Statistical Theory of Anisotropic Magnetohydrodynamic Turbulence: an Approach to Strong Shear Alfvén Turbulence by Direct-Interaction Approximation

Astronomy and Astrophysics – Astronomy

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Ism: General, Magnetohydrodynamics: Mhd, Turbulence

Scientific paper

We develop a statistical theory of strong, homogeneous, and anisotropic MHD turbulence within a framework of the Eulerian direct-interaction approximation (DIA). Analysis is concentrated on stationary shear Alfvén turbulence of which the mean magnetic field is uniform. We assume that timescales of the Alfvén wave and the energy cascade in the energy-containing range (ECR) are much larger than the cascade timescale in the inertial range (InR). Thereby, we can obtain DIA equations governing the time evolution of the propagator and the correlation functions in analytically solvable form. The solutions of the DIA equations include an Alfvén oscillation factor depending on k_z and a relaxation factor depending on k_⊥. Here k_z and k_⊥ are the wavenumbers parallel to and perpendicular to the mean magnetic field, respectively. Applying the result to the DIA equation of spectral energy transfer, we can show high anisotropy of energy cascades; that is, energy cascades to higher k_z modes are inhibited, hence only k_⊥ cascades occur. Thus, InR extends to much larger k_⊥ than ECR while the k_z-band broadening is suppressed. Motivated by this, we assume the functional form of the energy spectrum of InR to be E(k_⊥,k_z)~k^-mu_⊥delta(k_z) and find that mu=5/2 hence we obtain the corresponding one-dimensional spectrum, k_⊥-∞ ∞ dk_zE(k_⊥,k_z)~k^- 3/2_⊥. Furthermore, we show the importance of the three-wave resonances for energy cascades in MHD turbulence. Our theory probably suffers spurious convection effects, and therefore so does the resultant energy spectrum. Nevertheless, it can be a good starting point toward refined theories applicable to real astrophysical MHD turbulence.

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