So for a reversible process, the entropy is conserved for both the system and the surroundings (but not for each of them individually)?BvU said:Key word in the problem statement is 'reversible'. For reversible processes entropy is conserved.
Thank you so much!BvU said:Correct: there is an exchange of energy between the two.
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 surroundingsBvU said:Is it really clear to you that (A) and (B) are not true ?
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?BvU said:Nothing happens to the surroundings (if all that occurs is this adiabatic expansion). There is no ##\delta Q##, so no ## \delta S##.
More through energy conservation plus ##dQ = TdS##.Silviu said:change in entropy of the system exactly compensate the one of the surrounding
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.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?