Citation:
hampougny, L., Scheid, B., Korobkin, A. A., & Rodríguez-Rodríguez, J. (2021). Dip-coating flow in the presence of two immiscible liquids. Journal of Fluid Mechanics , 922, A26
xmlui.dri2xhtml.METS-1.0.item-contributor-funder:
Ministerio de Economía y Competitividad (España)
Sponsor:
L.C. acknowledges funding from the European Union's Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie grant agreement no. 882429. B.S. thanks the F.R.S-FNRS for financial support. A.A.K. thanks Universidad Carlos III de Madrid and Banco Santander for the financial support of his Chair of Excellence. J.R.-R. acknowledges the support of the Spanish Ministry of Economy and Competitiveness through grants DPI2017-88201-C3-3-R and DPI2018-102829-REDT, partly funded with European funds
Project:
Gobierno de España. DPI2017-88201-C3-3-R Gobierno de España. DPI2018-102829-REDT AT-2021
Dip coating is a common technique used to cover a solid surface with a thin liquid film,
the thickness of which was successfully predicted by the theory developed in the 1940s by
Landau & Levich (Acta Physicochem. URSS, vol. 17, 1942, pp. 141–153) and DerjagDip coating is a common technique used to cover a solid surface with a thin liquid film,
the thickness of which was successfully predicted by the theory developed in the 1940s by
Landau & Levich (Acta Physicochem. URSS, vol. 17, 1942, pp. 141–153) and Derjaguin
(Acta Physicochem. URSS, vol. 20, 1943, pp. 349–352). In this work, we present an
extension of their theory to the case where the dipping bath contains two immiscible
liquids, one lighter than the other, resulting in the entrainment of two thin films on the
substrate. We report how the thicknesses of the coated films depend on the capillary
number, on the ratios of the properties of the two liquids and on the relative thickness
of the upper fluid layer in the bath. We also show that the liquid/liquid and liquid/gas
interfaces evolve independently from each other as if only one liquid were coated, except
for a very small region where their separation falls quickly to its asymptotic value and
the shear stresses at the two interfaces peak. Interestingly, we find that the final coated
thicknesses are determined by the values of these maximum shear stresses.[+][-]