Zero-ith Law of Thermodynamics

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Discussion Overview

The discussion revolves around the Zeroth Law of Thermodynamics, exploring its definition, implications, and the concept of thermal equilibrium among thermodynamic systems. Participants delve into the mathematical and conceptual underpinnings of the law, as well as its relevance in various contexts.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants propose that the Zeroth Law states if system A is in thermal equilibrium with system C, and system B is also in thermal equilibrium with C, then A and B are in thermal equilibrium, even if separated by an adiabatic barrier.
  • Others argue that the law implies a useful measure called "temperature," suggesting that if A is warmer than B and B is warmer than C, then A must be warmer than C.
  • A participant references a university physics book to support the definition of the Zeroth Law, emphasizing the relationship between systems A, B, and C.
  • Another participant notes that while temperature can be equated, the heat content of the systems may differ, highlighting the importance of defining "thermal equilibrium" correctly.
  • One contributor mentions that the equality of temperature among systems is contingent upon the validity of the Second Law of Thermodynamics, suggesting a connection to entropy.
  • A later reply discusses the implications of the Zeroth Law in the context of metals and semiconductors, particularly regarding Fermi energy and chemical potential.

Areas of Agreement / Disagreement

Participants express a range of interpretations regarding the implications and definitions related to the Zeroth Law. There is no clear consensus, as some points are contested and various perspectives are presented.

Contextual Notes

Participants highlight the need for clarity in defining terms such as "thermal equilibrium" and "temperature," indicating that assumptions about these concepts may vary. The discussion also touches on the relationship between the Zeroth Law and the Second Law of Thermodynamics without resolving the complexities involved.

Mk
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I believe that the law states that if a thermodynamic system A is in thermal equilibrium with another system C, and a thermodynamic system B is also in thermal equilibrium with C, then A and B are in thermal equilibrium. This applies even if A and B are separated by an adiabatic barrier (one through which NO heat can flow)
 
It essentially says that there is a useful measure we call "temperature". IOW, the numbers make sense; If A is warmer than B and B is warmer than C, then A is warmer than C.
 
krab said:
It essentially says that there is a useful measure we call "temperature". IOW, the numbers make sense; If A is warmer than B and B is warmer than C, then A is warmer than C.


It sounds like basic math, if A is greater than B and B is greater than C than A is greater than C. :confused:
 
From a University Physics Book (Young and Freedman):
If C is initially in thermal equilibrium with both A and B, then A and B are also in thermal equilibrium with each other. This result is called the zeroth law of thermodynamics.
 
Again, if C=A=B, A=B


Mk said:
It sounds like basic math, if A is greater than B and B is greater than C than A is greater than C. :confused:
 
Mk said:
It sounds like basic math, if A is greater than B and B is greater than C than A is greater than C. :confused:
True, but remember that "temperature" is some real property.
This means, that the physicist must explicitly assume that it is meaningful to measure as a number this real property.
There exist other properties in the world which it is doubtful can ever be quantified, for example, "kindness".

A physicist who wish to develop a mathematical model of the world, is limited in talking about structures of the world which is "mathematizable".
 
If we have two thermodynamic systems which are in thermal equilibrium, there is a function of their state variables which has the same value in both systems. That function is called temperature.

So the Zeroth principle says: Let have three thermodynamic systems, we say that if A is in thermal equilibrium with C, and also with B, C and B are at thermal equilibrium.
 
Mk said:
Again, if C=A=B, A=B

There are several things that make this actually non-trivial:

1. Remember that you are equating the temperature parameter. There's nothing that says that the heat content of these A,B, and C are the same. They each could have a different heat capacity, mass, etc., but yet, all at the same temperatures. So establishing what we mean by "thermal equilibrium" is crucial. It means that only temperature is the valid parameter that is relevant, not heat content, etc, etc.

2. That equality will not be true if the 2nd Law is violated. So this is indirectly an entropy manifestation. I have seen many quacks who implicitly make use of the thermal equilibrium principle and yet, attack the validity of the 2nd law.

3. The 0th law is the very reason why, when metals and semiconductors of various kinds come in contact with each other, everything is scalled according to the location of the Fermi energy (or the chemical potential for semiconductors to be exact).

Zz.
 

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