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Equation of state of Fe3+-bearing phase-X
We investigated the high-pressure behaviour of Fe 3+ -bearing hydrous phase-X, (K 1.307 Na 0.015 )(Mg 1.504 Fe 0.373 3+ Al 0.053 Ti 0.004 4+ )Si 2 O 7 H 0.36 , up to 34 GPa at room temperature by synchrotron X-ray powder diffraction. The lattice parameters behave anisotropically, with the [001] dire...
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Published in: | Physics and chemistry of minerals 2012-07, Vol.39 (7), p.553-559 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
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Summary: | We investigated the high-pressure behaviour of Fe
3+
-bearing hydrous phase-X, (K
1.307
Na
0.015
)(Mg
1.504
Fe
0.373
3+
Al
0.053
Ti
0.004
4+
)Si
2
O
7
H
0.36
, up to 34 GPa at room temperature by synchrotron X-ray powder diffraction. The lattice parameters behave anisotropically, with the [001] direction stiffer than [100]. In the 10
−4
to 22 GPa pressure range, the axial bulk moduli are
K
0
a
= 112(3) GPa and
K
′ = 4, and
K
0
c
= 158(2) GPa and
K
′ = 4, and the anisotropy of the lattice parameters is β
0
c
:β
0
a
= 0.71:1. The cell volumes are fitted by a second-order Birch–Murnaghan equation of state giving a bulk modulus of
K
0
= 127(1) GPa and
K
′ = 4 in the same pressure range. After 22 GPa, a discontinuity in volume and lattice parameters can be recognized. Sample did not become amorphous up to 34 GPa. The coupled substitution K + Mg = [] + Fe
3+
has only a limited influence on the bulk modulus and structural stability of phase-X. |
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ISSN: | 0342-1791 1432-2021 |
DOI: | 10.1007/s00269-012-0511-2 |