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首页> 外文期刊>Journal of Fluid Mechanics >Hydrodynamics of swimming in stingrays: numerical simulations and the role of the leading-edge vortex
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Hydrodynamics of swimming in stingrays: numerical simulations and the role of the leading-edge vortex

机译:在黄貂鱼中游泳的流体力学:数值模拟和前沿涡旋的作用

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Stingrays, in contrast with many other aquatic animals, have flattened disk-shaped bodies with expanded pectoral 'wings', which are used for locomotion in water. To discover the key features of stingray locomotion, large-eddy simulations of a self-propelled stingray, modelled closely after the freshwater stingray, Potamotrygon orbignyi, are performed. The stingray's body motion was prescribed based on three-dimensional experimental measurement of wing and body kinematics in live stingrays at two different swimming speeds of 1.5 and 2.5L s(-1) (L is the disk length of the stingray). The swimming speeds predicted by the self-propelled simulations were within 12% of the nominal swimming speeds in the experiments. It was found that the fast-swimming stingray (Reynolds number Re = 23 000 and Strouhal number St = 0.27) is approximately 12% more efficient than the slow-swimming one (Re = 13 500, St = 0.34). This is related to the wake of the fast- and slow-swimming stingrays, which was visualized along with the pressure on the stingray's body. A horseshoe vortex was discovered to be present at the anterior margin of the stingray, creating a low-pressure region that enhances thrust for both fast and slow swimming speeds. Furthermore, it was found that a leading-edge vortex (LEV) on the pectoral disk of swimming stingrays generates a low-pressure region in the fast-swimming stingray, whereas the low- and high-pressure regions in the slow-swimming one are in the back half of the wing and not close to any vortical structures. The undulatory motion creates thrust by accelerating the adjacent fluid (the added-mass mechanism), which is maximized in the back of the wing because of higher undulations and velocities in the back. However, the thrust enhancement by the LEV occurs in the front portion of the wing. By computing the forces on the front half and the back half of the wing, it was found that the contribution of the back half of the wing to thrust in a slow-swimming stingray is several-fold higher than in the fast-swimming one. This indicates that the LEV enhances thrust in fast-swimming stingrays and improves the efficiency of swimming.
机译:与许多其他水生动物相比,黄貂鱼的圆盘状身体变扁平,具有扩展的胸“翼”,用于在水中运动。为了发现黄貂鱼运动的关键特征,对自推进式黄貂鱼进行大涡模拟,并在淡水黄貂鱼Potamotrygon orbignyi之后进行了建模。根据在三个不同的游泳速度1.5和2.5L s(-1)(L是圆盘的盘长)下,对活live的翼和身体运动进行三维实验测量,规定了prescribed的身体运动。自推进模拟预测的游泳速度在实验中的标称游泳速度的12%以内。发现快速游动的黄貂鱼(雷诺数Re = 23 000,斯特劳哈尔数St = 0.27)比慢游动的黄貂鱼(Re = 13 500,St = 0.34)高约12%。这与快速和缓慢游动的黄貂鱼的唤醒有关,该现象与黄貂鱼身上的压力一并显示。发现在黄貂鱼的前缘存在马蹄涡,形成了一个低压区域,该区域增强了快速和慢速游泳时的推力。此外,还发现游泳swimming鱼的胸盘上的前沿涡流(LEV)在快速游泳的ing鱼中产生低压区域,而在慢速游泳的ing鱼中的低压和高压区域则是低压区。在机翼的后半部,不靠近任何涡旋结构。起伏运动通过加速相邻的流体(附加质量机制)而产生推力,由于机翼后部的起伏和速度较高,因此在机翼后部最大化。但是,LEV的推力增强发生在机翼的前部。通过计算机翼前半部和后半部的力,发现机翼后半部对推入缓慢游泳的黄貂鱼的贡献要比快速游泳的黄貂鱼高几倍。这表明LEV可以增强快速游泳的黄貂鱼的推力并提高游泳效率。

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