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336 Other Direct Filter <strong>Design</strong> Methods<br />

load effects on mapping and input standing-wave ratio. A theorem concerning<br />

composite bilinear functions between different unit circles is provided as a<br />

fundamental analysis tool for obtaining concise design results.<br />

The load effect analysis is extended to derive a design basis for filters that<br />

absorb rather than reflect energy. These may be viewed as frequency-selective<br />

attenuators (pads). They are substantially less selective than reflection filters,<br />

but there are many important applications for impedance control and damping<br />

<strong>of</strong> spurious oscillations in system stopbands. <strong>Design</strong> graphs for several <strong>of</strong><br />

these invulnerable (load-independent) filters will be provided.<br />

9.1. Equal-Stub Admittance Filters<br />

The direct-coupled filter design method in Chapter Eight provided a means<br />

for designing transmission line filters, as shown in Figure 9.1. For I-ohm<br />

terminations, the shorted-circuited, quarter-wave transmission line resonators<br />

have loaded Q values<br />

QLK =Y OK*' (9.1)<br />

according to (8.50). Note that the internal resonators in Figure 9.1 c have been<br />

divided into two parallelled resonators so that each may have half the required<br />

Yo (and to minimize the generation or' extraneous electromagnetic modes).<br />

Even so, the Q is too low and the bandwidth too wide for direct-coupled-filter<br />

predictions to apply (see Section 8.5.2), since the transmission line normalized<br />

admittance is within the range 0.1

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