2010
DOI: 10.1016/j.compchemeng.2009.08.004
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A simple numerical solution to the Ward–Tordai equation for the adsorption of non-ionic surfactants

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Cited by 55 publications
(39 citation statements)
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“…(40) is the analytical solution of the classical Ward and Tordai problem with the governing equation (18) in the sharp interface model, and it can be numerically solved with a given adsorption isotherm which relates the interface excess w 0 to w s [47].…”
Section: Adsorption Dynamicsmentioning
confidence: 99%
“…(40) is the analytical solution of the classical Ward and Tordai problem with the governing equation (18) in the sharp interface model, and it can be numerically solved with a given adsorption isotherm which relates the interface excess w 0 to w s [47].…”
Section: Adsorption Dynamicsmentioning
confidence: 99%
“…The Ward-Tordai diffusion model [9], subsequently developed as asymptotic solutions by Fainerman et al [40], and presented as a numerical solution by Li et al [41], describes how the adsorption kinetics of a non-ionic soluble surfactant is governed by a twostep process: (1) the diffusion of molecules from the bulk solution to the subsurface (i.e., the layer immediately below the surface layer, at a thickness of only a few molecular diameters); (2) the molecular diffusion and adsorption from the subsurface layer to the interface [4,5]. Thus, when, as in the ''interfacial areaexpansion method", a new clean surface is created and presented to a surfactant solution, a finite time is required for the excess surface concentration C(t) to reach equilibrium with the bulk concentration, C 0 , and attain its equilibrium value, C eq .…”
Section: Dynamic Behavior: the Ward-tordai Diffusion Modelmentioning
confidence: 99%
“…15,20 Tensiometry is widely used for both equilibrium and dynamic measurements but provides limited information on adsorption-desorption processes due to the predominance of diffusion at large scales. 13,[21][22][23] Deviations of the experimental data from the minimal diffusive-limited model introduced by Ward and Tordai are almost systematically observed, and attributed to curvature effects, [24][25][26][27] convective currents, 23,28,29 or adsorption barriers. 14,17 These adsorption barriers are revealed in the transfer-limited regimes which dominate at small dimensions 21,30 and in convective systems, 29,31 namely under the conditions relevant to emulsication or foaming.…”
Section: Introductionmentioning
confidence: 96%