There has been a large body of work on the deposition of colloidal particle
s onto many different kinds and shapes of surfaces. Nearly all work in the
past has involved flowing systems in which a well-defined hydrodynamic laye
r exists at the collector surface with certain advantages and disadvantages
. We have chosen a still system in which transport of particles to the coll
ector surface occurs solely by diffusion. Both particles and surfaces were
negatively charged, so that deposition was driven by dispersion forces. A p
hotomicroscopic technique has been used to determine absolute values of ini
tial rates of deposition. Three monodisperse polystyrene colloids of variou
s particle sizes and surface charge densities were synthesized. Their zeta
potentials were determined by microelectrophoresis in Ba(NO3)(2) solutions.
Collector surfaces were glass and glass coated with polystyrene. Their zet
a potentials were determined from their streaming potentials in various con
centrations of electrolyte. Direct determination of diffusion coefficients
indicate that the particles behave normally. Initial deposition rates exhib
it strong dependence on ionic strength, indicating large electrical double
layer effects. Like the work of others, rates of deposition fell off with t
ime, perhaps due to the presence of 'hot spots', i.e. highly localized area
s of greater reactivity. The most regular behavior occurred in deposition o
n polystyrene-coated glass, presumably because roughness and highly reactiv
e sites on the glass surface were largely eliminated. Absolute rates were s
everal times theoretical for fastest deposition. It is speculated that the
hydrophobic effect plays a significant role in accelerating particles towar
ds the collector. Plots of log (initial rate constant) vs. log (ionic stren
gth) were linear and generally in the order anticipated by Reerink-Overbeek
theory. (C) 1999 Elsevier Science B.V. All rights reserved.