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Wake of two side-by-side square cylinders at low Reynolds numbers

机译:在低雷诺数下唤醒两个并排的方形气缸

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摘要

Wake of two side-by-side square cylinders was investigated through direct numerical simulation at low Reynolds numbers (16-200). The gap between the two cylinders varied from 0 to 10D, where D is the dimension of the square cylinder (edge length). 9 different wake patterns and their dependency on both the Reynolds number and gap spacing were identified and analysed. A system classification map, demarcated by the Reynolds number and gap ratio g* (g/D, where g is the gap spacing between 2 cylinders), was derived for these 9 wake modes. Steady-state wake (mode I) was observed when the Reynolds number is lower than the critical Reynolds number, which depends on g*. For the gap ratio less than 0.7, only single vortex street was observed. The single vortex street wake can be either symmetric and periodic (mode II), or asymmetric and periodic (mode III), or irregular (mode IV). In this gap ratio range (less than 0.7), shedding frequency decreases with the gap ratio due to the damping role of the gap flow. For the gap ratio larger than 0.7, two vortex streets were also observed. For the gap ratio larger than 1, only two vortex streets were observed. Vortex shedding can be either synchronized and in-phase (mode V), synchronized and anti-phase (mode VI), in-phase dominated with low frequency modulation (mode VII), anti-phase dominated with low frequency modulation (mode VIII), asymmetric synchronized anti-phase (mode IX), or irregular (mode IV). For the gap ratio larger than 4, only synchronized anti-phase mode was observed under the conditions of this study. In the two vortex streets regime, shedding frequency is higher than that of a single cylinder, due to a stronger gap flow than that in the freestream side. The impact of gap ratio and Reynolds number on the drag and lift forces was also studied. Published by AIP Publishing.
机译:通过在低雷诺数(16-200)下的直接数值模拟研究了两个并排的方形圆柱的苏醒。两个圆柱体之间的间隙从0到10D不等,其中D是方形圆柱体的尺寸(边缘长度)。识别并分析了9种不同的尾流模式及其对雷诺数和间隙间距的依赖性。对于这9个唤醒模式,得出了由雷诺数和间隙比g *(g / D,其中g是2个圆柱体之间的间隙间距)划分的系统分类图。当雷诺数低于临界雷诺数(取决于g *)时,观察到稳态唤醒(模式I)。当间隙比小于0.7时,仅观察到单个涡街。单个涡街唤醒可以是对称和周期性的(模式II),也可以是非对称和周期性的(模式III),也可以是不规则的(模式IV)。在该间隙比范围(小于0.7)中,由于间隙流的阻尼作用,脱落频率随着间隙比而降低。对于大于0.7的间隙比,还观察到两个涡街。当间隙比大于1时,仅观察到两个涡街。涡流脱落可以是同步和同相(模式V),同步和反相(模式VI),以低频调制为主的同相(模式VII),以低频调制为主的反相(模式VIII)。 ,非对称同步反相(模式IX)或不规则同步(模式IV)。对于大于4的间隙比,在此研究条件下仅观察到同步反相模式。在两个涡街状态下,由于间隙流比自由流侧的间隙流强,所以脱落频率高于单个气缸。还研究了间隙比和雷诺数对阻力和升力的影响。由AIP Publishing发布。

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