Classical Approach to Constrained and Unconstrained Molecular Dynamics
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Classical Approach to Constrained and Unconstrained Molecular Dynamics - Ajith Gunaratne
CLASSICAL
APPROACH
to
CONSTRAINED AND UNCONSTRAINED
MOLECULAR DYNAMICS
781080FCsc.tifAJITH GUNARATNE
Copyright © 2018 by Ajith Gunaratne. 781080
Library of Congress Control Number: Pending
All rights reserved. No part of this book may be reproduced or transmitted in any form or by any means, electronic or mechanical, including photocopying, recording, or by any information storage and retrieval system, without permission in writing from the copyright owner.
The views expressed in this work are solely those of the author and do not necessarily reflect the views of the publisher, and the publisher hereby disclaims any responsibility for them.
Rev. date: 07/20/2018
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CONTENTS
LIST OF TABLES
LIST OF FIGURES
ABSTRACT
CHAPTER 1.
INTRODUCTION AND BACKGROUND
1.1 Introduction
1.2 Background
1.2.1 Protein
1.3 Empirical force field
1.3.1 Introduction
1.3.2 Bond stretching potential - φb
1.3.3 Angle bending potential - φθ
1.3.4 Torsion potential - φτ
1.3.5 Potential of non-bonding interactions - φnb
1.4 Molecular dynamic simulations
1.4.1 Introduction
1.4.2 History
1.4.3 Limitations
1.5 Unconstrained molecular dynamic simulations
1.5.1 Verlet algorithm
1.5.2 Leap-Frog algorithm
1.5.3 Predictor-Corrector algorithm
1.5.4 Velocity version of Verlet algorithm
1.5.5 Beemans algorithm
1.5.6 Symplectic integrators
1.6 Constrained molecular dynamic simulations
1.6.1 Shake algorithm
1.6.2 Rattle algorithm
1.6.3 Stochastic method
1.6.4 Velocity rescaling
1.7 Review
CHAPTER 2.
LAGRANGE MULTIPLIER METHOD
2.0.1 Lagrange multiplier method
2.0.2 Time dependent Lagrange multiplier method for molecular dynamics
2.1 Review
CHAPTER 3.
PENALTY AND BARRIER METHODS
3.0.1 History
3.0.2 Constraints
3.0.3 Penalty function method
3.0.4 Karush-Kuhn-Tucker multipliers
3.0.5 Exact penalty function
3.0.6 Barrier method
3.1 Review
CHAPTER 4.
MOLECULAR DYNAMICS, PENALTY FUNCTION METHOD AND ITS PROPERTIES
4.0.1 Constrained molecular dynamics and penalty function method
4.1 Analysis of molecular dynamics
4.1.1 Root Mean Square Deviation (RMSD)
4.1.2 Velocity Autocorrelation Function (VAF)
4.1.3 Ramachandran Plots
4.2 Review
CHAPTER 5.
IMPLEMENTATION PROCEDURE
5.1 Introduction
5.1.1 Penalty function implementation on Argon clusters
5.2 CHARMM settings
5.2.1 CHARMM minimization energy process
5.2.2 Minimization methods
5.2.3 CHARMM force field
5.2.4 Convergence criteria
5.3 Penalty method implementation
5.4 Review
CHAPTER 6.
RESULTS, SUMMARY AND DISCUSSION
6.0.1 Analysis of dynamics
6.1 Review
CHAPTER 7.
EVALUATION/CONCLUSION
APPENDIX A.
FORTRAN PROGRAM FOR PENALTY FUNCTION METHOD FOR ARGON CLUSTERS
A.0.1 Main program
A.0.2 Sub program Verlet
A.0.3 Sub program Init velocity
A.0.4 Sub program read files
A.0.5 Sub program distance
APPENDIX B.
HIGH PERFORMANCE FORTRAN PROGRAM FOR PENALTY FUNCTION METHOD FOR ARGON CLUSTERS
B.0.1 Sub program - Verlet
B.0.2 Sub program - Position Init
B.0.3 Sub program - Init velocity
B.0.4 Sub program - bubble sort
BIBLIOGRAPHY
LIST OF TABLES
Table 5.1 Final steps of energy minimization
Table 5.2 Computing time of VL, SH and PL run. *Computing time for the 25ps simulation after equilibrium
Table 5.3 Root mean square deviation (RMSD) of backbone atoms
LIST OF FIGURES
Figures 1.1 The chemical formulas of 20 amino acids (47). Plot is created by Chemsketch software. (Advanced Chemistry Development Lab - www.acdlabs.com).
Figures 1.2 The space filling model of 20 amino acids. VMD visualization software is used. Color is based on ResID.
Figures 1.3 Three dimensional structure of Bovine Pancreatic Trypsin Inhibitor (BPTI) protein with 58 residuals. Data are downloaded from protein data bank (PDB) which released on 18-Jan-1983 (7). VMD visualization software is used. Color is based on ResID.
Figures 1.4 Bond stretching potential energy.
Figures 1.5 Angle bending potential energy.
Figures 1.6 Torsion potential energy.
Figures 1.7 Lennard Johnes potential of single pair of atoms.
Figures 5.1 The figure is illustrated potential energy changes when penalty term change.
Figures 5.2 The flow chart of the penalty function algorithm for Argon cluster simulation.
Figures 5.3 Changes in potential energy of the trajectory for argon cluster 13 produced by the penalty function method. Here, randomly selected 60% of all distances were constrained to their distances in the global energy minimum configuration. The trajectory already approached to the global energy minimum (-44.3) of the cluster in 3000 time steps while the trajectory generated by the Verlet remained in high energy. The time step is 0.032ps and penalty term updated every 500 iteration by 1.
Figures 5.4 Changes in potential energy of the trajectory for argon cluster 13 produced by the penalty function method. Randomly selected 60% of all distances were constrained to their distances in the global energy minimum configuration. The time step is 0.032ps and penalty term updated every 1000 iteration by 5.
Figures 5.5 Changes in potential energy of argon cluster 24. Solid and dotted lines show the potential energy of the trajectory produced by the Verlet (VL) and penalty function (PL) methods, respectively. Here, randomly selected 50% of all distances were constrained to their distances in the global energy minimum configuration (-97.349).
Figures 5.6 CHARMM simulation procedure.
Figures 5.7 Basic steps of molecular dynamic simulation procedure.
Figures 5.8 Initial BPTI structure downloaded from PDB data bank. Picture uses display style cartoon, coloring is based on RESID and use VMD software.
Figures 5.9 BPTI with four water molecules. Picture uses display style CPK. VMD software is used to create picture. Color is based on RESID.
Figures 5.10 The figure is showed sequence of BPTI (9).
Figures 5.11 This picture shows BPTI with all hydrogen atoms. There are 904 atoms in total. Picture uses display style CPK and coloring is based on RESID.
Figures 5.12 This picture shows minimized BPTI stricture with all hydrogen atoms. Display style is CPK and coloring is based on RESID. VMD is used.
Figures 5.13 Average of 25ps structure of equilibrium period of BPTI structure including all hydrogen atoms. CPK display style and color is based on RESID. The picture is created by using VMD software.
Figures 5.14 Simulation time for VL, SH and PL. *Heating - bring the system to normal temperature; §Equilibrium - the time for the system to reach the equilibrium; ¶Production - stable dynamic results for analysis.
Figures 6.1 Temperature distribution of Shake and Penalty run.
Figures 6.2 Temperature distribution of Verlet run.
Figures 6.3 The average backbone RMS fluctuations of the residues in the 25ps production simulations.
Figures 6.4 The average Cα RMS fluctuations in the 25ps production simulations.
Figures 6.5 The average RMS fluctuations of the HN atoms in the 25ps production simulations.
Figures 6.6 The average RMS fluctuations of the non-backbone atoms in the 25ps production simulations.
Figures 6.7 The velocity auto correlations of the Cα atom of 51 CY S based on the trajectories produced by VL, SH, and PL in a time period of 0.1ps.
DEDICATION
This work is dedicated to my loving wife Nilanthi Gunaratne, energetic, bright, boundless sons Chamara Gunaratne and Chanith Gunaratne, who has been a constant source of support and encouragement and trust, I would not have been able to complete this work. . I am truly thankful for having you in my life. This work is also dedicated to my parents, Mr and Mrs Gunaratne, who have always loved me unconditionally and whose good examples have taught me to work hard for the things that I aspire to achieve.