TY - GEN
T1 - Numerical simulation of gas hydrate dissociation in artificial sediment
AU - Temma, Norio
AU - Sakamoto, Yasuhide
AU - Komai, Takeshi
AU - Yamaguchi, Tsutomu
AU - Zyvoloski, George
AU - Pawar, Rajesh
PY - 2006
Y1 - 2006
N2 - Methane Hydrate (MH) is considered to be one of the new-generation energy resources. To support the method of extraction of methane gas from MH, laboratory experiments have been performed at the National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba in Japan. In this paper, we present the results of the numerical simulation of these experiments. In these calculations, Finite Element Heat and Mass Transfer code, developed at the Los Alamos National Laboratory was used. In these experiments, temperature, pressure and cumulative gas production were measured. From this data, we suppose that MH growth/dissociation occurred by the flow of the hot water. Also, we assume that the variation of pressure in this experiment is caused by the change of MH fraction. Thus, we think the SH_max This is the maximum fraction of MH. Using the SH_max, we express the relation between MH fraction (SH) and the absolute permeability (k). This is as follows; k = ko (1 - SH/SH_max) N Using this model, we obtain the good match of the behavior of pressure in the experiment.
AB - Methane Hydrate (MH) is considered to be one of the new-generation energy resources. To support the method of extraction of methane gas from MH, laboratory experiments have been performed at the National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba in Japan. In this paper, we present the results of the numerical simulation of these experiments. In these calculations, Finite Element Heat and Mass Transfer code, developed at the Los Alamos National Laboratory was used. In these experiments, temperature, pressure and cumulative gas production were measured. From this data, we suppose that MH growth/dissociation occurred by the flow of the hot water. Also, we assume that the variation of pressure in this experiment is caused by the change of MH fraction. Thus, we think the SH_max This is the maximum fraction of MH. Using the SH_max, we express the relation between MH fraction (SH) and the absolute permeability (k). This is as follows; k = ko (1 - SH/SH_max) N Using this model, we obtain the good match of the behavior of pressure in the experiment.
KW - Dissociation
KW - Growth
KW - Hydrate
KW - Lab. Experiment
KW - Permeability
KW - Simulation
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M3 - Conference contribution
AN - SCOPUS:36749041269
SN - 1880653664
SN - 9781880653661
T3 - Proceedings of the International Offshore and Polar Engineering Conference
SP - 299
EP - 303
BT - Proceedings of The Sixteenth 2006 International Offshore and Polar Engineering Conference, ISOPE 2006
T2 - 16th 2006 International Offshore and Polar Engineering Conference, ISOPE 2006
Y2 - 28 May 2006 through 2 June 2006
ER -