Aqueous Electrolytes near Hydrophobic Surfaces: Dynamic Effects of
Ion Specificity and Hydrodynamic Slip
²
David M. Huang, Ce ´cile Cottin-Bizonne, Christophe Ybert, and Lyde ´ric Bocquet*
UniVersite ´ de Lyon, UniVersite ´ Lyon 1, LPMCN, and CNRS, UMR 5586,
F-69622 Villeurbanne Cedex, France
ReceiVed July 19, 2007. In Final Form: September 20, 2007
We demonstrate, using molecular-dynamics computer simulations, the strong influence of surface wettability on
the equilibrium structure of the electrical double layer at solid interfaces and on electrokinetic transport in aqueous
electrolytes due to the effects of interfacial ion specificity and hydrodynamic slip. In particular, we show that anomalous
electrokinetic effects such as nonzero zeta potentials for uncharged surfaces are general features of electro-osmotic
flow in hydrophobic channels for electrolytes with substantial cation/anion size asymmetry, as a result of the stronger
attraction of the larger ion to the “vapor-liquid-like” interface induced by a hydrophobic surface. We establish that
the simulated velocity profiles obey continuum hydrodynamics on the nanoscopic length scales studied and show that
the anomalous flow profiles can be accurately predicted by using a modified Poisson-Boltzmann description for the
ion density distributions that incorporates an ion-size-dependent hydrophobic solvation energy as a crucial component.
We also demonstrate that, counterintuitively, the flow for a charge-neutral fluid is independent of the solid-fluid
friction coefficient.
1. Introduction
The rapid development of microfluidics
1,2
has spurred great
interest in recent years in the fundamental physics of fluid flow
on micrometer and smaller length scales. The violation of the
no-slip boundary condition (BC) of macroscopic hydrodynamics
that has been observed in a variety of systems at these length
scales
3-5
has particularly important implications for microfluidics
in that it offers the possibility of substantial flow amplification.
Hydrodynamic slip at the solid-liquid interface has been shown
to be controlled largely by the wetting properties of the liquid
on the solid surface: although the no-slip BC is satisfied by
solvophilic (hydrophilic for the case of water as the solvent)
surfaces, solvophobic (hydrophobic) surfaces can exhibit finite
slip.
6,7
The small length scale structure of the fluid interface, besides
controlling hydrodynamic slip, also plays an important role in
electrokinetic transport, a popular means of inducing fluid flow
in microfluidic devices,
2
because the magnitude and direction of
fluid flow depend sensitively on the interfacial distribution of
dissolved ions. In fact, the interplay between hydrodynamic slip
and the interfacial ion distribution can provide a powerful means
of microfluidic flow control.
8
The interfacial structure of
electrolyte interfaces also plays an important role in many other
phenomena, both static and dynamic, mediated by ions at aqueous
interfaces, in areas as diverse as biology,
9
atmospheric chemistry,
10
and colloid science.
11
The study of interactions between
hydrophobic surfaces in aqueous solutions (generally containing
dissolved ions) is an area of particular interest
12
because of their
importance in processes such as protein folding and micelle
formation.
Many such interfacial phenomena are strongly affected by the
identity of the cation or anion in solution,
9,13,14
contrary to
traditional theories of electrolyte interfaces such as the Gouy-
Chapman model of the electrical double layer
11
in which only
differences in ion valency are taken into account. Such trends
in physical phenomena as a function of cation or anion type are
generally referred to as Hofmeister series and are ubiquitous in
biology and physical chemistry.
13
Although in some cases the
observed ion-specific Hofmeister series are likely due to particular
ion-surface interactions,
15
in others the effects arise purely as
a result of the interfacial structure of water.
For example, the significant dependence of the air-water
surface tension on anion type for halide salts
15
has been explained
in terms of the differing propensities of the ions for the vapor-
liquid interface. Recent spectroscopic experiments
16,17
and
computer simulations
18,19
have indeed shown that the larger
bromide and iodide ions exhibit enhanced interfacial concentra-
tions. It has been suggested that the depleted water density near
²
Part of the Molecular and Surface Forces special issue.
* To whom correspondence should be addressed. E-mail: lyderic.
bocquet@univ-lyon1.fr.
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1442 Langmuir 2008, 24, 1442-1450
10.1021/la7021787 CCC: $40.75 © 2008 American Chemical Society
Published on Web 12/06/2007