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Experiments on non-resonant sloshing in a rectangular tank with large amplitude lateral oscillation

机译:大振幅横向振动矩形水箱中非共振晃荡实验

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Flow of two dimensional nonlinear sloshing in a rigid rectangular tank with free surface is considered. The flow is generated by oscillating the container in a lateral harmonic motion, i.e., d* = A* sin(2πf*t*) where d* denotes the displacement of the container externally forced, A* the amplitude of displacement and/ the frequency. Thus, the maximum stroke, S*, of the container for a cycle, measured by a distance from the leftmost to the rightmost location on the container movement, is defined as S* = 2A*. It has performed a sequence of experiments on a variety of S*- and f*-values to investigate large amplitude sloshing flows at off-resonant condition far from the system natural frequency, where large amplitude means that the stroke, S*, of the container movement is comparable with the breadth, L', of the container, i.e., S*/L*~O(1) and the excitation acceleration is also comparable with the gravity, i.e., π~2(S*f*)~2/g*~O(1). Through PIV experiment, it shows that the flow physics on nonlinear off-resonant sloshing problem can be characterized into a combination of three peculiar sloshing motions: (1) standing wave motions which is similar with those of linear sloshing during run-down process, (2) run-up phenomenon like hydraulic jump along the vertical sidewall at the moment of turn-around of the container and (3) gradually propagating bore motion from one sidewall to the opposite wall which is similar with dam breaking problem.
机译:考虑具有自由表面的刚性矩形罐中二维非线性晃动的流动。通过以横向谐波运动使容器振动来产生流量,即d * = A * sin(2πf* t *),其中d *表示容器在外力作用下的位移,A *表示位移的幅度和/或频率。因此,将容器在一个循环中的最大行程S *定义为S * = 2A *,该最大行程S *由容器移动最左边到最右边的距离测量。它已对各种S *和f *值进行了一系列实验,以研究在远离系统自然频率的非共振条件下的大振幅晃荡流,其中大振幅表示电机的冲程S *。容器的运动与容器的宽度L'相称,即S * / L *〜O(1),激发加速度也与重力相称,即π〜2(S * f *)〜 2 /克*〜O(1)。通过PIV实验,表明非线性失谐晃荡问题的流动物理特性可以归纳为三种特殊的晃荡运动的组合:(1)驻波运动,其在下降过程中与线性晃荡相似,( 2)加速现象,例如在集装箱转弯时沿垂直侧壁发生水力跃迁,以及(3)逐渐使钻孔运动从一个侧壁向相对的壁传播,这与溃坝问题类似。

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