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On Wed, 11 Oct 2006 16:32:50 GMT, "Frank's"
wrote: .... One thing that has bothered me about small loop modeling. When driven with a voltage source; loops of length 0.1 wavelengths exhibit a radiated power ,and efficiency, of 0. In other words the structure loss is than the input power. Removing the wire conductivity loading corrects the problem. In your particular case, at 5 MHz, the real input impedance is more than three orders of magnitude greater than the radiation resistance. I guess it could just be numerical rounding errors, but have gotten identical results when using double precision. Hi Frank, That is interesting. I haven't pursued modelling the loop being excited directly, but I accept your observations. I have no idea what causes the problem. Perhaps a NEC guru may have an explanation? I thinking about the impact of error in the estimate of either radiation resistance or loss resistance of the conductor in the scenario that I did model, it should be low, probably insignificant. The magnitude of both components is small relative to the load impedance and the loop's own reactance, and does not influence the loop current (and therefore the load voltage) much. Whilst it would be interesting to know if it is a fault in modelling, or just numerical stability in the computation engine, I suspect the effect you observed probable does not give great concern for the accuracy of my receive loop models. I would like to have modelled insulated wire in the loops, but don't have NEC-4... so I will build the loops from bare wire, although I think it would make very little difference, even more so at the lower frequency side of the range. Thanks, appreciate the thoughts. Owen -- |
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