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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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