Randomly forced resistive magnetic relaxation yields, in the zero-resistivity limit, random MHS equilibria; in 2D the limit measure has zero mass on finite Fourier mode equilibria.
Computation of Magnetohydrodynamic Equilibria with Voigt Regularization
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abstract
This work presents the first numerical investigation of using Voigt regularization as a method for obtaining magnetohydrodynamic (MHD) equilibria without the assumption of nested magnetic flux surfaces. Voigt regularization modifies the MHD dynamics by introducing additional terms that vanish in the infinite-time limit, allowing for magnetic reconnection and the formation of magnetic islands, which can overlap and produce field-line chaos. The utility of this approach is demonstrated through numerical solutions of two-dimensional ideal and resistive test problems. Our results show that Voigt regularization can significantly accelerate the convergence to solutions in resistive MHD problems, while also highlighting challenges in applying the method to ideal MHD systems. This research opens up new possibilities for developing more efficient and robust MHD equilibrium solvers, which could contribute to the design and optimization of future fusion devices.
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MHS equilibria in the non-resistive limit to the randomly forced resistive magnetic relaxation equations
Randomly forced resistive magnetic relaxation yields, in the zero-resistivity limit, random MHS equilibria; in 2D the limit measure has zero mass on finite Fourier mode equilibria.