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![]() -- .................................................. .......... Regards from Reg, G4FGQ For Free Radio Design Software go to http://www.btinternet.com/~g4fgq.regp .................................................. .......... "Cecil Moore" wrote in message ... Reg Edwards wrote: Take a close-wound wire helix of diameter D metres and having N = 500 turns per meter. Wire diameter approx 2mm. All formulae available from Terman, Kraus, ARRL, etc., etc. C = 55.5 / (Ln( 2 * H / D ) - 1) picofarads per meter. L = Square( N * Pi * D ) / 10 microhenrys per meter. TransLine impedance, Zo = Sqrt( L / C ) ohms. Propagation Velocity = 1 / Sqrt( L * C ) metres per second. Take a length of H =1.5 metres of this helix and use it as a short vertical antenna above a good ground. It will resonate as a 1/4-wave vertical at 3.5 MHz. Zo = 3243 ohms. Velocity factor = 0.0701 Radiation Resistance = 0.176 ohms. etc., etc., It's so simple you can't believe it. ;o) Thanks Reg, this one is a keeper. If you made the helix long enough to cause a phase reversal in the current, would the world come to an end? -- 73, Cecil ======================== I forgot to say it will also have a 'cosine' current distribution between base and top. The antenna 'end effect' can be accounted for if necessary. When the helix is not close wound, the increase in velocity factor and the reduction in Zo can be accounted for. Axial mode radiation cannot be distinguished from normal mode but this is of negligible consequence until helix circumference approaches 1/4 wavelength which it never does in the present context. ---- Reg. |
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