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410 Chapter 8 IIR FILTER DESIGN<br />

Magnitude Response<br />

Magnitude in dB<br />

|H|<br />

1<br />

0.4467<br />

decibels<br />

0<br />

7<br />

16<br />

0.1585<br />

0<br />

0 0.2 0.3 0.5<br />

Analog frequency in π units<br />

30<br />

0 0.2 0.3 0.5<br />

Analog frequency in π units<br />

1<br />

Phase Response<br />

0.2<br />

Impulse Response<br />

0.5<br />

0.15<br />

radians<br />

0<br />

−0.5<br />

ha(t)<br />

0.1<br />

0.05<br />

−1<br />

0 0.2 0.3 0.5<br />

Analog frequency in π units<br />

0<br />

0 10 20 30<br />

time in seconds<br />

FIGURE 8.15 Butterworth analog filter in Example 8.4<br />

8.3.5 CHEBYSHEV LOWPASS FILTERS<br />

There are two types of Chebyshev filters. The Chebyshev-I filters have<br />

equiripple response in the passband, while the Chebyshev-II filters have<br />

equiripple response in the stopband. Butterworth filters have monotonic<br />

response in both bands. Recall our discussions regarding equiripple FIR<br />

filters. We noted that by choosing a filter that has an equiripple rather<br />

than a monotonic behavior, we can obtain a lower-order filter. Therefore<br />

Chebyshev filters provide lower order than Butterworth filters for the<br />

same specifications.<br />

The magnitude-squared response of a Chebyshev-I filter is<br />

|H a (jΩ)| 2 =<br />

1<br />

( ) (8.52)<br />

Ω<br />

Ω c<br />

1+ɛ 2 T 2 N<br />

where N is the order of the filter, ɛ is the passband ripple factor, which is<br />

related to R p , and T N (x)istheNth-order Chebyshev polynomial given by<br />

{ (<br />

cos N cos −1 (x) ) , 0 ≤ x ≤ 1<br />

T N (x) =<br />

cosh ( cosh −1 (x) ) , 1

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