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Frequency-Response Matching Using
Digital Filter Design Methods
Given force inputs and velocity outputs, the frequency response
of an ideal mass was given in Eq.
(7.1.2) as
and the frequency response for a
spring was given by Eq.

(
7.1.3) as
Thus, an
ideal mass is an
integrator and an ideal spring is a
differentiator. The modeling problem for
masses and springs
can thus be posed as a problem in
digital filter design given
the above desired frequency responses. More generally, the
admittance
frequency response ``seen'' at the port of a general

th-order
LTI
system is, from Eq.

(
8.3),
 |
(9.14) |
where we assume

. Similarly, point-to-point
``trans-admittances'' can be defined as the velocity
Laplace transform
at one point on the physical object divided by the driving-force
Laplace transform at some other point. There is also of course no
requirement to always use driving force and observed velocity as the
physical variables; velocity-to-force, force-to-force,
velocity-to-velocity, force-to-acceleration, etc., can all be used to
define
transfer functions from one point to another in the system.
For simplicity, however, we will prefer admittance transfer functions
here.
Subsections
Previous: Delay Loop ExpansionNext: Ideal Differentiator (Spring Admittance)
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.