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Force Waves at a Rigid Termination

To find out how force waves recoil from a rigid termination, we may convert velocity waves to force waves by means of the Ohm's law relations of Eq. (4.6), and then use Eq. (4.10), and then Eq. (4.6) again:

\begin{eqnarray*}
f^{{+}}(n) &=&Rv^{+}(n) \,\mathrel{\mathop=}\,-Rv^{-}(n) \,\ma...
...el{\mathop=}\,Rv^{+}(n-N/2) \,\mathrel{\mathop=}\,f^{{+}}(n-N/2)
\end{eqnarray*}

Thus, force waves reflect from a rigid termination with no sign inversion:5.1

\begin{eqnarray*}
f^{{+}}(n) &=& f^{{-}}(n) \\
f^{{-}}(n+N/2) &=& f^{{+}}(n-N/2)
\end{eqnarray*}


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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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