Concetti Chiave
A robust fourth-order finite-difference discretization scheme is proposed for the strongly anisotropic heat transport equation characteristic of hot, fusion-grade plasmas. The scheme transforms mixed-derivative diffusion fluxes into nonlinear advective fluxes, enabling accurate multi-dimensional heat transport simulations with up to seven orders of magnitude of heat-transport-coefficient anisotropies.
Sintesi
The study proposes a practical implicit Eulerian spatio-temporal discretization for the strongly anisotropic heat transport equation in magnetized plasmas. Key features of the scheme include:
- Manageable numerical pollution for reasonable anisotropies up to χ∥/χ⊥ ∼ 10^7.
- Numerical robustness against developing negative temperatures for fourth-order accurate discretizations, and strict positivity for second-order ones.
- Strict local conservation properties.
- Suitability for modern nonlinear solvers (e.g., Jacobian-free Newton-Krylov) with efficient multigrid preconditioning for scalability.
- Compatibility and ease of implementation in existing finite-difference multiphysics simulation codes.
The scheme employs nonlinear flux limiters to reformulate mixed-derivative terms in the diffusion operator as nonlinear advection operators. This allows the use of positivity-preserving limiters that are compatible with nonlinear iterative solvers. The study also develops effective and scalable multigrid preconditioning strategies to render the linear and nonlinear iteration count manageable for sufficiently large timesteps.
The performance and accuracy of the scheme are demonstrated through several challenging numerical tests, including fully featured MHD simulations of kink instabilities in a Bennett pinch in 2D, and in the ITER fusion reactor in 3D. The results show that the scheme can handle very large anisotropies with minor performance degradation under mesh refinement, and that the average number of GMRES iterations per timestep scales as the square-root of the implicit timestep.
Statistiche
The maximum heat-transport anisotropy ratio considered in the tests is χ∥/χ⊥ = 2 × 10^6.
The maximum implicit timestep used in the tests is 3.1 × 10^6 times larger than the explicit stability limit.
Citazioni
"The numerical challenges are present both spatially and temporally. Spatially, strongly anisotropic diffusion equations suffer from numerical pollution of the perpendicular dynamics from the large parallel transport term, and the lack of a maximum principle (which may lead to negative temperatures)."
"Temporally, explicit methods are constrained to very small time steps due to the Courant stability condition, determined by the largest diffusion coefficient (i.e., the parallel transport one). For implicit methods, the issue is the near-degeneracy of the associated algebraic systems due to the strong transport anisotropy, and the ill-conditioning of associated algebraic systems that makes them difficult to invert using modern, efficient iterative methods."