A planet has a liquid iron core of radius with electrical conductivity

PHYSICS · Multi-part · Fermi University Physics · Plasma Physics · Earth, Climate & Energy Physics · The solid Earth: structure, fields and thermal history

The Solid Earth, Ch The geomagnetic field: potential, spectrum, induction and the palaeomagnetic record

Problem

A planet has a liquid iron core of radius rc=2000 kmr_{\rm c}=2000\,\mathrm{km} with electrical conductivity σe=5×105 S m−1\sigma_e=5\times10^{5}\,\mathrm{S\,m^{-1}}. Take μ0=4π×10−7 H m−1\mu_0=4\pi\times10^{-7}\,\mathrm{H\,m^{-1}} and 1 yr=3.156×107 s1\,\mathrm{yr}=3.156\times10^{7}\,\mathrm{s}. ((a)) Compute the magnetic diffusivity ηm\eta_m and the magnetic diffusion time τd=rc2/(π2ηm)\tau_d=r_{\rm c}^2/(\pi^2\eta_m) of the core, in kyr. ((b)) Repeated surveys, continued down to the core surface, show a patch of radial flux drifting westward at 0.5∘ yr−10.5^\circ\,\mathrm{yr^{-1}} near the core's equator. Treating the flux as frozen in, infer the flow speed at the top of the core in m s−1\mathrm{m\,s^{-1}}. ((c)) How long does a patch 1000 km1000\,\mathrm{km} across take to drift its own width, and is frozen flux a good approximation over that time?

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