Digital Signal Processing Reference
In-Depth Information
in Step 2, and the cut-off frequency
ω
c
, using the following transformation:
H
(
s
)
=
H
(
S
)
S
=
s
/ω
c
.
Note that the transformation
S
=
s
/
ω
c
represents scaling in the Laplace domain.
It is therefore clear that the normalized cut-off frequency of 1 radian/s used in
the normalized Butterworth filter is transformed to a value of
ω
c
as required in
Step 3.
Step 5
Sketch the magnitude spectrum from the transfer function
H
(
s
) deter-
mined in Step 4. Confirm that the transfer function satisfies the initial design
specifications.
Examples 7.5 and 7.6 illustrate the application of the design algorithm.
Example 7.5
Design a Butterworth lowpass filter with the following specifications:
pass band (0
≤ω≤
5 radians/s)
0
.
8
≤
H
(
ω
)
≤
1;
stop band (
ω >
20 radians/s)
H
(
ω
)
≤
0
.
20
.
Solution
Using Step 1 of Algorithm 7.3.1.1, the gain terms
G
p
and
G
s
are given by
1
(1
− δ
p
)
2
1
0
.
8
2
=
−
1
=
−
1
=
0
.
5625
G
p
and
1
(
δ
s
)
2
1
0
.
2
2
G
s
=
−
1
=
−
1
=
24
.
Using Eq. (7.29), the order of the Butterworth filter is given by
=
1
2
ln(
G
p
/
G
s
)
ln(
ω
p
/ω
s
)
=
1
2
ln(0
.
5625
/
24)
ln(5
/
20)
N
=
1
.
3538
.
We round off the order of the filter to the higher integer value as
N
=
2.
Using Step 2 of Algorithm 7.3.1.1, the transfer function
H
(
S
) of the normal-
ized Butterworth filter with a cut-off frequency of 1 radian/s is given by
H
(
S
)
=
1
S
2
+
1
.
414
S
+
1
.
Using the pass-band constraint, Eq. (7.31), in Step 3 of Algorithm 7.3.1.1, the
cut-off frequency of the required Butterworth filter is given by
ω
p
(
G
p
)
1
/
2
N
5
(0
.
5625)
1
/
4
ω
c
=
=
=
5
.
7735 radians/s
.
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