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https://hdl.handle.net/20.500.14094/0100476312
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2025-09-11
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0100476312 (fulltext)
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メタデータID
0100476312
アクセス権
open access
出版タイプ
Accepted Manuscript
タイトル
Liquid film thickness of upward air–water annular flow after passing through 90° bend
著者
Kurimoto, Ryo ; Takeuchi, Yuji ; Minagawa, Hisato ; Yasuda, Takahiro
著者ID
A2770
研究者ID
1000090711903
KUID
https://kuid-rm-web.ofc.kobe-u.ac.jp/search/detail?systemId=b495814e377be56e520e17560c007669
著者名
Kurimoto, Ryo
栗本, 遼
クリモト, リョウ
所属機関名
工学研究科
著者名
Takeuchi, Yuji
著者名
Minagawa, Hisato
著者ID
A1453
研究者ID
1000030614135
KUID
https://kuid-rm-web.ofc.kobe-u.ac.jp/search/detail?systemId=0e49c0893c2808ac520e17560c007669
著者名
Yasuda, Takahiro
保多, 隆裕
ヤスダ, タカヒロ
所属機関名
未来医工学研究開発センター
言語
English (英語)
収録物名
Experimental Thermal and Fluid Science
巻(号)
139
ページ
110735
出版者
Elsevier
刊行日
2022-11-01
公開日
2024-07-16
抄録
Axial development of the base film thickness of an upward air–water annular flow after passing through a 90° bend was investigated. The pipe diameter D of the channel was 5.0 mm. The ratios, R*, of the radius of curvature of a bend to D were 6.0 and 10. The dimensionless axial distances, z* (=z/D), of measurement positions were 4, 12 and 20, where z is the axial coordinate in the vertical section. The circumferential measurement positions, θ, from the outer side to the inner side of the bend at each z* were 0, 45, 90, 135 and 180°. The liquid film thicknesses on the top and bottom sides in the horizontal section were also measured. At z* = 4, the base film at θ = 0° was thicker than that at the other θ in most of the present experimental conditions. In contrast, the circumferential distribution of the base film thickness was symmetric even at z* = 4 in the cases of high gas volumetric flux and low liquid volumetric flux. The circumferential distributions of the base film thicknesses at z* = 12 and 20 were symmetric in all experimental conditions. At z* = 12 and 20, the circumferential averaged base film thickness after passing through the bend with R* = 10 was larger than that after passing through the bend with R* = 6. The axial velocity in the liquid film was also measured. The circumferential distribution of the axial velocity was nearly symmetric at z* = 12 and 20.
キーワード
Upward annular flow
Liquid film thickness
90° bend
Laser-induced fluorescence
Liquid film velocity
カテゴリ
工学研究科
未来医工学研究開発センター
学術雑誌論文
権利
© 2022 Elsevier Inc.
This manuscript version is made available under the CC-BY-NC-ND 4.0 license http://creativecommons.org/licenses/by-nc-nd/4.0/
関連情報
DOI
https://doi.org/10.1016/j.expthermflusci.2022.110735
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資源タイプ
journal article
ISSN
0894-1777
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eISSN
1879-2286
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NCID
AA11527517
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