Thermodynamic equilibrium and Entropy

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Homework Help Overview

The discussion revolves around the equilibrium condition for an isolated thermodynamic system, specifically focusing on entropy and its implications in both reversible and irreversible processes.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the relationship between entropy change (dS) and heat transfer (dQ), questioning whether dS=0 accurately represents the equilibrium condition. They discuss the implications of maximum entropy and the conditions under which entropy remains constant.

Discussion Status

There is an ongoing exploration of the definitions and relationships between entropy and heat transfer. Some participants suggest that the original poster's interpretation of dS=0 may not fully capture the nuances of the equilibrium condition, indicating a productive dialogue without clear consensus.

Contextual Notes

Participants note the importance of considering both the system and surroundings when discussing entropy changes, as well as the potential need for clarification from the instructor regarding the expectations for the test question.

DieCommie
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I got this question wrong on a test:

What is the equilibrium condition for an isolated system?

I think the answer he wanted is the system is a maximum entropy, and that makes sense to me. But I put dS =0, which I think is basically the same thing. dS would be zero iff the system is at maximum entropy.

Or am I way off? :smile:
 
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[tex]\Delta S=0[/tex] is the condition for equilibrium for a completely isolated system.

The entropy of the system will increase according to the second law until the system hits maximum entropy, at which point
[tex]\Delta S=0[/tex]

Saying this should be the same as saying that the entropy is at a maximum.

Was there any other information given with the question?
 
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The full question is this

Write down the relationship between heat transfer dQ and entropy change dS for an infinitesimal reversible process, in which heat is supplied to a system at temperature T. How is this expression modified for an irreversible process? What is the equilibrium condition for an isolated system?I got the first two parts right. After looking at it again, I think I go half credit for the dS=0.
 
Well, I'm assuming for one of the first two parts that you stated somewhere that:

[tex]\Delta S = \int\frac{dq}{T}[/tex]

For [tex]\Delta S[/tex] to be zero, dq would also have to be constant at 0. Maybe your professor wanted you to state the heat transfer would also have to be zero. You may want to discuss this problem with him.

I'm no expert though, maybe someone else here has a little more insight, but I agree with you.
 
I did write down that integral for clausius' theorem.The first two parts...

"Write down the relationship between heat transfer dQ and entropy change dS for an infinitesimal reversible process, in which heat is supplied to a system at temperature T." dQ=TdS

"How is this expression modified for an irreversible process?" dQ<TdS

"What is the equilibrium condition for an isolated system?" I put dS=0. My classmate put "The system is at maximum equilibrium" and got it right.

Im not going to argue the half point with him, as that will do me no good. I am going to ask him if dS=0 is an equilibrium condition.
 
G01 said:
Well, I'm assuming for one of the first two parts that you stated somewhere that:

[tex]\Delta S = \int\frac{dq}{T}[/tex]

For [tex]\Delta S[/tex] to be zero, dq would also have to be constant at 0.
Not so. In order to determine the total change in entropy when heat flows, you have to look at the system and surroundings, which includes both reservoirs.

[tex]\Delta S = \Delta S_H + \Delta S_C = \int dS_H + \int dS_C = \int dQ_H/T_H + \int dQ_C/T_C[/tex]

So for [itex]\Delta S = 0[/itex]:

[tex]\int dQ_H/T_H + \int dQ_C/T_C = 0[/tex]

[tex]\int dQ_H/T_H = - \int dQ_C/T_C[/tex]

AM
 
DieCommie said:
The full question is this

Write down the relationship between heat transfer dQ and entropy change dS for an infinitesimal reversible process, in which heat is supplied to a system at temperature T. How is this expression modified for an irreversible process? What is the equilibrium condition for an isolated system?
Since the temperature difference is infinitesimal, [itex]T_H = T_C[/itex] and [itex]Q_H = -Q_C[/itex], [itex]dS_H = dQ_H/T_H[/itex] and [itex]dS_C = dQ_C/T_C = -Q_H/T_H[/itex], so

[itex]dS = dS_H + dS_C = dQ_H/T_H - dQ_H/T_H = 0[/itex]

If the temperature difference is non-zero, [itex]T_H > T_C[/itex] and [itex]Q_H = -Q_C[/itex], [itex]dS_H = dQ_H/T_H[/itex] and [itex]dS_C = dQ_C/T_C > -Q_H/T_H[/itex], so

[itex]dS = dS_C + dS_H = dQ_C/T_C - dQ_H/T_H > 0[/itex]

So these are the only two possibilities for a system moving to thermal equilibrium. What is the condition for thermal equilibrium then, in terms of dS?

AM
 
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