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

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8 Chapter 1 — Introducti<strong>on</strong>Poirier, 1994).1.3.3 Energy sources <str<strong>on</strong>g>and</str<strong>on</strong>g> <str<strong>on</strong>g>core</str<strong>on</strong>g> moti<strong>on</strong>sThe liquid ir<strong>on</strong> <str<strong>on</strong>g>in</str<strong>on</strong>g> Earth’s <str<strong>on</strong>g>core</str<strong>on</strong>g> is thought to be undergo<str<strong>on</strong>g>in</str<strong>on</strong>g>g vigorous moti<strong>on</strong>. On shorttime scales of hours to days disturbances driven by <str<strong>on</strong>g>core</str<strong>on</strong>g>-mantle coupl<str<strong>on</strong>g>in</str<strong>on</strong>g>g <str<strong>on</strong>g>and</str<strong>on</strong>g> tidal forc<str<strong>on</strong>g>in</str<strong>on</strong>g>gwill produce a broad spectrum of <str<strong>on</strong>g>in</str<strong>on</strong>g>ternal gravity <str<strong>on</strong>g>and</str<strong>on</strong>g> <str<strong>on</strong>g>in</str<strong>on</strong>g>ertial <str<strong>on</strong>g>waves</str<strong>on</strong>g> (Aldridge, 2003). Ithas been suggested that precessi<strong>on</strong>al <str<strong>on</strong>g>and</str<strong>on</strong>g> tidal stra<str<strong>on</strong>g>in</str<strong>on</strong>g>s could produce <str<strong>on</strong>g>in</str<strong>on</strong>g>stabilities lead<str<strong>on</strong>g>in</str<strong>on</strong>g>gto large amplitude flows <str<strong>on</strong>g>in</str<strong>on</strong>g> the <str<strong>on</strong>g>core</str<strong>on</strong>g> (Malkus, 1994). On l<strong>on</strong>ger time scales the presenceof a variety of energy sources suggests that c<strong>on</strong>vecti<strong>on</strong> is occurr<str<strong>on</strong>g>in</str<strong>on</strong>g>g <str<strong>on</strong>g>in</str<strong>on</strong>g> the outer <str<strong>on</strong>g>core</str<strong>on</strong>g>.These energy sources <str<strong>on</strong>g>in</str<strong>on</strong>g>clude secular cool<str<strong>on</strong>g>in</str<strong>on</strong>g>g of the <str<strong>on</strong>g>core</str<strong>on</strong>g> <str<strong>on</strong>g>in</str<strong>on</strong>g> the aftermath of planetaryformati<strong>on</strong>, release of latent heat <str<strong>on</strong>g>and</str<strong>on</strong>g> buoyant light material at the <str<strong>on</strong>g>in</str<strong>on</strong>g>ner-<str<strong>on</strong>g>core</str<strong>on</strong>g> boundaryas the <str<strong>on</strong>g>in</str<strong>on</strong>g>ner <str<strong>on</strong>g>core</str<strong>on</strong>g> solidifies, <str<strong>on</strong>g>and</str<strong>on</strong>g> radioactive heat<str<strong>on</strong>g>in</str<strong>on</strong>g>g (see, for example, Gubb<str<strong>on</strong>g>in</str<strong>on</strong>g>s et al.(2003; 2004); Roberts et al. (2003)).Due to the very low viscosity of liquid ir<strong>on</strong> <str<strong>on</strong>g>in</str<strong>on</strong>g> the <str<strong>on</strong>g>core</str<strong>on</strong>g>, vigorous c<strong>on</strong>vective moti<strong>on</strong>sare expected to be dom<str<strong>on</strong>g>in</str<strong>on</strong>g>ated by the <str<strong>on</strong>g>in</str<strong>on</strong>g>fluence of the Coriolis forces (a c<strong>on</strong>sequence ofplanetary rotati<strong>on</strong>) <str<strong>on</strong>g>and</str<strong>on</strong>g> the str<strong>on</strong>g magnetic fields present there. N<strong>on</strong>l<str<strong>on</strong>g>in</str<strong>on</strong>g>ear <str<strong>on</strong>g>in</str<strong>on</strong>g>teracti<strong>on</strong>sbetween flow, magnetic <str<strong>on</strong>g>and</str<strong>on</strong>g> buoyancy fields will produce complex, time-dependent flowpatterns. The presence of magnetic fields <str<strong>on</strong>g>in</str<strong>on</strong>g> an electrically c<strong>on</strong>duct<str<strong>on</strong>g>in</str<strong>on</strong>g>g fluid also permitsa class of fluid moti<strong>on</strong>s known as hydromagnetic <str<strong>on</strong>g>waves</str<strong>on</strong>g>. These arise because the distorti<strong>on</strong>of magnetic fields by fluid moti<strong>on</strong> produces a magnetic (Lorentz) force oppos<str<strong>on</strong>g>in</str<strong>on</strong>g>gthat distorti<strong>on</strong>. In comb<str<strong>on</strong>g>in</str<strong>on</strong>g>ati<strong>on</strong> with fluid <str<strong>on</strong>g>in</str<strong>on</strong>g>ertia this magnetic restor<str<strong>on</strong>g>in</str<strong>on</strong>g>g force leads totransverse wave moti<strong>on</strong>s (Alfvén, 1942). The form of these hydromagnetic <str<strong>on</strong>g>waves</str<strong>on</strong>g> will bestr<strong>on</strong>gly <str<strong>on</strong>g>in</str<strong>on</strong>g>fluenced by rapid rotati<strong>on</strong> (Lehnert, 1954), unstable stratificati<strong>on</strong> (Brag<str<strong>on</strong>g>in</str<strong>on</strong>g>sky,1964), <str<strong>on</strong>g>and</str<strong>on</strong>g> spherical geometry (Hide, 1966) all of which are thought to be important <str<strong>on</strong>g>in</str<strong>on</strong>g>Earth’s outer <str<strong>on</strong>g>core</str<strong>on</strong>g>.1.3.4 The geodynamo mechanismThe generati<strong>on</strong> of the geomagnetic field <str<strong>on</strong>g>in</str<strong>on</strong>g> Earth’s <str<strong>on</strong>g>core</str<strong>on</strong>g> is now fairly well understoodthanks <str<strong>on</strong>g>in</str<strong>on</strong>g> particular to recent advances <str<strong>on</strong>g>in</str<strong>on</strong>g> computati<strong>on</strong>al modell<str<strong>on</strong>g>in</str<strong>on</strong>g>g (see, for example,Roberts <str<strong>on</strong>g>and</str<strong>on</strong>g> Glatzmaier (2000a)). The high temperatures <str<strong>on</strong>g>in</str<strong>on</strong>g> the <str<strong>on</strong>g>core</str<strong>on</strong>g> <str<strong>on</strong>g>and</str<strong>on</strong>g> the timedependenceof the observed field rule out an explanati<strong>on</strong> <str<strong>on</strong>g>in</str<strong>on</strong>g> terms of permanent magnetism.Instead, a mechanism produc<str<strong>on</strong>g>in</str<strong>on</strong>g>g a rapidly evolv<str<strong>on</strong>g>in</str<strong>on</strong>g>g, self-susta<str<strong>on</strong>g>in</str<strong>on</strong>g><str<strong>on</strong>g>in</str<strong>on</strong>g>g, magneticfield is required. A dynamo explanati<strong>on</strong> is the <strong>on</strong>ly reas<strong>on</strong>able c<str<strong>on</strong>g>and</str<strong>on</strong>g>idate for such amechanism (see, for example, Gubb<str<strong>on</strong>g>in</str<strong>on</strong>g>s <str<strong>on</strong>g>and</str<strong>on</strong>g> Masters (1979)). A dynamo is a system thatc<strong>on</strong>verts k<str<strong>on</strong>g>in</str<strong>on</strong>g>etic energy <str<strong>on</strong>g>in</str<strong>on</strong>g>to magnetic energy by moti<strong>on</strong>al <str<strong>on</strong>g>in</str<strong>on</strong>g>ducti<strong>on</strong> given some <str<strong>on</strong>g>in</str<strong>on</strong>g>itialseed magnetic field (Roberts, 1994). Moti<strong>on</strong>s of electrically c<strong>on</strong>duct<str<strong>on</strong>g>in</str<strong>on</strong>g>g fluid <str<strong>on</strong>g>in</str<strong>on</strong>g> Earth’s<str<strong>on</strong>g>core</str<strong>on</strong>g> mov<str<strong>on</strong>g>in</str<strong>on</strong>g>g through a weak pre-exist<str<strong>on</strong>g>in</str<strong>on</strong>g>g magnetic field (e.g. the <str<strong>on</strong>g>in</str<strong>on</strong>g>ter-planetary magneticfield) will generate electrical currents. These electrical currents produce magnetic

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