David: >St three days without posting, I know this thread seems to have >gracefully gone it's way, but I'll try, nevertheless, to cobble >together the various thoughts I had had. 8 days now and counting. I think it's dead. Let's try moving it to to pianotech and see what comes out of the woodwork. I love hypothetical pianos. Lots of questions....Some speculative answers, and a comment on some experiments with low friction bearings. >Your hypothetical piano questions address tunability, tuning >stability, and the effect of bearing point friction upon the wave >form and wave duration. What is it you are trying to accomplish? >The Boston model that inspired this thread would seem to have some >significant design issues in this area, but is the implication that >the basic concept (pin block, tuning pin, etc.) is inadequate? The specifics of the Boston problem (obviously important to the original question) aren't relevant to my hypothetical piano. I'd say this addresses the first two questions directly, and the last point indirectly (and unpredictably). It also allows you to use a long backlength without the concern it will unduly affect stability. >Tunability would depend upon the level of refinement of the >mechanical system that would control the tension. I don't have the >information readily available that correlates tension with >frequency, but such a system would have to be able to acheive, in a >linear fashion, what we do with the combination of turning the pin, >flexing the pin, test blows, etc. Not necessarily. A regular tuning system, as long as it was reasonably secure, would work just as well as for a regular configuration. As for test blows, you wouldn't need any, because tension would instantly equalize in the various string sections as soon as it is changed. >Tuning Stability - I don't remember if a recent (?) past thread ever >determined exactly why strings go out of tune. Is the assumption >that, by reducing friction at bearing points, the tension of the >various lengths will be more equalized than what we generally >achieve, and thus, less prone to change? Longest strings (overall wires) minimizes the effects of any instability on pitch. >What tension values (or range of values) would you insert into a >formula that described the tension relationships between the various >sections in a stably tuned string? How much variation in tension >would be viable between the front section and vibrating section; >between the latter and the back length? How do you measure that >tension? First two points would depend on whether friciton at the bearing is actual zero, or just minimal. Tension is easy to measure in experiments, simply by monitoring pitch. I've done experiments with minimized friction bearings. You set up two equal string segments and equal pitches, then crank the tension up and down. The extent to which the pitch in the segments varies is a proxy for the tension variation and that is a measure of how low the friction is in the bearings. Several cycles up and down will give a hysteresis loop, unless the bearing friction is zero. If this topic is interesting I would consider writing up the results for the journal. >Does the friction at the agraffe and bridge pin have any role in the >definition and containment of vibrational energy or is that solely a >function of deflection? I suspect not, since the string is stiff, and the motion is primarily in the directions perpendicular to the string. Longitudinal virbrations will pass through bridge pins anyway, friction of not. >Why do you say that the longer the non-speaking length, the better? Because, with say zero friction bearings, any change in string tension from sideways excursion (e.g. when struck), will be (temporarily) distributed over the entire wire, not just the speaking length. So the the proportional change in length (strain) is less, and so is the change in stress, and so is change in pitch. >Why, from what's been discussed, do you find "same total string >lengths within trichord" to be advantageous? Because any instability in the length will transfer to a strain change. If the instability is about the same for each string in the trichord, the strain change in each will be similar, and so will the pitch change. The trichord would stay locked, even it it goes out of tune a bit. Stephen -- Dr Stephen Birkett Piano Design Lab Department of Systems Design Engineering University of Waterloo, Waterloo ON Canada N2L 3G1 tel: 519-888-4567 Ext. 3792 Lab room E3-3160 Ext. 7115 mailto: sbirkett[at]real.uwaterloo.ca http://real.uwaterloo.ca/~sbirkett
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