simulating peo melts using connectivity-altering monte carlo simulating peo melts using...
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Simulating PEO melts usingSimulating PEO melts usingconnectivity-altering Monte connectivity-altering Monte
CarloCarlo
by Collin D. Wick and Doros N. by Collin D. Wick and Doros N. TheodorouTheodorou
Acknowledgements:Acknowledgements:NSF-MPS distinguished international NSF-MPS distinguished international
postdoctoral fellowship.postdoctoral fellowship.Krell InstituteKrell Institute
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IntroductionIntroductionPoly(ethylene glycol) (X=H) and poly(ethylene oxide) dimethyl ether (X=CH3) have the same interior segments, but different endpoints.
The volumetric properties of the two systems as a function of chain length behave quite differently.
CH2
O CH2[ ]n
X XO
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Molecular Simulation Molecular Simulation TechniquesTechniques
Two predominate simulation techniques Two predominate simulation techniques are used.are used.
Molecular Dynamics: the system follows Molecular Dynamics: the system follows Newton’s equations of motion, following Newton’s equations of motion, following their real dynamical trajectory.their real dynamical trajectory.
Monte Carlo: the system randomly moves Monte Carlo: the system randomly moves from one state to another with no set from one state to another with no set trajectory. trajectory.
The technique we use is Monte Carlo.The technique we use is Monte Carlo.
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Designing a Monte Carlo Designing a Monte Carlo MoveMove
)]/)(/(,1min[. to state from
transferfor the prob. acceptance
. to state from
transfer for the prob. transition
state in be density to prob.
TTP
P
T
PTPT
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The Benefit of Monte CarloThe Benefit of Monte Carlo
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Metropolis AcceptanceMetropolis Acceptance
bath. pressure
outside withons FluctuatiVolume
]/)(exp[/
:moves rotation and nTranslatio
]/,1min[
BTkuuB
P
TT
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Configurational-bias Monte Configurational-bias Monte CarloCarlo
n
nstep
nn
nstep
n
nstep
nni
nchoi
jj
ii
n
nstep
ni
WWP
B
BW
TkuB
WBT
TT
)(/)(
)(
)/exp(
)/(
11
1
1
B
1
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Connectivity-Altering MC Connectivity-Altering MC (End-Bridging Move)(End-Bridging Move)
End-bridging (EB) End-bridging (EB) move from move from toto
Use SAFE-CBMC to Use SAFE-CBMC to regrow the regrow the segmentssegments
For PEG, regrow OH For PEG, regrow OH group from group from
Repeat for reverse Repeat for reverse movemove
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Double Bridging MoveDouble Bridging Move
Double-bridging (DB) move from to and from.Use SAFE-CBMC to regrow the segments.Repeat for reverse move.
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TraPPE-UA Force FieldTraPPE-UA Force Field
Transferable potentials for phase Transferable potentials for phase equilibria-united atom form.equilibria-united atom form.
Enforces transferability in the fitting of Enforces transferability in the fitting of new groups.new groups.
Utilizes pseudo-atoms for alkyl groups Utilizes pseudo-atoms for alkyl groups located at carbon centers, and treats located at carbon centers, and treats all non-alkyl atoms explicitly.all non-alkyl atoms explicitly.
Fixed bond lengthsFixed bond lengths
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Potential FormPotential Form
ij
ji
ij
ij
ij
ijijij r
rrru
c
cccu
ku
0
612
NB
33
2210torsion
20
0bend
44)(
nsinteractio bonded-nonfor termscouloumbic LJ
))(cos1(
))(cos1())cos(1()(
nsinteractio dihedralfor series Cosine
)(2
)(
potential bending bond Harmonic
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Parameterizing TraPPE-UAParameterizing TraPPE-UA
Bonded interactions are taken from existing force Bonded interactions are taken from existing force fields.fields.
Lennard-Jones and Coulombic interactions are fit Lennard-Jones and Coulombic interactions are fit to reproduce vapor-liquid coexistence curves.to reproduce vapor-liquid coexistence curves.
For PEODME, all nonbonded parameters were fit For PEODME, all nonbonded parameters were fit to small ether molecules. to small ether molecules.
For PEG, all nonbonded parameters were fit to For PEG, all nonbonded parameters were fit to small alkanol and glycol molecules.small alkanol and glycol molecules.
Oxygens have negative charges, and methyl, Oxygens have negative charges, and methyl, methylene, and hydrogens have positive charges.methylene, and hydrogens have positive charges.
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Simulation DetailsSimulation Details Polydisperse melts of PEG and PEODME Polydisperse melts of PEG and PEODME
were simulated with chain length were simulated with chain length evenly distributed over a selected evenly distributed over a selected range.range.
Simulation runs consisted of four runs Simulation runs consisted of four runs of 200,000 MC cycles (one MC cycle is of 200,000 MC cycles (one MC cycle is N N MC moves).MC moves).
Periodic boundary conditions were Periodic boundary conditions were used.used.
Pressure and temperature were set for Pressure and temperature were set for each simulation run.each simulation run.
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Number, molecular weight, and Number, molecular weight, and polydispersity of polymerspolydispersity of polymers
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Percentage and acceptance of Percentage and acceptance of select MC movesselect MC moves
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Center of Mass MovementCenter of Mass MovementTop: PEODME-Top: PEODME-
30003000
Bottom: PEG-Bottom: PEG-30003000
Solid line: both Solid line: both EB and DB EB and DB movesmoves
Dotted line: DB Dotted line: DB move onlymove only
Dashed line: EB Dashed line: EB move onlymove only
Dot-dashed line: Dot-dashed line: neither DB neither DB or EB moves or EB moves usedused
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End-Group MovementEnd-Group MovementTop: PEODME-Top: PEODME-
30003000
Bottom: PEG-Bottom: PEG-30003000
Solid line: both Solid line: both EB and DB EB and DB movesmoves
Dotted line: DB Dotted line: DB move onlymove only
Dashed line: EB Dashed line: EB move onlymove only
Dot-dashed line: Dot-dashed line: neither DB neither DB or EB moves or EB moves usedused
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Decay of End-to-End VectorDecay of End-to-End VectorTop: PEODME-Top: PEODME-
30003000
Bottom: PEG-Bottom: PEG-30003000
Solid line: both Solid line: both EB and DB EB and DB movesmoves
Dotted line: DB Dotted line: DB move onlymove only
Dashed line: EB Dashed line: EB move onlymove only
Dot-dashed line: Dot-dashed line: neither DB neither DB or EB moves or EB moves usedused
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Specific DensitiesSpecific Densities
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Static Structure Factor Static Structure Factor (T=383K)(T=383K)
sim, PEODME-3000: solid line exp, PEG-20000: dotted line
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Characteristic Ratio PlotCharacteristic Ratio PlotTop: PEODMETop: PEODME
Bottom: PEGBottom: PEG
Circles: points Circles: points using end-using end-to-end to-end distancedistance
Squares: points Squares: points using radii using radii of gyrationof gyration
Solid lines: fit Solid lines: fit to circlesto circles
Dotted lines: fit Dotted lines: fit to squaresto squares 5.5 Experiment C
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3-d Radial Distribution 3-d Radial Distribution FunctionFunction
3-d radial-angular distribution function: =angle for O-CH3—(any
other heavy atom) for PEODME (top) and CH2-O—
(any other heavy atom) for PEG (bottom).
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Integral of 3-d RDFIntegral of 3-d RDFDistance where the integral of the 3-d radial-angular distribution function is unity at fixed or the distance where another heavy atom is most likely present at fixed
Integrating out these curves give a total end-group excluded volume: 162 angstroms for PEODME and 127 angstroms for PEG.
solid line: solid line: PEGPEG
dotted dotted line: line: PEODMEPEODME
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ConclusionsConclusions
Endbridging and double-bridging do Endbridging and double-bridging do reasonably well in equilibrating the PEO reasonably well in equilibrating the PEO melts, but better for PEODME than for PEG.melts, but better for PEODME than for PEG.
The TraPPE-UA force field does an excellent The TraPPE-UA force field does an excellent job of reproducing densities, and a good job job of reproducing densities, and a good job of reproducing structural properties of PEO.of reproducing structural properties of PEO.
The Molecular weight dependence of the The Molecular weight dependence of the volumetric properties can be related to volumetric properties can be related to differences in excluded volume of endgroups.differences in excluded volume of endgroups.