Issue 53, 2014

A non-Bornian analysis of the Gibbs energy of hydration for organic ions

Abstract

Recently, a non-Bornian model was successfully applied to evaluate the Gibbs energy of hydration (ΔG°hyd) for spherical ions (mainly inorganic ions). In this model, the long-range, Born-type electrostatic ion–solvent interaction is not explicitly included in the calculation of ΔG°hyd, since its contribution is small, whereas the short-range interaction, including Coulomb, polarization, and charge-transfer interactions, is considered as the dominant factor that determines the ΔG°hyd of ions. The ΔG°hyd scaled by the surface area of an ion can be given by a quadratic function of the surface field strength (E) of the ion. In this study, the non-Bornian model was further applied to organic ions with charged groups. Using the Gaussian 09 program package, the geometries of ions in vacuum were optimized at the B3LYP/6-311++G(2d,p) level, and the partial atomic charges were computed in the Mulliken, Merz-Kollman (MK), natural population analysis (NPA), Hirshfeld, and ChelpG methods. Introducing a new subprogram, we could estimate local electric fields on the ion surface (van der Waals surface or solvent-accessible surface (SAS)). This enabled us to perform regression analyses based on the non-Bornian model, by using the experimental values of ΔG°hyd for 109 ions. When the NPA-SAS combination was chosen, the best regression result was obtained, giving the mean absolute error of 4.3 kcal mol−1. The non-Bornian model would provide a simple and relatively accurate way of determining ΔG°hyd of ions.

Graphical abstract: A non-Bornian analysis of the Gibbs energy of hydration for organic ions

Supplementary files

Article information

Article type
Paper
Submitted
19 Mar 2014
Accepted
10 Jun 2014
First published
11 Jun 2014

RSC Adv., 2014,4, 27634-27641

Author version available

A non-Bornian analysis of the Gibbs energy of hydration for organic ions

W. Murakami, M. Yamamoto, K. Eda and T. Osakai, RSC Adv., 2014, 4, 27634 DOI: 10.1039/C4RA02422B

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