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Non-synchronous FM demodulation

Short answer

Non-synchronous FM demodulation uses a limiter, bandpass filter, differentiator, and envelope detector. The FM signal is differentiated to produce an AM-FM signal whose envelope is proportional to the message, then envelope detection recovers m(t).

Explain with necessary mathematical relations, the demodulation of FM wave using non-synchronous method.

Non-synchronous (non-coherent) FM demodulation recovers the message without generating a local carrier in phase with the received carrier. The standard method is differentiation followed by envelope detection (the discriminator method).

FM  +-------+ +-----+ +------------+ +--------+ m(t)
--->|Limiter|>| BPF |>|Differentia-|>|Envelope|---->
    +-------+ +-----+ |tor j2pi af | |detector|
                      +------------+ +--------+

Received FM (after limiter and BPF):

s(t)=Accos⁡[2πfct+2πkf∫0tm(τ) dτ]s(t) = A_c\cos\left[2\pi f_c t + 2\pi k_f\int_0^t m(\tau)\,d\tau\right]

Step 1: Differentiation. A circuit whose gain rises linearly with frequency, H(f)=j2πafH(f) = j2\pi a f, acts as a differentiator:

v1(t)=ads(t)dt=−2πaAc[fc+kfm(t)]sin⁡[2πfct+2πkf∫0tm(τ) dτ]v_1(t) = a\frac{ds(t)}{dt} = -2\pi a A_c\left[f_c + k_f m(t)\right]\sin\left[2\pi f_c t + 2\pi k_f\int_0^t m(\tau)\,d\tau\right]

v1(t)v_1(t) is still FM, but its amplitude now varies as fc+kfm(t)f_c + k_f m(t), i.e. it is an AM–FM wave.

Step 2: Envelope detection. Since fc≫kf∣m(t)∣f_c \gg k_f|m(t)|, the envelope is always positive:

v2(t)=2πaAc[fc+kfm(t)]v_2(t) = 2\pi a A_c\left[f_c + k_f m(t)\right]

Step 3: DC removal. A blocking capacitor removes 2πaAcfc2\pi a A_c f_c:

y(t)=2πaAckf m(t)  ∝  m(t)y(t) = 2\pi a A_c k_f\, m(t) \;\propto\; m(t)

Practical circuits:

  • Slope detector: a tuned circuit with resonance slightly above fcf_c; the carrier sits on its sloping skirt, so amplitude varies with frequency. Simple but non-linear.
  • Balanced slope detector: two tuned circuits at fc±δff_c \pm \delta f with diode detectors connected back to back; the output is the difference, giving an S-shaped, more linear response and no DC.
  • Foster–Seeley discriminator and ratio detector: use the phase shift of a double-tuned transformer.
  • Zero-crossing detector: counts zero crossings; the average of a pulse train triggered at each crossing is proportional to the instantaneous frequency.

Role of the limiter: the envelope detector also responds to amplitude noise. The limiter makes the input amplitude constant so that only frequency variations reach the output.

✓ Answer checked by Claude Opus 5.5 (high effort)

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