Sign in

username:

password:



Not a member?

Search Online Books



Search tips

Free Online Books

Chapters

Chapter Contents:

Search Physical Audio Signal Processing

  

Book Index | Global Index


Would you like to be notified by email when Julius Orion Smith III publishes a new entry into his blog?

  

Wave Digital Mass

In the case of a mass $ m$, we have

$\displaystyle R(s) = ms
$

which implies its reflectance is, from Eq.$ \,$(Q.13),

$\displaystyle S_m(s) = \frac{ms - R_0}{ms + R_0}
$

Setting $ R_0= m$ gives

$\displaystyle S_m(s) = \frac{s - 1 }{s + 1}
$

and this choice also turns out to eliminate the delay-free path in the digital version. In view of the expression for the inverse bilinear transform in Eq.$ \,$(Q.12), i.e., $ z=(1+s)/(1-s)$, the bilinear transform of $ S(s)$ is immediately seen to be

$\displaystyle \fbox{$\displaystyle \tilde{S}_m(z) = -z^{-1}$}
$

where we defined $ \tilde{S}_m(z) \isdef S_m\left(\frac{z-1}{z+1}\right)$. The corresponding difference equation for the wave digital mass is

$\displaystyle f^{{-}}(n) = - f^{{+}}(n-1)
$

and its wave flow diagram is drawn in Fig.Q.2.

Figure Q.2: Wave flow diagram for the wave digital mass. Note that the wave variables are written in the time domain as is customary in digital filter diagrams, while it would be more consistent (with the $ z^{-1}$ block) to keep them in the frequency domain as $ F^{+}(z)$ and $ F^{-}(z)$.
\includegraphics{eps/lWaveDigitalMass}

Thus, the wave digital mass is simply a unit-sample delay and a negation. The fact that the value of the mass has been canceled out will be addressed below in the subsection on ``adaptors,'' i.e., it only affects interconnection with other elements. For now, just remember that the reference impedance was chosen to be equal to the mass in order to get this simple wave flow diagram. Also note that the WDF mass simulator has no delay-free path from input to output.


Order a Hardcopy of Physical Audio Signal Processing

Previous: Summary of Wave Digital Elements
Next: Wave Digital Spring

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.


Comments


No comments yet for this page


Add a Comment
You need to login before