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Richard Clark wrote in
: On Sat, 12 Jun 2010 19:52:15 GMT, Owen Duffy wrote: .... My recollection of Walt's tests were that they tested at points other than Zl=0 and Zl=infinity. Steps 1 and 2 are quite explicit. I have reviewed Walt's additional material at http://www.w2du.com/r3ch19a.pdf . Walt's load at step 1 is stated as 50+j0 without tolerance, but I accept that Walt is thorough and would have confidence that it is low in error. He reports Pf=100W and Pr=0, again accepted as indicating that the load and calibration impedance of the '43 are similar, and probably quite close to the nominal impedance, close enough for the purpose at hand. At Step 8, he substitutes a load with measured impedance and calculated rho^2 as 0.235, VSWR(50) is approximately 3. Reported Pf=95W, Pr=25W, and on that basis rho^2=0.263. The discrepency in rho is not discussed in the paper. A key observation between Step 1 and Step 8 is that changing from a VSWR (50)=1 load to a VSWR(50)=3 load resulted in a 5% change in observed Pf. This observation depends on the difference between two direct readings from a single instrument (the Bird 43), and the accuracy of calibration of both the Bird 43 and the 50 ohm load to their nominal 50+j0 impedance. I have given a mathematical development at http://vk1od.net/blog/?p=1028 of why Pf should be independent of load impedance. The observed change in Pf at 5% is rather small considering the load change, and suggests that Zs in this case is probably quite close to 50 +j0 although the experiment was limited to just one load case. I make the "just one load case" condition because in my experience, a transmitter might exhibit insignificant change in Pf for some load variations, but for others it is signficant. The case I documented earlier is one such example. Owen |
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