An explicit mapped tent pitching scheme for Maxwell equations
An explicit mapped tent pitching scheme for Maxwell equations
复制标题
麦克斯韦方程的显式映射帐篷倾斜方案
DOI:
10.1007/978-3-030-39647-3_28
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发表时间:
2020
期刊:
影响因子:
--
通讯作者:
Wintersteiger, Christoph
中科院分区:
文献类型:
--
作者:
Gopalakrishnan, Jay;Hochsteger, Matthias;Schöberl, Joachim;Wintersteiger, Christoph
Electromagnetic waves propagate at the speed of light. Thus, the field at a certain point in space and time depends only on field values within a dependency cone. A tent pitching method introduces a special “causal” spacetime mesh that respects this finite speed of propagation. It is not limited to Maxwell equations, but can be applied to general hyperbolic equations. A tent pitching method requires a numerical scheme to discretize the equation on that mesh. Discontinuous Galerkin (DG) methods are of particular interest since they offer a systematic avenue to build high order methods. For a given initial condition at the bottom of a tent, the discrete equations may be solved within each individual tent, up to the tent top. The computed solution at the tent top provides initial conditions for the tents that follow later in time. This method is highly parallel, since many tents can be solved independently. Methods using such tent-pitched meshes may be traced back to [5, 7]. More recent works [1, 6, 8] develop Spacetime DG (SDG) methods within tents by formulating local variational problems, for which linear systems are set up and solved. Although these systems are local, the matrix size can grow rapidly with the polynomial order, especially in four-dimensional spacetime tents. In this context