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

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3. RF MEASUREMENT ON COUPLED CAVITIES 75<br />

Δ f [MHz]<br />

0<br />

−2<br />

−4<br />

−6<br />

−8<br />

−10<br />

−12<br />

0 2 4 6 8 10<br />

[half turns]<br />

Figure 5.5. The change in frequency due to a metallic<br />

plunger for the measurement <strong>of</strong> r over Q.<br />

the calculati<strong>on</strong> it is <strong>on</strong>ly necessary to use known relative steps advancement<br />

for the plunger, rather than exact measurement <strong>of</strong> how much the<br />

plunger penetrates into the cavity.<br />

C<strong>on</strong>sider, for example, the figure 5.5. It shows the typical change<br />

in frequency due to a 2.3 mm diameter cylindrical plunger which penetrates,<br />

through a c<strong>on</strong>ductor plane, an half pill-box like cavity with a<br />

res<strong>on</strong>ant frequency <strong>of</strong> 3.0359 GHz. The plunger is moved through a<br />

series <strong>of</strong> positi<strong>on</strong>s at which the changes <strong>of</strong> res<strong>on</strong>ant frequency are measured.<br />

The slope is determined from a numerical interpolati<strong>on</strong> <strong>of</strong> the<br />

curve.<br />

3. RF Measurement <strong>on</strong> coupled cavities<br />

From the electromagnetic theory it is known that two or more res<strong>on</strong>ators<br />

coupled together lose their single res<strong>on</strong>ant frequencies <str<strong>on</strong>g>and</str<strong>on</strong>g> meet<br />

in a number <strong>of</strong> modes equal to the number <strong>of</strong> res<strong>on</strong>ators [17]; those frequencies<br />

mainly depend from the single res<strong>on</strong>ant frequencies <str<strong>on</strong>g>and</str<strong>on</strong>g> from<br />

the coupling between the res<strong>on</strong>ators. In few words, the res<strong>on</strong>ant modes<br />

<strong>of</strong> the coupled cavities corresp<strong>on</strong>d to all the possible ways to satisfy<br />

the new boundary c<strong>on</strong>diti<strong>on</strong>.<br />

From the single cavity point <strong>of</strong> view, also the own res<strong>on</strong>ant frequency<br />

is modified from the coupling mechanism. For example, an<br />

aperture between two cavities in a z<strong>on</strong>e where the magnetic field is<br />

str<strong>on</strong>g changes the stored magnetic energy <strong>of</strong> the cavities <str<strong>on</strong>g>and</str<strong>on</strong>g>, as a<br />

c<strong>on</strong>sequence, the single res<strong>on</strong>ant frequencies.

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