Why is entropy zero in an adiabatic process?

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Discussion Overview

The discussion centers on the concept of entropy in adiabatic processes, particularly addressing why the change in entropy is considered zero in such processes. Participants explore the relationship between heat exchange and entropy, and the implications for reversible and irreversible processes.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants assert that in an adiabatic process, since there is no heat exchange (dQ=0), the change in entropy (dS) is also zero, leading to the conclusion that entropy is constant in reversible adiabatic processes.
  • Others clarify that while the change in entropy is zero, this does not imply that the absolute value of entropy is zero; rather, it indicates that the entropy remains the same before and after the process.
  • A later reply introduces the distinction that the correct expression for entropy change is dS ≥ dQ/T, emphasizing that equality holds only for reversible processes and that non-reversible processes, like free expansion, can result in an increase in entropy despite no heat transfer or work being done.
  • Some participants express the need for clarification regarding the distinction between change in entropy and absolute entropy in the context of the thread title.

Areas of Agreement / Disagreement

Participants generally agree that the change in entropy is zero for reversible adiabatic processes, but there is disagreement regarding the implications of this for the absolute value of entropy and the treatment of non-reversible processes.

Contextual Notes

There are unresolved nuances regarding the definitions of entropy and the conditions under which the expressions for entropy change apply, particularly in the context of reversible versus irreversible processes.

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No heat exchange is facilitated during an adiabatic process. Change is heat is zero.
How does this relates to the entropy being zero?
∫dQ/T?
But this could really just mean that the integral is of any constant.
 
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Heat exchange and change in entropy are related.. dS=dQ/T. If the process is adiabatic then dQ=0 and change in entropy dS=0/T=0 or ΔS=∫dQ/T=∫0/T=0. So entropy is constant (S=constant) in reversible adiabatic process. It doesn't mean that the entropy of the system is 0, it means that the change in the entropy of the system is 0. ie. entropy of the system is same before and after the process.
 
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Arcone said:
Heat exchange and change in entropy are related.. dS=dQ/T. If the process is adiabatic then dQ=0 and change in entropy dS=0/T=0 or ΔS=∫dQ/T=∫0/T=0. So entropy is constant (S=constant) in reversible adiabatic process. It doesn't mean that the entropy of the system is 0, it means that the change in the entropy of the system is 0. ie. entropy of the system is same before and after the process.
The correct expression is ##dS \ge \frac {dQ}T##, not ##dS = \frac {dQ}T##. The latter holds if and only equal if the process is reversible. Free expansion is the canonical example of a non-reversible adiabatic process. Entropy increases in free expansion even though there is no heat transfer to/from the system and no work done on/by the system.
 
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D H said:
The correct expression is ##dS \ge \frac {dQ}T##, not ##dS = \frac {dQ}T##. The latter holds if and only equal if the process is reversible. Free expansion is the canonical example of a non-reversible adiabatic process. Entropy increases in free expansion even though there is heat transfer and work are zero.
Hi DH. I think you meant "even though there is no heat transfer..."

Chet
 
Arcone said:
Heat exchange and change in entropy are related.. dS=dQ/T. If the process is adiabatic then dQ=0 and change in entropy dS=0/T=0 or ΔS=∫dQ/T=∫0/T=0. So entropy is constant (S=constant) in reversible adiabatic process. It doesn't mean that the entropy of the system is 0, it means that the change in the entropy of the system is 0. ie. entropy of the system is same before and after the process.

D H said:
The correct expression is ##dS \ge \frac {dQ}T##, not ##dS = \frac {dQ}T##. The latter holds if and only equal if the process is reversible. Free expansion is the canonical example of a non-reversible adiabatic process. Entropy increases in free expansion even though there is heat transfer and work are zero.

Thanks! The first post cleared things up. The second refined the understanding.
 
Please note that it is the CHANGE in entropy, not the absolute value of the entropy, that is zero. This needs to be clarified in light of the title of the thread.

Zz.
 
ZapperZ said:
Please note that it is the CHANGE in entropy, not the absolute value of the entropy, that is zero. This needs to be clarified in light of the title of the thread.

Zz.

You are right. But it was a legitimate mistake. I thought the entropy was zero and so asked why could it have been other arbitrary constant. Perhaps, the mod could do some editing.
 
Chestermiller said:
Hi DH. I think you meant "even though there is no heat transfer..."
Yes, I did. Thanks. Post edited to reflect the missing "no".
 

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