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Beat (acoustics)

Interference pattern between signals of similar frequency

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Through Sound, Frequency and Amplitude

With tuning instruments that can produce sustained tones, beats can be readily recognized. Tuning two tones to a unison will present a peculiar effect: when the two tones are close in pitch but not identical, the difference in frequency generates the beating. The volume varies as in a tremolo while the sounds alternately interfere constructively and destructively. As the two tones gradually approach unison, the beating slows down and may become so slow as to be imperceptible. As the two tones get further apart, their beat frequency begins approaching the range of human pitch perception, the beating starts to sound like a note, and a combination tone is produced.

Mathematics and physics of beat tones

This phenomenon is best known in acoustics or music, though it can be found in any linear system:

According to the law of superposition, two tones sounding simultaneously are superimposed in a very simple way: one adds their amplitudes.

If a graph is drawn to show the function corresponding to the total sound of two strings, it can be seen that maxima and minima are no longer constant (as when a pure note is played), but change over time: when the two waves are nearly 180 degrees out of phase the maxima of one wave cancel the minima of the other, whereas when they are nearly in phase their maxima sum up, raising the perceived volume.

It can be proven (with the help of a sum-to-product trigonometric identity) that the sum of two unit-amplitude sine waves can be expressed as a carrier wave of frequency ⁠f1 + f2/2⁠ whose amplitude is modulated by an envelope wave of frequency ⁠f1 − f2/2⁠:

cos⁡(2πf1t)+cos⁡(2πf2t)=2cos⁡(2πf1+f22t)⏟carriercos⁡(2πf1−f22t)⏟envelope

Since every other burst in the modulation pattern is inverted, each peak is replaced by a trough and vice versa. The envelope is perceived to have twice the frequency of the modulating cosine, which means the audible beat frequency (if it is in the audible range) is:

fbeat=f1−f2.

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