19 - Lecture notes for Clay Mineralogy

The Geochemistry of clay minerals
Suggested reading:

Reading: Newman 203-236




Equilibrium adsorption and ion exchange.

The typically small grain size (<2 µm) of clay minerals results in the presence of large surface areas. These surface areas are available for exchange of ions and molecules between the solids and surrounding solutions.

Exchange of ions involves adsorption and desorption which are commonly fast (on geological time scales).

This exchange process can be treated as an equilibrium process.

The kinetics of adsorption in natural environments is poorly understood (implications for waste treatment and disposal).

Adsorption takes place because of the attraction of ions to a surface. The strength of the bonding varies from weak van der Waals (physical adsorption) to moderate absorbtion (electostatic adsorption) to strong chemical bonds (chemisorption), henceforth simply referred to as adsorption.

This process involves neutral species (H
2O, H4SiO4, organic molecules) and ions.

Example of kaolinite: Notice in the schematic diagram below that for 1:1 structures, positive ions are attracted to the light-blue tetrahedral basal oxygen surface. At the same time, negative ions are attracted to the dark-blue octahedral hydroxyl surface.


Example of vermiculite or smectite. The case for low-charge 2:1 structures is notably different from 1:1 structures. The schematic diagram below shows that 2:1 structures have mostly positive ions are attracted to the light-blue tetrahedral basal oxygen surfaces.


Surface charge properties

One way in which surface charge can develop is by adsorption of an ion where the solid acts as an electrode. (e.g., H
+ and OH- on the surfaces of clays).

In clay-aqueous systems the potential of the surface is determined by the activity of ions (e.g., H
+ or pH) which react with the mineral surface.

The simultaneous adsorption of protons and hydroxyls as well as other potential determining cations and anions, leads to the concept of zero point of charge or ZPC, where the total charge from the cations and anions at the surface is equal to zero.

The charge must be zero and this does not necessarily mean the number of cations versus anions in the solution are equal. For clay minerals the potential determining ions are H+ and OH- and complex ions formed by bonding with H+ and OH-.

For example on the basal oxygen surface of kaolinite or illite, the O
2- ions bond with H+ to form hydroxyls. These surfaces further react as either acids or bases with other protons or hydroxyls: The surface charge is therefore, pH dependent. The broken Si-O bonds and Al-OH bonds along the surfaces of the clay crystals result in hydrolysis.


Low pH


MOH + H
+ --> MOH2+


High pH


MOH + OH
---> MO- + H2O

The potential at the surface is determined by the activity of these ions given by the Nernst Equation, where:

At equilibrium, the electric potential (E) is equal to the standard state electric potential (E
o ) and the relationship:

E = E
o - (RT/nF) ln (a/ao)

where: R = gas constant (8.314 J mol-1 K-1), F= Faraday constant  (p96485 C),T = emperature  in Kelvin,  n = number of molar equivalents of electrons transferred


The pH that corresponds to the ZPC is referred to as the pHZPC or the isoelectric point.


1. With pH's below the pHZPC the solid has would have anion exchange capacity.

2. pH's at the pHZPC , the solid would have no exchange capacity.

3. pH's above the pHZPC, the solid would have cation exchange capacity.



Table of pH for zero point of charge for clay minerals. Note that in Georgia Piedmont soils, the typical pH is below 4, in Georgia estuarine systems typical pH is 7.5.

 Mineral

 pHZPC

Gibbsite

10

  Hematite

  4.2 - 6.9

Goethite

 5.9 - 6.7

 Na-feldspar

 6.8

 Kaolinite

 2 - 4.6

 Montmorillonite

 <2 - 3

 Quartz

 1 - 3


Note that Al and Fe hydroxides have a high pHZPC .
Kaolinite and montmorillonite have low pHZPC.

The ZPC is determined from a titration curve where pH is varied (see figure 3.2 from Eslinger and Pevear).


The adsorption of potential-determining ions results in the development of a electric double layer.

inner layer
- fixed and contains potential determining ions
outer layer - mobile diffuse layer of freely moving counter ions

There are numerous models devised to predict the distribution of surface-species. The two simplest models that give a reasonable representation of the ion distributions are the Gouy and Stern models.

See figures 3.3 and 3.4 from Eslinger and Peaver

Potential determining ions need not be protons and hydroxyl.

Organic anions from the dissociation of humic and fulvic acids. Deprotonated carboxyl groups (e.g., RCOO
-).