Understanding the Limit of Irreversibility: Free Expansion Explanation

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SUMMARY

The discussion centers on the concept of free expansion in thermodynamics, highlighting its role as the limit of irreversibility where potential work is converted to heat. It emphasizes that while free expansion leads to a loss of thermodynamic equilibrium, the gas retains kinetic energy and can perform work on itself. The maximum entropy change occurs when internal energy is released as heat to a reservoir near absolute zero, resulting in a total entropy change of the universe that reflects the degradation of usable energy.

PREREQUISITES
  • Understanding of thermodynamic principles, specifically entropy and equilibrium.
  • Familiarity with the ideal gas law (PV = nRT).
  • Knowledge of kinetic energy concepts in thermodynamics.
  • Basic grasp of heat transfer and temperature scales, particularly near absolute zero.
NEXT STEPS
  • Study the implications of the second law of thermodynamics on entropy and irreversibility.
  • Explore the concept of thermodynamic equilibrium and its significance in gas behavior.
  • Investigate the relationship between internal energy and work in expanding gases.
  • Learn about heat transfer mechanisms at low temperatures and their effects on entropy.
USEFUL FOR

This discussion is beneficial for students and professionals in physics, particularly those focusing on thermodynamics, as well as engineers and researchers interested in energy systems and entropy analysis.

asdf1
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Why does free expansion represent the limit of irreversibility at which all of the "potential" work is degraded to heat.
 
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asdf1 said:
Why does free expansion represent the limit of irreversibility at which all of the "potential" work is degraded to heat.
Entropy measures irreversibility, or loss of ability to do work. The greater the net increase in entropy, the greater the irreversibility.

The free expansion of a gas itself does not necessarily result in a total loss of the gas' ability to do work. It causes the gas to lose thermodynamic equilibrium. The temperature of an expanding gas ball is not defined, due to the loss of equilibrium. Contrary to general belief, the free expansion of gas actually does work - on itself. If you think of a sphere of gas as concentric shells of gas, the outer shell does no work, but the inner shells push out and accelerate the outer shells. The freely expanding gas has kinetic energy and, therefore, an ability to do work.

To maximize the entropy change, you would have to take all the internal energy of the gas (U = PV = nRT) and release it as heat to a reservoir that is arbitrarily close to absolute 0 degrees K (ie 0+dT). The change in entropy of the gas would be [itex]\Delta S_{gas} = -Q/T[/itex] and the change in entropy of the reservoir would be [itex]\Delta S_{res} = Q/(0+dT)[/itex]. The entropy change of the universe is sum of these changes:

[tex]\Delta S_{univ} = \Delta S_{gas} + \Delta S_{res} = Q/(0+dT) - Q/T[/tex].

The gas and reservoir at close to absolute 0 has no ability to do work. So the change in entropy is maximum.

AM
 
i see~
thanks! :)
 

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