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摩擦層に於けるレイノルズ應力・混合距離及び亂れ生成のエネルギーの分布(應用力學)
https://jaxa.repo.nii.ac.jp/records/34744
https://jaxa.repo.nii.ac.jp/records/34744e8712d01-4ac5-49b3-90be-08754b64ff21
| 名前 / ファイル | ライセンス | アクション |
|---|---|---|
SA3406584.pdf (1.1 MB)
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| Item type | 紀要論文 / Departmental Bulletin Paper(1) | |||||||||
|---|---|---|---|---|---|---|---|---|---|---|
| 公開日 | 2015-03-26 | |||||||||
| タイトル | ||||||||||
| タイトル | 摩擦層に於けるレイノルズ應力・混合距離及び亂れ生成のエネルギーの分布(應用力學) | |||||||||
| 言語 | ||||||||||
| 言語 | jpn | |||||||||
| 資源タイプ | ||||||||||
| 資源タイプ識別子 | http://purl.org/coar/resource_type/c_6501 | |||||||||
| 資源タイプ | departmental bulletin paper | |||||||||
| その他のタイトル（英） | ||||||||||
| その他のタイトル | The Distributions of Reynolds' Stress, Mixture Length and the Energy Transformed from Mean Flow to Fluctuating Flow in the Boundary Layer.(Applied Mechanics) | |||||||||
| 著者 |
深津, 了藏
× 深津, 了藏
× Fukatsu, Ryozo
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| 著者所属 | ||||||||||
| 東京大學理工學研究所 | ||||||||||
| 著者所属（英） | ||||||||||
| en | ||||||||||
| THE INSTITUTE OF SCIENCE AND TECHNOLOGY, UNIVERSITY OF TOKYO | ||||||||||
| 出版者 | ||||||||||
| 出版者 | 東京大学理工学研究所 | |||||||||
| 書誌情報 |
東京大學理工學研究所報告 巻 3, 号 7/8, p. 228-238, 発行日 1950-01-20 |
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| 抄録（英） | ||||||||||
| 内容記述タイプ | Other | |||||||||
| 内容記述 | Reynolds' stress, mixture length and the energy transformed from mean flow to fluctuating flow in the boundary layer were calculated from the measured values of mean velocity using the fundamental equation of fluctuating boundary layer flow. Following important results were obtained : Even in the apparent state of laminar flow before the transition, u'v'≠0 and the additional flow is neither Tollmien's wave nor G.I. Taylor's oscillation. The theory of laminar separation and the theory of instantaneous separation fail to tell the truth about the transition, because distributions near the surface contribute very little to the transformation of energy. The true state of transition is a kind of unstable oscillation with increasing amplitude and with the energy transformation from mean flow to fluctuating flow which is performed within relatively wide range with its centre near 1/4δ from the surface until it reaches the maximum at the midway. Then the flow changes to the type of fully developed turbulent flow with the most of the turbulent energy transformation taking place very near the surface. | |||||||||
| ISSN | ||||||||||
| 収録物識別子タイプ | ISSN | |||||||||
| 収録物識別子 | 0371-6090 | |||||||||
| 書誌レコードID | ||||||||||
| 収録物識別子タイプ | NCID | |||||||||
| 収録物識別子 | AN00162611 | |||||||||
| 資料番号 | ||||||||||
| 内容記述タイプ | Other | |||||||||
| 内容記述 | 資料番号: SA3406584000 | |||||||||
