Ron writes:
>I never have liked the strings of a unison moving in opposition theory.
>I don't think that's even possible in a piano.
Hot damn, chaos comes again!
This is how it seems to me:
If two strings are struck, it is not logical to me that the system will
be so perfect that they move in phase, and the least bit out of phase will
create, due to coupling, an alternating system of energy transfer between the
two. In a coupled system, if one string is unstruck and another is, the
unstruck string will begin moving, but it will NOT move in phase with the
first. It will absorb energy from the struck string and, in an attempt to
"catch-up", will lag behind. At some point, energy will equalize and the
two strings will go in and out of phase, but the period at which they will be
in phase is temporal.
With three strings struck, there is a tertiary transfer created which is
far more complex and contains more resultant modes of vibration, and the
three strings will never be totally in phase.
I can't see these things happening, but the logic of G. Weinreich seems to
explain what I hear happening as I fecklessly move strings around while
listening to the results. There is a fixed amount of energy in the string
when set into motion, so faster transfer (via bridge movement) to the
soundboard will result in greater momentary amplitude but faster decay. The
unison that contains its own choral effect will seemingly go on longer. I
think a really good tuner can manipulate the unison to give the best
compromise. Setting three strings of all unisons to "dead-on" ETD setting
will not only create some unisons better than others, but will often create
unisons that lack the sustain of the micro-mistuned ones. I think the ear is
the better judge of unisons because of this.
My normal unison is formed by setting two strings to the SAT, and then
tuning the middle string aurally. This allows a more consistant sounding set
of unisons, and I feel like the piano's sustain is brought under my control.
It also side-steps the question of flattening of the unison by the addition
of the second or third string. I don't see that in my results, and even so,
it appears that what Virgil Smith is pointing out as an effect of unison
flattening is in the .3 or less cent range, and that is easily obviated by
choice of stretch made earlier.
Regards,
Ed Foote
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