Adsorption in Slit Pores and Pore-Size Distribution: A Molecular Layer Structure

Anew approach is developed to analyze the thermodynamic properties of a sub-critical fluid adsorbed in a slit pore of activated carbon. The approach is based on a representation that an adsorbed fluid forms an ordered structure close to a smoothed solid surface. This ordered structure is modelled as...

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Main Authors: E.A. Ustinov, D.D. Do
Format: Article
Language:English
Published: SAGE Publications 2006-02-01
Series:Adsorption Science & Technology
Online Access:https://doi.org/10.1260/026361706778062531
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author E.A. Ustinov
D.D. Do
author_facet E.A. Ustinov
D.D. Do
author_sort E.A. Ustinov
collection DOAJ
description Anew approach is developed to analyze the thermodynamic properties of a sub-critical fluid adsorbed in a slit pore of activated carbon. The approach is based on a representation that an adsorbed fluid forms an ordered structure close to a smoothed solid surface. This ordered structure is modelled as a collection of parallel molecular layers. Such a structure allows us to express the Helmholtz free energy of a molecular layer as the sum of the intrinsic Helmholtz free energy specific to that layer and the potential energy of interaction of that layer with all other layers and the solid surface. The intrinsic Helmholtz free energy of a molecular layer is a function (at given temperature) of its two-dimensional density and it can be readily obtained from bulk-phase properties, while the interlayer potential energy interaction is determined by using the 10–4 Lennard-Jones potential. The positions of all layers close to the graphite surface or in a slit pore are considered to correspond to the minimum of the potential energy of the system. This model has led to accurate predictions of nitrogen and argon adsorption on carbon black at their normal boiling points. In the case of adsorption in slit pores, local isotherms are determined from the minimization of the grand potential. The model provides a reasonable description of the 0–1 monolayer transition, phase transition and packing effect. The adsorption of nitrogen at 77.35 K and argon at 87.29 K on activated carbons is analyzed to illustrate the potential of this theory, and the derived pore-size distribution is compared favourably with that obtained by the Density Functional Theory (DFT). The model is less time-consuming than methods such as the DFT and Monte-Carlo simulation, and most importantly it can be readily extended to the adsorption of mixtures and capillary condensation phenomena.
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spelling doaj.art-a26a32a54ff84541b6f2802d0bf58e342024-03-02T00:26:32ZengSAGE PublicationsAdsorption Science & Technology0263-61742048-40382006-02-012410.1260/026361706778062531Adsorption in Slit Pores and Pore-Size Distribution: A Molecular Layer StructureE.A. UstinovD.D. DoAnew approach is developed to analyze the thermodynamic properties of a sub-critical fluid adsorbed in a slit pore of activated carbon. The approach is based on a representation that an adsorbed fluid forms an ordered structure close to a smoothed solid surface. This ordered structure is modelled as a collection of parallel molecular layers. Such a structure allows us to express the Helmholtz free energy of a molecular layer as the sum of the intrinsic Helmholtz free energy specific to that layer and the potential energy of interaction of that layer with all other layers and the solid surface. The intrinsic Helmholtz free energy of a molecular layer is a function (at given temperature) of its two-dimensional density and it can be readily obtained from bulk-phase properties, while the interlayer potential energy interaction is determined by using the 10–4 Lennard-Jones potential. The positions of all layers close to the graphite surface or in a slit pore are considered to correspond to the minimum of the potential energy of the system. This model has led to accurate predictions of nitrogen and argon adsorption on carbon black at their normal boiling points. In the case of adsorption in slit pores, local isotherms are determined from the minimization of the grand potential. The model provides a reasonable description of the 0–1 monolayer transition, phase transition and packing effect. The adsorption of nitrogen at 77.35 K and argon at 87.29 K on activated carbons is analyzed to illustrate the potential of this theory, and the derived pore-size distribution is compared favourably with that obtained by the Density Functional Theory (DFT). The model is less time-consuming than methods such as the DFT and Monte-Carlo simulation, and most importantly it can be readily extended to the adsorption of mixtures and capillary condensation phenomena.https://doi.org/10.1260/026361706778062531
spellingShingle E.A. Ustinov
D.D. Do
Adsorption in Slit Pores and Pore-Size Distribution: A Molecular Layer Structure
Adsorption Science & Technology
title Adsorption in Slit Pores and Pore-Size Distribution: A Molecular Layer Structure
title_full Adsorption in Slit Pores and Pore-Size Distribution: A Molecular Layer Structure
title_fullStr Adsorption in Slit Pores and Pore-Size Distribution: A Molecular Layer Structure
title_full_unstemmed Adsorption in Slit Pores and Pore-Size Distribution: A Molecular Layer Structure
title_short Adsorption in Slit Pores and Pore-Size Distribution: A Molecular Layer Structure
title_sort adsorption in slit pores and pore size distribution a molecular layer structure
url https://doi.org/10.1260/026361706778062531
work_keys_str_mv AT eaustinov adsorptioninslitporesandporesizedistributionamolecularlayerstructure
AT dddo adsorptioninslitporesandporesizedistributionamolecularlayerstructure