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We have just discussed the coupling between vertical and horizontal
planes of vibration along a single string. There is also important
coupling among different strings on the same instrument. For example,
modern pianos are constructed having up to three physical strings
associated with each key. These strings are slightly mistuned in
order to sculpt the shape of the decay envelope, including its beating
characteristics and two-stage decay. A two-stage decay is desired in
piano strings in order to provide a strong initial attack followed by
a long-sustaining ``aftersound'' [547], [18, Weinreich
chapter].
A simple approximation to the effect of coupled strings is obtained by
simply summing two or more slightly detuned strings. While this can
provide a realistic beating effect in the amplitude envelope, it does
not provide a true two-stage decay. A more realistic simulation of
coupling requires signal to flow from each coupled string into all
others.
When the bridge moves in response to string vibrations, traveling
waves are generated along all other strings attached to the bridge.
In the simplest case of a bridge modeled as a rigid body, the
generated wave is identical on all strings. In
§C.13, an efficient scattering formulation
of string coupling at a bridge is derived for this case
[443]. It can be seen as a simplification of the
general coupling matrix shown in Fig.6.20 for the two-string
(or two-polarization) case. Additionally, an eigenanalysis of the
coupling matrix is performed, thereby extending the analysis of
§6.12.2 above.
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