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Nonlinear Spring Model
In the musical acoustics literature, the piano hammer is classically
modeled as a nonlinear spring
[493,63,178,76,60,486,164].10.14Specifically, the piano-hammer damping in Fig.9.22 is
typically approximated by
, and the spring
is
nonlinear and memoryless according to a simple power
law:
where

for a linear spring, and generally

for pianos. A
fairly complete model across the piano keyboard (based on acoustic
piano measurements) is as follows [
487]:
The upward force applied to the string by the hammer is therefore
 |
(10.20) |
This force is balanced at all times by the downward string force
(string tension times slope difference), exactly as analyzed in
§
9.3.1 above.
Previous: Piano Hammer ModelingNext: Including Hysteresis
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.