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On Apr 23, 7:06*am, Cecil Moore wrote:
Roy Lewallen wrote: If you look at the transmission line properties of a vertical, you see that the two conductors (the antenna and ground plane) get farther and farther apart as the distance from the feedpoint increases. This behaves like a transmission line whose impedance increases with distance from the feedpoint and, in fact, a TDR response shows just this characteristic. It's open circuited at the end, so it behaves pretty much like an open circuited transmission line, resulting in the same reflections and resulting standing waves you see on a real antenna. The Z0 characteristic impedance that matters is the one that exists at the coil-stinger junction which can be estimated from the single-wire transmission line Z0 equation. It's usually in the neighborhood of a few hundred ohms. For instance, a #14 horizontal wire at 30 feet has a Z0 very close to 600 ohms according to the formula. One difficulty is accounting for the radiation, which adds resistance to the feedpoint. I've never seen an attempt at simulating it with distributed resistance, which I don't think would work except over a narrow frequency range. I have simulated such using EZNEC's wire resistivity option. The resistance wire simulates the radiation "loss" from the antenna. But for a standing wave antenna, the "loss" to radiation is only about 20% of the total energy stored on the standing wave antenna. Therefore, a qualitative conceptual analysis can be done assuming lossless conditions just as it can be done with transmission lines. But one shortcoming of many antenna transmission line analogies is the attempt to assign a single "average" or "effective" characteristic impedance to the antenna, rather than the actual varying value. This is where a lot of care has to be taken to assure that the model is valid in the regime where it's being used. Seems EZNEC automatically compensates for the varying Z0 so all we need to estimate is the single effective Z0 at the coil to stinger impedance discontinuity. There's no reason you can't also include a loading coil in the transmission line model, and Boyer devotes much of the second part of his article to doing just that. A solenoidal coil raises the characteristic impedance of the length of "line" it occupies, because of the increase in L/C ratio in that section. The traveling wave delay in that section of the transmission line also increases due to the increased LC product. Are you saying the physics of the delay through a loading coil changes between a traveling wave and a standing wave??? The standing wave is composed of a forward traveling wave and a reflected traveling wave. They would experience the same delay that you are talking about above. So why didn't you use a traveling wave to measure the delay through a loading coil??? Exactly how can the following antenna current (from EZNEC) be used to calculate delay? The current changes phase by 2.71 degrees in 90 degrees of antenna. If the antenna was lossless, i.e. no radiation, that current would not change phase at all. * * * * * * * * * * * *EZNEC+ ver. 4.0 thin-wire 1/4WL vertical * * 4/23/2009 * * 6:52:13 AM * * * * * --------------- CURRENT DATA --------------- Frequency = 7.29 MHz Wire No. 1: Segment *Conn * * *Magnitude (A.) *Phase (Deg.) 1 * * * *Ground * * 1 * * * * * * * *0.00 2 * * * * * * * * * .97651 * * * * *-0.42 3 * * * * * * * * * .93005 * * * * *-0.83 4 * * * * * * * * * .86159 * * * * *-1.19 5 * * * * * * * * * .77258 * * * * *-1.50 6 * * * * * * * * * .66485 * * * * *-1.78 7 * * * * * * * * * .54059 * * * * *-2.04 8 * * * * * * * * * .40213 * * * * *-2.28 9 * * * * * * * * * .25161 * * * * *-2.50 10 * * * Open * * * .08883 * * * * *-2.71 -- 73, Cecil, IEEE, OOTC, *http://www.w5dxp.com Cecil The problem in this debate is that others are concentrating on resonance where as you are thinking in terms of anti resonance which portends to a higher impedance and also the condition of equilibrium. When considering the boundary law one must recognise that momentum increases and decreases twice per period. Thus when considering the boundary laws the negative area of the sine wave must be placed underneath the positive area such that momentum is taken account of. When the diagram provided by Best on this thread was shown what it described was the period was extended by the containment within the boundary and where that containment extended the period which is now longer than the period of non containment.In one case you have accelleration and deaccelleration which is depicted as the emmission of energy or flux. Consevation of energy laws demands that for balance we must take into account the energy or flux that enters the boundary to maintain equilibrium which is depicted by the negative area of the sine wave period such that this area is placed directly under the positive area while still remaining within the arbritrary boundary. Thus we have effectively changed the period when looking at a coil where the slow wave is now half of the original wave as is theresonant point is half of the anti resonant point which in terms of Newton and Maxwell represents the point of equilibrium. When using the resonant point in terms of relativity ie Maxwell you are seeing movement of a charge from "a" to "b" which when repeated is repetitive movement in a single direction. When using the anti resonant point the charge returns to the starting point and if time is regarded as /dt then the charge only moves in the vertical direction. Thus in terms of Earth mass consists of energy movement in the ":z" plan and with respect to the Universe the energy movement is solely in the "x" or "y": direction until this action is equated with an action from the opposite direction as per the law of Newton. Thus like Einstein viewing the same action of Newton this thread is viewing the same problem where one is static and one is relative but never the less the same problem but relatively different. Pure physics my dear Watson viewed fron different vantage points., one takes equilibrium into account where as the other doesn't. Not "babble"' David just an explanation per classical physics which is the sole and only root of both mechanical and electrical engineering Best regards Art Unwin KB9MZ xg(uk) |
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