GRE Entropy Question: Problem 21 in Attached File - Solution Debate

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The discussion centers on the interpretation of entropy in reversible processes, specifically in relation to a GRE problem. Participants debate whether the correct answer is C or D, emphasizing that in reversible processes, entropy is conserved overall, though not individually for the system and surroundings. It is clarified that during adiabatic transformations, the entropy of the surroundings remains unchanged due to no heat exchange. The conversation also highlights that in isothermal and constant volume processes, the changes in entropy of the system and surroundings compensate each other due to the nature of reversible processes. The key takeaway is that the infinitesimal temperature difference in reversible processes allows for equal and opposite changes in entropy.
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Homework Statement


It is problem 21 in the attached file.

Homework Equations

The Attempt at a Solution


The answer seems to be C. I thought it is D. Can someone explain it to me please?
 

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Key word in the problem statement is 'reversible'. For reversible processes entropy is conserved.
 
BvU said:
Key word in the problem statement is 'reversible'. For reversible processes entropy is conserved.
So for a reversible process, the entropy is conserved for both the system and the surroundings (but not for each of them individually)?
 
Correct: there is an exchange of energy between the two.
 
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BvU said:
Correct: there is an exchange of energy between the two.
Thank you so much!
 
Is it really clear to you that (A) and (B) are not true ?
 
BvU said:
Is it really clear to you that (A) and (B) are not true ?
For the gas it is clear that the entropy is constant only during the adiabatic transformation. However I am not sure how can I calculate the entropy of the surroundings
 
Nothing happens to the surroundings (if all that occurs is this adiabatic expansion). There is no ##\delta Q##, so no ## \delta S##.
 
BvU said:
Nothing happens to the surroundings (if all that occurs is this adiabatic expansion). There is no ##\delta Q##, so no ## \delta S##.
No, sorry. I meant in the other 2 cases the isothermal and constant volume. How can I know that the change in entropy of the system exactly compensate the one of the surrounding? It is just by the definition of reversible process or there is something more to it?
 
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Not much more to it. Reversibility means you can also go through the process in the other direction - in which case ##\delta S## comes out the same value but with opposite sign. That can only be correct if it is zero.
Silviu said:
change in entropy of the system exactly compensate the one of the surrounding
More through energy conservation plus ##dQ = TdS##.
 
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Silviu said:
No, sorry. I meant in the other 2 cases the isothermal and constant volume. How can I know that the change in entropy of the system exactly compensate the one of the surrounding? It is just by the definition of reversible process or there is something more to it?
For a reversible process, when heat is transferred, the temperature difference between the gas and its surroundings is infinitesimal. There has to be some difference in temperature, otherwise heat won't flow, but since the two are essentially at the same temperature, the decrease in entropy of one is equal to the increase of the other.
 
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