Mb. Baker et Em. Stolper, DETERMINING THE COMPOSITION OF HIGH-PRESSURE MANTLE MELTS USING DIAMOND AGGREGATES, Geochimica et cosmochimica acta, 58(13), 1994, pp. 2811-2827
We present a new experimental technique for circumventing the quenchin
g problems that have plagued high-pressure peridotite melting studies.
A thin layer of approximately 50 mum diamonds is placed above a layer
of peridotite powder. Partial melt extracted from the peridotite laye
r collects in the pore spaces between the diamonds and equilibrates di
ffusively with the residual peridotite mineralogy. Isolated from the c
rystalline residue, the melt quenches to a glass that records the comp
osition of the liquid coexisting with the residual crystalline phases
under the conditions of the experiment. We have used this technique to
investigate partial melting of a fertile mantle composition at 10 kba
r and a temperature range of 1270-1390-degrees. Oxide concentrations i
n the liquids from the longest duration runs (up to 151 hours) vary sy
stematically with increasing temperature: TiO2, Al2O3, and Na2O decrea
se monotonically, while Cr2O3, FeO, and MgO increase steadily. CaO sh
ows more complicated behavior, first increasing and then decreasing, w
ith the crest in the temperature-CaO trend approximately coincident wi
th the disappearance of clinopyroxene from the residue between 1330 an
d 1350-degrees-C. Overall variation in silica content with temperature
is small, and there appears to be a minimum at about 12% melting. The
compositions of liquids produced in time series, temperature reversal
, and two-stage experiments (conducted to test the technique) all indi
cate that our experimentally determined liquid compositions represent
close approaches to equilibrium. Calculated melt fractions (F) also va
ry systematically with temperature. The slope of the T(degrees-C)-F cu
rve is not constant over the spinel lherzolite melting interval, but d
ecreases as temperature increases from 1270 to 1330-degrees-C. Extrapo
lating the curve back to zero melt suggests that the anhydrous solidus
temperature for our peridotite starting composition is approximately
1240-degrees-C. At temperatures below the cpx-out curve, melt generati
on occurs via the reaction, 0.38 opx + 0.71 cpx + 0. 13 sp --> 0.22 ol
iv + 1.0 liq, and the proportions of minerals that enter the melt appe
ar to be independent of temperature. At temperatures above cpx-out, th
e less well constrained melting reaction is: 1.06 opx + 0.04 sp = 0.1
oliv + 1 liq. The fact that all of the 10 kbar melts have FeO content
s that are substantially lower than those reported in any primitive MO
RB glasses further strengthens the conclusions that these glasses are
not 10 kbar primary melts, that they involve a component of higher pre
ssure partial melting, and that they have evolved by significant olivi
ne fractionation from more primitive liquids. Our experimental data al
so provide an independent check of the results of recent peridotite pa
rtial melting calculations. Efforts to parameterize the experimental d
atabase on peridotite melting, and to calculate melt compositions as a
function of P, T, and F are partially successful in reproducing the c
ompositional trends determined in this study.