The heat flow crossing the core-mantle boundary is estimated to be

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

The Solid Earth, Ch Dating, heat flow and the thermal history of the Earth

Problem

The heat flow crossing the core-mantle boundary is estimated to be Qc=9 TWQ_c=9\,\mathrm{TW}. The core's adiabatic temperature gradient follows (dT/dz)ad=αVgT/cp(\mathrm{d}T/\mathrm{d}z)_{\rm ad}=\alpha_VgT/c_p with αV=10−5 K−1\alpha_V=10^{-5}\,\mathrm{K^{-1}}, g=10.7 m s−2g=10.7\,\mathrm{m\,s^{-2}}, T=4000 KT=4000\,\mathrm{K} and cp=750 J kg−1 K−1c_p=750\,\mathrm{J\,kg^{-1}\,K^{-1}}; take the core's thermal conductivity to be kcore=40 W m−1 K−1k_{\rm core}=40\,\mathrm{W\,m^{-1}\,K^{-1}} and its surface area to be 4πrc2=1.52×1014 m24\pi r_c^2=1.52\times10^{14}\,\mathrm{m^2}. Someone argues: "the whole 9 TW9\,\mathrm{TW} leaves the core, so the whole 9 TW9\,\mathrm{TW} is available to drive the geodynamo." ((a)) Compute the heat conducted down the adiabat, in TW. ((b)) Say whether the argument is correct, and if not, how much of the 9 TW9\,\mathrm{TW} can actually drive thermally driven convection, and what becomes of the rest.

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