Investigating Popular Water Models Albert DeFusco, Ken Jordan Center for Molecular and Materials Simulations.

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Presentation transcript:

Investigating Popular Water Models Albert DeFusco, Ken Jordan Center for Molecular and Materials Simulations

What are we modeling?

Electrostatics Interaction of charge densities Polarization Distortions of charge density of one monomer due to the electric field from other monomers Exchange / Repulsion Short range interactions Dispersion Long range interactions Making Simple Models

Overview Elec.Pol.Rep.Disp. DC Charges Single dipole Oxygen: Lennard-Jones TTM2-R Charges (damped) Distributed dipoles Oxygen: R 12,R 10,R 6 AMOEBA Multipoles Distributed dipoles All atom Buffered 14-7 DPP Charges Distributed Dipoles All atom exponential Oxygen: damped R 6

Difference Plots Point Charges compared to MP2/aug-cc- pVTZ ๏ E(DPP)-E(MP2)

Difference Plots Point Charges compared to MP2/aug-cc- pVTZ ๏ E(DPP)-E(MP2) large region of difference ๏ Two out-of-plane regions where “lone pair electrons” may reside

Difference Plots Multipoles charge, dipole, quadrupole from MP2/aug-cc-pVTZ calculation compared to MP2/aug-cc-pVTZ ๏ E(GDMA)-E(MP2)

Difference Plots Multipoles Very close to MP2 Can be expensive to implement

Polarization by induced dipoles Induced dipole is the most popular method Single site ๏ tends to underpolarize Distributed polarizability ๏ must be damped at short range Can be compared to 3-body energies

Polarization Energy Single site: underpolarized distributed: over damped

3-body Decomposition water hexamer isomers

DPP has only point-charges!

Repulsion/Dispersion Typically just oxygens are allowed to interact ๏ Dang-Chang and TTM2-R Using all atoms allows for greater geometric flexibility ๏ AMOEBA and DPP

Relaxed flap angles Interaction energy θdθd θaθa

Relaxed versus fixed

Distributed Point Polarizable Model Point charges ๏ undamped interaction allows for charge-penetration- like effects Distributed induced dipoles ๏ improves 3-body interactions Repulsion / Dispersion ๏ all-atom repulsion ๏ damped R 6 dispersion

Acknowledgments The Jordan Group Dr. Thomas Sommerfeld Dr. Daniel Schofield Jun Cui Valerie McCarthy

Distributed Multipoles Based on Stone’s Generalized Distributed Multipole Analysis (GDMA) ๏ Point-moment expansion from ab initio density AMOEBA ๏ Up to quadrupole on each atom ๏ scaled to fix dimer geometry q,µ,Θ q,µ,Θ q,µ,Θ

Point Charges Reproduce experimental dipole ๏ 1.85 Debye Negative charge on the M-site ๏ 0.2 Å towards the hydrogens q+q+ µ 2q–