TY - JOUR
T1 - Slip-induced suppression of Marangoni film thickening in surfactant-retarded Landau-Levich-Bretherton flows
AU - Halpern, David
AU - Li, Yen Ching
AU - Wei, Hsien Hung
N1 - Publisher Copyright:
© 2015 Cambridge University Press.
PY - 2015/10/25
Y1 - 2015/10/25
N2 - We report that the well-known Marangoni film thickening in surfactant-laden Landau-Levich-Bretherton coating flow can be completely suppressed by wall slip. The analysis is made by mainly looking at how the deposited film thickness varies with the capillary number and the dimensionless slip length in the presence of a trace amount of insoluble surfactant, where is the slip length and is the radius of the meniscus. When slip effects are weak at sufficiently large (but still ) such that , the film thickness can still vary as and be thickened by surfactant as if wall slip were absent. However, when slip effects become strong by lowering to , the film, especially when surface diffusion of surfactant is negligible, does not get thinner according to the strong-slip quadratic law reported previously (Liao et al., Phys. Rev. Lett., vol. 111, 2013, 136001; Li et al., J. Fluid Mech., vol. 741, 2014, pp. 200-227). Instead, the film behaves as if both surfactant and wall slip were absent, precisely following the no-slip law without surfactant. Effects of surface diffusion are also examined, revealing three distinct regimes as is varied from small to large values: the strong-slip quadratic scaling without surfactant, the no-slip scaling without surfactant and the film thickening along the no-slip scaling with surfactant. An experiment is also suggested to test the above findings.
AB - We report that the well-known Marangoni film thickening in surfactant-laden Landau-Levich-Bretherton coating flow can be completely suppressed by wall slip. The analysis is made by mainly looking at how the deposited film thickness varies with the capillary number and the dimensionless slip length in the presence of a trace amount of insoluble surfactant, where is the slip length and is the radius of the meniscus. When slip effects are weak at sufficiently large (but still ) such that , the film thickness can still vary as and be thickened by surfactant as if wall slip were absent. However, when slip effects become strong by lowering to , the film, especially when surface diffusion of surfactant is negligible, does not get thinner according to the strong-slip quadratic law reported previously (Liao et al., Phys. Rev. Lett., vol. 111, 2013, 136001; Li et al., J. Fluid Mech., vol. 741, 2014, pp. 200-227). Instead, the film behaves as if both surfactant and wall slip were absent, precisely following the no-slip law without surfactant. Effects of surface diffusion are also examined, revealing three distinct regimes as is varied from small to large values: the strong-slip quadratic scaling without surfactant, the no-slip scaling without surfactant and the film thickening along the no-slip scaling with surfactant. An experiment is also suggested to test the above findings.
UR - http://www.scopus.com/inward/record.url?scp=84959010783&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84959010783&partnerID=8YFLogxK
U2 - 10.1017/jfm.2015.508
DO - 10.1017/jfm.2015.508
M3 - Article
AN - SCOPUS:84959010783
SN - 0022-1120
VL - 781
SP - 578
EP - 594
JO - Journal of Fluid Mechanics
JF - Journal of Fluid Mechanics
ER -