TY - JOUR
T1 - Measurements of clathrate-hydrate film thickness using laser interferometry
AU - Ohmura, Ryo
AU - Kashiwazaki, Shigetoyo
AU - Mori, Yasuhiko H.
N1 - Funding Information:
We thank K. Fukumoto, a graduate student in the Department of Mechanical Engineering, Keio University, for his assistance in designing and constructing the experimental apparatus. This study was subsidized by the Keio Gijuku Fukuzawa Memorial Fund and by Grants-in-Aid for Scientific Research from the Japan Society for the Promotion of Science (Grant Nos. 10450088 and 3580). R.O. thanks the Research Fellowship of the JSPS for Young Scientists for financial support.
PY - 2000/9/15
Y1 - 2000/9/15
N2 - Using a laser interferometer having a resolution of approximately 1 μm, we directly measured the thicknesses of clathrate-hydrate films at the planar interface between a liquid hydrofluorocarbon, R-134a (CH2FCF3), and liquid water. The interferometer was mounted on a specially designed, pressure- and temperature-controlled cell filled with both liquids. After a hydrate film was formed with either pure water having no prior contact with R-134a or water presaturated with R-134a, we made a series of intermittent measurements until the film was aged up to 150 h. For hydrate films formed with pure water held at a large subcooling (approximately 7 K) below the triple (liquid-R-134a/hydrate/liquid-water) equilibrium temperature, the initial thickness was approximately 10 μm. This thickness was maintained for a few tens of hours; then it gradually increased, reaching approximately 30 μm 100 h after the film formed. With pure water at a smaller subcooling (≲2 K), the thickness of hydrate films was initially as large as approximately 80 μm; it rapidly decreased to 15-20 μm and then increased to 30-40 μm 150 h after the film formed. With presaturated water at small subcoolings (≲2 K), each hydrate film was a mosaic of polygonal hydrate crystal plates. Each plate was several millimeters wide and 20-170 μm thick. No measurement could be made with presaturated water at a large subcooling (≳6 K) because of sword-like hydrate crystals that have grown in crowds into the water phase from the hydrate film surface.
AB - Using a laser interferometer having a resolution of approximately 1 μm, we directly measured the thicknesses of clathrate-hydrate films at the planar interface between a liquid hydrofluorocarbon, R-134a (CH2FCF3), and liquid water. The interferometer was mounted on a specially designed, pressure- and temperature-controlled cell filled with both liquids. After a hydrate film was formed with either pure water having no prior contact with R-134a or water presaturated with R-134a, we made a series of intermittent measurements until the film was aged up to 150 h. For hydrate films formed with pure water held at a large subcooling (approximately 7 K) below the triple (liquid-R-134a/hydrate/liquid-water) equilibrium temperature, the initial thickness was approximately 10 μm. This thickness was maintained for a few tens of hours; then it gradually increased, reaching approximately 30 μm 100 h after the film formed. With pure water at a smaller subcooling (≲2 K), the thickness of hydrate films was initially as large as approximately 80 μm; it rapidly decreased to 15-20 μm and then increased to 30-40 μm 150 h after the film formed. With presaturated water at small subcoolings (≲2 K), each hydrate film was a mosaic of polygonal hydrate crystal plates. Each plate was several millimeters wide and 20-170 μm thick. No measurement could be made with presaturated water at a large subcooling (≳6 K) because of sword-like hydrate crystals that have grown in crowds into the water phase from the hydrate film surface.
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U2 - 10.1016/S0022-0248(00)00564-9
DO - 10.1016/S0022-0248(00)00564-9
M3 - Article
AN - SCOPUS:0034276052
SN - 0022-0248
VL - 218
SP - 372
EP - 380
JO - Journal of Crystal Growth
JF - Journal of Crystal Growth
IS - 2
ER -