Effects of the DC component

Multiplying out the above equation, we obtain

$\displaystyle x(t) = A_0\cos(2\pi f_c t) + \cos(2\pi f_\Delta t)\cos(2\pi f_c t).
$

The carrier frequency is now present in the spectrum.

The second term can be expanded in the same way as was done for RM (i.e. the sidebands are identical).

Figure 7: Spectrum of amplitude modulation.
\begin{figure}\centerline{%
\input{amspec.pstex_t}}\end{figure}


``Music 171: Amplitude Modulation'' by Tamara Smyth, Department of Music, University of California, San Diego (UCSD).
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Copyright © 2019-11-05 by Tamara Smyth.
Please email errata, comments, and suggestions to Tamara Smyth<trsmyth@ucsd.edu>