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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