Modulation Index cont.

Without going any further in solving this equation, it is possible to get a sense of the effect of the modulation index $ I(t)$ from

$\displaystyle f_i(t)$ $\displaystyle =$ $\displaystyle f_c - I(t)f_m\sin(2\pi f_mt + \phi_m) +$  
    $\displaystyle \qquad \qquad \frac{dI(t)}{dt}\cos(2\pi f_mt + \phi_m)/2\pi.$  

We may see that if $ I(t)$ is a constant (and it's derivative is zero), the third term goes away and the instantaneous frequency becomes

$\displaystyle f_i(t) = f_c - I(t)f_m\sin(2\pi f_mt + \phi_m).
$

Notice now that in the second term, the quantity $ I(t)f_m$ multiplies a sinusoidal variation of frequency $ f_m$, indicating that $ I(t)$ determines the maximum amount by which the instantaneous frequency deviates from the carrier frequency $ f_c$.

Since the modulating frequency $ f_m$ is at audio rates, this translates to addition of harmonic content.

Since $ I(t)$ is a function of time, the harmonic content, and thus the timbre, of the synthesized sound may vary with time.


``Music 270a: Modulation'' by Tamara Smyth, Department of Music, University of California, San Diego (UCSD).
Download PDF version (modulation.pdf)
Download compressed PostScript version (modulation.ps.gz)
Download PDF `4 up' version (modulation_4up.pdf)
Download compressed PostScript `4 up' version (modulation_4up.ps.gz)

Copyright © 2019-10-28 by Tamara Smyth.
Please email errata, comments, and suggestions to Tamara Smyth<trsmyth@ucsd.edu>