ISRO Scientist/Engineer SC (Electronics) study materials
ISRO Scientist/Engineer SC (Electronics) study resources

ISRO Scientist/Engineer SC (Electronics): Communication Systems (Analog and Digital)

ISRO Scientist/Engineer SC (Electronics) · Work through your exam, one topic at a time.

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Communication Systems (Analog and Digital)

Communication Systems (Analog and Digital) tests modulation, bandwidth, noise performance, sampling and digital link budgets. Questions often ask for one number plus a reason.

Core rules

  • AM: s(t)=Ac[1+m cos ωmt]cos ωct; m≤1 avoids overmodulation. Bandwidth = 2fm. Sideband power fraction = m²/(2+m²).
  • FM: Carson's rule B ≈ 2(Δf + fm); modulation index β = Δf/fm. FM trades bandwidth for SNR.
  • Nyquist: fs ≥ 2fmax; PCM bit rate = n fs. Quantisation SNR for a full-scale sinusoid ≈ 6.02n + 1.76 dB.
  • Matched filter maximises SNR at sampling; BER for BPSK/QPSK is Q(sqrt(2Eb/N0)).
  • Shannon capacity C = B log2(1+S/N); it is an upper bound, not a modulation scheme.
  • Coherent detection needs carrier recovery; non-coherent detection is simpler but costs about 3 dB.

Worked example

A voice signal is sampled at 8 kHz and quantised to 8 bits. Bit rate = 8000×8 = 64 kbit/s. Quantisation SNR ≈ 6.02×8 + 1.76 = 49.9 dB for a full-scale sinusoid. If the signal occupies only half the full-scale range, SNR falls by 6 dB to about 43.9 dB. This is why companding is used in telephony: it preserves small-signal resolution.

Traps

  • Using 2fm for FM bandwidth instead of Carson's rule.
  • Forgetting the 1.76 dB term or applying the formula to a non-sinusoidal signal.
  • Confusing Eb/N0 with SNR without accounting for bandwidth.
  • Sampling at exactly Nyquist with non-ideal filters.
  • Assuming Shannon capacity is achievable with any simple scheme.