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Fully nonlinear simulation of resonant motion of liquid confined between floating structures

机译:浮动结构之间的液体共振运动的完全非线性模拟

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摘要

A finite element based numerical method is employed to analyze the resonant oscillations of the liquid confined within multiple floating bodies based on fully nonlinear wave theory. The velocity potentials at each time step are obtained through the finite element method (FEM) with quadratic shape functions. The matrix equation of the FEM is solved through an iteration. The waves at the open boundary are absorbed by the method of combination of the damping zone method and the Sommerfeld-Orlanski equation. Numerical examples are given by floating two rectangular cylinders, two wedge-shaped cylinders and two semi elliptic cylinders undergoing forced oscillations at the resonant frequencies. The numerical results are compared with the first and second order solutions by previous study, which showed that the first order resonance happens at the odd order natural frequencies ω_(2i-i)(i = 1, 2, ...) and second order resonance at the half of even order ω_(2i)/2(i = 1, 2, ...) for antisymmetric motions and happen at ω_(2i)(I = 1, 2, ) and ω_(2i)/2(i = 1, 2 ...) for symmetric motions, and it is found that they are in good agreement in smaller amplitude motions within a sufficiently long period of time. However, difference begins to appear as time increases further. This happens even in smaller amplitude motions. In all the calculated cases, the results always become periodic in time eventually.
机译:基于完全非线性波动理论,基于有限元的数值方法被用来分析封闭在多个浮体中的液体的共振。通过具有二次形状函数的有限元方法(FEM)获得每个时间步的速度势。 FEM的矩阵方程式通过迭代求解。开放边界处的波通过阻尼区方法和Sommerfeld-Orlanski方程相结合的方法吸收。通过浮动两个矩形圆柱体,两个楔形圆柱体和两个半椭圆形圆柱体在共振频率下进行强制振荡给出了数值示例。通过先前的研究将数值结果与一阶和二阶解进行比较,结果表明一阶共振发生在奇数阶固有频率ω_(2i-i)(i = 1,2,...)和二阶固有频率上反对称运动在偶数阶ω_(2i)/ 2(i = 1,2,...)的一半处发生共振,并在ω_(2i)(I = 1,2,)和ω_(2i)/ 2(对于对称运动,i = 1,2 ...),并且发现它们在足够长的时间段内以较小幅度的运动非常吻合。但是,随着时间的增加,差异开始出现。即使在较小幅度的运动中也会发生这种情况。在所有计算的情况下,结果最终总是在时间上变为周期性的。

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