As far as r.f. resistances –
I looked through my trusty old “Radio Engineers’ Handbook” by Terman for wire a.c. resistances. On page 35 of my edition is the wanted information. This is Section 2 of the book called Circuit Elements, part 4. Resistance at Radio Frequencies – Skin Effect. There is equation (6) for a.c. resistance and then Figure 4 follows, which is a graph for r.f. resistance versus frequency based on equation (6). If I pick on the graph a solid copper wire of the same area as the 0.003” cladding on the surface of a #8 AWG, which is about equal to a #18, I came up with a resistance of 332 milliOhms for 10 feet at 1.8 MHz., if I did all conversion math correctly. This is 5.2 times the dc resistance of # 18 solid copper wire. So it appears that the wire you have is o.k. at 160 meters.
Tom,
Thanks for all the research. I probably have most of the reference material, but that would have taken me hours.
I haven't studied the graphs yet and that will likely clarify my question, but at first glance it would appear to me that copper clad, or thin hollow copper tubing would have less rf resistance than would solid copper wire of the same (copper) cross-sectional area, since (in the cited example), due to the skin effect, a substantial portion of the copper in #18 solid would carry little or no rf current, whereas nearly all the copper in the .003" #8 cladding, which lies almost entirely within the first skin depth, would carry rf current.
For the radiating part of the antenna, or for long stretches of OWL, I would want to use hard-drawn solid copper to avoid stretching. I did check some on-line vendors, and found that #8 is THE one size that is hard to find. #4, #6, #10, #12 and #14 are readily available, but not #8. I did find an outfit in CA that lists #8 bare solid hard-drawn copper, but they didn't list prices. But my test results showed that the #8 copper clad I have on hand is perfectly satisfactory, so I didn't bother to enquire further. I might have decided otherwise if I were using the line to run a high SWR tuned feeder, or as a short wire antenna with low radiation resistance, but running flat circa 450-ohm line, the loss is negligible, much less than measured with an equivalent length of fresh RG-213 or RG-214. At a kilowatt of carrier, the rf current in 450-ohm line is approximately 1.5 amps.
But then, many of the commercial wire antenna arrays from the 1920s on, used phosphor bronze wire for antennas, and phosphor bronze despite its excellent mechanical properties has a relatively small fraction of the conductivity of copper. Even #18 solid copper would probably have less rf resistance.
Considering the rf current and voltage at a given power level (at low SWR), I would say that 450 ohms is far more optimum for a transmission line Zo, than is 50 ohms.
What I don't understand is why the vendors have such an aversion to #8 gauge.