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Theoretical description of the adsorption and the wetting behavior of alkanes on water

机译:烷烃在水中的吸附和润湿行为的理论描述

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The wetting behavior of alkanes of medium chain length (e.g., pentane, hexane, and heptane) on water is more complex than the usually observed first-order wetting transition from partial to complete wetting by showing a sequence of two transitions. In this sequential-wetting scenario, a first-order transition from a microscopically thin to a mesoscopically thick layer of liquid on the substrate surface is followed by a continuous divergence of the film thickness upon increase of the temperature. This critical transition to complete wetting at T-w,T-c is solely determined by long-range interactions between substrate and adsorbate, which are well-described by Dzyaloshinskii-Lifshitz-Pitaevskii [Adv. Phys. 10, 165 (1961)] theory in terms of the static dielectric constants and the refractive indices of the media involved. The first-order thin-thick transition, however, which occurs at a lower temperature T-w,T-1, results from an interplay of short-range and long-range forces and is notoriously more difficult to describe because a satisfactory theory of the short-range interactions between substrate and adsorbate is still missing. The approach presented in this paper attempts to account for the short-range interactions in an effective way: Within a Cahn-type [J. Chem. Phys. 66, 3667 (1977)] theory that has been augmented for long-range interactions and modified to treat the first layer of adsorbed molecules in a lattice-gas approach, the contact energy is deduced from the surface pressure, which in turn is calculated using a two-dimensional van der Waals equation of state and an expression for the Henry's law constant that was derived by Hirasaki [J. Adhes. Sci. Technol. 7, 285 (1993)]. The method uses only the dielectric properties of the isolated bulk media and simple assumptions on the size and the shape of the adsorbed alkane molecules and leads to satisfactory results for the transition temperatures T-w,T-1 and T-w,T-c. (c) 2006 American Institute of Physics.
机译:中链长度的烷烃(例如戊烷,己烷和庚烷)在水上的润湿行为比通常观察到的从部分润湿到完全润湿的一阶润湿转变要复杂得多,这是通过显示两个过渡序列来实现的。在这种顺序润湿的情况下,从基体表面上的液体的微观层到介观层的第一层过渡是随着温度的升高薄膜厚度连续发散。在T-w,T-c处完成润湿的这一关键转变完全取决于底物和被吸附物之间的远程相互作用,Dzyaloshinskii-Lifshitz-Pitaevskii对此进行了充分描述[Adv。物理10,165(1961)]理论上涉及静态介电常数和所涉及介质的折射率。然而,一阶薄厚度转变发生在较低的温度Tw,T-1上,是由于短程和长程力的相互作用而产生的,并且由于难以令人满意地描述了短程理论,因此更难以描述底物和被吸附物之间的高范围相互作用仍然缺失。本文提出的方法试图以一种有效的方式解释短程相互作用:在Cahn型内[J.化学物理[66,3667(1977)]理论已经得到增强,可以进行长距离相互作用,并经过改进以处理晶格气体方法中的第一层吸附分子,其接触能从表面压力中推导出来,而表面压力又可以通过使用Hirasaki推导的二维范德华状态方程和亨利定律的表达式[J.胶粘剂。科学技术。 7,285(1993)]。该方法仅使用了分离的块状介质的介电特性,并且对吸附的烷烃分子的大小和形状进行了简单假设,从而得出了转变温度T-w,T-1和T-w,T-c令人满意的结果。 (c)2006年美国物理研究所。

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