A rich spectrum of interfacial dynamic with and without
contact-line resistance have been studied. Drops are found to pinch off
from a rivulet on the underside of an inclined plane when two conditions
are met: a jetting mechanism when drop front steepens beyond a critical
value and a pinching mechanism when the transverse curvature exceeds another.
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Falloff
by the jet mechanism at high flow rates.A steepened hump is observed behind
the jet.
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Fall off by the pinch-off mechanism.The last hump is barely supercritical while the first two are barely subcritical.The subcritical drops traverse the entire plane without falling off.Different drops are on different sides of criticality because, at this critical condition, a fallen drop can reduce the local flow rate to subcritical values. |
Both conditions are determined analytically by matched
asymptotycs and correlated to experimental data. Rivulet formation from
a straight contact line driven by gravity can occur, when the film behind
the contact line cannot sustain a nose coonfiguration across the entire
front as the film thins.
A typical set of fall-off data for the glycerin-water solution with error bars attached. The solid lines correspond to our theoretical predictions.The the limiting pinching asymptote is also shown |
The liquid rolls in a nose front and suffers less resistance
than the sliding motion in a wedge front - the alternative front
configuration specified by gravity and capillary forces. As a result, only
parts of the front continue to roll and form rivulets. The position and
speed at the point of rivulet formation are determined by matched asymptotics.
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Fingering
of Castor oil on dry (a) and prewetted (b, c) plane. On a dry plane, fingering
behavior of highly-wetting Castor oil is qualitatively similar to that
of glycerine.The solid line is the |
(a) Normalised position plots for the straight front before fingering and a finger and a minimum after fingering for (+) the Castor oil and (o) glycerine data. (b) Normalised plots of the front and finger position as functions of time for 5 glycerine runs. |
Representative publications: