Clausius inequality temperature

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SUMMARY

The Clausius inequality defines the temperature T as that at the interface between the system and its surroundings, specifically where the differential heat dQ enters. In irreversible processes, the temperature within the system is typically non-uniform. The inequality is mathematically represented as ΔS≥∫_0^t∫_A{(q/T)·n dA}dt, where q is the local heat flux vector, n is the inwardly directed unit normal, and the area integral encompasses the entire interface. This formulation emphasizes the importance of the interface temperature in thermodynamic processes.

PREREQUISITES
  • Understanding of thermodynamic principles, specifically the Clausius inequality.
  • Familiarity with heat transfer concepts and local heat flux vectors.
  • Knowledge of irreversible processes in thermodynamics.
  • Basic calculus for interpreting integrals in thermodynamic equations.
NEXT STEPS
  • Study the derivation and applications of the Clausius inequality in thermodynamics.
  • Explore the concept of local heat flux and its role in energy transfer.
  • Investigate the implications of temperature gradients in irreversible processes.
  • Learn about the principles of entropy and its relation to thermodynamic systems.
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Students and professionals in thermodynamics, physicists, and engineers focusing on heat transfer and entropy in irreversible processes will benefit from this discussion.

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in the clausius inequality is the temperature that of the system or of the surroundings? or is it temperature of the body receiving positive heat?
(assuming the irreversibility is due to heat transfer with finite temperature difference)
[borgnakke and sonntag-principle of entropy increase for control volume]
 
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In the Clausius inequality, T is the temperature at the interface between the system and the surroundings, at the location where dQ is entering. In an irreversible process, the temperature within the system is not usually uniform.

A more precise representation of the Clausius inequality is given by:
ΔS≥\int_0^t\int_A{(\frac{\vec{q }}{T})\centerdot \vec{n} dA}dt
where \vec{q} is the local heat flux vector at the interface, \vec{n} is an inwardly directed unit normal across the interface drawn from the surroundings to the system, and T is the temperature at the interface. The area integral is over the entire instantaneous interface between the system and the surroundings (the interface may be moving during the process), and the time integral is over the (irreversible) process from the initial thermodynamic equilibrium state to the final equilibrium state.
 

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