Path: utzoo!utgpu!news-server.csri.toronto.edu!cs.utexas.edu!usc!wuarchive!udel!rochester!pt.cs.cmu.edu!o.gp.cs.cmu.edu!andrew.cmu.edu!nsv+ From: nsv+@andrew.cmu.edu (Ned S. VanderVen) Newsgroups: comp.music Subject: Re: Musical Frequencies Message-ID: Date: 21 Dec 90 23:56:16 GMT References: <4193@mindlink.UUCP>, <506@anaxagoras.ils.nwu.edu> Organization: Physics, Carnegie Mellon, Pittsburgh, PA Lines: 45 In-Reply-To: <506@anaxagoras.ils.nwu.edu> As several recent posts have noted, the stiffness of real strings results in inharmonicity of the series of normal mode frequencies (characteristic frequencies of vibration), and to compensate for this the octaves must be "stretched." But all the explanations posted so far have described the phenomenon incorrectly. First of all, the stiffness results in a series of normal mode frequencies that are sharp, not flat, compared with the harmonic series, and these departures from the harmonic series become progressively sharper for the higher modes of the string. Secondly, a note is not "stretched" in order that its perceived pitch sound "correct" when played alone. Octaves are stretch-tuned in order that the two notes will be relatively free of beats when sounded together. To illustrate how this works, suppose that because of inharmonicity a string of fundamental frequency f has a second-mode frequency of 2.02 f rather than the harmonic value of exactly 2 f. The string sounding an octave higher should be tuned so that its fundamental is equal to the second mode frequency of the lower note in order that no beats be heard when the notes are sounded together. In this example the octave would have to be tuned to a fundamental frequency of 2.02 f to reduce the beat frequency to zero. This sharpening of the octave is the phenomenon of "stretching." The situation is actually more complicated than this because the fourth mode of the lower string will beat with the second mode of the upper string, and no tuning will eliminate all the beats. In practice the tuner will adjust for the most consonant interval, and stretching inevitably results. The inharmonicity depends on several factors: the diameter, length, tension, and elastic modulus of the string. It increases with increasing diameter and elastic modulus, but decreases with increasing length and tension. In pianos the inharmonicity is least in the middle of the keyboard, and that is where the octaves are stretched least. On concert grands the bass strings are long enough that the inharmonicity is not much greater than in the middle of the keyboard, but on a small upright, whose bass strings are too short, the inharmonicity can be severe, and the lower octaves are widely stretched. This, incidentally, provides a test of whether the stretching is due to inharmonicities in the strings or to non-linearities in the hearing mechanism. If it were due primarily to the hearing mechanism we would expect the stretching on all pianos to be about the same. In practice the stretching varies with the instrument, and experiments by Backus have shown that string inharmonicity accounts for nearly all of it.