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首页> 外文期刊>Colloids and Surfaces, A. Physicochemical and Engineering Aspects >Influence of adsorption kinetics and bubble motion on stability of the foam films formed at n-octanol, n-hexanol and n-butanol solution surface
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Influence of adsorption kinetics and bubble motion on stability of the foam films formed at n-octanol, n-hexanol and n-butanol solution surface

机译:吸附动力学和气泡运动对在正辛醇,正己醇和正丁醇溶液表面形成的泡沫膜稳定性的影响

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Lifetimes of single bubbles at surface of n-octanol solutions of various concentrations were determined for two different locations of the surface in respect to the capillary orifice at which the bubbles were formed. It was found that when solution surface was located 'far' (L = 39.5 cm) the average lifetimes of bubbles were shorter than that ones at the solution surface located 'close' (L = 4 cm) to the point of the bubbles formation. The bubble departing from the capillary orifice has the adsorption coverage determined by the mutual ratio of velocity of its formation and kinetics of surfactant adsorption. The degree of surfactant coverage over the surface of the growing bubble was calculated assuming that the surfactant adsorption at the surface of the departing bubble is governed by convective-diffusion. It was demonstrated that for the time of bubble growth t(growth) = 0. 16 s encountered in our experiments the departing bubbles had practically equilibrium coverage's in n-butanol and n-hexanol solutions, while in n-octanol solutions the adsorption coverage was much smaller than the equilibrium one. Thus, unlike for shorter chain n-alkanols, even for the location 'close' the partially non-symmetrical film is formed when in n-octanol solutions the bubble arrives at the free solution surface. For the location 'far', the bubble motion through the solution causes further disequilibration of the surfactant coverage over its surface. The bubble reaches the solution surface with its upstream pole practically devoid of surfactant and the fully non-symmetrical film is formed. Such fully non-symmetrical film is less stable than the film formed at the location 'close'. Our results show that the lifetime of the foam film formed by a single bubble arriving at the solution surface strongly depends on 'history' of the bubble formation and motion. (C) 2001 Elsevier Science B.V. All rights reserved. [References: 31]
机译:对于表面上相对于形成气泡的毛细管孔的两个不同位置,确定了各种浓度的正辛醇溶液表面的单个气泡的寿命。已经发现,当溶液表面位于“远”(L = 39.5 cm)时,气泡的平均寿命要短于位于溶液表面“接近”(L = 4 cm)的气泡的平均寿命。离开毛细管孔的气泡的吸附覆盖率取决于其形成速度与表面活性剂吸附动力学的比值。假设表面活性剂在离去的气泡表面上的吸附受对流扩散控制,则计算表面活性剂在生长的气泡表面上的覆盖程度。结果表明,在气泡生长时间t(growth)= 0。16 s的实验中,在正丁醇和正己醇溶液中,离去的气泡实际上具有平衡覆盖度,而在正辛醇溶液中,吸附覆盖度为比平衡状态小得多。因此,与较短链的正链烷醇不同,即使是在“封闭”位置,当气泡在正辛醇溶液中到达游离溶液表面时,也会形成部分不对称的薄膜。对于“远”位置,气泡通过溶液的运动导致表面活性剂在其表面上的覆盖范围进一步失衡。气泡以其上游极几乎没有表面活性剂到达溶液表面,并形成了完全不对称的膜。这种完全不对称的膜比在“闭合”位置形成的膜不稳定。我们的结果表明,由单个气泡到达溶液表面形成的泡沫膜的寿命在很大程度上取决于气泡形成和运动的“历史”。 (C)2001 Elsevier Science B.V.保留所有权利。 [参考:31]

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