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Wes,
What you have posted is very interesting and is not spewing out alot of stuff regarding isentropic gain etc that is really not relevent to an actual testing range. Rather than deflect away from Reg's needs may I go back to the "compared to a dipole" statement which Richard keeps brushing off. If the gains are different then the angle for max radiation is different and if you do not take this into account by searching for the individual point of maximum gain position then the the measurements are in total error. To put antennas at the same height and then measuring at the same stationary point for receive, switching back and forth is not a true comparison because of the different elevation angles. If one was to compare a long yagi to a dipole ando make it a true comparison measurement one must surely take into account the two degree or so difference when positioning the listening posts and not relying on a single listening position which to me appears to be a NO No . Richards response to the "error" question totally ignored TOA saying they are usually the same . He also ignored what he considered as an "equal" height for the curtain, i.e the top,bottom or the center line of the curtain array which alone would introduce error with respect to comparible measurement. If Richard was pointing out that his was a typical professional method of measurement then I would view his statement in complete disbelief. Your posting, thankyou, confirms my thinking in that the use of a dipole only confirms the reliability of the set up used and that is the end of it with respect to measurement of a competing antenna where I suspect a pro lab would identify the particular resulting elevation measurement. If the last sentence is in error I would apreciate a correction Regards Art "Wes Stewart" wrote in message ... On Sun, 24 Apr 2005 05:44:34 +0000 (UTC), "Reg Edwards" wrote: All electrical calibration and testing laboratories issue tables of claimed accuracies of measurements. Measurement uncertainties stated on calibration certificates are legally binding. All stated measurement results must be traceable to International Standards or a laboratory or testing station loses its status. Consequently there is no incentive for a laboratory to overstate its capabilities in its sales literature. Indeed, it is dangerous, illegal even! Naturally, laboratories can differ widely, one from another. It would be interesting to compare laboratory uncertainties with performance figures claimed by antenna manufacturers. Or anyone else. Does anyone have typical examples of measurement uncertainties claimed by antenna testing stations? Answers in decibels please. A reply from a testing station, at HF or VHF, would be specially appreciated. As stated by Ian, there's no simple answer. The bane of antenna testing is reflections reflections reflections. It may come as a surprise to our correspondent who likes to disparage "gurus" that "standard-gain" antennas are widely used as reference standards. To head off the question of how the standard gain is determined, that is done by testing three "identical" antennas in pairs; each one against the other two, with one the source and the other the receiver. A bit of algebra and you have the gain of each one individually. http://www.mi-technologies.com/literature/a00-044.pdf The foregoing paper might help answer Reg's question about achievable accuracy. While not addressing hf and vhf measurements, some of the following might be of interest. Indoor measurements are usually conducted in anechoic chambers where the shape is often tapered to control reflections and the walls are covered in absorber material. A chamber will have a "quiet zone" where the reflections are specified to be X db down. Very often the antennas under test are being characterized for side lobe levels or in the case of monopulse radar, the null depth of the difference pattern(s). If you're trying to measure a 60 dB null, it doesn't pay to have a quiet zone of -40 dB. These measurements also require an amplitude and phase front that mimics a source at infinite distance. This used to require huge chambers, often hundreds of feet long. A new way to accomplish this is to "fold" the range by using specially shaped reflectors to flatten the amplitude/phase across the test aperature. This has the added benefit of shorter cables between sources, DUT and measurement receiver. At X and K band, cable loss can be a killer. Likewise moving cables around and even temperature changes can affect the measurments. I have used such a range to measure antennas from L to Ka band. Outdoor ranges often "feature" the ground reflection, since it is difficult to eliminate it physically. This is particularly true at hf/vhf. I have used a technique that utilized the time-domain capability of a modern network analyzer (HP-8510) to identify the reflection and then place absorber material to attenuate it. Similarly, a frequency-domain measurement, that includes ground reflection, can be transformed to the time domain where the reflection is gated out and then transformed back to the frequency domain for "reflection free" analysis. See also: http://www.lehman-inc.com/pdf/mag2.pdf |
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