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2012 | OriginalPaper | Chapter

2. Postulates of Thermodynamics

Author : Dr. Ernő Keszei

Published in: Chemical Thermodynamics

Publisher: Springer Berlin Heidelberg

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Abstract

In this chapter, postulates are announced in the form taken from the book of Herbert B. Callen, ready for actual thermodynamic calculations. The explanation of what a phenomenological or macroscopic treatment means is followed by the specification of equilibrium. Postulate 1 exactly defines thermodynamic equilibrium. Its important consequence – the measurability of internal energy – is described in details. Postulate 2 – the criterion of equilibrium, and the existence of entropy – is formulated in connection with composite systems and internal constraints. Postulate 3 specifies mathematical properties of the entropy function, like additivity, differentiability, and monotonity with respect to energy. An important consequence of these properties is the homogeneous first-order nature of this function. Extensive and intensive properties are also defined here. Euler relation and Gibbs–Duhem equation is derived and explained. There is a first mention of the fundamental equation which describes all possible states of a thermodynamic system. Postulate 4 specifies the scale of entropy and the possibility to completely determine its value. The second part of the chapter explains the relation of equations of state and the fundamental equation, followed by two model systems to demonstrate these relations; the ideal gas and the ideal van der Waals fluid.

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Footnotes
1
The term internal energy refers to the energy content of the thermodynamic system which does not include either the kinetic energy or the potential energy acting on the whole system. In other words, it is the energy of the system if the entire system as a whole has zero velocity, zero angular momentum and there is no field acting on the system as a whole. It can be considered as the sum of the energy of the particles in their microscopic modes of motion without the above mentioned contributions. However, as the scale of the energy is not absolute (we can determine it only up to an additive constant), we can restrict the microscopic modes to contribute to the internal energy. Nuclear energy is usually not included in the summation to get the internal energy as it does not change in typical everyday applications of thermodynamics.
 
2
This scale has been suggested by the Swedish astronomer Anders Celsius (1701–1744).
 
3
This scale has been suggested by the German physicist Daniel Gabriel Fahrenheit (1686–1736).
 
4
William Thomson (1824–1907) – after his ennoblement by Queen Victoria, Baron Kelvin of Largs or Lord Kelvin – was a Scottish physicist. He had an important contribution to the establishment of the science of thermodynamics.
 
5
Leonhard Euler (1707–1783) was a Swiss mathematician and physicist working mainly in Saint Petersburg (Russia). He was the most prolific and important scientist of the eighteenth century. His results concerning homogeneous functions are among his “humble” achievements compared to his other theorems.
 
6
Josiah Willard Gibbs (1839–1903) was an American physicist. He was one of the first scientists in the United States who had all of his university studies in the US. His important contributions to thermodynamics included the general theory of phase equilibria and surface equilibria. His formal foundations of statistical thermodynamics are still in use.
 
7
Johannes Diderik van der Waals (1837–1923), the Dutch physicist conceived the first equation of state describing both gases and liquids, later named after him. He also interpreted molecular interactions playing a role in the underlying principles, later called van der Waals forces.
 
Literature
go back to reference Callen HB (1985) Thermodynamics and an introduction to thermostatistics, 2nd edn. Wiley, New York Callen HB (1985) Thermodynamics and an introduction to thermostatistics, 2nd edn. Wiley, New York
go back to reference Mohr PJ, Taylor BN, Newell DB (2007) CODATA recommended values of the fundamental physical constants: 2006. National Institute of Standards and Technology, Gaithersburg, MD Mohr PJ, Taylor BN, Newell DB (2007) CODATA recommended values of the fundamental physical constants: 2006. National Institute of Standards and Technology, Gaithersburg, MD
Metadata
Title
Postulates of Thermodynamics
Author
Dr. Ernő Keszei
Copyright Year
2012
Publisher
Springer Berlin Heidelberg
DOI
https://doi.org/10.1007/978-3-642-19864-9_2

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