2011
DOI: 10.1051/0004-6361/201016372
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Oscillatory dynamos and their induction mechanisms

Abstract: Context. Large-scale magnetic fields resulting from hydromagnetic dynamo action may differ substantially in their time dependence. Cyclic field variations, characteristic for the solar magnetic field, are often explained by an important Ω-effect, i.e., by the stretching of field lines because of strong differential rotation. Aims. The dynamo mechanism of a convective, oscillatory dynamo model is investigated. Methods. We solve the MHD-equations for a conducting Boussinesq fluid in a rotating spherical shell. W… Show more

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Cited by 59 publications
(36 citation statements)
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“…It is then a daunting possibility that we could be forced to stretch our simulations over very long temporal base-lines to find the actual long-lasting field configuration. More positively, our result, while in a different geometry, increases the importance of recent work on nonoscillatory αΩ and oscillatory α 2 modes in spherical shells for the solar dynamo (Mitra et al 2010;Schrinner et al 2011).…”
Section: Discussionmentioning
confidence: 49%
“…It is then a daunting possibility that we could be forced to stretch our simulations over very long temporal base-lines to find the actual long-lasting field configuration. More positively, our result, while in a different geometry, increases the importance of recent work on nonoscillatory αΩ and oscillatory α 2 modes in spherical shells for the solar dynamo (Mitra et al 2010;Schrinner et al 2011).…”
Section: Discussionmentioning
confidence: 49%
“…A butterfly diagram (not shown) of the azimuthally averaged radial field also shows poleward-propagating features. Such travelling nonaxisymmetric dynamo solutions have previously been observed in dynamos with free-slip boundary conditions (Schrinner et al 2011(Schrinner et al , 2012Käpylä et al 2013) and can be described in terms of the classical Parker-waves (Busse & Simitev 2006;Goudard & Dormy 2008;Schrinner et al 2012).…”
Section: Hydrodynamical Convectionmentioning
confidence: 99%
“…The first solar-like solutions, however, were obtained only recently (Schrinner et al 2011;Käpylä et al 2012;Augustson et al 2015), and only a couple of them have been run up to time scales of interest for detecting the irregular variations: the EULAG code Millennium simulation at solar rotation Norton et al 2014, hereafter EULAG-MHD) covers roughly 20 magnetic cycles of 80 years cycle length, while the ASH code simulation (Augustson et al 2015, hereafter ABMT), rotating at three times the solar rate, covers roughly 24 cycles with a cycle length of 6.2 years. The former does not exhibit significant irregular behavior and only very weak latitudinal migration of the magnetic field, while the latter produces a clearer equatorward migrating branch at lower latitudes and a poleward migrating branch at higher latitudes, especially pronounced in the radial field.…”
Section: Introductionmentioning
confidence: 99%