1 |
|
2 |
|
3 |
\chapter{\label{chapt:intro}Introduction and Theoretical Background} |
4 |
|
5 |
|
6 |
|
7 |
\section{\label{introSec:theory}Theoretical Background} |
8 |
|
9 |
The techniques used in the course of this research fall under the two |
10 |
main classes of molecular simulation: Molecular Dynamics and Monte |
11 |
Carlo. Molecular Dynamic simulations integrate the equations of motion |
12 |
for a given system of particles, allowing the researher to gain |
13 |
insight into the time dependent evolution of a system. Diffusion |
14 |
phenomena are readily studied with this simulation technique, making |
15 |
Molecular Dynamics the main simulation technique used in this |
16 |
research. Other aspects of the research fall under the Monte Carlo |
17 |
class of simulations. In Monte Carlo, the configuration space |
18 |
available to the collection of particles is sampled stochastichally, |
19 |
or randomly. Each configuration is chosen with a given probability |
20 |
based on the Maxwell Boltzman distribution. These types of simulations |
21 |
are best used to probe properties of a system that are only dependent |
22 |
only on the state of the system. Structural information about a system |
23 |
is most readily obtained through these types of methods. |
24 |
|
25 |
Although the two techniques employed seem dissimilar, they are both |
26 |
linked by the overarching principles of Statistical |
27 |
Thermodynamics. Statistical Thermodynamics governs the behavior of |
28 |
both classes of simulations and dictates what each method can and |
29 |
cannot do. When investigating a system, one most first analyze what |
30 |
thermodynamic properties of the system are being probed, then chose |
31 |
which method best suits that objective. |
32 |
|
33 |
\subsection{\label{introSec:statThermo}Statistical Thermodynamics} |
34 |
|
35 |
ergodic hypothesis |
36 |
|
37 |
enesemble averages |
38 |
|
39 |
\subsection{\label{introSec:monteCarlo}Monte Carlo Simulations} |
40 |
|
41 |
The Monte Carlo method was developed by Metropolis and Ulam for their |
42 |
work in fissionable material.\cite{metropolis:1949} The method is so |
43 |
named, because it heavily uses random numbers in the solution of the |
44 |
problem. |
45 |
|
46 |
|
47 |
\subsection{\label{introSec:md}Molecular Dynamics Simulations} |
48 |
|
49 |
time averages |
50 |
|
51 |
time integrating schemes |
52 |
|
53 |
time reversible |
54 |
|
55 |
symplectic methods |
56 |
|
57 |
Extended ensembles (NVT NPT) |
58 |
|
59 |
constrained dynamics |
60 |
|
61 |
\section{\label{introSec:chapterLayout}Chapter Layout} |
62 |
|
63 |
\subsection{\label{introSec:RSA}Random Sequential Adsorption} |
64 |
|
65 |
\subsection{\label{introSec:OOPSE}The OOPSE Simulation Package} |
66 |
|
67 |
\subsection{\label{introSec:bilayers}A Mesoscale Model for Phospholipid Bilayers} |