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arXiv 1012.2494math.NAcs.NAphysics.plasm-ph
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Vlasov-Poisson 方程的保正高阶半拉格朗日间断 Galerkin 格式

A positivity-preserving high-order semi-Lagrangian discontinuous Galerkin scheme for the Vlasov-Poisson equations

University of Wisconsin(威斯康星大学)

J. A. Rossmanith, D. C. Seal

AI总结:

针对 Vlasov-Poisson 方程,提出一种基于算子分裂的半拉格朗日间断 Galerkin 方法,实现质量守恒、保正性和高阶时间精度。

摘要:

Vlasov-Poisson 方程描述无碰撞等离子体的演化,通过概率密度函数(PDF)表示,该函数通过静电力自相互作用。数值求解该系统的主要困难之一是与中等至大速度相关的 PDF 部分带来的严格时间步长限制。等离子体物理社区中消除这些时间步长限制的主流方法是所谓的粒子网格(PIC)方法,它将分布函数离散为一组宏粒子,而电场在网格上表示。存在几种替代方法,包括完全拉格朗日、完全欧拉和所谓的半拉格朗日方法。本工作的重点是半拉格朗日方法,它从 PDF 和电场的基于网格的欧拉表示开始,然后通过拉格朗日动力学演化 PDF,最后将演化后的场投影回原始欧拉网格。特别地,我们在本工作中开发了一种方法,通过相空间中的高阶间断 Galerkin(DG)方法和时间上的算子分裂半拉格朗日方法离散 1+1 维 Vlasov-Poisson 系统。通过 Strang 算子分裂相对容易实现二阶时间精度。通过额外的工作,使用高阶分裂和高阶特征线法,我们还展示了如何将该格式推进到四阶时间精度。我们展示了如何解析所有拉格朗日动力学,使得质量精确守恒、保持正性并实现高阶精度。泊松方程通过最小模板局部间断 Galerkin(LDG)方法求解至高阶。我们在几个标准测试案例上测试了所提出的格式。

英文摘要:

The Vlasov-Poisson equations describe the evolution of a collisionless plasma, represented through a probability density function (PDF) that self-interacts via an electrostatic force. One of the main difficulties in numerically solving this system is the severe time-step restriction that arises from parts of the PDF associated with moderate-to-large velocities. The dominant approach in the plasma physics community for removing these time-step restrictions is the so-called particle-in-cell (PIC) method, which discretizes the distribution function into a set of macro-particles, while the electric field is represented on a mesh. Several alternatives to this approach exist, including fully Lagrangian, fully Eulerian, and so-called semi-Lagrangian methods. The focus of this work is the semi-Lagrangian approach, which begins with a grid-based Eulerian representation of both the PDF and the electric field, then evolves the PDF via Lagrangian dynamics, and finally projects this evolved field back onto the original Eulerian mesh. In particular, we develop in this work a method that discretizes the 1+1 Vlasov-Poisson system via a high-order discontinuous Galerkin (DG) method in phase space, and an operator split, semi-Lagrangian method in time. Second-order accuracy in time is relatively easy to achieve via Strang operator splitting. With additional work, using higher-order splitting and a higher-order method of characteristics, we also demonstrate how to push this scheme to fourth-order accuracy in time. We show how to resolve all of the Lagrangian dynamics in such a way that mass is exactly conserved, positivity is maintained, and high-order accuracy is achieved. The Poisson equation is solved to high-order via the smallest stencil local discontinuous Galerkin (LDG) approach. We test the proposed scheme on several standard test cases.

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