The time-dependent drop distribution of a dilute, polydisperse emulsion is
measured in a simple shear flow. The suspending fluid is much more viscous
than the dispersed phase (1:1000). Drops are found to drift away from eithe
r bounding wall and accumulate near the center of the gap, due to the aniso
tropy of droplet-plane interactions. An expression for this drift velocity
has been derived for single drops by Chan and Leal [J. Fluid Mech. 92, 131
(1979)] and was in agreement with isolated drop migration observed in our w
ork. Eventually the inward drift is balanced by a shear-induced gradient di
ffusivity, and a steady-state concentration distribution is reached. When t
he drops are sufficiently far from either wall a self-similar, parabolic co
ncentration profile is predicted at all times. Droplet diffusivities were d
etermined for capillary numbers Ca=(gamma) over dot (a) over bar<<mu>/sigma
between 0.17 and 0.92, where (gamma) over dot is the shear rate, (a) over
bar is the mean drop radius, mu is the viscosity of the suspending fluid, a
nd sigma the interfacial tension. The values obtained are an order of magni
tude lower than theoretical predictions of Loewenberg made in the limit of
small deformation. (C) 2001 American Institute of Physics.