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#1
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On Jul 4, 5:29 pm, rick frazier wrote:
Not sure where you get the swr repetitive over a band of frequencies stuff, (perhaps I don't read enough of the group messages) but to reply relative to dummy loads in general.... This comes from the radiator listed on my page unwinantennas.com/ Yep, Dummy Loads do radiate, they just don't radiate very well. In very true fact, most of them are encased in a metal enclosure of some sort to provide two major functions, reducing the radiation, and to provide oil or other medium for cooling. On the other hand, your statement/question concerning whether anything that conducts also radiates, the answer is "yes" so long as it isn't In a very general sense this is true because most if not all materials at room temperature have resistivity which is a measure of radiation. But there are some materials that lose their resistivity at extremely low temperatures of which the best known is a super conductor shielded by something else, the skin effect helps provide that shielding (coax, with fields on the center conductor and the inside of the shield) or in a configuration that cancels the radiation with an equal and opposite radiation (twisted pairs, ladder line). I have doubts about twisted pairs which is what I use for my antennas. The reason for crossed wires for me is to cancel lumped capacitances and where the reversal of turns cancels imposed loaded inductances Thus the length of wire used consists of only distributed loads as required by Maxwells law with length being N times wavelength. I have seen reference to canceled radiation in some antenna books but if I remember correctly the cancelling effect occurs on near field radiation only. Relative to carbon life forms, I've successfully loaded a tree and made (local) contacts, but the efficiency was probably near zero. Though many items may conduct and therefore radiate, their efficiency and effectivity as an antenna can be so low as to be readily compared to transmitting on a dummy load. Thus it is not unusual to hear ham conversations describing a given antenna/configuration as a dummy load... Interesting that you refer to life forms where carbon undergoes various changes and classifications as it decays, (c13) in the extreme. Tho I have seen some strata of earth listed as a carbon but then elsewhere as a mineral which I find confusing! Ofcourse a tree consist of molecules of water which is a diamagnetic material. Thus will have particals drawn to rest upon it to radiate as well as particles released by updrafts in a rainstorm allowing the particles to return back to a suitable place in quantum form as with lightning Good posting Regards Art KB9MZ --Rick Art Unwin wrote: I am trying to understand why a low swr repetitive over a band of frequencies is considered by hams to be a dummy load.! This consistently shows up in statements by the itelligensia of this newsgroup. Following up on the logic of that idea it would suggest that if swr was totally constant ( not sure how that could be) then all radiation must be zero or self cancelling.? This thus suggests that if a log periodic antenna was unlimitted in the number of elements used would in the limit drop down to zero radiation!. So following the thinking of this group the oscillations that I show on my page unwinantennas.com/ as a progression towards zero radiation since Q eventually is going to equal zero. Is this why the decreasing oscillation is defined as a dummy load on this newsgroup? The term comes up so often that I am compelled to look for what I am missing, especially since carbon is conductive and thus in the minds of many must therefore be radiative! Ofcourse the statement bandied around that if a material is condunctive then it must radiatiate could become fact instead of an old wives tales if stated enough times. Art |
#2
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Gentlemen,
Well, I'm afraid it's time to reveal the truth to Art. Now that he's hit upon the tree thing, he honestly doesn't have far to go before discovering all of our secrets. While I admit that he hasn't yet touched on the mysteries of citric acid, he will shortly, I mean, it's only a very short jump, right? Art, You have been the focus of a conspiracy. Yes, your suspicions have been correct, it was a conspiracy by those of us 'in the know'. We have been doing all that we can to deter you from your venture into these mysteries. I'm sure you can see where the world is just not ready for them as yet. That was the reason, the world is just not ready for the revelation yet. But it's time for this to end, the conspiracy thingy I mean. Congratulations, I really didn't think you would make it, but you have. I also believe you can understand that it takes time to turn this action of ours around and give you the deserved recognition you have earned. Be patient, it will happen shortly. In the mean time, you might give further thought on that citric acid (limes, lemons, etc.) thing and particle release. I knew you were 'close' when you mentioned trees! Hang on, it's coming... - 'Doc |
#3
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"Art Unwin" wrote
On Jul 4, 5:29 pm, rick frazier wrote: Not sure where you get the swr repetitive over a band of frequencies stuff, (perhaps I don't read enough of the group messages) but to reply relative to dummy loads in general.... This comes from the radiator listed on my page unwinantennas.com/ _______________________ Art - The most important measure of an antenna is the amount of field intensity it can produce at a given distance in a given direction, per watt of applied r-f power. So far you have written nothing specific about this for the "Unwin" antenna. Note that a transmission line feeding a 20 dB series attenuator attached to the input of a 100% efficient antenna will show very high return loss to the r-f source ( 40 dB plus the twice the cable loss). But that antenna system will radiate little of the available EM energy, nonetheless. Could you please comment on the measured or at least the calculated RADIATION CHARACTERISTICS of your antenna, compared to a matched 1/2-wave dipole at that frequency (or an isotropic radiator), and tell us how you arrived at them? If you can do that, and your results can be scientifically duplicated by others, you will have removed the source of a lot of the skepticism you read here and in your similar threads on eHam.net. Otherwise it will be "more of the same," which (let us hope) is or should not be your goal. RF |
#4
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On Jul 5, 8:21 am, "Richard Fry" wrote:
"Art Unwin" wrote On Jul 4, 5:29 pm, rick frazier wrote: Not sure where you get the swr repetitive over a band of frequencies stuff, (perhaps I don't read enough of the group messages) but to reply relative to dummy loads in general.... This comes from the radiator listed on my page unwinantennas.com/ _______________________ Art - The most important measure of an antenna is the amount of field intensity it can produce at a given distance in a given direction, per watt of applied r-f power. So far you have written nothing specific about this for the "Unwin" antenna. Note that a transmission line feeding a 20 dB series attenuator attached to the input of a 100% efficient antenna will show very high return loss to the r-f source ( 40 dB plus the twice the cable loss). But that antenna system will radiate little of the available EM energy, nonetheless. Could you please comment on the measured or at least the calculated RADIATION CHARACTERISTICS of your antenna, compared to a matched 1/2-wave dipole at that frequency (or an isotropic radiator), and tell us how you arrived at them? If you can do that, and your results can be scientifically duplicated by others, you will have removed the source of a lot of the skepticism you read here and in your similar threads on eHam.net. Otherwise it will be "more of the same," which (let us hope) is or should not be your goal. RF No.More of the same is not my goal nor is it to respond to every request. The mathematision or doctorrate type can do it solely by mathematics. The computor program is built on those mathematics. and a antenna program will ALWAYs produce radiators in equilibrium which means at an angle. Even without a optimiser you can do it on Eznec but it would be laborious but it can be done. People are enamoured with the Yagi so thay always insert planar type figures thus the program which is designed around equilibrium. If the goal is small efficient radiators then equilibrium must be present starting with a full wavelength that can then be placed in a small volume. It is the smaller efficient radiators and arrays that I have pursued since radiation per unit length is solely a measure that correlates with resistivity and it is that where my conclusions lie. Gain itself is a whole different matter cannot show it's worth |
#5
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![]() "Art Unwin" wrote in message ... On Jul 5, 8:21 am, "Richard Fry" wrote: "Art Unwin" wrote On Jul 4, 5:29 pm, rick frazier wrote: Not sure where you get the swr repetitive over a band of frequencies stuff, (perhaps I don't read enough of the group messages) but to reply relative to dummy loads in general.... This comes from the radiator listed on my page unwinantennas.com/ _______________________ Art - The most important measure of an antenna is the amount of field intensity it can produce at a given distance in a given direction, per watt of applied r-f power. So far you have written nothing specific about this for the "Unwin" antenna. Note that a transmission line feeding a 20 dB series attenuator attached to the input of a 100% efficient antenna will show very high return loss to the r-f source ( 40 dB plus the twice the cable loss). But that antenna system will radiate little of the available EM energy, nonetheless. Could you please comment on the measured or at least the calculated RADIATION CHARACTERISTICS of your antenna, compared to a matched 1/2-wave dipole at that frequency (or an isotropic radiator), and tell us how you arrived at them? If you can do that, and your results can be scientifically duplicated by others, you will have removed the source of a lot of the skepticism you read here and in your similar threads on eHam.net. Otherwise it will be "more of the same," which (let us hope) is or should not be your goal. RF No.More of the same is not my goal nor is it to respond to every request. The mathematision or doctorrate type can do it solely by mathematics. The computor program is built on those mathematics. and a antenna program will ALWAYs produce radiators in equilibrium which means at an angle. Even without a optimiser you can do it on Eznec but it would be laborious but it can be done. People are enamoured with the Yagi so thay always insert planar type figures thus the program which is designed around equilibrium. If the goal is small efficient radiators then equilibrium must be present starting with a full wavelength that can then be placed in a small volume. It is the smaller efficient radiators and arrays that I have pursued since radiation per unit length is solely a measure that correlates with resistivity and it is that where my conclusions lie. Gain itself is a whole different matter cannot show it's worth in other words, he hasn't, he won't, and he doesn't care... therefore, more of the same handwaving and meaningless bafflegab. he doesn't have the math background to present his theory in any kind of a coherent form, nor of course could he ever measure his neutrino/carbon vortex crud because it doesn't exist, so he keeps going back to the same old crap... its not even funny any more, just sad. |
#6
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On Jul 5, 11:47 am, "Dave" wrote:
"Art Unwin" wrote in message ... On Jul 5, 8:21 am, "Richard Fry" wrote: "Art Unwin" wrote On Jul 4, 5:29 pm, rick frazier wrote: Not sure where you get the swr repetitive over a band of frequencies stuff, (perhaps I don't read enough of the group messages) but to reply relative to dummy loads in general.... This comes from the radiator listed on my page unwinantennas.com/ _______________________ Art - The most important measure of an antenna is the amount of field intensity it can produce at a given distance in a given direction, per watt of applied r-f power. So far you have written nothing specific about this for the "Unwin" antenna. Note that a transmission line feeding a 20 dB series attenuator attached to the input of a 100% efficient antenna will show very high return loss to the r-f source ( 40 dB plus the twice the cable loss). But that antenna system will radiate little of the available EM energy, nonetheless. Could you please comment on the measured or at least the calculated RADIATION CHARACTERISTICS of your antenna, compared to a matched 1/2-wave dipole at that frequency (or an isotropic radiator), and tell us how you arrived at them? If you can do that, and your results can be scientifically duplicated by others, you will have removed the source of a lot of the skepticism you read here and in your similar threads on eHam.net. Otherwise it will be "more of the same," which (let us hope) is or should not be your goal. RF No.More of the same is not my goal nor is it to respond to every request. The mathematision or doctorrate type can do it solely by mathematics. The computor program is built on those mathematics. and a antenna program will ALWAYs produce radiators in equilibrium which means at an angle. Even without a optimiser you can do it on Eznec but it would be laborious but it can be done. People are enamoured with the Yagi so thay always insert planar type figures thus the program which is designed around equilibrium. If the goal is small efficient radiators then equilibrium must be present starting with a full wavelength that can then be placed in a small volume. It is the smaller efficient radiators and arrays that I have pursued since radiation per unit length is solely a measure that correlates with resistivity and it is that where my conclusions lie. Gain itself is a whole different matter cannot show it's worth in other words, he hasn't, he won't, and he doesn't care... therefore, more of the same handwaving and meaningless bafflegab. he doesn't have the math background to present his theory in any kind of a coherent form, nor of course could he ever measure his neutrino/carbon vortex crud because it doesn't exist, so he keeps going back to the same old crap... its not even funny any more, just sad. David, at this stage in life it would very difficult for me to go thru the math from the start in the exercise of adding a a radiator and a time varying field to a Gaussian field to show it is the same asMaxwell equation, very few of us are. But when you come across a theorem that makes sense to you it is gravy added when a mathematician comes along to supply the mathematics which you can follow in part. Then when antenna computor programs supply the ingredients of such an analysis which proves the same you have to get excited. When you then apply what is revealed in such a trail and succeed in making a smaller antenna that anybody has made you stop questioning what you have found. As an aside, where do you view the atributes of an antenna with near constant SWR reponse would find most use. I know most will jump to dummy load but this I ask in serious form. |
#7
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![]() "Art Unwin" wrote in message ... On Jul 5, 11:47 am, "Dave" wrote: "Art Unwin" wrote in message ... On Jul 5, 8:21 am, "Richard Fry" wrote: "Art Unwin" wrote On Jul 4, 5:29 pm, rick frazier wrote: Not sure where you get the swr repetitive over a band of frequencies stuff, (perhaps I don't read enough of the group messages) but to reply relative to dummy loads in general.... This comes from the radiator listed on my page unwinantennas.com/ _______________________ Art - The most important measure of an antenna is the amount of field intensity it can produce at a given distance in a given direction, per watt of applied r-f power. So far you have written nothing specific about this for the "Unwin" antenna. Note that a transmission line feeding a 20 dB series attenuator attached to the input of a 100% efficient antenna will show very high return loss to the r-f source ( 40 dB plus the twice the cable loss). But that antenna system will radiate little of the available EM energy, nonetheless. Could you please comment on the measured or at least the calculated RADIATION CHARACTERISTICS of your antenna, compared to a matched 1/2-wave dipole at that frequency (or an isotropic radiator), and tell us how you arrived at them? If you can do that, and your results can be scientifically duplicated by others, you will have removed the source of a lot of the skepticism you read here and in your similar threads on eHam.net. Otherwise it will be "more of the same," which (let us hope) is or should not be your goal. RF No.More of the same is not my goal nor is it to respond to every request. The mathematision or doctorrate type can do it solely by mathematics. The computor program is built on those mathematics. and a antenna program will ALWAYs produce radiators in equilibrium which means at an angle. Even without a optimiser you can do it on Eznec but it would be laborious but it can be done. People are enamoured with the Yagi so thay always insert planar type figures thus the program which is designed around equilibrium. If the goal is small efficient radiators then equilibrium must be present starting with a full wavelength that can then be placed in a small volume. It is the smaller efficient radiators and arrays that I have pursued since radiation per unit length is solely a measure that correlates with resistivity and it is that where my conclusions lie. Gain itself is a whole different matter cannot show it's worth in other words, he hasn't, he won't, and he doesn't care... therefore, more of the same handwaving and meaningless bafflegab. he doesn't have the math background to present his theory in any kind of a coherent form, nor of course could he ever measure his neutrino/carbon vortex crud because it doesn't exist, so he keeps going back to the same old crap... its not even funny any more, just sad. David, at this stage in life it would very difficult for me to go thru the math from the start in the exercise of adding a a radiator and a time varying field to a Gaussian field to show it is the same asMaxwell equation, very few of us are. But when you come across a theorem that makes sense to you it is gravy added when a mathematician comes along to supply the mathematics which you can follow in part. Then when antenna computor programs supply the ingredients of such an analysis which proves the same you have to get excited. When you then apply what is revealed in such a trail and succeed in making a smaller antenna that anybody has made you stop questioning what you have found. As an aside, where do you view the atributes of an antenna with near constant SWR reponse would find most use. I know most will jump to dummy load but this I ask in serious form. I already gave you the quote that shows that Gauss's Law is part of Maxwell's equations already, you need no math for that. and since all the antenna design programs are based on Maxwell's equations they of course comply with Gauss's law... nothing exciting there. the only use for a constant swr is to keep modern transceivers, that don't have a tuner, happy. swr has no correlation to performance of an antenna as far as gain or f/b or takeoff angle, things that are important to antenna design. i can take any antenna and give it a flat swr, there used to be a tuner on the market that did just that, until the league lab x-rayed it and found it was nothing but a dummy load potted in epoxy. the funny thing is, people liked it because it did exactly as it claimed, gave a perfect match across a wide frequency range... they didn't care that it turned a good percentage of their power into heat. so air cooled dummy loads as antennas can work, as long as you don't have anything better to compare it to... but I do, so I don't want one. |
#8
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On Jul 5, 1:32 pm, "Dave" wrote:
"Art Unwin" wrote in message ... On Jul 5, 11:47 am, "Dave" wrote: "Art Unwin" wrote in message ... On Jul 5, 8:21 am, "Richard Fry" wrote: "Art Unwin" wrote On Jul 4, 5:29 pm, rick frazier wrote: Not sure where you get the swr repetitive over a band of frequencies stuff, (perhaps I don't read enough of the group messages) but to reply relative to dummy loads in general.... This comes from the radiator listed on my page unwinantennas.com/ _______________________ Art - The most important measure of an antenna is the amount of field intensity it can produce at a given distance in a given direction, per watt of applied r-f power. So far you have written nothing specific about this for the "Unwin" antenna. Note that a transmission line feeding a 20 dB series attenuator attached to the input of a 100% efficient antenna will show very high return loss to the r-f source ( 40 dB plus the twice the cable loss). But that antenna system will radiate little of the available EM energy, nonetheless. Could you please comment on the measured or at least the calculated RADIATION CHARACTERISTICS of your antenna, compared to a matched 1/2-wave dipole at that frequency (or an isotropic radiator), and tell us how you arrived at them? If you can do that, and your results can be scientifically duplicated by others, you will have removed the source of a lot of the skepticism you read here and in your similar threads on eHam.net. Otherwise it will be "more of the same," which (let us hope) is or should not be your goal. RF No.More of the same is not my goal nor is it to respond to every request. The mathematision or doctorrate type can do it solely by mathematics. The computor program is built on those mathematics. and a antenna program will ALWAYs produce radiators in equilibrium which means at an angle. Even without a optimiser you can do it on Eznec but it would be laborious but it can be done. People are enamoured with the Yagi so thay always insert planar type figures thus the program which is designed around equilibrium. If the goal is small efficient radiators then equilibrium must be present starting with a full wavelength that can then be placed in a small volume. It is the smaller efficient radiators and arrays that I have pursued since radiation per unit length is solely a measure that correlates with resistivity and it is that where my conclusions lie. Gain itself is a whole different matter cannot show it's worth in other words, he hasn't, he won't, and he doesn't care... therefore, more of the same handwaving and meaningless bafflegab. he doesn't have the math background to present his theory in any kind of a coherent form, nor of course could he ever measure his neutrino/carbon vortex crud because it doesn't exist, so he keeps going back to the same old crap... its not even funny any more, just sad. David, at this stage in life it would very difficult for me to go thru the math from the start in the exercise of adding a a radiator and a time varying field to a Gaussian field to show it is the same asMaxwell equation, very few of us are. But when you come across a theorem that makes sense to you it is gravy added when a mathematician comes along to supply the mathematics which you can follow in part. Then when antenna computor programs supply the ingredients of such an analysis which proves the same you have to get excited. When you then apply what is revealed in such a trail and succeed in making a smaller antenna that anybody has made you stop questioning what you have found. As an aside, where do you view the atributes of an antenna with near constant SWR reponse would find most use. I know most will jump to dummy load but this I ask in serious form. I already gave you the quote that shows that Gauss's Law is part of Maxwell's equations already, you need no math for that. and since all the antenna design programs are based on Maxwell's equations they of course comply with Gauss's law... nothing exciting there. the only use for a constant swr is to keep modern transceivers, that don't have a tuner, happy. swr has no correlation to performance of an antenna as far as gain or f/b or takeoff angle, things that are important to antenna design. i can take any antenna and give it a flat swr, there used to be a tuner on the market that did just that, until the league lab x-rayed it and found it was nothing but a dummy load potted in epoxy. the funny thing is, people liked it because it did exactly as it claimed, gave a perfect match across a wide frequency range... they didn't care that it turned a good percentage of their power into heat. so air cooled dummy loads as antennas can work, as long as you don't have anything better to compare it to... but I do, so I don't want one. David ,Gauss did a lot of work in his life time for which he is recognised. Are you saying that the "Gaussian law of static" was a prime mover of Maxwells laws. If this is so why does not Maxwells laws provide the role of particles in radiation? From my view point Gauss's contribution was supplied in other ways that did not include the statics law but then I look forward to you showing me where I am wrong |
#9
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Art Unwin wrote:
On Jul 5, 11:47 am, "Dave" wrote: David, at this stage in life it would very difficult for me to go thru the math from the start in the exercise of adding a a radiator and a time varying field to a Gaussian field to show it is the same asMaxwell equation, very few of us are. At this stage of my life, Arthur, it has become very difficult for me to take you seriously. Dave K8MN |
#10
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Art wrote:
"The computer program is built on those mathematics, and an antenna program will ALLWAYS produce radiators in equalibrium which means at an angle." Arnold B. Bailey disagrees in "TV and Other Receiving Antennas". On page 367 he writes: "The directional action of a rod antenna best can be analyzed by considering the rod as consisting of many tiny sections, connected together to form a metallic circuit. A typical small segment X - X is shown in Fig. 7-28 B; its position in a half-wave center-fed antenna is indicated in part (A) of the figure. Each tiny section may be taken sufficiently short compared to a wavelength so that the electromagnetic wave acts practically instantaneously throughout one section, and hence induces a substantially uniform current in that section. Such a short antenna segment has a simple directional response pattern, indicated in Fig. 7-28B, which is basic for all directivity calculations, since all antenns may be considered to be made up of these tiny segments. This fundamental response pattern varies as the cosine of the angle (which we shall call theta) between the direction of the incoming wave and the perpendicular through the center of the segment X - X, as indicated in part (B) of the figure. If E stands for the value of the field intensity (strength of the electric vector), then we can characterize the directional response by the relation Ecos theta, which gives us the relative magnitude of E for any wave direction relative to the antenna." You probably have seen the figure-eight pattern of a dipole antenna and are already aware that maximum response is broadside to the antenna at its center. If the antenna is tilted away from the perpendicular its response is diminished. Other antennas have a similar response as all are made up of elemental segments. Best regards, Richard Harrison, KB5WZI |
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