A while back, someone asked about total string tension and bearing changes with pitch changes. I'm sorry, I don't remember who. I didn't have anything set up specifically for this at the time, but I got curious and finally got around to chasing it down the other evening. Here's what I found. Using: Freq=fork*0.0625*2^((U-1)/12) Tension=((Freq*L*d)/20833)^2*(1+W*(D^2/d^2-1))+Ns where fork=pitch at A4, U=unison #, L=speaking length in inches, d=core diameter in mils, D=overall diameter in mils, Ns= number of strings in unison, and W=.89 for copper. In an unspecified 6 foot piano with bearing ranging from 1/2 degree in the bass, to a little over 1.5 degree in the treble, here are some of the results at different pitches. pitch total tension total bearing @445 40,487 655 @440 39,583 640 @435 38,688 626 @430 37,804 612 @425 36,930 597 The bearing angles would decrease as the tension was raised and the soundboard deflected, so the total bearing load deviation should be less than these figures would indicate, centered around the 640 @ A440. It would take way too much time and effort to set the bearing load and angle routines up to reflect the change unless it was actually good for something besides being really neat, so this will have to do for now. The tension figures should be pretty close unless I messed something up. This should give you and me a rough idea of what a piano has to accommodate in load change with a pitch correction. It also indicates to me that I overestimated the effect of tension changes on soundboard load, and therefore deflection, and that Dr. Sanderson was most likely correct in saying that plate flex is a bigger factor in pitch drop during a pitch raise. A bit more evidence toward obtaining part of a complete education. If anyone cares, you're welcome. If anyone has corrections on my method, I'm interested. This is the sort of thing it's hard to get answers to. Ron
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