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Threshold effect in envelope detection of DSB-FC

Short answer

Below a carrier-to-noise ratio of about 10 dB, the output SNR of an envelope detector for DSB-FC collapses abruptly because the message is multiplied by a random noise term rather than being additive. This non-linear threshold effect does not occur in coherent detection.

With necessary derivations, explain the threshold effect in envelope detector for DSB-FC modulation in analog communication system.

An envelope detector is a non-linear device whose output follows the magnitude of the resultant of signal plus noise. Its noise performance changes sharply when the carrier-to-noise ratio drops below a certain level; this is the threshold effect.

Envelope detector input. DSB-FC signal plus narrowband noise:

x(t)=Ac[1+kam(t)]cos⁡ωct+nc(t)cos⁡ωct−ns(t)sin⁡ωctx(t)=A_c[1+k_am(t)]\cos\omega_ct+n_c(t)\cos\omega_ct-n_s(t)\sin\omega_ct

The envelope detector output is the magnitude of the resultant phasor:

y(t)={Ac[1+kam(t)]+nc(t)}2+ns2(t)y(t)=\sqrt{\{A_c[1+k_am(t)]+n_c(t)\}^2+n_s^2(t)}
              n_s
          .---->           resultant length = y(t)
         /    ^
        /     | n_c
  ----------->+
  Ac[1+ka m(t)]

Case 1: high carrier-to-noise ratio (Ac[1+kam]≫A_c[1+k_am]\gg noise). The quadrature term is negligible:

y(t)≈Ac+Ackam(t)+nc(t)y(t)\approx A_c+A_ck_am(t)+n_c(t)

The message appears additively with the noise. After removing DC, SNRo=Ac2ka2P2N0W\text{SNR}_o=\dfrac{A_c^2k_a^2P}{2N_0W}, the same as coherent detection. Figure of merit ka2P1+ka2P\frac{k_a^2P}{1+k_a^2P} (=1/3=1/3 for a single tone with μ=1\mu=1).

Case 2: low carrier-to-noise ratio (noise ≫\gg carrier). Write the noise as n(t)=r(t)cos⁡[ωct+ψ(t)]n(t)=r(t)\cos[\omega_ct+\psi(t)], with Rayleigh envelope rr and uniform phase ψ\psi. Then

y(t)=r2+2rAc[1+kam]cos⁡ψ+Ac2[1+kam]2≈r(t)1+2Acr(t)[1+kam(t)]cos⁡ψ(t)≈r(t)+Accos⁡ψ(t)+Ackam(t)cos⁡ψ(t)\begin{aligned} y(t) &= \sqrt{r^2+2rA_c[1+k_am]\cos\psi+A_c^2[1+k_am]^2} \\ &\approx r(t)\sqrt{1+\frac{2A_c}{r(t)}[1+k_am(t)]\cos\psi(t)} \\ &\approx r(t)+A_c\cos\psi(t)+A_ck_am(t)\cos\psi(t) \end{aligned}

using 1+x≈1+x/2\sqrt{1+x}\approx1+x/2. Now the message m(t)m(t) is multiplied by the random noise cos⁡ψ(t)\cos\psi(t); there is no term proportional to m(t)m(t) alone. The message is mutilated and cannot be recovered; output SNR collapses.

Threshold effect. The change from Case 1 to Case 2 is not gradual: below a certain carrier-to-noise ratio, the threshold (roughly 10 dB carrier-to-noise ratio), the output SNR falls much faster than the input SNR. The threshold is a property of non-linear (envelope) detection; coherent detection of DSB-FC, DSB-SC or SSB has no threshold, because the product detector is linear and the message always stays additive with noise.

 SNRo (dB)                 coherent / envelope
     |                   . (above threshold)
     |                 .
     |               .
     |             .  <- threshold
     |          ..'
     |      ..''    envelope detector
     |  ..''        (below threshold)
     +-------------------------> CNR (dB)

✓ Answer checked by Claude Opus 5.5 (high effort)

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