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Lagrangian-Eulerian enforcement of non-homogeneous boundary conditions in the Particle Finite Element Method

机译:拉格朗日 - 欧拉·欧拉斯在颗粒有限元法中强制执行非均质边界条件

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摘要

The Particle Finite Element Method (PFEM) is a Lagrangian finite element method with frequent remeshing, particularly suited for the simulation of fluid motions with evolving free surfaces, e.g., in the case of breaking waves or fluid-structure interactions with large displacements of the interaction surface. While the method has been successfully employed in a number of different engineering applications, there are several circumstances of practical interest where the Lagrangian nature of the method makes it difficult to enforce non-homogeneous boundary conditions. A novel mixed Lagrangian-Eulerian technique is proposed to the purpose of simplifying the imposition of this type of conditions with the PFEM. The method is simple to implement and computationally convenient, since only nodes on the boundary are considered Eulerian, while nodes inside the fluid body maintain their Lagrangian nature. A number of 2D and 3D examples, with analytical and numerical validations, confirm the excellent performance of the method.
机译:颗粒有限元方法(PFEM)是一种频繁倒闭的拉格朗日有限元方法,特别适用于模拟流体运动,其具有不断的自由表面,例如,在断开波浪或流体 - 结构与相互作用的大型位移的情况下的情况下表面。虽然该方法已经成功地在许多不同的工程应用中使用,但是在虽然具有若干实际兴趣的情况下,该方法的拉格朗日性质使得难以实施非均匀的边界条件。提出了一种新颖的混合拉格朗日 - 欧拉欧洲技术,以简化与PFEM的这种类型的条件施加。该方法易于实施和计算方便,因为边界上的节点被视为欧拉,而流体体内的节点保持着他们的拉格朗日性质。许多2D和3D示例,具有分析和数值验证,确认了该方法的优异性能。

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