Monte Carlo computer simulation of sub-critical Lennard-Jones particles
<p>Cluster characteristics of the 3D Lennard-Jones, LJ, fluid are determined by Metropolis Monte Carlo computer simulations. The percolation probability and cluster distribution is calculated for several state points in the gas-liquid equilibrium region of the LJ fluid. The cluster number dist...
Main Author: | |
---|---|
Other Authors: | |
Format: | Others |
Language: | en |
Published: |
Virginia Tech
2014
|
Subjects: | |
Online Access: | http://hdl.handle.net/10919/45998 http://scholar.lib.vt.edu/theses/available/etd-11242009-020125/ |
id |
ndltd-VTETD-oai-vtechworks.lib.vt.edu-10919-45998 |
---|---|
record_format |
oai_dc |
spelling |
ndltd-VTETD-oai-vtechworks.lib.vt.edu-10919-459982021-05-08T05:26:56Z Monte Carlo computer simulation of sub-critical Lennard-Jones particles Gregory, Victor Paul Chemistry Schug, John C. Marand, Hervé L. Schick, G. Alan LD5655.V855 1991.G745 Monte Carlo method -- Computer programs -- Research Particles -- Research <p>Cluster characteristics of the 3D Lennard-Jones, LJ, fluid are determined by Metropolis Monte Carlo computer simulations. The percolation probability and cluster distribution is calculated for several state points in the gas-liquid equilibrium region of the LJ fluid. The cluster number distribution is used to analyze the distribution of clusters above and below the percolation threshold. Using scaling theory, the critical exponent, Ï , is determined from the cluster distributions. Deviation from the scaling law is evaluated using a modified scaling law that includes a surface term. It is found that the surface term is unnecessary in the gas-like area of the phase diagram. The density profiles of large non-percolating clusters are calculated in order to study the surface structure of the clusters. The coordination number within a cluster is calculated directly in the simulation and, with the cluster energy, is used to discern the amount of "liquid-like" structure of the cluster. The radius of gyration, R g, as a function of cluster size determines the fractal dimension, D f of the non-percolating and clusters above and below the percolation threshold density. Finite size effects are briefly studied and presented for a few of points.</p> Master of Science 2014-03-14T21:50:34Z 2014-03-14T21:50:34Z 1991-03-05 2009-11-24 2009-11-15 2009-11-24 Thesis Text etd-11242009-020125 http://hdl.handle.net/10919/45998 http://scholar.lib.vt.edu/theses/available/etd-11242009-020125/ en OCLC# 24041368 LD5655.V855_1991.G745.pdf vi, 87 leaves BTD application/pdf application/pdf Virginia Tech |
collection |
NDLTD |
language |
en |
format |
Others
|
sources |
NDLTD |
topic |
LD5655.V855 1991.G745 Monte Carlo method -- Computer programs -- Research Particles -- Research |
spellingShingle |
LD5655.V855 1991.G745 Monte Carlo method -- Computer programs -- Research Particles -- Research Gregory, Victor Paul Monte Carlo computer simulation of sub-critical Lennard-Jones particles |
description |
<p>Cluster characteristics of the 3D Lennard-Jones, LJ, fluid are determined by
Metropolis Monte Carlo computer simulations. The percolation probability and
cluster distribution is calculated for several state points in the gas-liquid equilibrium
region of the LJ fluid. The cluster number distribution is used to analyze the
distribution of clusters above and below the percolation threshold. Using scaling
theory, the critical exponent, Ï , is determined from the cluster distributions.
Deviation from the scaling law is evaluated using a modified scaling law that includes
a surface term. It is found that the surface term is unnecessary in the gas-like area of
the phase diagram. The density profiles of large non-percolating clusters are
calculated in order to study the surface structure of the clusters. The coordination
number within a cluster is calculated directly in the simulation and, with the cluster
energy, is used to discern the amount of "liquid-like" structure of the cluster. The
radius of gyration, R g, as a function of cluster size determines the fractal dimension,
D f of the non-percolating and clusters above and below the percolation threshold
density. Finite size effects are briefly studied and presented for a few of points.</p> === Master of Science |
author2 |
Chemistry |
author_facet |
Chemistry Gregory, Victor Paul |
author |
Gregory, Victor Paul |
author_sort |
Gregory, Victor Paul |
title |
Monte Carlo computer simulation of sub-critical Lennard-Jones particles |
title_short |
Monte Carlo computer simulation of sub-critical Lennard-Jones particles |
title_full |
Monte Carlo computer simulation of sub-critical Lennard-Jones particles |
title_fullStr |
Monte Carlo computer simulation of sub-critical Lennard-Jones particles |
title_full_unstemmed |
Monte Carlo computer simulation of sub-critical Lennard-Jones particles |
title_sort |
monte carlo computer simulation of sub-critical lennard-jones particles |
publisher |
Virginia Tech |
publishDate |
2014 |
url |
http://hdl.handle.net/10919/45998 http://scholar.lib.vt.edu/theses/available/etd-11242009-020125/ |
work_keys_str_mv |
AT gregoryvictorpaul montecarlocomputersimulationofsubcriticallennardjonesparticles |
_version_ |
1719403424673431552 |