1998
DOI: 10.1103/physreve.57.r21
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von Kármán–Howarth equation for magnetohydrodynamics and its consequences on third-order longitudinal structure and correlation functions

Abstract: A derivation in variable dimension of the scaling laws for mixed third-order longitudinal structure and correlation functions for incompressible magnetized flows is given for arbitrary correlation between the velocity and magnetic field with full isotropy, homogeneity, and incompressibility assumed. When close to equipartition between kinetic and magnetic energy, the scaling relations involve only structure functions in a manner similar to the '' 4 5 law'' of Kolmogorov.

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Cited by 305 publications
(256 citation statements)
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“…These triple correlations are time dependent, although this is not indicated in the notation here. One can demonstrate that the pressure terms do not contribute to (2.5) (Politano & Pouquet 1998b), as is also the case for hydrodynamics (de Kármán & Howarth 1938).…”
Section: Von Kármán-howarth Equations For Mhdmentioning
confidence: 92%
“…These triple correlations are time dependent, although this is not indicated in the notation here. One can demonstrate that the pressure terms do not contribute to (2.5) (Politano & Pouquet 1998b), as is also the case for hydrodynamics (de Kármán & Howarth 1938).…”
Section: Von Kármán-howarth Equations For Mhdmentioning
confidence: 92%
“…For K-41 hydrodynamic turbulence for we have the "4/5" law <δv 3 L >∼−4/5L (e.g. Frisch, 1995) determined from the Navier-Stokes equations (for the equivalent relation for isotropic MHD see Politano and Pouquet, 1998). This follows since <δv 3 >/L is the energy transfer rate.…”
Section: Scaling Exponents Mhd Turbulence Models and Similarity Analmentioning
confidence: 92%
“…Note that the term involving mixed correlations of the velocity and magnetic fields contains the field B rather than its increment δB -this hints at the nonlocality of the interaction between u and B, which, as explained in §1, is the fundamental feature of MHD turbulence. Equation (2.2) was derived by Chandrasekhar (1951) (see also Politano & Pouquet 1998b). He also found the two other exact laws of MHD turbulence by constructing evolution equations analogous to equation (2.1) for B i B ′ j and u i B ′ j (representing the magnetic-energy and the cross-helicity budgets, respectively).…”
Section: Exact Scaling Laws For Isotropic Mhd Turbulencementioning
confidence: 99%