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Convective instabilities in liquid layers with free upper surface under the action of an inclined temperature gradient

Phys. Fluids 21, 112102 (2009); doi:10.1063/1.3251755

Published 3 November 2009

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A. I. Mizev1 and D. Schwabe2
1Institute of Continuous Media Mechanics, Ural Branch of the RAS, Koroleva Street 1, Perm 614013, Russia
2Physikalisches Institut, Justus-Liebig-Universität Giessen, Heinrich-Buff-Ring 16, D-35392 Giessen, Germany

We present the results of an experimental study of convective instabilities in a horizontal liquid layer with free upper surface under the action of an inclined temperature gradient, i.e., when horizontal and vertical temperature gradients are applied at the same time. Silicone oil of 10 cSt (Prandtl number Pr=102) was employed as the test fluid. We investigated the layers with different thicknesses to examine the influence of gravity on the formation of the convective patterns. It is found out that the system behavior appreciably depends on the dynamic Bond number, which shows a relation of buoyancy and thermocapillary forces. In the case of small dynamic Bond numbers, when the influence of buoyancy is minimal, four different flow patterns, according to the combination of the vertical and horizontal Marangoni numbers, have been found: steady parallel flow, Bénard–Marangoni cells, drifting Bénard–Marangoni cells, and longitudinal rolls. At larger dynamic Bond number, when the influence of buoyancy becomes considerable, new convective structures, named by us the “surface longitudinal rolls” and the “surface drifting cells,” appear in addition to the patterns listed above. These instabilities exist only in the surface part of the thermocapillary flow, whereas the return flow remains stable. Under large enough dynamic Bond number these patterns become the dominating ones, forcing out the classical Bénard–Marangoni instability. We give a phenomenological description of the obtained convective patterns and present the stability diagram in the plane of the vertical and the horizontal Marangoni numbers. ©2009 American Institute of Physics
History: Received 11 July 2008; accepted 30 September 2009; published 3 November 2009
Permalink: http://link.aip.org/link/?PHFLE6/21/112102/1
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KEYWORDS and PACS

Keywords
PACS
  • 47.20.Bp
    Buoyancy-driven flow instabilities
  • 47.54.De
    Experimental aspects of pattern selection and formation
  • 68.03.Cd
    Surface tension and related phenomena
  • 47.55.pf
    Marangoni convection
  • 47.55.nb
    Capillary and thermocapillary flows
  • YEAR: 2009

PUBLICATION DATA

ISSN:
1070-6631 (print)   1089-7666 (online)
Publisher:
AIP is a member of CrossRef AIP

REFERENCES (41)

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  1. H. Bénard, “Les tourbillons cellulaires dans une nappe liquide,” Rev. Gén Sci. Pures Appl. 11, 1261 (1900).
  2. J. R. A. Pearson, “On convection cells induced by surface tension,” J. Fluid Mech. 4, 489 (1958).
  3. E. L. Koschmieder, Bénard Cells and Taylor Vortices (Cambridge University Press, Cambridge, 1993).
  4. D. Schwabe, “Marangoni instabilities in small circular containers under microgravity,” Exp. Fluids 40, 942 (2006).
  5. R. V. Birikh, “Thermocapillary convection in horizontal layer of liquid,” J. Appl. Mech. Tech. Phys. 7, 43 (1966).
  6. D. Schwabe, “Marangoni effects in crystal growth melts,” PCH, PhysicoChem. Hydrodyn. 2, 263 (1981).
  7. D. Schwabe, “Surface-tension-driven flow in crystal growth melts,” in Crystals Growth, Properties, and Applications, edited by H. C. Freyhardt (Springer, Berlin, 1988), Vol. 11.
  8. M. K. Smith and S. H. Davis, “Instabilities of dynamic thermocapillary liquid layers. Part 1: Convective instabilities,” J. Fluid Mech. 132, 119 (1983).
  9. J. Burguete, N. Mukolobwiez, F. Daviaud, N. Garnier, and A. Chiffaudel, “Buoyant thermocapillary instabilities in an extended liquid layer subjected to a horizontal temperature gradient,” Phys. Fluids 13, 2773 (2001).
  10. S. Benz and D. Schwabe, “The three-dimensional stationary instability in dynamic thermocapillary shallow cavities,” Exp. Fluids 31, 409 (2001).
  11. D. Schwabe, U. Möller, J. Schneider, and A. Scharmann, “Instabilities of shallow dynamic thermocapillary liquid layers,” Phys. Fluids A 4, 2368 (1992).
  12. D. Villers and J. K. Platten, “Coupled buoyancy and Marangoni convection in acetone: Experiments and comparison with numerical simulations,” J. Fluid Mech. 234, 487 (1992).
  13. R. Riley and G. Neitzel, “Instability of thermocapillary-buoyancy convection in shallow layers. Part 1. Characterization of steady and oscillatory instabilities,” J. Fluid Mech. 359, 143 (1998).
  14. N. Garnier and A. Chiffauded, “Two dimensional hydrothermal waves in an extended cylindrical vessel,” Eur. Phys. J. B 19, 87 (2001).
  15. D. Schwabe, “Hydrothermal waves in a liquid bridge with aspect ratio near the Rayleigh limit under microgravity,” Phys. Fluids 17, 112104 (2005).
  16. V. M. Shevtsova, A. A. Nepomnyashchy, and J. C. Legros, “Thermocapillary-buoyancy convection in shallow cavity heated from the side,” Phys. Rev. E 67, 066308 (2003).
  17. S. Madruga, C. Perez-Garcia, and G. Lebon, “Convective instabilities in two superposed horizontal liquid layers heated laterally,” Phys. Rev. E 68, 041607 (2003).
  18. S. Madruga, C. Perez-Garcia, and G. Lebon, “Instabilities in two-liquid layers subject to a horizontal temperature gradient,” Theor. Comput. Fluid Dyn. 18, 277 (2004).
  19. A. Nepomnyashchy and I. Simanovskii, “Convective flows in a two-layer system with a temperature gradient along the interface,” Phys. Fluids 18, 032105 (2006).
  20. A. A. Nepomnyashchy, I. B. Simanovskii, and L. M. Braverman, “Stability of thermocapillary flows with inclined temperature gradient,” J. Fluid Mech. 442, 141 (2001).
  21. O. E. Shklyaev and A. A. Nepomnyashchy, “Thermocapillary flows under an inclined temperature gradient,” J. Fluid Mech. 504, 99 (2004).
  22. I. Ueno, T. Kurosawa, and H. Kawamura, “Thermocapillary convection in thin liquid layer with temperature gradient inclined to free surface,” Heat Transfer, Proceedings of the 12th International Heat Transfer Conference, Grenoble, France, 18–23 August 2002, (Elsevier, Amsterdam, 2002), pp. 129–133.
  23. D. A. Nield, “Surface tension and buoyancy effects in cellular convection,” J. Fluid Mech. 19, 341 (1964).
  24. D. Schwabe and J. Metzger, “Coupling and separation of buoyant and thermocapillary convection,” J. Cryst. Growth 97, 23 (1989).
  25. D. Schwabe and H. Dürr, “Holographic interferometry and flow visualization in an open rectangular gap,” Microgravity Sci. Technol. 9, 201 (1996).
  26. P. Hintz, D. Schwabe, and H. Wilke, “Convection in a Czochralski crucible—Part 1: Non-rotating crystal,” J. Cryst. Growth 222, 343 (2001).
  27. D. Schwabe, “Convective structures in complex systems with partly free surface,” J. Phys.: Conf. Ser. 64, 012001 (2007).
  28. B. Cockayne and M. B. Gates, “Growth striations in vertically pulled oxide and fluoride single crystals,” J. Mater. Sci. 2, 118 (1967).
  29. D. C. Miller, “The role of fluid flow phenomena in the Czochralski growth of oxides,” in Materials Processing in the Reduced Gravity of Space, edited by G. E. Rindone (North-Holland, New York, 1982), pp. 372–387.
  30. H. Kawamura, E. Tagaya, and Y. Hoshino, “A consideration on the relation between the oscillatory thermocapillary flow in a liquid bridge and the hydrothermal wave in a thin liquid layer,” Heat Mass Transfer 50, 1263 (2007).
  31. A. Sen and S. Davis, “Steady thermocapillary flows in two-dimensional slots,” J. Fluid Mech. 121, 163 (1982).
  32. E. L. Koschmieder and S. A. Prahl, “Surface-tension driven Bénard convection in small containers,” J. Fluid Mech. 215, 571 (1990).
  33. M. Schatz, S. Van Hook, W. McCormick, J. B. Swift, and H. Swinney, “Onset of surface-tension-driven Bénard convection,” Phys. Rev. Lett. 75, 1938 (1995).
  34. M. Schatz and P. Neitzel, “Experiments on thermocapillary instabilities,” Annu. Rev. Fluid Mech. 33, 93 (2001).
  35. Z. Zhu and Q. Liu, “Experimental investigation of thermocapillary convection in a liquid layer with evaporating interface,” Chin. Phys. Lett. 25, 4046 (2008).
  36. N. A. Ospennikov and D. Schwabe, “Thermocapillary flow without return flow-linear flow,” Exp. Fluids 36, 938 (2004).
  37. E. Scriven and C. V. Sternling, “On cellular convection driven by surface-tension gradients: Effects of mean surface tension and surface viscosity,” J. Fluid Mech. 19, 321 (1964).
  38. J. C. Loulergue, “Competition between Marangoni and Archimedian forces to determine the surface profile of a liquid heated open to air,” Lect. Notes Phys. 210, 358 (1984).
  39. P. Cerisier and G. Lebon, “Surface deflection in Bénard-Marangoni convection,” Lect. Notes Phys. 467, 117 (1996).
  40. A. Mizev, “Experimental investigation of thermocapillary convection induced by a local temperature inhomogeneity near the liquid surface. 1. Solid source of heat,” J. Appl. Mech. Tech. Phys. 45, 486 (2004).
  41. A. Mitchell, “Fundamental development in electron-beam melting processes,” in Proceedings of the Electron Beam Melting and Refining State of the Art 1997 Conference, Reno, Nevada, USA, 5–7 October 1997, edited by Bakish Materials Corporation, pp. 28–36.

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