Sound Wave Physics: X-Axis vs. Trough

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SUMMARY

The discussion centers on the behavior of sound waves as represented by sine waves on an oscilloscope. It establishes that sound is not silent at the x-axis or the trough; silence occurs only when there is no wave present. The amplitude of the wave determines loudness, with the x-axis representing the highest rate of change in the wave. Additionally, it highlights that sound pressure and velocity are affected by the position of the loudspeaker cone and the finite speed of sound, approximately 340 m/s, which causes a time delay in sound perception at varying distances from the source.

PREREQUISITES
  • Understanding of sine waves and their representation on an oscilloscope
  • Basic knowledge of sound wave physics, including amplitude and frequency
  • Familiarity with sound pressure and velocity concepts
  • Awareness of the speed of sound in air (approximately 340 m/s)
NEXT STEPS
  • Research the principles of wave propagation in different media
  • Explore the effects of amplitude and frequency on sound perception
  • Learn about the design and function of loudspeakers in sound reproduction
  • Investigate the concept of phase delay in sound waves
USEFUL FOR

Students of physics, audio engineers, sound designers, and anyone interested in the principles of sound wave behavior and acoustics.

ZB08
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Hi, easy one but can't really get my head around it. The physics teacher today showed sound as Sine wave on an oscilloscope. If I was actually listening to this sound wave, where would it be silent, on the x-axis or at the trough? Please explain.
 
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Sound is dependent on the amplitude, so it is zero on the axis.
 
If you are listening to it, you are "hearing the sound" with your brain. Not with your ears, and certainly not with a scientific measuring instrument! For almost all the frequency range where you hear anything at all, the loudness you hear will be constant.

On the other hand it we are talking about measuring what happens to the air wth scientific instruments rather than "what you hear", loudspeakers are designed so the position of the moving cone follows the voltage graph that you see on the oscilloscpe. (But a real loudspeaker isn't perfect, and won't follow it exactly). The change in air pressure, close to the speaker, is zero when the cone is at its mid point. However the velocity of the air close to the speaker is zero when the speaker is at the max and min displacements.

But further away from the speaker, there is a "time delay" because the speed of sound is finite - about 340 m/s so the peaks and troughs of the pressure and velocity further away from the speaker "lag behind" the movement of the speaker by an amount that is proportional to the distance away.
 
ZB08 said:
Hi, easy one but can't really get my head around it. The physics teacher today showed sound as Sine wave on an oscilloscope. If I was actually listening to this sound wave, where would it be silent, on the x-axis or at the trough? Please explain.

It wouldn't be silent anywhere. It would only be silent if there was no wave at all; just a flat line. At the x-axis the wave actually has the highest rate of change. The rate of change is zero at the peak and the trough but even then there would still be sound.
 
Thanks everybody
 

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