Hostname: page-component-586b7cd67f-rcrh6 Total loading time: 0 Render date: 2024-11-30T05:42:18.831Z Has data issue: false hasContentIssue false

Instability and symmetry breaking in binary evaporating thin films over a solid spherical dome

Published online by Cambridge University Press:  12 March 2021

Xingyi Shi
Affiliation:
Department of Chemical Engineering, Stanford University, Stanford, CA94305, USA
Mariana Rodríguez-Hakim
Affiliation:
Department of Chemical Engineering, Stanford University, Stanford, CA94305, USA Department of Materials, ETH Zürich, Vladimir-Prelog-Weg 5, 8093Zurich, Switzerland
Eric S.G. Shaqfeh*
Affiliation:
Department of Chemical Engineering, Stanford University, Stanford, CA94305, USA Department of Mechanical Engineering, Stanford University, Stanford, CA94305, USA
Gerald G. Fuller
Affiliation:
Department of Chemical Engineering, Stanford University, Stanford, CA94305, USA
*
Email address for correspondence: [email protected]

Abstract

We examine the axisymmetric and non-axisymmetric flows of thin fluid films over a spherical glass dome. A thin film is formed by raising a submerged dome through a silicone oil mixture composed of a volatile, low surface tension species (1 cSt, solvent) and a non-volatile species at a higher surface tension (5 cSt, initial solute volume fraction $\phi _0$). Evaporation of the 1 cSt silicone oil establishes a concentration gradient and, thus, a surface tension gradient that drives a Marangoni flow that leads to the formation of an initially axisymmetric mound. Experimentally, when $\phi _0 \leqslant 0.3\,\%$, the mound grows axisymmetrically for long times (Rodríguez-Hakim et al., Phys. Rev. Fluids, vol. 4, 2019, pp. 1–22), whereas when $\phi _0 \geqslant 0.35\,\%$, the mound discharges in a preferred direction, thereby breaking symmetry. Using lubrication theory and numerical solutions, we demonstrate that, under the right conditions, external disturbances can cause an imbalance between the Marangoni flow and the capillary flow, leading to symmetry breaking. In both experiments and simulations, we observe that (i) the apparent, most amplified disturbance has an azimuthal wavenumber of unity, and (ii) an enhanced Marangoni driving force (larger $\phi _0$) leads to an earlier onset of the instability. The linear stability analysis shows that capillarity and diffusion stabilize the system, while Marangoni driving forces contribute to the growth in the disturbances.

Type
JFM Papers
Copyright
© The Author(s), 2021. Published by Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

Balay, S., et al. . 2019 Petsc users manual. https://www.mcs.anl.gov/petscGoogle Scholar
Baldessari, F., Homsy, G.M. & Leal, L.G. 2007 Linear stability of a draining film squeezed between two approaching droplets. J. Colloid Interface Sci. 307 (1), 188202.CrossRefGoogle ScholarPubMed
Balestra, G., Badaoui, M., Ducimetière, Y. & Gallaire, F. 2019 Fingering instability on curved substrates: optimal initial film and substrate perturbations. J. Fluid Mech. 868, 726761.CrossRefGoogle Scholar
Balestra, G., Kofman, N., Brun, P.-T., Scheid, B. & Gallaire, F. 2017 Three-dimensional Rayleigh–Taylor instability under a unidirectional curved substrate. J. Fluid Mech. 837, 1947.CrossRefGoogle Scholar
Braun, R.J. 2012 Dynamics of the tear film. Annu. Rev. Fluid Mech. 44, 267297.CrossRefGoogle Scholar
Burrill, K.A. & Woods, D.R. 1973 Film shapes for deformable drops at liquid-liquid interfaces. II. The mechanisms of film drainage. J. Colloid Interface Sci. 42 (1), 1534.CrossRefGoogle Scholar
Chan, D.Y.C., Klaseboer, E. & Manica, R. 2011 Film drainage and coalescence between deformable drops and bubbles. Soft Matt. 7 (6), 22352264.CrossRefGoogle Scholar
Craster, R.V. & Matar, O.K. 2009 Dynamics and stability of thin liquid films. Rev. Mod. Phys. 81 (3), 11311198.CrossRefGoogle Scholar
Evans, D.E. & Sheehan, M.C. 2002 Don't be fobbed off: the substance of beer foam – a review. J. Am. Soc. Brew. Chem. 60 (2), 4757.Google Scholar
Fournier, J.B. & Cazabat, A.M. 1992 Tears of wine. Europhys. Lett. 20 (6), 517.CrossRefGoogle Scholar
Gumerman, R.J. & Homsy, G.M. 1975 The stability of radially bounded thin films. Chem. Engng Commun. 2 (1), 2736.CrossRefGoogle Scholar
Hosoi, A.E. & Bush, J.W.M. 2001 Evaporative instabilities in climbing films. J. Fluid Mech. 442, 217.CrossRefGoogle Scholar
Joye, J., Hirasaki, G.J. & Miller, C.A. 1994 Asymmetric drainage in foam films. Langmuir 10 (9), 31743179.CrossRefGoogle Scholar
Kannan, A., Shieh, I.C. & Fuller, G.G. 2019 Linking aggregation and interfacial properties in monoclonal antibody-surfactant formulations. J. Colloid Interface Sci. 550, 128138.CrossRefGoogle ScholarPubMed
Karakashev, S.I. & Manev, E.D. 2015 Hydrodynamics of thin liquid films: retrospective and perspectives. Adv. Colloid Interface Sci. 222, 398412.CrossRefGoogle Scholar
Kaur, S. & Leal, L.G. 2009 Three-dimensional stability of a thin film between two approaching drops. Phys. Fluids 21 (7), 072101.CrossRefGoogle Scholar
Lawrence, C.J. 1988 The mechanics of spin coating of polymer films. Phys. Fluids 31 (10), 27862795.CrossRefGoogle Scholar
Mohseni, K. & Colonius, T. 2000 Numerical treatment of polar coordinate singularities. J. Comput. Phys. 157 (2), 787795.CrossRefGoogle Scholar
Oron, A., Davis, S.H. & Bankoff, S.G. 1997 Long-scale evolution of thin liquid films. Rev. Mod. Phys. 69 (3), 931.CrossRefGoogle Scholar
Rabiah, N.I., Scales, C.W. & Fuller, G.G. 2019 The influence of protein deposition on contact lens tear film stability. Colloids Surf. B 180, 229236.CrossRefGoogle ScholarPubMed
Rodríguez-Hakim, M., Barakat, J.M., Shi, X., Shaqfeh, E.S.G. & Fuller, G.G. 2019 Evaporation-driven solutocapillary flow of thin liquid films over curved substrates. Phys. Rev. Fluids 4 (3), 122.CrossRefGoogle Scholar
Schmid, P.J. 2007 Nonmodal stability theory. Annu. Rev. Fluid Mech. 39, 129162.CrossRefGoogle Scholar
Shi, X., Fuller, G. & Shaqfeh, E. 2020 Oscillatory spontaneous dimpling in evaporating curved thin films. J. Fluid Mech. 889, A25.CrossRefGoogle Scholar
Takagi, D. & Huppert, H.E. 2010 Flow and instability of thin films on a cylinder and sphere. J. Fluid Mech. 647, 221.CrossRefGoogle Scholar
Velev, O.D., Constantinides, G.N., Avraam, D.G., Payatakes, A.C. & Borwankar, R.P. 1995 Investigation of thin liquid films of small diameters and high capillary pressures by a miniaturized cell. J. Colloid Interface Sci. 175 (1), 6876.CrossRefGoogle Scholar
Velev, O.D., Gurkov, T.D. & Borwankar, R.P. 1993 Spontaneous cyclic dimpling in emulsion films due to surfactant mass transfer between the phases. J. Colloid Interface Sci. 159, 497497.CrossRefGoogle Scholar
Venerus, D.C. & Simavilla, D.N. 2015 Tears of wine: new insights on an old phenomenon. Sci. Rep. 5, 16162.CrossRefGoogle Scholar
Walls, D.J., Meiburg, E. & Fuller, G.G. 2018 The shape evolution of liquid droplets in miscible environments. J. Fluid Mech. 852, 422452.CrossRefGoogle Scholar
Zdravkov, A.N., Peters, G.W.M. & Meijer, H.E.H. 2006 Film drainage and interfacial instabilities in polymeric systems with diffuse interfaces. J. Colloid Interface Sci. 296 (1), 8694.CrossRefGoogle ScholarPubMed