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Structure-preserving discretization of incompressible fluids

机译:不可压缩流体的保结构离散化

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摘要

The geometric nature of Euler fluids has been clearly identified and extensively studied over the years, culminating with Lagrangian and Hamiltonian descriptions of fluid dynamics where the configuration space is defined as the volume-preserving diffeomorphisms, and Kelvin's circulation theorem is viewed as a consequence of Noether's theorem associated with the particle relabeling symmetry of fluid mechanics. However computational approaches to fluid mechanics have been largely derived from a numericalanalytic point of view, and are rarely designed with structure preservation in mind, and often suffer from spurious numerical artifacts such as energy and circulation drift. In contrast, this paper geometrically derives discrete equations of motion for fluid dynamics from first principles in a purely Eulerian form. Our approach approximates the group of volume-preserving diffeomorphisms using a finite-dimensional Lie group, and associated discrete Euler equations are derived from a variational principle with non-holonomic constraints. The resulting discrete equations of motion yield a structure-preserving time integrator with good long-term energy behavior and for which an exact discrete Kelvin's circulation theorem holds.
机译:多年来,欧拉流体的几何性质已被清楚地识别并进行了广泛的研究,最终以流体动力学的拉格朗日和汉密尔顿主义描述为最终结果,其中构型空间被定义为体积守恒的微分形,开尔文的循环定理被认为是Noether的结果。定理与流体力学的粒子重新标记对称性有关。然而,流体力学的计算方法主要是从数值分析的观点出发的,很少考虑结构的保留而设计,并且经常遭受虚假的数值假象,例如能量和循环漂移。相反,本文从纯粹的欧拉形式的第一原理以几何学的方式导出了流体动力学的离散运动方程。我们的方法使用有限维李群来近似表示保体积微分群,并且相关联的离散欧拉方程是从具有非完整约束的变分原理导出的。由此产生的离散运动方程式产生了一个具有良好长期能量行为的结构保持时间积分器,并为此保留了精确的离散开尔文循环定理。

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