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Interpretation of the Time-Domain KW Converter

As shown above, driving a single displacement sample $ y_{n,m}$ in the FDTD corresponds to driving a velocity input at position $ m$ on two alternating subgrids over time. Therefore, the filter $ H(z)=1-z^{-2}$ acts as the filter $ H(z)=1-z^{-1}$ on either subgrid alone--a first-order difference. Since displacement is being simulated, velocity inputs must be numerically integrated. The first-order difference can be seen as canceling this integration, thereby converting a velocity input to a displacement input, as in Eq.$ \,$(P.23).


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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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