Digital Signal Processing Reference
In-Depth Information
This leads to the assertion
¼ ln{ s ( n )} þ 1
1
s ( n )
A ( z , n )
c i ( n ) z i
ln
:
(7 : 15)
If the N pre predictor coefficients a i ( n ) [or a i ( n )] are known we can derive a simple
recursive computation of the linear predictive cepstral coefficients c i ( n ) by differentiat-
ing both sides of (7.15) with respect to z and equating the coefficients of alike
powers of z
"
(
)
#
"
#
N pre
ln 1 X
dz 1
1
d
dz
d
a i ( n ) z i
c i ( n ) z i
¼
1
(7 : 16)
"
# 1
X
N pre
1 þ X
N pre
¼ 1
1
ia i ( n ) z i 1
a i ( n ) z i
ic i ( n ) z i 1
:
1
1
Multiplying both sides of (7.16) with [ 1 þ P N pre
1 a i ( n ) z i ] leads to
X
N pre
¼ 1
1
1
1
X
N pre
ia i ( n ) z i 1
ic i ( n ) z i 1
kc k ( n ) a i ( n ) z ki 1
:
(7 : 17)
1
1
If we now consider the equation above for equal powers of z , we find that starting from
the left, the first two terms only contribute a single term each up to z N pre 1 . We will
label the order with i . The last term in contrast produces an amount of terms that
depends on i . Setting all terms that belong to the same power of z equal results in
ia i ( n ) ¼ ic i ( n ) X
i 1
kc k ( n ) a ik ( n ),
for i [ {1, ... , N pre } :
(7 : 18)
1
Solving this equation for c i ( n ) results in
i X
i 1
1
c i ( n ) ¼ a i ( n ) þ
kc k ( n ) a ik ( n ),
for i [ {1, ... , N pre } :
(7 : 19)
1
For i . N pre the first term on the right side still needs to be considered in (7.17)
whereas the term on the left side does not contribute any more to powers of z larger
than N pre 1 and can therefore be omitted. Therefore, we can solve (7.17)
 
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