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#1
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![]() "Art Unwin" wrote in message ... On Sep 26, 7:49 am, "Rectifier" wrote: "Art Unwin" wrote in message ... When modelling antennas and also building them it is obvious that maximum gain comes about when resistance aproaches zero. Soooooooo common sence says that the best antenna gain comes about when the anti resonant point can be easily fed, welllll thats how my antennas work. Unfortunatelly, the antenna was resonant on top band but with a very low resistance so I have to start all over again. The noise level did increase by 7 S units where modelling showed 9 dbi gain ! Maybe I should use two radiators instead of the single one. O well, I have to make changes so the anti resonance point is available at top band. David, IT IS a topsy turvy world so I am not available to listenning to the wobbly heads on the radio. Oh shame for shame Art Uh, resistance? Are you talking about DC resistance? What about impedence? You also stated, "Unfortunatelly, the antenna was resonant on top band but with a very low resistance so I have to start all over again" after saying, "maximum gain comes about when resistance aproaches zero." Which is it? Is your low resistance good nor not? I feed antennas with a resistive feads without reactance, when it becomes an impedance I retune or should I say the radio retunes the antenna to make it resistive to make it resistive OK Art. I hate to put it this way, but you really need to take a course or two to get on the same page and be understood in these subjects. Even a few nights with the ARRL Handbook may help bridge the gap. For instance. With Lumped Constants, when inductive reactance and capacitive reactance are equal, the circuit is in resonance. Any series resistance in the circuit will become a significant load and result in loss. In an antenna, there will be a characteristic impedance of the feed point. Although it may include the loss resistance, other factors determine that impedance. Since there are nodes of high and low impedance on the antenna, the feed point may be modified or relocated for different impedance. Also because of the nodes, there will be high and low currents along the antenna. Where the current is high, the losses in the resistance will be greater and most greatly affect the Q. |
#2
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On Sep 26, 10:52*am, "JB" wrote:
"Art Unwin" wrote in message ... On Sep 26, 7:49 am, "Rectifier" wrote: "Art Unwin" wrote in message .... When modelling antennas and also building them it is obvious that maximum gain comes about when resistance aproaches zero. Soooooooo common sence says that the best antenna gain comes about when the anti resonant point can be easily fed, welllll thats how my antennas work. Unfortunatelly, the antenna was resonant on top band but with a very low resistance so I have to start all over again. The noise level did increase by 7 S units where modelling showed 9 dbi gain ! Maybe I should use two radiators instead of the single one. O well, I have to make changes so the anti resonance point is available at top band. David, IT IS a topsy turvy world so I am not available to listenning to the wobbly heads on the radio. Oh shame for shame Art Uh, resistance? Are you talking about DC resistance? What about impedence? You also stated, "Unfortunatelly, the antenna was resonant on top band but with a very low resistance so I have to start all over again" after saying, "maximum gain comes about when resistance aproaches zero." Which is it? Is your low resistance good nor not? I feed antennas with a resistive feads without reactance, when it becomes an impedance I retune or should I say the radio retunes the antenna to make it resistive to make it resistive OK Art. *I hate to put it this way, but you really need to take a course or two to get on the same page and be understood in these subjects. *Even a few nights with the ARRL Handbook may help bridge the gap. For instance. *With Lumped Constants, when inductive reactance and capacitive reactance are equal, the circuit is in resonance. *Any series resistance in the circuit will become a significant load and result in loss. In an antenna, there will be a characteristic impedance of the feed point.. Although it may include the loss resistance, other factors determine that impedance. *Since there are nodes of high and low impedance on the antenna, the feed point may be modified or relocated for different impedance. *Also because of the nodes, there will be high and low currents along the antenna. Where the current is high, the losses in the resistance will be greater and most greatly affect the Q. I do not have any lumped constants. Maxwell's laws do not include lumped loads only distributed loads and my antennas revolve solely around the laws of Maxwell which being based on equilibrium includes all four forces of the standard model I have no problem with your suggestion, it is that I am just to busy at what I do. True ,you can feed at any point but there are penalties with that aproach which I don't want to mess with, I prefer to have continual tuning or adjustment at the antenna. Just a reminder but my design is not focussed around a planar form that concentrates on inter coupling of radiators . Best regards no offence taken Art |
#3
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![]() "Art Unwin" wrote: I do not have any lumped constants. Maxwell's laws do not include lumped loads only distributed loads and my antennas revolve solely around the laws of Maxwell which being based on equilibrium includes all four forces of the standard model Art: Of course you have lumped elements in your "antenna". You have a shoebox full of wire, fashoned into contra-wound coils. Also, the tuning device you described is a variometer, again replete with COILS. These coils constitute "lumped constants", as you call them. Mistakes like this show that your equilibrium is tilted. Mike W5CHR Memphis Tenn |
#4
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On Sep 26, 11:44*am, "Mike Lucas" wrote:
"Art Unwin" wrote: I do not have any lumped constants. *Maxwell's laws do not include lumped loads only distributed loads and my antennas revolve solely around the laws of Maxwell which *being based on equilibrium includes all four forces of the standard model Art: * * Of course you have lumped elements in your "antenna". You have a shoebox full of wire, fashoned into contra-wound coils. Also, the tuning device you described is a variometer, again replete with COILS. These coils constitute "lumped constants", as you call them. Mistakes like this show that your equilibrium is tilted. Mike W5CHR Memphis Tenn If you say so Rectifier I am having a rethink on where to feed it aproach. Have to sleep on it I will keep hold of that antenna but I am working on the winter one at the moment Regards Art |
#5
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![]() "Art Unwin" wrote in message ... On Sep 26, 11:44 am, "Mike Lucas" wrote: "Art Unwin" wrote: I do not have any lumped constants. Maxwell's laws do not include lumped loads only distributed loads and my antennas revolve solely around the laws of Maxwell which being based on equilibrium includes all four forces of the standard model Art: Of course you have lumped elements in your "antenna". You have a shoebox full of wire, fashoned into contra-wound coils. Also, the tuning device you described is a variometer, again replete with COILS. These coils constitute "lumped constants", as you call them. Mistakes like this show that your equilibrium is tilted. Mike W5CHR Memphis Tenn -If you say so -Rectifier -I am having a rethink on where to feed it aproach. Have to sleep on it -I will keep hold of that antenna but I am working on the winter one at -the moment -Regards -Art I merely used Lumped Constants as an example to describe the relationship between Inductive and Capacitive reactance, resistance, then to go on and show how it is differently applied to antennas and impedance. Where to feed it is exactly the point in providing a transition between the feedline and antenna. For example: Lumped Constants in an antenna tuner not only adjust reactance by providing the conjugate reactance to whatever is presented at its input terminals, but also adjusts impedance, akin to adjusting where the current minima and maxima will be in relation to the tuner's output terminals. There are a great many ways to physically do that, either by linear loading, lumped constants, transmission lines, transitions, transformers. Look into the feed methods used for Yagis. |
#6
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![]() "JB" wrote in message ... Look into the feed methods used for Yagis. now you've done it... now you will be on art's hit list. anything to do with the infamous 1 dimensional yagi antenna is the root of all evil that holds us hostage to old ways and prevents us from following in art's divine footsteps. after all, his 3d optimized diamagnetic anti-gravity static netrino tilted shoebox full of wire in front of a 3' reflector would outperform any yagi design on any band! Of course he still hasn't figured out how my 3d antenna made out of ferromagnetic materials could possibly radiate without his jumping static netrinos all over it. |
#7
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On Sep 26, 3:16*pm, "Dave" wrote:
"JB" wrote in message ... *Look into the feed methods used for Yagis. now you've done it... now you will be on art's hit list. *anything to do with the infamous 1 dimensional yagi antenna is the root of all evil that holds us hostage to old ways and prevents us from following in art's divine footsteps. *after all, his 3d optimized diamagnetic anti-gravity static netrino tilted shoebox full of wire in front of a 3' reflector would outperform any yagi design on any band! *Of course he still hasn't figured out how my 3d antenna made out of ferromagnetic materials could possibly radiate without his jumping static netrinos all over it. David I have used Yagi's for decades. Nothing wrong with them, they harfest more than 90% of radiation available and are directive and very easy to make. What I am pursueing is a different aproach to radiation in an effort to make smaller and efficient antennas without resorting to fractional wavelength. It should not matter to you if I succeed or not. We have had many years of the Yagi without much improvement so I am turning antennas on its head and starting again from where the Masters put their ideas together. Maxwell just played with numbers and equations supplied to him by the forerunners he just wasn't interested in equilibrium he was interested in the interplay of numbers only. It is our good luck that all the forerunners included the consequences of equilibrium in all their functions so whether Maxwell was interested or not the equilibrium format was included whether he understood that or not. Now you and everybody else knows that computor programs were built solely around Maxwells laws with the condition of equilibrium. Whether you like it or not the program had to be extended so it was of use to amateurs who used intercoupling of elements as a short cut to approximations of radiation which foirtunatelly are quite good such that we have become lazy in poursueing the laws of the Universe on the assumption that there is no such thing as a Universal law. I believe there is a universal law and I will not be detered from that search from the likes of you who apparently solved all the laws of nature before I started. If nyou got there then so can I Have a happy week end and for goodness sake quit the drinking and savore the World as it is Regards Arti |
#8
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On Sep 26, 3:16*pm, "Dave" wrote:
"JB" wrote in message ... *Look into the feed methods used for Yagis. now you've done it... now you will be on art's hit list. *anything to do with the infamous 1 dimensional yagi antenna is the root of all evil that holds us hostage to old ways and prevents us from following in art's divine footsteps. *after all, his 3d optimized diamagnetic anti-gravity static netrino tilted shoebox full of wire in front of a 3' reflector would outperform any yagi design on any band! *Of course he still hasn't figured out how my 3d antenna made out of ferromagnetic materials could possibly radiate without his jumping static netrinos all over it. David If a radiator is ferromagnetic it will still create eddy currents but on a smaller scale than with diamagnetic material as well as the material being lossier because of the hysteresis. The bottom line is that the eddy current becomes swamped by the initiating current and the same goes for the magnetic fields. Keep the above in mind and then review a tank circuit to see the implications of the above, I am sure you will be surprised if you are familiar with the attributes that a tank circuit has beyond the slosh back and forth. You should look up wilkpedia for aluminum scrap metal sorting to see the different projection angles ( levitation) of the different materials being sorted into the separate containers. Move beyond non magnetic stainless steel and the elevation angles change very quickly. As far as neutrinuos goes you would have to look very hard for a material that would absorb a non bound free electron I believe it is less than 5% of the materials on Earth that would interfere with the placement of a free electron which would put it somewhere below 1/2% in termns of volume. Remember the less the ratio of eddy current the less force available for spin which would cut out all DXing. Put that bottle down and get that brain of yours back in order. Why not watch the debate with a cup of hot tea? Art of the Earths volume. Art |
#9
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On Sep 26, 2:40*pm, "JB" wrote:
"Art Unwin" wrote in message ... On Sep 26, 11:44 am, "Mike Lucas" wrote: "Art Unwin" wrote: I do not have any lumped constants. Maxwell's laws do not include lumped loads only distributed loads and my antennas revolve solely around the laws of Maxwell which being based on equilibrium includes all four forces of the standard model Art: Of course you have lumped elements in your "antenna". You have a shoebox full of wire, fashoned into contra-wound coils. Also, the tuning device you described is a variometer, again replete with COILS. These coils constitute "lumped constants", as you call them. Mistakes like this show that your equilibrium is tilted. Mike W5CHR Memphis Tenn -If you say so -Rectifier -I am having a rethink on where to feed it aproach. Have to sleep on it -I will keep hold of that antenna but I am working on the winter one at -the moment -Regards -Art I merely used Lumped Constants as an example to describe the relationship between Inductive and Capacitive reactance, resistance, then to go on and show how it is differently applied to antennas and impedance. *Where to feed it is exactly the point in providing a transition between the feedline and antenna. *For example: *Lumped Constants in an antenna tuner not only adjust reactance by providing the conjugate reactance to whatever is presented at its input terminals, but also adjusts impedance, akin to adjusting where the current minima and maxima will be in relation to the tuner's output terminals. *There are a great many ways to physically do that, either by linear loading, lumped constants, transmission lines, transitions, transformers. *Look into the feed methods used for Yagis. Mike I am not a total newby to antennas. I understand them in my own way very well.I obviously have a problem in communication I am changing the dimensional structure purely to get the anti resonant point at the center of the top band instead of the standard resonant point which is too low to realistically to use. Now the antiresonant point will be between 100 and 200 ohms resistive which allows me to feed it directly from a 50 ohm transmission line (3/4 andrews) with negligable losses as the mismatch is resistive. Past work and experimental results lead me to belive I have a beam for top band with approx 9/10 dbi gain when a reflector is not used. Now who in the World would throw away the thought of such a antenna because of the silly aproach of old timers who consider all is known otherwise they would have changed things a long while ago? The design with all info will eventually appear on my page. Up to now I have tried to share everything but old timers on retirement close their minds and cannot abide change. If I see from past postings that a dialog could be rewarding I will respond but they are few and far between. There has not been one person on this newsgroup over the last few years who is able to look at a Gaussian field with an applied time varient field and a radiator and mathematically prove that the results are the same as Maxwell. True the units are different between Gauss and Maxwell but to deny the mathematical equivalence without doing the math is unconciousable Art Regards Art |
#10
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"Art Unwin" wrote
... Now the antiresonant point will be between 100 and 200 ohms resistive which allows me to feed it directly from a 50 ohm transmission line (3/4 andrews) with negligable losses as the mismatch is resistive. __________ Art - An antenna with an input impedance of 150 + j 0 ohms has a reflection coefficient of 0.5 (50%), a return loss of 6.02 dB, and an SWR of 3:1 to a 50 ohm source. Probably not many transmitters would be happy with that magnitude of load mismatch. Do you maintain that the losses defined by these parameters are negligible to amateur radio operators? RF |
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