Numerical Analysis of Second-Order Mean Wave Forces by a Stabilized Higher Order Boundary Element Method

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Abstract

A stabilized Higher-Order Boundary Element Method (HOBEM) based on cubic shape functions is presented to solve the linear wave-structure interaction with the presence of steady or slowly varying velocities. The m-terms which involves second derivatives of local steady flow are difficult to calculate accurately on structure surfaces with high curvatures. They are also not integrable at the sharp corners. A formulation of the Boundary Value Problem (BVP) in a body-fixed coordinate system is thus adopted, which avoids the calculation of the m-terms. The use of body-fixed coordinate system also avoid the inconsistency in the traditional perturbation method when 2nd order slowly-vary motions are larger than the linear motions. The stabilized numerical method presented in this paper is based on streamline integration and biased differencing scheme along the streamlines. The presence of convective terms in the kinematic and dynamic free surface conditions will lead to instable solution if the explicit method is used. Thus a fully implicit scheme is used in this paper for the time integration of kinematic and dynamic free surface conditions. In an implicit scheme, solution of an additional matrix equation is normally required due to the fact that the presence of convective terms are approximated using the variables at current time step rather than the previous time steps only. A method that avoids solving such matrix equation is presented in this paper, which will reduce the computational efforts in the implicit method. The methodology is applicable on unstructured meshes. It can also be used in general second order wave-structure interaction analysis with presence of steady or slowly-varying velocities.
用稳定高阶边界元法数值分析二阶平均波浪力
提出了一种基于三次形状函数的稳定高阶边界元法(HOBEM),用于求解存在定速或慢速变化的线性波-结构相互作用问题。在高曲率结构表面上,涉及局部定常流二阶导数的m项难以精确计算。它们在尖角处也是不可积的。采用定体坐标系下边值问题(BVP)的表述,避免了m项的计算。采用定体坐标系也避免了传统摄动法在二阶慢变运动大于线性运动时的不一致性。本文提出的稳定数值方法是基于流线积分和沿流线的偏微分格式。在运动和动力自由曲面条件下存在对流项,采用显式方法求解会导致求解不稳定。因此,本文采用一种完全隐式格式对运动和动力自由曲面条件进行时间积分。在隐式格式中,通常需要解一个额外的矩阵方程,因为对流项的存在是用当前时间步长的变量来近似的,而不是只用以前的时间步长的变量。本文提出了一种避免求解此类矩阵方程的方法,减少了隐式方法的计算量。该方法适用于非结构化网格。它也可用于一般的二阶波-结构相互作用分析,其中存在稳定或缓慢变化的速度。
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