Wave Frequency in Piston: Pressure Variation & Adiabatic Compression

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SUMMARY

The fundamental frequency of oscillation in a piston, as described by A.P. French, is determined by the formula ν = 1/4L √(γp/ρ), where p represents the equilibrium pressure, γ is the adiabatic compression factor, and ρ is the gas density. The discussion clarifies that while pressure does vary during compression, the formula specifically utilizes the pressure at equilibrium, ensuring accurate calculations of wave frequency within the piston. This distinction is crucial for understanding the behavior of sound waves in compressible fluids.

PREREQUISITES
  • Understanding of wave mechanics
  • Familiarity with thermodynamics, specifically adiabatic processes
  • Knowledge of fluid dynamics, particularly gas behavior under compression
  • Basic mathematical skills for manipulating equations
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  • Study the principles of adiabatic compression in gases
  • Learn about the derivation and applications of wave equations in fluid dynamics
  • Explore the relationship between pressure, density, and temperature in gases
  • Investigate the effects of varying pressure on sound wave propagation in different mediums
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Physics students, engineers working with gas dynamics, and anyone interested in the acoustic properties of gases under compression.

WiFO215
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When you have a wave in sound inside a piston of length L, A.P. French says that the fundamenal frequency [tex]\nu[/tex] of an oscillation is given by

[tex]\nu[/tex] = 1/4L [tex]\sqrt{(\gamma[/tex] p / [tex]\rho)}[/tex]

Where p is the pressure, [tex]\gamma[/tex] is the factor that accounts for adiabatic compression of the gas, and [tex]\rho[/tex] is it's density.

My question is this : doesn't the pressure p vary as you compress the gas? How can you assume it to be constant?
 
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Hold up. I think I got it. That's not ANY pressure that you plug into that formula, it's the pressure when the gas is at equilibrium.
 

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