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Interfacial waves and the dynamics of backflow in falling liquid films

Published online by Cambridge University Press:  31 May 2013

Emmanuel O. Doro
Affiliation:
G. W. Woodruff School of Mechanical Engineering, Georgia Institute of Technology, Atlanta, GA 30332, USA
Cyrus K. Aidun*
Affiliation:
G. W. Woodruff School of Mechanical Engineering, Georgia Institute of Technology, Atlanta, GA 30332, USA
*
Email address for correspondence: [email protected]

Abstract

By studying the dynamics of the streamwise pressure gradient at the wavefront of travelling interfacial waves, we investigate the formation and evolution of backflow regions for the sinusoidal and teardrop-shaped surface wave regimes of laminar falling liquid films. The magnitude of the wavefront streamwise pressure gradient grows as the flow inlet disturbance increases in amplitude and steepness. At large enough values, the adverse pressure gradient induces flow separation and subsequently backflow at the large-amplitude wavefront. The backflow region evolves from a closed circulation to an open vortex as the wave grows to saturation. The dynamics of the streamwise pressure gradient at the sinusoidal wavefront approaches a stable fixed point at saturation. Thus, the open vortex retains its structure as the wave continues downstream. The streamwise pressure gradient at the wavefront of the teardrop-shaped pulse evolves similarly to a time-periodic function with multiple minima/maxima. This phenomenon is a consequence of the interaction between the teardrop-shaped wave and newly formed preceding capillary waves. The nature of the teardrop pulse–capillary wave interaction is such that a decrease in magnitude of the streamwise pressure gradient at the teardrop-shaped wavefront is followed by an increase at the capillary wavefront and vice versa. The increased adverse pressure gradient at the capillary wavefront induces a second open vortex backflow, while the teardrop-shaped wavefront’s open vortex reverts to a closed circulation. This interaction between the waves continues as the teardrop pulse–capillary wavetrain travels downstream, leading to multiple capillary waves and backflow regions.

Type
Papers
Copyright
©2013 Cambridge University Press 

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References

Alekseenko, S. V., Nakoryakov, V. E. & Pokusaev, B. G. 1994 Wave Flow of Liquid Films. Begell House.Google Scholar
Benjamin, T. B. 1957 Wave formation in laminar flow down an inclined plane. J. Fluid Mech. 2 (6), 554573.CrossRefGoogle Scholar
Berberovic, E., van Hinsberg, N. P., Jarkirlic, S., Roisman, V. I. & Tropea, C. 2009 Drop impact onto a liquid layer of finite thickness: dynamics of the cavity evolution. Phys. Rev. E 79 (3), 036306.Google Scholar
Brackbill, J. U., Kothe, D. B. & Zemach, C. 1992 A continuum method for modelling surface tension. J. Comput. Phys. 100, 335354.CrossRefGoogle Scholar
Cerne, G., Petelin, S. & Tiselj, I. 2001 Coupling of the interface tracking and the two-fluid models for the simulation of incompressible two-phase flow. J. Comput. Phys. 171 (2), 776804.CrossRefGoogle Scholar
Chang, H.-C. 1994 Wave evolution on a falling film. Annu. Rev. Fluid Mech. 26, 103136.Google Scholar
Demekhin, E. A., Kaplan, M. A. & Shkadov, V. Y. 1987 Mathematical models of the theory of viscous liquid films. Fluid Dyn. 22, 885893.CrossRefGoogle Scholar
Dietze, G. F., Al-Sibai, F. & Kneer, R. 2009 Experimental study of flow separation in laminar falling liquid films. J. Fluid Mech. 637, 73104.Google Scholar
Dietze, G. F. & Kneer, R. 2011 Flow separation in falling liquid films. Frontiers Heat Mass Transfer 2, 033001.Google Scholar
Dietze, G. F., Leefken, A. & Kneer, R. 2008 Investigation of the backflow phenomenon in falling liquid films. J. Fluid Mech. 595, 435459.CrossRefGoogle Scholar
Gao, D., Morley, N. B. & Dhir, V. 2003 Numerical simulation of wavy falling film flow using VOF method. J. Comput. Phys. 192, 624642.Google Scholar
Hirt, C. W. & Nichols, B. D. 1981 Volume of fluid (VOF) method for the dynamics of free boundaries. J. Comput. Phys. 39, 201225.Google Scholar
Islam, M. A., Miyara, A., Nosoko, T. & Setoguchi, T. 2007 Numerical investigation of kinetic energy and surface energy of wavy falling liquid film. J. Therm. Sci. 16, 237242.Google Scholar
Jayanti, S. & Hewitt, G. F. 1995 Hydrodynamics and heat transfer of wavy thin film flow. Intl J. Heat Mass Transfer 40 (1), 179190.Google Scholar
Kapitza, P. L. & Kapitza, S. P. 1965 Wave Flow on Thin Layers of a Viscous Fluid. Collected Papers of P. L. Kapitza (ed. Haar, D. T.), vol. 2, pp. 662709. Pergamon.Google Scholar
Kunugi, T. & Kino, C. 2005 DNS of falling film structure and heat transfer via MARS method. Comput. Struct. 83, 455462.CrossRefGoogle Scholar
Kutateladze, S. S. & Gogonin, I. I. 1979 Heat transfer in film condensation of slowly moving vapour. Intl J. Heat Mass Transfer 22, 15931599.Google Scholar
Malamataris, N. A. & Balakotaiah, V. 2008 Flow structure underneath the large amplitude waves of a vertically falling film. AIChE J. 54, 17251740.Google Scholar
Malamataris, N. A., Vlachogiannis, M. & Bontozoglou, V. 2002 Solitary waves on inclined films: flow structure and binary interactions. Phys. Fluids 14, 10821094.Google Scholar
Massot, C., Irani, F. & Lightfoot, E. N. 1966 Modified description of wave motion in a falling film. AIChE J. 14, 445455.Google Scholar
Miyara, A. 1999 Numerical analysis on flow dynamics and heat transfer of falling liquid films with interfacial waves. Heat Mass Transfer 35, 298306.Google Scholar
Miyara, A. 2000 Numerical simulation of wavy liquid film flowing down on a vertical wall and an inclined wall. Intl J. Therm. Sci. 39, 10151027.CrossRefGoogle Scholar
Nosoko, T. & Miyara, A. 2004 The evolution and subsequent dynamics of waves on a vertically falling liquid film. Phys. Fluids 16 (4), 11181126.Google Scholar
Nosoko, T., Yoshimura, P. N., Nagata, T. & Oyakawa, K. 1996 Characteristics of two-dimensional waves on a falling liquid film. Chem. Engng Sci. 51 (5), 725732.Google Scholar
OpenCFD. 2011 The open source CFD toolbox. http://www.openfoam.com.Google Scholar
Pradas, M., Kalliadasis, S. & Tseluiko, D. 2012 Binary interactions of solitary pulses in falling liquid films. IMA J. Appl. Maths 77, 408419.Google Scholar
Ramaswamy, B., Chippada, S. & Joo, S. W. 1996 A full-scale numerical study of interfacial instabilities in thin-film flows. J. Fluid Mech. 325, 163194.CrossRefGoogle Scholar
Salamon, T. R., Amstrong, R. C. & Brown, R. A. 1994 Traveling waves on vertical films: numerical analysis using the finite element method. Phys. Fluids 6, 22022220.Google Scholar
Xu, Z. F., Khoo, B. C. & Wijeysundera, N. E. 2008 Mass transfer across the falling film: simulations and experiments. Chem. Engng Sci. 63, 25592575.CrossRefGoogle Scholar
Yih, C. S. 1963 Stability of liquid flow down an inclined plane. Phys. Fluids 6, 321334.Google Scholar