Digital Signal Processing Reference
In-Depth Information
From ( 3.22 ), we get:
f X 1 X 2 ðx 1 ; x 2 Þ¼ 1
=
2 dðx 1 1 Þdðx 2 1 Þþ 1
=
4 dðx 1 1 Þdðx 2 Þþ 1
=
4 dðx 1 Þdðx 2 1 Þ:
(3.31)
Next, in Fig. 3.7 we compare one-dimensional and two-dimensional PDFs.
The shaded area in Fig. 3.7a represents the probability that the random variable
X is in the infinitesimal interval [ x , x +d x ]:
A ¼ Px< X x þ d x
f
g:
(3.32)
From here, considering that d x is an infinitesimal interval, the PDF in the interval
[ x , x +d x ] is constant, resulting in:
f X ðxÞ d x ¼ A ¼ Px< X x þ d x
f
g:
(3.33)
Similarly, the volume in Fig. 3.7b presents the probability that the random
variables
X 1 and
X 2 are in the intervals [ x 1 ,
x 1 +d x 1 ] and [ x 2 ,
x 2 +d x 2 ],
respectively.
The equivalent probability
Px 1 < X 1 x 1 þ d x 1 ; x 2 < X 2 x 2 þ d x 2
f
g
(3.34)
corresponds to the elemental volume V , with a base of (d x 1 d x 2 ) and height of
f X 1 X 2 ðx 1 ; x 2 Þ :
f X 1 X 2 ðx 1 ; x 2 Þ d x 1 d x 2 ¼ V ¼ Px 1 < X 1 x 1 þ d x 1 ; x 2 < X 2 x 2 þ d x 2
f
g:
(3.35)
Fig. 3.7 One-dimensional and two-dimensional PDFs
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