Turbulent relaxation processes in magnetohydrodynamics

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Abstract
Competing processes previously called ‘‘selective decay’’ and ‘‘dynamic alignment’’ are studied numerically for two‐dimensional magnetohydrodynamic turbulence. In selective decay, the energy decays relatively to mean‐square vector potential, and in dynamic alignment, the energy decays relatively to cross helicity. In the former case, the kinetic (fluid) energy decays to zero and the magnetic energy occupies the largest scales allowed by the boundary conditions. In the latter case, the velocity field and magnetic field become aligned and energetically equipartitioned. An extensive study of the initial value problem, with viscous and resistive dissipation, indicates that four distinct regimes of behavior are possible: a magnetically dominated regime, a velocity dominated regime, a dynamic alignment dominated regime, and a transition regime separating the others in parameter space. An analytical variational problem predicts several features seen in the computations, including geometrical alignment of velocity and magnetic fields, constraints on global quantities in the long‐time limit, and in some cases, condensation to long wavelength modes.

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