Digital Signal Processing Reference
In-Depth Information
Solution Parameters of the equations result from the sampling frequency and are
equal:
N
1
¼
f
S
=
f
1
¼
1000
=
50
¼
20
;
X
1
¼
2p
=
N
1
¼
2p
=
20
¼
p
=
10
;
cos
ð
X
1
Þ¼
cos
ð
p
=
10
Þ¼
0
:
951
;
sin
ð
X
1
Þ¼
sin
ð
p
=
10
Þ¼
0
:
309
:
Substituting the values to the general equations one obtains specific algorithms
for magnitude measurement, and for:
• orthogonalization by single delay, k
¼
1(
8.73
)
x
1
ð
n
Þþ
x
1
ð
n
k
Þ
cos
ð
kX
1
Þ
x
1
ð
n
Þ
s
2
X
1m
¼
sin
ð
kX
1
Þ
s
x
1
ð
n
Þþ
x
1
ð
n
1
Þ
0
:
951x
1
ð
n
Þ
2
¼
;
0
:
309
• orthogonalization by double delay, k = 1(
6.41
)
s
x
1
ð
n
k
Þþ
x
1
ð
n
2k
Þ
x
1
ð
n
Þ
2
X
1m
¼
2 sin
ð
kX
1
Þ
s
x
1
ð
n
1
Þþ
x
1
ð
n
2
Þ
x
1
ð
n
Þ
0
:
618
2
¼
;
• orthogonalization by single delay, k
¼
N
1
=
4
;
q
x
1
ð
n
Þþ
x
1
ð
n
N
1
=
4
Þ
q
x
1
ð
n
Þþ
x
1
ð
n
5
Þ
X
1m
¼
¼
:
Example 8.7 Provide full-cycle magnitude measurement algorithms with appli-
cation of Walsh filters of I and II order. Assume sampling rate f
S
= 1000 Hz.
Solution For the sampling frequency f
S
= 1000 Hz the number of samples per
cycle is N
1
¼
20
:
Thus the output signals y
ð
n
Þ
of respective Walsh filters are
produced according to the following equations processing input values x
ð
n
Þ;
(
6.22
),
(
6.25
):
y
1C
ð
n
Þ¼
X
x
ð
n
k
Þþ
X
x
ð
n
k
Þ
X
4
14
19
x
ð
n
k
Þ;
k
¼
0
k
¼
5
15
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