(a) The MgO equilibrium concentration in the core (same figure as
Extended Data Fig. 4b),
corresponding to our nominal CMB temperature evolution. The onset of MgO
exsolution from the core occurs when the MgO equilibrium concentration drops
below the MgO content in the core, which is reported here in two cases: 2.9
wt.% for the Mars-sized impactor, and 2.1 wt.% for the
“fast-spinning” impactor. For the thermal evolution model in
Extended Data Fig. 4a, this onset
is at 1.1 Ga and 2.3 Ga, respectively. (b) and (c) Exsolution power for
these two cases which is proportional to the MgO exsolution rate plotted in
Extended Data Fig. 4d. It is
noteworthy that power at a given time is independent of initial MgO content
(as long as MgO is being exsolved). The latter only affects the onset of
exsolution and therefore the duration of energy release. We also note that
the power produced is in excess of 3 TW, and therefore sufficient to drive a
dynamo by compositional buoyancy. Finally, the power drops dramatically with
the onset of inner core growth, because of the associated drop in core
cooling rate and MgO exsolution rate. The core at the present day is still
exsolving MgO, and should produce ~1 TW of power, significantly less
than the power produced by inner core growth.