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In order to obtain complete information concerning the velocity fields during the \u0027uniting\u0027 of two circular vortex rings, phase-locked velocity measurement was carried out by using a single inclined hot wire point by point all over the flow field, and the vorticity fields were computed from the measured velocity fields. The vortex tubes representing the vortex rings were computed as well as the behavior of the fluid material initially held within the vortex ring, and the important differences among the vorticity, vortex tubes, and fluid material being transported by following the velocity field were explained so as not to misread the real phenomenon and the substance of the physical mechanism. The through process can be divided into the terms of formation \u0026 approaching, first cross-linking \u0026 unlinking, second cross-linking \u0026 unlinking and decay. The first cross-linking \u0026 unlinking is \u0027positive\u0027 and finishes successfully by the continuous and increasing driving force on the adjoined original \u0027near\u0027 segments being pressed against each other, while the second cross-linking \u0026 unlinking is \u0027negative\u0027 and depends on the initial condition due to the monotonously decreasing driving force on the adjoined original \u0027far\u0027 segments in the united vortex ring. As the continuous induced velocities on the approaching and adjoining segments force the segments harder against each other, the flow region in their gap is narrowed, and immediately after the gap cannot hold the whole flux the flow overflows outward to create another velocity gradient that is observed as the sudden appearance of two new concentrated vorticity regions between the adjacent vortex tubes. Therefore, the vorticity in the adjoined original vortex tubes is transported, although no vorticity cancellation is recognized in the present measurement because the time scale of cancellation is much longer than that of the cross-linking \u0026 unlinking. Moreover, several regulations for the quantitative description of the cross-linking \u0026 unlinking process were derived to obtain the time scale in addition to the progress rate of the uniting. Furthermore, the \u0027tail\u0027 parts of the fluid material are observed both during the isolating phase after the formation of the vortex rings and from the \u0027pull out\u0027 phase in the second cross-linking \u0026 unlinking through the decay phase. The \u0027cap\u0027 of the fluid material is observed during the second cross-linking \u0026 unlinking phase that originates in the accumulated fluid material around the neutral center line in the first cross-linking \u0026 unlinking. 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Hot Wire Measurement of Cross-linking and Unlinking in Uniting Two Circular Vortex Rings
https://jaxa.repo.nii.ac.jp/records/31405
https://jaxa.repo.nii.ac.jp/records/3140540532e63-8d4f-4392-b17e-ddb1dc5c4c54
名前 / ファイル | ライセンス | アクション |
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SA0035103.pdf (5.5 MB)
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Item type | 紀要論文 / Departmental Bulletin Paper(1) | |||||
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公開日 | 2015-03-26 | |||||
タイトル | ||||||
言語 | en | |||||
タイトル | Hot Wire Measurement of Cross-linking and Unlinking in Uniting Two Circular Vortex Rings | |||||
言語 | ||||||
言語 | eng | |||||
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 | |||||
著者 |
井筒, 直樹
× 井筒, 直樹× 大島, 裕子× IZUTSU, Naoki× OSHIMA, Yuko |
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著者所属 | ||||||
お茶の水女子大学 | ||||||
著者所属(英) | ||||||
en | ||||||
Faculty of Science, Ochanomizu University:(Present address Research and Development Center, Ricoh Co.Ltd.) | ||||||
出版者 | ||||||
出版者 | 宇宙科学研究所 | |||||
出版者(英) | ||||||
出版者 | Institute of Space and Astronautical Science | |||||
書誌情報 |
en : The Institute of Space and Astronautical Science report 巻 638, p. 1-50, 発行日 1991-03 |
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抄録(英) | ||||||
内容記述タイプ | Other | |||||
内容記述 | A laminar circular vortex ring with excellent reproducibility can be generated by pushing a mass of air through a circular orifice drilled on a buffer plate placed in front of a loudspeaker, which is driven by a stepwise voltage signal. In order to obtain complete information concerning the velocity fields during the 'uniting' of two circular vortex rings, phase-locked velocity measurement was carried out by using a single inclined hot wire point by point all over the flow field, and the vorticity fields were computed from the measured velocity fields. The vortex tubes representing the vortex rings were computed as well as the behavior of the fluid material initially held within the vortex ring, and the important differences among the vorticity, vortex tubes, and fluid material being transported by following the velocity field were explained so as not to misread the real phenomenon and the substance of the physical mechanism. The through process can be divided into the terms of formation & approaching, first cross-linking & unlinking, second cross-linking & unlinking and decay. The first cross-linking & unlinking is 'positive' and finishes successfully by the continuous and increasing driving force on the adjoined original 'near' segments being pressed against each other, while the second cross-linking & unlinking is 'negative' and depends on the initial condition due to the monotonously decreasing driving force on the adjoined original 'far' segments in the united vortex ring. As the continuous induced velocities on the approaching and adjoining segments force the segments harder against each other, the flow region in their gap is narrowed, and immediately after the gap cannot hold the whole flux the flow overflows outward to create another velocity gradient that is observed as the sudden appearance of two new concentrated vorticity regions between the adjacent vortex tubes. Therefore, the vorticity in the adjoined original vortex tubes is transported, although no vorticity cancellation is recognized in the present measurement because the time scale of cancellation is much longer than that of the cross-linking & unlinking. Moreover, several regulations for the quantitative description of the cross-linking & unlinking process were derived to obtain the time scale in addition to the progress rate of the uniting. Furthermore, the 'tail' parts of the fluid material are observed both during the isolating phase after the formation of the vortex rings and from the 'pull out' phase in the second cross-linking & unlinking through the decay phase. The 'cap' of the fluid material is observed during the second cross-linking & unlinking phase that originates in the accumulated fluid material around the neutral center line in the first cross-linking & unlinking. Both the 'tail' and the 'cap' have no vorticity although the 'trail' appearing in the formation process has vorticity. | |||||
ISSN | ||||||
収録物識別子タイプ | ISSN | |||||
収録物識別子 | 0285-6808 | |||||
書誌レコードID | ||||||
収録物識別子タイプ | NCID | |||||
収録物識別子 | AA10632072 | |||||
資料番号 | ||||||
内容記述タイプ | Other | |||||
内容記述 | 資料番号: SA0035103000 |