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Theory, Design and Tests on a Prototype Module of a Compact ...

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5. COUPLING BETWEEN WAVEGUIDE AND BRIDGE COUPLER 39<br />

Zo<br />

d1 d2<br />

jXi<br />

Figure 3.13. The equivalent circuit <strong>of</strong> the structure<br />

simulated with MAFIA. Two transmissi<strong>on</strong> lines <str<strong>on</strong>g>and</str<strong>on</strong>g> a<br />

purely reactance.<br />

<strong>on</strong> the waveguides lengths. These waveguide lengths are <strong>on</strong>ly a tool we<br />

use to explore the behaviour.<br />

X i [kΩ]<br />

40<br />

20<br />

0<br />

−20<br />

−40<br />

−60<br />

−80<br />

3 3.05 3.1 3.15<br />

f [GHz]<br />

Zo<br />

35x10x2mm iris<br />

Figure 3.14. An example <strong>of</strong> reactance coming from<br />

MAFIA. The iris has dimensi<strong>on</strong>s 35 × 10 × 2 mm (model<br />

made in Naples).<br />

In figure 3.14 the reactance crosses the frequency axes, i.e. has zero<br />

value, after it has a res<strong>on</strong>ant behaviour <str<strong>on</strong>g>and</str<strong>on</strong>g> asymptotically goes to zero<br />

for frequencies approaching infinity. The behaviour is always <strong>of</strong> this<br />

type, in spite <strong>of</strong> different irises <str<strong>on</strong>g>and</str<strong>on</strong>g> bridge coupler cavity dimensi<strong>on</strong>s.<br />

Such a behaviour is well fitted by the equivalent circuit shown in<br />

figure 3.15 <strong>on</strong> the left: the parallel elements give the res<strong>on</strong>ant behaviour<br />

<str<strong>on</strong>g>and</str<strong>on</strong>g> at high frequency the reactance is mainly due to the capacitance<br />

C1. The correct values for these elements can be found by a least<br />

square fitting. But, more important is the interpretati<strong>on</strong> <strong>of</strong> the lumped

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