2011
DOI: 10.1098/rspa.2011.0305
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Topology-dominated dynamic wetting of the precursor chain in a hydrophilic interior corner

Abstract: The topology-dominated dynamic wetting of a droplet in a hydrophilic interior corner was explored using molecular dynamics simulations and molecular kinetic theory. A wetting transition in the interior corner of a single-file water-molecule precursor chain (PC), which eliminated the stress singularity and advanced much faster than the precursor film, was controlled by the interior angle. Owing to the confinement in the interior corner, the potential surface is lower and smoother. The one-dimensional hydrogen-b… Show more

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Cited by 45 publications
(30 citation statements)
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“…Once the PF came into contact with the pillars, it accelerated, especially at the interior corner between the pillar and the substrate, shown in figure 6(d). Because of the confinement, the potential surface at the interior corner is lower and smoother than that on the solid surface (Yuan & Zhao 2012). Hence a confined liquid molecule chain propagating ahead of the bulk droplet, i.e.…”
Section: Molecular Dynamics Simulationsmentioning
confidence: 99%
See 1 more Smart Citation
“…Once the PF came into contact with the pillars, it accelerated, especially at the interior corner between the pillar and the substrate, shown in figure 6(d). Because of the confinement, the potential surface at the interior corner is lower and smoother than that on the solid surface (Yuan & Zhao 2012). Hence a confined liquid molecule chain propagating ahead of the bulk droplet, i.e.…”
Section: Molecular Dynamics Simulationsmentioning
confidence: 99%
“…At the microscopic level, driven by the hydrodynamic pressure, the fringe advances on the base of the PF and fills the space among the pillars, as shown in figure 1(c). On one hand, the grooves between the pillars provide excess driving force to the PF and the fringe (Yuan & Zhao 2012); on the other hand, the pillars bring extra potential barriers to the PF and excess resistance to the fringe. How could these two opposite effects brought by the pillars achieve a balance in the fast advancing MCL?…”
Section: Introductionmentioning
confidence: 99%
“…The radius of curvature of the liquid in the inset was about 2 μm in the order of w. Hence, the local Laplace pressure P c1 ∼ γ LV /w ∼ 10 3 Pa, which provided additional driving energy to pull the liquid to spread with a fast velocity along the corner between the pillars and the substrate. 32 The liquid near the pillars quickly accommodated to the square shape and was pinned by the pillars at 0.4 ms. Meanwhile, the rest part of the MCL still kept spreading in a line with a slow velocity.…”
Section: -mentioning
confidence: 99%
“…It should be noted that the similar monatomic chains were reported only in a few experiments [16] or modeled in simulations [17,18]. However, in recent years, research on the electron transport properties of molecular devices has attracted increasing attention.…”
Section: Introductionmentioning
confidence: 99%