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398 Chapter 8 IIR FILTER DESIGN<br />

Unit circle<br />

(a)<br />

(b)<br />

FIGURE 8.9<br />

Pole-zero locations for (a) one-pole and (b) two-pole allpass filter<br />

The general form for the system function of an allpass filter with real<br />

coefficients may be expressed in factored form as<br />

H(z) =<br />

∏N R<br />

k=1<br />

z −1 − α k<br />

∏N C<br />

1 − α k z −1<br />

k=1<br />

(z −1 − β k )(z −1 − β ∗ k )<br />

(1 − β k z −1 )(1 − β ∗ k z−1 )<br />

(8.33)<br />

where N R is the number of real poles and zeros and N C is the number<br />

of complex-conjugate pairs of poles and zeros. For a causal and stable<br />

system, we require that |α k | < 1 and |β k | < 1.<br />

Allpass filters are usually employed as phase equalizers. When placed<br />

in cascade with a system that has an undesirable phase response, a phase<br />

equalizer is designed to compensate for the poor phase characteristics of<br />

the system and thus result in an overall linear phase system.<br />

8.2.5 DIGITAL SINUSOIDAL OSCILLATORS<br />

A digital sinusoidal oscillator can be viewed as a limiting form of a 2-pole<br />

resonator for which the complex-conjugate poles are located on the unit<br />

10<br />

Magnitude Response<br />

1<br />

Phase Response<br />

Decibel<br />

0<br />

Radians / π<br />

0.5<br />

0<br />

– 0.5<br />

–40<br />

–1 0 1<br />

ω in π units<br />

–1<br />

–1 0 1<br />

ω in π units<br />

FIGURE 8.10 Magnitude and phase responses for 1-pole (solid line) and 2-pole<br />

(dotted line) allpass filters<br />

Copyright 2010 Cengage Learning. All Rights Reserved. May not be copied, scanned, or duplicated, in whole or in part. Due to electronic rights, some third party content may be suppressed from the eBook and/or eChapter(s).<br />

Editorial review has deemed that any suppressed content does not materially affect the overall learning experience. Cengage Learning reserves the right to remove additional content at any time if subsequent rights restrictions require it.

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