The backward integration of the mantle's energy balance in section 3.7,
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 backward integration of the mantle's energy balance in section 3.7, CmdTm/dt=H(t)−Q(Tm), gave a runaway rather than a gentle cooling history, because Q(Tm)∝(Tm−Ts)4/3e−Ea/3RTm depends steeply on Tm.
((a)) Show that the logarithmic sensitivity of Q to Tm is dTmdlnQ=3(Tm−Ts)4+3RTm2Ea.
((b)) Evaluate this sensitivity at today's mantle temperature Tm,0=1623K, for Ts=300K and Ea=300kJmol−1.
((c)) For a present Urey ratio of 0.5, the text gives today's net cooling rate as 114KGyr−1. Using the sensitivity from part (b), estimate the fractional change in Q implied by a single 100Myr backward step taken at that rate, and say whether a single such step looks safe.
((d)) The chapter states that the runaway is not an artefact of the 0.1Myr step used there. Using your answer to part (c), explain in one or two sentences why making the step size smaller could not remove it.