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Exponentially Decaying Traveling Waves

Let $ g(r,\omega)$ denote the decay factor associated with propagation of a plane wave over distance $ r$ at frequency $ \omega $ rad/sec. For an ideal plane wave, there is no ``spreading loss'' (attenuation by $ 1/r$). Under uniform conditions, the amount of attenuation (in dB) is proportional to the distance traveled; in other words, the attenuation factors for two successive segments of a propagation path are multiplicative:

$\displaystyle g(r_1+r_2,\omega) =
g(r_1,\omega)g(r_2,\omega)
$

This property implies that $ g$ is an exponential function of distance $ r$.3.3

Frequency-independent air absorption is easily modeled in an acoustic simulation by making the substitution

$\displaystyle z^{-1}\leftarrow gz^{-1}
$

in the transfer function of the simulating delay line, where $ g$ denotes the attenuation associated with propagation during one sampling period ($ T$ seconds). Thus, to simulate absorption corresponding to an $ M$-sample delay, the difference equation Eq.$ \,$(2.1) on page [*] becomes

$\displaystyle y(n) = g^Mx(n-M),
$

as depicted in Fig.2.9.


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Next: Frequency-Dependent Air-Absorption Filtering

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About the Author: 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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