
Transport Properties and Potential Energy Models for Monatomic Gases
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Content
- 1: THE MONATOMIC BOLTZMANN EQUATION
- 1.1: The Boltzmann equation for dilute monatomic gases
- 1.2: Equations of change and collisional invariants
- 1.3: Entropy production
- 1.4: The equilibrium state
- 1.5: Linearization of the Boltzmann equation
- 1.6: The Boltzmann equations for mixtures
- 2: SOLUTIONS OF THE BOLTZMANN EQUATION
- 2.1: Chapman-Enskog solution for pure monatomic gases
- 2.2: Chapman-Enskog solution for binary mixtures
- 2.3: Matrix approximations for the inverse collision operator
- 2.4: The transport coefficients
- 2.5: Effective cross sections
- 2.6: Dynamical models for binary atomic interactions
- 2.7: The moment method
- 2.8: Kinetic models
- 3: REALISTIC INTERATOMIC POTENTIAL ENERGY FUNCTIONS
- 3.1: The need for realistic potential energy functions
- 3.2: The Mie/Lennard-Jones potential energy functions
- 3.3: Hartree-Fock plus damped dispersion semi-empirical models
- 3.4: Exchange-coulomb semi-empirical models
- 3.5: Modern empirical multiproperty-fit potential energy functions
- 3.6: Direct inversions of experimental data
- 3.7: Ab initio calculation of potential energy functions
- 3.8: Interactions between pairs of ground-term noble gas atoms
- 3.9: Interactions involving open-shell atoms
- 4: COMPARISON BETWEEN THEORY AND EXPERIMENT
- 4.1: Comparison between theory and experiment
- 4.2: Correlation concept
- 4.3: Binary mixtures of noble gases
- 5: FROM AB INITIO CALCULATIONS TO SPECTROSCOPIC AND THERMOPHYSICAL PROPERTIES
- 5.1: Ab initio calculations
- 5.2: Fitting of analytic potential energy functions
- 5.3: Spectroscopic properties
- 5.4: Thermophysical properties
- Appendix A: MATHEMATICAL APPENDICES
- A.1: Maxwellian averages
- A.2: Special functions
- A.3: Vectors and tensors
- A.4: Spherical harmonics and spherical tensors
- References
- Index
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