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Owen Duffy wrote:
Isn't hopping onto the rotor (assuming synchronous speed) to make your observations called moving from the time domain to the frequency domain, and all the mathematical shortcuts are only valid if all quantities share the same angular velocity (or frequency), implying sinusoidal waveform. I guess a departure from the strict phasor environment is for example when we consider a noise vector rotating about the end of a carrier phasor in exploring FM detector S/N vs C/N. That's why it's essential to not forget the implied exp(j * omega * t) term -- all waveforms in an analysis must include it, and it must be the same omega for all. In addition to inherently non-sinusoidal waveforms, waveforms resulting from any nonlinear operation, such as frequency modulation or multiplying or squaring waveforms, can't be analyzed in that environment. Roy Lewallen, W7EL |
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