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

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Discussion Overview

The discussion revolves around the implications of the second law of thermodynamics in the context of a thermodynamic system with two independent variables, specifically examining transformations at constant volume. Participants explore the relationship between heat transfer, internal energy, and entropy in reversible and irreversible processes.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant describes two transformations at constant volume: a reversible process and an irreversible process, both involving the same amount of heat Q, leading to the same change in internal energy.
  • Another participant questions the notion of volume being both constant and a variable in this context.
  • A different participant argues that adding heat to a gas in a fixed volume will change the final energy of the system and that pressure changes must be considered to maintain entropy relations, thus not violating the second law.
  • Another participant challenges the assumptions made in the initial argument, stating that heat transfer for irreversible processes is less than TdS, implying that the end states of the two transformations cannot be the same.

Areas of Agreement / Disagreement

Participants express disagreement regarding the implications of the second law of thermodynamics and the assumptions made about the transformations. No consensus is reached on the validity of the initial claims or the interpretations of the second law.

Contextual Notes

Participants highlight potential inconsistencies in assumptions regarding heat transfer and the nature of reversible versus irreversible processes. The discussion remains open to interpretation without resolving these complexities.

oramao
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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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