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AN10079809-20000930-0039.pdf
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Title |
Title |
MHD(電磁流体力学)発電機内におけるプラズマ流の3次元数値シミュレーション
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Kana |
MHD デンジ リュウタイ リキガク ハツデンキナイ ニオケル プラズマリュウ ノ 3ジゲン スウチ シュミレーション
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Romanization |
MHD denji ryutai rikigaku hatsudenkinai niokeru purazumaryu no 3jigen suchi shumireshon
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Three-dimensional numerical simulation of plasma flow in MHD generator
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小林, 宏充
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コバヤシ, ヒロミチ
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Romanization |
Kobayashi, Hiromichi
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慶應義塾大学日吉紀要刊行委員会
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ケイオウ ギジュク ダイガク ヒヨシ キヨウ カンコウ イインカイ
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Romanization |
Keio gijuku daigaku hiyoshi kiyo kanko iinkai
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2000
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慶應義塾大学日吉紀要. 自然科学
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28
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2000
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9
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Start page |
39
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End page |
46
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Abstract |
Three-dimensional flows of nonequilibrium plasma in a disk MHDgenerator are examined numerically by taking into account the change of gasproperties. The nonuniform plasma of "streamer" owing to weak ionization ofseed material has a spiral structure in r-Bplane, and the plasma becomes almostuniform between the walls in r-z plane. In addition to the streamer, the nonunifor-mplasma of "domain" owing to weak ionization of noble gas is revealed. Thedomain has the structure perpendicular to the streamer. In a strong MHD interac-tion case, the static pressure considerably increases in the upstream region of ageneration channel, and the pseudo-shock waves appear in the generator, but theplasma is almost uniform along e-direction. The boundary layer in the strongMHD interaction is considerably thick, and in the broad region near the wall theHall current flows reversely. In the weak MHD interaction case, the current flowstoward downstream even near walls. In the strong interaction case, however, thecurrent near walls flows mainly e-direction, and exists like leak current.
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three-dimensional simulation.
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Departmental Bulletin Paper
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