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圆管潜射流生成偶极子涡特性实验
引用本文:陈科,尤云祥,胡天群. 圆管潜射流生成偶极子涡特性实验[J]. 物理学报, 2013, 62(19): 194702-194702. DOI: 10.7498/aps.62.194702
作者姓名:陈科  尤云祥  胡天群
作者单位:上海交通大学, 海洋工程国家重点实验室, 上海 200240
基金项目:国家自然科学基金,海洋工程国家重点实验室基金(
摘    要:利用溢流恒压装置产生具有稳定出流速度的圆管潜射流, 结合染色液流态显示方法, 在多种射流无量纲潜深d/H、雷诺数Re以及限制数C的组合下, 实验研究了该潜射流动量在有限深密度均匀流体中的演化特性, 其中d为射流潜深, H为水深. 研究表明, 当C<1时潜射流表现为深水特征, 而当1≤ C<2时潜射流表现为过渡特征, 在这两种情况下均不产生任何形式的大尺度相干结构; 当2≤ C<10时潜射流表现为浅水特征, 而C≥10时潜射流表现为极浅水特征, 在这两种情况下均产生大尺度的偶极子涡结构. 对极浅水特征潜射流, 在各种无量纲潜深下, 偶极子涡结构的无量纲形成时间tf*与无量纲射流时间Tinj*均满足相同的正比例关系; 对浅水特征潜射流, 当d/H=0.5时, tf*与Tinj*满足某种线性关系, 但对其他无量纲潜深, tf*与Tinj*之间无明显规律.关键词:圆管潜射流限制数偶极子涡结构形成时间

关 键 词:圆管潜射流  限制数  偶极子涡结构  形成时间
收稿时间:2013-05-06

Experiments on vortex dipoles generated by a submerged round jet
Chen Ke You , Yun-Xiang , Hu Tian-Qun. Experiments on vortex dipoles generated by a submerged round jet[J]. Acta Physica Sinica, 2013, 62(19): 194702-194702. DOI: 10.7498/aps.62.194702
Authors:Chen Ke You    Yun-Xiang    Hu Tian-Qun
Abstract:The formation mechanism and evolution characteristics of a submerged round jet in a uniform fluid of finite depth are investigated experimentally. A spillover system is designed to produce a continuous horizontal jet in the background fluid with a constant velocity, and the flow is visualized by the dyed liquid. Experiments are conducted under different combinations of Reynolds number Re, confinement number C and nondimensional draft d/H, where d is the vertical distance from the jet to the free surface, and H is the depth of the ambient fluid. Four flow patterns are identified for various C. When C<1, the jet shows a deep-water pattern, while for 1≤ C<2, it shows the transitional pattern, the jets do not develop a structured flow for the two jet patterns. When 2≤ C<10, the jet shows the shallow-water pattern, while if C≥10, the jet shows the extreme-shallow-water pattern. In both these two patterns, the jets generate vortex dipole structures. In the extreme-shallow water pattern, the nondimensional vortex formation time tf* for the vortex dipole structure is proportional to the nondimensional injection time Tinj* for various draft d/H. In the shallow-water pattern, tf* depends linearly on Tinj*Re1/2 when the draft d/H=0.5; however, there is no observable relationships between tf* and Tinj* for other draft d/H.
Keywords:submerged round jetconfinement numbervortex dipoleformation time
Keywords:submerged round jet  confinement number  vortex dipole  formation time
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