Simple Applications of Macroscopic Thermodynamics

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SUMMARY

The discussion focuses on measuring the specific heat ratio "gamma" of an ideal gas confined in a vertical cylindrical container with a freely moving piston. The key parameters involved include the mass of the piston (m), gravitational acceleration (g), cross-sectional area (A), atmospheric pressure (p0), initial gas volume (V0), and the oscillation frequency (nu). The relationship between pressure and volume is governed by the equation pV(gamma) = constant, and the problem emphasizes that the gas remains in internal equilibrium while undergoing adiabatic oscillations. Participants seek guidance on incorporating potential energy and work done into their calculations.

PREREQUISITES
  • Understanding of ideal gas laws and thermodynamic principles
  • Familiarity with adiabatic processes in thermodynamics
  • Knowledge of oscillatory motion and restoring forces
  • Basic calculus for analyzing energy changes and work done
NEXT STEPS
  • Study the derivation of the specific heat ratio "gamma" in adiabatic processes
  • Learn about the relationship between pressure, volume, and frequency in oscillatory systems
  • Explore potential energy concepts in the context of harmonic motion
  • Investigate the implications of the first law of thermodynamics on adiabatic systems
USEFUL FOR

Students and professionals in physics and engineering, particularly those focusing on thermodynamics and fluid mechanics, will benefit from this discussion.

vladittude0583
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Homework Statement



The following describes a method used to measure the specific heat ratio "gamma" of a gas. The gas, assumed ideal, is confined within a vertical cylindrical container and supports a freely moving piston of mass m. The piston and cylinder both same the same cross-sectional area A. Atmospheric pressue is p0, and when the piston is in equilibrium under the influence of gravity (acceleration g) and the gas pressure, the volume of the gas is V0. The piston is now displaced slightly from its equilibrium position and is found to oscillate about this position with frequency "nu." The oscillations of the piston are slow enough that the gas always remains in internal equilibrium, but fast enough that the gas cannot exchange heat with the outside. The variations in gas pressure and volume are thus adiabatic. Express "gamma" in terms of m, g, A, p0, V0, and "nu"

Homework Equations



pV(gamma)=constant.

The Attempt at a Solution



1) Since the gas cannot exchange heat with the outside, then I know that Q = 0 right?
2) When the piston is in equilibrium under "g" and the gas pressure, the force from the gas has to exactly balance out the gravitational force due to the piston right?
3) Do I have to take into consideration of potential energy in terms of oscillatory motion?
4) Since Q = 0, then we know that the change in energy is equal to the work done right?
5) Any advice towards the correct direction to solving this problem would be greatly appreciated.
6) Thanks!
 
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vladittude0583 said:
5) Any advice towards the correct direction to solving this problem would be greatly appreciated.

Sinusoidal oscillations generally occur when there's a restoring force that increases with displacement. In this case, the pressure increases slightly when the volume decreases due to the piston moving downwards, and this causes the piston to rebound. You'll probably want to look into the relationship between this restoring force and the frequency of oscillation.
 

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