Abstract

We present a history of thermodynamics. Part 1 discusses definitions, a pre-history of heat and temperature, and steam engine efficiency, which motivated thermodynamics. Part 2 considers in detail three heat conservation-based foundational papers by Carnot, Clapeyron, and Thomson. For a reversible Carnot cycle operating between thermal reservoirs with Celsius temperatures t and , heat Q from the hot reservoir, and net work W, Clapeyron derived , with material-independent. Thomson used to define an absolute temperature but, unaware that an additional criterion was needed, he first proposed a logarithmic function of the ideal gas temperature . Part 3, following a discussion of conservation of energy, considers in detail a number of energy conservation-based papers by Clausius and Thomson. As noted by Gibbs, in 1850, Clausius established the first modern form of thermodynamics, followed by Thomson’s 1851 rephrasing of what he called the Second Law. In 1854, Clausius theoretically established for a simple Carnot cycle the condition . He generalized it to , and then . This both implied a new thermodynamic state function and, with appropriate integration factor , the thermodynamic temperature. In 1865, Clausius named this new state function the entropy S.

Highlights

  • An article on the history of thermodynamics can do no worse than begin by citing the first usage of any version of the word thermodynamics

  • This work traces the origins of thermodynamics, with an emphasis on the logical order of the concepts

  • We note that the material-independent efficiency of a reversible heat engine defines only a well-ordered set of numbers corresponding to temperature, consistent with Thomson’s proposal of two distinct material-independent temperature scales, the second being the ideal gas scale in Kelvin units

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Summary

Introduction

An article on the history of thermodynamics can do no worse than begin by citing the first usage of any version of the word thermodynamics. In 1854, Clausius brought thermodynamics to a more mature form by establishing the uniqueness of a quantity equivalent to what in 1865 he called the entropy S That is, he showed that, on using the ideal gas temperature scale Tg and measuring the heat flow dQ into the system, for any closed. 0 for all paths in p-v space, one can determine which of two or more temperature scales is “better” [18] This resolution led me to study how Clausius’s entropy became established in the lore of physics, and the meaningful study of Clausius led to the study of his predecessors, and the present work

An Overview
Outline of Thermodynamics Prehistory
Outline of Thermodynamics Based on Conservation of Heat
Outline of Thermodynamics Based on Conservation of Energy
Additional Topics
On Definitions
Energy and Work
Temperature
Heat as Fluid—Caloric
Heat as Motion—Vis Viva
On the Steam Engine
Carnot
Analyzing the Efficiency of Heat Engines
Difficulties with Carnot’s Analysis
Clapeyron
Ideal Gas and Heat Function Q
Ideal Gas and Carnot Efficiency
Ideal Gas and dependence of Q on v
Ideal Gas and Specific Heats
General Case
Thomson 1848
Thomson 1849
The Thomson Brothers and the Ice-Water Transition
Thomson’s 1849 Paper Itself
Thomson’s Four-Part Appendix
On Energy Conservation
10. Clausius 1850
10.1. Ideal Gas and Specific Heats
10.2. Ideal Gas and Adiabatic Condition
10.3. Thermodynamic Efficiency
10.5. Steam and Clausius-Clapeyron Equation
11. Thomson 1851
12. Clausius 1854
12.1. Clausius’s Two Types of “Equivalences of Transformation”
12.2. The Reversibility Condition
12.3. Finding the Absolute Temperature
13. Thomson-Joule 1854
14. Priority Disputes
15. Clausius and Entropy 1865
16. Rankine
17. On Entropy Production and Wasted Energy
18. Conclusions
43. Original
45. Original
Full Text
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