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Physics · Ch 15 — Communication Systems

Amplitude Modulation

15.8

Amplitude Modulation

Amplitude Modulation

In amplitude modulation (AM), the amplitude of the carrier wave is varied in proportion to the instantaneous value of the message signal, while the carrier's frequency stays fixed.

Taking a carrier c(t)=Acsin⁡(ωct)c(t) = A_c\sin(\omega_c t) and a message/modulating signal m(t)=Amsin⁡(ωmt)m(t) = A_m\sin(\omega_m t) (with ωm=2πfm\omega_m = 2\pi f_m), the amplitude-modulated signal is:

cm(t)=(Ac+Amsin⁡(ωmt))sin⁡(ωct)(Eq. 15.3)c_m(t) = (A_c + A_m\sin(\omega_m t))\sin(\omega_c t) \quad \text{(Eq. 15.3)}

which can be rewritten as:

cm(t)=Ac[1+μsin⁡(ωmt)]sin⁡(ωct)(Eq. 15.4)c_m(t) = A_c\left[1 + \mu\sin(\omega_m t)\right]\sin(\omega_c t) \quad \text{(Eq. 15.4)}

where μ=Am/Ac\mu = A_m/A_c is the modulation index, kept at or below 1 in practice to avoid distortion of the transmitted signal.

Using the identity sin⁡Asin⁡B=12[cos⁡(A−B)−cos⁡(A+B)]\sin A\sin B = \tfrac{1}{2}[\cos(A-B) - \cos(A+B)], Eq. 15.4 expands to:

cm(t)=Acsin⁡(ωct)+μAc2cos⁡[(ωc−ωm)t]−μAc2cos⁡[(ωc+ωm)t](Eq. 15.5)c_m(t) = A_c\sin(\omega_c t) + \frac{\mu A_c}{2}\cos\left[(\omega_c-\omega_m)t\right] - \frac{\mu A_c}{2}\cos\left[(\omega_c+\omega_m)t\right] \quad \text{(Eq. 15.5)} …

Figure 15.9A plot of amplitude versus omega for an amplitude modulated signal.

What this figure shows. Line spectrum plot, vertical axis 'Amplitude' with two marked levels A_c (top, dotted horizontal line) and muA_c/2 (lower, dotted horizontal line); horizontal axis 'omega in radians' (unlabelled scale) extending to the right with an arrowhead. Three vertical solid lines (spectral lines) rise from the axis: a shorter line at (omega_c - omega_m) reaching the muA_c/2 level, a taller line at omega_c reaching the A_c level, and another shorter line at (omega_c + omega_m) reaching the mu*A_c/2 level, the classic AM spectrum with a tall carrier line flanked by two shorter sym …