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

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Homework Help Overview

The discussion revolves around a GRE problem related to entropy, specifically focusing on the implications of reversible processes in thermodynamics. Participants are examining the conditions under which entropy is conserved and how it relates to the system and surroundings during various transformations.

Discussion Character

  • Conceptual clarification, Assumption checking, Mixed

Approaches and Questions Raised

  • Participants are debating the correct answer to the problem, with some asserting that the key term 'reversible' indicates that entropy is conserved. Others are questioning how to calculate the entropy of the surroundings and whether the change in entropy of the system compensates for that of the surroundings.

Discussion Status

The discussion is active, with participants providing insights into the nature of reversible processes and entropy. Some have offered clarifications regarding energy exchange and the conditions under which entropy remains constant, while others are exploring the implications of these concepts without reaching a definitive conclusion.

Contextual Notes

There is a focus on the definitions and assumptions surrounding reversible processes, particularly in relation to adiabatic and isothermal transformations. Participants are navigating the complexities of how entropy behaves in these contexts, indicating a lack of consensus on certain interpretations.

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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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