Export citation

Export citation

Choose format for download:

Download Citation
  • Access by Xinjiang University

Role of edge effects and fluid depth in azimuthal Faraday waves

P. Wilson1, X. Shao2, J. R. Saylor1, and J. B. Bostwick1,*

  • 1Department of Mechanical Engineering, Clemson University, Clemson, South Carolina 29634, USA
  • 2Department of Chemical and Biomolecular Engineering, Johns Hopkins University, Baltimore, Maryland 21218, USA

  • *jbostwi@clemson.edu

Phys. Rev. Fluids 7, 014803 – Published 24 January, 2022

DOI: https://doi.org/10.1103/PhysRevFluids.7.014803

Abstract

Faraday waves are created in experiment by mechanically vibrating a cylindrical container. Frequency scans are performed, and the acceleration threshold above which a surface wave appears is measured using a laser light approach, giving the instability tongue in frequency-acceleration space. The spatial structure of the surface wave, which conforms to the cylindrical container for wavelengths comparable to the container size, is determined using long-exposure-time white light imaging and is defined by the mode number pair (n,). Edge conditions at the container sidewall are controlled to create a (i) pinned or (ii) freely sliding contact-line. The driving frequency with the smallest threshold acceleration is identified as the natural frequency for that particular mode number pair. A theoretical model is developed using a viscous potential approximation to compute the natural oscillations of a viscoelastic material in a cylindrical container with a flat interface for both a pinned and a freely sliding contact-line. A closed-form expression is given for the freely sliding case, and a Rayleigh-Ritz procedure is used for the pinned case. The agreement is good between theoretical predictions and experimental observations for Triton/water mixtures, glycerol/water mixtures, and agarose gels, notwithstanding the large range in parameter space and the very different boundary conditions considered.

Physics Subject Headings (PhySH)

Article Text

References (68)

  1. M. Faraday, XVII. On a peculiar class of acoustical figures; and on certain forms assumed by groups of particles upon vibrating elastic surfaces, Philos. Trans. R. Soc. London 299 (1831).
  2. J. Miles and D. Henderson, Parametrically forced surface waves, Annu. Rev. Fluid Mech. 22, 143 (1990).
  3. M. Perlin and W. W. Schultz, Capillary effects on surface waves, Annu. Rev. Fluid Mech. 32, 241 (2000).
  4. A. James, B. Vukasinovic, M. K. Smith, and A. Glezer, Vibration-induced drop atomization and bursting, J. Fluid Mech. 476, 1 (2003).
  5. B. Vukasinovic, M. K. Smith, and A. Glezer, Dynamics of a sessile drop in forced vibration, J. Fluid Mech. 587, 395 (2007).
  6. C. S. Tsai, R. W. Mao, S. K. Lin, Y. Zhu, and S. C. Tsai, Faraday instability-based micro droplet ejection for inhalation drug delivery, Technology 02, 75 (2014).
  7. P. H. Wright and J. R. Saylor, Patterning of particulate films using Faraday waves, Rev. Sci. Instrum. 74, 4063 (2003).
  8. J. R. Saylor and A. L. Kinard, Simulation of particle deposition beneath Faraday waves in thin liquid films, Phys. Fluids 17, 047106 (2005).
  9. A. Briard, L. Gostiaux, and B.-J. Gréa, The turbulent Faraday instability in miscible fluids, J. Fluid Mech. 883, A57(2020).
  10. J. R. Saylor and R. A. Handler, Gas transport across an air/water interface populated with capillary waves, Phys. Fluids 9, 2529 (1997).
  11. J. R. Saylor and R. A. Handler, Capillary wave gas exchange in the presence of surfactants, Exp. Fluids 27, 332 (1999).
  12. J. R. Saylor, The rôle of capillary waves in oceanic air/water gas exchange, Tellus B: Chem. Phys. Meteorol. 51, 616 (1999).
  13. P. Chen, S. Güven, O. B. Usta, M. L. Yarmush, and U. Demirci, Biotunable acoustic node assembly of organoids, Adv. Healthcare Mater. 4, 1937 (2015).
  14. S. Guven, P. Chen, F. Inci, S. Tasoglu, B. Erkmen, and U. Demirci, Multiscale assembly for tissue engineering and regenerative medicine, Trends Biotechnol. 33, 269 (2015).
  15. S. V. Murphy and A. Atala, 3D bioprinting of tissues and organs, Nat. Biotechnol. 32, 773 (2014).
  16. R. Fan, M. Piou, E. Darling, D. Cormier, J. Sun, and J. Wan, Bio-printing cell-laden matrigel–agarose constructs, J. Biomater. Appl. 31, 684 (2016).
  17. B. Christiansen, P. Alstrom, and M. T. Levinsen, Ordered Capillary-Wave States: Quasicrystals, Hexagons, and Radial Waves, Phys. Rev. Lett. 68, 2157 (1992).
  18. K. Kumar and K. M. S. Bajaj, Competing patterns in the Faraday experiment, Phys. Rev. E 52, R4606 (1995).
  19. W. S. Edwards and S. Fauve, Patterns and quasi-patterns in the Faraday experiment, J. Fluid Mech. 278, 123 (1994).
  20. T. B. Benjamin and F. J. Ursell, The stability of the plane free surface of a liquid in vertical periodic motion, Proc. R. Soc. London, Ser. A 225, 505 (1954).
  21. K. Kumar, Linear theory of faraday instability in viscous liquids, Proc. R. Soc. London, Ser. A 452, 1113 (1996).
  22. H. W. Müller, H. Wittmer, C. Wagner, J. Albers, and K. Knorr, Analytic Stability Theory for Faraday Waves and the Observation of the Harmonic Surface Response, Phys. Rev. Lett. 78, 2357 (1997).
  23. S. Kumar, Parametrically driven surface waves in viscoelastic liquids, Phys. Fluids 11, 1970 (1999).
  24. C. Wagner, H. W. Müller, and K. Knorr, Faraday Waves on a Viscoelastic Liquid, Phys. Rev. Lett. 83, 308 (1999).
  25. D. Joseph, T. Funada, and J. Wang, Potential Flows of Viscous and Viscoelastic Liquids, Cambridge Aerospace Series (Cambridge University Press, Cambridge, 2007)
  26. X. Shao, G. Bevilacqua, P. Ciarletta, J. R. Saylor, and J. B. Bostwick, Experimental observation of Faraday waves in soft gels, Phys. Rev. E 102, 060602(R) (2020).
  27. T. G. Mezger, The Rheology Handbook: For Users of Rotational and Oscillatory Rheometers (Vincentz Network, Hannover, 2006).
  28. R. W. Style, A. Jagota, C.-Y. Hui, and E. R. Dufresne, Elastocapillarity: Surface tension and the mechanics of soft solids, Annu. Rev. Condens. Matter Phys. 8, 99 (2017).
  29. J. Bico, É. Reyssat, and B. Roman, Elastocapillarity: When surface tension deforms elastic solids, Annu. Rev. Fluid Mech. 50, 629 (2018).
  30. S. Douady and S. Fauve, Pattern selection in Faraday instability, Europhys. Lett. 6, 221 (1988).
  31. S. Douady, Experimental study of the Faraday instability, J. Fluid Mech. 221, 383 (1990).
  32. D. M. Henderson and J. W. Miles, Single-mode Faraday waves in small cylinders, J. Fluid Mech. 213, 95 (1990).
  33. D. M. Henderson and J. W. Miles, Faraday waves in 2:1 internal resonance, J. Fluid Mech. 222, 449 (1991).
  34. W. Batson, F. Zoueshtiagh, and R. Narayanan, The Faraday threshold in small cylinders and the sidewall non-ideality, J. Fluid Mech. 729, 496 (2013).
  35. K. Ward, F. Zoueshtiagh, and R. Narayanan, Faraday instability in double-interface fluid layers, Phys. Rev. Fluids 4, 043903 (2019).
  36. X. Shao, C. T. Gabbard, J. B. Bostwick, and J. R. Saylor, On the role of meniscus geometry in capillary wave generation, Exp. Fluids 62, 59 (2021).
  37. J. B. Bostwick and P. H. Steen, Capillary oscillations of a constrained liquid drop, Phys. Fluids 21, 032108 (2009).
  38. J. B. Bostwick and P. H. Steen, Static rivulet instabilities: varicose and sinuous modes, J. Fluid Mech. 837, 819 (2018).
  39. T. B. Benjamin and J. C. Scott, Gravity-capillary waves with edge constraints, J. Fluid Mech. 92, 241 (1979).
  40. J. Graham-Eagle, A new method for calculating eigenvalues with applications to gravity-capillary waves with edge constraints, in Mathematical Proceedings of the Cambridge Philosophical Society ( Cambridge University Press, Cambridge, 1983), Vol. 94, pp. 553–564.
  41. A. Prosperetti, Linear oscillations of constrained drops, bubbles, and plane liquid surfaces, Phys. Fluids 24, 032109 (2012).
  42. S. H. Davis, Moving contact lines and rivulet instabilities. Part 1. The static rivulet, J. Fluid Mech. 98, 225 (1980).
  43. D. V. Lyubimov, T. P. Lyubimova, and S. V. Shklyaev, Behavior of a drop on an oscillating solid plate, Phys. Fluids 18, 012101 (2006).
  44. J. B. Bostwick and P. H. Steen, Response of driven sessile drops with contact-line dissipation, Soft Matter 12, 8919 (2016).
  45. J. B. Bostwick and P. H. Steen, Stability of constrained capillary surfaces, Annu. Rev. Fluid Mech. 47, 539 (2015).
  46. X. Shao, P. Wilson, J. R. Saylor, and J. B. Bostwick, Surface wave pattern formation in a cylindrical container, J. Fluid Mech. 915, A19 (2021).
  47. K. Takamura, H. Fischer, and N. R. Morrow, Physical properties of aqueous glycerol solutions, J. Pet. Sci. Eng. 98–99, 50 (2012).
  48. Q. Jiang, Y. C. Chiew, and J. E. Valentini, Damping of cylindrical propagating capillary waves on monolayer-covered surfaces, Langmuir 8, 2747 (1992).
  49. J. R. Saylor, Internal reflection beneath capillary water waves: A method for measuring wave slope, Appl. Opt. 36, 1121 (1997).
  50. A. V. Kityk, J. Embs, V. V. Mekhonoshin, and C. Wagner, Spatiotemporal characterization of interfacial Faraday waves by means of a light absorption technique, Phys. Rev. E 72, 036209 (2005).
  51. F. Moisy, M. Rabaud, and K. Salsac, A synthetic Schlieren method for the measurement of the topography of a liquid surface, Exp. Fluids 46, 1021 (2009).
  52. S. L. Strickland, M. Shearer, and K. E. Daniels, Spatiotemporal measurement of surfactant distribution on gravity-capillary waves, J. Fluid Mech. 777, 523 (2015).
  53. H. Lamb, Hydrodynamics (Cambridge University Press, Cambridge, 1932).
  54. X. Shao, P. Wilson, J. B. Bostwick, and J. R. Saylor, Viscoelastic effects in circular edge waves, J. Fluid Mech. 919, A18 (2021).
  55. J. C. Padrino, T. Funada, and D. D. Joseph, Purely irrotational theories for the viscous effects on the oscillations of drops and bubbles, Int. J. Multiphase Flow 34, 61 (2008).
  56. J. L. Harden, H. Pleiner, and P. A. Pincus, Hydrodynamic surface modes on concentrated polymer solutions and gels, J. Chem. Phys. 94, 5208 (1991).
  57. M. Tokita and K. Hikichi, Mechanical studies of sol-gel transition: Universal behavior of elastic modulus, Phys. Rev. A 35, 4329 (1987).
  58. L. A. Segel, Mathematics Applied to Continuum Mechanics (Dover, New York, 1987).
  59. J. B. Bostwick and P. H. Steen, Coupled oscillations of deformable spherical-cap droplets. Part 1. Inviscid motions, J. Fluid Mech. 714, 312 (2013).
  60. J. B. Bostwick and P. H. Steen, Coupled oscillations of deformable spherical-cap droplets. Part 2. Viscous motions, J. Fluid Mech. 714, 336 (2013).
  61. D. M. Henderson and J. W. Miles, Surface-wave damping in a circular cylinder with a fixed contact line, J. Fluid Mech. 275, 285 (1994).
  62. J. A. Nicolás, The viscous damping of capillary-gravity waves in a brimful circular cylinder, Phys. Fluids 14, 1910 (2002).
  63. J. A. Nicolás, Effects of static contact angles on inviscid gravity-capillary waves, Phys. Fluids 17, 022101 (2005).
  64. R. Kidambi, Capillary damping of inviscid surface waves in a circular cylinder, J. Fluid Mech. 627, 323 (2009).
  65. R. Kidambi, Meniscus effects on the frequency and damping of capillary-gravity waves in a brimful circular cylinder, Wave Motion 46, 144 (2009).
  66. J. B. Bostwick and P. H. Steen, Dynamics of sessile drops. Part 1. Inviscid theory, J. Fluid Mech. 760, 5 (2014).
  67. C.-T. Chang, J. B. Bostwick, S. Daniel, and P. H. Steen, Dynamics of sessile drops. Part 2. Experiment, J. Fluid Mech. 768, 442 (2015).
  68. P. H. Steen, C.-T. Chang, and J. B. Bostwick, Droplet motions fill a periodic table, Proc. Natl. Acad. Sci. USA 116, 4849 (2019).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation