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#1
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![]() "Richard Clark" schreef in bericht ... On Thu, 24 Feb 2011 20:17:33 +0100, "RadioWave" radio@oidar wrote: Hi Richard, Thank you for the explanations. I have not had the intention to start a scientific discussion here on this subject. To me it is a hobby. With my homepage I just want to share some of my experience with magnetic loop antennas, just like many other radio amateurs do. And of course I am willing to reply to reactions from readers. But I will not further discuss about scientifically details. Thank you. Best Regards 73, Norbert PA7NR |
#2
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Hello Richard,
I agree with you that several statements on Norbert's site will not hold when scientifically reviewed. However I think the way you respond will likely not result in better statements. As the name of the newsgroup indicates; this is a radio amateur group and Norbert site starts with "Dutch amateur radio station". This may require another approach then you should use in a professional environment. If you prefer that, Edaboard.com (just an example) is a more suitable place. Now the result is a professional reaction of Norbert: Thank you for the explanations. I have not had the intention to start a scientific discussion here on this subject. To me it is a hobby. With my homepage I just want to share some of my experience with magnetic loop antennas, just like many other radio amateurs do. And of course I am willing to reply to reactions from readers. But I will not further discuss about scientifically details. Thank you. Best Regards 73, Norbert PA7NR Because of rain, I had to stop some activity so I took a pocket calculator, some of my own course material and a used envelope within reach. A loop with diameter = 1.27m (4m perimeter), made from 20mm (diameter) copper has an inductance of about 3.4 uH (reactance of about 77 Ohm at 3.6 MHz). Radiation resistance (no coupling with other objects) will be about 1 mOhm. AC copper resistance due to skin effect will be about 30 mOhm (based on uniform current distribution over the circumference of the tubing). Q factor should be in the range of 2500 Radiation efficiency will be about 3% Directivity is 1.5 Voltage between ends (100W input): 6.3 kVp. Current through loop about 82 Ap A half wave dipole will have about 1kVp at each end (depends on conductor thickness). Effective area of antenna will be about 23 sqm (in free space). 1Vrms incident plane wave field (2.65mW/sqm) will result in about 61mW output power (about 150Vp across the tuning capacitor). You probably know that measuring a lower Q factor may result in less overall efficiency (coupling to dissipative objects) or higher overall efficiency (coupling to metallic conductors that reradiate). With kind regards, Wim PA3DJS www.tetech.nl without abc, PM will reach me very likely |
#3
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On Sat, 26 Feb 2011 07:30:00 -0800 (PST), Wimpie
wrote: Hi Wimpie, This may require another approach then you should use in a professional environment. If you prefer that, Edaboard.com (just an example) is a more suitable place. Now the result is a professional reaction of Norbert: Curious combination of conflicting sentiments, there. What is suitable, and how should we recognize it? Radiation resistance (no coupling with other objects) will be about 1 mOhm. There are many source for computation, I chose one that closely agrees with several at hand. Perhaps I made an entry error, so I will take the opportunity to examine that possibility he Rr = 80 · pi² · (dl/lambda)² 80 · 9.87 · (2/80)² 790 · (0.025)² 790 · 0.0006 0.49 Ohm Of course, the possibility of mis-entry remains, and cross checking is helpful given an in dependant validation. If I examine my text further it uses as an example a smaller loop at a lower frequency dl = 1m F = 1MHz (lambda = 300) resulting in Rr = 0.0084 Ohm which is roughly 10 times your computed radiation resistance for a larger loop at a smaller wavelength. Now, having said that, and examining my text for further possibilities of error, I find that, yes, I made an error. My computation was based for an electric dipole, not a loop. Let us examine the Rr for a loop from the equation from the same source: Rr = 320 · pi^6 · (r/Lambda)^4 320 · 961 · (1/80)^4 307,645 · 2.44^-8 0.0075 Ohm This, too, is very different from your calculation, but certainly that error is eclipsed by my own first reckoning. However, what does this say about efficiency based upon the original design (but computed for another)? However, I did first ask Norbert for the equation used and the parameters entered. Testing those results did not appear to be appealing in the face of contradicting testimonial. It should come as no surprise that many testimonials are tested here. Testimonials stand or fall in such tests, and those tests are retested (as has given rise to this and your response). Curiously we entered into this with how the loop has superior qualities over the standard dipole, and then the same loop is cited as being very inefficient. How such contradictions are held within the space of a short thread is certainly a denial of engineering professionalism, but denial is not the standard of merit that is typically lauded in this forum. A hearty defense of wounded ego raises suspicion even further. One consequence of that demurral brings us to a rather remarkable insight in comparing the radiation resistance of the electric dipole to the loop within the same spread of the loop (and in certainly a smaller volume of space). The electric dipole enjoys 60 times more radiation resistance that certainly impacts efficiency to the same degree. This, of course, presumes no further errors in computation or application. 73's Richard Clark, KB7QHC |
#4
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On 2/27/2011 11:03 PM, Richard Clark wrote:
On Sat, 26 Feb 2011 07:30:00 -0800 (PST), wrote: Hi Wimpie, This may require another approach then you should use in a professional environment. If you prefer that, Edaboard.com (just an example) is a more suitable place. Now the result is a professional reaction of Norbert: Curious combination of conflicting sentiments, there. What is suitable, and how should we recognize it? Radiation resistance (no coupling with other objects) will be about 1 mOhm. There are many source for computation, I chose one that closely agrees with several at hand. Perhaps I made an entry error, so I will take the opportunity to examine that possibility he Rr = 80 · pi² · (dl/lambda)² 80 · 9.87 · (2/80)² 790 · (0.025)² 790 · 0.0006 0.49 Ohm Of course, the possibility of mis-entry remains, and cross checking is helpful given an in dependant validation. If I examine my text further it uses as an example a smaller loop at a lower frequency dl = 1m F = 1MHz (lambda = 300) resulting in Rr = 0.0084 Ohm which is roughly 10 times your computed radiation resistance for a larger loop at a smaller wavelength. Now, having said that, and examining my text for further possibilities of error, I find that, yes, I made an error. My computation was based for an electric dipole, not a loop. Let us examine the Rr for a loop from the equation from the same source: Rr = 320 · pi^6 · (r/Lambda)^4 320 · 961 · (1/80)^4 307,645 · 2.44^-8 0.0075 Ohm This, too, is very different from your calculation, but certainly that error is eclipsed by my own first reckoning. However, what does this say about efficiency based upon the original design (but computed for another)? However, I did first ask Norbert for the equation used and the parameters entered. Testing those results did not appear to be appealing in the face of contradicting testimonial. It should come as no surprise that many testimonials are tested here. Testimonials stand or fall in such tests, and those tests are retested (as has given rise to this and your response). Curiously we entered into this with how the loop has superior qualities over the standard dipole, and then the same loop is cited as being very inefficient. How such contradictions are held within the space of a short thread is certainly a denial of engineering professionalism, but denial is not the standard of merit that is typically lauded in this forum. A hearty defense of wounded ego raises suspicion even further. One consequence of that demurral brings us to a rather remarkable insight in comparing the radiation resistance of the electric dipole to the loop within the same spread of the loop (and in certainly a smaller volume of space). The electric dipole enjoys 60 times more radiation resistance that certainly impacts efficiency to the same degree. This, of course, presumes no further errors in computation or application. 73's Richard Clark, KB7QHC Wimpie is right, Richard. Please go back to your laboratory and speak to someone who understands your dumb-ass dialect. Also, please don't discourage those who are trying to contribute their experiences here. Try to be positive for a change. John |
#5
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On Sun, 27 Feb 2011 23:14:34 -0600, John - KD5YI
wrote: Wimpie is right, Richard. I presume Wimpie can speak for himself. As he offered musings that were done on the back of a handy envelope, there is every chance he is not right. I offered a similar chance that I was not right either, but I offered complete (two in fact) equations that no one has disputed, and none have faulted for computation. I admitted a misapplication of one - which also passed without comment. Considering Wimpie's work was not done for the antenna under consideration (the size of his being much smaller where radiation resistance varies by the FOURTH POWER of size) - what does "right" mean? 73's Richard Clark, KB7QHC |
#6
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On 28 feb, 20:53, Richard Clark wrote:
On Sun, 27 Feb 2011 23:14:34 -0600, John - KD5YI wrote: Wimpie is right, Richard. I presume Wimpie can speak for himself. *As he offered musings that were done on the back of a handy envelope, there is every chance he is not right. *I offered a similar chance that I was not right either, but I offered complete (two in fact) equations that no one has disputed, and none have faulted for computation. *I admitted a misapplication of one - which also passed without comment. Considering Wimpie's work was not done for the antenna under consideration (the size of his being much smaller where radiation resistance varies by the FOURTH POWER of size) - what does "right" mean? 73's Richard Clark, KB7QHC Hello Richard, Your formulas can be disputed: When using (from http://www.ece.msstate.edu/~donohoe/ece4990notes5.pdf): Rr_loop = 320*(pi)^4*A^2/lambda^4 for f = 3.6 MHz, Dloop = 1.27m (so A = 1.27 m^2), Rr_loop = 0.001 mOhm. This result agrees the number in my previous calculation (for the same situation). From the same source, but for a dipole of 1.27m with large end- plates, Rr_dipole = 80*(pi)^2*le^2/lambda^2 = 0.18 Rr_dipole = 0.045 Ohm (without large end-plates). This is roughly a factor 45 or 180 more (for the dipole). Maybe somebody can confirm the above calculations. The actual efficiency depends on the required (space consuming) reactive component to cancel the capacitive (dipole) or inductive (loop) behavior. The advantage of the loop (especially for reception) is that you need a variable capacitor instead of a variable loop, and matching / balun function can be made easily. He also mentioned the vertical radiation component (NVIS operation) together with the nulls in the horizontal plane. Regarding claims, Norbert didn't make claims about the high efficiency. Please read his conclusion that starts with "despite the low efficiency of 3%….". His stated 3% reasonably agrees with my 3% (though you think that the calculation may be wrong). The claim with regards to performance comparable to a half wave or vertical antenna is for higher frequencies (where the loop's efficiency increases significantly). Of course I have serious doubts about the conclusions regarding general noise cancelling properties, but the conclusions can be right for that special RF-environment. Whether they apply for another situation, can be food for the radio amateur experimenter (or professional?). With kind regards, Wim PA3DJS www.tetech.nl |
#7
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#8
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On 2/28/2011 1:53 PM, Richard Clark wrote:
On Sun, 27 Feb 2011 23:14:34 -0600, John - wrote: Wimpie is right, Richard. I presume Wimpie can speak for himself. As he offered musings that were done on the back of a handy envelope, there is every chance he is not right. I offered a similar chance that I was not right either, but I offered complete (two in fact) equations that no one has disputed, and none have faulted for computation. I admitted a misapplication of one - which also passed without comment. Considering Wimpie's work was not done for the antenna under consideration (the size of his being much smaller where radiation resistance varies by the FOURTH POWER of size) - what does "right" mean? 73's Richard Clark, KB7QHC I didn't mean Wimpie was right about his technical response. I meant he was right about a part of his message which you cut: "I agree with you that several statements on Norbert's site will not hold when scientifically reviewed. However I think the way you respond will likely not result in better statements." "As the name of the newsgroup indicates; this is a radio amateur group and Norbert site starts with "Dutch amateur radio station". This may require another approach then you should use in a professional environment. If you prefer that, Edaboard.com (just an example) is a more suitable place." John |
#9
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On Mon, 28 Feb 2011 15:36:27 -0600, John - KD5YI
wrote: I didn't mean Wimpie was right about his technical response. I meant he was right about a part of his message which you cut: I selectively quote to make the response specific to the point being responded to (like I am right now). It saves room, is not ambiguous, and serves the technical community by confining discussion to technical matters. 73's Richard Clark, KB7QHC |
#10
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On 28 feb, 20:53, Richard Clark wrote:
On Sun, 27 Feb 2011 23:14:34 -0600, John - KD5YI wrote: Wimpie is right, Richard. I presume Wimpie can speak for himself. *As he offered musings that were done on the back of a handy envelope, there is every chance he is not right. *I offered a similar chance that I was not right either, but I offered complete (two in fact) equations that no one has disputed, and none have faulted for computation. *I admitted a misapplication of one - which also passed without comment. Considering Wimpie's work was not done for the antenna under consideration (the size of his being much smaller where radiation resistance varies by the FOURTH POWER of size) - what does "right" mean? 73's Richard Clark, KB7QHC Hello Richard, you used r = 1m (as you have r in your formulas), that is D = 2m, 6.28m circumference. I used D = 1.27m (4m perimeter), that is r = 0.635 m. Quote from Norbert's site: "When a magnetic loop antenna is used for 3.5 MHz with a perimeter of 4 meter (13.3 foot) , it has an efficiency of approximately 3%." Maybe this helps you to explain the difference between your and my result, Wim PA3DJS www.tetech.nl Don't forget to remove abc in case of PM. |
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