Translational and rotational near-wall diffusion of
spherical colloids studied by evanescent wave
scattering
Maciej Lisicki,
*
a
Bogdan Cichocki,
a
Simon A. Rogers,
b
Jan K. G. Dhont
cd
and Peter R. Lang
c
In this article we extend recent experimental developments [Rogers et al., Phys. Rev. Lett., 2012, 109,
098305] by providing a suitable theoretical framework for the derivation of exact expressions for the first
cumulant (initial decay rate) of the correlation function measured in Evanescent Wave Dynamic Light
Scattering (EWDLS) experiments. We focus on a dilute suspension of optically anisotropic spherical
Brownian particles diffusing near a planar hard wall. In such a system, translational and rotational
diffusion are hindered by hydrodynamic interactions with the boundary which reflects the flow incident
upon it, affecting the motion of colloids. The validity of the approximation by the first cumulant for
moderate times is assessed by juxtaposition to Brownian dynamics simulations, and compared with
experimental results. The presented method for the analysis of experimental data allows the
determination of penetration-depth-averaged rotational diffusion coefficients of spherical colloids at
low density.
1 Introduction
Rotational diffusion plays a crucial role in a number of physical,
chemical, and biological processes occurring in a variety of
systems. Notable examples include microrheology, in which
frequency-dependent viscoelastic shear moduli can be investi-
gated by measuring rotational diffusion of a tracer sphere;
1
random reorientation of biomacromolecules in membranes
(like proteins in human erythrocyte membrane,
2
or rhodopsin
chromophores
3
); rotational-diffusion controlled chemical reac-
tivity;
4–6
and gaseous combustion models, where rotational
diffusion is of importance for the interpretation of coherent
anti-Stokes Raman spectroscopy data.
7
Much attention has
been devoted over the last decade to rotational diffusion of bulk
systems, particularly in the context of macromolecules. Similar
systems in geometrical connement are, however, much less
understood, and are becoming a very active eld of research.
This is motivated by the fundamental importance of the effects
of connement for macromolecular solutions, which are most
pronounced in the small-scale channel ows which are an
inherent feature of micro-,
8
nano-
9
and optouidics.
10
An
illustrative example may be given in the rapidly growing “lab-
on-a-chip” applications, in which a single colloid might be used
as a micropump,
11
or by investigation of swimming microor-
ganisms,
12
nutrition of which is strongly inuenced by their
hydrodynamic interactions;
13
conned geometry plays a key role
also in chip-based capillary electrophoresis
14
and sorting of
white blood cells.
4
To investigate the effects of connement on rotational
diffusion of Brownian particles, we have employed Evanes-
cent Wave Dynamic Light Scattering
15
(EWDLS), which is a
technique that probes the near-wall dynamics of submicron-
sized particles. In the experiments, only the region of the
sample close to the boundary is illuminated, as the electric
eld strength of an evanescent wave decays with distance z
away from the wall as exp(kz/2). The characteristic length
scale 2/k, called the penetration depth, is typically of the order
of several hundred nanometers. Using this feature, one can
infer information on the effects of hydrodynamic interactions
with the surface on the dynamics of suspended colloids. By
changing the scattering vector q, the system is probed on
different length scales.
Starting with the pioneering work by Lan and Ostrowsky,
15
EWDLS has been employed frequently to investigate the near
surface dynamics of so matter. The translational diffusion of
colloids has been studied in dilute solutions
16–18
and in
suspensions with volume fractions up to 45 percent.
19,20,21
The
dynamics of stiff polymers adsorbed to the interface
22
were
investigated as well as the collective motion of end-graed
polymer brushes.
23,24
With a setup that allows independent
a
Institute of Theoretical Physics, Faculty of Physics, University of Warsaw, ul. Ho˙ za 69,
00-681 Warsaw, Poland. E-mail: mklis@fuw.edu.pl
b
Department of Chemical and Biomolecular Engineering, University of Delaware,
Newark, DE 19716, USA
c
ICS-3, Institute of Complex Systems, Forschungszentrum J¨ ulich, D-52425 J¨ ulich,
Germany
d
Heinrich-Heine University, Department of Physics, D¨ usseldorf, Germany
Cite this: Soft Matter, 2014, 10, 4312
Received 7th January 2014
Accepted 9th April 2014
DOI: 10.1039/c4sm00148f
www.rsc.org/softmatter
4312 | Soft Matter, 2014, 10, 4312–4323 This journal is © The Royal Society of Chemistry 2014
Soft Matter
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