Abstract

We investigate the stability properties for a family of equations introduced by Moffatt to model magnetic relaxation. These models preserve the topology of magnetic streamlines, contain a cubic nonlinearity, and yet have a favorable L2L^2 energy structure. We consider the local and global in time well-posedness of these models and establish a difference between the behavior as t→∞t\to \infty with respect to weak and strong norms.

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