Abstract
GEOCHEMISTRY GEOPHYSICS GEOSYSTEMS,
VOL. 4,
1017,
24 PP., 2003
doi:10.1029/2002GC000399 [Citation]
Buoyancy of the continental upper mantle
Department of Geology and Geophysics, MIT-Woods Hole Oceanographic Institution Joint Program, Woods Hole, Massachusetts 02543, USA
Department of Geology and Geophysics, Woods Hole Oceanographic Institution, Woods Hole, Massachusetts 02543, USA
Department of Geology and Geophysics, Woods Hole Oceanographic Institution, Woods Hole, Massachusetts 02543, USA
The thermal boundary layer beneath continental cratons extends into the Earth's mantle to depths of at least 200 km. It has
been proposed that chemical depletion of the lithospheric mantle during partial melting offsets the effect of increased density
from conductive cooling, resulting in neutral buoyancy with respect to the underlying asthenosphere. Mineral compositions
of garnet peridotite xenoliths in the Kaapvaal craton give equilibration temperatures and pressures that define a continental
conductive geotherm intersecting a mantle adiabat with a potential temperature of 1300°C at ∼60 kbar. We calculated normative
densities for a “low-temperature” garnet and spinel peridotite xenolith suite using Mg#. At their temperatures and pressures
of equilibration, all the low-temperature peridotites are positively buoyant with respect to the convecting mantle, which
is inconsistent with the hypothesis of a neutrally buoyant thermal boundary layer. To account for the possibility that pressure,
temperature, and mineral proportions may have varied over time, equilibrium solidus mineral assemblages for the low-temperature
xenoliths over a range of pressures and temperatures were generated by free energy minimization using the program Perplex (
Received 21 June 2002; accepted 15 October 2002; published 18 February 2003.
Citation: (2003), Buoyancy of the continental upper mantle, Geochem. Geophys. Geosyst., 4(2), 1017, doi:10.1029/2002GC000399.
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