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#111
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Yuri Blanarovich wrote:
Experiment #1: I will drive DC current through the coil in order to generate heat and observe the temperatures across the coil. Any problems with that? Of course there's a problem with that, Yuri. You absolutely must use a "physically small" coil so the gurus will be right. :-) -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#112
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While I normally can see your point, even if I disagree with your
conclusions. In this case Cecil, your just plain wrong! "Cecil Moore" wrote in message Thanks for the tips, Wes, and it does work. The names of the .EZ files are on the .gif graphic that I prepared which illustrates the current magnitudes and phases for 3/2WL phased arrays. http://www.qsl.net/w5dxp/phasesbw.gif -- 73, Cecil, W5DXP -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#113
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Art Unwin KB9MZ wrote:
Did you find something wrong with my suggestion above? Nope, nothing "wrong". I just avoid making assertions when I'm not 95% certain that I am correct. Thus, most of the time, I am unresponsive. I am 95% certain that the average humongous mobile loading coil is not "physically small" and is more like a certain percentage of a helical antenna which indeed does obviously demonstrate a net current gradient. -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#114
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Wes Stewart wrote:
wrote: |A quick scan of your article produces nothing new. Fine. Then this thread is closed. I apologize, Wes. After closer inspection, I have to disagree with myself. Imax is the reference zero degree point for the "cosine rule". If that point occurs inside the loading coil, then the number of degrees occupied by the loading coil becomes ArcCos(Iin/Imax) + ArcCos(Iout/Imax) This helps to resolve the problem I was having with ArcCos(Iout/Iin). If, as you say, the current maximum point occurs inside the coil, then the forward current and reflected current are in-phase inside the coil and the coil occupies much more of the antenna than ArcCos(Iout/Imax) I do believe a "Thank you very much" is in order. For your antenna, the calculated degrees that the coil occupies is within 1.5 degrees of the estimated degrees. -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#115
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W4JLE wrote:
While I normally can see your point, even if I disagree with your conclusions. In this case Cecil, your just plain wrong! Would you mind telling me what I am wrong about? I presently have no clue. I freely admit to being wrong about what the stock market has done this year. Is that what you are talking about? -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#116
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Richard Clark wrote,
On 31 Jan 2004 19:32:18 GMT, (Tdonaly) wrote: I have to eschew Gesundheit Thank you. |
#117
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Where do I begin...
To limit the universe, I disagree with the data referenced on your web page purporting to show how EZNEC got it wrong. Your just plain wrong. "Cecil Moore" wrote in message ... W4JLE wrote: While I normally can see your point, even if I disagree with your conclusions. In this case Cecil, your just plain wrong! Would you mind telling me what I am wrong about? I presently have no clue. I freely admit to being wrong about what the stock market has done this year. Is that what you are talking about? -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#118
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W4JLE wrote:
Where do I begin... To limit the universe, I disagree with the data referenced on your web page purporting to show how EZNEC got it wrong. Your just plain wrong. I am not trying to be hardnosed about this. I am actually trying to be gentle about challenging someone's religion. If an inductive stub is properly modeled by EZNEC, why is an equivalent inductive coil not properly modeled? By properly modeled, I mean in agreement with reality. EZNEC assumes that the current travels through the lumped inductive reactance at faster than the speed of light. Why is it surprising to find out that doesn't match reality? What am I missing, besides religion based on math models? -- 73, Cecil http://www.qsl.net/w5dxp -----= Posted via Newsfeeds.Com, Uncensored Usenet News =----- http://www.newsfeeds.com - The #1 Newsgroup Service in the World! -----== Over 100,000 Newsgroups - 19 Different Servers! =----- |
#119
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Here's a post of mine from the thread titled 'colinear connundrum'
from a few years ago. Perhaps it will shed some light on the subject : Gray Frierson Haertig wrote: "One of the classic implementations of the collinear uses parallel resonant circuits as the phase inverting means between separate elements---." I`ve discussed the if and how a parallel resonant circuit can replace a short-circuit 1/4-wave stub as a phase inverter, and never been satisfied either. If considered as two terminal devices, a 1/4 wl stub, parallel resonant LC circuit and an insulator are equivalent, at least for steady state AC. Understanding the difference requires a slightly more elaborate model for the stub or LC circuit. The model must account for charge accumulation, or common mode current on the device. Classic network theory can be used if a third, or 'common mode center tap' is added to the device model. Consider the parallel resonant LC circuit with the center of the inductor (or capacitor) grounded. The impedance between the two 'hot' terminals will be very high as in the two terminal case. The ground connection introduces a new constraint. The voltage on a 'hot' terminal is now constrained to be equal in magnitude and of opposite polarity from the other 'hot' terminal. This is not the case for the two terminal device model. The three terminal device (center tap grounded) can be used as a polarity reversing 1:1 transformer by connecting one 'hot' terminal to a ground referenced source and driving a load with the other terminal. Of course the same effect could be accomplished without the capacitor if the center tapped inductor (autotransformer) had suitable properties. Note that if the two 'hot' terminals are shorted the impedance (common mode) to ground is zero. Observe: The differential mode impedance between 'hot' terminals is very high (ideally infinite). The common mode impedance to ground is zero. The voltage on the 'hot' terminals respect to ground is of equal magnitude and opposite polarity. But, as Gray noted, a perfect parallel resonant circuit is an insulator. So is the perfect short-circuit 1/4-wave stub. Now look at a 1/4 wl shorted stub far removed from ground. Viewed as a two terminal device it behaves similar to a parallel resonant LC circuit. If the two open 'hot' wires are shorted, the stub looks like a 1/4 wl long wire. The impedance with respect to ground is approximately 36 ohms, which is very small compared to the nearly infinite differential impedance. Think of it as a single 1/4 wl counterpoise; adding a second colinear 'radial' results in an even lower ( 36/2 ohms) 'virtual ground' impedance. Thus the 1/4 wl stub behaves similar to the parallel resonant LC circuit with the grounded center tap. The common mode behavior of the freespace 1/4 wl stub provides the low impedance 'virtual ground'. Of course suppressing the common mode resonance by coiling the transmission line or applying a common mode choke has the effect of inserting a high impedance in series with the 'ground' connection. In reality, the common mode impedance to ground of an isolated LC circuit is not infinite. Both the inductor and capacitor have capacitance to space which will provide some 'grounding' effect. At MF through VHF, the components would generally need to be physically very large to have a usefully low common mode impedance to ground however. The opposite terminals of the parallel resonant circuit and the opposite terminals of the short-circuit stub are out of phase, in either case. They are equivalent. Coupling between the elements exists in an ordinary dipole, even though the elements are end-to-end. There must be enough coupling to complete the transmission circuit, else the antenna wouldn`t work. Turns out the mutual impedance between two isolated colinear dipole elements is of the wrong polarity for parasitic operation as a broadside array. As you might expect, the mutual impedance between elements is dominated by end to end capacitance which is wrong for broadside gain. The Yagi configuration has a natural tendency to provide broadside gain, while the colinear does not. I think equivalence is the key. If one works, the other must work too. As long as they are truly equivalent for the case being considered. Failing to consider common mode impedances is unfortunately a very common practice and will often lead to incorrect conclusions. The devil is often in the details. bart wb6hqk |
#120
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Bart
I am just not smart enough to follow all of your post. But in between the lines I see a correlation to what I suggested that Cecil does to modify his collinear dipoles in the center portion a replacement circuit for a dimensionless inductance to a circuit that have dimensions in every sense and is its equal. However he has rejected this aproach. I would also add that if he imposed a parallel circuit that over lapped the dipole at each side then he has achieved an increased radiation efficiency per unit length since the parallel circuit radiation is additive to the dipole radiation.. That would replace a large portion of the center of a extended zepp and also eliminate the stub portion.which are basically inefficient. ( Cecil has also rejected this notion in the past prefering his multi stub length arrangement as shown on his page.) However, the idea of a combination loop dipole in this circle just apears to bring gasps of horror.as does the replacement of inefficient parts ( low efficiency portions or same that has counter phase radiation.) Since your post is laced with technical stuff that I don't understand but deals with the advantages of a loop over a stub, perhaps those that are more enlightened than I of which their are many, will discuss further your contribution so that education will replace the frustration that unfortunately now abounds Regards Art "Bart Rowlett" wrote in message om... Here's a post of mine from the thread titled 'colinear connundrum' from a few years ago. Perhaps it will shed some light on the subject : Gray Frierson Haertig wrote: "One of the classic implementations of the collinear uses parallel resonant circuits as the phase inverting means between separate elements---." I`ve discussed the if and how a parallel resonant circuit can replace a short-circuit 1/4-wave stub as a phase inverter, and never been satisfied either. If considered as two terminal devices, a 1/4 wl stub, parallel resonant LC circuit and an insulator are equivalent, at least for steady state AC. Understanding the difference requires a slightly more elaborate model for the stub or LC circuit. The model must account for charge accumulation, or common mode current on the device. Classic network theory can be used if a third, or 'common mode center tap' is added to the device model. Consider the parallel resonant LC circuit with the center of the inductor (or capacitor) grounded. The impedance between the two 'hot' terminals will be very high as in the two terminal case. The ground connection introduces a new constraint. The voltage on a 'hot' terminal is now constrained to be equal in magnitude and of opposite polarity from the other 'hot' terminal. This is not the case for the two terminal device model. The three terminal device (center tap grounded) can be used as a polarity reversing 1:1 transformer by connecting one 'hot' terminal to a ground referenced source and driving a load with the other terminal. Of course the same effect could be accomplished without the capacitor if the center tapped inductor (autotransformer) had suitable properties. Note that if the two 'hot' terminals are shorted the impedance (common mode) to ground is zero. Observe: The differential mode impedance between 'hot' terminals is very high (ideally infinite). The common mode impedance to ground is zero. The voltage on the 'hot' terminals respect to ground is of equal magnitude and opposite polarity. But, as Gray noted, a perfect parallel resonant circuit is an insulator. So is the perfect short-circuit 1/4-wave stub. Now look at a 1/4 wl shorted stub far removed from ground. Viewed as a two terminal device it behaves similar to a parallel resonant LC circuit. If the two open 'hot' wires are shorted, the stub looks like a 1/4 wl long wire. The impedance with respect to ground is approximately 36 ohms, which is very small compared to the nearly infinite differential impedance. Think of it as a single 1/4 wl counterpoise; adding a second colinear 'radial' results in an even lower ( 36/2 ohms) 'virtual ground' impedance. Thus the 1/4 wl stub behaves similar to the parallel resonant LC circuit with the grounded center tap. The common mode behavior of the freespace 1/4 wl stub provides the low impedance 'virtual ground'. Of course suppressing the common mode resonance by coiling the transmission line or applying a common mode choke has the effect of inserting a high impedance in series with the 'ground' connection. In reality, the common mode impedance to ground of an isolated LC circuit is not infinite. Both the inductor and capacitor have capacitance to space which will provide some 'grounding' effect. At MF through VHF, the components would generally need to be physically very large to have a usefully low common mode impedance to ground however. The opposite terminals of the parallel resonant circuit and the opposite terminals of the short-circuit stub are out of phase, in either case. They are equivalent. Coupling between the elements exists in an ordinary dipole, even though the elements are end-to-end. There must be enough coupling to complete the transmission circuit, else the antenna wouldn`t work. Turns out the mutual impedance between two isolated colinear dipole elements is of the wrong polarity for parasitic operation as a broadside array. As you might expect, the mutual impedance between elements is dominated by end to end capacitance which is wrong for broadside gain. The Yagi configuration has a natural tendency to provide broadside gain, while the colinear does not. I think equivalence is the key. If one works, the other must work too. As long as they are truly equivalent for the case being considered. Failing to consider common mode impedances is unfortunately a very common practice and will often lead to incorrect conclusions. The devil is often in the details. bart wb6hqk |
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