WEKO3
アイテム
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同心円筒間の乱流テーラー渦流れに関する研究(k-εモデルによる予測)
http://hdl.handle.net/10191/5731
http://hdl.handle.net/10191/5731abd62d91-6a73-4bb2-997c-ba1aff618ccb
名前 / ファイル | ライセンス | アクション |
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9_0029.pdf (432.5 kB)
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Item type | 学術雑誌論文 / Journal Article(1) | |||||
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公開日 | 2008-04-08 | |||||
タイトル | ||||||
タイトル | 同心円筒間の乱流テーラー渦流れに関する研究(k-εモデルによる予測) | |||||
タイトル | ||||||
言語 | en | |||||
タイトル | 同心円筒間の乱流テーラー渦流れに関する研究(k-εモデルによる予測) | |||||
言語 | ||||||
言語 | jpn | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | Taylor Vortex | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | Concentric Cylinders | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | Turbulent Flow | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | Secondary Flow | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | Turbulent Model | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | Calculation | |||||
資源タイプ | ||||||
資源 | http://purl.org/coar/resource_type/c_6501 | |||||
タイプ | journal article | |||||
その他のタイトル | ||||||
その他のタイトル | An Analytical Study on the Turbulent Taylor Vortex Flow between Concentric Cylinders : Prediction of the Flow Field by using the κ-ε Model | |||||
著者 |
小林, 睦夫
× 小林, 睦夫× 前川, 博× 高橋, 武雄× 吉川, 実 |
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著者別名 | ||||||
識別子 | 45070 | |||||
識別子Scheme | WEKO | |||||
姓名 | Kobayashi, Mutsuo | |||||
著者別名 | ||||||
識別子 | 45071 | |||||
識別子Scheme | WEKO | |||||
姓名 | Maekawa, Hiroshi | |||||
著者別名 | ||||||
識別子 | 45072 | |||||
識別子Scheme | WEKO | |||||
姓名 | Takahashi, Takeo | |||||
著者別名 | ||||||
識別子 | 45073 | |||||
識別子Scheme | WEKO | |||||
姓名 | Yoshikawa, Minoru | |||||
抄録 | ||||||
内容記述タイプ | Abstract | |||||
内容記述 | The flow accompanied with turbulent Taylor vortices between inner-rotating and outer-stationary cylinders is analytically treated by using two kinds of κ-ε models. The results obtained with both models are generally in good agreement with the existing experimental results. No marked tendency for the secondary flow to disappear with increasing rotating speed is found within the range of the calculation. For a fixed value of Reynolds number, there exists a certain radius ratio which makes the intensity of the vortex maximum. The more this intensity decreases, the more the turbulence energy increases. As the radius ratio approaches unity, the intensity of the vortex decreases monotonously. Conversely, the intensity of the circumferential component of the secondary flow continues to increase until a radius ratio very close to unity. The hypothesis that the vortex determines its shape so that the total amount of the dissipation rate becomes maximum is substantially consistent with the experimental evidence. | |||||
書誌情報 |
日本機械学会論文集. B編 en : 日本機械学会論文集. B編 巻 56, 号 529, p. 2576-2581, 発行日 1990-09 |
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出版者 | ||||||
出版者 | 日本機械学会 | |||||
ISSN | ||||||
収録物識別子タイプ | ISSN | |||||
収録物識別子 | 03875016 | |||||
書誌レコードID | ||||||
収録物識別子タイプ | NCID | |||||
収録物識別子 | AN00187441 | |||||
権利 | ||||||
権利情報 | 日本機械学会 | |||||
権利 | ||||||
権利情報 | 本文データは学会の許諾に基づくCiNiiからの複製である | |||||
著者版フラグ | ||||||
値 | publisher | |||||
異版である | ||||||
関連タイプ | isVersionOf | |||||
識別子タイプ | URI | |||||
関連識別子 | http://ci.nii.ac.jp/naid/110002389185 |