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442 Chapter 8 IIR FILTER DESIGN<br />

1<br />

0.8913<br />

Magnitude Response<br />

1<br />

Phase Response<br />

|H|<br />

π units<br />

0<br />

0.1778<br />

decibels<br />

0<br />

0 0.2 0.3 1<br />

frequency in π units<br />

0<br />

1<br />

15<br />

Magnitude in dB<br />

Samples<br />

−1<br />

0 0.2 0.3 1<br />

frequency in π units<br />

15<br />

10<br />

5<br />

Group Delay<br />

0 0.2 0.3 1<br />

frequency in π units<br />

0<br />

0 0.2 0.3 1<br />

frequency in π units<br />

FIGURE 8.29<br />

Digital elliptic lowpass filter using bilinear transformation<br />

The advantages of this mapping are that (a) it is a stable design,<br />

(b) there is no aliasing, and (c) there is no restriction on the type of filter<br />

that can be transformed. Therefore this method is used exclusively in<br />

computer programs including MATLAB, as we shall see next.<br />

8.4.5 MATCHED-z TRANSFORMATION<br />

In this method of filter transformation, zeros and poles of H a (s) are directly<br />

mapped into zeros and poles in the z-plane using an exponential<br />

function. Given a root (zero or pole) at the location s = a in the s-plane,<br />

we map it in the z-plane at z = e aT where T is a sampling interval. Thus,<br />

the system function H a (s) with zeros {z k } and poles {p l } is mapped into<br />

the digital filter system function H(z) as<br />

∏ M<br />

k=1<br />

H a (s) =<br />

(s − z ∏ M<br />

(<br />

k)<br />

k=1 1 − e<br />

z k T z −1)<br />

∏ N<br />

l=1 (s − p → H(z) = ∏ N<br />

l)<br />

l=1 (s − (8.69)<br />

ep lT<br />

z −1 )<br />

Clearly the z-transform system function is “matched” to the s-domain<br />

system function.<br />

Note that this technique appears to be similar to the impulse invariance<br />

mapping in that the pole locations are identical and aliasing is unavoidable.<br />

However, these two techniques differ in zero locations. Also the<br />

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