Chirp Sinusoid

Now, let's make the phase quadratic, and thus non-linear with respect to time.

$\displaystyle \theta(t) = 2\pi\mu t^2 + 2\pi f_0 t + \phi.
$

The instantaneous frequency (the derivative of the phase $ \theta$), becomes

$\displaystyle \omega_i(t) = \frac{d}{dt}\theta(t) = 4\pi\mu t+ 2\pi f_0,
$

which in Hz becomes

$\displaystyle f_i(t) = 2\mu t + f_0.
$

Notice the frequency is no longer constant but changing linearly in time.

To create a sinusoid with frequency sweeping linearly from $ f_1$ to $ f_2$, consider the equation for a line $ y = mx + b$ to obtain

$\displaystyle f(t) = \frac{f_2-f_1}{2T}t + f_1,
$

where $ T$ is the duration of the sweep.


``Music 270a: Modulation'' by Tamara Smyth, Department of Music, University of California, San Diego (UCSD).
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Copyright © 2019-10-28 by Tamara Smyth.
Please email errata, comments, and suggestions to Tamara Smyth<trsmyth@ucsd.edu>