1969
DOI: 10.1073/pnas.63.2.292
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On the Behavior of a Capillary Surface in a Wedge

Abstract: Estimates above and below are obtained for the height of the equilibrium-free surface of a liquid when the liquid partially fills a cylindrical container whose cross section contains a corner with interior angle 2alpha. The surface is characterized by the condition that its mean curvature be proportional to its height above a reference plane (or, in the case of zero gravity, that the mean curvature be constant), and by the requirement that it meet the container wall with prescribed contact angle gamma. It turn… Show more

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Cited by 403 publications
(331 citation statements)
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“…The MCL was initially ( t = 0.47 s, figure 3b) linear on the substrate at a velocity U ∼ 0.01 mm s −1 (dashed blue line, figure 4b). Once the MCL reached the pillars ( t = 0.52 s, figure 3b), the excess driving force forced the MCL to accelerate, making the liquid propagate much faster at the interior corner between the pillar and the substrate, known as the Concus-Finn effect (Concus & Finn 1969). In an interior corner with opening angle 2α, the equilibrium velocity could be calculated as U = fU CA = f γ LV /µ (Weislogel & Lichter 1998), where f = sin α(cos θ 0 − sin α)/S is the topological coefficient for capillary flow at the interior corner.…”
Section: Multiscale Experimentsmentioning
confidence: 99%
“…The MCL was initially ( t = 0.47 s, figure 3b) linear on the substrate at a velocity U ∼ 0.01 mm s −1 (dashed blue line, figure 4b). Once the MCL reached the pillars ( t = 0.52 s, figure 3b), the excess driving force forced the MCL to accelerate, making the liquid propagate much faster at the interior corner between the pillar and the substrate, known as the Concus-Finn effect (Concus & Finn 1969). In an interior corner with opening angle 2α, the equilibrium velocity could be calculated as U = fU CA = f γ LV /µ (Weislogel & Lichter 1998), where f = sin α(cos θ 0 − sin α)/S is the topological coefficient for capillary flow at the interior corner.…”
Section: Multiscale Experimentsmentioning
confidence: 99%
“…For water filling in a specific single microcavity, an enhanced capillary rise, a gradient Taylor rise, [53,54] induced by the gradient wedge corner of the microcavity, contributes to the fast liquid flow. [55][56][57][58] The water firstly quickly spreads along the wedge, then pushes out the air, and finally converges at the front of the microcavity. The overall continuous unidirectional water transport is illustrated in Figure 1d.…”
Section: Introductionmentioning
confidence: 99%
“…Fluid behavior in low gravity is strongly influenced by container geometry [4] and even small changes may have drastic effects. This was unexpectedly demonstrated in a recent experiment where a small container asymmetry caused fluid to unexpectedly shift entirely to one side of a container [5].…”
Section: Motivationmentioning
confidence: 99%