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Yagi efficiency
Remember only R is of consideration for the addition of power from each
element which provides flux unless you can quantasize reaction for me as producing the emmision of flux other than a indication of the direction it takes . I assume you are talking about radiation resistance. There are other R's that cause loss of desired radiation including conduction-dielectric losses. Some signal is lost to the ground after being radiated. Assuming that your definition of efficiency includes beam efficiency, I would suggest taking an optimized two-element Yagi into EZNEC and determining the maximum gain. Then replace the reflector by an element identical to the driven element including the source signal. Using the same amount of total driving power, if you can come up with a gain superior to the Yagi, would that prove the point you are trying to make? -- 73, Cecil http://www.w5dxp.com |
Yagi efficiency
Jimmie D wrote:
The radiation IS NOT cancelled ... Doesn't the performance of non-reflecting glass depend upon EM wave cancellation? Doesn't the gain of a beam depend upon EM wave cancellation in some other direction? -- 73, Cecil http://www.w5dxp.com |
Yagi efficiency
Dave wrote:
art wrote: David are you going nuts? I used the word impedance whichcan mean two components only one of which is used for power. No! You used the phrase "reactive impedance". It was more than likely an inclusive statement, not an exclusive one. I suspect Art meant, "a reactive impedance term value" when he said "a reactive impedance value". -- 73, Cecil http://www.w5dxp.com |
Yagi efficiency
"Cecil Moore" wrote in message .. . Jimmie D wrote: The radiation IS NOT cancelled ... Doesn't the performance of non-reflecting glass depend upon EM wave cancellation? Doesn't the gain of a beam depend upon EM wave cancellation in some other direction? -- 73, Cecil http://www.w5dxp.com The radiation is not cancelled in the way ART means, One of the problems of replying to his post is you can not do really do it without sounding like an idiot. |
Yagi efficiency
Doesn't the performance of non-reflecting glass depend upon EM wave cancellation? This I can respond to (though I doubt that I should) The term usually used is "anti-reflective" and refers to a specific multi-coating technique on the glass (or other medium). the "anti" refers to destructive wave interference for reflected light by varying the refractive index of successive coatings. Thus, MORE of the incident travels through the medium than is reflected back If the goal is to increase the % of light refracted THROUGH the medium, then anti-reflective coating increases the efficiency. Take the same glass without the AR coating, and LESS light is refracting THROUGH the medium (more reflecting back): lower efficiency. This definition of efficiency only makes sense when you're interested in light refracted through the glass. P-in / P-out does not = this definition of efficiency. The efficiency definition implies interest in directionality. Is this not where the confusion lies in all these posts? John PS, Think of a simple flashlight with a mirror and a lens. As a simple analogy, the filament of the light is the driven element with a mirror behind and a lens in front...a LIGHT Yagi, no? No diff in P-in/p-out...just all light directed out of the flashlight into a beam. |
Yagi efficiency
Cecil Moore wrote: art wrote: But the yagi then goes on to upset things by adding which have a reactive impedance which detracts from the purly resistive value of the impedance which means losses ... Actually Art, adding reactance reduces the current in the element thus *decreasing* losses below what a resonant passive element would have. Pure reactance is lossless. This current that you are referring to, I used P =I squared R which leads to lower power. Where did I go wrong Regards Art Seems to me that the reactance in the passive elements provides a phase shift that causes destructive interference in the desired places and constructive interference in the desired places. I came in late and thus apologize if anyone else has stated this earlier. -- 73, Cecil http://www.w5dxp.com |
Yagi efficiency
Cecil Moore wrote: art wrote: But the yagi then goes on to upset things by adding which have a reactive impedance which detracts from the purly resistive value of the impedance which means losses ... Actually Art, adding reactance reduces the current in the element thus *decreasing* losses below what a resonant passive element would have. Pure reactance is lossless. This current that you are referring to, I used P =I squared R which leads to lower power. Where did I go wrong Regards Art Seems to me that the reactance in the passive elements provides a phase shift that causes destructive interference in the desired places and constructive interference in the desired places. I came in late and thus apologize if anyone else has stated this earlier. -- 73, Cecil http://www.w5dxp.com |
Yagi efficiency
PS,
Think of a simple flashlight with a mirror and a lens. As a simple analogy, the filament of the light is the driven element with a mirror behind and a lens in front...a LIGHT Yagi, no? No diff in P-in/p-out...just all light directed out of the flashlight into a beam. John, You're right about the efficiency, but be careful with the flashlight analogy. A light yagi might have ~ 200 nanometer long elements. An 20m band reflector analogous to that in a mini maglight would have to be 800 miles in diameter. The analogy with respect to efficiency is fine... but there's no HF antenna that can form a beam like that. 73, Dan |
Yagi efficiency
Interesting Jimmy
Could you show me how me how a vector directed at a socalled reflector behaves with respect to a constant plane without the implication of a neutralising effect. Now the reflector "works" only as a part of a particular plane so please go on from there. I often read of additive and subtractive radiation in books written by the masters and I have seemed to have got the wrong idea about these matters Art Jimmie D wrote: "art" wrote in message oups.com... From a theoretical way of getting at the answer it seems a logical way of proceding. So now to the rest of the task.1 how do we determine volumes that you talk about that are a result of deflection 2 How do we determine radiation that was cancelled or neutralised and 3 How do you determine the radiation volume created by ground reflection so we can work back to search for ground losses. That last one really bothers me as I have never got a good handle on the contribution of ground reflection to any particular part of the radiation envelope. Art Denny wrote: For those who wish to actually learn and not just insult each other, get a calculator, learn how to calculate Cosine Theta a trivial math problem that any 9th grader can be taught in 5 minutes flat, get a BIG piece of paper reason to come, and actually calculate the shape and vector length of the lobes of a two element Yagi-Uda antenna... Do the calculation in both the horizonal and vertical planes... From that you can calculate the volume of each lobe, which is proportional to the percentage of power in each lobe... From that number you can very simply calculate what percentage went into the lobes you prefer and what went in the lobes you don't prefer... Now, the reason for the BIG piece of paper... The antenna patterns you see on the screen with EZNEC, or in the antenna handbooks, are logarithmic, not linear and there are flavors to them, ARRL, linear logarithmic, modified logarithmic... So, the patterns are distorted... Why is that? Because if they were linear and the front lobe and the rear lobe are to the same scale the front lobe will take up the entire length of the screen/paper and the rear lobe will need a magnifying glass to be seen... A rear lobe that is 20dB down from the front lobe is down by the power ratio of 100... So, if your forward lobe calculates out to be 10 inches long, the rear lobe will be be 1/10 of an inch.... I'll let you figure out the size of a lobe that is 30dB down (get out your microscope) For those who want to review do a search on Joseph Reisert, who has published numerous writings on antennas and patterns... There many are others also, but Joe is published on the web, and very readable... cheers ... denny / k8do The radiation IS NOT cancelled or Neutralized. You need to learn more about what is going on with an antenna. I suggest you do some serious reading, actually reading with an open mind and not reading trying to find little phrases that seem to you to prove your beliefs. It should be fairly obvious that if an antenna worked by neutralization or cancelation that it would take more energy to cancel out radiation in the undesired direction of a yagi than is available in the desired direction. Therefore a Yagi or any other antenna does not work by cancellation. I gues I could express this a lot better but its late and whats the use. |
Yagi efficiency
Cecil Moore wrote: Remember only R is of consideration for the addition of power from each element which provides flux unless you can quantasize reaction for me as producing the emmision of flux other than a indication of the direction it takes . I agree there are other losses but to prevent including losses that are outside the E and H process change over such as ground reflections etc is it not better to just accept The pure resistance only so there is no need to characterize individual losses Once you go beyond the near field it gets complicated as losses are created outside the EH generation process. Ii am not sure how the EZNEC thing functions but if you design the array where all elements are driven you can then use the individual element impedances to determine overall efficiency.i.e. power in versus power out Fortunately thats the way my program can operate Art I assume you are talking about radiation resistance. There are other R's that cause loss of desired radiation including conduction-dielectric losses. Some signal is lost to the ground after being radiated. snipe? -- 73, Cecil http://www.w5dxp.com |
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