2006
DOI: 10.1209/epl/i2006-10160-3
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Slip-controlled thin-film dynamics

Abstract: PACS. 83.80.Sg -Polymer melts. PACS. 47.15.gm -Thin film flows. PACS. 83.50.Lh -Slip boundary effects (interfacial and free surface flows).Abstract. -In this study, we present a novel method to assess the slip length and the viscosity of thin films of highly viscous Newtonian liquids. We quantitatively analyse dewetting fronts of low molecular weight polystyrene melts on Octadecyl-(OTS) and Dodecyltrichlorosilane (DTS) polymer brushes. Using a thin film (lubrication) model derived in the limit of large slip le… Show more

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Cited by 58 publications
(67 citation statements)
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“…9,12 The enhancement of the depletion layer with temperature is also contrary to the temperature dependent reduction of slip length observed in polystyrene on OTS. 28 Accordingly, the enhancement of the depleted layer contradicts the amount of surface slip. Thus, in addition to slip lengths calculated via formula (3), which are orders of magnitude smaller than the reported literature values, the opposite trend of the depletion effect with interfacial energy we observe shows that the presence of a depletion layer alone cannot explain surface slippage of hexadecane.…”
Section: Discussionmentioning
confidence: 99%
“…9,12 The enhancement of the depletion layer with temperature is also contrary to the temperature dependent reduction of slip length observed in polystyrene on OTS. 28 Accordingly, the enhancement of the depleted layer contradicts the amount of surface slip. Thus, in addition to slip lengths calculated via formula (3), which are orders of magnitude smaller than the reported literature values, the opposite trend of the depletion effect with interfacial energy we observe shows that the presence of a depletion layer alone cannot explain surface slippage of hexadecane.…”
Section: Discussionmentioning
confidence: 99%
“…From the dynamics of hole growth 27,28,34-40 as well as from the shape of the liquid rim surrounding the hole one can get information about the slip or no-slip boundary condition of the liquid close to the solid substrate. 17,41,42 In the late stage, the straight ribbons that separate two coalescing holes decay into droplets due to the Rayleigh-Plateau instability, 43 c.f. Fig.…”
Section: Experimental Model Systems For Simple Liquidsmentioning
confidence: 99%
“…While the interface shape is monotonous at the bubble's advancing side, the thin film at the rear exhibits steady capillary waves, that are comoving with the bubble. The ripples are found in many other flow phenomena, for example in dip-coating processes, for both plunging and withdrawing plates (Wilson 1982;Snoeijer et al 2008;Maleki et al 2011), spreading droplets on a pre-wetted film (Tanner 1979;Tuck & Schwartz 1990;Cormier et al 2012;Bergemann et al 2018;Teisala et al 2018), dewetting fronts (Fetzer et al 2006;Snoeijer & Eggers 2010), and levelling of capillary films Salez et al 2012;Ilton et al 2016). Apart from their intrinsic interest, the ripples are important for establishing boundary conditions in coating problems (Bretherton 1961;Taroni et al 2012;Giavedoni & Saita 1999), and give rise to intricate bifurcation scenarios for the forced wetting transition (Ziegler et al 2009;Köpf & Thiele 2014;Lin et al 2016).…”
Section: Introductionmentioning
confidence: 99%