Depending on the modulation index chosen, the carrier and certain sideband frequencies may actually be suppressed. Zero crossings of the Bessel functions, Jn(β), occur where the corresponding sideband, n, disappears for a given modulation index, β. The composite spectrum for a single tone consists of lines at the carrier and upper and lower sidebands (of opposite phase), with amplitudes determined by the Bessel function values at those frequencies.| FM General Equation | |||||
| Let the carrier be xc(t) = Xc·cos (Ωct), and the modulating signal be xm(t) = β·sin (Ωmt) | Then x(t) = Xc·cos [Ωct + β·sin (Ωmt)] | ||||
| Modulation Index | |||||
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| Narrowband FM (NBFM) | |||||
Narrowband FM is defined as the condition where β is small enough to make all terms after the first two in the series expansion of the FM equation negligible. Narrowband Approximation: β = Δω/Ωm < 0.2 (could be as high as 0.5, though) BW ~ 2ωm | |||||
| Wideband FM (WBFM) | |||||
| Wideband FM is defined as when a significant number of sidebands have significant amplitudes. BW ~ 2Δω | |||||
| Carson's Rule | |||||
| J.R. Carson showed in the 1920's that a good approximation that for both very small and very large β, BW ~ 2 (Δω + Ωm/sub>)) = 2*Ωm/sub> (1 + β) | |||||
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