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Current across the antenna loading coil - from scratch
John Popelish wrote:
If we assume the coil is an idealized lumped inductance with no stray capacitance at all (not a real inductor) then it would have the same instantaneous current at each end and that current would be zero, since it has zero size. In other words it would fit entirely in the point that holds the node. Real inductors with stray capacitance and imperfect magnetic coupling for all parts of its internal current path, would have a phase shift in the current at opposite ends, so they would have current at their ends that was 180 degrees out of phase, if they were centered on the node points. For half of each cycle, current would be entering each end, and for the other half of each cycle, current would be leaving each end. Both those currents would detour out the sides f the inductor into displacement current through the stray capacitance of the surface of the inductor to its surroundings. I think (with very little actual knowledge of the software) this conceptual model is how EZNEC handles current through a modeled inductor and how it can have different currents at the inductor ends, without being aware of whether those currents are driven by traveling or standing waves. It is all based on current through inductor segments and voltage across capacitive segments. If the segments are small enough, it is a good approximation of a distributed solution. There are two ways of modeling an inductor in EZNEC. One is by using an inductive "load". This is a pure lumped inductance, which takes up zero physical space and whose currents are equal at its two terminals. It does not couple or react at all to its surroundings other than via its terminals, and its voltage-current characteristics are dictated by that of a pure inductance, v = L di/dt. For a number of reasons discussed many times here, this isn't a good model for many or most typical loading coils. The other way of modeling an inductor in EZNEC is by making it from conductors -- "wires" -- arranged in a polygonal helix. (EZNEC v. 4.0 provides an automated way to generate this structure.) These wires are treated exactly the same as all other wires in the model. As long as the turns aren't too close together (conservatively, closer than several wire diameters, but in practice good results are usually obtained with spacing as close as one diameter air space between wires), it does a very good job of calculating the inductor currents and radiation. (It's a little generous about loss if the turns are close because it doesn't account for proximity effect.) EZNEC calculates the total current by first calculating the self and mutual impedances of every segment in the model from a fundamental equation, then using Ohm's law to find the total current in each segment from those impedances and the voltages from the user specified sources.(*) It's not aware of traveling or standing waves. The presence or absence of standing waves -- that is, a changing magnitude of current with position -- can be seen by viewing its output. Displacement current is a consequence of mutual coupling between segments -- in a dipole, the dominant coupling is to the other half of the dipole, and in a grounded monopole, to ground. However, each segment couples to every other, even on its own wire, and it's this coupling which brings about the current distribution that ultimately occurs. EZNEC deals only with total currents and makes no effort to detect, use, or break up total current into individual traveling waves. It isn't aware of whether currents are "driven by traveling or standing waves" if for no other reason that no currents are ever "driven by" traveling or standing waves. Voltage differences cause currents which can be described as traveling waves. When multiple traveling waves are summed to find a total current, the amplitude of the sinusoidal current varies with position along the line, and this envelope is called a "standing wave". A standing wave is simply a description of the magnitude distribution of the total current along a wire or transmission line. It doesn't drive or cause anything -- it's a description of an effect, not a cause. All the fuss about standing waves is a diversion which confuses the issue and deflects attention from the salient issues involved in understanding the topic under discussion. (*) This is a simplified explanation. For details, see Part I of the NEC-2 manual. Roy Lewallen, W7EL |
Current across the antenna loading coil - from scratch
This is freakin unbelievable.
You think you are making fool of me and rest of us? You are not answering questions, nor engaging in the exchange. You keep pulling out crap, like first the current is equal, then "" I can change current difference at each end of the inductor all over the place depending on the design of the loading coil, with NO change in the loading coil position or antenna lengths." You are getting tangled in your own webs!!! Tell us what is wrong with W9UCW setup and results. Where did he screw up, what is wrong, and show what you have measured in THE SAME type of setup. Not freakin W8JI coils, not at the base, no weird frequency, not twist and dance. Just take 40m shorted vertical, make it resonant with DECENT coil like he has about 2/3 up the mast, stick the RF ammeters at both ends and give us the readings. You have the pictures, you should be able to replicate the setup. Then you tell us that the current is the same at both ends, show us the pictures and describe your setup, meters, frequency and results. This goes for the rest of the "gurus" that insist on the same. Then model the loading coil as a solenoid or loading stub of same inductance in EZNEC and show us what you get. Cecil did it, and the silence is deafening!!! Can you explain what is "wrong" with Cecil's examples? Looks like Belrose should get another pHDuuhh for starting all this misconception and misinformation in ham literature. Pathetic is that some of the "gurus" that should know better, are on the same bandwagon to la-la land. Stop crap and twist and dance, answer the freakin questions or say nothing. We are not idiots that you BS with "you don't know what I mean by impedance". So what happened to impedance? Now you know what it is, or is pink electron displacement capacitance current phasor phase mumbo jumbo? wrote in message ps.com... Yuri Blanarovich wrote: Let's back off one more giant step back to measurements. Show where W9UCW was "cheating" in his test setup, pictures and comments at http://www.k3bu.us/loadingcoils.htm where he shows clearly that RF current drops significantly across (through) the loading coil, just like it drops across (through) the resonant antenna (piece of wire or tubing) from max at the base, to zero at the tip. Displacement currents in the inductor and the very high reactance of the very short antenna above the coil explain current difference. Current cannot vanish Yuri. It has to have an alternative path. Have you heard of standing waves? I can change current difference at each end of the inductor all over the place depending on the design of the loading coil, with NO change in the loading coil position or antenna lengths. That is the progress, first current can't change, now you can make it. It is the theory you have, that the current is tied to the "missing degrees", that is wrong. Without displacement currents there is no current difference at each end of the coil, it is not caused by "missing degrees. It is caused by the capacitance above the coil being very low and the capacitance of the coil to the outside world being much larger. The current is not all gone in the first few turns either. It is a series reactance/shunt reactance problem. 73 Tom PRICELESS!!!!! So WHAT IS THE CURRENT AT THE TOP OF THE RESONANT 90 deg (any) VERTICAL? Same as at the base, because "Current can not vanish Yuri"? You are jerking our chain or have a real problem. Suggestion: do some reading on impedance, resonance, standing waves, current and voltage distribution along the antennas, and look at the current curves in books and as produced by EZNEC. Looks like you have no clue how antennas work. You can have another "last word" that will "show" that you "know" what you are talking about. 73 Yuri |
Current across the antenna loading coil - from scratch
wrote:
Current cannot vanish Yuri. It has to have an alternative path. Forward current is one amp at zero degrees. Reflected current is one amp at 180 degrees. That creates a standing wave current node where net current is zero. It has "vanished" due to superposition. -- 73, Cecil http://www.qsl.net/w5dxp |
Current across the antenna loading coil - from scratch
Roy Lewallen wrote:
EZNEC deals only with total currents and makes no effort to detect, use, or break up total current into individual traveling waves. Then, without effort, EZNEC accurately reports the presence of traveling waves or standing waves as can be seen from the graph of the EZNEC results at: http://www.qsl.net/w5dxp/travstnd.GIF The graph on the left is for traveling wave current. Its magnitude is fixed and its phase varies with wire length. Traveling wave phase can be used to determine the phase shift through the wire (or through a coil). The graph on the right is for standing wave current. Its phase is fixed and its magnitude varies with wire length. Standing wave magnitude can be used to determine the phase shift through the wire (or through a coil) by taking the arc-cosine of the magnitude. -- 73, Cecil http://www.qsl.net/w5dxp |
Current across the antenna loading coil - from scratch
Yuri Blanarovich wrote:
Just take 40m shorted vertical, make it resonant with DECENT coil like he has about 2/3 up the mast, stick the RF ammeters at both ends and give us the readings. You have the pictures, you should be able to replicate the setup. What is it you are after? I already posted, years ago, measurements at: http://www.w8ji.com/mobile_antenna_c...ts_at_w8ji.htm Then you tell us that the current is the same at both ends, show us the pictures and describe your setup, meters, frequency and results. I think what is happening here is you are getting angry and not paying attention to what people are saying. I've already said it is possible to have different currents at each end of a loading coil. What I disagree with you about is you seem to attribute that difference to some magical property related to the distribution of current based on electrical degrees the loading coil replaces or standing waves, and that is very simply and clearly wrong. Current cannot "drop" or be "dropped". It can be divided between paths, but it cannot vanish into thin air. The mechanism that allows current to change in an antenna is displacement current, and it comes from capacitance. The only thing wrong with Barry's setup is he uses large meters compared to the size of the coil, and they are invasive. The meter requires cutting the leads and adding a fairly large bulk into the system. I'd never use thermocoupler meters to measure high impedance systems, magnetic-field coupling systems can be smaller, have less distributed capacitance, and don't require rerouting leads. Current transformer systems are also more accurate and can have much better resolution, and can even be used to determine phase. Let's not let the measurement method overshadow the real disagreement, however. The real disagreement is you seem to be saying the missing area of antenna replaced by the inductor and standing wave patterns of current distribution in the antenna are what causes the loading coil to behave as it does. Barry also proposed that, if I am not mistaken. That is not true. The single thing that allows an inductor to have a current difference and phase shift in current along the coil or at each terminal is the capacitance of the coil to the outside world. That is why we would have to be very careful NOT to disturb the coil by mounting other large measurement devices on the coil. This goes for the rest of the "gurus" that insist on the same. The "gurus" you despise go back to Maxwell, who described displacement current: http://maxwell.byu.edu/~spencerr/websumm122/node72.html The term displacement current is not an invention of those you call "gurus". It is part of physics dating way back to the 19th century. THAT is why so many people are trying to tell you about displacement currents, it isn't to make you feel bad. You have to include displacement currents in any model, or you cannot have a current taper along the length of a conductor. Then model the loading coil as a solenoid or loading stub of same inductance in EZNEC and show us what you get. Cecil did it, and the silence is deafening!!! Can you explain what is "wrong" with Cecil's examples? Sure. His explanation of what is happening and the fact he picked a very special conditions just to satisfy a twisted theory. Roy showed in his models why Cecil's conclusions were wrong. Practical measurements will show the same thing. The ONLY thing that allows a conductor to have current taper along its length is displacment current. That is a function of the capacitance from that conductor to the world around that conductor compared to the impedance presented by the system beyond that point. It is NOT determined by standing waves. It is not determined by "missing length replaxed by coil". Looks like Belrose should get another pHDuuhh for starting all this misconception and misinformation in ham literature. Pathetic is that some of the "gurus" that should know better, are on the same bandwagon to la-la land. I'm not sure what motivates you to attack everyone, but at least you universally seem to hate almost everyone. Jack Belrose is a great guy and has contributed a great deal with his work. If you finmd something wrong with what he is saying, tell us what it is. Don't attack the person, point out the error. Stop crap and twist and dance, answer the freakin questions or say nothing. We are not idiots I suppose everyone has a right to their own opinions on that topic. I've done my best to answer the questions. I hope this post helps clarify things. Calm down, there is no need to get upset. Did this help answer your questions? 73 Tom |
Current across the antenna loading coil - from scratch
wrote:
I already posted, years ago, measurements at: http://www.w8ji.com/mobile_antenna_c...ts_at_w8ji.htm Those are RMS standing wave measurements. To see what is wrong with using RMS standing wave measurements please see: http://www.qsl.net/w5dxp/travstnd.GIF I think what is happening here is you are getting angry and not paying attention to what people are saying. I've already said it is possible to have different currents at each end of a loading coil. And there phase information in those standing wave current magnitudes. There is no phase information is standing wave current phase. What I disagree with you about is you seem to attribute that difference to some magical property related to the distribution of current based on electrical degrees the loading coil replaces or standing waves, and that is very simply and clearly wrong. No, it is your misconceptions about standing wave current that are very simply and clearly wrong. Current cannot "drop" or be "dropped". RF current drops with the attenuation factor, just like RF voltage does. Clinging to the lumped circuit model presuppositions is what causes you to make silly assertions like the above. Standing wave current periodically drops to zero in unterminated transmission lines. The single thing that allows an inductor to have a current difference and phase shift in current along the coil or at each terminal is the capacitance of the coil to the outside world. Is capacitance to the outside world also what allows a wire to have zero current at one point and two amps of current 90 degrees away. Of course not! The degrees of delay through the coil is primarily responsible for the difference in current. That, and where it is places on the standing wave current curve. You have to include displacement currents in any model, or you cannot have a current taper along the length of a conductor. We are talking about displacement current to earth ground and there is zero displacement current to the outside world ground yet there's SWR current taper on coaxial transmission lines. Maybe it's time for you to learn how to add phasors? Sure. His explanation of what is happening and the fact he picked a very special conditions just to satisfy a twisted theory. Roy showed in his models why Cecil's conclusions were wrong. Practical measurements will show the same thing. Roy used standing wave current phase to try to measure the delay through a coil. That's an invalid measurement. None of my conditions are special. They just seem special to your lumped circuit model. The distributed network model works for all conditions. -- 73, Cecil http://www.qsl.net/w5dxp |
Current across the antenna loading coil - from scratch
Roy Lewallen wrote:
Jack Belrose, VE2CV, is a highly respected engineer and scientist with an extensive and distinguished professional history. So are a lot of people who disagree with you. No one is always right, ... You have known for a year now that standing wave current phase cannot be used to determine the delay through a coil yet you continue to post those invalid results. Guess you are proof of your own statement. -- 73, Cecil http://www.qsl.net/w5dxp |
Current across the antenna loading coil - from scratch
Tom, W8JI wrote:
"The ONLY thing that allows a conductor to have current taper along its length is displacement current." In a-c circuits, added to ordinary conduction current there is displacement current, at right angles to the direction of propagation, determined by the rate at which the field energy changes. Also at right angles to the direction of propagation, and determined by the rate at which energy changes, there is a changing magnetic field, in addition to the changing electric field. Together the electric and magnetic fields exchange energy and produce radiation. Displacement current which is the a-c current through a capacitor, that has no d-c conduction, is not the"ONLY" thing that allows a conductor to have a current taper along its length.. A conductor can lose energy through dissipation and radiation forever, not just relocate it temporarily through storage in a reactance. The dissipation line at the end of a rhombic antenna does not handle the entire output of the transmitter at its other end. Most of the energy is already radiated by the time it reaches the dissipation line. Best regards, Richard Harrison, KB5WZI |
Current across the antenna loading coil - from scratch
Cecil Moore wrote:
We are talking about displacement current to earth ground and there is zero displacement current to the outside world ground yet there's SWR current taper on coaxial transmission lines. Maybe it's time for you to learn how to add phasors? Cecil, Sorry, you cannot pick and choose which displacement currents to consider. It might be helpful to go back to review the fundamentals of Maxwell's equations, including the continuity equation for current, before making these inane comments. 73, Gene W4SZ |
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