Regarding a formula for calculating the longitudinal mode partial, this is what I am using: LM=100355/(SQRT(((OD^2/CD^2)*(WM/100))+0.11)*L) where LM is longitudinal mode frequency in Hz OD is the overall diameter, including wound string wrap, in thousandths of an inch CD is the core wire diameter, in thousandths of an inch WM is a constant specific to the wrap material, for copper, 89 and L is speaking length., in inches I'll let you deal with the metric conversions. I am in China at the moment, and do not have access to my library, but I believe I got that formula from a book on longitudinal mode partials, written by Ellis? and available, I think, from the PTG store. I am not a mathematician, so I cannot confirm the veracity of this formula, but you can take it for what it is worth, or buy the book from PTG. Regarding Harold Conklin's work, I worked for Baldwin for 10 years and had access to Mr. Conklin's research notes, fascinating material. His winding machinery was rather complex, but Baldwin's string maker, at the time, did produce strings to his specifications, although the more practice machinery that they used to make the strings was not as precise as he had envisioned in his design. A weakness of his wound string design was that the core wires were of an unusually small diameter, and prone to breaking more easily than "typical" bass strings. To some extent, what was gained in avoidance of conflicts between longitudinal partials and harmonic transverse partials was lost in string longevity in heavy use environments (that is, very heavy handed pianists). Frank Emerson
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