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#1
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![]() THE ONLY WAY TO ACCURATELY MODEL A LOADED VERTICAL and similar coil and capacitance loaded structures, is as follows. Let's take the most simple structure consisting of 3 sections - top, centre and bottom. The top is usually referred to as a whip or a rod. The centre section is a loading coil. The bottom section can be referred to as the mast. All three sections have length and external diameter. All three sections have uniformly-distributed inductance, capacitance and resistance per unit length. All calculable from dimensions. It is inescapable, therefore, the structure consists of - THREE CASCADED TRANSMISSION LINES SECTIONS. As with ALL transmissions lines, each section has a characteristic impedance Zo, attenuation and phase-shift per unit length. All caculable from dimensions. The centre section, a solenoidal loading coil, clearly has inductance extra to that due to the length of the coil former. The extra inductance is calculable from the number of coil turns per unit length. If necessary self-capacitance can be included. ALL sections have a UNIFORMLY DISTRIBUTED radiation resistance which is extra to conductor loss resistance. The two resistances are combined by simple addition. Radiation resistance is itself obtained from the length of a section. CALCULATING PROCEDURE / PRINCIPLES. This is done by using classical transmission formulae or by the well known sufficiently accurate approximations. Looking upwards from the base of the antenna - (1) Calculate the input impedance at the bottom of the whip (or rod). The whip is a transmission line open circuit at the top end. (2) Calculate the input impedance at the bottom end of the loading coil, the centre section. The centre section is a transmission line terminated by the input impedance of the whip above it. (3) Calculate the impedance looking up from the base of the antenna. The feedpoint impedance. The bottom antenna section being a transmission line terminated by the input impedance of the centre antenna section, the loading coil. (4) Connect a generator, the transmitter, between the base of the antenna and ground. The ground will have its own 'input' resistance depending on the ground electrodes or perhaps the vehicle characteristics. (5) Using classical transmission line formulae, or their close approximations, the amps, volts, relative phase-angles, can be calculated, IF NECESSARY, at any point along the antenna, at any point along the coil, from its base to the extreme tip of the whip (6) But a full analysis is unnecessary. Nevertheless there's a big bunch of calculations to be done to calculate radiating efficiency, a single number, the ultimate solitary objective. Of what use to anybody is the difference between input and output currents of the loading coil? (7) The radiation pattern is eventually available. But even CB-ers are familiar with the radiation pattern of a simple vertical antenna, loaded or not, which is less than 5/8ths wavelengths in height. (8) By an obvious extension of the above principles, a top hat on the top of the whip, such as a set of radial wires within a ring, can be automatically accounted for. Now, you old-wives, what can be more simple than THAT? KISS! I'm very sorry, due to recommendations by the medical profession, I have to decline invitations to tea-parties in Boston, Mass. And stop haggling amongst youselves. You have quite enough problems to sort out on your side of the Atlantic. As examples of practical use of the foregoing principles, download in a few seconds and run immediately short, self-contained programs LOADCOIL and TOPHAT2 from website below. Free to USA citizens. ---- .................................................. .......... Regards from Reg, G4FGQ For Free Radio Design Software go to http://www.btinternet.com/~g4fgq.regp .................................................. .......... |
#2
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![]() "Reg Edwards" wrote in message ... THE ONLY WAY TO ACCURATELY MODEL A LOADED VERTICAL snip All three sections have uniformly-distributed inductance, capacitance and resistance per unit length. All calculable from dimensions. snip THREE CASCADED TRANSMISSION LINES SECTIONS. snip Now, you old-wives, what can be more simple than THAT? KISS! snip simple or accurate??? you can't have both. in this case you have ignored, among other things, that the capacitance between each infinitesimal part of each vertical piece to the rest of the world is different. therefore your transmission line sections are not uniform from end to end as needed to use the classical transmission line formulations. Then of course you must also consider that the actual radiated part of the field makes those 'transmission lines' appear extremely lossy... unfortunately that loss is not the R and G type loss as the transmission line formulas use, though those losses do also exist. |
#3
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![]() David Robbins wrote: --------------- simple or accurate??? you can't have both. in this case you have ignored, among other things, that the capacitance between each infinitesimal part of each vertical piece to the rest of the world is different. therefore your transmission line sections are not uniform from end to end as needed to use the classical transmission line formulations. --------------- But, since the 'classic' antenna calculations are only approximate, how much additional error would Reg's method entail, if any? I think the "simple -vs- accurate" thingy is one of the things that Reg was getting at. Very 'fiddly' (Hey Reg! I picked up an 'English' word, or would that be an 'UK-ism', sort of like an 'American-ism'?)... 'Doc |
#4
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On Fri, 05 Dec 2003 12:06:42 -0600, 'Doc wrote:
But, since the 'classic' antenna calculations are only approximate, how much additional error would Reg's method entail, if any? Hi Doc, Or more to the tenor of the purpose, how much accuracy would they add? The point was in critical thinking and David's post extended that horizon. This is all for the purpose of deriving a drive point Z, which is the Three Card Monty of analysis. 73's Richard Clark, KB7QHC |
#5
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![]() When you can write AND DEMONSTRATE QUANTITATIVELY programs which provide even more accurate models/results than what I have provided then please make them available to the world. You have much to learn. From the zero level of bafflegab you have just produced I'll give you another 40 years. As things are you are well on your way to joining the 'old wives' brigade. But please believe me. I have no wish to be unkind or discourage your admirable young man's enterprise. By all means keep persisting. --- Yours, Reg. |
#6
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![]() "Reg Edwards" wrote in message ... When you can write AND DEMONSTRATE QUANTITATIVELY programs which provide even more accurate models/results than what I have provided then please make them available to the world. You have much to learn. From the zero level of bafflegab you have just produced I'll give you another 40 years. As things are you are well on your way to joining the 'old wives' brigade. But please believe me. I have no wish to be unkind or discourage your admirable young man's enterprise. By all means keep persisting. --- Yours, Reg. it would help if you provided your model. |
#7
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Reg,
I recommend the following pair of wonderful articles. Part one is in HAM RADIO, April, 1977, pp. 52-58. The second in May, 1977, pp. 29-39. The full reference is: Boyer, Joseph M. (W6UYH): "The Antenna-Transmission Line Analog". Mr Boyer simplifies the antenna analysis by equating parts of the antenna to transmission lines along the same lines that you have. Regards Nat |
#8
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David,
I do like your reply to Reg since it evokes more thought to the transmission line theory talk. But the main point Reg, is I believe that all the group is in in agreement with respect to current change and a 'large ' inductance, and those bonded to 50/60 hertz type thinking have fled. The only important thing left for some is to not over react at the knowledge that lumped loads are theoretical in nature since viewing same can provide advantages in solutions for networks whether it be household frequency or broadcast style frequencies. Knowledge is what is valuable, whether that knoweledge is inconsequential or not to ones needs. As far as our problems in the U.S.A. Reg. As I pointed out in a Letter to the Editor when presented with terrorism by the Stern gang in London the U.K. handed the problem of a homeland for Jews to the U.N. The U.N. never anticipated that the U.S. by virtue of its veto, would support an expansion of lands in the same way we did against the American Indian, forgetting that if you can't kill them all then you have a world wide conflict with respect to those who practice Islam. Cheers and beers Art "David Robbins" wrote in message ... "Reg Edwards" wrote in message ... THE ONLY WAY TO ACCURATELY MODEL A LOADED VERTICAL snip All three sections have uniformly-distributed inductance, capacitance and resistance per unit length. All calculable from dimensions. snip THREE CASCADED TRANSMISSION LINES SECTIONS. snip Now, you old-wives, what can be more simple than THAT? KISS! snip simple or accurate??? you can't have both. in this case you have ignored, among other things, that the capacitance between each infinitesimal part of each vertical piece to the rest of the world is different. therefore your transmission line sections are not uniform from end to end as needed to use the classical transmission line formulations. Then of course you must also consider that the actual radiated part of the field makes those 'transmission lines' appear extremely lossy... unfortunately that loss is not the R and G type loss as the transmission line formulas use, though those losses do also exist. |
#9
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it would help if you provided your model.
======================== There's a dozen of them to choose from at my website. Some been sitting there for years. Moneyback guarantee. Present download rate averages around 200 per day. When can we expect one of yours? Try an easy one first. What about doing a 10 feet length of 14 gauge plastic-insulated stuff? Don't forget end-effect or you'll receive hate-mail from people suffering from delusions of accuracy. --- Reg |
#10
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"Nat Gurumoorthy" wrote Reg,
I recommend the following pair of wonderful articles. Part one is in HAM RADIO, April, 1977, pp. 52-58. The second in May, 1977, pp. 29-39. The full reference is: Boyer, Joseph M. (W6UYH): "The Antenna-Transmission Line Analog". Mr Boyer simplifies the antenna analysis by equating parts of the antenna to transmission lines along the same lines that you have. Regards Nat ================================ Nat, Antennas and transmission lines are not just analogues - Antennas ARE transmission lines with controlled 'leakage'. In fact, as people forever complain on these walls, it is impossible to prevent a transmission line FROM leaking. Genuine guru's lump the names 'lines' and 'antennas' together in one volume. They may mention in passing that the mathematics are identical to both in case a casual reader doesn't realise it. But if Terman disdainfully omits mention of the obvious there's always the danger that his disciples may think it doesn't exist. I produced the brief semi-serious description just for the purpose described in the subject line ;o) ---- Reg, G4FGQ |
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