The force on a charged solid particle (of general shape) suspended in
a flowing polar fluid (e.g. an aqueous electrolyte solution) in the pr
esence of a solid bounding wall (of general shape) is obtained for the
situation in which the electrical double-layer thickness is very much
smaller than the particle size (and the distance between particle and
wall). The very general results so obtained are applied to the sedime
ntation of a charged spherical particle in an unbounded polar fluid (w
ith no walls present) for which the drag force is found to be in compl
ete agreement with Ohshima et al. (1984). However, there is disagreeme
nt between the present results and those obtained in a number of publi
shed papers owing to incorrect assumptions being made in the latter as
to what physical mechanism gives rise to the dominant contribution to
the electroviscous force on the particle.