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A Transition in the Ni2+ Complex
Structure from Six- to Four-Coordinate upon Formation of Ion Pair
Species in Supercritical Water: An XAFS, NIR and MD Study
M. M. Hoffmann, J. G. Darab, B. J. Palmer, and J. L. Fulton, J.
Phys. Chem. A, 103, 8471-8482, (1999)
Abstract: The coordination structure about Ni2+
in water at temperatures up to 525°C was measured using x-ray
absorption fine structure (XAFS). The solutions containing 0.2 m
NiBr2 and 0.2 m NiBr2/0.8
m NaBr were explored at pressures up to 720 bar. For certain systems,
both Ni and Br XAFS were acquired and a global model was used to
fit the two independent sets of XAFS data. These two independent
measurements gave excellent agreement on the coordination structure
of the Ni2+/Br- contact ion pairing. The result
is a complete picture of the coordination structure of the contact
ion pairing including the coordination numbers, distances for the
water-ion and ion-ion associations and also a high-quality measurement
of the binding strength and amount of disorder (Debye-Waller factor
and the anharmonicity) of the Ni2+/Br- association.
The XAFS measurements strongly indicate a transitional change
in the coordination of Ni2+ from the octahedral Ni2+(H2O)6
species at room temperature to four-coordinate structures at supercritical
conditions (e.g. T > 375°C). Specifically the equilibrium
structure at 425°C is found to be Ni2+(Br-)3.3(H2O)1.0
for the aqueous solution of 0.2 m NiBr2 with
0.8 m NaBr. At 325°C, the octahedral species still exists but
it is in equilibrium with new species of lower-coordination. Above
425°C, at moderate pressures up to 700 bar, the stable structures
are a family of four-coordinated species (NiBr(H2O)3ïBr,
NiBr2(H2O)2,
NiBr3(H2O)ïNa)
where the degree of Br- adduction and replacement of
H2O in the inner shell depends upon the overall Br- concentration.
The most likely symmetry of these species is a distorted tetrahedron.
Measurements of the Ni pre-edge 1s-to-3d and to 1s-to-4p transitions
using X-ray absorption confirm that a symmetry change occurs at
high temperature and the results are consistent with the XAFS and
MD conclusion of a distorted tetrahedral structure. This observation
is further confirmed by near-IR spectra of the same system.
Molecular dynamics simulations under identical conditions were used
to verify the experimental findings. Although we found qualitative
agreement between the experimental and simulated first-shell coordination
structure, it is clear that refinements of the intermolecular potentials
are required to quantitatively capture the true high-temperature
structure.
For information about supercritical fluid capabilities at PNNL, please contact Clement Yonker, at (509) 372-4748, clem.yonker@pnl.gov.
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