Spelling suggestions: "subject:"lattice sas"" "subject:"lattice suas""
1 |
Dynamical and statistical properties of Lorentz lattice gasesKhlabystova, Milena 05 1900 (has links)
No description available.
|
2 |
Fluids confined by nanopatterned substratesEisenhuettenstadt 20 November 2001 (has links) (PDF)
No description available.
|
3 |
Lattice-gas automata and lattice Boltzmann equations for two-dimensional hydrodynamicsLuo, Li-Shi 05 1900 (has links)
No description available.
|
4 |
Flameletモデルを適用した燃焼場の格子ガスシミュレーションYAMAMOTO, Kazuhiro, 山本, 和弘 05 1900 (has links)
No description available.
|
5 |
The lattice gas model and Lattice Boltzmann model on hexagonal gridsJin, Kang, Meir, Amnon J. January 2005 (has links) (PDF)
Thesis(M.S.)--Auburn University, 2005. / Abstract. Vita. Includes bibliographic references (p.30-31).
|
6 |
Stochastic driven systems far from equilibrium /Kim, Kyung Hyuk, January 2006 (has links)
Thesis (Ph. D.)--University of Washington, 2006. / Vita. Includes bibliographical references (p. 96-107).
|
7 |
Monte Carlo and Series Expansion Studies of the Anisotropic Driven Ising Lattice Gas Phase DiagramShaw, Leah Belinda 27 April 1999 (has links)
While the statistical mechanics of systems in thermal equilibrium is a well established discipline, nonequilibrium systems are fundamentally much less well understood, even though most natural phenomena fall into the latter category. In particular, there is as yet no nonequilibrium analog for the systematic formalism of Gibbs ensembles. Rather than deal with the difficult problem of general nonequilibrium systems, this study is restricted to the steady states of a simple model whose equilibrium properties are well known.
The Ising lattice gas displays a number of surprising phenomena when driven into nonequilibrium steady states. This study extends previous work to a more general model with anisotropic interparticle interactions. Using Monte Carlo simulations, we obtain the phase diagram for the model, controlled by the driving field, temperature, and anisotropy parameter α. Under saturation drive, the shift in the transition temperature between ordered and disordered states can be either positive or negative, depending on α ≡ √(𝐽<sub>∥</sub>/𝐽<sub>⟂</sub>). The possible existence at large α of an additional phase ordered in only one direction is discussed. For finite drives, both first and second order transitions are observed. A novel technique for locating the first order transition line is presented.
Some aspects of the phase diagram can be predicted by investigating the two-point correlation function to first order in a high temperature series expansion. However, the series expansion fails to predict even qualitatively the α-dependence of the critical temperature. / Master of Science
|
8 |
The virial equation of state for hard particles on two-dimensional lattices /Clymer, Janis Ellen January 1983 (has links)
No description available.
|
9 |
Phase Diagram of a Driven Lattice Gas of Two Species with Attractive InteractionsLyman, Edward 05 May 2004 (has links)
We study the phase diagram of an interacting lattice gas of two species of particles and holes, driven out of equilibrium by a local hopping bias (denoted by `E').
Particles interact by excluded volume and nearest-neighbor attractions. We present a detailed Monte Carlo investigation of the phase diagram. Three phases are found, with a homogenous phase at high temperatures and two distinct ordered phases at lower temperatures. Which ordered phase is observed depends on the parameter f, which controls the ratio of the two types of particles. At small f, there is nearly a single species, and a transition is observed into a KLS-type ordered phase. At larger f, the minority species are sufficiently dense to form a transverse blockage, and a sequence of two transitions are observed as the temperature is lowered.
First, a continuous boundary is crossed into an SHZ-type ordered phase, then at a lower temperature a first-order boundary is crossed into the KLS-type ordered phase. At some critical value of f is a bicritical point, where the first-order line branches from the two continuous boundaries. We also consider correlations in the homogenous phase, by constructing a continuum description and comparing to the results of simulations. Long range correlations are present in both the theoretical results and the simulations, though certain details of the theory do not fit the observations very well. Finally, we examine the beahvior of three-point correlations in the single-species (KLS) limit. Nontrivial three-point correlations are directly related to the nonzero bias E. We therefore consider the behavior of the three-point correlations as a function of E. We find that the three-point signal saturates very rapidly with E. There are some difficulties interpreting the data at small E. / Ph. D.
|
10 |
Theoretical and Simulation Studies of a Driven Diffusive SystemRudzinsky, Michael Steven 12 February 2000 (has links)
We explore steady-state properties of a driven lattice gas, which is a simple model of interacting many-particle systems, driven far from equilibrium by an external field. First, we study a system on a square lattice with periodic boundary conditions (PBC) along both principal lattice axes, while the drive acts along only one of these axes. For such systems, we analyze the full distribution of structure factors. Next, we investigate the effects of imposing other boundary conditions on the system. In particular, we focus on models with shifted periodic boundary conditions (SPBC) along one axis and open boundary conditions (OBC) along the other axis. The OBC allow us to have a steady flux of particles through the system while the SPBC permits us to drive the system in a range of possibilities. Using Monte Carlo simulation techniques, we discover a rich variety of phenomena, especially at low temperatures. A continuum theory for the densities, based on Langevin equations, is formulated and its predictions compared to simulation data. Many large scale properties are described successfully. / Ph. D.
|
Page generated in 0.0358 seconds