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Experimental investigation of the creeping motion of a drop in a vertical tube
Authors:M Coutanceau  A Texier
Institution:(1) Laboratoire de Mécanique des Fluides (UA 191), 40 Avenue du Recteur Pineau, F-86022 Poitiers Cedex, France
Abstract:New experimental data regarding the motion of a drop along the axis of a vertical tube, filled with another highly viscous liquid, are obtained. The experiments are realised with sufficiently large drops for an internal circulation to develop and also for different pairs of fluids; the preponderant role of the gravity on the drop shape and consequently on its terminal velocity is pointed out. Moreover, by means of a visualization technique, details on the flow both inside and outside the drop are given.List of symbols g gravity acceleration - r distance from the drop center - R equivalent radius of the drop, i.e. the radius of the sphere having the same volume as the drop - R EQ radius of the equatorial section of the drop - R T tube radius - L AX half length of the drop - U 0 terminal velocity of the drop - P s Poiseuille number= U 0 mgr e /4 Deltarhov g R 2 - Fr Fronde number = U 0 2 rhov e /2 g R delta rhov - Re Reynolds number = 2 U 0 R rhov e /mgr e - E o Eötvös number = 4g Deltarhov R 2/sgr - Gcy deformation parameter = mgr e U 0/sgr - Deltarhov apparent density of the suspended liquid= |rhov i rhov e | - mgr i viscosity of the suspended liquid - mgr e viscosity of the suspending liquid - lambda drop-to-tube radius ratio = R/R T - lambda EQ equatorial drop-to-tube radius ratio = R EQ/R T - sgr interfacial tension
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