How Modulating Amplitude Affects FM Bandwidth (Mathematical Derivation)
1. FM Signal Definition
s(t) = Ac cos(2π fc t + φ(t))
Where the phase is:
φ(t) = 2Ï€ kf ∫ m(t) dt
- kf = frequency sensitivity (Hz/Volt)
- m(t) = modulating signal
2. Sinusoidal Modulating Signal
m(t) = Am cos(2Ï€ fm t)
Integrating:
∫ m(t) dt = (Am / 2Ï€ fm) sin(2Ï€ fm t)
Substitute into phase:
φ(t) = (kf Am / fm) sin(2π fm t)
3. Modulation Index
β = kf Am / fm
FM signal becomes:
s(t) = Ac cos(2π fc t + β sin(2π fm t))
4. Frequency Deviation
Δf = kf Am
Δf ∝ Am
5. FM Spectrum (Bessel Expansion)
s(t) = Ac Σ Jn(β) cos(2π(fc + n fm)t)
- Jn(β) = Bessel functions
- Number of significant sidebands depends on β
As β increases, more sidebands become significant → wider spectrum.
6. Carson’s Rule
B ≈ 2(Δf + fm)
Substitute Δf:
B ≈ 2(kf Am + fm)
7. Final Relationship
B ∝ Am (for constant fm and kf)
Interpretation
- Increase Am → increases Δf
- Increases modulation index β
- More sidebands appear
- Bandwidth increases
Conclusion
Am ↑ → Δf ↑ → β ↑ → Bandwidth ↑