Implementing IIR/FIR Filters
Implementing IIR/FIR Filters
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