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A mixed implicit–explicit finite difference scheme for heat transport in magnetised plasmas

机译:磁化等离子体传热的混合隐式-显式有限差分格式

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摘要

An explicit/implicit domain decomposition method is applied to the time-dependent heat-conduction problem in a 2-d, strongly anisotropic medium (a magnetised plasma), using a formulation of the spatial derivatives which avoids the pollution of perpendicular by parallel heat fluxes. The time-stepping at the sub-domain boundaries is done using a DuFort–Frankel scheme, which leads to a time step limit given not by instabilities, but by the damping rate of numerical oscillations driven by inconsistencies in the formulation of initial conditions or the temporal variations in the true physical solution. These limitations can be minimized, however, by aligning the subdomain boundaries as much as possible with magnetic flux surfaces. The time step limit depends on the ratio of the implicit grid spacing to the distance between subdomain boundaries (DuFort–Frankel lines in 2-d, surfaces in 3-d).
机译:显式/隐式域分解方法适用于二维强各向异性介质(磁化等离子体)中随时间变化的导热问题,采用空间导数公式,避免了平行热通量对垂直方向的污染。使用DuFort-Frankel方案完成子域边界上的时间步长,这导致了时间步长限制,而不是由不稳定性引起,而是由初始条件或公式的不一致性所驱动的数值振荡的阻尼率给出的。真实物理解中的时间变化。但是,可以通过将子域边界与磁通量表面尽可能对齐来使这些限制最小化。时间步长限制取决于隐式网格间距与子域边界之间的距离的比例(二维中的DuFort–Frankel线,三维中的表面)。

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