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Spectral energy dynamics in magnetohydrodynamic turbulence

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arxiv physics/0509019 v1 pith:FFSFJ4NG submitted 2005-09-02 physics.flu-dyn physics.plasm-ph

classification physics.flu-dynphysics.plasm-ph
keywords mathrmenergyperpcasefieldisotropicmagneticmean
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abstract

Spectral direct numerical simulations of incompressible MHD turbulence at a resolution of up to $1024^3$ collocation points are presented for a statistically isotropic system as well as for a setup with an imposed strong mean magnetic field. The spectra of residual energy, $E_k^\mathrm{R}=|E_k^\mathrm{M}-E_k^\mathrm{K}|$, and total energy, $E_k=E^\mathrm{K}_k+E^\mathrm{M}_k$, are observed to scale self-similarly in the inertial range as $E_k^\mathrm{R}\sim k^{-7/3}$, $E_k\sim k^{-5/3}$ (isotropic case) and $E^\mathrm{R}_{k_\perp}\sim k_\perp^{-2}$, $E_{k_\perp}\sim k_\perp^{-3/2}$ (anisotropic case, perpendicular to the mean field direction). A model of dynamic equilibrium between kinetic and magnetic energy, based on the corresponding evolution equations of the eddy-damped quasi-normal Markovian (EDQNM) closure approximation, explains the findings. The assumed interplay of turbulent dynamo and Alfv\'en effect yields $E_k^\mathrm{R}\sim k E^2_k$ which is confirmed by the simulations.

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  1. Polarization geometry of magnetohydrodynamic turbulence

    astro-ph.SR 2026-07 conditional novelty 6.0 of 10

    MHD turbulence can be described by a polarization vector on a generalized Poincaré sphere whose rotation and diffusion map onto k^-1, k^-3/2, and k^-5/3 spectral regimes.

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