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Today I Learned: Berkeley Has Two Ham Radio Clubs; Emperical Evidence and Dipole Conductor Diameter

 There are more radio stations than I thought at UC Berkeley. To be specific, there's two. Yesterday, the KD0FNR Rockmite was seen by both of them: the first piece of evidence that changing the conductor diameter of the half wave dipole had a measurable effect. As it  turns out, changing the dipole conductor width led to more questions than answers & also better propagation... maybe.


The aerial wires for the Rockmite's dipole have always seemed somewhat vanishingly small to me. I don't have an exact size right now, but if I had to guess, I'd go with them being 24 AWG or about 02 inches in diameter. They're signle stranded wires that break at the BNC to banana plug adapter about once a week, gradually shortening the antenna and raising its resonant frequency.

Out of a suspicion (vague recolection from EM class?) that a higher diameter wire would result in better power output, and some vaguely supporting research materials, I swapped out the single strand wires for a 16 AWG wire yesterday.


The above picture shows the first issue I encountered with the wire. It's too large to be easily inserted into the adapter. As you can see, I figured out a workaround. There were other issues with the antenna mostly revolving around it's increased weight per foot.

The nice thing though, was that the results were immediately different. Not long after changing out the wire, the Rockmite hit two stations in Berkeley: W6BB and NU6XB. The last time it hit one of the stations was  several weeks ago. The other station was new to the Rockmite. Both were at Berkeley, and might have been different antennas from the same radio club? I'm looking forward to researching the  history of the clubs.

In general, I learned that I have way more to learn. The wire change definitely caused different results. That's good. There a lot of reasons this could be though:

  • The increased weight of the wire led to it having a feedpoint  altitude in the backyard that was about a foot lower. This would have increased the angle of radiation launch from the antenna making it more likely to hit Berkeley.
  • While it wouldn't have been an issue for the Berkeley spots, (they were made at 14:10 GMT, or 6:10 PST when there's little evidence of ionospheric skip propagation from the home station), the results observed during the rest of the day could have been due to the ionosphere being different from one day to the next.
One final note, I found out this morning that half wave dipoles have an impedance of 72 ohms in free space??? This makes our usual 50  ohm cable choice seem odd. Again, I'm looking forward to doing more research in this regard.
Update:
This makes more sense of the 72 ohms:
If a horizontally polarized ½ wave antenna (dipole) is greater than 0.2 wavelengths above ground, the feed-point impedance will not be noticeably affected. At 0.1 wavelength above ground the feed-point impedance of such an antenna will be closer to 20 ohms, rather than the 72 ohms expected at optimum height. For example, an 80 meter dipole needs to be about 50 feet above ground and away from other objects for best results, and then a 75 ohm transmission line cable would be used. If a 50 ohm cable is desired (to better match with the radio) the antenna height could be more like 35 feet above ground. Experimentation is the best means of determining the best height because one cannot be sure where the true ground level is located (it may be under the earth level).


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