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Hydromagnetic waves in Earth's core and their influence on ...

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iAbstractIn this thesis east-west moti<strong>on</strong>s of Earth’s magnetic field <strong>on</strong> time scales of centuriesto millennia <str<strong>on</strong>g>and</str<strong>on</strong>g> associated patterns of field evoluti<strong>on</strong> at the <str<strong>on</strong>g>core</str<strong>on</strong>g> surface are studied.The hypothesis that hydromagnetic <str<strong>on</strong>g>waves</str<strong>on</strong>g> <str<strong>on</strong>g>in</str<strong>on</strong>g> Earth’s <str<strong>on</strong>g>core</str<strong>on</strong>g> c<strong>on</strong>tribute to such changes is<str<strong>on</strong>g>in</str<strong>on</strong>g>vestigated by compar<str<strong>on</strong>g>in</str<strong>on</strong>g>g analysis of historical <str<strong>on</strong>g>and</str<strong>on</strong>g> archeomagnetic observati<strong>on</strong>s withpredicti<strong>on</strong>s from analytical <str<strong>on</strong>g>and</str<strong>on</strong>g> numerical wave models.Geomagnetic field models are analysed <str<strong>on</strong>g>in</str<strong>on</strong>g> order to quantify the characteristics of radialmagnetic field (B r ) evoluti<strong>on</strong> at the <str<strong>on</strong>g>core</str<strong>on</strong>g> surface. In the historical model gufm1, spatially<str<strong>on</strong>g>and</str<strong>on</strong>g> temporally coherent (wave-like) patterns are identified <str<strong>on</strong>g>in</str<strong>on</strong>g> B r . Particularly strik<str<strong>on</strong>g>in</str<strong>on</strong>g>gis a low latitude signal with azimuthal wavenumber m=5 that travels westwards at∼17 km yr −1 . Study<str<strong>on</strong>g>in</str<strong>on</strong>g>g the archeomagnetic model CALS7K.1, episodes of both eastward<str<strong>on</strong>g>and</str<strong>on</strong>g> westward moti<strong>on</strong> of wave-like patterns <str<strong>on</strong>g>in</str<strong>on</strong>g> B r are observed. Analysis of the evoluti<strong>on</strong>of fields <str<strong>on</strong>g>and</str<strong>on</strong>g> underly<str<strong>on</strong>g>in</str<strong>on</strong>g>g flows from geodynamo simulati<strong>on</strong>s is used to illustrate that<str<strong>on</strong>g>in</str<strong>on</strong>g>ability to resolve the smallest length scales of the field makes quantitative <str<strong>on</strong>g>in</str<strong>on</strong>g>ferencesc<strong>on</strong>cern<str<strong>on</strong>g>in</str<strong>on</strong>g>g the flow difficult, unless the flow is large scale. Furthermore, it is foundazimuthal moti<strong>on</strong>s of patterns <str<strong>on</strong>g>in</str<strong>on</strong>g> B r can be produced by hydromagnetic <str<strong>on</strong>g>waves</str<strong>on</strong>g> <str<strong>on</strong>g>in</str<strong>on</strong>g> thesimulati<strong>on</strong>s. The rema<str<strong>on</strong>g>in</str<strong>on</strong>g>der of the thesis addresses whether hydromagnetic <str<strong>on</strong>g>waves</str<strong>on</strong>g> <str<strong>on</strong>g>in</str<strong>on</strong>g> the<str<strong>on</strong>g>core</str<strong>on</strong>g> could be the orig<str<strong>on</strong>g>in</str<strong>on</strong>g> of azimuthal geomagnetic secular variati<strong>on</strong>.Magneto-Rossby <str<strong>on</strong>g>waves</str<strong>on</strong>g> driven by c<strong>on</strong>vecti<strong>on</strong> (with a dynamical balance between magneticforces, latitude-dependent Coriolis forces, <str<strong>on</strong>g>and</str<strong>on</strong>g> buoyancy forces) are proposed as asuitable c<str<strong>on</strong>g>and</str<strong>on</strong>g>idate for hydromagnetic <str<strong>on</strong>g>waves</str<strong>on</strong>g> <str<strong>on</strong>g>in</str<strong>on</strong>g> the <str<strong>on</strong>g>core</str<strong>on</strong>g>. When driven by thermal c<strong>on</strong>vecti<strong>on</strong>,such <str<strong>on</strong>g>waves</str<strong>on</strong>g> propagate <strong>on</strong> the thermal diffusi<strong>on</strong> time scale. C<strong>on</strong>vecti<strong>on</strong>-drivenmagneto-Rossby <str<strong>on</strong>g>waves</str<strong>on</strong>g> are found to exhibit dispersive behaviour <str<strong>on</strong>g>and</str<strong>on</strong>g> a dependence ofpropagati<strong>on</strong> speed <strong>on</strong> latitude. It is shown that such hydromagnetic <str<strong>on</strong>g>waves</str<strong>on</strong>g> <str<strong>on</strong>g>in</str<strong>on</strong>g> the <str<strong>on</strong>g>core</str<strong>on</strong>g>could produce wave-like patterns <str<strong>on</strong>g>in</str<strong>on</strong>g> B r <str<strong>on</strong>g>in</str<strong>on</strong>g> two ways. One mechanism <str<strong>on</strong>g>in</str<strong>on</strong>g>volves the distorti<strong>on</strong>of toroidal magnetic field with<str<strong>on</strong>g>in</str<strong>on</strong>g> the <str<strong>on</strong>g>core</str<strong>on</strong>g> by wave flows produc<str<strong>on</strong>g>in</str<strong>on</strong>g>g new, spatiallyperiodic <str<strong>on</strong>g>and</str<strong>on</strong>g> azimuthally drift<str<strong>on</strong>g>in</str<strong>on</strong>g>g, c<strong>on</strong>centrati<strong>on</strong>s of B r . This mechanism is <str<strong>on</strong>g>in</str<strong>on</strong>g>vestigatedus<str<strong>on</strong>g>in</str<strong>on</strong>g>g a 3D, l<str<strong>on</strong>g>in</str<strong>on</strong>g>ear, dynamical model with spherical geometry <str<strong>on</strong>g>and</str<strong>on</strong>g> an imposed toroidalmagnetic field. When this toroidal magnetic field is equatorially symmetric, wave-likepatterns <str<strong>on</strong>g>in</str<strong>on</strong>g> B r centred <strong>on</strong> the equator are obta<str<strong>on</strong>g>in</str<strong>on</strong>g>ed. Wave flows are found to c<strong>on</strong>sist ofalternat<str<strong>on</strong>g>in</str<strong>on</strong>g>g regi<strong>on</strong>s of flow c<strong>on</strong>vergence <str<strong>on</strong>g>and</str<strong>on</strong>g> divergence close to the outer boundary. Asec<strong>on</strong>d mechanism whereby hydromagnetic <str<strong>on</strong>g>waves</str<strong>on</strong>g> can produce spatially <str<strong>on</strong>g>and</str<strong>on</strong>g> temporallycoherent patterns <str<strong>on</strong>g>in</str<strong>on</strong>g> B r <str<strong>on</strong>g>in</str<strong>on</strong>g>volves advecti<strong>on</strong> of exist<str<strong>on</strong>g>in</str<strong>on</strong>g>g B r by the wave flows. This mechanismis studied us<str<strong>on</strong>g>in</str<strong>on</strong>g>g a 1D, diffusi<strong>on</strong>less, analytical model <str<strong>on</strong>g>and</str<strong>on</strong>g> a 2D numerical model<strong>on</strong> a spherical surface <str<strong>on</strong>g>in</str<strong>on</strong>g>clud<str<strong>on</strong>g>in</str<strong>on</strong>g>g limited magnetic diffusi<strong>on</strong>. It is found that propagat<str<strong>on</strong>g>in</str<strong>on</strong>g>gc<strong>on</strong>centrati<strong>on</strong>s <str<strong>on</strong>g>in</str<strong>on</strong>g> B r are produced that pulsate <str<strong>on</strong>g>in</str<strong>on</strong>g> amplitude if the wave propagati<strong>on</strong>speed is faster than the fluid moti<strong>on</strong>s with<str<strong>on</strong>g>in</str<strong>on</strong>g> the wave. Both mechanisms could feasiblybe <str<strong>on</strong>g>in</str<strong>on</strong>g>volved <str<strong>on</strong>g>in</str<strong>on</strong>g> produc<str<strong>on</strong>g>in</str<strong>on</strong>g>g the wave-like patterns <str<strong>on</strong>g>in</str<strong>on</strong>g> B r identified at the <str<strong>on</strong>g>core</str<strong>on</strong>g> surface.

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