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Articles

Kinetic-magnetic energy exchanges in rotating magnetohydrodynamic turbulence

ORCID Icon, , , , &
Pages 263-284 | Received 10 Apr 2019, Accepted 03 May 2019, Published online: 31 May 2019
 

ABSTRACT

We use direct numerical simulations to study the dynamics of incompressible homogeneous turbulence subjected to a uniform magnetic field B in a rotating frame with rotation vector Ω. We consider two cases: ΩB and ΩB. The initial state is homogeneous isotropic hydrodynamic turbulence with Reynolds number Re=ull/ν170. The magnetic Prandtl number Pm=ν/η=1 and the Elsasser number Λ=B2/(2Ωη)=0.5, 0.9 or 2. For both the cases ΩB and ΩB, the total energy decays as t5/7 for Λ=0.5 and 0.9, and as t6/7 for Λ=2. In the spectral range 2 < k < 20, the kinetic energy spectrum scales as kp where p increases with time (2p4.2). This scaling is similar to that observed in quasi-static MHD. The two rotating MHD flow cases differ mainly in how kinetic and magnetic fluctuations exchange energy, with a mechanism mostly driven by the dynamics of the spectral buffer layer around kΩ=|Ωk|/Ω0. At kΩ=0, the inertial and Alfvén waves frequencies vanish when ΩB, but only the inertial waves frequency vanishes when ΩB. When ΩB, rotation results in an increased reduction of magnetic fluctuations generation. In terms of anisotropy, we show that the elongated structures occurring in rapidly non-magnetised rotating flows are distorted or inhibited for ΩB, and weakened for ΩB.

Disclosure statement

No potential conflict of interest was reported by the authors.

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