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Example AM Spectra

Equation (4.4) can be used to write down the spectral representation of $ x_m(t)$ by inspection, as shown in Fig.4.12. In the example of Fig.4.12, we have $ f_c=100$ Hz and $ f_m=20$ Hz, where, as always, $ \omega=2\pi f$. For comparison, the spectral magnitude of an unmodulated $ 100$ Hz sinusoid is shown in Fig.4.6. Note in Fig.4.12 how each of the two sinusoidal components at $ \pm100$ Hz have been ``split'' into two ``side bands'', one $ 20$ Hz higher and the other $ 20$ Hz lower, that is, $ \pm100\pm20=\{-120,-80,80,120\}$. Note also how the amplitude of the split component is divided equally among its two side bands.

Figure: Spectral magnitude representation of the sinusoidally modulated sinusoid $ \sin(40\pi t)\sin(200\pi t)$ defined in Eq.$ \,$(4.3). Phase is not shown.
\begin{figure}\input fig/sineamfd.pstex_t
\end{figure}

Recall that $ x_m(t)$ was defined as the second term of Eq.$ \,$(4.1). The first term is simply the original unmodulated signal. Therefore, we have effectively been considering AM with a ``very large'' modulation index. In the more general case of Eq.$ \,$(4.1) with $ a_m(t)$ given by Eq.$ \,$(4.2), the magnitude of the spectral representation appears as shown in Fig.4.13.

Figure: Spectral representation of the sinusoidally modulated sinusoid $ [1+ \sin(40\pi t)]\sin(200\pi t)$ from Eq.$ \,$(4.1), with $ \alpha =1$, and $ a_m(t)$ given by Eq.$ \,$(4.2).
\begin{figure}\input fig/sineamgfd.pstex_t
\end{figure}


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Next: Sinusoidal Frequency Modulation (FM)

written by Julius Orion Smith III
Julius Smith's background is in electrical engineering (BS Rice 1975, PhD Stanford 1983). He is presently Professor of Music and Associate Professor (by courtesy) of Electrical Engineering at Stanford's Center for Computer Research in Music and Acoustics (CCRMA), teaching courses and pursuing research related to signal processing applied to music and audio systems. See http://ccrma.stanford.edu/~jos/ for details.


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