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Acoustic Resonance

Level 1 - Physics topic page in Sound.

Principle

Acoustic resonance occurs when driving efficiently excites an allowed air-column mode.

Notation

\(f\)
driving frequency
\(\mathrm{Hz}\)
\(f_n\)
natural frequency
\(\mathrm{Hz}\)
\(L\)
resonator length
\(\mathrm{m}\)
\(v\)
sound speed
\(\mathrm{m\,s^{-1}}\)
\(Q\)
quality factor
1

Method

A resonator stores acoustic energy in a standing wave. The response is largest when the drive matches one of the allowed frequencies.

Resonance condition
\[f=f_n\]
Open-open modes
\[f_n=\frac{nv}{2L}\]
Open-closed modes
\[f_n=\frac{(2n-1)v}{4L}\]
Sharpness measure
\[Q=\frac{f_0}{\Delta f}\]
\Delta f is the frequency width of the strong-response region.

Changing the effective length changes the resonant frequencies. Changing temperature changes them through the sound speed.

Rules

These are the compact resonance relations.

Resonance
\[f=f_n\]
Open-open modes
\[f_n=\frac{nv}{2L}\]
Open-closed modes
\[f_n=\frac{(2n-1)v}{4L}\]
Quality factor
\[Q=\frac{f_0}{\Delta f}\]

Examples

Question
A closed tube resonates at its fundamental when driven at
\[170\,\mathrm{Hz}\]
Estimate its length using
\[v=340\,\mathrm{m\,s^{-1}}\]
Answer
For an open-closed fundamental,
\[f_1=\frac{v}{4L}\]
so
\[L=\frac{v}{4f_1}=\frac{340}{4(170)}=0.50\,\mathrm{m}\]

Checks

  • Resonance amplifies an allowed mode; it does not create arbitrary frequencies.
  • Effective length can differ from the physical tube length near open ends.
  • A higher \(Q\) means a narrower resonance peak.
  • Strong resonance still needs energy input from the driver.