Modal energy distribution in closed pipe resonance

AI Thread Summary
The distribution of energy among vibrational modes in a closed pipe or plucked string is determined by the initial excitation conditions and the system's geometry. Performing a Fourier series expansion on the wave function reveals the relative strengths of each harmonic, which directly influences the timbre of the sound produced. Different instruments, like the alto recorder and transverse flute, exhibit varying overtone structures, affecting their sound quality. The position of plucking a string alters the modal spectrum, with central plucking exciting the lowest mode and odd harmonics, while off-center plucking changes the timbre. Additionally, simultaneous displacements at different points can create unique spectral outcomes.
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When one causes the air column in a closed pipe to vibrate in its well-known modes (harmonics) or a plucked string to vibrate similarly, how is the exciting energy distributed amongst the modes?
 
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This sounds like a Fourier Analysis problem. You'd have to take your actual wave function, and perform a Fourier series expansion on it to determine the relative strengths of each harmonic.

The exact makeup of each harmonic influences what in music we call timbre. An alto recorder, for example, has very few overtones and has a "purer" sound than a transverse flute.
 
The system geometry (size and length of pipe, mass density, tension and length of string) determine the possible modes that could be excited. The "excitation" or initial condition determines which ones actually are, and how much energy goes into each. For a string, you can change the modal spectrum by plucking it at different positions from the end. Pluck at the center and and you excite the lowest mode plus odd harmonics. Pluck elsewhere and the spectrum (timbre) changes. Pull at two points simultaneously with different displacements (amplitudes) and you can get still different spectra.
 
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