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Z
1
e
A
q
t
C
q
C
q
e
A
q
t
dt
Q
q
¼
ð
7
Þ
0
Z
1
e
A
q
t
B
q
B
q
e
A
q
t
dt
P
q
¼
ð
8
Þ
0
The solution of the stable switched linear system in the sense of Lyapunov is
obtained by solving the following two equations for each subsystem (Andres et al.
2013
; Antoulas
2009
; Kouki et al.
2013b
; Mehrmann et al.
2012
):
P
q
A
q
þ
B
q
B
q
¼
A
q
P
q
þ
0
ð
9
Þ
A
q
Q
q
þ
C
q
C
q
¼
Q
q
A
q
þ
0
ð
10
Þ
The solutions of these two equations are P and Q (Antoulas
2009
; Gugercin
2008
). P
q
2
R
n
n
and Q
q
2
R
n
n
are called the reachability and the observability
gramians matrices, respectively.
The Eq. (
9
) is proved by the following formulation (Bao et al.
2006
):
Z
1
½A
q
e
A
q
t
B
q
B
q
e
A
q
t
þ
e
A
q
t
B
q
B
q
e
A
q
t
A
T
A
q
P
q
þ
P
q
A
q
¼
dt
0
ð
11
Þ
Z
1
e
A
q
t
B
q
B
q
e
A
q
t
B
q
B
q
¼
d
ð
Þ
0
The Eq. (
10
) is proved by the following formulation:
Z
1
A
q
e
A
q
t
C
q
C
q
e
A
q
t
e
A
q
t
C
q
C
q
e
A
q
t
A
A
q
Q
q
þ
Q
q
A
q
¼
½
þ
dt
0
ð
12
Þ
Z
1
e
A
q
t
C
q
C
q
e
A
q
t
C
q
C
q
¼
d
ð
Þ
0
nite gramians in the frequency time of the system (
1
) are obtained by
these relationships:
The in
þ1
1
2
A
q
Þ
1
C
q
C
q
ð
A
q
Þ
1
dw
Q
q
¼
ð
iw
q
I
q
iw
q
I
q
ð
13
Þ
P
1
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