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A nonlinear dynamo wave riding on a spatially varying background


Bassom, AP and Kuzanyan, KM and Soward, AM, A nonlinear dynamo wave riding on a spatially varying background, Proceedings of the Royal Society A, 455, (1984) pp. 1443-1481. ISSN 1364-5021 (1999) [Refereed Article]

Copyright Statement

c 1999 The Royal Society

DOI: doi:10.1098/rspa.1999.0368


A systematic asymptotic investigation of a pair of coupled nonlinear one–dimensional amplitude equations, which provide a simplified model of solar and stellar magnetic activity cycles, is presented. Specifically, an αΩ–dynamo in a thin shell of small gap–to–radius ratio 𝛆 (≪ 1) is considered, in which the Ω–effect (the differential rotation) is prescribed but the α–effect is quenched by the finite–amplitude magnetic field. The unquenched system is characterized by a latitudinally θ–dependent dynamo number D, with a symmetric single–hump profile, which vanishes at both the pole, θ = π/2, and the equator, θ = 0, and has a maximum, D, at mid–latitude, θM = π/4. The shape D(θ)/D is fixed, so that there is only a single driving parameter D. At onset of global instability, D = DL(ε): = DT + O(ε), a travelling wave, of frequency ω = ωL(ε): = ωT+ O(ε) and wavelength O(ε), is localized at a low latitude θPT(< θM); DT and ωT are constants independent of ε. As a consequence of the spatial separation of θPT and θM, the squared field amplitude increases linearly with the excess dynamo number DDL in the weakly nonlinear regime, as usual, but with a large constant of proportionality dependent on some numerically small power of exp(1/ε). Whether the bifurcation is sub– or supercritical is extremely sensitive to the value of ε. In the nonlinear regime, the travelling wave localized at θPT at global onset expands and lies under an asymmetric envelope that vanishes smoothly at a low latitude θP but terminates abruptly on a length O(ε) – comparable to the wavelength – across a front at high latitude θF. The criterion of Dee and Langer, applied to the local linear evanescent disturbance ahead of the front, determines the lowest order value of the frequency close to the global onset value ωT. The global transition is characterized by the abrupt shift of θF from θPT to θM; during that passage, D executes O(ε-1) oscillations of increasing magnitude about DL. Fully developed nonlinearity occurs when θF > θM. In that regime, Meunier and co–workers showed that the O(1) quantities θFθM and (ωωT)/ε2/3 increase together in concert with DDT. By analysing the detailed structure of the front of width O(ε), we obtain ω correct to the higher order O(ε) and show improved agreement with numerical integrations performed by Meunier and co–workers of the complete governing equations at finite ε.

Item Details

Item Type:Refereed Article
Keywords:stellar dynamos, finite-amplitude waves, fronts, small aspect ratios, multiple-scale methods
Research Division:Mathematical Sciences
Research Group:Applied Mathematics
Research Field:Theoretical and Applied Mechanics
Objective Division:Expanding Knowledge
Objective Group:Expanding Knowledge
Objective Field:Expanding Knowledge in the Mathematical Sciences
Author:Bassom, AP (Professor Andrew Bassom)
ID Code:108041
Year Published:1999
Web of Science® Times Cited:21
Deposited By:Mathematics and Physics
Deposited On:2016-04-05
Last Modified:2016-07-08

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