I found some recordings of individual piano notes at U of Iowa. They are recorded with a Steinway B, with the left mic 8" above center bass strings, and the right mic 8" above center treble strings. Here are the spectra of a few notes (A0, B0, C1, D1, E1, G1).
http://theremin.music.uiowa.edu/MISpiano.html
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It is interesting to see that the fundamentals mostly only showed up on 1 channel for A0, B0 and C1, with C1 switched to right channel from left. By about E1, the volume of the channels are comparable. I think it is because the Steinway B is not of sufficient size and/or rigid enough to radiate the fundamentals of the lower notes as proper acoustic waves. The "sounds" picked up by the mics were probably either
evanescent waves and/or hydrodynamic waves, which decay exponentially with distance, and would not be detected (either by ear or mics) at the typical listening distance.
My interpretation/theory on these plots is that the strings themselves are vibrating at the fundamental, and when the mic is close enough to it, it can be picked up. But the vibration of the strings must pass through the bridge and to the soundboard in order to be heard by the audience. I'm willing to bet that the bridge and the soundboard is unable to transmit such low frequencies.
Very interesting! Thank you.
Very stimulating thread! I had never read anything other than "pistonic driver motion" about producing sound, and it is fascinating to learn how some musical instruments produce useful sound. The parts of the thread about perception of absolute pitch are hard for me to grasp, because I do not know the "ABCs" of music, have never played any musical instrument and can't carry a tune
. But I find it enjoyable to follow along and analyze the logic of the arguments anyway.
Never heard of evanescent waves before either. Just googling the term shows a lot of hits to explanations of apparently well understood evanescent waves in the well known phenomenon of total internal reflection in the field of electromagnetism. The phenomenon in acoustics seems to be not as widely known, and the description
@NTK linked to is very illuminating. The evanescent waves in this case are a type of hydrodynamic motion impressed on the fluid, and do not propagate to the farfield at acoustic speed, and attenuate exponentially quickly with distance from the surface producing them.
Googling basic facts about how a piano makes sound, and assuming that the strings of the Steinway B used to make those recordings have been designed and tensioned/tuned to produce the right notes, and that the strings are "fixed" at both ends of their speaking length,
speed of flexural wave in A0 string = 2 x speaking length x fundamental frequency = 2 x 1.5m x 27.5Hz = 82.5 m/s. This is much smaller than the speed of sound in air at room temperature of about 343 m/s. Making the sweeping assumption, with vigorous motions of my hands, that the string radiates sound in its plane of vibration like the bending plate example that
@NTK linked to (and would have an oval-ish sound polar in the cross-sectional plane), it seems that the A0 string (and the B0 and C1 maybe; I do not know their frequencies) does not radiate acoustic waves but produces evanescent waves instead that would not be sensible at any appreciable distance as
@NTK pointed out. As
@LeftCoastTim pointed out, perhaps the string vibrations do not get through the bridge to the soundboard. Even if they did manage to set the soundboard in vibration, the same problem might occur with the soundboard as with the string. The speed of transverse flexural waves in the soundboard is unknown to me. Making yet more sweeping assumptions that the soundboard is flexible enough to work by flexural wave mechanism (rather than pistonic motion of a rigid soundboard with infinite wave speed), and that the soundboard length is just barely sufficient to support the A0 fundamental frequency, and keeping in mind that the soundboard at the bridge would be a "free" end (anti-node of the standing wave) so that the strings and bridge can move it transversely to its plane, the wave speed in the soundboard would be 4 x speaking length x frequency = 165 m/s. Still much less than the speed of sound in air. So in this case too, the soundboard would produce evanescent 27.5 Hz waves instead of acoustic waves, according to the mathematical analysis cited at the link
@NTK provided. The soundboard is actually a plate, and so fits the evanescent wave example better than does the string. If the preceding speculation resembles the real physics at all, the first company to support and move the soundboard in pistonic motion for low frequencies would produce a grand piano that trumps the Bosendorfer Imperial. Maybe beryllium or carbon-fiber-reinforced composite soundboards on polymer suspensions?