Determination of the Driving Force for the Hydration of the Swelling Clays from Computation of the Hydration Energy of the Interlayer Cations and the Clay Layer

The key feature of swelling clays such as montmorillonite, in contrast with the nonswelling clays, is their ability to adsorb water in the interlayer space. This interlayer water interacts with the interlayer cations or with the silicate layer surface inside the interlayer space, or with both. However, no direct experimental technique offers the possibility to determine separately these two contributions. In order to determine the hydration energy for interlayer alkali cations, we use a combination of electrostatic calculations of the surface energy and measurements of immersion heats in clays. The results show that Li+ and Na+ cations are characterized by a strongly exothermic hydration energy in the interlayer space, in contrast with K+, Rb+, and Cs+ which have a much lower hydration energy in the interlayer space. The extreme situation is that of Cs+, for which an endothermic hydration energy value is obtained. These trends are in good agreement with results from molecular modeling calculations and con...

[1]  J. Douillard,et al.  Study of the surface energy of montmorillonite using PACHA formalism. , 2007, Journal of colloid and interface science.

[2]  J. Douillard,et al.  Determination of the surface energy of kaolinite and serpentine using PACHA formalism-comparison with immersion experiments. , 2006, Journal of colloid and interface science.

[3]  B. Smit,et al.  Hysteresis in clay swelling induced by hydrogen bonding: accurate prediction of swelling states. , 2006, Langmuir : the ACS journal of surfaces and colloids.

[4]  E. Rinnert,et al.  Hydration of a synthetic clay with tetrahedral charges: a multidisciplinary experimental and numerical study. , 2005, The journal of physical chemistry. B.

[5]  B. Lanson,et al.  Investigation of smectite hydration properties by modeling experimental X-ray diffraction patterns: Part I. Montmorillonite hydration properties , 2005 .

[6]  J. Douillard,et al.  Calculation of surface enthalpy of solids from an ab initio electronegativity based model: case of ice. , 2003, Journal of colloid and interface science.

[7]  D. Lévesque,et al.  Microscopic simulation of structure and dynamics of water and counterions in a monohydrated montmorillonite , 2002 .

[8]  M. Henry Nonempirical quantification of molecular interactions in supramolecular assemblies. , 2002, Chemphyschem : a European journal of chemical physics and physical chemistry.

[9]  M. Chávez-Páez,et al.  Monte Carlo simulations of Ca-montmorillonite hydrates , 2001 .

[10]  J. B. Mann,et al.  Configuration Energies of the Main Group Elements , 2000 .

[11]  J. Leszczynski,et al.  The interaction of nitrobenzene with the hydrate basal surface of montmorillonite: an ab initio study , 2000 .

[12]  A. Chatterjee,et al.  A DFT study on clay–cation–water interaction in montmorillonite and beidellite , 1999 .

[13]  J. Douillard,et al.  Thermodynamic Analysis of the Immersion of a Swelling Clay , 1998 .

[14]  P. F. Low,et al.  Changes in the Si−O Vibrations of Smectite Layers Accompanying the Sorption of Interlayer Water , 1996 .

[15]  G. Sposito,et al.  Monte Carlo Simulation of Interlayer Molecular Structure in Swelling Clay Minerals. 1. Methodology , 1995 .

[16]  M. L. Thompson,et al.  Hysteresis in Crystalline Swelling of Smectites , 1995 .

[17]  A. Delville Monte Carlo Simulations of Surface Hydration: An Application to Clay Wetting , 1995 .

[18]  Yizhak Marcus,et al.  A simple empirical model describing the thermodynamics of hydration of ions of widely varying charges, sizes, and shapes , 1994 .

[19]  R. Schoonheydt,et al.  The EEM approach to chemical hardness in molecules and solids: Fundamentals and applications , 1993 .

[20]  R. Nalewajski The hardness based molecular charge sensitivities and their use in the theory of chemical reactivity , 1993 .

[21]  A. Delville Structure of liquids at a solid interface: an application to the swelling of clay by water , 1992 .

[22]  Tsutomu Sato,et al.  Effects of Layer Charge, Charge Location, and Energy Change on Expansion Properties of Dioctahedral Smectites , 1992 .

[23]  A. Delville Modeling the clay-water interface , 1991 .

[24]  Leland C. Allen,et al.  Electronegativity is the average one-electron energy of the valence-shell electrons in ground-state free atoms , 1989 .

[25]  P. L. Hall,et al.  Adsorption of Water by Homoionic Exchange Forms of Wyoming Montmorillonite (Swy-1) , 1989 .

[26]  K. D. Collins,et al.  The Hofmeister effect and the behaviour of water at interfaces , 1985, Quarterly Reviews of Biophysics.

[27]  R. Nalewajski A study of electronegativity equalization , 1985 .

[28]  V. Drits,et al.  The distribution of octahedral cations in the 2:1 layers of dioctahedral smectites studied by oblique-texture electron diffraction , 1984, Clay Minerals.

[29]  R. Keren,et al.  Water Vapor Isotherms and Heat of Immersion of Na/Ca-Montmorillonite Systems—I: Homoionic Clay , 1975 .

[30]  K. Norrish,et al.  The swelling of montmorillonite , 1954 .

[31]  L. A. Wood,et al.  Adsorption of Water Vapor by Montmorillonite. I. Heat of Desorption and Application of BET Theory1 , 1952 .

[32]  R. T. Sanderson,et al.  An Interpretation of Bond Lengths and a Classification of Bonds. , 1951, Science.

[33]  Linus Pauling,et al.  THE NATURE OF THE CHEMICAL BOND. IV. THE ENERGY OF SINGLE BONDS AND THE RELATIVE ELECTRONEGATIVITY OF ATOMS , 1932 .