Hi to all: One of my pet peeves is the passing on of information saying that the higher partials run sharp because of the space which the nodes take up. Such an article ran in the 1949 series of the Piano Technician by George --------. If you simply look at the nodal point of any sine wave, the bending takes place at the loops, not at the nodes. The nodes are the pivot points. Stiffness does affect the higher partials more than the lower partials, but it's not because of the nodes. The very high partials are more rod like than string like. I used to demonstrate this by having a very flexible felt temperament strip in my hand. Its longer segments (partials) would vibrate quite freely and for a longer time when held between my two outstretched arms (tension being the chief restorative force). But, if I had just a short segment (1/2 inch) protruding from between two fingers, I could flip it with the other hand and it would vibrate like a rod (stiffness being the only restoring factor) The stiffer a segment is, the more like a rod will it vibrate. The second partial of a rod (tuning fork) is more than 2 1/2 octaves above the fundamental. Check it out. The clang tone of an A4 fork is sharper than E7. Of course piano strings are not nearly that stiff, but it is a good example of what stiffness can do. In piano strings we have two restorative forces acting at once. Tension and stiffness. After striking a string, the tension tends to bring it eventually to a place of rest. But, stiffness also plays a very small part. Flexible strings such as guitar or violin strings have little or no measureable inharmonicity. With piano strings, you can measure it. Bowed piano strings do not show inharmonicity according to experiments which others have done (I tried, but without rosin, I could not get a steady state going). My violin strings do exhibit a strange phenomenon in that the fundamental of a bowed string gives a higher pitch that the same plucked string (drives me bananas). Or, if I bow a string and lift the bow, the residual pitch immediately drops. The only explanation I have for this is that when the bow is lifted, the additional tension provided by the bowing is removed. But, I don't think it has anything much to do with inharmonicity. If inharmonicity only is considered in the scaling of a piano, one could end up with a very weak but clear sounding piano. Tension and projection are equally important. Early pianos were designed with no consideration of inharmonicity. Some made no sense at all. Others were designed with very smooth tension as the primary consideration. The resultant inharmonicity jumps made it difficult to keep the 3rds, 10ths and 17ths running smoothly up the scale without distorting the octaves and vice versa. The early Yamaha and Kawai grands had generally lower inharmonicity than they do now. Their designers apparently feel that power is more in demand today than before. They still maintain fairly smooth scales. The effects of poor inharmonicity show up more in small scaled pianos which in order to maintain power have thicker strings in the tenor and/or resort to having wound strings placed in that area to help maintain power. This is not a bad idea, but they are just seldom properly balanced. If one used the longest plain strings in the tenor which would not crowd the soundboard perimeter too closely, and then had foreshortened wound strings blended in to fit with the tension and inharmonicity of the plain strings, those scales would be more easily tuneable and the voicers would have fewer difficulties in blending in the tone going across the break. Of course, this would require some changes in the tenor bridge to accommodate the shorter wound strings. The Walter piano is a good example of proper blending across the break (the Verticals or the Grands). It should be noted that they wisely avoided wound strings on the Tenor bridge and provided the proper length differential between the upper Bass wound strings and the lower Tenor plain strings. Jim Coleman, Sr.
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