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arXiv 0910.3175physics.flu-dyn
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激波加速涡环

Shock accelerated vortex ring

N. Haehn, C. Weber, J. Oakley, M. Anderson, D. Rothamer, R. Bonazza

摘要:

激波与球形密度不均匀体的相互作用通过斜压涡度的脉冲沉积导致涡环的发展。目前的流体动力学视频显示这种现象,并在威斯康星州激波管实验室(WiSTL)的9.2米,向下射击激波管进行了实验研究。该管具有方形内部横截面(0.25 m x 0.25 m),具有用于光学访问的多个熔融石英窗口。球形肥皂泡是由一个可伸缩的注射器产生的,并释放到自由落体200毫秒前的初始冲击加速。向下运动的M = 2.07的冲击波使气泡冲动地加速并从管端壁反射。反射的冲击波使气泡重新加速(再冲击),气泡现在已经发展成涡环,沉积了额外的涡量。在没有任何流动扰动的情况下,反射激波后面的流动是静止的。因此,任何观察到的涡环运动都是由于环流造成的。冲击涡环成像在12,500 fps的平面米氏散射。

英文摘要:

The interaction of a shock wave with a spherical density inhomogeneity leads to the development of a vortex ring through the impulsive deposition of baroclinic vorticity. The present fluid dynamics videos display this phenomenon and were experimentally investigated at the Wisconsin Shock Tube Laboratory's (WiSTL) 9.2 m, downward firing shock tube. The tube has a square internal cross-section (0.25 m x 0.25 m) with multiple fused silica windows for optical access. The spherical soap bubble is generated by means of a pneumatically retracted injector and released into free-fall 200 ms prior to initial shock acceleration. The downward moving, M = 2.07 shock wave impulsively accelerates the bubble and reflects off the tube end wall. The reflected shock wave re-accelerates the bubble (reshock), which has now developed into a vortex ring, depositing additional vorticity. In the absence of any flow disturbances, the flow behind the reflected shock wave is stationary. As a result, any observed motion of the vortex ring is due to circulation. The shocked vortex ring is imaged at 12,500 fps with planar Mie scattering.

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