Digital Signal Processing Reference
In-Depth Information
Denoting a power, which belongs to a infinitesimal frequency band d
f
,as
S
(
f
)d
f
,
we get:
ð
f
k
P
k
¼
Sð f Þ
d
f ;
(7.45)
0
or generally
ð
f
Pð f Þ¼
Sð f Þ
d
f :
(7.46)
0
From here, we have:
d
P
ð
f
Þ
d
f
Sð f Þ¼
:
(7.47)
The obtained result, shown in Fig.
7.5a
, is the spectral density of a random
signal, and is, naturally, defined only for the positive frequencies. However, the
negative frequencies are introduced in a frequency analysis for mathematical
reasons in order to present the Fourier series in exponential form.
Therefore, in order to obtain the mathematical spectral density, all values of
S
(
f
)
are halved, and the top part of the plot is mapped to the left part, resulting in the
diagram shown in Fig.
7.5b
.
Therefore,
f
k
ð
f
k
ð
P
k
¼
Sðf Þ
d
f ¼
S
xx
ðf Þ
d
f :
(7.48)
0
f
k
Fig. 7.5
Physical (
a
) and mathematical spectral density (
b
)
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