2011
DOI: 10.1016/j.colsurfa.2010.09.002
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Enabling the enhancement of electroosmotic flow over superhydrophobic surfaces by induced charges

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Cited by 21 publications
(17 citation statements)
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“…In section III C, we will compare these results with the more exact ones based on expressions (11), (14), (21) and (23). Additionally we also compare with numerical calculations, using the nonlinear Poisson-Boltzmann equation instead of relying on the linearised Debye-Hückel approximation.…”
Section: Resultsmentioning
confidence: 97%
See 1 more Smart Citation
“…In section III C, we will compare these results with the more exact ones based on expressions (11), (14), (21) and (23). Additionally we also compare with numerical calculations, using the nonlinear Poisson-Boltzmann equation instead of relying on the linearised Debye-Hückel approximation.…”
Section: Resultsmentioning
confidence: 97%
“…This latter condition seems nontrivial at first, since any ions that are preferentially attracted to the surface are expected to attract an equal amount of opposite charge in a diffuse cloud just as on a solid surface. However, a net charge is a) Corresponding author: baier@csi.tu-darmstadt.de attracted to the surface when an electric field is applied normal to the fluid-air interface 20 , for example by embedding electrodes within the grooves 21 .…”
Section: Introductionmentioning
confidence: 99%
“…Instead of air being enclosed in the corrugations, other materials like for instance oil could be employed, which promises an improved stability of the Cassie state against pressure (Wong et al 2011) or enhanced electrical properties (Steffes, Baier & Hardt 2011). The choice of an appropriate groove-filling medium provides the chance to specifically tailor the surface properties, for examples in terms of phobicity and philicity, not only with regard to water, but to any desired fluid.…”
Section: Introductionmentioning
confidence: 99%
“…Next, the velocity field w q |i (originating from the charge accumulated at the gas-liquid interface) is described. In the limit of an infinitely thin EDL as treated herein, the overall electro-osmotic force per volume on the ion cloud accumulating in the vicinity of the free surface can be replaced [38,39] by an effective stress condition η(∂ y w q |i ) |i = −q |i ∂ z φ st = −τ ∞,q , while in the bulk (∂ 2…”
Section: Velocitymentioning
confidence: 99%