Molecular modeling of the dissociation of methane hydrate in contact with a silica surface

We use constant energy, constant volume (NVE) molecular dynamics simulations to study the dissociation of the fully occupied structure I methane hydrate in a confined geometry between two hydroxylated silica surfaces between 36 and 41 Å apart, at initial temperatures of 283, 293, and 303 K. Simulati...

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Published in:The Journal of Physical Chemistry B
Main Authors: Bagherzadeh, S. Alireza, Englezos, Peter, Alavi, Saman, Ripmeester, John A.
Format: Article in Journal/Newspaper
Language:English
Published: 2012
Subjects:
Online Access:https://doi.org/10.1021/jp2086544
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spelling ftnrccanada:oai:cisti-icist.nrc-cnrc.ca:cistinparc:21268881 2023-05-15T17:11:39+02:00 Molecular modeling of the dissociation of methane hydrate in contact with a silica surface Bagherzadeh, S. Alireza Englezos, Peter Alavi, Saman Ripmeester, John A. 2012-03-15 text https://doi.org/10.1021/jp2086544 https://nrc-publications.canada.ca/eng/view/object/?id=d9b4b06a-037d-4284-b64b-96e065f70164 https://nrc-publications.canada.ca/fra/voir/objet/?id=d9b4b06a-037d-4284-b64b-96e065f70164 eng eng issn:1520-6106 issn:1520-5207 The Journal of Physical Chemistry B, Volume: 116, Issue: 10, Publication date: 2012-03-15, Pages: 3188–3197 doi:10.1021/jp2086544 article 2012 ftnrccanada https://doi.org/10.1021/jp2086544 2021-09-01T06:26:33Z We use constant energy, constant volume (NVE) molecular dynamics simulations to study the dissociation of the fully occupied structure I methane hydrate in a confined geometry between two hydroxylated silica surfaces between 36 and 41 Å apart, at initial temperatures of 283, 293, and 303 K. Simulations of the two-phase hydrate/water system are performed in the presence of silica, with and without a 3 Å thick buffering water layer between the hydrate phase and silica surfaces. Faster decomposition is observed in the presence of silica, where the hydrate phase is prone to decomposition from four surfaces, as compared to only two sides in the case of the hydrate/water simulations. The existence of the water layer between the hydrate phase and the silica surface stabilizes the hydrate phase relative to the case where the hydrate is in direct contact with silica. Hydrates bound between the silica surfaces dissociate layer-by-layer in a shrinking core manner with a curved decomposition front which extends over a 5–8 Å thickness. Labeling water molecules shows that there is exchange of water molecules between the surrounding liquid and intact cages in the methane hydrate phase. In all cases, decomposition of the methane hydrate phase led to the formation of methane nanobubbles in the liquid water phase. Peer reviewed: Yes NRC publication: Yes Article in Journal/Newspaper Methane hydrate National Research Council Canada: NRC Publications Archive The Journal of Physical Chemistry B 116 10 3188 3197
institution Open Polar
collection National Research Council Canada: NRC Publications Archive
op_collection_id ftnrccanada
language English
description We use constant energy, constant volume (NVE) molecular dynamics simulations to study the dissociation of the fully occupied structure I methane hydrate in a confined geometry between two hydroxylated silica surfaces between 36 and 41 Å apart, at initial temperatures of 283, 293, and 303 K. Simulations of the two-phase hydrate/water system are performed in the presence of silica, with and without a 3 Å thick buffering water layer between the hydrate phase and silica surfaces. Faster decomposition is observed in the presence of silica, where the hydrate phase is prone to decomposition from four surfaces, as compared to only two sides in the case of the hydrate/water simulations. The existence of the water layer between the hydrate phase and the silica surface stabilizes the hydrate phase relative to the case where the hydrate is in direct contact with silica. Hydrates bound between the silica surfaces dissociate layer-by-layer in a shrinking core manner with a curved decomposition front which extends over a 5–8 Å thickness. Labeling water molecules shows that there is exchange of water molecules between the surrounding liquid and intact cages in the methane hydrate phase. In all cases, decomposition of the methane hydrate phase led to the formation of methane nanobubbles in the liquid water phase. Peer reviewed: Yes NRC publication: Yes
format Article in Journal/Newspaper
author Bagherzadeh, S. Alireza
Englezos, Peter
Alavi, Saman
Ripmeester, John A.
spellingShingle Bagherzadeh, S. Alireza
Englezos, Peter
Alavi, Saman
Ripmeester, John A.
Molecular modeling of the dissociation of methane hydrate in contact with a silica surface
author_facet Bagherzadeh, S. Alireza
Englezos, Peter
Alavi, Saman
Ripmeester, John A.
author_sort Bagherzadeh, S. Alireza
title Molecular modeling of the dissociation of methane hydrate in contact with a silica surface
title_short Molecular modeling of the dissociation of methane hydrate in contact with a silica surface
title_full Molecular modeling of the dissociation of methane hydrate in contact with a silica surface
title_fullStr Molecular modeling of the dissociation of methane hydrate in contact with a silica surface
title_full_unstemmed Molecular modeling of the dissociation of methane hydrate in contact with a silica surface
title_sort molecular modeling of the dissociation of methane hydrate in contact with a silica surface
publishDate 2012
url https://doi.org/10.1021/jp2086544
https://nrc-publications.canada.ca/eng/view/object/?id=d9b4b06a-037d-4284-b64b-96e065f70164
https://nrc-publications.canada.ca/fra/voir/objet/?id=d9b4b06a-037d-4284-b64b-96e065f70164
genre Methane hydrate
genre_facet Methane hydrate
op_relation issn:1520-6106
issn:1520-5207
The Journal of Physical Chemistry B, Volume: 116, Issue: 10, Publication date: 2012-03-15, Pages: 3188–3197
doi:10.1021/jp2086544
op_doi https://doi.org/10.1021/jp2086544
container_title The Journal of Physical Chemistry B
container_volume 116
container_issue 10
container_start_page 3188
op_container_end_page 3197
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