Turbulent magnetic Prandtl number and magnetic diffusivity quenching from simulations
Tarek A. Yousef, Axel Brandenburg, G. Rüdiger
Abstract
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Tarek A. Yousef, Axel Brandenburg, G. Rüdiger
Abstract
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Forced turbulence simulations are used to determine the turbulent kinematic viscosity, , from the decay rate of a large scale velocity field. Likewise, the turbulent magnetic diffusivity, , is determined from the decay of a large scale magnetic field. In the kinematic regime, when the field is weak, the turbulent magnetic Prandtl number, , is about unity. When the field is nonhelical, is quenched when magnetic and kinetic energies become comparable. For helical fields the quenching is stronger and can be described by a dynamical quenching formula.
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Forced turbulence simulations are used to determine the turbulent kinematic viscosity, , from the decay rate of a large scale velocity field. Likewise, the turbulent magnetic diffusivity, , is determined from the decay of a large scale magnetic field. In the kinematic regime, when the field is weak, the turbulent magnetic Prandtl number, , is about unity. When the field is nonhelical, is quenched when magnetic and kinetic energies become comparable. For helical fields the quenching is stronger and can be described by a dynamical quenching formula.
Key concepts: Magnetic Prandtl number, Magnetic diffusivity, Prandtl number, Turbulence, Magnetic field, Physics, Turbulent Prandtl number, Thermal diffusivity