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Art Unwin wrote:
You based your proof of a magnetic wave in a vacuum but it is an accelerating charge which obviously must have mass, that is radiation ala the particle. The accelerating charges are slow-moving electrons. The RF current moves at the speed of light in the (conductive) medium. Therefore, the RF current is associated with photons emitted by the electrons. Photons have zero rest mass and zero electric charge. Photons are the particles associated with RF waves. -- 73, Cecil, IEEE, OOTC, http://www.w5dxp.com |
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Roy Lewallen wrote:
What is the delay through a physically very small toroidal coil with the same inductance as the solenoidal coil? Why? A toroidal coil cannot be modeled using the Dr. Corum formulas. But I will take a stab at the answer. In a physically very small toroidal coil, all the turns are tightly coupled, i.e. the flux caused by one coil links all of the other windings so the delay should be quite small. In any case, one cannot use a current with unchanging phase (referenced to the source phase) to calculate the delay through anything. The only phase information left in a standing wave is in the magnitude. If the current magnitude at the bottom of the coil is 1.0, the phase shift is the ARCCOSine of the current magnitude at the top of the coil for a base-loaded resonant antenna. Actual phase measurements on the current in standing-wave antennas is meaningless. We already know it hardly changes at all with length. EZNEC confirms that statement. In an air-core solenoidal coil, like the one w8ji used, the flux linkage tends to be associated with adjacent turns so all the flux does not link all the coils. Tom's coil was 100 turns, 10 TPI, 2" diameter. The first turn was 10 inches away from the last turn. The delay through that coil calculates out to be about 25 nS. If we setup a 2" transmit coil and a 2" receive coil 10 inches away in air, the energy transfer efficiency would be very small. I don't have a formula for such but I assume one (or more) exists. Bottom line: There are now formulas for calculating the Z0 and VF of large air-core loading coils which are known to be in the family of *slow-wave* devices. I doubt that a toroidal coil is in the family of slow-wave devices. -- 73, Cecil, IEEE, OOTC, http://www.w5dxp.com |
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steveeh131047 wrote:
Tom, Yes I have EZNEC and recognise what a great tool it is. Its predictions were the benchmark against which I tested the various coil models I read about, and no-one has yet suggested that it can't be trusted for modelling a helix. I'm not on some "philosophical quest" - I'm just an old, retired, guy who still likes learning and wants to understand more about how things work; I hope that never leaves me! I stumbled on this discussion quite by chance and tried to understand the various "positions" being taken. Perhaps I'm over-simplifying, but it seemed to me there was a group who favoured the transmission-line model and a group against it. I've tried dispassionately to understand the various arguments and to form my own conclusions. Now here's my problem: * The results I get using a model based on transmission-line analysis are very close to my EZNEC predictions - not perfect, but way better than any lumped-element analysis results * I don't see quantitative, non-empirical, arguments being put forward to support lumped-element analysis * I see numeric arguments being put forward by Cecil to support a transmission-line approach - they look convincing to me and, although I see a lot of unpleasant personal attacks on him, I don't see any scientific challenge to his figures * On the other hand I see folk whose work I rate highly, seemingly willfully to misunderstand some of the points which Cecil puts forward Please don't think I'm trying to defend Cecil - I wouldn't be so presumptuous, and anyway he's old enough to look after himself! I'm just trying to understand why, what seems to me to be such a persuasive argument, generates such opposition. Either there's some glaring technical error here which I haven't yet spotted, or perhaps there's a long "history" between various "personalities" of which I'm ignorant? Still confused, Steve G3TXQ There aren't many people who would support a lumped-element analysis on this newsgroup. Most people know the limitations of using network theory in these circumstances. The technical arguments against Cecil's approach were offered a long time ago. This latest is just a flareup that will soon die down. You shouldn't be confused. The transmission line model of antennas is well accepted and hoary with age, particularly for bi-conical antennas (see Schelkunoff). There are a couple of other types of models with equal validity. If you really want to know the physical score, though, you have to get an electromagnetics text that discusses the integral equations that govern antenna behavior. Pay particular attention to the parts that explain why numerical methods like EZNEC have to be used for solutions rather than the symbolic math most people would expect and want. 73, Tom Donaly, KA6RUH |
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steveeh131047 wrote:
. . . Now here's my problem: * The results I get using a model based on transmission-line analysis are very close to my EZNEC predictions - not perfect, but way better than any lumped-element analysis results * I don't see quantitative, non-empirical, arguments being put forward to support lumped-element analysis * I see numeric arguments being put forward by Cecil to support a transmission-line approach - they look convincing to me and, although I see a lot of unpleasant personal attacks on him, I don't see any scientific challenge to his figures * On the other hand I see folk whose work I rate highly, seemingly willfully to misunderstand some of the points which Cecil puts forward Please don't think I'm trying to defend Cecil - I wouldn't be so presumptuous, and anyway he's old enough to look after himself! I'm just trying to understand why, what seems to me to be such a persuasive argument, generates such opposition. Either there's some glaring technical error here which I haven't yet spotted, or perhaps there's a long "history" between various "personalities" of which I'm ignorant? Still confused, Steve G3TXQ Some of your questions can be answered by doing a google groups search of this newsgroup for the topic "Current in antenna coils controversy" in 2003. There are several other lengthy threads at later dates, such as "Current across the loading coil - from scratch", "Loading coils; was : Vincent antenna", "Standing-Wave Current vs Traveling-Wave Current", and a number of threads prior to 2003. Roy Lewallen, W7EL |
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Jim Kelley wrote:
... and as any good dry labber knows, it's a dead giveaway to report a precision greater than one can actually measure. :-) I have reported no precision - my 100 MHz scope has not been calibrated since I retired. It doesn't take much precision to know that there's something wrong when two measurements are a magnitude apart or when someone asserts a 3 nS delay through a 10 inch long slow-wave solenoid coil with a VF of 0.033. :-) -- 73, Cecil, IEEE, OOTC, http://www.w5dxp.com |
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Tom Donaly wrote:
There aren't many people who would support a lumped-element analysis on this newsgroup. Most people know the limitations of using network theory in these circumstances. The technical arguments against Cecil's approach were offered a long time ago. This latest is just a flareup that will soon die down. You shouldn't be confused. The transmission line model of antennas is well accepted and hoary with age, particularly for bi-conical antennas (see Schelkunoff). There are a couple of other types of models with equal validity. If you really want to know the physical score, though, you have to get an electromagnetics text that discusses the integral equations that govern antenna behavior. Pay particular attention to the parts that explain why numerical methods like EZNEC have to be used for solutions rather than the symbolic math most people would expect and want. 73, Tom Donaly, KA6RUH I did and do support lumped element analysis for a very small toroidal loading inductor, and extensively posted the reasons why in this newsgroup about six years ago ("Current in antenna coils controversy", 2003). Cecil and Yuri were arguing that the coil would replace some number of "degrees of antenna" and its current therefore would have a substantial phase difference between input and output ends. I made and posted careful measurements to support my statement, after which Cecil invented his "standing wave current" and went off in various directions. Roy Lewallen, W7EL |
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Jim Lux wrote:
Tom Donaly wrote: Finally, a modest question: if you have EZNEC, why would you be wasting time with something inferior? The gold standard is the gold standard. Perhaps more the silver or electrum standard. EZNEC doesn't do dielectric loading, for instance. (unless you get the Nec4 engine from Roy) All program types, including the demo, of EZNEC v. 4.0 and later do dielectric loading similar to NEC-4. (The method came from sources other than NEC-4.) Like the NEC-4 implementation, it's of limited accuracy and usefulness -- it's really good only for thin wire insulation of moderate permittivity. And, it's a MoM code, so things not well represented by collections of wires aren't necessarily modeled well. Absolutely true. And it can't handle things like patch antennas or antennas printed on a PCB. Roy Lewallen, W7EL |
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Jim Lux wrote:
Roy Lewallen wrote: Let's see how well the principles involved are understood. What is the delay through a physically very small toroidal coil with the same inductance as the solenoidal coil? Why? As in a coil wound on a toroidal magnetic core? or a air cored solenoid bent in a circle? I'll say one wound on a magnetic core, simply to keep the size small, the coupling tight, and the field confined. I don't, however, care how long a piece of wire it's wound with. Roy Lewallen, W7EL |
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On Apr 23, 10:10*pm, Roy Lewallen wrote:
Some of your questions can be answered by doing a google groups search of this newsgroup for the topic "Current in antenna coils controversy" in 2003. Roy, I've glanced at some of those references and it looks like there's years of "catch-up" reading for me :) It seems like the starting point for one of the earliest discussions was whether or not there is a variation in current amplitude along the length of a loading coil, with some pretty strong opinion saying that there isn't. I don't want to go over old ground, but perhaps you can give me a simple answer to this one question: When I use EZNEC to model a 6ft whip above a loading coil (40T, 6" diameter, 12" long), and look at the current distribution across the coil at the resonant frequency of the antenna (3.79 MHz), I see 1A at the base of the coil increasing to 1.07A at the centre of the coil and then dropping to 0.69A at the top of the coil. My question is: "Can I believe that I would see a similar current variation in the 'real world', or is this some failing of EZNEC to model the antenna properly?" Regards, Steve G3TXQ |
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steveeh131047 wrote:
Roy, I've glanced at some of those references and it looks like there's years of "catch-up" reading for me :) It seems like the starting point for one of the earliest discussions was whether or not there is a variation in current amplitude along the length of a loading coil, with some pretty strong opinion saying that there isn't. I don't want to go over old ground, but perhaps you can give me a simple answer to this one question: When I use EZNEC to model a 6ft whip above a loading coil (40T, 6" diameter, 12" long), and look at the current distribution across the coil at the resonant frequency of the antenna (3.79 MHz), I see 1A at the base of the coil increasing to 1.07A at the centre of the coil and then dropping to 0.69A at the top of the coil. My question is: "Can I believe that I would see a similar current variation in the 'real world', or is this some failing of EZNEC to model the antenna properly?" Regards, Steve G3TXQ Yes, you would see this in the real world. EZNEC does a very good job of modeling a wire antenna with a loading coil, provided that you model the coil as a wire helix rather than lumped "load", and you can trust the results. As I've implied, a lumped load is quite a good model for a physically small, essentially non-radiating loading coil like a toroid on a magnetic core. Roy Lewallen, W7EL |
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On Apr 23, 10:44*pm, Roy Lewallen wrote:
Yes, you would see this in the real world. EZNEC does a very good job of modeling a wire antenna with a loading coil, provided that you model the coil as a wire helix rather than lumped "load", and you can trust the results. As I've implied, a lumped load is quite a good model for a physically small, essentially non-radiating loading coil like a toroid on a magnetic core. Roy: thanks for the unequivocal and clear answer. Steve G3TXQ |
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On Apr 23, 3:22*pm, Cecil Moore wrote:
Art Unwin wrote: You based your proof of a magnetic wave in a vacuum but it is an accelerating charge which obviously must have mass, that is radiation ala the particle. The accelerating charges are slow-moving electrons. The RF current moves at the speed of light in the (conductive) medium. Therefore, the RF current is associated with photons emitted by the electrons. Photons have zero rest mass and zero electric charge. Photons are the particles associated with RF waves. -- 73, Cecil, IEEE, OOTC, *http://www.w5dxp.com Cecil there you go again with the idea that zero mass and zero energy is something that can exist which some have termed as "photons" Point to the laws of nature that support that notion. At one time it was the same as a particle without mass. Presence science now state that particular particle does have mass which is why the World spent millions for the CERN project. Your technical expertise is built on the state of science 50 years ago and you are now building a castle on sand or excuses to justify your unwillingness to embrace change. It took 7 days to build the Universe by the initial expenditure of kinetic energy which embraces the laws of nature and the concept of a cycle or equilibrium. Remember the words" let there be light" which aligns with energy expenditure upon mass ie everything starts with the expenditure of energy upon or from mass it is not a chicken or egg analogy. And it is expenditure of energy upon mass that makes it a particle unconnected to all mass around it such that the particle is unbound and cannot be absorbed by another state. Lets face it, Adam and Eve knew nothing regarding equilibrium and the notion of frequency or period. All the work had been completed way belong that came upon the scene,, which is why religeon exists as the sole explanation of who and what was and is in charge with respect to the laws of nature. Again it is impossible for something to exist without mass. Art |
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"Tom Donaly" wrote in
: .... not be easy. Finally, a modest question: if you have EZNEC, why would you be wasting time with something inferior? The gold standard is the gold standard. NEC (in whatever form) might give a good estimate of the inductance of some helices, although many practical inductors require smaller segment lengths that would normally be advised for NEC models, but it does not provide a good loss estimate in many interesting cases. My post entitled was about that topic, and apart from Jim's suggestion of a sensitivity analysis, there was no solution to evaluating the effective resistance of an inductor of closely spaced turns (so proximity effect is signficant) made from a braided round conductor and with a thin dielectric jacket. All three of these factors are, as I understand it, not modelled in NEC-2. Owen |
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On Apr 23, 4:10*pm, Roy Lewallen wrote:
steveeh131047 wrote: . . . Now here's my problem: * The results I get using a model based on transmission-line analysis are very close to my EZNEC predictions - not perfect, but way better than any lumped-element analysis results * I don't see quantitative, non-empirical, arguments being put forward to support lumped-element analysis * I see numeric arguments being put forward by Cecil to support a transmission-line approach - they look convincing to me and, although I see a lot of unpleasant personal attacks on him, I don't see any scientific challenge to his figures * On the other hand I see folk whose work I rate highly, seemingly willfully to misunderstand some of the points which Cecil puts forward Please don't think I'm trying to defend Cecil - I wouldn't be so presumptuous, and anyway he's old enough to look after himself! I'm just trying to understand why, what seems to me to be such a persuasive argument, generates such opposition. Either there's some glaring technical error here which I haven't yet spotted, or perhaps there's a long "history" between various "personalities" of which I'm ignorant? Still confused, Steve G3TXQ Some of your questions can be answered by doing a google groups search of this newsgroup for the topic "Current in antenna coils controversy" in 2003. There are several other lengthy threads at later dates, such as "Current across the loading coil - from scratch", "Loading coils; was : Vincent antenna", "Standing-Wave Current vs Traveling-Wave Current", and a number of threads prior to 2003. Roy Lewallen, W7EL This is so wrong. The term "wave" is an adjective and a "particle" is a noun. An adjective is the enunciation of a function that describes a noun. Art |
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Cecil Moore wrote:
Jim Kelley wrote: ... and as any good dry labber knows, it's a dead giveaway to report a precision greater than one can actually measure. :-) I have reported no precision - my 100 MHz scope has not been calibrated since I retired. Precision is the number of sig figs. You "might" have calculated three, rounded up, and reported two. ac6xg |
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Roy Lewallen wrote:
I did and do support lumped element analysis for a very small toroidal loading inductor, and extensively posted the reasons why in this newsgroup about six years ago ("Current in antenna coils controversy", 2003). Cecil and Yuri were arguing that the coil would replace some number of "degrees of antenna" and its current therefore would have a substantial phase difference between input and output ends. I made and posted careful measurements to support my statement, after which Cecil invented his "standing wave current" and went off in various directions. I didn't invent "standing wave current". Standing wave current is what EZNEC displays for standing wave antennas. Standing wave current is what Kraus describes graphically on page 464, Figure 14-2, of "Antennas ...", 3rd edition. Standing wave current is what Ramo and Whinnery describe mathematically in "Fields and Waves ...". It has been at least 5 years since I explained why the phase of the current on a standing wave antenna cannot be used to determine the delay in a wire or in a coil. EZNEC, Kraus, Balanis, and Ramo and Whinnery all agree with me and disagree with you. I explained, 5 years ago, how the magnitude of the current can be used to calculate the delay through a coil. All my explanations fell on deaf ears and you called them gobblygook, or some such. Once again, most of the current in a standing wave antenna is of the form, I = Imax*cos(kx)*cos(wt) For any given time = t1, the phase of the current all up and down the antenna does not change with x. The phase is the same at the feedpoint, at the bottom of the coil, at the top of the coil, and at the top of the stinger. The phase of that current cannot be used to calculate delay in a wire or through a coil. You once said you were quick to admit a mistake. It has been 5+ years since you made that conceptual mistake and you have not admitted it yet. -- 73, Cecil, IEEE, OOTC, http://www.w5dxp.com |
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steveeh131047 wrote:
I see 1A at the base of the coil increasing to 1.07A at the centre of the coil and then dropping to 0.69A at the top of the coil. FYI Steve, five years ago I showed Roy how to estimate the phase shift through the coil using ARCSIN(0.69) = ~46 degrees. To this day, he refuses to acknowledge what EZNEC is telling him about current on a standing wave antenna which is: A current phase measurement on a standing wave antenna is meaningless. Here's a couple of graphic that illustrate what I am saying: http://www.w5dxp.com/coil.gif http://www.w5dxp.com/phasor.gif These graphs are very close to your measurements above. -- 73, Cecil, IEEE, OOTC, http://www.w5dxp.com |
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Art Unwin wrote:
Cecil there you go again with the idea that zero mass and zero energy is something that can exist which some have termed as "photons" Point to the laws of nature that support that notion. It's part of the standard model, Art, with which I am not about to disagree. http://en.wikipedia.org/wiki/Standard_Model -- 73, Cecil, IEEE, OOTC, http://www.w5dxp.com |
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On Apr 23, 4:36*pm, steveeh131047 wrote:
On Apr 23, 10:10*pm, Roy Lewallen wrote: Some of your questions can be answered by doing a google groups search of this newsgroup for the topic "Current in antenna coils controversy" in 2003. Roy, I've glanced at some of those references and it looks like there's years of "catch-up" reading for me :) It seems like the starting point for one of the earliest discussions was whether or not there is a variation in current amplitude along the length of a loading coil, with some pretty strong opinion saying that there isn't. I don't want to go over old ground, but perhaps you can give me a simple answer to this one question: When I use EZNEC to model a 6ft whip above a loading coil (40T, 6" diameter, 12" long), and look at the current distribution across the coil at the resonant frequency of the antenna (3.79 MHz), I see 1A at the base of the coil increasing to 1.07A at the centre of the coil and then dropping to 0.69A at the top of the coil. My question is: "Can I believe that I would see a similar current variation in the 'real world', or is this some failing of EZNEC to model the antenna properly?" Regards, Steve G3TXQ Steve. To determine the accuracy of Eznec first requires the use of a program with the ability to change input so that it relates to the requirements of Maxwell' radiation laws This means a program with an optimiser function which adheres strictly with Maxwells laws and its applicability produced which means all forces are accounted for. You have then established a datum line for a radiator where all forces are accounted for per Maxwell. When that final configuration per Maxwell' laws emerges one should be able to insert this same configuration into Eznec to check to see if all relative factors are the same as that provided by the program with optimizer abilities. Any differences that come about is a measurement of deviation from Maxwell's laws and thus its applicability. There are other programs that are available that are useable only for predetermined planar forms such as the Yagi where all forces are not accounted for such as the Corriollis effect i.e. that force is ignored thus Maxwells laws are not applicable. Regards Art Art |
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Jim Lux wrote:
Tom Donaly wrote: Finally, a modest question: if you have EZNEC, why would you be wasting time with something inferior? The gold standard is the gold standard. Perhaps more the silver or electrum standard. EZNEC doesn't do dielectric loading, for instance. (unless you get the Nec4 engine from Roy) And, it's a MoM code, so things not well represented by collections of wires aren't necessarily modeled well. Nothing is perfect, but which is better, EZNEC or the Cecil-Corum method of modeling antennas? 73, Tom Donaly, KA6RUH |
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Roy Lewallen wrote:
Tom Donaly wrote: There aren't many people who would support a lumped-element analysis on this newsgroup. Most people know the limitations of using network theory in these circumstances. The technical arguments against Cecil's approach were offered a long time ago. This latest is just a flareup that will soon die down. You shouldn't be confused. The transmission line model of antennas is well accepted and hoary with age, particularly for bi-conical antennas (see Schelkunoff). There are a couple of other types of models with equal validity. If you really want to know the physical score, though, you have to get an electromagnetics text that discusses the integral equations that govern antenna behavior. Pay particular attention to the parts that explain why numerical methods like EZNEC have to be used for solutions rather than the symbolic math most people would expect and want. 73, Tom Donaly, KA6RUH I did and do support lumped element analysis for a very small toroidal loading inductor, and extensively posted the reasons why in this newsgroup about six years ago ("Current in antenna coils controversy", 2003). Cecil and Yuri were arguing that the coil would replace some number of "degrees of antenna" and its current therefore would have a substantial phase difference between input and output ends. I made and posted careful measurements to support my statement, after which Cecil invented his "standing wave current" and went off in various directions. Roy Lewallen, W7EL I should have specified a large, solenoidal loading coil such as Cecil is so fond of using. Cecil has since eschewed his "degrees of antenna" position, but, for some reason, he keeps claiming your tests on the small solenoid were wrong. 73, Tom Donaly, KA6RUH |
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Owen Duffy wrote:
"Tom Donaly" wrote in : ... not be easy. Finally, a modest question: if you have EZNEC, why would you be wasting time with something inferior? The gold standard is the gold standard. NEC (in whatever form) might give a good estimate of the inductance of some helices, although many practical inductors require smaller segment lengths that would normally be advised for NEC models, but it does not provide a good loss estimate in many interesting cases. My post entitled was about that topic, and apart from Jim's suggestion of a sensitivity analysis, there was no solution to evaluating the effective resistance of an inductor of closely spaced turns (so proximity effect is signficant) made from a braided round conductor and with a thin dielectric jacket. All three of these factors are, as I understand it, not modelled in NEC-2. Owen So, what does model all the factors you mentioned, and how well does the Cecil-Corum method do in this regard? 73, Tom Donaly, KA6RUH |
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On Apr 23, 2:32*pm, Roy Lewallen wrote:
Jim Lux wrote: Roy Lewallen wrote: Let's see how well the principles involved are understood. What is the delay through a physically very small toroidal coil with the same inductance as the solenoidal coil? Why? As in a coil wound on a toroidal magnetic core? or a air cored solenoid bent in a circle? I'll say one wound on a magnetic core, simply to keep the size small, the coupling tight, and the field confined. I don't, however, care how long a piece of wire it's wound with. Roy Lewallen, W7EL There are some other configurations that I personally think are interesting to ponder. You might never actually build one this way, but you'll probably gain some insights considering it: an antenna, say a nominally 1/4 wave vertical for 40 meters made from 4" diameter aluminum tube (irrigation pipe) twenty feet long, resonated with a loading coil placed inside the tube across a gap of two or three inches in the pipe. Capacitance from the coil is almost entirely to the pipe in this case, not to the world outside the pipe, so the effect is capacitance in parallel with the coil, not as in a transmission line where the capacitance is to ground. That's a different situation than one where a coil with a diameter much larger than the antenna conductor is used, where the coil has significant capacitance to the outside world (e.g. to ground). It's also worth considering that the charge distribution on an antenna is dynamic, so it's probably not a good idea to try to analyze the antenna as if there was the same capacitance to ground from the coil as there would be if the charge distribution on the antenna wire were static (that is, the DC case, or at a frequency that's a tiny fraction of the lowest natural resonance of the antenna system). Analyzing exactly how even a simple wire antenna works in detail is far from trivial, and when you add in a coil that has significant physical size, it further complicates things. If you use a simplified model, it can be useful to gain insights into what's going on, but don't expect the details to be correct. Be wary about gaining insights that aren't actually true. Cheers, Tom |
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On Apr 23, 3:22*pm, Cecil Moore wrote:
Art Unwin wrote: You based your proof of a magnetic wave in a vacuum but it is an accelerating charge which obviously must have mass, that is radiation ala the particle. The accelerating charges are slow-moving electrons. The RF current moves at the speed of light in the (conductive) medium. Therefore, the RF current is associated with photons emitted by the electrons. Photons have zero rest mass and zero electric charge. Photons are the particles associated with RF waves. -- 73, Cecil, IEEE, OOTC, *http://www.w5dxp.com You are quoting the aproach of the bookswhere it is acknowledged that radiationn cannot fully be explained For me I am quoting an alternative that does provide the explanation. If current moves at the speed of light within the Universe ( the speed of light relative to Earth is slower which creates delay compared to the former. Insertion of Plank's constant I believe is a metric that represents the ratio of that delay) it imparts the same speed to a static particle when impacted, where the acceleration is determined by Newton's law u.t +f.t sq/2. Since the particle is static the "u.t" portion equals zero and f.t.sq/2 is the acceleration from zero to that of the speed of current of the particle, which is a measure of the expended kinetic energy that creates the initial format of radiation. I state again without mass there can be no acceleration.Period Regards Art |
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Roy Lewallen wrote:
Regards, Steve G3TXQ Yes, you would see this in the real world. EZNEC does a very good job of modeling a wire antenna with a loading coil, provided that you model the coil as a wire helix rather than lumped "load", and you can trust the results. As I've implied, a lumped load is quite a good model for a physically small, essentially non-radiating loading coil like a toroid on a magnetic core. Roy Lewallen, W7EL which makes perfect sense... NEC is a MoM code and is ideally suited to calculating the current induced in one wire by the currents in other wires. I should think it would do an excellent job modeling a air core solenoid, especially if the wire diameter is small compared to the spacing between turns,etc, assuming that you don't get into numerical precision problems. |
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"Art Unwin" wrote in message ... I state again and again, and again, adding bafflegab and gobbledygook with every iteration... I love it art, how much deeper can you go with this? |
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Roy Lewallen wrote:
Jim Lux wrote: Tom Donaly wrote: Finally, a modest question: if you have EZNEC, why would you be wasting time with something inferior? The gold standard is the gold standard. Perhaps more the silver or electrum standard. EZNEC doesn't do dielectric loading, for instance. (unless you get the Nec4 engine from Roy) All program types, including the demo, of EZNEC v. 4.0 and later do dielectric loading similar to NEC-4. (The method came from sources other than NEC-4.) Like the NEC-4 implementation, it's of limited accuracy and usefulness -- it's really good only for thin wire insulation of moderate permittivity. I stand corrected. Thanks. And, it's a MoM code, so things not well represented by collections of wires aren't necessarily modeled well. Absolutely true. And it can't handle things like patch antennas or antennas printed on a PCB. NEC does OK at microstrip patches with air dielectric (or foam with very low permittivity). I've used it to model an array of 9 patches and the port to port coupling calculated by NEC and measured by a VNA were pretty close (within measurement uncertainty). It's pretty darn slow at this, though (lots and lots of wires in each patch), I used lumped loads for the matching network model (capacitive probe feed) |
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Tom Donaly wrote:
Jim Lux wrote: Tom Donaly wrote: Finally, a modest question: if you have EZNEC, why would you be wasting time with something inferior? The gold standard is the gold standard. Perhaps more the silver or electrum standard. EZNEC doesn't do dielectric loading, for instance. (unless you get the Nec4 engine from Roy) And, it's a MoM code, so things not well represented by collections of wires aren't necessarily modeled well. Nothing is perfect, but which is better, EZNEC or the Cecil-Corum method of modeling antennas? Depends on what your modeling needs are. NEC and it's ilk are more generalized, but take more computational effort. The Corums have an analytical approximation that is reasonably good for a certain class of configurations, although I have to say that for the original Corum application of Tesla Coils, a lumped approximation gets you almost as close, at much less work, considering the usual construction tolerances in a tesla coil. Modern Tesla Coil modeling is typically done with either a lumped model or a FEM code that assumes it's axially symmetric and often an assumed voltage distribution. The assumed distribution the result of a combination of more detailed analytical modeling and some experimental measurements on real coils, and speeds up the computation drastically, while not adversely affecting the accuracy of the results (that is, the changes are less than a few percent, comparable to construction tolerances on these things). 73, Tom Donaly, KA6RUH |
Loading coils: was Dish reflector
Tom Donaly wrote:
Nothing is perfect, but which is better, EZNEC or the Cecil-Corum method of modeling antennas? EZNEC and the Cecil-Corum method are in agreement. How would you measure the delay through a wire or through a coil using the following current reported by EZNEC through a 90 degree monopole? EZNEC+ ver. 4.0 thin-wire 1/4WL vertical 4/23/2009 8:01:44 PM --------------- 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 Exactly how does one use a current that changes phase by 2.71 degrees in 90 degrees of antenna to obtain the delay through anything? Your silence on this subject speaks volumes. -- 73, Cecil, IEEE, OOTC, http://www.w5dxp.com |
Loading coils: was Dish reflector
Tom Donaly wrote:
I should have specified a large, solenoidal loading coil such as Cecil is so fond of using. Cecil has since eschewed his "degrees of antenna" position, but, for some reason, he keeps claiming your tests on the small solenoid were wrong. Yes, I have fine-tuned my concepts over the past 5 years. What rational person would not adjust their concepts to match the technical evidence? (It's a rhetorical question. We all know who refuses to do that.) Roy's tests were wrong in the sense that they were meaningless no matter how accurate the readings. Quoting my web page: "All of the reported conclusions based on loading coil measurements using the current on standing-wave antennas are conceptually flawed." -- 73, Cecil, IEEE, OOTC, http://www.w5dxp.com |
Loading coils: was Dish reflector
On Apr 23, 6:59*pm, K7ITM wrote:
On Apr 23, 2:32*pm, Roy Lewallen wrote: Jim Lux wrote: Roy Lewallen wrote: Let's see how well the principles involved are understood. What is the delay through a physically very small toroidal coil with the same inductance as the solenoidal coil? Why? As in a coil wound on a toroidal magnetic core? or a air cored solenoid bent in a circle? I'll say one wound on a magnetic core, simply to keep the size small, the coupling tight, and the field confined. I don't, however, care how long a piece of wire it's wound with. Roy Lewallen, W7EL There are some other configurations that I personally think are interesting to ponder. *You might never actually build one this way, but you'll probably gain some insights considering it: *an antenna, say a nominally 1/4 wave vertical for 40 meters made from 4" diameter aluminum tube (irrigation pipe) twenty feet long, resonated with a loading coil placed inside the tube across a gap of two or three inches in the pipe. *Capacitance from the coil is almost entirely to the pipe in this case, not to the world outside the pipe, so the effect is capacitance in parallel with the coil, not as in a transmission line where the capacitance is to ground. *That's a different situation than one where a coil with a diameter much larger than the antenna conductor is used, where the coil has significant capacitance to the outside world (e.g. to ground). It's also worth considering that the charge distribution on an antenna is dynamic, so it's probably not a good idea to try to analyze the antenna as if there was the same capacitance to ground from the coil as there would be if the charge distribution on the antenna wire were static (that is, the DC case, or at a frequency that's a tiny fraction of the lowest natural resonance of the antenna system). Analyzing exactly how even a simple wire antenna works in detail is far from trivial, and when you add in a coil that has significant physical size, it further complicates things. *If you use a simplified model, it can be useful to gain insights into what's going on, but don't expect the details to be correct. *Be wary about gaining insights that aren't actually true. Cheers, Tom Tom you are correct in not making a descision on the basis of one observation but consideration of all the observable facts. The analogy of this is only with the use of alln segtments of a jigsaw puzzle can there be confidance of the ensuing picture. Roy stated that his conclusion was only based on one observable and where his statement said he did not care beyond that single observable which matched a predetermined picture. An accurate production of the ensuing picture comes about only with a matching relationship between all the parts of the jigsaw and certainly not based on the visual of one. Your last sentence speaks volumes regarding Roy;'s responce Regards Art |
Loading coils: was Dish reflector
Jim Lux wrote:
Roy Lewallen wrote: Absolutely true. And it can't handle things like patch antennas or antennas printed on a PCB. NEC does OK at microstrip patches with air dielectric (or foam with very low permittivity). I've used it to model an array of 9 patches and the port to port coupling calculated by NEC and measured by a VNA were pretty close (within measurement uncertainty). Yes, I meant patch antennas with common dielectrics, which are far more common. It's of course the dielectric that NEC can't account for. I've designed quite a few antennas on PCB material, but use a fudge factor based on comparison between measured and EZNEC results of a simple antenna near the same frequency. This gets me pretty close, but even this approach wouldn't be adequate if field coupling through the dielectric is significant. It's pretty darn slow at this, though (lots and lots of wires in each patch), I used lumped loads for the matching network model (capacitive probe feed) For large models, calculation time goes up as the cube of the number of segments, so big models can get slow all right. However, EZNEC has undergone a pretty dramatic speed improvement over time as various code substitutions and updated compilers have been used, and it's much, much faster than older NEC compilations. And some versions of NEC have been similarly updated, so people using different NEC compilations can experience pretty different calculation speeds. Roy Lewallen, W7EL |
Loading coils: was Dish reflector
On Apr 23, 7:42*pm, "Dave" wrote:
"Art Unwin" wrote in message ... I state again and again, and again, adding bafflegab and gobbledygook with every iteration... I love it art, how much deeper can you go with this? Well I am following the laws of physics. Since you were asleep during part of the lecture When the examination comes along you can only rely on baffle gab rather than ALLthe facts given during the lecture. Fortunately, one can graduate by providing some incorrect answers up to a limit where as total attention is the only route to a 100 percent score. You would be wise to accept that your knowledge on physics is not totally without error because of the baffle gab that you provided instead Regards Art |
Loading coils: was Dish reflector
On Apr 23, 7:49*pm, Jim Lux wrote:
Tom Donaly wrote: Jim Lux wrote: Tom Donaly wrote: Finally, a modest question: if you have EZNEC, why would you be wasting time with something inferior? The gold standard is the gold standard. Perhaps more the silver or electrum standard. EZNEC doesn't do dielectric loading, for instance. (unless you get the Nec4 engine from Roy) And, it's a MoM code, so things not well represented by collections of wires aren't necessarily modeled well. Nothing is perfect, but which is better, EZNEC or the Cecil-Corum method of modeling antennas? Depends on what your modeling needs are. *NEC and it's ilk are more generalized, but take more computational effort. *The Corums have an analytical approximation that is reasonably good for a certain class of configurations, although I have to say that for the original Corum application of Tesla Coils, a lumped approximation gets you almost as close, at much less work, considering the usual construction tolerances in a tesla coil. *Modern Tesla Coil modeling is typically done with either a lumped model or a FEM code that assumes it's axially symmetric and often an assumed voltage distribution. The assumed distribution the result of a combination of more detailed analytical modeling and some experimental measurements on real coils, and speeds up the computation drastically, while not adversely affecting the accuracy of the results (that is, the changes are less than a few percent, comparable to construction tolerances on these things). 73, Tom Donaly, KA6RUH You are correct in pointing out that a Tesla coil is a lumped inductance. A "preponderance" of a lumped load disqualifies the use of Maxwell's statements The only metrics he supplied to justify the presence of equilibrium were distributed loads and no more. Regards Art |
Loading coils: was Dish reflector
On Apr 23, 7:40*pm, Jim Lux wrote:
Roy Lewallen wrote: Regards, Steve G3TXQ Yes, you would see this in the real world. EZNEC does a very good job of modeling a wire antenna with a loading coil, provided that you model the coil as a wire helix rather than lumped "load", and you can trust the results. As I've implied, a lumped load is quite a good model for a physically small, essentially non-radiating loading coil like a toroid on a magnetic core. Roy Lewallen, W7EL which makes perfect sense... NEC is a MoM code and is ideally suited to calculating the current induced in one wire by the currents in other wires. I should think it would do an excellent job modeling a air core solenoid, especially if the wire diameter is small compared to the spacing between turns,etc, assuming that you don't get into numerical precision problems. If eznec does not take into account dielectric loading then the application is not in equilibrium and thus Maxwells laws are not applicable. Maxwells laws are based solely on the presence of equilibrium or accountability of all loads applied which when all are added equals zero per Newtons laws. Regards Art |
Loading coils: was Dish reflector
On Apr 23, 8:43*pm, Roy Lewallen wrote:
Jim Lux wrote: Roy Lewallen wrote: Absolutely true. And it can't handle things like patch antennas or antennas printed on a PCB. NEC does OK at microstrip patches with air dielectric (or foam with very low permittivity). *I've used it to model an array of 9 patches and the port to port coupling calculated by NEC and measured by a VNA were pretty close (within measurement uncertainty). Yes, I meant patch antennas with common dielectrics, which are far more common. It's of course the dielectric that NEC can't account for. I've designed quite a few antennas on PCB material, but use a fudge factor based on comparison between measured and EZNEC results of a simple antenna near the same frequency. This gets me pretty close, but even this approach wouldn't be adequate if field coupling through the dielectric is significant. Exactly. Maxwells law application is solely on the condition of all forces be accounted for such that the summation is equal zero. Omission of consideration of a force that is present prevents the summation from equaling zero which means the creation of an error. Very simple my dear Watson. This is tantamount to creating an abitrary border where one omits recording the full amount of flux created. Regards Art It's pretty darn slow at this, though (lots and lots of wires in each patch), I used lumped loads for the matching network model (capacitive probe feed) For large models, calculation time goes up as the cube of the number of segments, so big models can get slow all right. However, EZNEC has undergone a pretty dramatic speed improvement over time as various code substitutions and updated compilers have been used, and it's much, much faster than older NEC compilations. And some versions of NEC have been similarly updated, so people using different NEC compilations can experience pretty different calculation speeds. Roy Lewallen, W7EL |
Loading coils: was Dish reflector
K7ITM wrote:
On Apr 23, 2:32 pm, Roy Lewallen wrote: Jim Lux wrote: Roy Lewallen wrote: Let's see how well the principles involved are understood. What is the delay through a physically very small toroidal coil with the same inductance as the solenoidal coil? Why? As in a coil wound on a toroidal magnetic core? or a air cored solenoid bent in a circle? I'll say one wound on a magnetic core, simply to keep the size small, the coupling tight, and the field confined. I don't, however, care how long a piece of wire it's wound with. Roy Lewallen, W7EL There are some other configurations that I personally think are interesting to ponder. You might never actually build one this way, but you'll probably gain some insights considering it: an antenna, say a nominally 1/4 wave vertical for 40 meters made from 4" diameter aluminum tube (irrigation pipe) twenty feet long, resonated with a loading coil placed inside the tube across a gap of two or three inches in the pipe. Capacitance from the coil is almost entirely to the pipe in this case, not to the world outside the pipe, so the effect is capacitance in parallel with the coil, not as in a transmission line where the capacitance is to ground. That's a different situation than one where a coil with a diameter much larger than the antenna conductor is used, where the coil has significant capacitance to the outside world (e.g. to ground). It's also worth considering that the charge distribution on an antenna is dynamic, so it's probably not a good idea to try to analyze the antenna as if there was the same capacitance to ground from the coil as there would be if the charge distribution on the antenna wire were static (that is, the DC case, or at a frequency that's a tiny fraction of the lowest natural resonance of the antenna system). Analyzing exactly how even a simple wire antenna works in detail is far from trivial, and when you add in a coil that has significant physical size, it further complicates things. If you use a simplified model, it can be useful to gain insights into what's going on, but don't expect the details to be correct. Be wary about gaining insights that aren't actually true. Cheers, Tom I didn't do exactly as you say, Tom, but I did take a homemade coil (140mm long, 155mm in diameter) and wrapped it with a sheet of .005 inch copper foil separated by a couple of strips of double sided foam tape. It acted more like a transmission line than the bare coil, but it had some peculiarities that made its behavior puzzling to say the least. 73, Tom Donaly, KA6RUH |
Loading coils: was Dish reflector
On Apr 23, 8:04*pm, Cecil Moore wrote:
Tom Donaly wrote: Nothing is perfect, but which is better, EZNEC or the Cecil-Corum method of modeling antennas? EZNEC and the Cecil-Corum method are in agreement. Correct but the solution is in error as equilibrium demands that the radiator is in equilibrium ie equal to a period or multiples there of. Both of the above determined that resonance alone without reference to the period was a reflection of equilibrium. This may account for Krauss's error in determiming gain via Maxwells law by determining a half wave was in equilibrium and thus determined gain was approx 3db more than that was actually attainable. Later measurements mad by others show that Kraus over estimated the gain by 100 % the equivalent of 3db or the doubling of gain or energy expenditure.This error is actually a reflection of pitch of windings which is a fraction of the possible generated electric field for maximum efficiency. Lesson One must account for all actual vectors used within a boundary for equilibrium where the addition of all vectors finish at the starting point of the period. The idea that a coil does not radiate is fallacious since the charge is still accelerating but to a lesser extent than when current moves along a straight wire. The total velocity factor is the average velocity of that of a slow wave plus the velocity without the addition of lumped loads ie straight radiator addition.This being equal to the total length of wire required with tha absence of lumped loading ie straight. Regards Art -- 73, Cecil, IEEE, OOTC, *http://www.w5dxp.com |
Loading coils: was Dish reflector now: Delay Lines
"Jim Kelley" wrote in message
... For a more quantitative illustration of how distributed reactance in transmission lines causes delay see http://www.rhombus-ind.com/dlcat/app1_pas.pdf 73, ac6xg In graduate school, more years ago than I care to admit, I scrapped a surplus computer for parts. The computer had been custom built for the Savannah River nuclear facility. In addition to the many hundreds of 2N404A germanium transistors, I found the core memory made of ferrite cores about 0.1 inches in diameter and about 30 mils thick. But the most unusual thing, at least to me, was a flexible coaxial cable about six feet long made of a ferrite-loaded rubber core wound with 40 gauge enameled wire, wrapped in a thin cellulose acetate film (Scotch tape?), covered with a braid shield with a vinyl covering. Of course, it was a distributed delay line. I never measured its impedance and delay properties accurately, but the cable had a significant delay that could easily be seen on a 5 MHz bandwidth scope. Even with an approximate termination, the cable's losses were quite high. This was obviously a commercial cable, but in all of the years since, I have never seen anything like it. By the way, after dismantling one panel covered with terminal strips, I found a typed note inside that said, "Built by pigmies in darkest Africa." -- 73, Dr. Barry L. Ornitz WA4VZQ |
Loading coils: was Dish reflector
On Thu, 23 Apr 2009 15:29:04 -0700, Jim Kelley
wrote: Cecil Moore wrote: Jim Kelley wrote: ... and as any good dry labber knows, it's a dead giveaway to report a precision greater than one can actually measure. :-) I have reported no precision - my 100 MHz scope has not been calibrated since I retired. Precision is the number of sig figs. You "might" have calculated three, rounded up, and reported two. Precision is NOT accuracy. Resolution is NOT precision. Accuracy is defined with precision to a resolution. You can state a value with great precision and be 100% in error. 100 V is quite precise; "about" 100 V is less precise. 100 V has three places of resolution. If the true value is actually 201.45 V then 100 V is precise, somewhat resolved, but inaccurate. On the other hand, 201.45 V is very precise, highly resolved, and accurate to within 0.005 V (if we are to trust it as a reference) or 25 parts per million. I can anticipate the objection (to confound my statement above) that 100 V has both resolution and precision. True, but that objection would miss the point. Some standards are nominal (or cardinal) values such as an 1 MHz URQ-23 frequency standard: 1 place of resolution, but highly precise with an accuracy of (from my experience) of 6 parts per trillion (after calibration against a cesium beam standard). I can anticipate the fine objection that the nominal value of 1 is actually 1.00000000000. Again, true, but in a world where you own an URQ-23 (and no one has access to HP 5071 cesium clocks), then you get to snub that objection and demand: "It IS exactly 1!" 73's Richard Clark, KB7QHC |
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