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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