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Mechanism of Hexane Displaced by Supercritical Carbon Dioxide: Insights from Molecular Simulations

Supercritical carbon dioxide (sCO(2)) has great potential for displacing shale oil as a result of its high solubility and low surface tension and viscosity, but the underlying mechanisms have remained unclear up to now. By conducting equilibrium molecular dynamics (EMD) simulations, we found that th...

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Autores principales: Song, Jiasheng, Zhu, Zhuangying, Liu, Lang
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9736652/
https://www.ncbi.nlm.nih.gov/pubmed/36500433
http://dx.doi.org/10.3390/molecules27238340
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author Song, Jiasheng
Zhu, Zhuangying
Liu, Lang
author_facet Song, Jiasheng
Zhu, Zhuangying
Liu, Lang
author_sort Song, Jiasheng
collection PubMed
description Supercritical carbon dioxide (sCO(2)) has great potential for displacing shale oil as a result of its high solubility and low surface tension and viscosity, but the underlying mechanisms have remained unclear up to now. By conducting equilibrium molecular dynamics (EMD) simulations, we found that the displacing process could be divided into three steps: the CO(2) molecules were firstly injected in the central region of shale slit, then tended to adsorb on the SiO(2)-OH wall surface and mix with hexane, resulting in loose hexane layer on the shale surface, and finally displaced hexane from the wall due to strong interactions between CO(2) and wall. In that process, the displacing velocity and efficiency of hexane exhibit parabolic and increased trends with pressure, respectively. To gain deep insights into this phenomenon, we further performed non-equilibrium molecular dynamics (NEMD) simulations and found that both the Onsager coefficients of CO(2) and hexane were correlated to increase with pressure, until the diffusion rate of hexane being suppressed by the highly dense distribution of CO(2) molecules at 12 MPa. The rapid transportation of CO(2) molecules in the binary components (CO(2) and hexane) actually promoted the hexane diffusion, which facilitated hexane flowing out of the nanochannel and subsequently enhanced oil recovery efficiency. The displacing process could occur effectively at pressures higher than 7.5 MPa, after which the interaction energies of the CO(2)-wall were stronger than that of the hexane-wall. Taking displacing velocity and efficiency and hexane diffusion rate into consideration, the optimal injection pressure was found at 10.5 MPa in this work. This study provides detailed insights into CO(2) displacing shale oil and is in favor of deepening the understanding of shale oil exploitation and utilization.
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spelling pubmed-97366522022-12-11 Mechanism of Hexane Displaced by Supercritical Carbon Dioxide: Insights from Molecular Simulations Song, Jiasheng Zhu, Zhuangying Liu, Lang Molecules Article Supercritical carbon dioxide (sCO(2)) has great potential for displacing shale oil as a result of its high solubility and low surface tension and viscosity, but the underlying mechanisms have remained unclear up to now. By conducting equilibrium molecular dynamics (EMD) simulations, we found that the displacing process could be divided into three steps: the CO(2) molecules were firstly injected in the central region of shale slit, then tended to adsorb on the SiO(2)-OH wall surface and mix with hexane, resulting in loose hexane layer on the shale surface, and finally displaced hexane from the wall due to strong interactions between CO(2) and wall. In that process, the displacing velocity and efficiency of hexane exhibit parabolic and increased trends with pressure, respectively. To gain deep insights into this phenomenon, we further performed non-equilibrium molecular dynamics (NEMD) simulations and found that both the Onsager coefficients of CO(2) and hexane were correlated to increase with pressure, until the diffusion rate of hexane being suppressed by the highly dense distribution of CO(2) molecules at 12 MPa. The rapid transportation of CO(2) molecules in the binary components (CO(2) and hexane) actually promoted the hexane diffusion, which facilitated hexane flowing out of the nanochannel and subsequently enhanced oil recovery efficiency. The displacing process could occur effectively at pressures higher than 7.5 MPa, after which the interaction energies of the CO(2)-wall were stronger than that of the hexane-wall. Taking displacing velocity and efficiency and hexane diffusion rate into consideration, the optimal injection pressure was found at 10.5 MPa in this work. This study provides detailed insights into CO(2) displacing shale oil and is in favor of deepening the understanding of shale oil exploitation and utilization. MDPI 2022-11-29 /pmc/articles/PMC9736652/ /pubmed/36500433 http://dx.doi.org/10.3390/molecules27238340 Text en © 2022 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Song, Jiasheng
Zhu, Zhuangying
Liu, Lang
Mechanism of Hexane Displaced by Supercritical Carbon Dioxide: Insights from Molecular Simulations
title Mechanism of Hexane Displaced by Supercritical Carbon Dioxide: Insights from Molecular Simulations
title_full Mechanism of Hexane Displaced by Supercritical Carbon Dioxide: Insights from Molecular Simulations
title_fullStr Mechanism of Hexane Displaced by Supercritical Carbon Dioxide: Insights from Molecular Simulations
title_full_unstemmed Mechanism of Hexane Displaced by Supercritical Carbon Dioxide: Insights from Molecular Simulations
title_short Mechanism of Hexane Displaced by Supercritical Carbon Dioxide: Insights from Molecular Simulations
title_sort mechanism of hexane displaced by supercritical carbon dioxide: insights from molecular simulations
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9736652/
https://www.ncbi.nlm.nih.gov/pubmed/36500433
http://dx.doi.org/10.3390/molecules27238340
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