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Atomistic simulation of trace element incorporation into garnets—comparison with experimental garnet-melt partitioning data
We have studied the energetics of trace element incorporation into pure almandine (Alm), grossular (Gros), pyrope (Py) and spessartine (Spes) garnets (X 3Al 2Si 3O 12, with X = Fe, Ca, Mg, Mn respectively), by means of computer simulations of perfect and defective lattices in the static limit. The s...
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Published in: | Geochimica et cosmochimica acta 2000-05, Vol.64 (9), p.1629-1639 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
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Online Access: | Get full text |
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Summary: | We have studied the energetics of trace element incorporation into pure almandine (Alm), grossular (Gros), pyrope (Py) and spessartine (Spes) garnets (X
3Al
2Si
3O
12, with X = Fe, Ca, Mg, Mn respectively), by means of computer simulations of perfect and defective lattices in the static limit. The simulations use a consistent set of interatomic potentials to describe the non-Coulombic interactions between the ions, and take explicit account of lattice relaxation associated with trace element incorporation. The calculated relaxation (strain) energies
U
rel
are compared to those obtained using the
Brice (1975) model of lattice relaxation, and the results compared to experimental garnet-melt trace element partitioning data interpreted using the same model.
Simulated
U
rel
associated with a wide range of homovalent (Ni, Mg, Co, Fe, Mn, Ca, Eu, Sr, Ba) and charge-compensated heterovalent (Sc, Lu, Yb, Ho, Gd, Eu, Nd, La, Li, Na, K, Rb) substitutions onto the garnet X-sites show a near-parabolic dependence on trace element radius, in agreement with the Brice model. From application of the Brice model we derived apparent X-site Young’s moduli
E
X
(1+, 2+, 3+) and the ‘ideal’ ionic radii
r
0
(1+, 2+, 3+), corresponding to the minima in plots of
U
rel
vs. radius. For both homovalent and heterovalent substitutions
r
0
increases in the order Py–Alm–Spes–Gros, consistent with crystallographic data on the size of garnet X-sites and with the results of garnet-melt partitioning studies. Each end-member also shows a marked increase in both the apparent
E
X
and
r
0
with increasing trace element charge (
Z
c
). The increase in
E
X
is consistent with values obtained by fitting to the Brice model of experimental garnet-melt partitioning data. However, the increase in
r
0
with increasing
Z
c
is contrary to experimental observation.
To estimate the influence of melt on the energetics of trace element incorporation, solution energies (
U
sol
) were calculated for appropriate exchange reactions between garnet and melt, using binary and other oxides to simulate cation co-ordination environment in the melt.
U
sol
also shows a parabolic dependence on trace element radius, with inter-garnet trends in
E
X
and
r
0
similar to those found for relaxation energies. However,
r
0
(
i+) obtained from minima in plots of
U
sol
vs. radius are located at markedly different positions, especially for heterovalent substitutions (
i = 1, 3). For each end-member garnet,
r
0
now decreases with increasin |
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ISSN: | 0016-7037 1872-9533 |
DOI: | 10.1016/S0016-7037(00)00336-7 |