Audited 31 Jul 2026·Last updated 15 Sept 2026·5 citations·Tier 1·0 uses

Beat Frequency Calculator

Beat frequency calculator: f_beat = |f₁ − f₂|. Why two close tones pulse, and how musicians use beats to tune to within a fraction of a hertz.

Beat Frequency Calculator

Hz
Hz
Beat frequency
4
Result of f_beat = |f₁ - f₂| using the entered coherent-SI magnitudes.
Model scope
Difference frequency for two steady sinusoidal components; audibility, nonlinear mixing products, time-varying pitch, spectral width, amplitude, and psychoacoustics are outside it.

Background.

Play two tones that are almost — but not quite — the same pitch, and you do not hear two notes. You hear one note that pulses, swelling and fading in a slow rhythm. Those pulses are beats, and their rate is the simplest formula in acoustics: the beat frequency is just the difference between the two tones, f_beat = |f₁ − f₂|.

The effect is pure superposition. When the two waves start in step they reinforce; because one completes cycles slightly faster, it steadily pulls ahead until the waves are in opposite phase and cancel; then it laps the slower wave and they reinforce again. Each lap is one beat, and laps happen exactly as often as the frequency gap dictates.

Beats are most useful precisely when they are slow. A gap of 4 Hz between two instruments is hard to name as a pitch difference — it is under a fiftieth of a semitone at concert pitch — yet it produces four unmistakable throbs every second. That inversion, where a tiny frequency error becomes a big audible rhythm, is why piano tuners, string players, and radio engineers have used beats as a precision instrument for centuries: tune until the beating slows to a stop, and the two frequencies match to well under a hertz.

This page computes the beat rate from two steady sine frequencies. It deliberately says nothing about loudness, audibility, or the fused-versus-rough character the ear assigns to faster beats — those live in psychoacoustics, and the scope note beside the result draws that boundary.

What is beat frequency calculator?

Beat frequency is the rate at which the combined loudness of two superposed tones rises and falls, equal to the absolute difference of their frequencies: f_beat = |f₁ − f₂|. Two tuning forks at 440 Hz and 444 Hz beat 4 times per second. The phenomenon requires no special medium or nonlinearity — it falls straight out of adding two sinusoids — and the perceived pitch of the pair sits near the average of the two frequencies while the beat rides on top as a loudness envelope.

How to use this calculator.

  1. Enter both frequencies in hertz — from a tuner app, signal generator, or instrument specification.
  2. Order does not matter: the formula takes the absolute difference, so 440 and 444 give the same 4 Hz as 444 and 440.
  3. Read the beat frequency as pulses per second; its reciprocal is the time between loudness peaks (4 Hz beats repeat every 0.25 s).
  4. Tuning in practice runs backwards: count the beats you hear against a reference tone, and you have measured your detuning directly.
  5. Expect the clean throb only while the gap is small — past roughly 15–20 Hz the ear stops resolving pulses and hears roughness, then two separate tones.

The formula.

f_beat = |f₁ - f₂|

Add two equal-amplitude sinusoids and a trigonometric identity does the rest: sin(2πf₁t) + sin(2πf₂t) = 2 cos(2π·½(f₁−f₂)t)·sin(2π·½(f₁+f₂)t). The second factor is a tone at the average frequency — what your ear assigns as pitch. The first is a slow envelope at half the difference frequency; but loudness peaks every time the cosine touches +1 or −1, twice per envelope cycle, so audible beats arrive at the full difference |f₁ − f₂|. That factor-of-two subtlety is the classic exam trap. The calculator subtracts and takes the absolute value in Decimal arithmetic, rounding once at the output — trivial mathematics, but the point of the page is the physics of why a difference is what you hear.

A worked example.

Example

An oboe sounds concert A at 440 Hz while a slightly sharp violin plays 444 Hz. What does the audience hear? The beat rate is the difference: f_beat = |440 − 444| = 4 Hz — four distinct swells of loudness every second, each 0.25 s apart, riding on a perceived pitch near the average, 442 Hz. The musical meaning of 4 Hz: at A4, one equal-tempered semitone spans about 26 Hz, so the violin is sharp by roughly a sixth of a semitone — an error too small to name by ear as a pitch, yet impossible to miss as a throb. The violinist flattens the string until the throbbing slows — 2 beats, 1, then a slow breathing and silence of beats at unison. Stopping the beats has tuned the pair to within a fraction of a hertz, better than most electronic tuners display.

frequency One Hz440
frequency Two Hz444

Frequently asked questions.

Why do I hear one pulsing tone instead of two separate notes?
Because the ear cannot resolve two frequencies only a few hertz apart — they fall within one critical band — so it fuses them into a single pitch at roughly the average frequency and hears the interference as a loudness envelope. Widen the gap past about 15–20 Hz and the fusion breaks: first into roughness, then into two distinct notes.
Does it matter which frequency is larger?
No. The envelope depends only on how fast the two waves slip relative to each other, which is the same whether the first or second tone is higher — hence the absolute value in f_beat = |f₁ − f₂|. What the sign would tell you is which source is sharp, and tuners recover that by nudging one source and watching whether the beating speeds up or slows down.
How do piano tuners use beats?
As a measuring instrument. A tuner strikes a tuning fork or an already-tuned string together with the target string and counts beats: 3 Hz of beating means 3 Hz of error. For intervals other than unisons they listen to beats between coinciding harmonics — equal temperament actually requires certain intervals to beat at prescribed slow rates, so the tuner adjusts until the beat rate is right, not until it vanishes.
Can beats occur with light or radio waves too?
Yes — superposition is universal. Two lasers with nearly equal optical frequencies produce an intensity beat a photodiode can read directly, which is how heterodyne detection measures otherwise-inaccessible optical frequency differences. Radio receivers exploit the same idea deliberately, mixing a signal with a local oscillator to shift it to a manageable intermediate frequency.
Why is the loudness envelope at half the difference frequency but the beats at the full difference?
The amplitude factor cos(2π·½(f₁−f₂)t) completes one cycle at half the difference frequency, but loudness depends on the magnitude of amplitude, which peaks at both the crest and the trough of that cosine. Two loudness maxima per envelope cycle restores the full |f₁ − f₂| as the audible beat rate — the ear counts 4 swells per second from a 2 Hz envelope.

How this page was produced

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Quanta Calculator
Primary sources
5 cited below
Method
f_beat = |f₁ - f₂|
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