Digital Signal Processing Reference
In-Depth Information
Table 7.2. Denominator
D
(
s
) for transfer function
H
(
s
) of the Butterworth filter
N
D
(
s
)
(
s
+
1)
(
s
2
+
1
.
414
s
+
1)
(
s
+
1)(
s
2
+
s
+
1)
(
s
2
+
0
.
7654
s
+
1)(
s
2
+
1
.
8478
s
+
1)
(
s
+
1)(
s
2
+
0
.
6810
s
+
1)(
s
2
+
1
.
6810
s
+
1)
(
s
2
+
0
.
5176
s
+
1)(
s
2
+
1
.
4142
s
+
1)(
s
2
+
1
.
9319
s
+
1)
(
s
+
1)(
s
2
+
0
.
4450
s
+
1)(
s
2
+
1
.
2470
s
+
1)(
s
2
+
1
.
8019
s
+
1)
(
s
2
+
0
.
3902
s
+
1)(
s
2
+
1
.
1111
s
+
1)(
s
2
+
1
.
6629
s
+
1)(
s
2
+
1
.
9616
s
+
1)
(
s
+
1)(
s
2
+
0
.
3473
s
+
1)(
s
2
+
s
+
1)(
s
2
+
1
.
5321
s
+
1)(
s
2
+
1
.
8794
s
+
1)
10
(
s
2
+
0
.
3129
s
+
1)(
s
2
+
0
.
9080
s
+
1)(
s
2
+
1
.
4142
s
+
1)(
s
2
+
1
.
7820
s
+
1)(
s
2
+
1
.
9754
s
+
1)
Butterworth filter are all real-valued. In general, Eq. (7.21) can be simplified as
follows:
1
D
(
s
)
1
H
(
s
)
=
=
(7.22)
s
N
+
a
N
−
1
s
N
−
1
++
a
1
s
+
1
and represents the transfer function of the normalized Butterworth filter of
order
N
.
Repeating Example 7.4 for different orders (1
≤
N
≤
10), the transfer func-
tions
H
(
s
) of the resulting normalized Butterworth filters can be similarly com-
puted. Since the numerator of the transfer function is always unity, Table 7.2
lists the polynomials for the denominator
D
(
s
) for 1
≤
N
≤
10.
7.3.1.1
Design steps for the lowpass Butterworth filter
In this section, we will design a Butterworth lowpass filter based on the spec-
ifications illustrated in Fig. 7.3(a). Mathematically, the specifications can be
expressed as follows:
pass band (0
≤ω≤ω
p
radians/s)
1
− δ
p
≤
H
(
ω
)
≤
1
+ δ
p
;
(7.23)
stop band (
ω >ω
s
radians/s)
H
(
ω
)
≤δ
s
.
(7.24)
At times, Eq. (7.23) is also expressed in terms of the pass-band ripple as
20 log
10
δ
p
dB. Similarly, Eq. (7.24) is expressed in terms of the stop-band
ripple as 20 log
10
δ
s
dB. The design of the Butterworth filter consists of the
following steps, which we refer to as Algorithm 7.3.1.1.
Step 1
Determine the order
N
of the Butterworth filter. To determine the order
N
of the filter, we calculate the gain of the filter at the corner frequencies
ω = ω
p
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