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Implementing IIR/FIR Filters

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Although this transformation was developed using a<br />

first-order system, it holds, in general, for an N th -order<br />

system (see Reference 14). By letting s = σ + jΩ and<br />

z = re jθ , it can be shown that the left-half plane in the<br />

s-domain is mapped inside the unit r = 1 circle in the<br />

z-domain under the bilinear transformation. More importantly,<br />

when r = 1 and σ = 0, the frequencies in the<br />

s-domain and the z-domain are related by:<br />

Ω<br />

or equivalently:<br />

2 θ<br />

= -tan-- T 2<br />

θ 2tan 1 – ΩT<br />

=<br />

-------<br />

2<br />

where: θ is the digital domain normalized<br />

frequency equal to 2πf/f s<br />

Eqn. 2-14<br />

Eqn. 2-15<br />

Ω is the analog domain frequency used<br />

in the analysis of the previous section<br />

On the jΩ axis or equivalently along the frequency<br />

axis, the scale has been changed nonlinearly. The<br />

gain and phase values depicted on the vertical axis<br />

of Figure 1-2, Figure 1-4, Figure 1-6, and Figure 1-8<br />

remain exactly the same in the digital domain (or zplane).<br />

The horizontal (frequency) axis is modified<br />

so that an infinite frequency in the analog domain<br />

maps to one-half of the sample frequency, f s /2, in<br />

the digital domain; whereas, for frequencies much<br />

less than f s /2, the mapping is approximately 1:1<br />

2-6 MOTOROLA

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