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You have to be careful in what you call the "carrier". As soon as you
start modulating the "carrier", you have more than one frequency component. At that time, only the component at the frequency of the original unmodulated signal is called the "carrier". So you have a modulated RF signal, part of which is the "carrier", and part of which is sidebands. General frequency domain analysis makes the assumption that each frequency component has existed forever and will exist forever. So under conditions of modulation with a periodic signal, you have three components: A "carrier", which is not modulated, but a steady, single frequency, constant amplitude signal; and two sidebands, each of which is a frequency shifted (and, for the LSB, reversed) replica of the modulating waveform. You can take each of these waveforms, add them together in the time domain, and get the familiar modulated envelope. So, the short answer is that the carrier, which is a frequency domain concept, is there even if you're modulating at 0.001 Hz. But to observe it, you've got to watch for much longer than 1000 seconds. You simply can't do a meaningful spectrum analysis of a signal in a time that's not a lot longer than the modulation period. Roy Lewallen, W7EL Gary Schafer wrote: Speaking of AM modulation,, we all know that the carrier amplitude does not change with modulation. Or does it? Here is a question that has plagued many for years: If you have a plate modulated transmitter, the plate voltage will swing down to zero and up to two times the plate voltage with 100% modulation. At 100% negative modulation the plate voltage is cutoff for the instant of the modulation negative peak. How is the carrier still transmitted during the time there is zero plate voltage? If we lower the modulation frequency to say 1 cps or even lower, 1 cycle per minute, then wouldn't the transmitter final be completely off for half that time and unable to produce any carrier output?? Question is, at what point does the carrier start to be effected? 73 Gary K4FMX |
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