Thermodynamic Systems with Two Independent Variables: The Flaw in the 2nd Law

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In a thermodynamic system with two independent variables, such as a gas at equilibrium, two transformations at constant volume yield the same change in internal energy when heat Q is added. However, the discussion highlights a contradiction with the second law of thermodynamics, which suggests that the final entropy should differ between reversible and irreversible processes. It is argued that while the final states may appear identical, the assumptions made about heat transfer are inconsistent, as irreversible processes involve less heat transfer than reversible ones. The pressure changes in a fixed volume container must be considered, as they influence entropy and maintain compliance with the second law. Overall, the discussion emphasizes the importance of accurately defining thermodynamic assumptions to avoid contradictions.
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Consider a thermodynamic system of two independent variables, like a gas inside a recipient,
at equilibrium.

We are now going to carry out two different transformations at constant volume:

Transformation 1) A reversible process where an amount of heat Q is "given" to the system
Transformation 2) An irreversible process where the same amount of heat Q is "given" to the system.

In both transformations the change of Internal energy (E) is the same, once volume is constant for both (Q=change of Internal energy)

Therefore if we choose as independent variables, Internal Energy and volume, we obtain:

Transformation 1) Initial state E1 and V and final state E2 and V
Transformation 2) Initial state E1 and V and final state E2 and V

As there are only two independent variables, the final state of the system is the same for transfomations 1 and 2 and therefore the final entropy is also the same in both cases. This is not what the 2nd law tells us
 
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How can volume be both a constant and a variable?
 
oramao said:
As there are only two independent variables, the final state of the system is the same for transfomations 1 and 2 and therefore the final entropy is also the same in both cases. This is not what the 2nd law tells us
How are you imagining that Q can be added to the system reversibly with no change in volume? What could be changing such that Q should reversibly enter this system? The reason Q moves around in reversible equilibria is that something is changing that forces Q to move to keep the entropy the same, so if nothing changes, there's no reason for Q to go anywhere-- unless it is not a reversible equilibrium (like a T difference).
 
A gas in a fixed volume container, with added heat to it, will change the final energy of the system. Remember, entropy relations for fixed volume have to account for the increase in pressure inside the container. Thus, the changing pressure keeps the entropy constant, thus not violating the 2nd law!
 
oramao said:
This is not what the 2nd law tells us

I think you have specified inconsistent assumptions. Kind of like proving that all triangles are isosceles: you start by picking any vertex and dropping the perpendicular to the midpoint of the other side ;-)

The "catch" in your assumptions, in addition to the comments provided by the others above, is that the heat transfer for an irreversible process is strictly less than TdS. Only for a reversible process does δQ=TdS. So the end states are not the same.

BBB
 
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