Second law of thermodynamics

The second law of thermodynamics for a reversible change (that is to say that the system evolves through a succession of equilibrium states) can be written as

$dQ=TdS$

Thus for a closed system, having a fixed number of atoms/molecules, one has

$dU=TdS-PdV$

where $U$ is the internal energy. For an open system:

$dU=TdS-PdV+\mu dN$

where $\mu$ is the chemical potential.

For $U(S,V)$ one has the following total differential

$dU={(\frac{\partial U}{\partial S})}_{V}dS+{(\frac{\partial U}{\partial V})}_{S}dV$

See also

• Entropy
• Fluctuation theorem
• H-theorem

References

Related reading

• Nicolas Léonard Sadi Carnot "Réflexions sur la puissance motrice du feu et sur les machines propres à développer cette puissance" (1824), printed in Annales scientifiques de l'École Normale Supérieure Sér. 2, 1 pp. 393-457 (1872)
• Esther Hänggi and Stephanie Wehner "A violation of the uncertainty principle implies a violation of the second law of thermodynamics", arXiv:1205.6894v1 [quant-ph] Thu, 31 May 2012
• K. S. Glavatskiy "Lagrangian formulation of irreversible thermodynamics and the second law of thermodynamics", Journal of Chemical Physics 142 204106 (2015)
• Arieh Ben-Naim "Discover Entropy and the Second Law of Thermodynamics: A Playful Way of Discovering a Law of Nature" World Scientific Publishing (2010) ISBN: 978-981-4299-75-6
• Arieh Ben-Naim "Entropy and the Second Law Interpretation and Misss-Interpretations", World Scientific Publishing (2012) ISBN 978-981-4407-55-7