Digital Signal Processing Reference
In-Depth Information
The second moment is equal to:
1
x 2 l e lx d x ¼ l 3 Þ
l 3
2
2
l 2 :
!
l 2 ¼
m 2 ¼
¼
(2.378)
0
From ( 2.377 ) and ( 2.378 ), using ( 2.337 ), the variance is:
2
l 2
1
l 2 ¼
1
l 2 :
s 2
¼ m 2 m 1 ¼
(2.379)
The third central moment is:
1
3
l e lx d x:
m 3 ¼
ðx 1 =lÞ
(2.380)
0
After brief calculations, we arrive at:
=l 3
m 3 ¼ 2
:
(2.381)
The nonzero third central moment is the result of asymmetry in the PDF.
Similarly, we get the fourth central moment:
1
4
=l 4
l e lx d x ¼ 9
m 4 ¼
ðx 1
=lÞ
:
(2.382)
0
From ( 2.372 ) and ( 2.379 )-( 2.381 ), the coefficient of skewness is given by:
3
m 3
s 3 ¼
EfðX mÞ
g
c s ¼
¼ 2
:
(2.383)
s 3
The positive value ( 2.383 ) shows that the density function is skewed to the right,
as it is shown in Fig. 2.51 .
Similarly, from ( 2.373 ), ( 2.379 ), and ( 2.382 ), the coefficients of kurtosis is
given as:
4
m 4
s 4 ¼
EfðX mÞ
g
c k ¼
¼ 9
:
(2.384)
s 4
The large coefficient of Kurtosis indicates that the density has a sharp peak near
its mean. This is confirmed in Fig. 2.51 .
Higher values of the moments do not have a similar physical interpretation, as do
the first four moments.
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