The electrophoretic motion of a dielectric sphere along the centerline
of a long circular pore is studied theoretically. The imposed electri
c field is constant and parallel to the nonconducting pore wall, and t
he particle and wall surfaces are assumed uniformly charged. Electrica
l double layers adjacent to solid surfaces are assumed to be thinner t
han particle radius and gap width between surfaces. The presence of th
e pore wall affects particle velocity: 1. an electroosmotic flow of th
e suspending fluid exists due to interaction between the electric fiel
d and the charged wall; 2. the local electric field on the particle su
rfaces is enhanced by the insulated wall, speeding up the particle, an
d 3. the wall increases viscous retardation of the moving particle. To
solve electrostatic and hydrodynamic governing equations, general sol
utions are constructed from fundamental solutions in both cylindrical
and spherical coordinate systems. Boundary conditions are enforced at
the pore wall by Fourier transforms and then on the particle surface b
y a collocation technique. Typical electric-field-line, equipotential-
line and streamline patterns for the fluid phase are exhibited, and co
rrections to the Smoluchowski equations for particle electrophoretic v
elocity are presented for various relative separation distances betwee
n the particle and wall. The presence of the pore wall always reduces
the electrophoretic velocity; however, the net wall effect is quire we
ak. even for very small gap width between the particle and wall.