About Reversible vs Irreversible Gas Compression and Expansion Work

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Discussion Overview

The discussion revolves around the concepts of reversible and irreversible gas compression and expansion work, focusing on the implications of Newton's third law in the context of an ideal gas contained in a cylinder with a massless piston. Participants seek clarification on the definitions and relationships between external pressure, thermodynamic pressure, and the effects of viscous stresses in irreversible processes.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant describes the application of Newton's third law to a massless piston, asserting that the external force per unit area applied to the piston equals the thermodynamic pressure of the gas at the piston interface.
  • Another participant agrees with the initial understanding but proposes a different definition of external pressure, suggesting it should be considered as the force per unit area that the piston applies to the gas.
  • There is a mention of the need to include viscous normal stress in the analysis of irreversible processes, indicating a potential complication in the relationship between pressures.
  • A participant points out a missing figure and a misstatement in the referenced insight, suggesting corrections to the descriptions of work done by viscous stresses and the plot of irreversible to reversible work ratios.

Areas of Agreement / Disagreement

Participants generally agree on the application of Newton's third law and the basic principles involved, but there are differing definitions and interpretations regarding the external pressure and the role of viscous stresses in irreversible processes. The discussion remains unresolved regarding the implications of these definitions.

Contextual Notes

There are limitations in the definitions of pressure and the treatment of the piston as part of the system, particularly in scenarios involving mass and thermal inertia. The discussion also highlights the complexity introduced by viscous stresses in irreversible processes.

cianfa72
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Hi,

reading the interesting Reversible vs Irreversible Gas Compression and Expansion Work insight by @Chestermiller I would like to ask for clarification on some points.

In the second bullet at the beginning
Since, by Newton’s third law, the external force per unit area exerted by the surroundings on the gas is equal to the gas thermodynamic pressure at the interface P.
my understanding is as follows: consider an ideal gas contained in a cylinder featuring a massless piston. An external force per unit area ##P_{ext}## is applied to the piston through a bunch of (external) bodies.

Applying the Newton's third laws to the massless piston we get two things:
  • the force per unit area the piston applies to the external bodies through the piston's outer edge is the same (in module) as the external force per unit area ##P_{ext}##
  • the force per unit area the thermodynamic pressure of the gas at the piston's inner edge ##P_I## (i.e. the thermodynamic pressure ##P_I## at the piston internal interface) applies to the piston is the same (in module) as the force the piston applies per unit area on the gas inside the cylinder
The above hold since otherwise the acceleration of the massless piston would be infinite.

Does it make sense ? Thank you.
 
Last edited:
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cianfa72 said:
Hi,

reading the interesting Reversible vs Irreversible Gas Compression and Expansion Work insight by @Chestermiller I would like to ask for clarification on some points.

In the second bullet at the beginning

my understanding is as follows: consider an ideal gas contained in a cylinder featuring a massless piston. An external force per unit area ##P_{ext}## is applied to the piston through a bunch of (external) bodies.

Applying the Newton's third laws to the massless piston we get two things:
  • the force per unit area the piston applies to the external bodies through the piston's outer edge is the same (in module) as the external force per unit area ##P_{ext}##
  • the force per unit area the thermodynamic pressure of the gas at the piston's inner edge ##P_I## (i.e. the thermodynamic pressure ##P_I## at the piston internal interface) applies to the piston is the same (in module) as the force the piston applies per unit area on the gas inside the cylinder
The above hold since otherwise the acceleration of the massless piston would be infinite.

Does it make sense ? Thank you.
Yes it does make sense. But, in the way that I define things, I would consider ##P_{ext}## to be the force per unit area that the inside face of the piston applies to the gas. Otherwise, based on the way you have defined ##P_{ext}##, I would have to include the piston as part of the system. Of course, in this situation it doesn't matter, but, if the piston had mass and thermal inertia, by my way of doing things, the piston would have to be included as part of the system.

Also, I should mention that, if the process is irreversible, the force per unit area applied by the gas to the inside face of the piston would conceptually have to include the viscous normal stress.
 
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Chestermiller said:
Yes it does make sense. But, in the way that I define things, I would consider ##P_{ext}## to be the force per unit area that the inside face of the piston applies to the gas. Otherwise, based on the way you have defined ##P_{ext}##, I would have to include the piston as part of the system. Of course, in this situation it doesn't matter, but, if the piston had mass and thermal inertia, by my way of doing things, the piston would have to be included as part of the system.
Yes, definitely.

Chestermiller said:
Also, I should mention that, if the process is irreversible, the force per unit area applied by the gas to the inside face of the piston would conceptually have to include the viscous normal stress.
Of course, as you explained in the 'Spring-Damper Model Analysis' and 'Ideal Gas Analysis' sections.
 
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cianfa72 said:
Yes, definitely.Of course, as you explained in the 'Spring-Damper Model Analysis' and 'Ideal Gas Analysis' sections.
You are wonderful. I hope that you continue to stay involved with Physics Forums. It's so nice to encounter someone like you who is on the same wavelength as I.
 
By the way: in the insight I do not see 'Figure 8 Work Done By Viscous Stresses on Piston' and the sentence
Fig. 9 shows a plot of the ratio of the irreversible work to the reversible work ##W_{Irr} / W_R## for the case of an ideal gas as a function of the expansion/compression volume ratio ##W_f / W_i##
should actually read:

Fig. 9 shows a plot of the ratio of the irreversible work to the reversible work ##W_{Irr} / W_R## for the case of an ideal gas as a function of the expansion/compression volume ratio ##V_f / V_i##
 
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