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A Complete <strong>Design</strong> Example 327<br />

using a high-impedance vector voltmeter:<br />

l. Adjacent node voltages should differ in phase by ± 90 degrees.<br />

2. Node voltage magnitudes are easily related to the node's parallel<br />

resistance, based on power.<br />

3. The L-section end-coupling phase should agree with (6.7) or (6.8), as<br />

appropriate.<br />

The swept-frequency display <strong>of</strong> input node voltage V, during the node-tuning<br />

sequence should appear as in Figure 8.29. Waveguide and other distributed<br />

filters are tuned according to the same principles, namely ideal resonator and<br />

inverter behavior. However, slotted lines and lightly coupled probes are <strong>of</strong>ten<br />

required. This is discussed by Matthaei et al. (1964, p. 668).<br />

Dishal (1951) gives relationships that enable the calculation <strong>of</strong> coupling<br />

coefficients as in (8.26), based on the frequencies <strong>of</strong> the response peaks in<br />

Figure 8.29. These are <strong>of</strong>ten useful for evaluating aperture and other inaccessible<br />

coupling implementations.<br />

8.5.6. Summary <strong>of</strong>Comments on a <strong>Design</strong> Procedure. A step-by-step design<br />

procedure for narrow-band, direct-coupled filters has been discussed in terms<br />

<strong>of</strong> the flowchart in Figure 8.28. The next section will proceed through almost<br />

all <strong>of</strong> these steps to illustrate the procedure in terms <strong>of</strong> the tabulated equations<br />

in Appendix G.<br />

<strong>Design</strong> step 13 is the observation <strong>of</strong> filter behavior in the laboratory. The<br />

intent <strong>of</strong> the design procedure is to produce a first-time design success. The<br />

physical properties <strong>of</strong> many sophisticated filters, especially microwave filters,<br />

make final tweaking in the laboratory very difficult and expensive. Besides the<br />

analysis to determine proper coupling coefficients just suggested, an optimizer<br />

used in conjunction with a network analysis program <strong>of</strong>ten can confirm the<br />

presence and values <strong>of</strong> parasitic elements not previously considered. Such<br />

optimization can then be used to predict new filter component values that<br />

may <strong>of</strong>fset the undesirable effects <strong>of</strong> the unexpected parasitic elements.<br />

Finally, the great virtue <strong>of</strong> the loaded-Q filter design method should now be<br />

apparent: it is a flexible procedure that accommodates component limitations<br />

in nearly every stage <strong>of</strong> the design.<br />

8.6. A Complete <strong>Design</strong> Example<br />

The design steps in Figure 8.28 will be calculated for the network in Figure 8.2<br />

using an undercoupled response shape with selectivity, as in Figure 8.3. The<br />

step numbers appear after the last decimal in the following paragraph numbers.<br />

The equation numbers correspond to those in Appendix G.

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