Book contents
- Frontmatter
- Contents
- Preface
- Acknowledgements
- 1 A simple model of fluid mechanics
- 2 Two routes to hydrodynamics
- 3 Inviscid two-dimensional lattice-gas hydrodynamics
- 4 Viscous two-dimensional hydrodynamics
- 5 Some simple three-dimensional models
- 6 The lattice-Boltzmann method
- 7 Using the Boltzmann method
- 8 Miscible fluids
- 9 Immiscible lattice gases
- 10 Lattice-Boltzmann method for immiscible fluids
- 11 Immiscible lattice gases in three dimensions
- 12 Liquid-gas models
- 13 Flow through porous media
- 14 Equilibrium statistical mechanics
- 15 Hydrodynamics in the Boltzmann approximation
- 16 Phase separation
- 17 Interfaces
- 18 Complex fluids and patterns
- Appendix A Tensor symmetry
- Appendix B Polytopes and their symmetry group
- Appendix C Classical compressible flow modeling
- Appendix D Incompressible limit
- Appendix E Derivation of the Gibbs distribution
- Appendix F Hydrodynamic response to forces at fluid interfaces
- Appendix G Answers to exercises
- Author Index
- Subject Index
Preface
Published online by Cambridge University Press: 23 September 2009
- Frontmatter
- Contents
- Preface
- Acknowledgements
- 1 A simple model of fluid mechanics
- 2 Two routes to hydrodynamics
- 3 Inviscid two-dimensional lattice-gas hydrodynamics
- 4 Viscous two-dimensional hydrodynamics
- 5 Some simple three-dimensional models
- 6 The lattice-Boltzmann method
- 7 Using the Boltzmann method
- 8 Miscible fluids
- 9 Immiscible lattice gases
- 10 Lattice-Boltzmann method for immiscible fluids
- 11 Immiscible lattice gases in three dimensions
- 12 Liquid-gas models
- 13 Flow through porous media
- 14 Equilibrium statistical mechanics
- 15 Hydrodynamics in the Boltzmann approximation
- 16 Phase separation
- 17 Interfaces
- 18 Complex fluids and patterns
- Appendix A Tensor symmetry
- Appendix B Polytopes and their symmetry group
- Appendix C Classical compressible flow modeling
- Appendix D Incompressible limit
- Appendix E Derivation of the Gibbs distribution
- Appendix F Hydrodynamic response to forces at fluid interfaces
- Appendix G Answers to exercises
- Author Index
- Subject Index
Summary
We believe that the computer simulation of physics should retain the elegance of physics itself. This book is about one approach towards this objective: lattice-gas cellular automata models of fluids.
Cellular automata are fully discrete models of physical and other systems. Lattice gases are just what the name says: a model of a gas on a grid. Thus lattice-gas cellular automata are a special kind of gas in which identical particles hop from site to site on a lattice at each tick of a clock. When particles meet they collide, but they always stay on the grid and appropriate physical quantities are always conserved.
Our subject is interesting because it provides a new way of thinking about the simulation of fluids. It also provides an instructive link between the microscopic world of molecular dynamics and the macroscopic world of fluid mechanics. Lastly, it allows us to create new computational tools that can be usefully applied to solve certain problems.
There are, broadly speaking, two ways to use computers to make progress in physics. The first approach is to use computers to compute a number, say the result of a certain integral or the hydrodynamic drag past a certain body. The second is to use computers as a kind of experimental laboratory, to explore the phenomena of interest much as an experimentalist would do him or herself. In the former case, realism is essential—if you do not solve the right equations, then you will not compute the right drag.
- Type
- Chapter
- Information
- Lattice-Gas Cellular AutomataSimple Models of Complex Hydrodynamics, pp. xv - xviiiPublisher: Cambridge University PressPrint publication year: 1997