Altug Iftar
E-ISSN: 2224-2856
125
Volume 19, 2024
[25] W. Michiels and S.-I. Niculescu, Stability and Stabilization
of Time-Delay Systems. Philadelphia: SIAM, 2007.
[26] W. Michiels and S.-I. Niculescu, Stability, Control, and
Computation for Time-Delay Systems: An Eigenvalue-
Based Approach. Philadelphia: SIAM, 2014.
[27] J. J. Loiseau, M. Cardelli, and X. Dusser, “Neutral-type
time-delay systems that are not formally stable are not
BIBO stabilizable, IMA Journal of Mathematical Control
and Information, vol. 19, pp. 217–227, 2002.
[28] S. G¨
um¨
us¸soy and W. Michiels, “Fixed-order H-infinity
control for interconnected systems using delay differen-
tial algebraic equations, SIAM Journal on Control and
Optimization, vol. 49, pp. 2212–2238, 2011.
[29] W. Michiels, “Spectrum-based stability analysis and stabil-
isation of systems described by delay differential algebraic
equations, IET Control Theory and Applications, vol. 5,
pp. 1829–1842, 2011.
[30] D. Pilbauer, T. Vyhlidal, and W. Michiels, “Spectral
design of output feedback controllers for systems pre-
compensated by input shapers, in Preprints of the 12th
IFAC Workshop on Time-delay Systems, (Ann Arbor, MI,
USA), June 2015.
Contribution of Individual Authors to
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(Ghostwriting Policy)
The author contributed in the present research, at all
stages from the formulation of the problem to the
final findings and solution.
Sources of Funding
This work has been supported by the Scientific Re-
search Projects Commission of Eskis¸ehir Technical
University.
Conflicts of Interest
The author has no conflicts of interest to declare that
are relevant to the content of this article.
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