The surface free energy of Ca-montmorillonite has been determined from measurement of the contact angle of water on an oriented deposit immersed in n-alkanes; the oriented deposits were equilibrated at different relative humidities. These experiments provided the polar, ~s, and dispersive, ~, components of the surface free energy 7s. The results indicate that: (I) ?~s is mainly due to dispersive forces (7~ -~ 145 mJ.m 2) and, to a lesser degree, polar forces (~ _~ 35 mJ.m z). (2) The value of the apparent surface free energy of the clay, y,, tends towards that measured for water when the solid water content exceeds 50 wt%. (3) The sorption of water molecules substantially modifies the surface free energy of the solid; ?s decreases from 180 mJ.m -2 to 60 mJ.m z when the water content increases from 0 to 50%. These results agree with other observations made on solids whose surface characteristics are similar to montmorillonite, i.e. micas, silicates and glasses. In addition, variations of ?s with water content can be related to the hydration processes of smectites. Finally, these results show that the silicate no longer influences the surface properties when the montmorillonite water content exceeds 60%, In order to analyse the extent to which organic compounds control clay wettability, we have measured the surface free energy of organo-mineral complexes. The organic and mineral phases were first investigated separately and then in association. In this paper we describe the surface free energy properties of calcium-montmorillonite, which is often used as a model material.
THEORY
Measurement of the surf ace free energy of a solidUnlike liquids, the surface free energy of solids can not be determined directly and indirect methods have had to be developed (Adamson, 1982). We chose to estimate the surface free energy of Ca-montmorillonite from contact-angle measurements of water on the clay. Since this material is a high-energy solid, the usual method in a liquidsolid-vapour system cannot be used; the solid surface is completely wetted by the liquid, the contact angle 0 then being zero. We used the alternative method developed by Tamai et al. (1967), where the vapour phase is replaced by a second liquid phase. This method has been tested by Schultz et al. (1977a,b) on high-energy solid surfaces. They used saturated hydrocarbons as a second liquid phase, which enabled them to determine finite contact angles.