Theory, Design and Tests on a Prototype Module of a Compact ...
Theory, Design and Tests on a Prototype Module of a Compact ...
Theory, Design and Tests on a Prototype Module of a Compact ...
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88 5. RADIOFREQUENCY MEASUREMENT<br />
Figure 5.17. The bead pulling result after the first operati<strong>on</strong><br />
<strong>on</strong> all the CCs.<br />
Figure 5.18. The bead pulling result for the tuners positi<strong>on</strong>s<br />
<strong>of</strong> table 5.2.<br />
to keep the bump stop-b<str<strong>on</strong>g>and</str<strong>on</strong>g> always to relatively big values, keeping<br />
in mind that at the end <strong>of</strong> the tuning procedure it should has been<br />
possible to decrease the stop-b<str<strong>on</strong>g>and</str<strong>on</strong>g>s using the CCs tuning.<br />
The figure 5.17 shows the bead pulling measurement after that the<br />
CCs enter inside <strong>of</strong> +0.3 mm <strong>on</strong> the left side. The π/2 frequency<br />
was unchanged <str<strong>on</strong>g>and</str<strong>on</strong>g> the bump stop-b<str<strong>on</strong>g>and</str<strong>on</strong>g> increased to +270 kHz. It is<br />
clear that the interventi<strong>on</strong> made worse the field level. This happened<br />
because the stop-b<str<strong>on</strong>g>and</str<strong>on</strong>g> was bigger than in the previous situati<strong>on</strong>. In<br />
fact, the entity <strong>of</strong> the bump <str<strong>on</strong>g>and</str<strong>on</strong>g> tilt effects are directly related to the<br />
entity <strong>of</strong> the respectively stop-b<str<strong>on</strong>g>and</str<strong>on</strong>g>s. The bigger is the stop-b<str<strong>on</strong>g>and</str<strong>on</strong>g>, the<br />
bigger is the effect <strong>of</strong> the nearest modes <strong>on</strong> the field level <strong>of</strong> π/2 mode.