Abstract:Experimental values of the wave length and wave velocity have been obtained far dilute sohtions of valeric and hexanoic acid for a vertical fulling liquid film. The wave length was unaffected by the surfactants for Reynolds numbers in the range 5 to 100; however, the wave velocity was decreased for increased surface concentrations of the two acids. This is in direct contradiction to previous theoretical work, and the explanation for the anomaly is that the free surface velocity is greatly retarded by the adsor… Show more
“…Finally, figure 9(d) presents the wave velocity of the marginally unstable mode at neutral stability as a function of the wavenumber and for different amounts of surfactant. In agreement with previous experimental and theoretical studies (Strobel & Whitaker 1969;Cerro & Whitaker 1971), we find that the addition of surfactant decreases the wave velocity, and more so the higher the wavenumber. It is also notable that the variation with M tot is strictly monotonic, reaching an asymptotic limit for high surfactant concentrations.…”
Section: Effect Of the Total Amount Of Surfactantsupporting
confidence: 93%
“…The theoretical results by Whitaker (1964) also suggested that the wave velocity should increase with increasing elasticity of the interface. However, the experimental work of Strobel & Whitaker (1969) indicated that the free-surface velocity actually decreases for increased surfactant concentration and this was later confirmed experimentally and theoretically by Cerro & Whitaker (1971). The latter work also noted that surface velocity depends strongly on the surface elasticity and is only mildly affected by surfactant diffusivity and interfacial mass transport.…”
We investigate the linear stability of a film flowing down a solid substrate in the presence of soluble surfactants. The Navier–Stokes equations for the liquid motion are considered, together with advection–diffusion equations for the concentrations of the species involved, which include monomers dissolved in the bulk and adsorbed at the liquid–air and at the liquid–substrate interfaces. The adsorption–desorption kinetics of the surfactant at both interfaces is explicitly accounted for. An Orr–Sommerfeld eigenvalue problem is formulated, and solved analytically in the limit of long-wave disturbances and numerically for arbitrary wavelength using a finite element method. An extensive parametric study is performed to reveal the role of surfactant solubility and adsorption–desorption kinetics. The results quantify the stabilizing effect of soluble surfactants due to the presence of Marangoni stresses, and indicate that moderately soluble surfactants may be more effective than insoluble ones. Disturbances of finite wavelength are stabilized by more than an order of magnitude, and their detailed behaviour depends in a non-monotonic way on the amount of surfactant and on its solubility and kinetics. The above predictions provide insights for the interpretation of recent experimental findings on the primary instability and on the ensuing unstable dynamics of liquid films doped with soluble surfactants.
“…Finally, figure 9(d) presents the wave velocity of the marginally unstable mode at neutral stability as a function of the wavenumber and for different amounts of surfactant. In agreement with previous experimental and theoretical studies (Strobel & Whitaker 1969;Cerro & Whitaker 1971), we find that the addition of surfactant decreases the wave velocity, and more so the higher the wavenumber. It is also notable that the variation with M tot is strictly monotonic, reaching an asymptotic limit for high surfactant concentrations.…”
Section: Effect Of the Total Amount Of Surfactantsupporting
confidence: 93%
“…The theoretical results by Whitaker (1964) also suggested that the wave velocity should increase with increasing elasticity of the interface. However, the experimental work of Strobel & Whitaker (1969) indicated that the free-surface velocity actually decreases for increased surfactant concentration and this was later confirmed experimentally and theoretically by Cerro & Whitaker (1971). The latter work also noted that surface velocity depends strongly on the surface elasticity and is only mildly affected by surfactant diffusivity and interfacial mass transport.…”
We investigate the linear stability of a film flowing down a solid substrate in the presence of soluble surfactants. The Navier–Stokes equations for the liquid motion are considered, together with advection–diffusion equations for the concentrations of the species involved, which include monomers dissolved in the bulk and adsorbed at the liquid–air and at the liquid–substrate interfaces. The adsorption–desorption kinetics of the surfactant at both interfaces is explicitly accounted for. An Orr–Sommerfeld eigenvalue problem is formulated, and solved analytically in the limit of long-wave disturbances and numerically for arbitrary wavelength using a finite element method. An extensive parametric study is performed to reveal the role of surfactant solubility and adsorption–desorption kinetics. The results quantify the stabilizing effect of soluble surfactants due to the presence of Marangoni stresses, and indicate that moderately soluble surfactants may be more effective than insoluble ones. Disturbances of finite wavelength are stabilized by more than an order of magnitude, and their detailed behaviour depends in a non-monotonic way on the amount of surfactant and on its solubility and kinetics. The above predictions provide insights for the interpretation of recent experimental findings on the primary instability and on the ensuing unstable dynamics of liquid films doped with soluble surfactants.
“…Since then, the flow in falling liquid films has been studied extensively through experimental measurements [10,45], low-dimensional modelling [46,47], and full numerical simulations [48]. The effects of many factors that influence the flow in falling films have been investigated, such as the effects of thermocapillarity [49], electric fields [50,51], and surfactants [52,53]. Different processes that may be involved in falling films have also been studied, such as heat transfer [54], mass transfer [55], chemical reactions [56], and phase change [57].…”
The impact of droplets on an inclined falling liquid film is studied experimentally using highspeed imaging. The falling film is created on a flat substrate with controllable thicknesses and flow rates. Droplets with different sizes and speeds are used to study the impact process under various Ohnesorge and Weber numbers, and film Reynolds numbers. A number of phenomena associated with droplet impact are identified and analysed, such as bouncing, partial coalescence, total coalescence, and splashing. The effects of droplet size, speed, as well the film flow rate are studied culminating in the generation of an impact regime map. The analysis of the lubrication force acted on the droplet via the gas layer shows that a higher flow rate in the liquid film produces a larger lubrication force, slows down the drainage process, and increases the probability of droplet bouncing. Our results demonstrate that the flowing film has a profound effect on the droplet impact process and associated phenomena, which are markedly more complex than those accompanying impact on initially quiescent films.
“…This result for the critical Reynolds number associated with insoluble surfactants has also been presented by Benjamin (1964) and by Anshus and Acrivos (1967). It was used originally by Strobel and Whitaker (1969) to estimate surface elasticities from wave inception line data, and more recently by Cerro and Whitaker (1971).…”
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