Dissolution Process Observation of Methane Bubbles in the Deep Ocean Simulator Facility
To investigate the temperature dependency of the methane bubble dissolution rate, buoyant single methane bubbles were held stationary in a countercurrent water flow at a pressure of 6.9 MPa and temperatures ranging from 288 K to 303 K. The 1 to 3 mm diameter bubbles were analyzed by observation thro...
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doaj-75333abdf1444101a52a4363ba4c9b822020-11-25T03:06:39ZengMDPI AGEnergies1996-10732020-08-01133938393810.3390/en13153938Dissolution Process Observation of Methane Bubbles in the Deep Ocean Simulator FacilityTsutomu Uchida0Ike Nagamine1Itsuka Yabe2Tatsunori Fukumaki3Ai Oyama4Brandon Yoza5Norio Tenma6Stephen M. Masutani7Division of Applied Physics, Faculty of Engineering, Hokkaido University, Sapporo 060-8628, JapanHawaii Natural Energy Institute, School of Ocean and Earth Science and Technology, University of Hawaii, Honolulu, HI 96822, USAJapan NUS Co., Ltd., Tokyo 160-0023, JapanJapan NUS Co., Ltd., Tokyo 160-0023, JapanHawaii Natural Energy Institute, School of Ocean and Earth Science and Technology, University of Hawaii, Honolulu, HI 96822, USAHawaii Natural Energy Institute, School of Ocean and Earth Science and Technology, University of Hawaii, Honolulu, HI 96822, USAResearch Institute of Energy Frontier, Department of Energy and Environment, AIST, Tsukuba 305-8569, JapanHawaii Natural Energy Institute, School of Ocean and Earth Science and Technology, University of Hawaii, Honolulu, HI 96822, USATo investigate the temperature dependency of the methane bubble dissolution rate, buoyant single methane bubbles were held stationary in a countercurrent water flow at a pressure of 6.9 MPa and temperatures ranging from 288 K to 303 K. The 1 to 3 mm diameter bubbles were analyzed by observation through the pressure chamber viewport using a bi-telecentric CCD camera. The dissolution rate in artificial seawater was approximately two times smaller than that in pure water. Furthermore, it was observed that the methane bubble dissolution rate increased with temperature, suggesting that bubble dissolution is a thermal activation process (the activation energy is estimated to be 9.0 kJ/mol). The results were different from the expected values calculated using the governing equation for methane dissolution in water. The dissolution modeling of methane bubbles in the mid-to-shallow depth of seawater was revised based on the current results.https://www.mdpi.com/1996-1073/13/15/3938bubble dissolutionnon-hydrate conditiontemperature dependencesalinity |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Tsutomu Uchida Ike Nagamine Itsuka Yabe Tatsunori Fukumaki Ai Oyama Brandon Yoza Norio Tenma Stephen M. Masutani |
spellingShingle |
Tsutomu Uchida Ike Nagamine Itsuka Yabe Tatsunori Fukumaki Ai Oyama Brandon Yoza Norio Tenma Stephen M. Masutani Dissolution Process Observation of Methane Bubbles in the Deep Ocean Simulator Facility Energies bubble dissolution non-hydrate condition temperature dependence salinity |
author_facet |
Tsutomu Uchida Ike Nagamine Itsuka Yabe Tatsunori Fukumaki Ai Oyama Brandon Yoza Norio Tenma Stephen M. Masutani |
author_sort |
Tsutomu Uchida |
title |
Dissolution Process Observation of Methane Bubbles in the Deep Ocean Simulator Facility |
title_short |
Dissolution Process Observation of Methane Bubbles in the Deep Ocean Simulator Facility |
title_full |
Dissolution Process Observation of Methane Bubbles in the Deep Ocean Simulator Facility |
title_fullStr |
Dissolution Process Observation of Methane Bubbles in the Deep Ocean Simulator Facility |
title_full_unstemmed |
Dissolution Process Observation of Methane Bubbles in the Deep Ocean Simulator Facility |
title_sort |
dissolution process observation of methane bubbles in the deep ocean simulator facility |
publisher |
MDPI AG |
series |
Energies |
issn |
1996-1073 |
publishDate |
2020-08-01 |
description |
To investigate the temperature dependency of the methane bubble dissolution rate, buoyant single methane bubbles were held stationary in a countercurrent water flow at a pressure of 6.9 MPa and temperatures ranging from 288 K to 303 K. The 1 to 3 mm diameter bubbles were analyzed by observation through the pressure chamber viewport using a bi-telecentric CCD camera. The dissolution rate in artificial seawater was approximately two times smaller than that in pure water. Furthermore, it was observed that the methane bubble dissolution rate increased with temperature, suggesting that bubble dissolution is a thermal activation process (the activation energy is estimated to be 9.0 kJ/mol). The results were different from the expected values calculated using the governing equation for methane dissolution in water. The dissolution modeling of methane bubbles in the mid-to-shallow depth of seawater was revised based on the current results. |
topic |
bubble dissolution non-hydrate condition temperature dependence salinity |
url |
https://www.mdpi.com/1996-1073/13/15/3938 |
work_keys_str_mv |
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