Is the 3rd law of thermodynamics necessary?

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Discussion Overview

The discussion centers around the necessity of the third law of thermodynamics and whether it can be derived from the second law. Participants explore the implications of absolute zero temperature and the relationship between temperature and entropy.

Discussion Character

  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • One participant questions if the third law can be derived from the second law, using Carnot's theorem to argue that a thermal reservoir at absolute zero would imply infinite efficiency, which contradicts the second law.
  • Another participant asserts the necessity of the third law, stating that it establishes a relationship between temperature and entropy, particularly that as temperature approaches absolute zero, entropy approaches zero.
  • A different participant disagrees with the possibility of deriving the third law from the second law, suggesting that such a derivation would be recognized as a theorem if it were valid.
  • Some participants express varying levels of understanding regarding the arguments presented, with one indicating comprehension and another expressing confusion.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the necessity of the third law or its derivation from the second law, with multiple competing views remaining in the discussion.

Contextual Notes

There are unresolved assumptions regarding the definitions of thermodynamic processes and the implications of absolute zero, as well as the relationship between the laws of thermodynamics.

Feynmanfan
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Here's a question my thermodynamics teacher was unable to answer. I present it to you and see where the flaw of my argument is.

Is it possible to derive the 3rd law of thermodynamics from the 2nd law?

Carnot's theorem (no other machine than Carnot's has maximum efficiency) tells us that when the process is reversible (Carnot engine)
Q2/Q1=T2/T1 and therefore it is possible to define an absolute temperature. Now if there were a thermal reservoir at T2=0, it would be possible to have a more efficient engine than Carnot's. T2=0 -> Q2=0 and efficiency=1
This argument holds the other way around, it is impossible to have Q2=0 (2nd law) therefore T2=0 cannot be zero.

Our teacher argues that Einstein tackled this problem and demostrated that it has no physical sense to talk about ADIABATIC and ISOTHERMAL processes at the same time (I mean simultaneously). This, I do not understand.

What do you think? Why do we need a 3rd law? Thanks for your help.
 
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Of course it is necessary
the 3rd law states that
" As the temperature tends to absolute zero the entropy also tends to zero. "

It must remembered that the entropy gives the direction of a process.
therefore, if entropy = o there is no thermodynamic process and the third law gives the relation temperature and entropy.
Sampath :smile:
 
No, it isn't possible. Else it would be stated as a theorem in theoretical thermodynamics. It can be however proven as being valid for every thermodynamical system for which one derives the thermodynamics starting from (equilibirum) statistical mechanics...

Daniel.
 
I get it.
Sampath
 
I don't.

~Kitty
 

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