Abstract
後部が細くなる円すいが一様流中で回転している場合の乱流境界層を実験的,理論的に調べた.測定された各方向の乱れ強さは回転と共に著しく増大している.これを乱れエネルギの生成項,輸送項,リチャードソン数によって調べた.計算は運動量積分方程式によるもので,一般化擬二次元性と壁面せん断応力の形を仮定している.計算結果は簡単な方法であるにもかかわらず,実験とよく一致している.
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