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394 Chapter 8 IIR FILTER DESIGN<br />

Imaginary Part<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

–0.2<br />

–0.4<br />

–0.6<br />

–0.8<br />

–1<br />

Pole–zero Plot<br />

2<br />

–1 –0.5 0 0.5 1<br />

Real Part<br />

FIGURE 8.5<br />

Decibel<br />

Radians / π<br />

10<br />

0<br />

Magnitude Response<br />

–50<br />

–1 0 1<br />

1<br />

0.5<br />

0<br />

–0.5<br />

Phase Response<br />

–1<br />

–1 0 1<br />

ω in π units<br />

Frequency response of a typical notch filter<br />

around the desired null are severely attenuated. To reduce the bandwidth<br />

of the null, we may resort to the more sophisticated, longer FIR<br />

filter designed according to the optimum equiripple design method described<br />

in Chapter 7. Alternatively, we could attempt to improve the frequency<br />

response of the filter by introducing poles in the system function.<br />

Imaginary Part<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

–0.2<br />

–0.4<br />

–0.6<br />

–0.8<br />

–1<br />

Pole–zero Plot<br />

2<br />

–1 –0.5 0 0.5 1<br />

Real Part<br />

Decibel<br />

Radians / π<br />

10<br />

0<br />

Magnitude Response<br />

–50<br />

–1 –1/4 0 1/4 1<br />

1<br />

0.5<br />

0<br />

–0.5<br />

Phase Response<br />

–1<br />

–1 –1/4 0 1/4 1<br />

ω in π units<br />

FIGURE 8.6 Frequency response of a notch filter with ω 0 = π/4<br />

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