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在弱吸引表面附近的超临界流体中,从吸附到解吸的非单调转变。

Nonmonotonic crossover from adsorption to desorption in supercritical fluid near a weakly attractive surface.

作者信息

Oleinikova Alla, Brovchenko Ivan

机构信息

Physical Chemistry, Dortmund University of Technology, Otto-Hahn-Strasse 6, Dortmund, D-44227, Germany.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2008 Dec;78(6 Pt 1):061601. doi: 10.1103/PhysRevE.78.061601. Epub 2008 Dec 2.

Abstract

The density profiles of a supercritical Lennard-Jones fluid near a weakly attractive surface are used to study the excess adsorption Gamma of supercritical fluid in a wide density range. We report the observation of two extrema of Gamma along the isotherm as a function of density. The attractive fluid-wall interaction potential tends to make Gamma positive, whereas the missing neighbor effect tends to make Gamma negative. The latter effect enhances with increasing fluid density due to the growth of the fluid-fluid attraction that results in the crossover from adsorption to depletion (Gamma=0) at some particular fluid density. With approaching the critical point, Gamma decreases as the bulk correlation length and passes through a minimum when the average density of confined fluid is close to the bulk critical density. Variation of Gamma with temperature and density is determined by the monotonic trend from adsorption to desorption upon increasing fluid density and by the increase of the absolute value of Gamma when approaching the critical point. Interplay of these trends results in two extrema of Gamma in the temperature-density plane. This effect may be responsible for the crossover from adsorption to desorption with approaching the critical temperature observed experimentally along the isotherms and along the critical isochore. The density profiles of a supercritical fluid are found to be exponential and the power law behavior predicted theoretically was not detected even when the bulk correlation length xi achieves 11 molecular diameters.

摘要

利用超临界 Lennard-Jones 流体在弱吸引表面附近的密度分布,研究了超临界流体在很宽密度范围内的过量吸附量 Γ。我们报告了沿等温线观察到的 Γ 随密度变化的两个极值。流体-壁的吸引相互作用势倾向于使 Γ 为正,而缺失近邻效应倾向于使 Γ 为负。随着流体密度的增加,由于流体-流体吸引力的增长,后一种效应增强,导致在某个特定流体密度下从吸附转变为耗尽(Γ = 0)。随着接近临界点,Γ 随着体相关长度减小,并在受限流体的平均密度接近体临界密度时经过一个最小值。Γ 随温度和密度的变化由流体密度增加时从吸附到解吸的单调趋势以及接近临界点时 Γ 绝对值的增加所决定。这些趋势的相互作用导致在温度-密度平面上出现 Γ 的两个极值。这种效应可能是沿等温线和沿临界等容线实验观察到的随着接近临界温度从吸附到解吸转变的原因。发现超临界流体的密度分布是指数型的,即使体相关长度 ξ 达到 11 个分子直径,理论预测的幂律行为也未被检测到。

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