The turbulent mixing of liquid mass caused by an air bubble rising near a wall in a still liquid in a pipe is investigated experimentally using a photochromic dye. A part of the liquid is activated by UV light and subjected to the fluid motion caused by a zigzag rising bubble of which Reynolds number is 214. The visualized mixing patterns showed that the dye is mixed by vortex motions in the bubble wake that is similar to the case of a bubble rising in the center of the pipe. The concentration distributions were deduced from the dye images using Lambert-Beer’s law and the turbulent diffusion coefficient (TDC) was evaluated from the temporal changes in the mass dispersion. The TDCs showed that a near-wall bubble generates stronger mixing than for a bubble in the center of the pipe. This stronger mixing can be attributed to the large-scale vortices observed for a near-wall bubble, which remains active for a longer time due to the lack of oppositely rotating vortices and mixes more fluids.
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ASME-JSME-KSME 2011 Joint Fluids Engineering Conference
July 24–29, 2011
Hamamatsu, Japan
Conference Sponsors:
- Fluids Engineering Division
ISBN:
978-0-7918-4440-3
PROCEEDINGS PAPER
Mixing of Matter by a Rising Bubble Near a Wall
Toru Koso,
Toru Koso
Kyushu University, Kasuga, Fukuoka, Japan
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Hiroyuki Iwashita,
Hiroyuki Iwashita
Kyushu University, Kasuga, Fukuoka, Japan
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Fumihiko Usuki
Fumihiko Usuki
Denso Co. Ltd., Kariya, Aichi, Japan
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Toru Koso
Kyushu University, Kasuga, Fukuoka, Japan
Hiroyuki Iwashita
Kyushu University, Kasuga, Fukuoka, Japan
Fumihiko Usuki
Denso Co. Ltd., Kariya, Aichi, Japan
Paper No:
AJK2011-21010, pp. 3755-3761; 7 pages
Published Online:
May 25, 2012
Citation
Koso, T, Iwashita, H, & Usuki, F. "Mixing of Matter by a Rising Bubble Near a Wall." Proceedings of the ASME-JSME-KSME 2011 Joint Fluids Engineering Conference. ASME-JSME-KSME 2011 Joint Fluids Engineering Conference: Volume 1, Symposia – Parts A, B, C, and D. Hamamatsu, Japan. July 24–29, 2011. pp. 3755-3761. ASME. https://doi.org/10.1115/AJK2011-21010
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