Modern PhysicsWaves with Calculus

Beats

Two tones of nearly equal frequency throb at the beat frequency |f₁ − f₂|.

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Play two notes that are almost the same pitch and you hear a single tone whose loudness throbs: wah, wah, wah. These are beats. Musicians use them to tune: as two strings come into tune, the beats slow down and finally stop. Beats are interference in time instead of in space.

Key idea

Two tones of frequencies $f_1$ and $f_2$ played together sound like one tone at the average frequency $\frac{f_1 + f_2}{2}$, swelling and fading at the beat frequency $$f_{\text{beat}} = |f_1 - f_2|.$$

Why it works

At one spot, the two sound waves are $\cos(2\pi f_1t)$ and $\cos(2\pi f_2t)$. The sum formula gives $$\cos(2\pi f_1t) + \cos(2\pi f_2t) = 2\cos\!\left(2\pi\,\frac{f_1 - f_2}{2}\,t\right)\cos\!\left(2\pi\,\frac{f_1 + f_2}{2}\,t\right).$$ The fast factor is the tone you hear. The slow factor is an envelope that sets the loudness. The envelope's frequency is $\frac{|f_1 - f_2|}{2}$, but loudness depends on the envelope's size, which peaks twice per cycle (at $+2$ and at $-2$). So the loudness throbs at twice that: $|f_1 - f_2|$. Said simply: the two waves drift in and out of step, and they get back in step once every $1/|f_1 - f_2|$ seconds.
Two tones (faint) and their sum (solid), slowed down. The dashed envelope swells and shrinks; there is one loud swell per $1/|f_1 - f_2|$ seconds. Change $f_2$ and watch the beats speed up or slow down.

Worked examples

Worked example: Count the beats

A tuning fork of 440 Hz and a piano string of 443 Hz sound together. What do you hear?
  1. Beat frequency: $|443 - 440| = 3$ Hz, so three swells of loudness per second.
  2. The tone itself is at $\frac{440 + 443}{2} = 441.5$ Hz.

Answer: A 441.5 Hz tone that throbs 3 times a second

Worked example: Tuning a guitar

A guitar string sounded with a 330 Hz fork gives 4 beats per second. Tightening the string slightly makes the beats faster. What was the string's frequency?
  1. The string is at $330 + 4 = 334$ Hz or $330 - 4 = 326$ Hz.
  2. Tightening raises a string's frequency ($f \propto \sqrt{F_T}$).
  3. If it were at 326 Hz, raising it would move it toward 330 Hz and slow the beats. The beats sped up, so it moved away from 330 Hz.

Answer: $334$ Hz (loosen it to tune)

Worked example: A small change in tension

Two identical strings both sound 220 Hz. The tension in one is raised by 2.0%. What beat frequency do you hear?
  1. For a string $f = \frac{1}{2L}\sqrt{F_T/\mu}$, so $f \propto \sqrt{F_T}$.
  2. New frequency: $220\sqrt{1.020} = 220 \times 1.00995 = 222.19$ Hz.
  3. Beats: $222.19 - 220 = 2.2$ Hz.

Answer: About $2.2$ beats per second

Common mistake

Taking the beat frequency as the average $\frac{f_1 + f_2}{2}$ or the sum $f_1 + f_2$. The average is the pitch you hear; the beats come from the difference. Another slip: using half the difference, the envelope's own frequency. Check with a case you can picture: tones at 100 Hz and 101 Hz get back in step once every second, so there is 1 beat per second, not 0.5.

Practice

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Builds on

Leads to

This is one of the top rungs of Waves, Optics and Modern Physics.

Sources and further reading

  • OpenStax University Physics Volume 1, 17.6 Beats
  • MIT OpenCourseWare 8.03SC Physics III: Vibrations and Waves (Fall 2016)
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