On the anatomy of the adsorption heat versus loading as a function of temperature and adsorbate for a graphitic surface

• Published in: Journal of colloid and interface science Vol. 325; no. 1; pp. 7 - 22
• Main Authors: Do, D.D., Nicholson, D., Do, H.D.
• Format: Journal Article
• Language: English
• Published: San Diego, CA Elsevier Inc 01-09-2008; Elsevier
• Subjects: 2D-phase transition; Adsorption; Chemistry; Colloidal state and disperse state; Exact sciences and technology; GCMC simulation; General and physical chemistry; Graphite; Isosteric heat; Surface physical chemistry; GCMC simulation; 2D-phase transition; Adsorption; Graphite; Isosteric heat; Water; Critical property; Monolayer; Support; Hydrogen; Entropy; Critical point; Review; Condensation; Phase transitions; Solid; Particle; Association; Energy; Fluid fluid; Classification; Adsorption;Isosteric heat;Graphite;GCMC simulation;2D-phase transition; Alkanol; Methanol; Attraction; Carbon black; Xenon; Orientation; Drop; Ammonia; Gases; Simulation; Benzene; Thermodynamic properties
• ISSN: 0021-9797; 1095-7103
• DOI: 10.1016/j.jcis.2008.05.027

In this paper we review and classify the various patterns of isosteric heat versus loading for adsorption of gases on graphitised thermal carbon black at temperatures ranging from below the 3D triple point to temperatures above it, but less than the 3D critical point. We have identified the features of heat curve and highlighted the microscopic origin of these features. The patterns vary with temperature and with the relative strength of the fluid–fluid interaction and solid–fluid interaction. For simple adsorptives (by simple we meant there is no strong association between fluid particles), the heat curve is typified by fluid–fluid attraction and layering phenomena. For adsorptives showing strong association such as water, ammonia and methanol, the heat curve essentially begins below the condensation heat and then approaches it as loading is increased. This is mainly due to the strong hydrogen bonding in these fluids. A third group includes adsorptives such as benzene, where the heat curve is constant in the sub-monolayer coverage region (but is higher than the condensation heat) and then drops off to the condensation heat when higher layers are formed. The constant heat in the sub-monolayer region is due to the balance between the energy factor (from fluid–fluid interaction) and entropy factor (due to re-orientation of adsorbed molecules). Our proposed classification is supported by detailed GCMC simulations of various gases that have been reported in the literature, and we supplement these with new results for the adsorption of xenon on graphite to investigate in more detail the change in heat pattern with temperature. Xenon is chosen because of its high fluid–fluid interaction, allowing us to study the 2D-phase transition in the first as well as higher layers.
Pattern of isosteric heat versus loading for adsorption of xenon on graphite at 90 K.