Consider the output of an envelope detector defined by Equation (2.92), which is reproduced here for convenience
Question:
Consider the output of an envelope detector defined by Equation (2.92), which is reproduced here for convenience y (t) = {[Ac + Ac ka m (t) + n l (t)] 2 + n2Q (t)} 1/2
(a) Assume that the probability of the event | nQ (t) | > ε Ac | 1 + ka m (t) | is equal to or less than δ1, where ε << 1. What is the probability that the effect of the quadrature component nQ (t) is negligible?
(b) Suppose that ka is adjusted relative to the message signal m (t) such that the probability of the event Ac [1 + ka m (t)] + n1 (t) < 0 is equal to δ. What is the probability that the approximation y (t) = Ac [1 + ka m (t)] = n1 (t) is valid?
(c) Comment on the significance of the result ion part (b) for the case when δ1 and δ2 are both small compared with unity.
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