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#21
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On Mon, 30 Apr 2007 06:37:10 -0500, "amdx" wrote:
Are you exploring an intellectual curiosity or trying to remedy a defect in application? No, I just have experienced the effect that Bill ask about and gave my own pet theory about why it happens. Now I'm looking for a little confirmation or where I went wrong. Hi Mike, Well, that is fine and good, but neither of you have given us any real data, and certainly no Q values to judge if what you both experienced was within the range of "normal" or out in left field. RF measurements are difficult to do to any particularly fine accuracy, and what was observed may have been simple variation due to the measurer's proximity (offering just one of many things that can go wrong). Loss still remains the province of resistance. Richard, That's like saying rain has water in it. No matter how many times you say it, I'm still going to agree with you. Then this diverges from Bill's premise of Capacitance being the source of loss and you and he are separable at this point of your common experience. Your best argument is that Capacitance exacerbates loss. I would rephrase that as "interwinding capacitance exacerbates loss". And with that, you have summed up my argument perfectly. You have helped reduce my argument to 4 words. Now, do you agree that interwinding capacitance will reduce Q? (yes, I know it's the province of resistance) Give me some metrics to show it is not skin effect. The issue at hand is your (both you and Bill, or either of you separately) loops keep changing to fit to the loss rather than to the application. It makes for a rather strained progression of design as loops are added, proximity becomes a greater issue, as coil length collapses, insulation is added, and as frequency shifts to follow these changes. It is as though a good 10M loop is evolving to operate poorly there or, worse, in the 160M band where its resonance has finally come to rest through optimizing for loss. I can imagine there being enough turn-to-turn capacitance to induce large currents, but so many correlating factors would have to ride along with this that they could easily eclipse that contribution of loss. In other words, it seems the goal of your argument is to raise that capacitance, which by ordinary means has you drawing the loops together (insulated or not). This compounds the skin effect and for a constant frequency demands a lower inductance. The lower inductance, in turn, then demands a smaller coil which forces a lower Radiation resistance. A smaller coil (to again follow the demand for more Capacitance) drives closer loops. It seems like this is in an infinite regress. 73's Richard Clark, KB7QHC |
#22
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![]() "Richard Clark" wrote in message ... On Mon, 30 Apr 2007 06:37:10 -0500, "amdx" wrote: Are you exploring an intellectual curiosity or trying to remedy a defect in application? No, I just have experienced the effect that Bill ask about and gave my own pet theory about why it happens. Now I'm looking for a little confirmation or where I went wrong. Hi Mike, Well, that is fine and good, but neither of you have given us any real data, and certainly no Q values to judge if what you both experienced was within the range of "normal" or out in left field. RF measurements are difficult to do to any particularly fine accuracy, and what was observed may have been simple variation due to the measurer's proximity (offering just one of many things that can go wrong). Yes, RF measurements are difficult to do to any particularly fine accuracy. And I claim no great knowledge of how to minimize errors or even how to recognize where they come from. Loss still remains the province of resistance. Richard, That's like saying rain has water in it. No matter how many times you say it, I'm still going to agree with you. Then this diverges from Bill's premise of Capacitance being the source of loss and you and he are separable at this point of your common experience. Your best argument is that Capacitance exacerbates loss. I would rephrase that as "interwinding capacitance exacerbates loss". And with that, you have summed up my argument perfectly. You have helped reduce my argument to 4 words. Now, do you agree that interwinding capacitance will reduce Q? (yes, I know it's the province of resistance) Give me some metrics to show it is not skin effect. The issue at hand is your (both you and Bill, or either of you separately) loops keep changing to fit to the loss rather than to the application. It makes for a rather strained progression of design as loops are added, proximity becomes a greater issue, as coil length collapses, insulation is added, and as frequency shifts to follow these changes. It is as though a good 10M loop is evolving to operate poorly there or, worse, in the 160M band where its resonance has finally come to rest through optimizing for loss. My experience is limited to winding small inductors rather than loop antennas. I can imagine there being enough turn-to-turn capacitance to induce large currents, but so many correlating factors would have to ride along with this that they could easily eclipse that contribution of loss. In other words, it seems the goal of your argument is to raise that capacitance, which by ordinary means has you drawing the loops together (insulated or not). This compounds the skin effect and for a constant frequency demands a lower inductance. The lower inductance, in turn, then demands a smaller coil which forces a lower Radiation resistance. A smaller coil (to again follow the demand for more Capacitance) drives closer loops. It seems like this is in an infinite regress. I don't understand why you think we want more interwinding capacitance, We want less. I will agree that the mechanics involved in trying to reduce interwinding capacitance will probably reduce proximity effects and so to seperate out any affect from the reduces interwinding capacitance would be difficult. I need to go, Later, thanks Richard |
#23
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![]() "amdx" wrote in message ... "Richard Clark" wrote in message ... On Mon, 30 Apr 2007 06:37:10 -0500, "amdx" wrote: Are you exploring an intellectual curiosity or trying to remedy a defect in application? No, I just have experienced the effect that Bill ask about and gave my own pet theory about why it happens. Now I'm looking for a little confirmation or where I went wrong. Hi Mike, Well, that is fine and good, but neither of you have given us any real data, and certainly no Q values to judge if what you both experienced was within the range of "normal" or out in left field. RF measurements are difficult to do to any particularly fine accuracy, and what was observed may have been simple variation due to the measurer's proximity (offering just one of many things that can go wrong). Yes, RF measurements are difficult to do to any particularly fine accuracy. And I claim no great knowledge of how to minimize errors or even how to recognize where they come from. Loss still remains the province of resistance. Richard, That's like saying rain has water in it. No matter how many times you say it, I'm still going to agree with you. Then this diverges from Bill's premise of Capacitance being the source of loss and you and he are separable at this point of your common experience. Your best argument is that Capacitance exacerbates loss. I would rephrase that as "interwinding capacitance exacerbates loss". And with that, you have summed up my argument perfectly. You have helped reduce my argument to 4 words. Now, do you agree that interwinding capacitance will reduce Q? (yes, I know it's the province of resistance) Give me some metrics to show it is not skin effect. The issue at hand is your (both you and Bill, or either of you separately) loops keep changing to fit to the loss rather than to the application. It makes for a rather strained progression of design as loops are added, proximity becomes a greater issue, as coil length collapses, insulation is added, and as frequency shifts to follow these changes. It is as though a good 10M loop is evolving to operate poorly there or, worse, in the 160M band where its resonance has finally come to rest through optimizing for loss. My experience is limited to winding small inductors rather than loop antennas. I can imagine there being enough turn-to-turn capacitance to induce large currents, but so many correlating factors would have to ride along with this that they could easily eclipse that contribution of loss. In other words, it seems the goal of your argument is to raise that capacitance, which by ordinary means has you drawing the loops together (insulated or not). This compounds the skin effect and for a constant frequency demands a lower inductance. The lower inductance, in turn, then demands a smaller coil which forces a lower Radiation resistance. A smaller coil (to again follow the demand for more Capacitance) drives closer loops. It seems like this is in an infinite regress. I don't understand why you think we want more interwinding capacitance, We want less. I will agree that the mechanics involved in trying to reduce interwinding capacitance will probably reduce proximity effects and so to seperate out any affect from the reduces interwinding capacitance would be difficult. I need to go, Later, thanks Richard Ok, I'm back. Richard, I was starting to lean towards proximity effect possibly causing all of the affect we have been discussing, so I did some Googling. I kept find the same line " increased capacitance lowers Q" But, I think you agree that as I said above most efforts to reduce capacitance will also reduce proximity effect. I ran across W8JI's page, he's usually pretty exacting in his wording, and he says, "Capacitance across any inductor carrying time-varying current increases circulating currents in the inductor, increasing loss while simultaneously reducing system bandwidth." snip "Anything that increases capacitance will reduce component Q" He never mentions the correlation between interwinding capacitance and proximity effect These line were taken from; http://www.w8ji.com/loading_inductors.htm What do you think? Mike |
#24
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On Mon, 30 Apr 2007 18:30:40 -0500, "amdx" wrote:
Richard, I was starting to lean towards proximity effect possibly causing all of the affect we have been discussing, so I did some Googling. I kept find the same line " increased capacitance lowers Q" But, I think you agree that as I said above most efforts to reduce capacitance will also reduce proximity effect. Hi Mike, Yup. I ran across W8JI's page, he's usually pretty exacting in his wording, and he says, "Capacitance across any inductor carrying time-varying current increases circulating currents in the inductor, increasing loss while simultaneously reducing system bandwidth." Tom is also given to non-sequiturs. He polishes his page off with a list of them such as "Optimum form factor varies with application." As they used to say, if you want to send a message, call Western Union. snip "Anything that increases capacitance will reduce component Q" He never mentions the correlation between interwinding capacitance and proximity effect There is not much that can be taken to the bank about what is NOT said. The moral of this is standard Engineering practice: start with a goal and design towards it. 73's Richard Clark, KB7QHC |
#25
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On Apr 29, 4:52 am, "amdx" wrote:
"Bill Bowden" wrote in message oups.com... Does anyone know why the distributed winding capacitance of a loop antenna, or any inductor, degrades the efficiency? -Bill Hi Bill. I agree with your assertion that distributed winding capacitance degrades efficiency. My thoughts about this are ; Assume a 10 turn loop, between each turn there is a capacitance, so, you have a complete circuit, (L,C,R) there is current flowing through this circuit that is not flowing through the entire 10 turn loop. (this happens in the other 9 turns also) I think these extra currents flowing that don't make the entire 10 turn circuit increase the losses. Anyone care to run with that, or explain it more clearly, or shoot it down. Mike I think you are right. Good explanation. -Bill |
#26
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![]() "Bill Bowden" wrote in message ups.com... On Apr 29, 4:52 am, "amdx" wrote: "Bill Bowden" wrote in message oups.com... Does anyone know why the distributed winding capacitance of a loop antenna, or any inductor, degrades the efficiency? -Bill Hi Bill. I agree with your assertion that distributed winding capacitance degrades efficiency. My thoughts about this are ; Assume a 10 turn loop, between each turn there is a capacitance, so, you have a complete circuit, (L,C,R) there is current flowing through this circuit that is not flowing through the entire 10 turn loop. (this happens in the other 9 turns also) I think these extra currents flowing that don't make the entire 10 turn circuit increase the losses. Anyone care to run with that, or explain it more clearly, or shoot it down. Mike I think you are right. Good explanation. -Bill Well Bill, That has been the theory I've been thinking with for 8 or 9 years now. However, if as Richard suggests the phenomena is caused by proximity effect, the techniques I used to lower interwinding capacitance and raise Q, would be the same I'd use to reduce proximity efect and raise Q. If there are circuilating currents caused by interwinding capacitance, it seems they would cause the proximity effect to be even stronger and pinch down the current flow area even more and raise losses. A question for all, Does a basketweave winding reduce proximity effect? Mike |
#27
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Bill Bowden wrote:
"Does anyone know why the distributed winding capacitance of a loop antenna, or any inductor, degrades the efficiency?" I`ll speculate that current to build the magnetic field and the current required to charge the stray capacitance of the inductor occur at different times. The magnetic field is the source of self-inductance of the coil, but the displacemnt current in the stray capactance is gratuitous and only adds loss to the coil. Best regards, Richard Harrison, KB5WZI |
#28
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Distributed capacitance may affect single-turn coils differently from
multiturn-coils. And those vary as their length to diameter ratio varies. Mike wrote: "Anything that increases capacitance will reduce component Q. I believe he was quoting W8JI. Mike also wrote: "What do you think?" In 1999 Tom Bruhns was experimenting, trying to find the relationship between coil Q and parasitic C. He picked up reports that helical resonators weere superior to short coaxial resonators. Tom also wrote: "Reg (Edwards,RJE) then thinks the internal coil capacitance is just femanding extra extra coil current and loss as the result of its cyclic charge and discharge." Reg seems to have had a nice explanation for coil loss from parasitic capacitance. Best regards, Richard Harrison, KB5WZI |
#29
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![]() "Richard Harrison" wrote in message ... Distributed capacitance may affect single-turn coils differently from multiturn-coils. And those vary as their length to diameter ratio varies. Mike wrote: "Anything that increases capacitance will reduce component Q. I believe he was quoting W8JI. Mike also wrote: "What do you think?" In 1999 Tom Bruhns was experimenting, trying to find the relationship between coil Q and parasitic C. He picked up reports that helical resonators weere superior to short coaxial resonators. Tom also wrote: "Reg (Edwards,RJE) then thinks the internal coil capacitance is just femanding extra extra coil current and loss as the result of its cyclic charge and discharge." Reg seems to have had a nice explanation for coil loss from parasitic capacitance. Do you know where this explanation might be found? Thanks, Mike |
#30
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amdx wrote:
Do you know where this explanation might be found? From "Current through coils", March 5, 2006 2:47pm Looks like Reg originated this thread. "Every coil has length. Both L and C are distributed. Therefore the coil behaves as a transmission line. There are standing waves. Current and voltage both vary with length." And on March 9: "The whole thing could be summarised in one short sentence - 'Coils are distributed transmission lines.' The same general equations apply to coils of all dimensions, for any number of turns, at all frequencies, in all applications. There's no need to unnecessarily complicate things by artificially dividing them into lumped and other varieties." -- 73, Cecil http://www.w5dxp.com |
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