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Roy Lewallen wrote:
The amplitudes of the sideband components are symmetrical (at least for modulation by a single sine wave), but the phases aren't. The phases of all the upper sideband components are in phase with the carrier; in the lower sideband, the odd order components (and only the odd order ones) are reversed in phase. I certainly didn't realize that until you pointed it out; I was generalzing from the narrowband FM situation where only the first sideband components are necessarily maintained and incorrectly assuming the same phase differences applied to the general case. However... Say you start with a baseband FM signal. Let's call the two sides of its Fourier transform L and R for the 'left' and 'right' halves. Now we mix up to the desired carrier frequency. At -f_c we have L at even greater negative frequencies and R at smaller negative frequencies. Ditto at f_c. If we now apply a low pass filter to select the lower sideband, we end up with R and L -- No information has been lost! (Likewise, with a high pass filter you have L and R left -- Same deal.) Fundamentally mixing ANY signal followed by SSB filtering shouldn't lose information. Yes, in practice we'll be talking about VSB instead of SSB, but I still think we're OK. Speaking of narrowband FM (NBFM)... and at the risk of splitting this topic... I had a discussion today with someone over the ability to use an envelope detector to recover narrowband FM signals. The output of the envelope detector is approximately 1+0.5*cos^2(2*pi*f*t), where f was the original modulating signal. The '1' will be killed by a capacitor, but that leaves the cosine squared term... which seems impossible to easily change back into cosine, since sqrt(x^2)=abs(x) and therefore it would appear that we've irreversably lost information. Comments? ---Joel Kolstad ....ambitious novice who'll be licensed shortly... ....and I still think C-QUAM AM stereo is quite clever... |
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