Optical Observation of Pool Boiling in Cooling Channels

In this paper, the phenomena of pool boiling and formation of flow convection in the cooling channels are observed by an optical method. The laser schlieren method with helium-neon laser of 7mW and a high speed camera with maximum shooting speed of 10, 000 frames per second are used to observe the f...

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Published inTEION KOGAKU (Journal of Cryogenics and Superconductivity Society of Japan) Vol. 28; no. 3; pp. 160 - 166
Main Authors FUCHINO, Shuichiro, NATORI, Naotake, ITO, Toshiaki, TAMADA, Noriharu
Format Journal Article
LanguageEnglish
Published CRYOGENICS AND SUPERCONDUCTIVITY SOCIETY OF JAPAN 1993
Online AccessGet full text
ISSN0389-2441
1880-0408
1880-0408
DOI10.2221/jcsj.28.160

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Abstract In this paper, the phenomena of pool boiling and formation of flow convection in the cooling channels are observed by an optical method. The laser schlieren method with helium-neon laser of 7mW and a high speed camera with maximum shooting speed of 10, 000 frames per second are used to observe the fast phenomena. Analyzing films, transient formations of the flow convection have been observed. A bubble cluster with the thickness of around a hundred μm boundary layer has been formed during first 10ms and after that a turbulent layer has developed. The phenomena of the overshooting of the flow convection have been observed during heating. The flow velocity induced from the elapsing time till the overshooting becomes at maximum is almost equal to the predicted flow velocity calculated from the energy conservation law.
AbstractList In this paper, the phenomena of pool boiling and formation of flow convection in the cooling channels are observed by an optical method. The laser schlieren method with helium-neon laser of 7mW and a high speed camera with maximum shooting speed of 10, 000 frames per second are used to observe the fast phenomena. Analyzing films, transient formations of the flow convection have been observed. A bubble cluster with the thickness of around a hundred μm boundary layer has been formed during first 10ms and after that a turbulent layer has developed. The phenomena of the overshooting of the flow convection have been observed during heating. The flow velocity induced from the elapsing time till the overshooting becomes at maximum is almost equal to the predicted flow velocity calculated from the energy conservation law.
Author ITO, Toshiaki
FUCHINO, Shuichiro
TAMADA, Noriharu
NATORI, Naotake
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References 7) A. Khalil, et al.: Cryoenics 21 (1981) 411
2) M. N. Wilson: Liquid Helium Technology, Proc. Int. Inst. Refrig. Commun. I (1966) 109
1) S. G. Sydoriak and T. R. Roberts: J. Appl. Phys. 28 (1956) 143
4) S. Lehongre, et al.: Proc. ICEC 2 (1968) 274
5) 佐藤新太郎, 尾形久直: 低温工学 12 (1977) 2
9) 塩治震太郎: 伝熱工学の基礎, オーム社, 東京 (1982) 164
6) H. Ogata and W. Nakayama: Adv. Cryog. Eng. 27 (1982) 309
8) 低温工学ハンドブック編集委員会編: 低温工学ハンドブック, 内田老鶴圃新社, 東京 (1982) 542
3) 平田郁之, 小俣虎之助: 低温工学 3 (1968) 120
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– reference: 6) H. Ogata and W. Nakayama: Adv. Cryog. Eng. 27 (1982) 309
– reference: 8) 低温工学ハンドブック編集委員会編: 低温工学ハンドブック, 内田老鶴圃新社, 東京 (1982) 542
– reference: 9) 塩治震太郎: 伝熱工学の基礎, オーム社, 東京 (1982) 164
– reference: 4) S. Lehongre, et al.: Proc. ICEC 2 (1968) 274
– reference: 7) A. Khalil, et al.: Cryoenics 21 (1981) 411
– reference: 5) 佐藤新太郎, 尾形久直: 低温工学 12 (1977) 2
– reference: 3) 平田郁之, 小俣虎之助: 低温工学 3 (1968) 120
– reference: 1) S. G. Sydoriak and T. R. Roberts: J. Appl. Phys. 28 (1956) 143
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Title Optical Observation of Pool Boiling in Cooling Channels
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