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Need for modulation; single tone AM expressions

Short answer

Modulation varies carrier amplitude, frequency, or phase. It is needed for practical antenna size, multiplexing, efficient radiation. Single-tone AM: s(t) = A_c[1+μ cos ω_m t] cos ω_c t; spectrum has carrier at f_c and sidebands at f_c±f_m with amplitude μA_c/2.

What do you understand by modulation? Why modulation is needed? Find the time and frequency domain expressions for standard AM wave for single tone message signal.

Modulation

Modulation is the process in which some characteristic (amplitude, frequency or phase) of a high-frequency carrier wave is varied in accordance with the instantaneous value of the message (modulating) signal. In amplitude modulation (AM) the carrier amplitude is varied.

Need for modulation

  1. Practical antenna height: antenna length ≈λ/4\approx\lambda/4; for 10 kHz audio it would be 7.5 km, but for a 1 MHz carrier only 75 m.
  2. Multiplexing: different stations use different carriers, so many signals share the same channel without interference.
  3. Efficient radiation and long range: high-frequency signals radiate and propagate much better.
  4. Narrowbanding: reduces the ratio of highest to lowest frequency, so one antenna and amplifier design works.
  5. Noise reduction: wideband schemes (FM) improve SNR.
  6. Channel matching: shifts the signal into the frequency band suited to the medium.

Time-domain expression of single-tone AM

Let the message be m(t)=Amcos⁡ωmtm(t)=A_m\cos\omega_mt and carrier c(t)=Accos⁡ωctc(t)=A_c\cos\omega_ct, with fc≫fmf_c\gg f_m. In standard AM the envelope is Ac+m(t)A_c+m(t):

s(t)=[Ac+Amcos⁡ωmt]cos⁡ωct=Ac[1+μcos⁡ωmt]cos⁡ωct,μ=AmAc\begin{aligned} s(t)&=[A_c+A_m\cos\omega_mt]\cos\omega_ct\\ &=A_c[1+\mu\cos\omega_mt]\cos\omega_ct,\qquad \mu=\frac{A_m}{A_c} \end{aligned}

where μ\mu is the modulation index (0≤μ≤10\le\mu\le1). Using cos⁡Acos⁡B=12[cos⁡(A+B)+cos⁡(A−B)]\cos A\cos B=\frac{1}{2}[\cos(A+B)+\cos(A-B)]:

s(t)=Accos⁡ωct⏟carrier+μAc2cos⁡(ωc+ωm)t⏟USB+μAc2cos⁡(ωc−ωm)t⏟LSBs(t)=\underbrace{A_c\cos\omega_ct}_{\text{carrier}}+\underbrace{\frac{\mu A_c}{2}\cos(\omega_c+\omega_m)t}_{\text{USB}}+\underbrace{\frac{\mu A_c}{2}\cos(\omega_c-\omega_m)t}_{\text{LSB}}
       Ac(1+mu)
   .-.   envelope    .-.
  /   \             /   \
 /     \    .-.    /     \   <- carrier inside envelope
        \  /   \  /
         '-     '-  Ac(1-mu)

Frequency-domain expression

Using cos⁡2πf0t↔12[δ(f−f0)+δ(f+f0)]\cos2\pi f_0t\leftrightarrow\frac{1}{2}[\delta(f-f_0)+\delta(f+f_0)]:

S(f)=Ac2[δ(f−fc)+δ(f+fc)]+μAc4[δ(f−fc−fm)+δ(f+fc+fm)]+μAc4[δ(f−fc+fm)+δ(f+fc−fm)]\begin{aligned} S(f)&=\frac{A_c}{2}\left[\delta(f-f_c)+\delta(f+f_c)\right]\\ &+\frac{\mu A_c}{4}\left[\delta(f-f_c-f_m)+\delta(f+f_c+f_m)\right]\\ &+\frac{\mu A_c}{4}\left[\delta(f-f_c+f_m)+\delta(f+f_c-f_m)\right] \end{aligned}
                 S(f)
       Ac/2               Ac/2
 muAc/4 |  muAc/4  muAc/4 |  muAc/4
   |    |    |       |    |    |
 --+----+----+---+---+----+----+--> f
  -fc-fm -fc -fc+fm 0 fc-fm fc fc+fm

Key results

  • Bandwidth: B=(fc+fm)−(fc−fm)=2fmB=(f_c+f_m)-(f_c-f_m)=2f_m.
  • Power: Pc=Ac22P_c=\frac{A_c^2}{2}, each sideband μ2Ac28\frac{\mu^2A_c^2}{8}, so total Pt=Pc(1+μ22)P_t=P_c\left(1+\frac{\mu^2}{2}\right).
  • Efficiency: η=μ22+μ2\eta=\frac{\mu^2}{2+\mu^2}; maximum 33.3% at μ=1\mu=1.

Example: Ac=10A_c=10 V, μ=0.5\mu=0.5, fc=1f_c=1 MHz, fm=1f_m=1 kHz gives lines of 10 V at 1 MHz and 2.5 V at 0.999 MHz and 1.001 MHz; bandwidth 2 kHz.

✓ Answer checked by Claude Opus 5.5 (high effort)

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