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304 P a r t I V : D i r e c t i o n a l H i g h - F r e q u e n c y A n t e n n a A r r a y s<br />

The first-time constructor of a gamma-matched driven element would be wise to<br />

make the gamma rod itself substantially longer than L/10, since these dimensions are<br />

only approximate, and both the position of the shorting bar and the setting of the capacitor<br />

will need to be varied by trial and error during the tune-up procedure described<br />

subsequently.<br />

The capacitor in series with the center conductor of the coaxial cable has a value of<br />

approximately 8 pF per meter of wavelength at the lowest frequency in the band of interest<br />

or approximately<br />

2400<br />

C (pF) =<br />

F (MHz)<br />

(12.2)<br />

For any transmitter power levels more than a few watts, the capacitor must be a<br />

high-voltage transmitting variable type. In general, gamma match capacitors are either<br />

air or vacuum variables although those found on the older Cushcraft family of four-element<br />

monobanders for 20, 15, and 10 m consist of a fixed length of RG-8 coaxial cable<br />

with the outer jacket and shield braid removed so that just the center conductor and<br />

dielectric remain. This insulated wire is inserted into a portion of the hollow aluminum<br />

gamma rod, where the center conductor of the stripped coaxial cable forms one plate of<br />

the capacitor and the hollow gamma tube is the other.<br />

Adjustment of the gamma match is accomplished in two steps:<br />

• Adjust the length of the driven element (or dipole) for resonance, using a noise<br />

bridge, wattmeter, dip meter, impedance bridge, or other means.<br />

• Alternately adjust the capacitor and the shorting bar/clamp for best impedance<br />

match between the antenna and the transmission line. Results of this tuning<br />

operation are best monitored at the antenna with a small portable analyzer (see<br />

Chap. 27) capable of measuring and displaying SWR or impedance curves over<br />

the frequency range of interest. The author uses a battery-powered AEA HF<br />

Analyst hauled to the top of his tower in a water bucket or hanging from his<br />

belt, but AEA and others have newer analyzers that are more compact and/or<br />

have more “bells and whistles” on them.<br />

If a good match (as indicated by very low SWR) cannot be obtained with the initial<br />

spacing of the gamma rod from the element, write down the best SWR obtained at the<br />

design frequency and then increase the distance of the gamma rod from the element<br />

and go through the adjustment process again. If the SWR obtained this time is lower<br />

than the value written down, continue to increase the gamma rod spacing until no further<br />

improvement is possible. If, on the other hand, the SWR increased, reduce the spacing<br />

between the rod and the element and perform the adjustment procedure again. In<br />

some Yagi designs, it may also be necessary to shorten the driven element to get a<br />

match.<br />

T Match<br />

Not much needs to be said about the T match since it is nothing more than a balanced<br />

(or two-sided) gamma match. All the design considerations are identical. Some antenna<br />

experimenters prefer the T match because it presumably provides a more symmetrical

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