The low-frequency dielectrophoresis in clay-water-electrolyte systems
is governed by the electrical double layer surrounding the clay partic
les. The dielectrophoretic force imposed on the double layer can be qu
antitatively accounted in terms of the Stern-Gouy double layer model a
nd its polarization and conduction in a non-uniform electric field. Th
e magnitude and direction of dielectrophoretic force are determined by
the effective polarizability and the intensity and configuration of t
he field. In most clay-water-electrolyte systems, the dielectrophoreti
c force imposed on clay particles through the electrical double layer
is towards the lower field intensity, thus water will be forced moving
to the central electrode. The theory was consistent with the experime
ntal observations in synthetic and natural clays.