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Earthquake induced sloshing and hydrodynamic pressures in rigid liquid storage tanks analyzed by coupled acoustic-structural and Euler-Lagrange methods

机译:刚性液体储罐中地震诱发的晃荡和水动力压力,通过声学-结构和欧拉-拉格朗日耦合法分析

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摘要

Three-dimensional (3-D) ground-supported cylindrical and rectangular rigid liquid storage tanks filled with water and subjected to seismic base excitation are investigated using finite element method (FEM). The analyses of the tanks are carried out using coupled acoustic-structural (CAS) and coupled Eulerian-Lagrangian (CEL) approaches of the FEM using Abaqus(center dot).. The CAS approach based on linear wave theory and the CEL approach based on non-linear wave theory are used here to study the fluid-structure interaction (FSI) behavior of the tanks. Sloshing displacement, impulsive, convective, and total hydrodynamic pressures are investigated for varying geometries of the tanks. The small amplitude sloshing and hydrodynamic pressure responses are compared between the two FE-based, CAS and CEL approaches. The results obtained from the present FE-based analysis approaches are found to be in close agreement with the experimentally obtained seismic response in the 3-D cylindrical and rectangular tanks subjected to seismic ground motions. The ratio of peak sloshing height (h) to liquid height in the tank (H-L) obtained in the cylindrical tank using the CAS approach is 0.0425 and that by the CEL is 0.039, whereas for rectangular tank it is 0.060 by the CAS approach and 0.046 by the CEL approach; thereby, signifying relatively small sloshing amplitude response. It is concluded that the non-linearity of the sloshing wave displacement does not play a significant role while calculating the hydrodynamic pressure distribution on the rigid tank walls.
机译:使用有限元方法(FEM)研究了装有水并经受地震基础激励的三维(3-D)地面支撑圆柱和矩形刚性液体储罐。使用Abaqus(中心点)对FEM进行耦合分析,采用耦合的声学结构(CAS)方法和耦合的欧拉-拉格朗日(CEL)方法进行油箱分析。基于线性波理论的CAS方法和基于线性波理论的CEL方法非线性波理论在这里用来研究储罐的流固耦合行为。研究了不同几何形状储罐的晃动位移,脉冲,对流和总流体动力压力。比较了两种基于有限元,CAS和CEL的方法之间的小幅度晃动和流体动力压力响应。发现从当前基于有限元分析方法获得的结果与经受地震地面运动的3-D圆柱形和矩形罐中通过实验获得的地震响应非常吻合。使用CAS方法获得的圆柱形储罐中的晃荡峰值高度(h)与储罐中液体高度(HL)之比为0.0425,通过CEL获得的峰值晃动高度(h)为0.039,而对于采用CAS方法的矩形储罐而言,其为0.060和0.046通过CEL方法;因此,表示相对较小的晃动幅度响应。结论是,在计算刚性罐壁上的动水压力分布时,晃荡位移的非线性不起作用。

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