Some models for the formation and dispersal of supercontinents
suggest a link between mantle convection, heat flow,
and the supercontinent cycle. Stationary supercontinents
insulate the mantle causing it to heat up, because the cooling
effects of subduction and seafloor spreading are absent. As
the mantle then heats up, convective upwelling is initiated,
causing dynamic and isostatic uplift of the continent, injection
of melts into the continental crust, and extensive crustal
melting. These crustal melts are widespread in the interiors of
some reconstructed supercontinents, such as the Proterozoic
anorogenic granites in interior North America, which were
situated in the center of the supercontinent of Rodinia when
they formed between one billion and 800 million years ago.
After intrusion of the anorogenic magmas, the lithosphere
is weakened and can be more easily driven apart by
divergent flow in the asthenosphere. Thermal effects in the
lower mantle lag behind surface motions. So, the present
Atlantic geoid high and associated hot spots represent a
“memory” of heating beneath Pangea. Likewise, the circum
Pangea subduction zones may have a memory in a global ring
of geoid lows.
Other models for relationships between supercontinents
and mantle convection suggest that supercontinents may also
result from mantle convection patterns. Continental fragments
may be swept toward convective downwellings, where
they reaggregate as supercontinents.
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