Digital Signal Processing Reference
In-Depth Information
where
d
CC
ð
n
Þ¼
X
n
a
c
ð
k
Þ
b
c
ð
k
Þ;
k
¼
0
d
CS
ð
n
Þ¼
X
n
a
c
ð
k
Þ
b
s
ð
k
Þ;
k
¼
0
d
SC
ð
n
Þ¼
X
n
a
s
ð
k
Þ
b
c
ð
k
Þ;
k
¼
0
d
SS
ð
n
Þ¼
X
n
a
s
ð
k
Þ
b
s
ð
k
Þ:
k
¼
0
For given orthogonal filters, i.e., for their impulse responses being known, it is
possible to calculate the above coefficients as a function of actual window length n.
If for instance full-cycle sine, cosine orthogonal filters are used, their impulse
responses are given by:
a
c
ð
k
Þ¼
cos
½ð
k
þ
0
:
5
Þ
X
1
¼
b
c
ð
k
Þ;
ð
9
:
8a
Þ
a
s
ð
k
Þ¼
sin
½ð
k
þ
0
:
5
Þ
X
1
¼
b
s
ð
k
Þ;
ð
9
:
8b
Þ
the coefficients of equations (
9.7a
,
b
) are following:
d
CC
ð
n
Þ¼
X
n
cos
2
½ð
k
þ
0
:
5
Þ
X
1
¼
n
þ
1
2
þ
sin
ð
nX
1
Þ
2 sin
ð
X
1
Þ
cos
ð
nX
1
Þ;
ð
9
:
9a
Þ
k
¼
0
d
SS
ð
n
Þ¼
X
n
sin
2
½ð
k
þ
0
:
5
Þ
X
1
¼
n
þ
1
2
sin
ð
nX
1
Þ
2 sin
ð
X
1
Þ
cos
ð
nX
1
Þ;
ð
9
:
9b
Þ
k
¼
0
d
CS
ð
n
Þ¼
d
SC
ð
n
Þ¼
X
n
cos
½ð
k
þ
0
:
5
Þ
X
1
sin
½ð
k
þ
0
:
5
Þ
X
1
¼
sin
ð
nX
1
Þ
2 sin
ð
X
1
Þ
sin
ð
nX
1
Þ:
ð
9
:
9c
Þ
k
¼
0
Substituting the above coefficients into output signals of orthogonal filters (
9.7a
,
b
)
and applying them in standard algorithm of magnitude measurement (sum of squared
orthogonal components) after simple rearrangements one obtains:
(
n
þ
1
2
sin
ð
nX
1
Þ
sin
ð
X
1
Þ
!
2
2
4
N
1
X
1m
ð
n
Þ¼
X
1m
þ
2 sin
ð
X
1
Þ
cos
½ð
n
þ
1
Þ
X
1
þ
2u
1
)
þð
n
þ
1
Þ
sin
ð
nX
1
Þ
:
ð
9
:
10
Þ
According to expectations the measured magnitude depends on initial phase
shift of the signal. Transients and steady state of magnitude measurement is shown
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