On the decay of low-magnetic-Reynolds-number turbulence in an imposed magnetic field

• Published in: Journal of fluid mechanics Vol. 651; pp. 295 - 318
• Main Authors: OKAMOTO, N., DAVIDSON, P. A., KANEDA, Y.
• Format: Journal Article
• Language: English
• Published: Cambridge, UK Cambridge University Press 25.05.2010
• Subjects: Decay; Exact sciences and technology; Fluid dynamics; Fluid mechanics; Fundamental areas of phenomenology (including applications); Isotropic turbulence; homogeneous turbulence; Magnetic fields; Physics; Physics of gases, plasmas and electric discharges; Physics of plasmas and electric discharges; Plasma turbulence; Reynolds number; Turbulent flow; Turbulent flows, convection, and heat transfer; Waves, oscillations, and instabilities in plasmas and intense beams; Low Reynolds number; Plasma turbulence; Theoretical study; Magnetic fields; Conducting fluid; MHD turbulence; Homogeneous turbulence
• ISSN: 0022-1120; 1469-7645
• DOI: 10.1017/S0022112009994137

We examine the integral properties of freely decaying homogeneous magnetohydrodynamic (MHD) turbulence subject to an imposed magnetic field B0 at low-magnetic Reynolds number. We confirm that, like conventional isotropic turbulence, the fully developed state possesses a Loitsyansky-like integral invariant, in this case I// = − ∫ r⊥2 〈 u⊥·u′⊥〉 dr, where 〈u(x) ·u(x + rc)〉 = 〈u·u′〉 is the usual two-point velocity correlation and the subscript ⊥ indicates components perpendicular to the imposed field. The conservation of I// for fully developed turbulence places a fundamental restriction on the way in which the integral scales can develop, i.e. it implies u⊥2 ℓ⊥4 ℓ// ≈ constant where u⊥, ℓ⊥ and ℓ// are integral scales. This constraint can be used to estimate the evolution of u⊥(t; B0), ℓ⊥(t; B0) and ℓ//(t; B0), and these theoretical decay laws are shown to be in good agreement with numerical simulations.