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Cecil Moore wrote:
Gene Fuller wrote: In order to support his point about using phasors interchangeably with field vectors, Cecil copied and posted a figure on his website under the page name of "EHWave.jpg". For the record, I have not used field vectors at all during this discussion. Everything I have ever posted have used phasors. From the IEEE Dictionary, "E and H are the electric and magnetic field vectors in phasor notation". That is what I have been doing all along. The "notation" is not the most important part. "Phasor notation" is simply a means expressing the phase in terms of complex numbers. The vector *direction* is all-important. That is the essential "vector" part of the Poynting analysis. The vector *direction* is not addressed at all by the phase or by phasor notation. Depending on the exact notation, the vector "magnitude" may be described by phasor notation. If one is going to correctly perform Poynting analysis, it is necessary to consider field vectors. There is no alternative. From "Optics" by Hecht: "Therefore, its instantaneous value [for the Poynting vector] would be an impractical quantity to measure directly. This suggests that we employ an averaging procedure." Virtually every time I have used the term, "Poynting vector", I have been talking about the average value, not the instantaneous value. Most of this discussion has been based upon a disagreement between your insistence that the instantaneous Poynting vector for a standing wave is always zero at all times and places, compared to my insistence that it is not zero at all times and places. I have no disagreement with Hecht. EHWave.JPG is a good representation of an EM traveling wave in phasor notation. If we project the fields onto the real axis, we obtain the conventional representation. The representation in EHWave.jpg is already shown in real axes. There is no projection needed. The whole point of that figure is to show a circularly polarized wave. The vector direction does indeed rotate around the propagation axis exactly as shown. The observed rotation angles around the propagation axis have nothing to do with phasors; they are real physical angles of the E-field and H-field. 73, Gene W4SZ |
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