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A three-dimensional finite element arbitrary Lagrangian-Eulerian method for shock hydrodynamics on unstructured grids

机译:非结构网格上冲击水动力的三维有限元任意拉格朗日-欧拉方法

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We present a three-dimensional (3D) finite element (FE) arbitrary Lagrangian-Eulerian (ALE) method for shock hydrodynamics on unstructured grids. The method is based on an FE Eulerian Godunov scheme for linear tetrahedra that has been extended to include mesh motion in an unsplit, flux-conservative formulation. The proposed method eliminates the splitting errors present in traditional Lagrange-plus-remap methods that occur during the remap phase. Unlike typical unsplit approaches, the mesh velocity is not determined by boundary motion but is instead based on the local fluid velocity. Smoothing operations are then applied to the mesh velocity to avoid mesh tangling. This approach allows the mesh to follow the fluid motion in a robust manner and leverage one of the primary advantages of Lagrangian schemes for shock hydrodynamics, namely that the resolution follows the flow. An approximate Riemann solver is used to calculate fluxes in the co-moving frame of the mesh. Results for a number of standard test problems are presented for 3D meshes of up to 10~7 tetrahedra. Global convergence rates of 0.8-1.0 are observed for shock dominated flows and 1.9 for smooth flows. We also demonstrate that the method satisfies the discrete geometric conservation law to truncation error, conserves total energy to machine precision, and preserves symmetry.
机译:我们提出了一种三维(3D)有限元(FE)任意Lagrangian-Eulerian(ALE)方法,用于非结构网格上的冲击流体动力学。该方法基于针对线性四面体的FE Eulerian Godunov方案,该方案已扩展为以未分裂的,通量守恒的公式包含网格运动。所提出的方法消除了在传统的Lagrange-plus-remap方法中出现在重映射阶段的分裂错误。与典型的非分裂方法不同,网格速度不是由边界运动确定的,而是基于局部流体速度的。然后将平滑操作应用于网格速度,以避免网格纠缠。这种方法允许网格以鲁棒的方式跟随流体运动,并利用Lagrangian方案的主要优点之一进行冲击流体动力学,即分辨率随流动而变化。近似的黎曼求解器用于计算网格的共同运动框架中的通量。给出了多达10到7个四面体的3D网格的许多标准测试问题的结果。对于冲击为主的流动,整体收敛速度为0.8-1.0,对于平稳流动,则为1.9。我们还证明了该方法满足截断误差的离散几何守恒定律,节省了总能量以提高机器精度,并保持了对称性。

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