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General Inverters, Resonators, and End Couplings 293<br />

It is important to interpret the three factors in (8.30). The first two terms<br />

have been extracted in the form typical <strong>of</strong> the simple capacitive inverter<br />

described in Section 8.2.1: B(wo) is an inverter Yo and (w/wo) is the linear<br />

frequency behavior <strong>of</strong> capacitive susceptance. Therefore, (8.30) was written<br />

with W > w n<br />

in mind, when the trap appears capacitive.<br />

The analysis in Section 8.1.3 showed that the Zo <strong>of</strong> each inverter was a.<br />

factor in the coefficient <strong>of</strong> the highest-degree frequency term in the response<br />

polynomial [see (8.10)-(8.12)]. The first two terms in (8.30) produce exactly<br />

the effect <strong>of</strong> a simple capacitive inverter. The effect <strong>of</strong> the third term in (8.30)<br />

is to increase the breakpoint <strong>of</strong> the asymptote for stopband selectivity by<br />

20 log <strong>of</strong> its inverse (inverting from admittance to impedance).<br />

The numerator and denominator <strong>of</strong> the third term are both positive when<br />

W > W n<br />

and W n<br />

> Woo Thus the third term is unity when<br />

[<br />

2]-1/2<br />

w/wn = 2-(::) . (8.31 )<br />

An analysis <strong>of</strong> the third term in (8.30) in light <strong>of</strong> (8.31) reveals that the trap<br />

increases selectivity above the trap frequency, except for the case where<br />

w n<br />

/ Wo Wo and W > W n<br />

leads to the following rule: classify the<br />

trap as a simple C inverter in (8.27), and increase the loss estimate by .<br />

(wn/wo)2- 1<br />

20 log 2<br />

l-(wn/w,)<br />

(8.32)<br />

When w n / W o

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