2016
DOI: 10.1093/mnras/stw3182
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Non-linear regimes in mean-field full-sphere dynamo

Abstract: The mean-field dynamo model is employed to study the non-linear dynamo regimes in a fully convective star of mass 0.3M rotating with period of 10 days. For the intermediate value of the parameter of the turbulent magnetic Prandl number, P m T = 3 we found the oscillating dynamo regimes with period about 40Yr. The higher P m T results to longer dynamo periods. If the large-scale flows is fixed we find that the dynamo transits from axisymmetric to non-axisymmetric regimes for the overcritical parameter of the αe… Show more

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Cited by 22 publications
(28 citation statements)
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“…This coexistence confirms the mean-field calculation (e.g. Rädler et al 1990;Elstner & Rüdiger 2007;Pipin 2017), where an anisotropic α tensor can generate non-axisymmetric fields.…”
Section: Anisotropy Of the α Tensorsupporting
confidence: 88%
“…This coexistence confirms the mean-field calculation (e.g. Rädler et al 1990;Elstner & Rüdiger 2007;Pipin 2017), where an anisotropic α tensor can generate non-axisymmetric fields.…”
Section: Anisotropy Of the α Tensorsupporting
confidence: 88%
“…This is a layer in the top 40 Mm of the Sun, where ∂Ω/∂r < 0, which causes equatorward migrating dynamo waves when α is positive in the northern hemisphere (Brandenburg 2005a). Such a dynamo model has been developed by and Pipin (2017). Cameron & Schüssler (2017) have presented an updated version of the one-dimensional phenomenological dynamo model of Leighton (1969) by including a number of effects such as the evolution of the radially integrated toroidal magnetic field, the latitudinal variation of the surface angular velocity, turbulent downward pumping, and several other features.…”
Section: The Solar Dynamo Dilemmamentioning
confidence: 99%
“…where, E = u × b is the mean electromotive force with u and b standing for the turbulent fluctuating velocity and magnetic field respectively. Similar to our recent paper (see, [67,62]), we employ the mean electromotive force in form: where symmetric tensor α ij models the generation of magnetic field by the α-effect; antisymmetric tensorγ ij controls the mean drift of the large-scale magnetic fields in turbulent medium, including the magnetic buoyancy; the tensor η ijk governs the turbulent diffusion. The reader can find further details about the E in the above cited papers.…”
Section: Dynamo Equationsmentioning
confidence: 99%