Helmholtz resonance is the phenomenon of air resonance in a cavity. The device was created in the 1860s by Hermann von Helmholtz to show the height of the various tones. An example of Helmholtz resonance is the sound created when one blows across the top of an empty bottle.
This effect is akin to that of a bungee-jumper bouncing on the end of a bungee rope, or a mass attached to a spring. Air trapped in the chamber acts as a spring. Air, being compressible, has a definite spring constant. Changes in the dimensions of the chamber adjust the properties of the spring: a larger chamber would make for a weaker spring, and vice-versa.
The air in the port acts as the mass. Since it is in motion, it possess some inertia. A longer port would make for a larger mass, and vice-versa. The diameter of the port is related to the mass of air and the volume of the chamber. A port that is too small in area for the chamber volume will "choke" the flow while one that is too large in area for the chamber volume tends to reduce the inertia in the port.
We can then easily derive the following formula for the resonance frequency:
Where v has units of velocity, and is a proportionality constant.
Helmholtz-Resonator | Risonanza di Helmholtz | Helmholtzresonator
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