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Early Reflections

The ``early reflections'' portion of the impulse response of a reverberant environment is often taken to be the first 100ms or so [294]. However, for greater accuracy, it should be extended to the time at which the reverberation reaches its asymptotic statistical behavior.3.5

Since the early reflections are relatively sparse and span a relatively short time, they are often implemented using tapped delay lines (TDL). This idea was apparently first suggested by Schroeder in 1970 [390] and evidently first implemented by Moorer [294].

If the computation is affordable, it is best to spatialize the early reflections [233] so that they come from the right directions in 3D space. It is known [57] that the early reflections have a strong influence on spatial impression, i.e., the listener's perception of the listening-space shape.

Figure 2.3 shows a general schematic of a reverberator with separate implementations of early and late reverberation. The taps on the TDL may include lowpass filtering for simulation of air absorption.

While the late reverb logically begins when the early reflections end, as implemented in Fig. 2.3, it may be more cost-effective in practice to feed the ``late reverb'' unit from an earlier tap (or set of taps) from the TDL, thus overlapping them somewhat. This can help when the late reverberator needs time to build up to full density.

Figure 2.3: Division of a reverberator into early and late sections.
\begin{figure}\input fig/revsplit.pstex_t
\end{figure}

It is often the case that early reflections can be worked into the late-reverberation simulation. For example, usually there are long delay lines in which the input signal can be summed at various points, thereby implementing a transposed tapped delay line (see §1.5.2).


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[How to cite and copy this work] 
``Physical Audio Signal Processing for Virtual Musical Instruments and Digital Audio Effects'', by Julius O. Smith III, (December 2005 Edition).
Copyright © 2006-07-01 by Julius O. Smith III
Center for Computer Research in Music and Acoustics (CCRMA),   Stanford University
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