Math 2.0

Classical thermodynamics, heat transfer Laws of thermodynamics Fact

Nernst heat theorem

Builds on EntropyThermodynamic temperatureIsothermal processThermodynamic equilibriumGibbs free energyEnthalpy

Statement

Let a system in internal equilibrium undergo an isothermal process at thermodynamic temperature TT between two equilibrium states. Let ΔS(T)\Delta S(T) be the change of its entropy in this process. Then ΔS(T)→0\Delta S(T) \to 0 as T→0+T \to 0^+.

Remarks

Walther Nernst first stated it for chemical reactions between condensed phases. In that form it says that the changes of Gibbs free energy and enthalpy of the reaction satisfy ΔG−ΔH=−T ΔS→0\Delta G - \Delta H = -T \, \Delta S \to 0 faster than TT. So the curves of ΔG\Delta G and ΔH\Delta H against TT meet at T=0T = 0 with a common horizontal tangent. The theorem is a postulate supported by experiment, and quantum statistical mechanics explains it when the ground state is not degenerate. It fails for systems that are not in internal equilibrium, such as glasses, which keep a residual entropy.

Going deeper

For a student

The Nernst heat theorem is one form of the third law of thermodynamics. It allows absolute values of entropy to be assigned, so that equilibrium constants of reactions can be computed from heat measurements alone. It also implies that heat capacities tend to 00 as T→0+T \to 0^+.

Reading path

To understand this page from the ground up, read these 7 pages in order. The foundations come first.

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  1. Enthalpy concept
  2. Entropy concept
  3. Gibbs free energy concept
  4. Isothermal process concept
  5. Thermodynamic equilibrium concept
  6. Thermodynamic temperature concept
  7. Nernst heat theorem statement

Where this leads

2 pages build on this one.

Further reading

  1. Web https://en.wikipedia.org/wiki/Nernst_heat_theorem
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MSC80A05, 80A10
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AboutEntropy
UsesEntropy, Thermodynamic temperature, Isothermal process, Thermodynamic equilibrium, Gibbs free energy, Enthalpy
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Changed3 November 2026

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