Book contents
- Frontmatter
- PREFACE TO THE SECOND EDITION
- Contents
- CHAP I INTRODUCTORY CHAPTER
- MATHEMATICAL THEORY OF A GAS IN A STEADY STATE
- CHAP II THE LAW OF DISTRIBUTION OF VELOCITIES: THE METHOD OF COLLISIONS
- CHAP III THE LAW OF DISTRIBUTION OF VELOCITIES: THE METHOD OF STATISTICAL MECHANICS
- CHAP IV THE LAW OF DISTRIBUTION OF VELOCITIES: COMPARISON BETWEEN THE METHODS OF THE TWO PRECEDING CHAPTERS
- CHAP V THE LAW OF DISTRIBUTION OF VELOCITIES: GENERAL STATISTICAL MECHANICS AND THERMODYNAMICS
- PHYSICAL PROPERTIES OF A GAS IN A STEADY STATE
- MATHEMATICAL THEORY OF A GAS NOT IN A STEADY STATE
- PHYSICAL PHENOMENA OF A GAS NOT IN A STEADY STATE
- RADIATION AND THE QUANTUM THEORY
- APPENDICES
CHAP IV - THE LAW OF DISTRIBUTION OF VELOCITIES: COMPARISON BETWEEN THE METHODS OF THE TWO PRECEDING CHAPTERS
Published online by Cambridge University Press: 05 July 2011
- Frontmatter
- PREFACE TO THE SECOND EDITION
- Contents
- CHAP I INTRODUCTORY CHAPTER
- MATHEMATICAL THEORY OF A GAS IN A STEADY STATE
- CHAP II THE LAW OF DISTRIBUTION OF VELOCITIES: THE METHOD OF COLLISIONS
- CHAP III THE LAW OF DISTRIBUTION OF VELOCITIES: THE METHOD OF STATISTICAL MECHANICS
- CHAP IV THE LAW OF DISTRIBUTION OF VELOCITIES: COMPARISON BETWEEN THE METHODS OF THE TWO PRECEDING CHAPTERS
- CHAP V THE LAW OF DISTRIBUTION OF VELOCITIES: GENERAL STATISTICAL MECHANICS AND THERMODYNAMICS
- PHYSICAL PROPERTIES OF A GAS IN A STEADY STATE
- MATHEMATICAL THEORY OF A GAS NOT IN A STEADY STATE
- PHYSICAL PHENOMENA OF A GAS NOT IN A STEADY STATE
- RADIATION AND THE QUANTUM THEORY
- APPENDICES
Summary
61. The problem of the present chapter will be to consider the relation between the methods of procedure adopted in Chapters II and III.
The discussion of Chapter II was based upon certain questions of probability, and an answer to these questions was made possible and was obtained by the help of the assumption of molecular chaos enunciated in § 15.
The discussion of Chapter III also rested, although in a different sense, upon the theory of probability. The generalised space filled with fluid supplied a basis for the calculation of probabilities, and as the motion of the fluid was proved to be steady-motion, it followed that this basis was independent of the time. For the present, we continue to take this generalised space as the basis of probability calculations. The question “What is the probability that a system satisfies condition p?” will be taken to mean: “For what proportion of the generalised space is condition p satisfied?” The further question: “Given that a system satisfies condition p, what is the probability that it also satisfies condition q?” will be interpreted to mean: “A point is selected at random from all those parts of the generalised space in which condition p is satisfied: what is the probability that at this point condition q also is satisfied?”
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- The Dynamical Theory of Gases , pp. 58 - 65Publisher: Cambridge University PressPrint publication year: 2009First published in: 1904