Formation of methane hydrate from polydisperse ice powders

Neutron diffraction runs and gas-consumption experiments based on pressure-volume-temperature measurements are conducted to study the kinetics of methane hydrate formation from hydrogenated and deuterated ice powder samples in the temperature range of 245-270 K up to high degrees of transformation....

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Main Authors: Kuhs W., Staykova D., Salamatin A.
Format: Article in Journal/Newspaper
Language:unknown
Published: 2006
Subjects:
Online Access:http://dspace.kpfu.ru/xmlui/handle/net/99021
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record_format openpolar
spelling ftkazanuniv:oai:dspace.kpfu.ru:net/99021 2023-05-15T17:11:53+02:00 Formation of methane hydrate from polydisperse ice powders Kuhs W. Staykova D. Salamatin A. 2006 http://dspace.kpfu.ru/xmlui/handle/net/99021 unknown Journal of Physical Chemistry B 26 13283 110 http://dspace.kpfu.ru/xmlui/bitstream/net/99021/1/SCOPUS15206106-2006-110-26-SID33746427132-a1.pdf 1520-6106 http://dspace.kpfu.ru/xmlui/handle/net/99021 SCOPUS15206106-2006-110-26-SID33746427132 Article 2006 ftkazanuniv 2022-01-01T09:34:30Z Neutron diffraction runs and gas-consumption experiments based on pressure-volume-temperature measurements are conducted to study the kinetics of methane hydrate formation from hydrogenated and deuterated ice powder samples in the temperature range of 245-270 K up to high degrees of transformation. An improved theory of the hydrate growth in a polydisperse ensemble of randomly packed ice spheres is developed to provide a quantitative interpretation of the data in terms of kinetic model parameters. This paper continues the research line of our earlier study which was limited to the monodisperse case and shorter reaction times (Staykova et al., 2003).1 As before, we distinguish the process of initial hydrate film spreading over the ice particle surface (stage I) and the subsequent hydrate shell growth (stage II) which includes two steps, i.e., an interfacial clathration reaction and the gas and water transport (diffusion) through the hydrate layer surrounding the shrinking ice cores. Although kinetics of hydrate formation at stage II is clearly dominated by the diffusion mechanism which becomes the limiting step at temperatures above 263 K, both steps are shown to be essential at lower temperatures. The permeation coefficient D is estimated as (1.46 ± 0.44) × 10-12 m2/h at 263 K with an activation energy QD ≈ 52.1 kJ/mol. This value is close to the energy of breaking hydrogen bonds in ice Ih and suggests that this process is the rate-limiting step in hydrate formation from ice in the slower diffusion-controlled part of the reaction. © 2006 American Chemical Society. Article in Journal/Newspaper Methane hydrate Kazan Federal University Digital Repository
institution Open Polar
collection Kazan Federal University Digital Repository
op_collection_id ftkazanuniv
language unknown
description Neutron diffraction runs and gas-consumption experiments based on pressure-volume-temperature measurements are conducted to study the kinetics of methane hydrate formation from hydrogenated and deuterated ice powder samples in the temperature range of 245-270 K up to high degrees of transformation. An improved theory of the hydrate growth in a polydisperse ensemble of randomly packed ice spheres is developed to provide a quantitative interpretation of the data in terms of kinetic model parameters. This paper continues the research line of our earlier study which was limited to the monodisperse case and shorter reaction times (Staykova et al., 2003).1 As before, we distinguish the process of initial hydrate film spreading over the ice particle surface (stage I) and the subsequent hydrate shell growth (stage II) which includes two steps, i.e., an interfacial clathration reaction and the gas and water transport (diffusion) through the hydrate layer surrounding the shrinking ice cores. Although kinetics of hydrate formation at stage II is clearly dominated by the diffusion mechanism which becomes the limiting step at temperatures above 263 K, both steps are shown to be essential at lower temperatures. The permeation coefficient D is estimated as (1.46 ± 0.44) × 10-12 m2/h at 263 K with an activation energy QD ≈ 52.1 kJ/mol. This value is close to the energy of breaking hydrogen bonds in ice Ih and suggests that this process is the rate-limiting step in hydrate formation from ice in the slower diffusion-controlled part of the reaction. © 2006 American Chemical Society.
format Article in Journal/Newspaper
author Kuhs W.
Staykova D.
Salamatin A.
spellingShingle Kuhs W.
Staykova D.
Salamatin A.
Formation of methane hydrate from polydisperse ice powders
author_facet Kuhs W.
Staykova D.
Salamatin A.
author_sort Kuhs W.
title Formation of methane hydrate from polydisperse ice powders
title_short Formation of methane hydrate from polydisperse ice powders
title_full Formation of methane hydrate from polydisperse ice powders
title_fullStr Formation of methane hydrate from polydisperse ice powders
title_full_unstemmed Formation of methane hydrate from polydisperse ice powders
title_sort formation of methane hydrate from polydisperse ice powders
publishDate 2006
url http://dspace.kpfu.ru/xmlui/handle/net/99021
genre Methane hydrate
genre_facet Methane hydrate
op_source SCOPUS15206106-2006-110-26-SID33746427132
op_relation Journal of Physical Chemistry B
26
13283
110
http://dspace.kpfu.ru/xmlui/bitstream/net/99021/1/SCOPUS15206106-2006-110-26-SID33746427132-a1.pdf
1520-6106
http://dspace.kpfu.ru/xmlui/handle/net/99021
_version_ 1766068635551399936