molecular dynamics simulations of diffusion in polymers
DESCRIPTION
Molecular Dynamics Simulations of Diffusion in Polymers. Zach Eldridge Department of Mechanical Engineering University of Arkansas Fayetteville, AR 72701 USA REU Advisor: Dr. Douglas Spearot Grad Student Advisor: Mr. Alex Sudibjo Research Symposium – July 20, 2009. Background. - PowerPoint PPT PresentationTRANSCRIPT
Molecular Dynamics Simulations of Diffusion in Polymers
Zach Eldridge
Department of Mechanical EngineeringUniversity of Arkansas
Fayetteville, AR 72701 USA
REU Advisor: Dr. Douglas SpearotGrad Student Advisor: Mr. Alex Sudibjo
Research Symposium – July 20, 2009
Multiscale Mechanics of Materials Laboratory, Department of Mechanical Engineering
Background
• What is Molecular Dynamics?• Molecular dynamics is a form of computer simulation used to
observe the behavior of atoms and molecules, which cannot be easily observed during experiments.
• Through the use of computer algorithms and known laws of physics, mathematics, and chemistry we are able conduct an experiment and model it through a simulation.
• Through analysis of the simulation we are able to study the behavior of the material.
Nano Indention
Multiscale Mechanics of Materials Laboratory, Department of Mechanical Engineering
My Project
• Objectives• The main objective of this research is to study diffusion of methane
gas penetrates through PDMS (Polydimethylsiloxane)• PDMS – the most widely used silicon based organic polymer. It is composed of Oxygen,
Siliocon and a methyl, CH3. Common uses include contact lenses and shampoo.
• Penetrate – Methane, CH4
PDMS 1 PDMS 2
• Molecular dynamics simulation will allow us to calculate the diffusion coefficients of the penetrate through the PDMS and evaluate the role of concentration and distribution of penetrates
Multiscale Mechanics of Materials Laboratory, Department of Mechanical Engineering
My Project
• Simulations Conditions• Concentrations – percent of the total weight of the system
• .264% = 15 atoms, .529% = 30 atoms, .793% = 45 atoms, 1.06% = 60 atoms
• Volumes – Initial volume of methane molecules
• 1000 Å3, 8000 Å3, 27000 Å3, 64000 Å3, 125000 Å3
• Temperatures – Temperature the simulation runs at
• 200 K, 250 K, 300 K, 350 K, 400 K
1000 Å3 initial volume 125000 Å3 initial volume
Multiscale Mechanics of Materials Laboratory, Department of Mechanical Engineering
Research Methods
• Create simulation in Linux using Lammps code
• Run simulation through a super computer, Trillion
• Output visual data to Ensight
• Output mean squared displacement data to Excel
• Normalize data and create graphs
• Use slope of trendline to calculate the diffusion coefficient D
• Solve for Q, activation energy Kcal/mol, using the value of D
• Average all Q and calculate D0, diffusion constant (cm2/s)
• Equations
• D = (1/6)slope
• Q = (Rln(D1 / D2))/( 1/T2 – 1/T1)
• D0 = D1/exp(-Q/RT1)
Multiscale Mechanics of Materials Laboratory, Department of Mechanical Engineering
Results
-20
0
20
40
60
80
100
120
140
10 20 30 40 50 60
Tota
l MSD
(Å
2 )
Time (ps)
Conc. = 1.06% Vol = 125000 Å3
200k
250k
300k
350k
400k
•Equilibrium Reached at 10 ps•Low fluctuation in MSD
-10
0
10
20
30
40
50
60
25 30 35 40 45 50 55
Tota
l MSD
(Å
2 )
Time (ps)
Conc. = .793% Vol = 125000 Å3
200k
250k
300k
350k
400k
•Equilibrium reached at 25 ps•Low fluctuation in MSD
Multiscale Mechanics of Materials Laboratory, Department of Mechanical Engineering
Results Cont.
•Equilibrium reached at 30 ps•High fluctuation in MSD
-10
0
10
20
30
40
50
60
30 35 40 45 50 55
Tota
l MSD
(Å2 )
Time (ps)
Conc. = 1.06 Vol = 1000 Å3
200k
250k
300k
350k
400k
Multiscale Mechanics of Materials Laboratory, Department of Mechanical Engineering
Results Cont.
Concentration Volume (Å3)
Temperature (K)
Average Q (Kcal/mol)
D0 x 10-3
(cm2/s)
1.06% 1000
125000
200250300350400
200250300350400
2.789
2.642
2.4 1.23 1.61 1.351.50
3.431.251.311.291.25
.793% 125000 200250300350400
2.704 4.51.01.1
5.971.0
Multiscale Mechanics of Materials Laboratory, Department of Mechanical Engineering
Conclusion
• Smaller the initial volume – longer it takes to reach equilibrium
• Larger concentration – less fluctuation in MSD values
• Smaller the initial concentration – longer it takes reach equilibrium
• D0 is concentration dependent• The values of D0 for concentration of .793% were between 19% -
37% below the values for 1.06%.
Multiscale Mechanics of Materials Laboratory, Department of Mechanical Engineering
Works cited
• (2009, May 11). Polydimethylsiloxane. Retrieved May 26, 2009, from Wikipedia Web site: http://en.wikipedia.org/wiki/Polydimethylsiloxane
• (2009, April 14). Arkansas High Performance Computing Center. Retrieved May 26, 2009, Web site: http://hpc.uark.edu/about.html
• Kam Liu, Wing Ensight.com. Retrieved May 26, 2009, Web site: http://www.ensight.com/component/option,com_zoom/Itemid,41/PageNo,2/catid,4/hit,1/key,15/page,view/
• Wag.caltech.edu. Retrieved May 26, 2009, from Gallery of Polymers and Polymer Simulation Web site: http://www.wag.caltech.edu/gallery/pvcdco2.gif
• Dr. Douglas Spearot – Faculty Advisor, Alex Sudibjo – Graduate Student Advisor
Multiscale Mechanics of Materials Laboratory, Department of Mechanical Engineering
Conclusion
Questions?