Digital Signal Processing Reference
In-Depth Information
ω
|
H
(
) |
G
m
n
= 1
n
= 2
−
ω
c
ω
c
0
Fig. 1.32
The magnitude frequency response of a Butterworth LPF
1.5.2 Butterworth LPF
The magnitude frequency response of a Butterworth LPF (B-LPF) is given by:
G
m
j
H
ð
x
Þj¼
r
;
ð
1
:
45
Þ
1
þ
x
c
2n
where G
m
is the maximum gain, n is the filter order, and x
c
is the cutoff frequency
(see Fig.
1.32
). The Butterworth LPF's magnitude function is maximally flat at
x = 0, i.e., all its 2n - 1 derivatives are equal to 0 at x = 0. At x = 0 (DC), the
filter gain=G
m
, and the power gain GP
o
= |H(0)|
2
= G
2
—this is the maximum
power gain of the filter. At x = x
c
(cutoff), the filter gain
¼
G
m
=
2
p
, and the power
gain GP
c
¼j
H
ð
x
c
Þj
2
¼
G
m
=
2
¼
half the maximum power gain GP
o
. In dB terms:
GP
c
(dB)
¼
10 log
10
ð
GP
o
=
2
Þ¼
GP
o
(dB)
10 log
10
2
¼
GP
o
(dB)
3
The cutoff frequency is also called the 3-dB frequency because the power is 3 dB
down from the power at DC.
As n increases, the cutoff becomes sharper, but more circuit components are
needed to build the filter. The Butterworth LPF has a flat response at x = 0. Its
transfer function for different orders can be obtained from Tables. The nth-order
B-LPF has n poles and no zeros in its transfer function.
1.5.3 Chebychev-I LPF
Chebychev-I filters tend to have sharper roll-off than Butterworth filters but have
ripple in the passband, as illustrated in Fig.
1.33
. The magnitude frequency
response of a Chebychev-I LPF (C-LPF) is given by:
G
m
1
þ
e
2
C
n
j
H
ð
x
Þj¼
r
;
x
x
c
Search WWH ::
Custom Search