What Determines the Speed of Sound in an Organ Pipe?

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SUMMARY

The speed of sound in an organ pipe is influenced by factors such as temperature and density, with the average speed of air molecules at a displacement antinode being approximately 500 m/s in still air. The wave speed in an infinitely long organ pipe can be calculated using the formula v = sqrt(γRT/M) or v = sqrt(γP/ρ). The lowest possible frequency of a stationary wave in a 2.5 m long organ pipe is determined to be 90 Hz, calculated using the fundamental frequency formula fn = n f1. Understanding the relationship between pressure, temperature, and density is crucial for determining sound speed in gases.

PREREQUISITES
  • Understanding of wave equations, specifically y = A sin(kx - ωt)
  • Familiarity with the ideal gas laws, including v = sqrt(γRT/M) and v = sqrt(γP/ρ)
  • Knowledge of standing waves and their characteristics in open and closed pipes
  • Basic principles of sound wave propagation and molecular motion in gases
NEXT STEPS
  • Research the effects of temperature on sound speed in gases
  • Study the principles of standing waves in both open and closed pipes
  • Explore the derivation and application of the wave equation for sound waves
  • Investigate experimental methods to measure sound speed in various media
USEFUL FOR

Students studying physics, particularly those focusing on acoustics, sound wave behavior, and wave mechanics in gases. This discussion is also beneficial for educators and researchers in the field of physics education.

  • #31
True! Thank you!
 
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  • #32
If you don't mind, can I just ask you one more thing please? What experimental evidence is there that sound travels in air as a progressive, longitudinal wave? I'm not sure which one fits proper experimental evidence.

You know what the funny thing is, for part iii where it was asking for the lowest possible frequency, I get the same answer with both methods: fn=n f1 and the way we did it. 90 Hz for both.
 
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