Digital Signal Processing Reference
In-Depth Information
Comparing ( 5.23 ) and ( 5.1 ), it follows that the random variable X from ( 5.23 )is
a lognormal variable which itself represents the product of a number of independent
variables, as can be seen in ( 5.19 ).
As a result, as the sum of a large number of independent random variables
approaches a normal random variable (central limit theorem) the product of a large
number of independent random variables gives rise to a lognormal variable .
The lognormal PDF can be used to describe the life distribution of many
semiconductor components, the failure of which is a result of cracks caused by
material fatigue [KLA89, p. 51].
5.2 Rayleigh Random Variable
5.2.1 Density Function
The Rayleigh density function is defined as:
f X ðxÞ¼kx k x 2
;
for
x 0
2
(5.24)
f X ðxÞ¼ 0
;
for
x <
0
where k is a positive constant.
The density function is also expressed using the parameter s 2 , which is related
with the constant k as follows:
s 2
¼ 1 =k;
(5.25)
resulting in:
1
s 2 x x 2
f X ðxÞ¼
;
for
x 0
2 s 2
(5.26)
f X ðxÞ¼ 0
;
for
x <
0
The Rayleigh random variable and the corresponding density for the parameter
s 2
¼ 4 are shown in Fig. 5.3 .
The Rayleigh density is useful in describing the envelope of a narrowband normal
noise. It is also important in the analysis of measurement errors [PEE93, p. 56].
Note that the random variable has only positive values and that the PDF is
asymmetrical and has a maximum value for
p
k
x ¼ s ¼ 1
=
:
(5.27)
r
k
e
¼ f X ðsÞ¼
1
1
s p ¼
f X
p
k
:
(5.28)
Search WWH ::




Custom Search