scholarly journals Influence of liquid drop properties on drop deformation at impaction of the drop with silicone oil surface

2000 ◽  
Vol 20 (2Supplement) ◽  
pp. 213-216
Author(s):  
Takahiro FUJIMATSU ◽  
Hideomi FUJITA ◽  
Masafumi Hirota ◽  
Takeshi ONO ◽  
Osamu OKADA
2010 ◽  
Vol 658 ◽  
pp. 438-462 ◽  
Author(s):  
JAMES Q. FENG

The steady axisymmetric flow internal and external to a deformable viscous liquid drop falling through a quiescent gas under the action of gravity is computed by solving the nonlinear Navier–Stokes equations using a Galerkin finite-element method with a boundary-fitted quadrilateral mesh. Considering typical values of the density and viscosity for common liquids and gases, numerical solutions are first computed for the liquid-to-gas density ratio ρ = 1000 and viscosity ratio μ from 50 to 1000. Visually noticeable drop deformation is shown to occur when the Weber number We ~ 5. For μ ≥ 100, drops of Reynolds number Re < 200 tend to have a rounded front and flattened or even dimpled rear, whereas those at Re > 200 a flattened front and somewhat rounded rear, with that at Re = 200 exhibiting an almost fore–aft symmetric shape. As an indicator of drop deformation, the axis ratio (defined as drop width versus height) increases with increasing We and μ, but decreases with increasing Re. By tracking the solution branches around turning points using an arclength continuation algorithm, critical values of We for the ‘shape instability’ are determined typically within the range of 10 to 20, depending on the value of Re (for Re ≥ 100). The drop shape can change drastically from prolate- to oblate-like when μ < 80 (for 100 ≤ Re ≤ 500). For example, for μ = 50 a drop at Re ≥ 200 exhibits a prolate shape when We < 10 and an upside-down button mushroom shape when We > 10. The various solutions computed at ρ = 1000 with the associated values of drag coefficient and drop shapes are found to be almost invariant at other values of ρ (e.g. from 500 to 1500) as long as the value of ρ/μ2 is fixed, despite the fact that the internal circulation intensity changes according to the value of μ. The computed values of drag coefficient are shown to agree quite well with an empirical formula for rigid spheres with the radius of the sphere replaced by the radius of the cross-sectional area.


2015 ◽  
Vol 60 (8) ◽  
pp. 1119-1125 ◽  
Author(s):  
R. S. Volkov ◽  
O. V. Vysokomornaya ◽  
G. V. Kuznetsov ◽  
P. A. Strizhak

1992 ◽  
Vol 241 ◽  
pp. 169-198 ◽  
Author(s):  
Osman A. Basaran

A fundamental understanding of nonlinear oscillations of a viscous liquid drop is needed in diverse areas of science and technology. In this paper, the moderate- to large-amplitude axisymmetric oscillations of a viscous liquid drop, which is immersed in dynamically inactive surroundings, are analysed by solving the free boundary problem comprised of the Navier–Stokes system and appropriate interfacial conditions at the drop–ambient fluid interface. The means are the Galerkin/finite-element technique, an implicit predictor-corrector method, and Newton's method for solving the resulting system of nonlinear algebraic equations. Attention is focused here on oscillations of drops that are released from an initial static deformation. Two dimensionless groups govern such nonlinear oscillations: a Reynolds number, Re, and some measure of the initial drop deformation. Accuracy is attested by demonstrating that (i) the drop volume remains virtually constant, (ii) dynamic response to small-and moderate-amplitude disturbances agrees with linear and perturbation theories, and (iii) large-amplitude oscillations compare well with the few published predictions made with the marker-and-cell method and experiments. The new results show that viscous drops that are released from an initially two-lobed configuration spend less time in prolate form than inviscid drops, in agreement with experiments. Moreover, the frequency of oscillation of viscous drops released from such initially two-lobed configurations decreases with the square of the initial amplitude of deformation as Re gets large for moderate-amplitude oscillations, but the change becomes less dramatic as Re falls and/or the initial amplitude of deformation rises. The rate at which these oscillations are damped during the first period rises as initial drop deformation increases; thereafter the damping rate is lower but remains virtually time-independent regardless of Re or the initial amplitude of deformation. The new results also show that finite viscosity has a much bigger effect on mode coupling phenomena and, in particular, on resonant mode interactions than might be anticipated based on results of computations incorporating only an infinitesimal amount of viscosity.


2014 ◽  
Vol 87 (6) ◽  
pp. 1351-1361 ◽  
Author(s):  
R. S. Volkov ◽  
A. O. Zhdanova ◽  
O. V. Vysokomornaya ◽  
G. V. Kuznetsov ◽  
P. A. Strizhak

SPE Journal ◽  
2015 ◽  
Vol 20 (05) ◽  
pp. 1135-1144 ◽  
Author(s):  
Zhibin Wang ◽  
Huifang Bai ◽  
Suyang Zhu ◽  
Haiquan Zhong ◽  
Yingchuan Li

Summary Experimental studies show that liquid drop is deformed from initial spherical shape into ellipsoid shape in annular-mist flow, and the available critical Weber number WeCrit determined by the experiment can vary from 2.2 to 60 for low-viscosity liquid. On the basis of the force equilibrium and the critical-Weber-number-calculation method proposed by Azzopardi (1985), this paper develops a new model to predict minimum gas rate. This model introduces a parameter Ck,Wecrit that describes the effect of liquid-drop deformation and the maximum drop-size difference on the minimum gas rate. The effect of liquid-droplet coalescence is also considered indirectly. A function to predict drop-deformation magnitude for different critical Weber numbers is developed on the basis of energy conservation. The function-prediction results are in good agreement with experimental data from the literature and the predicted result from the drop deformation/breakup model, and the average absolute deviation is 6.1%. The Ck,Wecrit calculated by the new model increases with the increase of the pressure and liquid amount and it varies from 3.99 to 7.3, which means the critical gas velocity increases with the increase of the pressure and liquid amount. Numerous gas-well data were used for the validation of these entrained models, including data from 33 low-pressure gas wells (wellhead pressure: 0.26–3.41 MPa) from Coleman et al. (1991) and 91 high-pressure gas wells (wellhead pressure: 0.7–56 MPa) from Turner et al. (1969). The result shows the new entrained model has a good comprehensive performance in judging liquid-loading status in both high- and low-pressure gas wells.


Author(s):  
Junya Onishi ◽  
Naoki Shikazono

Abstract Numerical simulation of drop motion on surfaces with micro patterns is conducted. The results are compared with existing experimental and analytical studies to validate the reliability of the numerical simulations. In the comparison of the liquid phase morphology on a surface with straight grooves, it is confirmed that a variety of liquid shapes, including droplets, filaments with positive/negative Laplace pressure and so on are successfully reproduced by the numerical simulation. Moreover, the numerically observed transition between these morphologies in a broad range of the groove aspect ratio and the static contact angle agrees with the morphology diagram which is obtained by a semi-analytic approach based on the surface free energy minimization. Furthermore, in the comparison of the spreading behaviors of a liquid drop on a surface with square pillars, it is shown that the numerical simulations can predict the time-dependent drop deformation during the spreading process. The comparison of the length of two spreading modes shows a quantitative agreement with the experimental results.


2000 ◽  
Vol 2000.1 (0) ◽  
pp. 809-810
Author(s):  
Takahiro FUJIMATSU ◽  
Hideomi FUJITA ◽  
Masafumi Hirota ◽  
Takesi ONO ◽  
Osamu OKADA

2016 ◽  
Vol 52 (1-2) ◽  
pp. 85-89 ◽  
Author(s):  
R. S. Volkov ◽  
M. V. Zabelin ◽  
P. A. Strizhak

Soft Matter ◽  
2018 ◽  
Vol 14 (26) ◽  
pp. 5442-5451 ◽  
Author(s):  
A. Mikkelsen ◽  
K. Khobaib ◽  
F. K. Eriksen ◽  
K. J. Måløy ◽  
Z. Rozynek

Utilizing electric fields, we have experimentally investigated the mechanics of particle-covered silicone oil drops suspended in castor oil, as well as particle assembly at drop surfaces.


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