Book contents
- Frontmatter
- Contents
- Preface
- 1 Introduction
- PART ONE FUNDAMENTALS OF STATISTICAL THERMODYNAMICS
- PART TWO QUANTUM MECHANICS AND SPECTROSCOPY
- PART THREE STATISTICAL THERMODYNAMICS IN THE DILUTE LIMIT
- PART FOUR STATISTICAL THERMODYNAMICS BEYOND THE DILUTE LIMIT
- PART FIVE NONEQUILIBRIUM STATISTICAL THERMODYNAMICS
- PART SIX THE ENSEMBLE METHOD OF STATISTICAL THERMODYNAMICS
- PART SEVEN APPENDICES
- A Physical Constants and Conversion Factors
- B Series and Integrals
- C Periodic Table
- D Mathematical Procedures
- E Thermochemical Data for Ideal Gases
- F Summary of Classical Thermodynamics
- G Review of Classical Mechanics
- H Review of Operator Theory
- I The Spherical Coordinate System
- J Electronic Energy Levels
- K Energy-Mode Parameters for Molecules
- L Normal Mode Analysis
- M Tabulation of Debye Function
- N Maxwell–Boltzmann Energy Distribution
- O Force Constants for the Lennard–Jones Potential
- P Collision Integrals for Calculating Transport Properties from the Lennard–Jones Potential
- Q Reduced Second Virial Coefficient from the Lennard–Jones Potential
- R References and Acknowledgments
- Index
C - Periodic Table
Published online by Cambridge University Press: 05 June 2012
Book contents
- Frontmatter
- Contents
- Preface
- 1 Introduction
- PART ONE FUNDAMENTALS OF STATISTICAL THERMODYNAMICS
- PART TWO QUANTUM MECHANICS AND SPECTROSCOPY
- PART THREE STATISTICAL THERMODYNAMICS IN THE DILUTE LIMIT
- PART FOUR STATISTICAL THERMODYNAMICS BEYOND THE DILUTE LIMIT
- PART FIVE NONEQUILIBRIUM STATISTICAL THERMODYNAMICS
- PART SIX THE ENSEMBLE METHOD OF STATISTICAL THERMODYNAMICS
- PART SEVEN APPENDICES
- A Physical Constants and Conversion Factors
- B Series and Integrals
- C Periodic Table
- D Mathematical Procedures
- E Thermochemical Data for Ideal Gases
- F Summary of Classical Thermodynamics
- G Review of Classical Mechanics
- H Review of Operator Theory
- I The Spherical Coordinate System
- J Electronic Energy Levels
- K Energy-Mode Parameters for Molecules
- L Normal Mode Analysis
- M Tabulation of Debye Function
- N Maxwell–Boltzmann Energy Distribution
- O Force Constants for the Lennard–Jones Potential
- P Collision Integrals for Calculating Transport Properties from the Lennard–Jones Potential
- Q Reduced Second Virial Coefficient from the Lennard–Jones Potential
- R References and Acknowledgments
- Index
Summary
The atomic number (top left) is the number of protons in the nucleus. The atomic mass (bottom) is weighted by mean isotopic abundances in the earth's surface. Atomic masses are relative to the mass of the carbon-12 isotope, defined to be exactly 12 atomic mass units (amu). If sufficiently stable isotopes do not exist for an element, the mass of its longest-lived isotope is indicated in parentheses. For elements 110–112, the mass numbers of the known isotopes are given. Reference: Schroeder (2000) as extracted from The European Physical JournalC3, 73 (1998).
Information
- Type
- Chapter
- Information
- Statistical ThermodynamicsFundamentals and Applications, pp. 391 - 392Publisher: Cambridge University PressPrint publication year: 2005
Accessibility standard: Unknown
Accessibility compliance for the PDF of this book is currently unknown
and may be updated in the future.