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
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