A new discrete velocity method for Navier-Stokes equationsThe relation between Latttice Boltzmann Method, which has recently become popular, and the Kinetic Schemes, which are routinely used in Computational Fluid Dynamics, is explored. A new discrete…Michael Junk, S. V. Raghurama Rao·Jul 22, 1999SaveLearn
Construction of Molecular Dynamics Like Cellular Automata Models for Simulation of Compressible Fluid Dynamic SystemsThis study aims at finding a method for constructing molecular dynamics like models using the formalism of cellular automata for fast simulation of fluid dynamic systems (including compressible…Himanshu Agrawal·May 13, 1999SaveLearn
Lattice Gases and Cellular AutomataWe review the class of cellular automata known as lattice gases, and their applications to problems in physics and materials science. The presentation is self-contained, and assumes very little prior…Bruce M. Boghosian·May 5, 1999SaveLearn
Cellular Automaton Rule184++C. A Simple Model for the Complex Dynamics of Various Particles FlowA cellular automaton named Rule 184++C is proposed as a meta-model to investigate the flow of various complex particles. In this model, unlike the granular pipe flow and the traffic flow, not only…A. Awazu·Feb 25, 1999SaveLearn
Exact results for deterministic cellular automata traffic modelsWe present a rigorous derivation of the flow at arbitrary time in a deterministic cellular automaton model of traffic flow. The derivation employs regularities in preimages of blocks of zeros,…Henryk Fuks·Feb 4, 1999SaveLearn
Crystalline ComputationA cellular automaton is a deterministic and exactly computable dynamical system which mimics certain fundamental aspects of physical dynamics such as spatial locality and finite entropy. CA systems…Norman Margolus·Nov 10, 1998SaveLearn
Cellular Automaton Model for Immunology of Tumor GrowthThe stochastic discrete space-time model of an immune response on tumor spreading in a two-dimensional square lattice has been developed. The immunity-tumor interactions are described at the cellular…Margarita Voitikova·Nov 2, 1998SaveLearn
Lattice-Gas Simulations of Ternary Amphiphilic Fluid Flow in Porous MediaWe develop our existing two-dimensional lattice-gas model to simulate the flow of single-phase, binary-immiscible and ternary-amphiphilic fluids. This involves the inclusion of fixed obstacles on the…P. V. Coveney, J. -B. Maillet, J. L. Wilson et al.·Oct 13, 1998SaveLearn
Inverse Chapman-Enskog Derivation of the Thermohydrodynamic Lattice-BGK Model for the Ideal GasA thermohydrodynamic lattice-BGK model for the ideal gas was derived by Alexander et al. in 1993, and generalized by McNamara et al. in the same year. In these works, particular forms for the…Bruce M. Boghosian, Peter V. Coveney·Oct 13, 1998SaveLearn
Lattice Boltzmann simulations of three-dimensional single droplet deformation and breakup under simple shear flowWe present three-dimensional numerical simulations of the classical Taylor experiment on droplet deformation within a shear flow. We have used the promising Lattice-Boltzmann method numerical scheme…Haowen Xi, Comer Duncan·Jul 29, 1998SaveLearn
Lattice-Boltzmann Simulations of Fluid Flows in MEMSThe lattice Boltzmann model is a simplified kinetic method based on the particle distribution function. We use this method to simulate problems in MEMS, in which the velocity slip near the wall plays…Xiaobo Nie, Gary D. Doolen, Shiyi Chen·Jun 11, 1998SaveLearn
Generalized Thermal Lattice GasesWe show how to employ thermal lattice gas models to describe non-equilibrium phenomena. This is achieved by relaxing the restrictions of the usual micro-canonical ensemble for these models via the…O. Baran, C. C. Wan, R. Harris·May 7, 1998SaveLearn
Effect of Boundary Conditions on Cellular Automata that Classify DensityThe properties of two-state nearest-neighbour cellular automata (CA) that are capable of density classification are discussed. It is shown that these CA actually conserve the total density, rather…N. Sukumar·Apr 1, 1998SaveLearn
Lindenmayer systems as a model of computationsLS is a particular type of computational processes simulating living tissue. They use an unlimited branching process arising from the simultaneous substitutions of some words instead of letters in…Yuri Ozhigov·Jan 17, 1998SaveLearn
Computations on Nondeterministic Cellular AutomataThe work is concerned with the trade-offs between the dimension and the time and space complexity of computations on nondeterministic cellular automata. It is proved, that 1). Every NCA A of…Yuri Ozhigov·Jan 16, 1998SaveLearn
Discretization of the velocity space in solution of the Boltzmann equationWe point out an equivalence between the discrete velocity method of solving the Boltzmann equation, of which the lattice Boltzmann equation method is a special example, and the approximations to the…Xiaowen Shan, Xiaoyi He·Dec 10, 1997SaveLearn
Lattice Fluid Dynamics from Perfect Discretizations of Continuum FlowsWe use renormalization group methods to derive equations of motion for large scale variables in fluid dynamics. The large scale variables are averages of the underlying continuum variables over cubic…E. Katz, U. -J. Wiese·Sep 12, 1997SaveLearn
Dynamic Predictions from Time Series Data- An Artificial Neural Network ApproachA hybrid approach, incorporating concepts of nonlinear dynamics in artificial neural networks (ANN), is proposed to model time series generated by complex dynamic systems. We introduce well known…D. R. Kulkarni, A. S. Pandya, J. C. Parikh·Jun 27, 1997SaveLearn
Phase Segregation Dynamics in Particle Systems with Long Range Interactions I: Macroscopic LimitsWe present and discuss the derivation of a nonlinear non-local integro-differential equation for the macroscopic time evolution of the conserved order parameter of a binary alloy undergoing phase…G. Giacomin, J. L. Lebowitz·Apr 29, 1997SaveLearn
Lattice Gas Prediction is P-completeWe show that predicting the HPP or FHP III lattice gas for finite time is equivalent to calculating the output of an arbitrary Boolean circuit, and is therefore P-complete: that is, it is just as…Cristopher Moore, Mats G. Nordahl·Apr 17, 1997SaveLearn
Solution of the Density Classification Problem with Two Cellular Automata RulesRecently, Land and Belew [Phys. Rev. Lett. 74, 5148 (1995)] have shown that no one-dimensional two-state cellular automaton which classifies binary strings according to their densities of 1's and…Henryk Fuks·Mar 7, 1997SaveLearn
A New Fast Method for Determining Local Properties of Striped PatternsFrom the striped coats of zebras to the ripples in windblown sand, the natural world abounds with locally banded patterns. Such patterns have been of great interest throughout history, and, in the…David A. Egolf, Ilarion V. Melnikov, Eberhard Bodenschatz·Feb 7, 1997SaveLearn
Simulation of Rayleigh-Bénard convection using lattice Boltzmann methodRayleigh-Bénard convection is numerically simulated in two- and three-dimensions using a recently developed two-component lattice Boltzmann equation (LBE) method. The density field of the second…Xiaowen Shan·Dec 9, 1996SaveLearn
Data Analysis Techniques for Resolving Nonlinear Processes in Plasmas : a ReviewThe growing need for a better understanding of nonlinear processes in plasma physics has in the last decades stimulated the development of new and more advanced data analysis techniques. This review…T. Dudok de Wit·Nov 22, 1996SaveLearn
On pressure and velocity flow boundary conditions and bounceback for the lattice Boltzmann BGK modelPressure (density) and velocity boundary conditions inside a flow domain are studied for 2-D and 3-D lattice Boltzmann BGK models (LBGK) and a new method to specify these conditions are proposed.…Qisu Zou, Xiaoyi He·Nov 21, 1996SaveLearn