gary36
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You understand that in the modulated signal carrier phase is "switched" by 180 degree for each half cycle of modulation signal? This has two consequences:Intention is to recover the value of Phi. The possible method is to compare a reference 1 KHz signal to the cos(phi-w2*t) signal and infer the value of phi implicitly.
Since carrier recovery was not so easy as mentioned in previous posts (for AM signal), I preferred some simple solution such as using tank circuit that could selectively pass on frequency and can have high Q compared to other implementations.
I suppose there is just a tiny amplitude of carrier present where we can't see it. And the op amp amplifies it. To me it's unexpected.Can you please elaborate your point mentioned in #22. I am not quite clear. Also I see that square wave generated from comparator is symmetrical whereas the source is not (discontinuity at zero crossings). Please clarify.
Phi, ϕ is an initial condition when t=0 and is also a constant like DC. The ONLY way to recover ϕ is with a stable 1kHz reference and a phase detector that is calibrated to ϕ=0 and phase locked to the carrier center frequency, f2.Intention is to recover the value of Phi. The possible method is to compare a reference 1 KHz signal to the cos(phi-w2*t) signal and infer the value of phi implicitly.
forgive my oversight, I was thinking FMI don't see how the 4046 detector is related to the discussed DSB AM signal with suppressed carrier.
I believe KarimF has the best design for AM-SC demodulator which he has used for many years.I don't see how the 4046 detector is related to the discussed DSB AM signal with suppressed carrier.
Without a universal time reference to measure "phi" when t=0, both at the transmitter and receiver, there is no possible way to recover it. Only changes in phase which is w2t can be demodulated. There are many static delays which affect the static constant of phi, including propagation delay & filter group delay.A sinw1t cos(phi-w2t).
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