Thermocapillary migration and interaction of drops: two non-merging drops in an aligned arrangement

2015 ◽  
Vol 766 ◽  
pp. 436-467 ◽  
Author(s):  
Zhaohua Yin ◽  
Qiaohong Li

AbstractA numerical study on the interaction of two spherical drops in thermocapillary migration in microgravity is presented. Unequal drop sizes in the axisymmetric model lead to strong drop interaction if the leading drop is smaller. The effect of the ratio of the two drop radii, their initial distance apart, and non-dimensional numbers on the interaction is studied in the case of non-merging drops in detail. The Marangoni number adopted in this paper is fairly large (around 100) so as to reveal the phenomena of real flows. As a result, the heat wake behind the leading drop plays an important role in drop interaction, and obviously different final drop distances and transient migration processes are observed for various sets of non-dimensional numbers. The influence of drop deformation on drop interaction is also investigated for relatively large capillary number (up to 0.2). Finally, some simulations are performed to explain the phenomena of drop interaction in previous experiments, and some suggestions for future experiments are also provided.

2021 ◽  
pp. 1-1
Author(s):  
Raphael Zanella ◽  
Caroline Nore ◽  
Xavier Mininger ◽  
Frederic Bouillault ◽  
Jean-Luc Guermond

2008 ◽  
Vol 155 (1-2) ◽  
pp. 80-93 ◽  
Author(s):  
Changkwon Chung ◽  
Martien A. Hulsen ◽  
Ju Min Kim ◽  
Kyung Hyun Ahn ◽  
Seung Jong Lee

2015 ◽  
Vol 92 (1) ◽  
Author(s):  
R. Pillai ◽  
J. D. Berry ◽  
D. J. E. Harvie ◽  
M. R. Davidson

2013 ◽  
Vol 683 ◽  
pp. 820-823
Author(s):  
Bambang Arip Dwiyantoro

Microdroplets on solid surface are very common phenomenon in many engineering applications. The microdroplet formed from the fluid remaining on the column of micropillar after dewetting process. In this study, we generated microdroplet with various patterns and simulated the microfluidic dynamic processes based on a deforming body-fitted grid approach. The simulation results provide for explaining the effects of Capillary number and the liquid thickness on micropillar surface in the growing droplet diameter and microdroplet formation time.


Author(s):  
Kazi M. Rahman ◽  
M. Ruhul Amin ◽  
Ahsan Mian

Abstract In the field of additive manufacturing process, laser cladding is widely considered due to its cost effectiveness, small localized heat generation, and full fusion to metals. Introducing nanoparticles with cladding metals produces metal matrix nanocomposites, which in turn improves the material characteristics of the clad layer. The governing equations that control the fluid flow are standard incompressible Navier–Stokes and heat diffusion equation, whereas the Euler–Lagrange approach has been considered for particle tracking. The mathematical formulation for solidification is adopted based on enthalpy porosity method. Liquid titanium has been considered as the initial condition where particle distribution has been assumed uniform throughout the geometry. A numerical model implemented in a commercial software based on control volume method has been developed, which allows to simulate the fluid flow during solidification as well as tracking nanoparticles during this process. A detailed parametric study has been conducted by changing the Marangoni number, convection heat transfer coefficient, constant temperature below the melting point of titanium, and insulated boundary conditions to analyze the behavior of the nanoparticle movement. The influence of increase in Marangoni number results in a higher concentration of nanoparticles in some portions of the geometry and lack of nanoparticles in rest of the geometry. The high concentration of nanoparticles decreases with a decrease in Marangoni number. Furthermore, an increase in the rate of solidification time limits the nanoparticle movement from its original position which results in different distribution patterns with respect to the solidification time.


1983 ◽  
Vol 23 (03) ◽  
pp. 461-474 ◽  
Author(s):  
N. Van Quy ◽  
J. Labrid

Abstract This paper describes an enhanced oil recovery (EOR) model involving use of chemical additives. The model is as general as possible in light of present phenomenological knowledge. It takes into consideration diffusion, exchanges between fluid phases. exchanges between fluids and solids, and convection (including gravity, relative permeabilities, viscosities, interfacial tensions (IFT's), and mobility reduction by polymers). Its main properties arethree-phase flow (aqueous, oleic, and microemulsion);that each phase can be represented by a mixture of seven components:overall flow is one dimensional (ID), but the sections of space considered may be constant or variable; and the porous medium may be heterogeneous. In addition to its compositional nature. which is required for describing changes in phase properties, the model must also account for ionic environment, loss of chemicals, and capillary number distribution. For these reasons, it differs from conventional multicomponent models. It is designed for simulating any EOR problem involving the addition of suitable chemicals to fluids to be injected continuously or in successive slugs. The model has been tested successfully by two-phase flow, four components (water, oil, polymer, and surfactant plus alcohol), and Winsor Type I environment experiments. It can be adapted to more and more complex phenomenological situations, depending on availability of data. Introduction Of the new techniques leading to increased oil production, EOR using chemical additives is one of the most promising. It involves adding sufficient amounts of chemical species to injected fluids to change phase properties, thereby enhancing oil flow. These changes occur in a highly complex way because of the superposition of several mass-transfer phenomena. The difficulties are increased because some of these phenomena, such as exchange between fluid phases and between fluids and solids, are not yet fully understood. A great deal of experimental research is being done to clarify this situation. However, no matter what experimental progress is made, it will never be easy to analyze all the mechanisms that occur simultaneously and to predict the behavior of the recovery process by pure reasoning or by intuition. A mathematical approach becomes necessary, and the first numerical studies of the problem can be found in the literature. Our contribution to this effort is described in this paper. It concerns developing a numerical model that is as general as possible within the scope of current phenomenological knowledge. The model is necessarily multicomponent and multiphase. However, it differs from ordinary compositional models by the number of new problems to be investigated. The principal problems include suitable ionic environment, loss of chemical additives, and capillary number distribution in space and time. SPEJ P. 461^


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