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![]() Dave wrote: thats the basic problem in this whole discussion. you are all talking about the same thing, just using different notation and incomplete statements so that none of you understands exactly what the others are trying to talk about... when really you are all saying the same thing. its kind of like after i graduated from college with an ee degree and my sister graduated from an air force basic electronics course, she tried to ask me something about currents in a transistor and i saw it all backwards... well of course she was talking electron flow and i was talking hole flow. we both got the same result but the notation was all different. That's not true at all Dave. Most of us know that current is current. It really only flows one direction at any instant of time. We can indeed consider systems as having current that flows two directions at one instant of time, but the results of that better agree with the actual real current that flows only in one direction at any instant of time or they are wrong. Also, behavior of basic components cannot change. A two terminal device like a loading coil cannot have differences in the current flowing through it at each terminal without a third path. (I assume we all know current is not an across vector and it does not "drop", the person who started this thread just used poor wording.) ARGH! maybe it really is more basic than different notations and terminology. when working with antennas and 'component's that are a significant fraction of a wavelength in size you must take into account the 'third path'... the 'third path' consists of the distributed capacitance and resistance that CAN be modeled with lumped components if you want to go through all the approximations and extra calculations that are required. if you are ignoring that 'path' when talking about relatively large loading coils then you will be wrong, how wrong depends on how large of course. i haven't been following all the different threads and junk in here, but if you are trying to analyze a significant sized loading coil without taking into account all the paths then you are going to likely be less accurate than cecil using a more complete distributed model. OBVIOUSLY if you are using a strict lumped model the current can't be different from one end to the other. And just as obviously if you make a really large loading coil, like a full '1/2 wave' slinky dipole, the current at the feedpoint end will be MUCH different than at the open end. You can both get the same results, but to do it with lumped elements requires the same calculations that are done by finite element simulations that try to do enough small lumped elements as possible to approximate the distributed equations that would give nice smooth results. Unfortunately cecil does not do a good job in relating the distributed model, and his constant references to 'optics' and the use of terms related to that field do nothing but confuse many of the people in here to think that he is in a different world. admit it cecil, while you may be correct, using a different set of terminology than most of the people in here has done nothing but add to the confusion factor in many of this long drawn out threads. I still think that if each of you explained the WHOLE problem in your own terminology, INCLUDING all the assumptions that are required for the models you are using, that you would find that each of you is correct. but because you are starting from different sets of assumptions you will never find a common ground. enough of this, back to assembling my new linear loaded 40m beam... why don't you go analyze that loading system for a while. |
#2
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Dave wrote:
admit it cecil, while you may be correct, using a different set of terminology than most of the people in here has done nothing but add to the confusion factor in many of this long drawn out threads. I have a limited technical library. I wish my RF references spelled out everything as well as "Optics", by Hecht, but mine don't. Light and RF are the same kind of EM waves, just at different frequencies. Hecht's material is certainly relevant to RF waves. And I make every effort to translate the technical jargon from one field to the other as best I know how. Hecht presents the best treatment of superposition, interference, and standing waves that I have ever seen. I wish I had an RF reference book as well written as "Optics". -- 73, Cecil http://www.qsl.net/w5dxp |
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