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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