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  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Biochemistry 20 (1981), S. 4936-4941 
    ISSN: 1520-4995
    Source: ACS Legacy Archives
    Topics: Biology , Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Biochemistry 27 (1988), S. 3487-3497 
    ISSN: 1520-4995
    Source: ACS Legacy Archives
    Topics: Biology , Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Biochemistry 22 (1983), S. 2884-2893 
    ISSN: 1520-4995
    Source: ACS Legacy Archives
    Topics: Biology , Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Journal of the American Chemical Society 115 (1993), S. 7439-7444 
    ISSN: 1520-5126
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 8954-8962 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A new closure to the Ornstein–Zernike equation is proposed for ionic liquids such as electrolytes. The closure is investigated numerically for a model electrolyte consisting of charged soft spheres in a uniform dielectric medium. The new closure, which we call the ionic Percus–Yevick (IPY) closure, may be viewed as a prescription for the so-called "bridge function,'' which is approximated by zero in the well-known hypernetted-chain (HNC) closure. Compared to the results of Monte Carlo simulations, the pair correlation functions predicted from this new closure for 2:2 electrolytes at low concentrations are in much better agreement than those predicted by the HNC closure. In particular, whereas the HNC approximation predicts incorrectly a peak in the pair correlation functions for like charges at an interionic separation of about two diameters at low concentrations, the new IPY closure predicts correctly no such peak. At higher concentrations, both the HNC and IPY closures yield correlation functions which are close to those calculated from Monte Carlo simulations, with the new IPY closure being more accurate for unlike charges and the HNC closure being slightly more accurate for like charges.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 89 (1988), S. 4315-4324 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The atom–atom pair correlation functions and thermodynamics of the central force model of water, introduced by Lemberg, Stillinger, and Rahman, have been calculated accurately by an integral equation method which incorporates two new developments. First, a rapid new scheme has been used to solve the Ornstein–Zernike equation. This scheme combines the renormalization methods of Allnatt, and Rossky and Friedman with an extension of the trigonometric basis-set solution of Labik and co-workers. Second, by adding approximate "bridge'' functions to the hypernetted-chain (HNC) integral equation, we have obtained predictions for liquid water in which the hydrogen bond length and number are in good agreement with "exact'' computer simulations of the same model force laws. In addition, for dilute ionic solutions, the ion–oxygen and ion–hydrogen coordination numbers display both the physically correct stoichiometry and good agreement with earlier simulations. These results represent a measurable improvement over both a previous HNC solution of the central force model and the ex-RISM integral equation solutions for the TIPS and other rigid molecule models of water.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 100 (1994), S. 9147-9155 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A new closure to the Ornstein–Zernike (OZ) equation is proposed for ionic liquids and is investigated for primitive models of high valency (2:2) aqueous electrolyte solutions and molten salts. The new closure, which is related to an earlier closure for the soft-sphere case proposed by Ichiye and Haymet, may be viewed as a prescription for the so-called "bridge functions.'' These functions are approximated by zero in the hypernetted-chain (HNC) closure which is generally used for ionic systems. In both the new closure and the soft-sphere closure, the recognition that the unlike bridge function is opposite in sign from the like bridge function leads to an approximation for these missing graphs by adding (for the unlike case) or subtracting (for the like case) a set of graphs similar to those used in Percus–Yevick theory to the HNC equation. Compared to the HNC closure, the pair correlation functions predicted for primitive models by the new closure are generally in much better agreement with Monte Carlo (MC) simulations of molten salts and aqueous 2:2 electrolytes. The fundamental improvement of this paper over the Ichiye–Haymet work is that the separation of long- and short-range part of c(r) for the hard-sphere case is clearly defined, whereas it was done numerically for the soft-sphere case. Moreover, the present theory is in better agreement with MC simulations both in the molten salt as well as in the dilute solution regimes than the soft-sphere case. Finally, a study was made of the transition of the like charge pair correlation functions from monotonic behavior at low densities to a nonmonotonic behavior at high densities. The new closure clearly predicts such a transition region at concentrations near 0.02 M and temperatures near 314 K. There is also a region below 0.02 M and 314 K where the new closure fails to converge. Compared to MC simulations, the critical region predicted by the new closure appears to be a lower estimate. However, for the HNC closure there is only a remote possibility of such a transition region since the correlation functions are nonmonotonic even at lower concentrations, a feature which is corrected in the new theory.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 111 (1999), S. 2701-2709 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Dynamical properties of the soft sticky dipole (SSD) model of water are calculated by means of molecular dynamics simulations. Since this is not a simple point model, the forces and torques arising from the SSD potential are derived here. Simulations are carried out in the microcanonical ensemble employing the Ewald method for the electrostatic interactions. Various time correlation functions and dynamical quantities associated with the translational and rotational motion of water molecules are evaluated and compared with those of two other commonly used models of liquid water, namely the transferable intermolecular potential-three points (TIP3P) and simple point charge/extended (SPC/E) models, and also with experiments. The dynamical properties of the SSD water model are found to be in good agreement with the experimental results and appear to be better than the TIP3P and SPC/E models in most cases, as has been previously shown for its thermodynamic, structural, and dielectric properties. Also, molecular dynamics simulations of the SSD model are found to run much faster than TIP3P, SPC/E, and other multisite models. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 99 (1995), S. 5187-5195 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 104 (1996), S. 7561-7571 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Marcus theory for electron transfer assumes a linear response of the solvent so that both the reactant and product free energy curves are parabolic functions of the solvent polarization, each with the same solvent force constant k characterizing the curvature. Simulation data by other workers indicate that the assumption of parabolic free energy curves is good for the Fe2+–Fe3+ self-exchange reaction but that the k of the reactant and product free energy curves are different for the reaction D0+A0→D1−+A1+. However, the fluctuations sampled in these simulations were not large enough to reach the activation barrier region, which was thus treated either by umbrella sampling or by parabolic extrapolation. Here, we present free energy curves calculated from a simple model of ionic solvation developed in an earlier paper by Hyun, Babu, and Ichiye, which we refer to here as the HBI model. The HBI model describes the nonlinearity of the solvent response due to the orientation of polar solvent molecules. Since it is a continuum model, it may be considered the first-order nonlinear correction to the linear response Born model. Moreover, in the limit of zero charge or infinite radius, the Born model and the Marcus relations are recovered. Here, the full free energy curves are calculated using analytic expressions from the HBI model. The HBI reactant and product curves have different k for D0+A0→D1−+A1+ as in the simulations, but examining the full curves shows they are nonparabolic due to the nonlinear response of the solvent. On the other hand, the HBI curves are close to parabolic for the Fe2+–Fe3+ reaction, also in agreement with simulations, while those for another self-exchange reaction D0−A1+ show greater deviations from parabolic behavior than the Fe2+–Fe3+ reaction. This indicates that transitions from neutral to charged species will have the largest deviations. Thus, the second moment of the polarization is shown to be a measure of the deviation from Marcus theory. Finally, since the HBI expressions for the free energy curves are not simple, the HBI curves are compared with various approximate parabolic descriptions of the curves, including Marcus parabolas. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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