Thermal conductivity of hydrate-bearing sediments

dc.contributor.author Cortes, Douglas D.
dc.contributor.author Martin, Ana I.
dc.contributor.author Yun, Tae Sup
dc.contributor.author Francisca, Franco M.
dc.contributor.author Santamarina, J. Carlos
dc.contributor.author Ruppel, Carolyn D.
dc.date.accessioned 2010-05-26T18:39:40Z
dc.date.available 2010-05-26T18:39:40Z
dc.date.issued 2009-11-18
dc.description Author Posting. © American Geophysical Union, 2009. This article is posted here by permission of American Geophysical Union for personal use, not for redistribution. The definitive version was published in Journal of Geophysical Research 114 (2009): B11103, doi:10.1029/2008JB006235. en_US
dc.description.abstract A thorough understanding of the thermal conductivity of hydrate-bearing sediments is necessary for evaluating phase transformation processes that would accompany energy production from gas hydrate deposits and for estimating regional heat flow based on the observed depth to the base of the gas hydrate stability zone. The coexistence of multiple phases (gas hydrate, liquid and gas pore fill, and solid sediment grains) and their complex spatial arrangement hinder the a priori prediction of the thermal conductivity of hydrate-bearing sediments. Previous studies have been unable to capture the full parameter space covered by variations in grain size, specific surface, degree of saturation, nature of pore filling material, and effective stress for hydrate-bearing samples. Here we report on systematic measurements of the thermal conductivity of air dry, water- and tetrohydrofuran (THF)-saturated, and THF hydrate–saturated sand and clay samples at vertical effective stress of 0.05 to 1 MPa (corresponding to depths as great as 100 m below seafloor). Results reveal that the bulk thermal conductivity of the samples in every case reflects a complex interplay among particle size, effective stress, porosity, and fluid-versus-hydrate filled pore spaces. The thermal conductivity of THF hydrate–bearing soils increases upon hydrate formation although the thermal conductivities of THF solution and THF hydrate are almost the same. Several mechanisms can contribute to this effect including cryogenic suction during hydrate crystal growth and the ensuing porosity reduction in the surrounding sediment, increased mean effective stress due to hydrate formation under zero lateral strain conditions, and decreased interface thermal impedance as grain-liquid interfaces are transformed into grain-hydrate interfaces. en_US
dc.description.sponsorship This work was supported by the Chevron Joint Industry Project on Methane Hydrates under contract DE-FC26- 01NT41330 to Georgia Institute of Technology from the U.S. Department of Energy’s National Energy Technology Laboratory. J.C.S. received additional support from the Goizueta Foundation. C.R. thanks the Petroleum Research Fund of the American Chemical Society under AC8–31351 for early support of thermal conductivity research on hydrate-bearing sediments at Georgia Institute of Technology. en_US
dc.format.mimetype application/pdf
dc.identifier.citation Journal of Geophysical Research 114 (2009): B11103 en_US
dc.identifier.doi 10.1029/2008JB006235
dc.identifier.uri https://hdl.handle.net/1912/3534
dc.language.iso en_US en_US
dc.publisher American Geophysical Union en_US
dc.relation.uri https://doi.org/10.1029/2008JB006235
dc.subject Gas hydrate en_US
dc.title Thermal conductivity of hydrate-bearing sediments en_US
dc.type Article en_US
dspace.entity.type Publication
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