Digital Signal Processing Reference
In-Depth Information
and the quantized filter, it allows us to make a suboptimal choice of the filter.
This is illustrated by the following example.
7.5 QUANTIZATION ANALYSIS OF IIR FILTERS
Let us select the same fifth-order IIR lowpass elliptic filter that was considered
in Example 6.17. Its transfer function
G(z)
is given by
0
.
1397
1
.
965
G(z)
=
(
1
+
1
.
337
z
−
1
+
2
.
251
z
−
2
+
2
.
251
z
−
3
+
1
.
337
z
−
4
z
−
5
)
+
×
(
1
−
1
.
629
z
−
1
+
2
.
256
z
−
2
−
1
.
597
z
−
3
+
0
.
8096
z
−
4
−
0
.
1866
z
−
5
)
(7.9)
The frequency specifications for the filter are given as
ω
p
=
0
.
4,
ω
s
=
0
.
6,
A
p
=
0
.
3dB,and
A
s
=
35 dB. The transfer function
G(z)
was decomposed as
the sum of two allpass filters
A
1
(z)
and
A
2
(z)
such that
G(z)
=
2
[
A
1
(z)
+
A
2
(z)
],
where
0
.
5089
−
0
.
6763
z
−
1
z
−
2
+
A
1
(z)
=
(7.10)
−
0
.
6763
z
−
1
+
0
.
5089
z
−
2
1
and
0
.
8805
−
0
.
5368
z
−
1
+
0
.
8805
z
−
2
−
0
.
4165
+
1
−
0
.
4165
z
−
1
z
−
2
z
−
1
+
A
2
(z)
=
(7.11)
1
−
0
.
5367
z
−
1
Recollect the following lattice coefficients used to realize the lattice structures
for
A
1
(z)
and
A
2
(z)
computed in Chapter 6:
For
A
1
(z)
:
−
0
.
4482
0
.
5089
K1
=
⎡
⎣
⎤
⎦
0
0
1
V1
=
For
A
2
(z)
:
−
0
.
2855
0
.
8805
K2
=
⎡
⎤
0
0
1
⎣
⎦
V2
=
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