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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 112 (2000), S. 4351-4356 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We report Monte Carlo simulations of dipolar hard-sphere fluids with a nonuniform distribution of the dipole strengths or different hard-sphere diameters. Dipolar polydispersity significantly reduces the spontaneous orientational order observed in the ferroelectric phase of monodisperse dipolar hard-sphere fluids at high densities and low temperatures. Equimolar binary mixtures of dipolar hard spheres of different diameters σa and σb also exhibit ferroelectric order. However, the order parameters are very dependent on the ratio σa/σb. Chains of dipolar hard spheres, typical of strongly interacting dipolar hard spheres at low densities and low temperatures, were observed in binary fluids of dipolar and neutral hard spheres of different sizes. © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 86 (1987), S. 1467-1473 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: An intermolecular potential function for the methyl chloride dimer which includes the electrostatic induction terms explicitly has been used in an NPT Monte Carlo statistical mechanics simulation of liquid methyl chloride at its normal boiling temperature (−23.76 °C). The nonadditive many-body induction energy is computed via an iterative procedure. It is found that the thermodynamic and structural results which are obtained with the present potential functions compare favorably with those of a previous simulation performed with effective potential functions. Modest structural changes are observed when the two simulations are compared. They mainly concern the organization around the methyl group. A detailed analysis of the electrostatic field in the liquid for both simulations shows that the mean electrostatic field is larger in the simulation with effective potential functions than with explicit induction functions. Furthermore, the induction potential functions give a more homogeneous electrostatic field within the liquid.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 111 (1999), S. 5067-5072 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We present structural and dynamics results based on Hellman–Feynman molecular dynamics for the liquid phase of the NaCs alloy at two Na concentrations (cNa=0.6 and 0.8) and for the Li0.61Na0.39 zero alloy at two temperatures (T=590 K and 690 K). For NaCs the calculated structure factor S(k) is in very good agreement with data from neutron scattering experiments and the partial structure factors are compared to semiexperimental, theoretical and classical molecular dynamics predictions. We predict similar values for the self-diffusion coefficients of Na and Cs atoms in the Na0.6Cs0.4 alloy. For LiNa the concentration–concentration structure factor is in good agreement with experimental data and our results for the dynamics are compared with data from classical molecular dynamics simulations. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 83 (1985), S. 3083-3094 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A Monte Carlo simulation of a solution of 1,2-dichloroethane in methyl chloride has been performed in the NPT ensemble. The solution serves as a model to study the differential solvation of the gauche and anti conformers of a polar solute in a polar solvent. The expected conformational change induced by the solvation in favor of the gauche conformer is well reproduced in the simulation. To explain it, the r−12, r−6, and r−1 contributions of the intermolecular potential functions (TIPS format) to the solute–solvent and solvent–solvent energies have been recorded during the simulation. The mean r−1 contributions are computed to be less than one-third of the sum of the r−12 and r−6 contributions; however, the computed difference of 2±0.5 kcal/mol between the gauche and anti solute–solvent mean energy is totally accounted for by the difference in the r−1 contributions. The analysis of the r−1 energy pair distribution shows that the main part of this difference comes from changes in the interaction of the solute with the nearest solvent neighbors. The gauche conformer shows at one and the same time more attractive and more repulsive interactions than the anti conformer. When the pure liquid, the anti and gauche solutions are compared, it is found that the solvent molecules experience, on the mean, nearly the same solvent–solvent interactions in the three cases.
    Type of Medium: Electronic Resource
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