Using a New Finite Slit Pore Model for NLDFT Analysis of Carbon Pore Structure

In this work, we present a model for analyzing activated carbon micropore structures based on graphene sheet walls of finite thickness and extent. This is a two-dimensional modification of the widely used infinite slit pore model that assumes graphite-like infinitely extended pore walls. The propose...

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Main Authors: Jacek Jagiello, Jeffrey Kenvin, James P. Olivier, Andrew R. Lupini, Cristian I. Contescu
Format: Article
Language:English
Published: SAGE Publishing 2011-08-01
Series:Adsorption Science & Technology
Online Access:https://doi.org/10.1260/0263-6174.29.8.769
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author Jacek Jagiello
Jeffrey Kenvin
James P. Olivier
Andrew R. Lupini
Cristian I. Contescu
author_facet Jacek Jagiello
Jeffrey Kenvin
James P. Olivier
Andrew R. Lupini
Cristian I. Contescu
author_sort Jacek Jagiello
collection DOAJ
description In this work, we present a model for analyzing activated carbon micropore structures based on graphene sheet walls of finite thickness and extent. This is a two-dimensional modification of the widely used infinite slit pore model that assumes graphite-like infinitely extended pore walls. The proposed model has two versions: (1) a strip pore constructed with graphene strip walls that have a finite length L in the x-direction and are infinite in the y-direction. Strip pores are open on both sides in the x-direction; (2) a channel pore, i.e. a strip pore partially closed along one edge by a perpendicularly orientated graphene wall. This more realistic model allows pore termination via both physical pore entrances and pore blockage. The model consequently introduces heterogeneity of the adsorption potential that is reduced near pore entrances and enhanced near the corners of pore walls. These energetically heterogeneous structures fill with adsorbate more gradually than homogeneous pores of the same width. As a result, the calculated adsorption isotherms are smoother and less steep for the finite versus the infinite pore model. In the application of this model for carbon characterization, it is necessary to make an assumption about the pore length. In this work, we made this assumption based on high-resolution scanning transmission electron microscopy (STEM) results. We find the agreement between the experiment and the model significantly better for the finite than for the infinite pore model.
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spelling doaj-art-9903bcd8edc440a491ef31babfd5ece42025-02-03T10:07:33ZengSAGE PublishingAdsorption Science & Technology0263-61742048-40382011-08-012910.1260/0263-6174.29.8.769Using a New Finite Slit Pore Model for NLDFT Analysis of Carbon Pore StructureJacek Jagiello0Jeffrey Kenvin1James P. Olivier2Andrew R. Lupini3Cristian I. Contescu4 Micromeritics Instrument Corporation, 4356 Communications Drive, Norcross, GA 30093, U.S.A. Micromeritics Instrument Corporation, 4356 Communications Drive, Norcross, GA 30093, U.S.A. Micromeritics Instrument Corporation, 4356 Communications Drive, Norcross, GA 30093, U.S.A. Division of Materials Science and Technology, Oak Ridge National Laboratory, Oak Ridge, TN 37831, U.S.A. Division of Materials Science and Technology, Oak Ridge National Laboratory, Oak Ridge, TN 37831, U.S.A.In this work, we present a model for analyzing activated carbon micropore structures based on graphene sheet walls of finite thickness and extent. This is a two-dimensional modification of the widely used infinite slit pore model that assumes graphite-like infinitely extended pore walls. The proposed model has two versions: (1) a strip pore constructed with graphene strip walls that have a finite length L in the x-direction and are infinite in the y-direction. Strip pores are open on both sides in the x-direction; (2) a channel pore, i.e. a strip pore partially closed along one edge by a perpendicularly orientated graphene wall. This more realistic model allows pore termination via both physical pore entrances and pore blockage. The model consequently introduces heterogeneity of the adsorption potential that is reduced near pore entrances and enhanced near the corners of pore walls. These energetically heterogeneous structures fill with adsorbate more gradually than homogeneous pores of the same width. As a result, the calculated adsorption isotherms are smoother and less steep for the finite versus the infinite pore model. In the application of this model for carbon characterization, it is necessary to make an assumption about the pore length. In this work, we made this assumption based on high-resolution scanning transmission electron microscopy (STEM) results. We find the agreement between the experiment and the model significantly better for the finite than for the infinite pore model.https://doi.org/10.1260/0263-6174.29.8.769
spellingShingle Jacek Jagiello
Jeffrey Kenvin
James P. Olivier
Andrew R. Lupini
Cristian I. Contescu
Using a New Finite Slit Pore Model for NLDFT Analysis of Carbon Pore Structure
Adsorption Science & Technology
title Using a New Finite Slit Pore Model for NLDFT Analysis of Carbon Pore Structure
title_full Using a New Finite Slit Pore Model for NLDFT Analysis of Carbon Pore Structure
title_fullStr Using a New Finite Slit Pore Model for NLDFT Analysis of Carbon Pore Structure
title_full_unstemmed Using a New Finite Slit Pore Model for NLDFT Analysis of Carbon Pore Structure
title_short Using a New Finite Slit Pore Model for NLDFT Analysis of Carbon Pore Structure
title_sort using a new finite slit pore model for nldft analysis of carbon pore structure
url https://doi.org/10.1260/0263-6174.29.8.769
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