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#1
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People have an extremely strong tendency to simplify the mass of
incoming data into simply digested and understood binary categories: Is it good, or is it evil? Does the antenna work, or doesn't it? And here the binary choice is between a 136 foot dipole and a shorter dipole. The answer here, as it is to so may binary questions, is that it behaves in some ways like one, some ways like the other, and some ways like neither. The helically wound antenna can be made resonant. A 136 foot dipole is resonant, but a shorter dipole isn't, unless loaded. It will be inefficient, which is also usually characteristic of a short dipole and not a 136 foot one. A short dipole with a properly designed matching network could be made to be more efficient than the helically wound antenna. The input resistance at resonance will be between that of a 136 foot dipole and a straight dipole the length of the helical antenna, unless the loss is exceptionally high. The bandwidth will be between that of a 136 foot dipole and one the length of the helical antenna, unless the loss is exceptionally high. The pattern will be more like that of a short dipole than that of a 136 foot dipole, although you wouldn't be able to tell the difference. It would even be hard to measure using professional equipment. Roy Lewallen, W7EL James barrett wrote: Hi, I just read instructions on building a "helically wound" antenna using a broom stick. http://www.hard-core-dx.com/nordicdx.../bromstik.html After reading this, I had an idea. I'm doing more google searches for this type of configuration, but wanted to ask here as well to get some opinions. What if I took two broom sticks, and wound each with about 68 feet of wire. Each stick making half of a dipole antenna. Then attach 450 ohm ladder line (or 50 ohm coaxial). How would this behave when connected to a tuner? Would it behave like a 136 foot dipole, or would it behave like a shorter dipole? Jim |
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#2
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Roy Lewallen wrote:
People have an extremely strong tendency to simplify the mass of incoming data into simply digested and understood binary categories: Is it good, or is it evil? Does the antenna work, or doesn't it? ... Uhh, yeah, that sums me up pretty much. You think I should be ashamed? JS |
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#3
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The answer here, as it is to so may binary questions, is that it behaves in some ways like one, some ways like the other, and some ways like neither. .. .. .. Roy Lewallen, W7EL If one were to find lossless material (superconductors?) for the short antenna and it's corresponding matching network, what would happen as the antenna became shorter and shorter compared with the half-wave dipole? Would it simply approach an isotropic radiator? Alan |
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#4
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Alan Peake wrote:
If one were to find lossless material (superconductors?) for the short antenna and it's corresponding matching network, what would happen as the antenna became shorter and shorter compared with the half-wave dipole? Would it simply approach an isotropic radiator? Alan If room temperature super-conductors were available, do you even realize the shape antennas would take? My gawd man, share some of that material here! The thought alone is inspiring! Regards, JS |
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#5
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John Smith wrote: Alan Peake wrote: If one were to find lossless material (superconductors?) for the short antenna and it's corresponding matching network, what would happen as the antenna became shorter and shorter compared with the half-wave dipole? Would it simply approach an isotropic radiator? Alan If room temperature super-conductors were available, do you even realize the shape antennas would take? My gawd man, share some of that material here! The thought alone is inspiring! Regards, JS Don't know what shape it would be but I'm sure I wouldn't recognize it! Alan |
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#6
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Alan Peake wrote:
"---what would happen as the antenna became shorter and shorter compared with the half-wave dipole?" Terman answers that question on page 871 of his 1955 opus: "The directive gain of the elementary doublet =1.5." For a resonant wire of 0.5 lambda, the gain is 1.64. There`s not much difference in directivity as the doublet shrinks to a vanishingly small size. The gains shown are power ratios, not dB`s. Comparison antenna is the isotropic of which Terman says: "Although an isotropic radiator of coherent waves does not exist because it cannot satisfy Maxwell`s equations, the properties of such an imaginary antenna are easily visualized, and the concept of an isotropic radiator is often found useful in the analysis of antenna systems." (Page 871 in the 1955 opus.) Best regards, Richard Harrison, KB5WZI |
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#7
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Alan Peake wrote:
If one were to find lossless material (superconductors?) for the short antenna and it's corresponding matching network, what would happen as the antenna became shorter and shorter compared with the half-wave dipole? Would it simply approach an isotropic radiator? Alan No. The answer can be found in any antenna textbook, because the lossless short dipole is a very good platform to illustrate a number of principles without the confounding additional consequences of loss. Briefly, -- The pattern of an infinitesimally short dipole is very similar to that of a half wave dipole. The difference is due to the triangular current distribution of the short dipole as opposed to the sinusoidal current distribution of the half wave dipole. Because the patterns are very similar and both antennas radiate all the applied power, the gain of the two antennas is nearly the same. The short dipole's pattern is a little fatter so it has slightly -- about a half dB -- less gain. But the pattern of even an infinitesimally short dipole retains the basic two-lobed dipole shape with around 1.7 dB gain over isotropic in its favored directions. -- The input resistance of the very short lossless dipole is very low and the capacitive reactance very high. The resistance approaches zero and the reactance negative infinity as the length approaches zero. There's no comparison to an isotropic radiator, since the latter is a purely fictional source with no even theoretical physical realization and therefore no definable input characteristics. -- The Q of the short dipole is very high, so the reactance varies very rapidly with frequency. A matched short antenna would have an extremely narrow bandwidth. Most of these properties of the dipoles can easily be observed with the free EZNEC demo program from http://eznec.com, and much more information about the properties of the short lossless dipole can be found in any antenna text. Roy Lewallen, W7EL |
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#8
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Roy Lewallen wrote:
... -- The Q of the short dipole is very high, so the reactance varies very rapidly with frequency. A matched short antenna would have an extremely narrow bandwidth. ... Roy Lewallen, W7EL And, here is where a DLM antenna is nice, keep the coils of low Q and bandwidth is "surprisingly wide." Regards, JS |
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#9
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On 4 Dec, 01:28, John Smith wrote:
Roy Lewallen wrote: ... -- The Q of the short dipole is very high, so the reactance varies very rapidly with frequency. A matched short antenna would have an extremely narrow bandwidth. ... Roy Lewallen, W7EL And, here is where a DLM antenna is nice, keep the coils of low Q and bandwidth is "surprisingly wide." Regards, JS Yup, My 160M antenna came at at a resistive 200 ohm plus resonance and with a bit of fiddling I now connect the coax direct and cover the whole band. Not sure if I would have been better off with keeping the high resistive impedance and using a transformer but snow is on the way so beggars can't be choosers. Regards Art KB9MZ........XG (uk) |
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#10
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Roy Lewallen wrote: Alan Peake wrote: If one were to find lossless material (superconductors?) for the short antenna and it's corresponding matching network, what would happen as the antenna became shorter and shorter compared with the half-wave dipole? Would it simply approach an isotropic radiator? Alan No. The answer can be found in any antenna textbook, .... etc. Roy Lewallen, W7EL Thanks Roy. Unfortunately, since I retired, I no longer have access to Jasik, Kraus etc. So, thanks for the answer. I should have realised that a dipole of any length is still a dipole and as such will not radiate off it's ends. Mind you, Eznec shows the average dipole, less than half-wave above ground, goes pretty close to an isotropic radiator for all practical purposes ![]() Alan |
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