@article {4441,
	title = {Theory of ion solvation dynamics in mixed dipolar solvents},
	journal = {Journal of Chemical Physics},
	volume = {109},
	number = {8},
	year = {1998},
	note = {ISI Document Delivery No.: 114ZNTimes Cited: 38Cited Reference Count: 32},
	month = {Aug},
	pages = {3222-3231},
	type = {Article},
	abstract = {Time dependent density functional theory in its "extended linear" or "surrogate" form is used to investigate the dynamics of selective ion solvation in binary dipolar solvents. It is shown that simple analytical approximations that trap the basic physics of the solvation process can be obtained. In particular, it is found that the relaxation of:the solvent number densities about a charged solute is governed by two distinct modes clearly associated with electrostriction and redistribution processes. This is consistent with the physical picture suggested by molecular dynamics (MD) simulations. The solvent polarization relaxation is also dominated by two modes associated with the-two rotational diffusion constants of the binary solvent. In addition to the analytical approximations, full numerical solutions of the extended linear theory are obtained and the dependence of the relaxation on solvent density and solute charge is discussed. Detailed comparisons of the theory with MD simulations for a closely related model indicate that the theory is qualitatively correct, but quantitatively poor generally predicting relaxation rates which are too fast. This is due mainly to the neglect of inertial or non-Markovian effects in the theoretical approach. (C) 1998 American Institute of Physics. [S0021-9606(98)50132-8]},
	keywords = {COLLECTIVE ORIENTATIONAL RELAXATION, DIELECTRIC-RELAXATION, ELECTROLYTE-SOLUTIONS, HARD-SPHERES, INVARIANT EXPANSION, LIQUIDS, MEAN, MIXTURES, MOLECULAR THEORY, ORNSTEIN-ZERNIKE EQUATION, SPHERICAL MODEL},
	isbn = {0021-9606},
	url = {<Go to ISI>://000075639200032},
	author = {Yoshimori, A. and Day, T. J. F. and Patey, G. N.}
}
@article {3924,
	title = {An investigation of the influence of solute size and insertion conditions on solvation thermodynamics},
	journal = {Journal of Chemical Physics},
	volume = {106},
	number = {19},
	year = {1997},
	note = {ISI Document Delivery No.: WZ032Times Cited: 32Cited Reference Count: 52},
	month = {May},
	pages = {8165-8195},
	type = {Article},
	abstract = {In this paper we examine the influence of solute size and insertion conditions on solvent structural changes and excess thermodynamic properties in the infinite dilution limit. A general integral equation approach which can be applied under arbitrary conditions is given and isothermal-isochoric and isothermal-isobaric insertions are discussed in detail. Scaling relationships valid in the large solute limit are determined for both structural and thermodynamic properties. This is done by considering macroscopic thermodynamic relationships and explicit evaluation of low solvent density expansions of pair correlation functions. The hypernetted-chain and reference hypernetted-chain closure approximations are used to obtain numerical results for the insertion of hard sphere solutes of varying diameter into hard sphere, dipolar hard sphere and water-like solvents. The results obtained give a good deal of insight into the nature of solvation of inert solutes. It is shown that for all three solvents the excess properties are very well represented by a function obtained by summing terms proportional to the solute volume, surface area and diameter. One would expect such a result for large solutes, but here we show that this expression extrapolates all the way down to solutes comparable in size to the solvent particles. Further, it is shown that both the numerical value, and, more importantly, the physical interpretation of the excess thermodynamic properties strongly depend on the insertion conditions. Under all insertion conditions the chemical potential is a local property in the sense that it is completely determined by solute-solvent correlations which are important only in the immediate vicinity of the solute. However, this is not true of the excess energy, enthalpy and entropy which all contain nonlocal contributions arising essentially from changes in the actual or effective solvent density depending on the insertion conditions. We demonstrate that the nonlocal contributions can be very significant and therefore the excess energies, enthalpies and entropies often cannot provide useful information about solvent structure near solutes. This has significant implications for models which attempt to rationalize excess thermodynamics in terms of local solvent structure in the vicinity of solute particles. (C) 1997 American Institute of Physics.},
	keywords = {COMPUTER-SIMULATION, ELECTROLYTE-SOLUTIONS, FREE-ENERGIES, HARD-SPHERES, HYDROPHOBIC HYDRATION, HYPERNETTED-CHAIN APPROXIMATION, INVARIANT EXPANSION, MEAN, ORNSTEIN-ZERNIKE EQUATION, SPHERICAL MODEL, TEMPERATURE-DEPENDENCE},
	isbn = {0021-9606},
	url = {<Go to ISI>://A1997WZ03200027},
	author = {Cann, N. M. and Patey, G. N.}
}
@article {7179,
	title = {A MEAN FIELD-THEORY FOR FLUIDS OF MULTIPOLAR PARTICLES IN CONTACT WITH A POLARIZABLE WALL},
	journal = {Journal of Chemical Physics},
	volume = {97},
	number = {6},
	year = {1992},
	note = {ISI Document Delivery No.: JN146Times Cited: 15Cited Reference Count: 27},
	month = {Sep},
	pages = {4372-4379},
	type = {Article},
	abstract = {Fluids of multipolar particles in contact with a semi-infinite polarizable hard wall are considered. A mean field theory which reduces the many-body electrostatic wall-solvent interactions to an effective pair potential is described. The effective potential can be employed in conjunction with the reference hypernetted-chain approximation, or some other integral equation theory, to obtain a self-consistent solution for the wall-solvent correlation function and hence the solvent structure at the interface. Explicit results are given for dipolar hard sphere fluids in contact with walls having dielectric constants ranging from 1 to infinity. For this system, it is shown that contributions to the wall-solvent potential from images of other particles are very important and act strongly against the direct "self-image" interaction.},
	keywords = {ASYMPTOTIC-BEHAVIOR, CHARGED SURFACES, DIPOLAR HARD-SPHERES, INVARIANT EXPANSION, LIQUID WATER, MOLECULAR-DYNAMICS, NONSPHERICAL PARTICLES, ORNSTEIN-ZERNIKE EQUATION, SPHERICAL MODEL, WATER-LIKE PARTICLES},
	isbn = {0021-9606},
	url = {<Go to ISI>://A1992JN14600051},
	author = {Berard, D. R. and Patey, G. N.}
}
@article {6968,
	title = {THE APPLICATION OF INTEGRAL-EQUATION THEORIES TO FLUIDS OF NONSPHERICAL PARTICLES NEAR A UNIFORM PLANAR WALL},
	journal = {Journal of Chemical Physics},
	volume = {95},
	number = {7},
	year = {1991},
	note = {ISI Document Delivery No.: GH356Times Cited: 37Cited Reference Count: 39},
	month = {Oct},
	pages = {5281-5288},
	type = {Article},
	abstract = {A general reduction of the Ornstein-Zernike equation is given for molecular fluids near a planar wall. This allows integral equation approximations such as the hypernetted-chain or reference hypernetted-chain (RHNC) theories to be solved numerically for such systems. Dipolar hard sphere fluids near a hard wall are considered in detail and RHNC solutions are obtained. The results are compared with previous calculations for curved surfaces. The RHNC result for the asymptotic behavior of the wall-solvent pair correlation function at large separations is derived and compared with expressions given by classical continuum theory and by exact analysis.},
	keywords = {AQUEOUS-ELECTROLYTE SOLUTIONS, DIPOLAR HARD-SPHERES, ELECTRICAL DOUBLE-LAYER, HYPERNETTED-CHAIN, INFINITE DILUTION, INVARIANT EXPANSION, MEAN, MOLECULAR-SOLVENT MODEL, ORIENTATIONAL, ORNSTEIN-ZERNIKE EQUATION, SPHERICAL MODEL, STRUCTURE},
	isbn = {0021-9606},
	url = {<Go to ISI>://A1991GH35600061},
	author = {Berard, D. R. and Patey, G. N.}
}
