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.
Global solutions to Stokes-Magneto equations with fractional dissipations
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abstract
In this paper, we investigate a Stokes-Magneto system with fractional diffusions. We first deal with the non-resistive case in $\mathbb{T}^{d}$ and establish the local and global well-posedness with initial magnetic field $\mathbf{b}_0\in H^{s}(\mathbb{T}^d)$. We also show the existence of a unique mild solution of the resistive case with initial data $\mathbf{b}_0$ in the critical $L^{p}(\mathbb{R}^d)$ space. Moreover, we show that $\|\mathbf{b}(t)\|_{L^{p}}$ converges to zero as $t\rightarrow\infty$ when the initial data is sufficiently small.
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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.