An experimental and theoretical study is described dealing with the dielect
rophoretic motion of individual particles in a static as well as in a flowi
ng suspension subject to high-gradient ac electric fields. The experiments
were performed on very dilute suspensions of neutrally buoyant hollow ceram
ic spheres in a specially designed device in which the electric-field lines
and the dielectrophoretic force were along the plane perpendicular to the
streamlines of the main flow. Upon application of a high-gradient field (si
milar to several kV/mm) to a quiescent suspension, the particles were found
to move away from the electrodes and then to concentrate above the grounde
d electrodes, forming a distinct boundary between the clean fluid and the r
emaining suspension. This same field, when applied to a flowing suspension,
caused the particles to concentrate within thin stripes parallel to the fl
ow above the grounded electrodes and to travel with the suspending fluid wi
thin these stripes. The theoretical model for the particle motion included
only the dielectrophoretic force and the viscous drag, and required no fitt
ing parameters because the particle polarizability was calculated independe
ntly by measuring the concentration dependence of the complex permittivity
of the suspension in a spatially uniform electric field of low strength (si
milar to several V/mm). The computed particle motions and pattern formation
s were found to be in a good agreement with the experimental data. These re
sults demonstrate that the expression for the dielectrophoretic force which
employs the value of the particle polarization measured in fields of low s
trength can be used for describing the particle motions in fields of high s
trength. This approach enables one to model a broad range of electro-hydrod
ynamic phenomena in suspensions irrespective of whether or not they are per
fectly insulating or perfectly conducting. (C) 2000 American Institute of P
hysics. [S0021-8979(00)04022-6].