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Re: [Amps] 200-ohm tank and "un-un" in HF amp design?

To: amps@contesting.com
Subject: Re: [Amps] 200-ohm tank and "un-un" in HF amp design?
From: Manfred Mornhinweg <manfred@ludens.cl>
Date: Mon, 21 Oct 2013 13:36:18 +0000
List-post: <amps@contesting.com">mailto:amps@contesting.com>
Hello,

it should be remembered that the values of loading capacitance, tuning capacitance and the inductance of the tank coil not only depend on impedances and frequency, but also on Q. The designer has a wide degree of control over these values.

For example, if we need to match 4000 ohm to 50 ohm, on 160 meters, and we have a loading capacitor of just 1000pF, and we don't want to add capacitors in parallel, we can pick a Q of 10. This leads to 215pF tuning capacitance (including tube and stray capacitance), a 35.8uH coil, and 882pF of loading capacitance.

If that's still too high, just let's decrease the Q to 9.5. That gives us 204pF, 37.2uH, and 645pF.

Still too high? Use Q=9. Then we get 194pF, 38.4uH, and just 272pF of loading capacitance!

In practice this would be done by tapping the tank coil at a spot where the Pi circuit tunes up with the loading capacitor at the center of its range, into a dummy load. Regardless of how much maximum capacitance that capacitor has! That will give us the best matching range possible for real antennas with non-perfect SWR. Of course, the smaller the loading cap is, the narrower this tuning range becomes.

The actual penalty of having a very high plate impedance is that we cannot use a lower Q. With 4000 ohm, we cannot go below a Q of 8.89. This makes tuning a bit touchy, and we need a VERY good tank coil to get acceptable losses. The loss depends on the ratio between the natural (unloaded) Q of the components, mainly the coil in practice, and the loaded Q. If the coil has a natural Q of 300, which is typical, and we are running it at a loaded Q of 10, it will loose one thirtieth of the total RF power. At 1500 watts, that's 50 watts heating the coil, which may be a problem.

If the plate impedance instead is just 2000 ohm, the minimal Q we can use is 6.4, in practice we might use 8 or so. That way the loss is a bit lower, and tuning is a bit broader.

Of course we cannot go too low with the loaded Q, because that will increase harmonic output to an unacceptable level. Old handbooks say that actually we shouldn't go lower than Q=10 or so.

On the highest bands, the problem is another one: All that tube capacitance and stray capacitance forces us to use a Q higher than we would like! For example, on 10 meters with a 4000 ohm plate, a Q of 10 would need a tuning capacitance of just 14pF. Good luck finding a tube, and a construction method, that keeps the tube and stray capacitance lower than this! Likely that capacitance will be higher, forcing us to use a higher Q. If the total tube and stray capacitance, plus the minimal capacitance of the tuning cap, is 40pF, we need to use a Q of 30 (or higher). At Q-30, the coil becomes only 0.83uH. With a natural coil Q of 300, we would have 150 watts of loss in that little coil! That's why many amps use coils wound from thick, broad silver plated copper strip for the high bands. Absolutely highest possible natural Q of that coil is a strict need! And of course tuning gets much more touchy than on the lower bands.

For these reasons, most amplifiers don't use the same loaded Q on all bands. They use higher Q on the higher bands, to accomodate the tube and stray capacitances, and lower Q on the lower bands, to keep the tuning and loading caps from growing too much, and to allow the use of smaller loading coils. High Q coils for low frequencies are large.

Well, that was a quick burst of antique tube technology, from my side. Since it's monday morning, I hope I may be forgiven. Now I switch back into 2013.

Manfred

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