| 1 |
|
\appendix |
| 2 |
< |
\chapter{\label{chapt:oopse}Object-Oriented Parallel Simulation Engine (OOPSE)} |
| 2 |
> |
\chapter{\label{chapt:oopse}Object-Oriented Parallel Simulation Engine} |
| 3 |
|
|
| 4 |
|
Designing object-oriented software is hard, and designing reusable |
| 5 |
|
object-oriented scientific software is even harder. Absence of |
| 14 |
|
coordination to enforce design and programming guidelines. Moreover, |
| 15 |
|
most MD programs also suffer from missing design and implement |
| 16 |
|
documents which is crucial to the maintenance and extensibility. |
| 17 |
+ |
Along the way of studying structural and dynamic processes in |
| 18 |
+ |
condensed phase systems like biological membranes and nanoparticles, |
| 19 |
+ |
we developed and maintained an Object-Oriented Parallel Simulation |
| 20 |
+ |
Engine ({\sc OOPSE}). This new molecular dynamics package has some |
| 21 |
+ |
unique features |
| 22 |
+ |
\begin{enumerate} |
| 23 |
+ |
\item {\sc OOPSE} performs Molecular Dynamics (MD) simulations on non-standard |
| 24 |
+ |
atom types (transition metals, point dipoles, sticky potentials, |
| 25 |
+ |
Gay-Berne ellipsoids, or other "lumpy"atoms with orientational |
| 26 |
+ |
degrees of freedom), as well as rigid bodies. |
| 27 |
+ |
\item {\sc OOPSE} uses a force-based decomposition algorithm using MPI on cheap |
| 28 |
+ |
Beowulf clusters to obtain very efficient parallelism. |
| 29 |
+ |
\item {\sc OOPSE} integrates the equations of motion using advanced methods for |
| 30 |
+ |
orientational dynamics in NVE, NVT, NPT, NPAT, and NP$\gamma$T |
| 31 |
+ |
ensembles. |
| 32 |
+ |
\item {\sc OOPSE} can carry out simulations on metallic systems using the |
| 33 |
+ |
Embedded Atom Method (EAM) as well as the Sutton-Chen potential. |
| 34 |
+ |
\item {\sc OOPSE} can perform simulations on Gay-Berne liquid crystals. |
| 35 |
+ |
\item {\sc OOPSE} can simulate systems containing the extremely efficient |
| 36 |
+ |
extended-Soft Sticky Dipole (SSD/E) model for water. |
| 37 |
+ |
\end{enumerate} |
| 38 |
|
|
| 39 |
|
\section{\label{appendixSection:architecture }Architecture} |
| 40 |
|
|
| 41 |
+ |
Mainly written by \texttt{C/C++} and \texttt{Fortran90}, {\sc OOPSE} |
| 42 |
+ |
uses C++ Standard Template Library (STL) and fortran modules as the |
| 43 |
+ |
foundation. As an extensive set of the STL and Fortran90 modules, |
| 44 |
+ |
{\sc Base Classes} provide generic implementations of mathematical |
| 45 |
+ |
objects (e.g., matrices, vectors, polynomials, random number |
| 46 |
+ |
generators) and advanced data structures and algorithms(e.g., tuple, |
| 47 |
+ |
bitset, generic data, string manipulation). The molecular data |
| 48 |
+ |
structures for the representation of atoms, bonds, bends, torsions, |
| 49 |
+ |
rigid bodies and molecules \textit{etc} are contained in the {\sc |
| 50 |
+ |
Kernel} which is implemented with {\sc Base Classes} and are |
| 51 |
+ |
carefully designed to provide maximum extensibility and flexibility. |
| 52 |
+ |
The functionality required for applications is provide by the third |
| 53 |
+ |
layer which contains Input/Output, Molecular Mechanics and Structure |
| 54 |
+ |
modules. Input/Output module not only implements general methods for |
| 55 |
+ |
file handling, but also defines a generic force field interface. |
| 56 |
+ |
Another important component of Input/Output module is the meta-data |
| 57 |
+ |
file parser, which is rewritten using ANother Tool for Language |
| 58 |
+ |
Recognition(ANTLR)\cite{Parr1995, Schaps1999} syntax. The Molecular |
| 59 |
+ |
Mechanics module consists of energy minimization and a wide |
| 60 |
+ |
varieties of integration methods(see Chap.~\ref{chapt:methodology}). |
| 61 |
+ |
The structure module contains a flexible and powerful selection |
| 62 |
+ |
library which syntax is elaborated in |
| 63 |
+ |
Sec.~\ref{appendixSection:syntax}. The top layer is made of the main |
| 64 |
+ |
program of the package, \texttt{oopse} and it corresponding parallel |
| 65 |
+ |
version \texttt{oopse\_MPI}, as well as other useful utilities, such |
| 66 |
+ |
as \texttt{StatProps} (see Sec.~\ref{appendixSection:StaticProps}), |
| 67 |
+ |
\texttt{DynamicProps} (see |
| 68 |
+ |
Sec.~\ref{appendixSection:appendixSection:DynamicProps}), |
| 69 |
+ |
\texttt{Dump2XYZ} (see |
| 70 |
+ |
Sec.~\ref{appendixSection:appendixSection:Dump2XYZ}), \texttt{Hydro} |
| 71 |
+ |
(see Sec.~\ref{appendixSection:appendixSection:hydrodynamics}) |
| 72 |
+ |
\textit{etc}. |
| 73 |
+ |
|
| 74 |
|
\begin{figure} |
| 75 |
|
\centering |
| 76 |
|
\includegraphics[width=\linewidth]{architecture.eps} |
| 77 |
< |
\caption[The architecture of {\sc oopse}-3.0] {The architecture of |
| 78 |
< |
{\sc oopse}-3.0.} \label{appendixFig:architecture} |
| 77 |
> |
\caption[The architecture of {\sc OOPSE}] {Overview of the structure |
| 78 |
> |
of {\sc OOPSE}} \label{appendixFig:architecture} |
| 79 |
|
\end{figure} |
| 80 |
|
|
| 81 |
|
\section{\label{appendixSection:desginPattern}Design Pattern} |
| 112 |
|
|
| 113 |
|
As one of the latest advanced techniques emerged from |
| 114 |
|
object-oriented community, design patterns were applied in some of |
| 115 |
< |
the modern scientific software applications, such as JMol, OOPSE |
| 116 |
< |
\cite{Meineke05} and PROTOMOL \cite{Matthey05} \textit{etc}. |
| 115 |
> |
the modern scientific software applications, such as JMol, {\sc |
| 116 |
> |
OOPSE}\cite{Meineke05} and PROTOMOL\cite{Matthey05} \textit{etc}. |
| 117 |
> |
The following sections enumerates some of the patterns used in {\sc |
| 118 |
> |
OOPSE}. |
| 119 |
|
|
| 120 |
|
\subsection{\label{appendixSection:singleton}Singleton} |
| 121 |
|
The Singleton pattern ensures that only one instance of a class is |
| 130 |
|
subclasses can then override to specify the derived type of product |
| 131 |
|
that will be created. |
| 132 |
|
|
| 77 |
– |
|
| 133 |
|
\subsection{\label{appendixSection:visitorPattern}Visitor} |
| 134 |
|
The purpose of the Visitor Pattern is to encapsulate an operation |
| 135 |
|
that you want to perform on the elements of a data structure. In |
| 137 |
|
structure without the need of changing the classes of the elements |
| 138 |
|
that you are operating on. |
| 139 |
|
|
| 85 |
– |
|
| 86 |
– |
\subsection{\label{appendixSection:templateMethod}Template Method} |
| 87 |
– |
|
| 140 |
|
\section{\label{appendixSection:concepts}Concepts} |
| 141 |
|
|
| 142 |
|
OOPSE manipulates both traditional atoms as well as some objects |
| 162 |
|
DirectionalAtom}s which behaves as a single unit. |
| 163 |
|
\end{itemize} |
| 164 |
|
|
| 165 |
< |
Every Molecule, Atom and DirectionalAtom in {\sc oopse} have their |
| 165 |
> |
Every Molecule, Atom and DirectionalAtom in {\sc OOPSE} have their |
| 166 |
|
own names which are specified in the {\tt .md} file. In contrast, |
| 167 |
|
RigidBodies are denoted by their membership and index inside a |
| 168 |
|
particular molecule: [MoleculeName]\_RB\_[index] (the contents |
| 173 |
|
\section{\label{appendixSection:syntax}Syntax of the Select Command} |
| 174 |
|
|
| 175 |
|
The most general form of the select command is: {\tt select {\it |
| 176 |
< |
expression}} |
| 177 |
< |
|
| 178 |
< |
This expression represents an arbitrary set of StuntDoubles (Atoms |
| 179 |
< |
or RigidBodies) in {\sc oopse}. Expressions are composed of either |
| 180 |
< |
name expressions, index expressions, predefined sets, user-defined |
| 181 |
< |
expressions, comparison operators, within expressions, or logical |
| 182 |
< |
combinations of the above expression types. Expressions can be |
| 131 |
< |
combined using parentheses and the Boolean operators. |
| 176 |
> |
expression}}. This expression represents an arbitrary set of |
| 177 |
> |
StuntDoubles (Atoms or RigidBodies) in {\sc OOPSE}. Expressions are |
| 178 |
> |
composed of either name expressions, index expressions, predefined |
| 179 |
> |
sets, user-defined expressions, comparison operators, within |
| 180 |
> |
expressions, or logical combinations of the above expression types. |
| 181 |
> |
Expressions can be combined using parentheses and the Boolean |
| 182 |
> |
operators. |
| 183 |
|
|
| 184 |
|
\subsection{\label{appendixSection:logical}Logical expressions} |
| 185 |
|
|
| 262 |
|
Users can define arbitrary terms to represent groups of |
| 263 |
|
StuntDoubles, and then use the define terms in select commands. The |
| 264 |
|
general form for the define command is: {\bf define {\it term |
| 265 |
< |
expression}} |
| 265 |
> |
expression}}. Once defined, the user can specify such terms in |
| 266 |
> |
boolean expressions |
| 267 |
|
|
| 216 |
– |
Once defined, the user can specify such terms in boolean expressions |
| 217 |
– |
|
| 268 |
|
{\tt define SSDWATER SSD or SSD1 or SSDRF} |
| 269 |
|
|
| 270 |
|
{\tt select SSDWATER} |
| 309 |
|
some or all of the configurations that are contained within a dump |
| 310 |
|
file. The most common example of a static property that can be |
| 311 |
|
computed is the pair distribution function between atoms of type $A$ |
| 312 |
< |
and other atoms of type $B$, $g_{AB}(r)$. StaticProps can also be |
| 313 |
< |
used to compute the density distributions of other molecules in a |
| 314 |
< |
reference frame {\it fixed to the body-fixed reference frame} of a |
| 315 |
< |
selected atom or rigid body. |
| 312 |
> |
and other atoms of type $B$, $g_{AB}(r)$. {\tt StaticProps} can |
| 313 |
> |
also be used to compute the density distributions of other molecules |
| 314 |
> |
in a reference frame {\it fixed to the body-fixed reference frame} |
| 315 |
> |
of a selected atom or rigid body. |
| 316 |
|
|
| 317 |
|
There are five seperate radial distribution functions availiable in |
| 318 |
|
OOPSE. Since every radial distrbution function invlove the |
| 366 |
|
Any two directional objects (DirectionalAtoms and RigidBodies) have |
| 367 |
|
a set of two angles ($\theta$, and $\omega$) between the z-axes of |
| 368 |
|
their body-fixed frames.} \label{oopseFig:gofr} |
| 369 |
+ |
\end{figure} |
| 370 |
+ |
|
| 371 |
+ |
Due to the fact that the selected StuntDoubles from two selections |
| 372 |
+ |
may be overlapped, {\tt StaticProps} performs the calculation in |
| 373 |
+ |
three stages which are illustrated in |
| 374 |
+ |
Fig.~\ref{oopseFig:staticPropsProcess}. |
| 375 |
+ |
|
| 376 |
+ |
\begin{figure} |
| 377 |
+ |
\centering |
| 378 |
+ |
\includegraphics[width=\linewidth]{staticPropsProcess.eps} |
| 379 |
+ |
\caption[A representation of the three-stage correlations in |
| 380 |
+ |
\texttt{StaticProps}]{This diagram illustrates three-stage |
| 381 |
+ |
processing used by \texttt{StaticProps}. $S_1$ and $S_2$ are the |
| 382 |
+ |
numbers of selected stuntdobules from {\tt -{}-sele1} and {\tt |
| 383 |
+ |
-{}-sele2} respectively, while $C$ is the number of stuntdobules |
| 384 |
+ |
appearing at both sets. The first stage($S_1-C$ and $S_2$) and |
| 385 |
+ |
second stages ($S_1$ and $S_2-C$) are completely non-overlapping. On |
| 386 |
+ |
the contrary, the third stage($C$ and $C$) are completely |
| 387 |
+ |
overlapping} \label{oopseFig:staticPropsProcess} |
| 388 |
|
\end{figure} |
| 389 |
|
|
| 390 |
|
The options available for {\tt StaticProps} are as follows: |
| 448 |
|
different vectors). The ability to use two selection scripts to |
| 449 |
|
select different types of atoms is already present in the code. |
| 450 |
|
|
| 451 |
+ |
For large simulations, the trajectory files can sometimes reach |
| 452 |
+ |
sizes in excess of several gigabytes. In order to effectively |
| 453 |
+ |
analyze that amount of data. In order to prevent a situation where |
| 454 |
+ |
the program runs out of memory due to large trajectories, |
| 455 |
+ |
\texttt{dynamicProps} will estimate the size of free memory at |
| 456 |
+ |
first, and determine the number of frames in each block, which |
| 457 |
+ |
allows the operating system to load two blocks of data |
| 458 |
+ |
simultaneously without swapping. Upon reading two blocks of the |
| 459 |
+ |
trajectory, \texttt{dynamicProps} will calculate the time |
| 460 |
+ |
correlation within the first block and the cross correlations |
| 461 |
+ |
between the two blocks. This second block is then freed and then |
| 462 |
+ |
incremented and the process repeated until the end of the |
| 463 |
+ |
trajectory. Once the end is reached, the first block is freed then |
| 464 |
+ |
incremented, until all frame pairs have been correlated in time. |
| 465 |
+ |
This process is illustrated in |
| 466 |
+ |
Fig.~\ref{oopseFig:dynamicPropsProcess}. |
| 467 |
+ |
|
| 468 |
+ |
\begin{figure} |
| 469 |
+ |
\centering |
| 470 |
+ |
\includegraphics[width=\linewidth]{dynamicPropsProcess.eps} |
| 471 |
+ |
\caption[A representation of the block correlations in |
| 472 |
+ |
\texttt{dynamicProps}]{This diagram illustrates block correlations |
| 473 |
+ |
processing in \texttt{dynamicProps}. The shaded region represents |
| 474 |
+ |
the self correlation of the block, and the open blocks are read one |
| 475 |
+ |
at a time and the cross correlations between blocks are calculated.} |
| 476 |
+ |
\label{oopseFig:dynamicPropsProcess} |
| 477 |
+ |
\end{figure} |
| 478 |
+ |
|
| 479 |
|
The options available for DynamicProps are as follows: |
| 480 |
|
\begin{longtable}[c]{|EFG|} |
| 481 |
|
\caption{DynamicProps Command-line Options} |
| 503 |
|
\subsection{\label{appendixSection:Dump2XYZ}Dump2XYZ} |
| 504 |
|
|
| 505 |
|
Dump2XYZ can transform an OOPSE dump file into a xyz file which can |
| 506 |
< |
be opened by other molecular dynamics viewers such as Jmol and VMD. |
| 507 |
< |
The options available for Dump2XYZ are as follows: |
| 506 |
> |
be opened by other molecular dynamics viewers such as Jmol and |
| 507 |
> |
VMD\cite{Humphrey1996}. The options available for Dump2XYZ are as |
| 508 |
> |
follows: |
| 509 |
|
|
| 510 |
|
|
| 511 |
|
\begin{longtable}[c]{|EFG|} |
| 535 |
|
& {\tt -{}-refsele} & In order to rotate the system, {\tt -{}-originsele} and {\tt -{}-refsele} must be given to define the new coordinate set. A StuntDouble which contains a dipole (the direction of the dipole is always (0, 0, 1) in body frame) is specified by {\tt -{}-originsele}. The new x-z plane is defined by the direction of the dipole and the StuntDouble is specified by {\tt -{}-refsele}. |
| 536 |
|
\end{longtable} |
| 537 |
|
|
| 538 |
< |
\subsection{\label{appendixSection:hydrodynamics}Hydrodynamics} |
| 539 |
< |
|
| 538 |
> |
\subsection{\label{appendixSection:hydrodynamics}Hydro} |
| 539 |
> |
The options available for Hydro are as follows: |
| 540 |
|
\begin{longtable}[c]{|EFG|} |
| 541 |
|
\caption{Hydrodynamics Command-line Options} |
| 542 |
|
\\ \hline |
| 549 |
|
-i & {\tt -{}-input} & input dump file \\ |
| 550 |
|
-o & {\tt -{}-output} & output file prefix (default=`hydro') \\ |
| 551 |
|
-b & {\tt -{}-beads} & generate the beads only, hydrodynamics calculation will not be performed (default=off)\\ |
| 552 |
< |
& {\tt -{}-model} & hydrodynamics model (support ``AnalyticalModel'', ``RoughShell'' and ``BeadModel'') \\ |
| 552 |
> |
& {\tt -{}-model} & hydrodynamics model (supports ``AnalyticalModel'', ``RoughShell'' and ``BeadModel'') \\ |
| 553 |
|
\end{longtable} |