Do D D, Do H D
School of Engineering, University of Queensland, St Lucia, QLD 4072, Australia.
J Colloid Interface Sci. 2007 Dec 15;316(2):317-30. doi: 10.1016/j.jcis.2007.08.020. Epub 2007 Aug 14.
In adsorption studies the choice of an appropriate void volume in the calculation of the adsorption isotherm is very crucial. It is often taken to be the apparent volume as determined by the helium expansion experiments. Unfortunately this method has difficulties especially when dealing with microporous solids, in which adsorption of helium might become significant at ambient temperatures. The amount adsorbed is traditionally obtained as the excess amount and the term "excess" refers to the excess over the amount occupying the apparent volume that has the same density as the bulk gas density. This could give rise to the maximum in the plot of excess amount versus pressure under supercritical conditions, and in some cases giving negative excess. Such behavior is difficult to analyze because the excess amount is not amenable to any classical thermodynamic treatments. In this paper we will present a method to determine the absolute void volume, and in that sense this volume is independent of temperature and adsorbate. The volume that is accessible to the centers of gas molecules is also investigated, and it is called the accessible volume. This volume depends on the choice of adsorbate, and it is appropriate to use this volume to calculate the pore density because we can assess how dense the adsorbed phase is. In the quest to determine the "absolute" adsorption isotherm so that a thermodynamics analysis can be applied, it is necessary to introduce the concept of "enclosing" volume, which is essentially the volume that encloses all solid particles, including all void spaces in them. The amount adsorbed is defined by the number of molecules residing in this volume. Having these volumes, we can derive the geometrical accessible void volume inside the particle and the solid volume, from which the particle and solid densities can be calculated.
在吸附研究中,在计算吸附等温线时选择合适的空体积至关重要。通常将其视为由氦气膨胀实验确定的表观体积。不幸的是,这种方法存在困难,特别是在处理微孔固体时,在环境温度下氦气的吸附可能会变得显著。传统上,吸附量是作为过量吸附量获得的,术语“过量”是指超过占据表观体积且具有与本体气体密度相同密度的量。这可能导致在超临界条件下过量吸附量与压力的关系图中出现最大值,并且在某些情况下会出现负的过量吸附量。这种行为难以分析,因为过量吸附量不适合任何经典的热力学处理方法。在本文中,我们将提出一种确定绝对空体积的方法,从这个意义上说,该体积与温度和吸附质无关。还研究了气体分子中心可及的体积,称为可及体积。该体积取决于吸附质的选择,使用该体积来计算孔密度是合适的,因为我们可以评估吸附相的密度。在寻求确定“绝对”吸附等温线以便能够应用热力学分析时,有必要引入“包封”体积的概念,它本质上是包围所有固体颗粒的体积,包括其中的所有空隙空间。吸附量由存在于该体积中的分子数定义。有了这些体积,我们可以推导出颗粒内部的几何可及空体积和固体体积,由此可以计算颗粒密度和固体密度。