RAMAN STUDY OF THE METHANE + TBME MIXED HYDRATE IN A DIAMOND ANVIL CELL

It is well known that methane hydrate undergoes several phase transformations at high pressures. At room temperature and low to moderate pressure, methane and water form a stable cubic structure I (sI) hydrate that is also known as MH-I. The structure is transformed to a hexagonal phase (sH/MH-II) a...

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Main Authors: Robin Susilo, Dennis D Klug, John A Ripmeester, Serge Desgreniers, Peter Englezos
Other Authors: The Pennsylvania State University CiteSeerX Archives
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Language:English
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Online Access:http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.504.2548
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spelling ftciteseerx:oai:CiteSeerX.psu:10.1.1.504.2548 2023-05-15T17:11:42+02:00 RAMAN STUDY OF THE METHANE + TBME MIXED HYDRATE IN A DIAMOND ANVIL CELL Robin Susilo Dennis D Klug John A Ripmeester Serge Desgreniers Peter Englezos The Pennsylvania State University CiteSeerX Archives application/pdf http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.504.2548 en eng http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.504.2548 Metadata may be used without restrictions as long as the oai identifier remains attached to it. https://circle.ubc.ca/bitstream/handle/2429/1025/5474.pdf;jsessionid=CE1E976ABB8BB269BBB94E677CE05897?sequence=1 Structure H hydrate high pressure methane TBME text ftciteseerx 2016-01-08T09:17:14Z It is well known that methane hydrate undergoes several phase transformations at high pressures. At room temperature and low to moderate pressure, methane and water form a stable cubic structure I (sI) hydrate that is also known as MH-I. The structure is transformed to a hexagonal phase (sH/MH-II) above 1.0GPa. Another phase transformation occurs above 1.9GPa where the filled ice structure (MH-III) is stable up to 40 GPa before a new high pressure phase transition occurs. Experiments at such high pressures have to be performed in a diamond anvil cell (DAC). Our main interest, though, is to form sH methane hydrate at a lower pressure than reported in previous studies but with some methane in the large cages consequently increasing the methane content. This can be accomplished by introducing the molecules of the large hydrate forming substance (tert-butyl methyl ether/TBME) at a concentration slightly below the stoichiometric amount as suggested by molecular dynamics simulations. In this study we have synthesized mixed methane hydrate of sI and sH and loaded the clathrate with methane into several DACs. Raman spectra were collected at room temperature and pressures in the range of 0.1 to 11.3 GPa. The existence of sH methane hydrate was observed down to 0.2 GPa. However, the existence of methane in the large cages was visible only at pressure higher than 1.0 GPa. The excess methane in the system apparently destabilizes the sH clathrate at pressure below 1.0 GPa as it transforms to sI clathrate. Text Methane hydrate Unknown Anvil ENVELOPE(-64.267,-64.267,-65.239,-65.239)
institution Open Polar
collection Unknown
op_collection_id ftciteseerx
language English
topic Structure H
hydrate
high pressure
methane
TBME
spellingShingle Structure H
hydrate
high pressure
methane
TBME
Robin Susilo
Dennis D Klug
John A Ripmeester
Serge Desgreniers
Peter Englezos
RAMAN STUDY OF THE METHANE + TBME MIXED HYDRATE IN A DIAMOND ANVIL CELL
topic_facet Structure H
hydrate
high pressure
methane
TBME
description It is well known that methane hydrate undergoes several phase transformations at high pressures. At room temperature and low to moderate pressure, methane and water form a stable cubic structure I (sI) hydrate that is also known as MH-I. The structure is transformed to a hexagonal phase (sH/MH-II) above 1.0GPa. Another phase transformation occurs above 1.9GPa where the filled ice structure (MH-III) is stable up to 40 GPa before a new high pressure phase transition occurs. Experiments at such high pressures have to be performed in a diamond anvil cell (DAC). Our main interest, though, is to form sH methane hydrate at a lower pressure than reported in previous studies but with some methane in the large cages consequently increasing the methane content. This can be accomplished by introducing the molecules of the large hydrate forming substance (tert-butyl methyl ether/TBME) at a concentration slightly below the stoichiometric amount as suggested by molecular dynamics simulations. In this study we have synthesized mixed methane hydrate of sI and sH and loaded the clathrate with methane into several DACs. Raman spectra were collected at room temperature and pressures in the range of 0.1 to 11.3 GPa. The existence of sH methane hydrate was observed down to 0.2 GPa. However, the existence of methane in the large cages was visible only at pressure higher than 1.0 GPa. The excess methane in the system apparently destabilizes the sH clathrate at pressure below 1.0 GPa as it transforms to sI clathrate.
author2 The Pennsylvania State University CiteSeerX Archives
format Text
author Robin Susilo
Dennis D Klug
John A Ripmeester
Serge Desgreniers
Peter Englezos
author_facet Robin Susilo
Dennis D Klug
John A Ripmeester
Serge Desgreniers
Peter Englezos
author_sort Robin Susilo
title RAMAN STUDY OF THE METHANE + TBME MIXED HYDRATE IN A DIAMOND ANVIL CELL
title_short RAMAN STUDY OF THE METHANE + TBME MIXED HYDRATE IN A DIAMOND ANVIL CELL
title_full RAMAN STUDY OF THE METHANE + TBME MIXED HYDRATE IN A DIAMOND ANVIL CELL
title_fullStr RAMAN STUDY OF THE METHANE + TBME MIXED HYDRATE IN A DIAMOND ANVIL CELL
title_full_unstemmed RAMAN STUDY OF THE METHANE + TBME MIXED HYDRATE IN A DIAMOND ANVIL CELL
title_sort raman study of the methane + tbme mixed hydrate in a diamond anvil cell
url http://citeseerx.ist.psu.edu/viewdoc/summary?doi=10.1.1.504.2548
long_lat ENVELOPE(-64.267,-64.267,-65.239,-65.239)
geographic Anvil
geographic_facet Anvil
genre Methane hydrate
genre_facet Methane hydrate
op_source https://circle.ubc.ca/bitstream/handle/2429/1025/5474.pdf;jsessionid=CE1E976ABB8BB269BBB94E677CE05897?sequence=1
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