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No that is not what it is all about. Some here object to the term of TOA and
want strict adherence to the description in terms of "elevation angle". This same subject came up a few months ago and went on for a long time. Now we are at it again and allowing the discussion to supplant original thoughts. You can now see that somebody has inventing a statement in straw man fashion and then using the lie as a truthful fact for the basis of an illicit attack. Anything goes I'll wager if you look up the thread of a few months ago on a TOA thread you will see contrary postings by the same persons that are posting now, this purely for the sake of a continueing augument. This group will never agree to anything other than all is known about antennas and will fight to the death if anybody alludes to anything that conflicts with this. It is for that reason the debate has been throttled and why TOA as shown in some computor programs is used as a diversionary tactic. I give up ! The world is flat. I will not disagree with that statement anymore so that emotions can now settle down and I can live in peace In addition: All is really known about antennas since there is no evidence of a scientific book that has been written about what is unknown about antennas. In addition : I urge all newcomers to the hobby to accept the notion that propagation can modify radiation immediately after emmission from a radiating antenna , this being a consensus of viewa by noted Gurus in the hobby In addition If a commercial computor program uses the term of TOA then it is not to be trusted aince it is based around terms that are known to be invalid and it must be left to the user to determine how far this invalidity extends with respect to results obtained. Many commercial programs use this same term so it is a case of buyer beware. Best regards Art "Fred W4JLE" wrote in message ... Art, propagation does indeed determine the takeoff angle. Let's call that pTOA. An antenna also has a design takeoff angle. We will call that aTOA. I think you may be using the term applied to an antenna, Don't confuse it with pTOA. two different animals with the same name. " wrote in message news:zgube.16975$c24.6191@attbi_s72... Richard, You are at it again, avoiding the supply of corroberation to what you say is true. Stick to the basic statement that you made, which from their silence, the gurus concur with. Your statement was that: propagation is what determines TOA and I ask for confirmation of the correctness of that statement from you in the nature of some written text. The gurus obviously accept your statement as fact, but I do not. Usually you refer to a text to back up your statement ,but this time you haven't, winging it and relying solely on the fact that the gurus agree with you. Surely you or some guru can come up with a written text that states that propagation is what determine TOA.! That is what this group is all about where gurus debunk the untruths and supply the real truths and not to let old wives tale dominate. You also stated that you made the ":assumption" presumably based on the "facts" stated above that the Curtain could be considered as similar to the dipole since propagation determines that they are the same. This is total junk ,in its entirety, unless you or the gurus can come up with a written text that confirmes their positions. Art "Richard Harrison" wrote in message ... Art Unwin wrote: "---may I go back to the "compared to a dipole" statement which Richard keeps brushing off." I accept a resonant dipole reference as a given. It is true that the antenna under test and the reference dipole have different radiation patterns. Our goal was to compare received signal strengths at locations of interest. The assumption was that on average, the propaqgation was nearly the same for the signals received from both transmitting antennas. Good or bad propagation, the difference between the signals depended on gain in the direction of the receiver as the transmitted power was the same to both antennas no matter where it landed. Kraus says on page 535 of his 3rd edition of "antennas": "Suppose that we express the gain with respect to a single lambda/2 element as the reference antenna. Let the same power P be supplied to this antenna. Then assuming no heat losses, the current Io is the sq rt of the power divided by the resistance of the reference antenna. In general, the gain in field intensity of an array over a reference antenna is given by the ratio of the field intensity from the array to the field intensity from the reference antenna when both are supplied with the same power P." Kraus` example was our intended case. Our expectations were met and our contractors were paid. Best regards, Richard Harrison, KB5WZI |
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