The
electrophoretic mobility and the zeta potential (ζ) of
fluorescently labeled colloidal silica rods, with an aspect ratio
of 3.8 and 6.1, were determined with microelectrophoresis measurements
using confocal microscopy. In the case where the colloidal particles
all move at the same speed parallel to the direction of the electric
field, we record a xyz-stack over the whole depth
of the capillary. This method is faster and more robust compared to
taking xyt-series at different depths inside the
capillary to obtain the parabolic flow profile, as was done in previous
work from our group. In some cases, rodlike particles do not move
all at the same speed in the electric field, but exhibit a velocity
that depends on the angle between the long axis of the rod and the
electric field. We measured the orientation-dependent velocity of
individual silica rods during electrophoresis as a function of κa, where κ–1 is the double layer
thickness and a is the radius of the rod associated
with the diameter. Thus, we determined the anisotropic electrophoretic
mobility of the silica rods with different sized double layers. The
size of the double layer was tuned by suspending silica rods in different
solvents at different electrolyte concentrations. We compared these
results with theoretical predictions. We show that even at already
relatively high κa when the Smoluchowski limiting
law is assumed to be valid (κa > 10), an
orientation
dependent velocity was measured. Furthermore, we observed that at
decreasing values of κa the anisotropy in the
electrophoretic mobility of the rods increases. However, in low polar
solvents with κa < 1, this trend was reversed:
the anisotropy in the electrophoretic mobility of the rods decreased.
We argue that this decrease is due to end effects, which was already
predicted theoretically. When end effects are not taken into account,
this will lead to strong underestimation of the experimentally determined
zeta potential.