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Vocoder Analysis


\begin{psfrags}
% latex2html id marker 28314\psfrag{x} []{ \normalsize$ x(t)$\...
...s/vocoder}
\caption{Channel vocoder block diagram.}
\end{figure}
\end{psfrags}

Vocoders decompose a signal into subbands. For each subband, either the magnitude (in the case of the channel vocoder), or the magnitude and phase (for the phase vocoder) is determined.

If we assume that we have at most 1 sinusoid with time varying parameters in each channel, then we can write down the following expression for $ x_k(t)$, the signal in the $ k^{th}$ subband:

$\displaystyle x_k(t)=a_k(t)\cos[ \omega_kt + \phi_k(t) ]
$

In the above expression, $ a_k(t) $ is an amplitude modulation term, $ \omega_k$ is a fixed channel center frequency, and $ \phi_k(t)$ is a phase (or frequency) modulation. Using these parameters, we can re-synthesize the signal using the oscillator summation.11.1Typically, the instantaneous phase modulation $ \phi_k(t)$ is differentiated to obtain instantaneous frequency deviation:

$\displaystyle \Delta \omega_k(t) \mathrel{\stackrel{\Delta}{=}}\frac{d}{dt} \phi_k(t)
$

Figure 10.8: Illustration of channel vocoder parameters in analysis (left) and synthesis (right).
\includegraphics[width=\textwidth]{eps/pvchan}


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Next: Computing the Vocoder Parameters

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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