-----Original Message-----
6.  Don't use a half wavelength at your desired frequency because it is very
difficult to match an antenna with nearly infinite reactivity.  You can put
a coil in series to make it about 0.75 wavelength so you can match it, but
it will not be easy.

-----------------------------

Not at all. I do it all the time. The reactance of a 1/2 wave wire is zero
(A 1/2 wave is, by definition, resonant. Resonant means it has zero
reactance). 

The impedance in a "real world" 1/2 wave antenna is something in the range
of 4000 or 5000 ohms, tops, and often much less. It's affected by the
length/diameter ratio. That's only the resistive value since the reactance
is zero.

Such an antenna is often referred to as a "Fuchs" antenna, since he
popularized it in the 1930's.

What I *have* noticed is that most commercial matching networks (ATUs) today
won't handle an impedance of several thousand ohms. Either they simply don't
have the range of adjustment needed or they'll arc over inside. That's
because of the very high RF voltages that are present when the impedance is
in the thousands of ohms. That's why you see *big* air variables or even
vacuum capacitors were commonly used in the ATUs from the 1930's and 40's
just as they were in the high-impedance "tank" circuit at the output of a
vacuum tube power amplifier.

Overall, it's wonderfully efficient antenna, as is any end fed, vertical,
inverted L or otherwise, that has a very high feed point impedance compared
to the impedance of the ground connection. Remember that the RF current is
divided between the antenna (almost all of it becoming electromagnetic
waves) and the ground connector according to Ohm's law. The two impedances
are in series, so the idea is to reduce the ground impedance as far as
possible while *raising* the radiator's impedance to a value as high as
possible. 

Since we're often constrained by a given radiator impedance, we're usually
struggling to reduce the ground impedance to improve the ratio and so the
efficiency.

Ron AC7AC

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