Definition of thermal equilibrium?

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Discussion Overview

The discussion revolves around the definition of thermal equilibrium, particularly in the context of thermodynamic systems and their interactions with heat reservoirs. Participants explore the nuances between thermal equilibrium and steady state, examining the implications of temperature gradients and heat exchange.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • One participant cites a definition of thermal equilibrium from Zemansky's book, expressing confusion about its vagueness, especially regarding systems in contact with heat reservoirs at different temperatures.
  • Another participant states that two bodies are in thermal equilibrium if they have the same temperature and that this condition must remain unchanged.
  • Some participants differentiate between thermal equilibrium and steady state, noting that thermal equilibrium implies no temperature gradient (Ṫ = 0 = ∇T), while steady state refers to a condition where temperature does not change over time (∂T/∂t = 0).
  • There is a suggestion that the definition of temperature relies on the definition of thermal equilibrium, indicating a potential foundational relationship between the two concepts.
  • One participant emphasizes that thermal equilibrium is characterized by no change in the coordinates of systems when separated by a diathermal wall, while also noting that steady state conditions do not involve changes over time.
  • Another participant adds that both systems must be separated from their surroundings by an adiabatic wall to maintain thermal equilibrium.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and implications of thermal equilibrium and steady state. There is no consensus on a singular definition of thermal equilibrium, and the discussion remains unresolved regarding the precise relationship between these concepts.

Contextual Notes

Participants highlight the need for clarity in definitions, particularly concerning the conditions under which temperature can be assigned to a system and the role of local thermal equilibrium.

Arham
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Hello

In Zemansky's book there is this definition of thermal equilibrium:

"Thermal equilibrium exists when there is no spontaneous change in the
coordinates of a system in mechanical and chemical equilibrium when it is
separated from its surroundings by diathermic walls. In other words, there is
no exchange of heat between the system and its surroundings."

This is vague for me. Consider a thermodynamic system in thermal contact with two heat reservoirs at different temperatures. When the system reaches steady state then there will be no change in the coordinates of system. We have a gradient of T in that case. And there will be no net exchange of heat.

What is your opinion?

Sorry for bad english. :shy:
 
Last edited:
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Two bodies are in thermal equilibrium if they have the same temperature and if that isn't going to change.

Ll.
 
You are having a confusion between Thermal Eqb. and Steady State.
Thermal Eqb.: Ṫ = 0 = ∇T
Steady State: ∂T/∂t = 0; where T = T(r,t) is the temperature of the system.
 
Llewlyn said:
Two bodies are in thermal equilibrium if they have the same temperature and if that isn't going to change.

Ll.

Thanks. But I think definition of temperature is based on definition of thermal equilibrium. In other words I think at first we must define thermal equilibrium, and then temperature.
 
Arijit Dutta said:
You are having a confusion between Thermal Eqb. and Steady State.
Thermal Eqb.: Ṫ = 0 = ∇T
Steady State: ∂T/∂t = 0; where T = T(r,t) is the temperature of the system.

Thanks. I know this. Look! When can we assign a temperature field to a system? When there is local thermal equilibrium in the system. But what is the exact definition of thermal equilibrium?
 
2 systems are said to be in thermal equilibrium with each other if there is no change in co- ordinates of either system when they are separated by a diathermal wall.
 
Arijit Dutta said:
2 systems are said to be in thermal equilibrium with each other if there is no change in co- ordinates of either system when they are separated by a diathermal wall.

Coordinates of a system in steady state don't change with time either.
 
Last edited:
I should have added- both the systems must be separated from their surroundings by adiabatic wall.
 
Arijit Dutta said:
I should have added- both the systems must be separated from their surroundings by adiabatic wall.

Consider just these two systems: 1. The under study system which is in steady state, and 2. the rest of the world.
 

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