Definitions of tuning terms
© 1998 by Joseph L. Monzo
All definitions by Joe Monzo unless otherwise cited
spring
From John de Laubenfels,
Tuning
List posting:
First, about my general spring model. It is an analog of the physical
world; there, springs behave as follows: resisting force is proportional
to displacement times spring constant. The energy held by a spring is
the integral of force over distance of displacement, which works out to
being proportional to the SQUARE of displacement.
In my model, energy is the analog of
pain, refering to the displeasure
of our ears to out-of-tune intervals (chords being represented in this
model as a set of
dyads,
with some awareness of
otonal vs.
utonal
chords). Displacement is the analog of tuning motion, with the
rest point being exact
JI.
By setting up a big spring matrix and relaxing it successively, I can
minimize pain and hope to approach a nicely tuned piece (it can be
shown that minimum energy is equivalent to each node of the matrix
relaxing fully; i.e., having zero net force). For each sequence read
into the program, I create three kinds of springs:
There's more, of course: a minor third
in 12-tET is either 6/5 or 7/6,
and a major second has three possible JI
values (10/9, 9/8, or 8/7).
And, even a major third
might be 9/7 rather than 5/4! A part of the
program that is not always fully ideal at the moment makes the
decision about what JI intervals to shoot for in setting up the
vertical intervals in the spring matrix. At present, I do not modify
the target tuning of a spring once it is created.
[from Joe Monzo, JustMusic: A New Harmony]
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