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

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7. MEASUREMENT OF THE WAVEGUIDE-MODULE COUPLING 93<br />

Figure 5.24. Coupling through an iris. Sketch <strong>of</strong> a<br />

res<strong>on</strong>ant cavity coupled with a transmissi<strong>on</strong> line.<br />

Figure 5.25. Coupling through an iris. The generator<br />

is referred to the sec<strong>on</strong>dary.<br />

These set <strong>of</strong> parameters are involved in a equivalent circuit that represent<br />

the cavity in <strong>on</strong>e mode <str<strong>on</strong>g>and</str<strong>on</strong>g> can be used in most applicati<strong>on</strong>s.<br />

7.2. Equivalent circuits, definiti<strong>on</strong>s <strong>of</strong> Q0, QL, Qext <str<strong>on</strong>g>and</str<strong>on</strong>g> coupling<br />

coefficient β. C<strong>on</strong>sider a signal generator c<strong>on</strong>nected to a transmissi<strong>on</strong><br />

line, those characteristic impedance Z0 is equal to the internal<br />

impedance <strong>of</strong> the generator. The transmissi<strong>on</strong> line is coupled to a res<strong>on</strong>ant<br />

cavity through a magnetic coupling mechanism. The res<strong>on</strong>ant<br />

cavity is represented by a lumped circuit as it is shown in figure 5.24.<br />

The magnetic coupling mechanism is represented as a transformer,<br />

where L1 is the auto-inductance <str<strong>on</strong>g>and</str<strong>on</strong>g> M is the mutual-inductance <strong>of</strong><br />

the transformer. The coupling mechanism is supposed to be without<br />

loss.<br />

We can either refer the cavity impedance to the primary or to refer<br />

the generator to the sec<strong>on</strong>dary. The latter case leads to the definiti<strong>on</strong><br />

<strong>of</strong> matched generator, whose internal impedance is<br />

<str<strong>on</strong>g>and</str<strong>on</strong>g> this leads to the circuit <strong>of</strong> figure 5.25.<br />

Z = (ωM)2<br />

, (5.16)<br />

jωL1 + Z0

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