Film Stratification in the Presence of Colloidal Particles
Gopi Nath Sethumadhavan, Alex Nikolov, and Darsh Wasan*
Department of Chemical and Environmental Engineering, Illinois Institute of Technology,
Chicago, Illinois 60616
Received July 3, 2000. In Final Form: January 4, 2001
This is probably the first study about the drainage of curved liquid films in the presence of colloidal
particles. The systems did not contain any surfactant. In the presence of monodispersed colloidal particles,
thinning occurs in a stepwise manner (stratification). It has been shown that the size of the film is an
important parameter in the stepwise thinning process. This investigation found a critical film size below
which at least one layer of particles stays in the film at equilibrium; a “spot” (a thinner section of the film),
even if formed, does not expand and is in equilibrium with the film. The area of the spot expands linearly
with time. The rate of spot-area expansion increases linearly with the film perimeter and can be increased
or decreased merely by changing the film size. The stepwise film thinning and the effects of film size and
particle concentration on film stability are discussed on the basis of the diffusive-osmotic mechanism.
Introduction
The phenomenon of particle layering between flat hard
walls has been observed
1,2
and understood through
computer simulations
3-6
and theoretical modeling.
7,8
When
a colloidal solution is present between two close flat walls
(for example, a thin liquid film), the confinement causes
the particles to form a layered structure parallel to the
walls. Layering is an entropic phenomenon and occurs
because the particles have a finite size that limits the
number that can occupy the layer closest to the walls.
Such layering naturally produces oscillatory decay in the
number-density of particles near the walls. The concen-
tration of colloidal particles between the flat walls (i.e.,
in the film) is higher than that in the bulk and produces
a stabilizing pressure (“disjoining pressure”) that has the
same oscillatory nature. Even though the phenomenon of
particle layering is well understood, its implications to
the mechanism of stepwise film thinning are not clear.
The two widely discussed mechanisms, (1) the “hole-
sheeting” model
9,10
and (2) the diffusive-osmotic model,
11
predict different stepwise behavior. This study is aimed
at checking their validity against experimental observa-
tions.
In colloidal dispersions such as foams and emulsions,
curved films are susceptible to earliest rupture (for
example, on the top of a foam). Therefore, we have used
curved films, free of surfactants, to study solely the effect
of hydrophilic colloidal particles on the stratification of
thin liquid films.
Experimental Section
Materials. Dispersion of monodispersed 8 nm silica particles
at 5% and 80 nm particles at 10% v/v from Nalco Chemicals,
Naperville, IL, were used in these experiments. The 80 nm system
produced a total of four step-transitions during thinning and
was found to have an effective particle volume fraction of 0.35,
accounting for the double layer thickness (for details on meth-
odology refer to ref 12). By use of a similar method, the 8 nm
system was found to produce a total of three step-transitions
during thinning and had an effective particle volume fraction of
0.25. The foam films in both the systems were stabilized only by
colloidal particles.
Experimental Methods. All experiments were carried out
at room temperature (24 °C). We used an experimental technique
(Figure 1) similar to one developed recently
13
to investigate film
thinning of curved films. An air bubble is formed from a tiny
capillary (radius ≈ 0.5 mm) and the solution level around the
bubble is lowered until the film size is of the required dimensions
(diameter <500 μm). In the reflected light interference micro-
scopic technique, white light from the top incident on the film
surface is reflected from the bottom and the top surface of the
film producing interference patterns. The microscope was used
in conjunction with a CCD camera, a video recorder, and an
image analyzer to monitor the interference patterns as a function
of time. From the color of the interference pattern, we can
calculate the film thickness as a function of time, allowing us to
monitor the thinning process. The size of the bubble affects the
capillary pressure (Pc), which is monitored using a sensitive
pressure transducer. The film curvature and the equilibrium
disjoining pressure (Πeqb ) Pc/2)
14
are affected by changing the
bubble size. In all of the curved film experiments reported here
we used a capillary pressure of 1800 ( 20 dyn/cm
2
. The sys-
tem was sealed to prevent any water evaporation from the
solution.
Results and Discussions
When flat films containing colloidal particles thin to a
thickness of a few particle diameters, further thinning
occurs in a stepwise manner.
12,15
The same was observed
here in curved films. When the film reached a thickness
* To whom all correspondence should be addressed.
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2059 Langmuir 2001, 17, 2059-2062
10.1021/la000936l CCC: $20.00 © 2001 American Chemical Society
Published on Web 03/08/2001