Publication | Closed Access
Effect of Electrostatic Force Truncation on Interfacial and Transport Properties of Water
382
Citations
40
References
1996
Year
Spherical TruncationElectrohydrodynamicsEngineeringFluid MechanicsWettingComputational ChemistryChemistryMolecular DynamicsFluid PropertiesTransport PropertiesCapillarity PhenomenonTransport PhenomenaMolecular SimulationBiophysicsElectrostatic Force TruncationEwald SummationTruncation MethodsInterfacial ProcessInterfacial PhenomenonConfined Water HydrodynamicsCivil EngineeringApplied PhysicsInterfacial PhenomenaInterfacial Study
The study compares Ewald summation with spherical truncation to demonstrate the critical need for fully accounting for Coulombic forces in molecular dynamics simulations of interfacial water. Ewald summation was implemented on a distributed memory parallel computer, with detailed computational procedures provided for large‑system simulations. Truncation at 12 Å increases interfacial structure, raising surface tension by 50 % and surface potential by 100 %, alters orientational polarization decay, and causes bulk viscosity and diffusion to differ by up to 100 %, with Ewald‑derived diffusion further from experiment, indicating a need to reparametrize the TIP3P model for Ewald use.
The importance of accurately accounting for all Coulombic forces in molecular dynamics simulations of water at interfaces is demonstrated by comparing the Ewald summation technique with various spherical truncation methods. The increased structure induced by truncation methods at 12 Å leads to water/vapor surface tensions and surface potentials that are respectively 50% and 100% greater than obtained with Ewald. The orientational polarization of water at the lipid/water interface is analyzed within the Marcelja−Radic theory of the hydration force, yielding decay parameters of 2.6 and 1.8 Å for spherical truncation and Ewald, respectively, as compared with 1.7−2.1 Å obtained from experiment. Bulk water transport properties such as the viscosity and diffusion constants differ by as much as 100% between simulations carried out with and without truncation; this may be related to ordering in the neighborhood of the cutoff radius. The diffusion constant calculated from the Ewald simulation is significantly further from experiment than the cutoff result, pointing out the need to reparametrize the TIP3P water model for use with Ewald summation. Appendices describe a method for carrying out the Ewald summation on a distributed memory parallel computer and other computational details relevant when simulating large systems.
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