Musical instruments - beats phenomenon

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SUMMARY

The beats phenomenon occurs when two sinusoidal signals of slightly different frequencies, f and f', are combined, resulting in a waveform described by f(t) = sin(f*t) + sin(f'*t). This can be mathematically expressed as f(t) = 2 * sin(0.5*(f+f')*t) * cos(0.5*(f-f')*t), where the cos() function represents the slowly varying amplitude perceived as beats. The frequency of the beats is determined by the difference in frequencies, f - f', while the average frequency is 0.5*(f+f'). This phenomenon is also applicable to real signals containing harmonics.

PREREQUISITES
  • Understanding of sinusoidal waveforms
  • Basic knowledge of frequency and amplitude concepts
  • Familiarity with trigonometric identities
  • Experience with mathematical modeling of sound waves
NEXT STEPS
  • Explore the mathematical derivation of wave interference
  • Learn about the Fourier Transform and its application in sound analysis
  • Investigate the effects of harmonics on sound perception
  • Study the practical applications of beats in music production and acoustics
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Musicians, audio engineers, acoustics researchers, and students studying sound wave phenomena will benefit from this discussion.

CAF123
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Can anyone give me a description of the beats phenomenon associated with musical instruments (or in general, any waves with which beats are associated).
I have looked at numerous textbooks however I feel I don't completely understand the concept still.
Thanks
 
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Suppose you are hearing two sinusoid signals of slightly different frequencies f and f'. Say the phases are such that you are hearing the time-dependent waveform f(t) = sin(f*t)+sin(f'*t).

Mathematically, this is the same as

f(t) = 2 * sin(0.5*(f+f')*t) * cos(0.5*(f-f')*t)

Since f-f' is small, the cos() will be a slowly varying function of time, while the sin() will vary quickly in time. The cos() will be heard as beats, i.e. a slowly varying amplitude of the quickly oscillating signal with frequency 0.5*(f+f') which is the average of f and f'.

It will be very similar for real signals cantaining harmonics.
 
Just a small correction, if frequency is f, the waveform is sin(2π f t).
 

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