MULTINUCLEAR NMR, RAMAN, EXAFS, AND X-RAY-DIFFRACTION STUDIES OF URANYL CARBONATE COMPLEXES IN NEAR-NEUTRAL AQUEOUS-SOLUTION - X-RAY STRUCTURE OF C(NH2)(3)](6)[(UO2)(3)(CO3)(6)]CENTER-DOT-6.5H(2)O
Pg. Allen et al., MULTINUCLEAR NMR, RAMAN, EXAFS, AND X-RAY-DIFFRACTION STUDIES OF URANYL CARBONATE COMPLEXES IN NEAR-NEUTRAL AQUEOUS-SOLUTION - X-RAY STRUCTURE OF C(NH2)(3)](6)[(UO2)(3)(CO3)(6)]CENTER-DOT-6.5H(2)O, Inorganic chemistry, 34(19), 1995, pp. 4797-4807
C-13 and O-17 NMR and Raman spectroscopies were used to monitor the fr
actions of UO2(CO3)(3)(4-) (1) and (UO2)(3)(CO3)(6)(6-) (2) in aqueous
carbonate solutions as a function of pH, ionic strength, carbonate co
ncentration, uranium concentration, and temperature. The multinuclear
NMR and Raman data are consistent with the formation of (UO2)(3)(CO3)(
6)(6-). The pH dependence of the C-13 NMR spectra was used to determin
e the equilibrium constant for the reaction 3UO(2)(CO3)(3)(4-) + 3H(+)
reversible arrow (UO2)(3)(CO3)(6)(6-) + 3HCO(3)(-), log K = 18.1(+/-
0.5) at I-m = 2.5 m and 25 degrees C, and corresponds to log beta(36)
= 55.6(+/- 0.5) for the reaction 3UO(2)(2+) + 6CO(3)(2-) reversible ar
row (UO2)(3)(CO3)(6)(6-) under the same conditions. Raman spectra show
ed the uranyl nu(1) stretching band at 831.6 cm(-1) for monomeric 1 an
d at 812.5 cm(-1) for trimeric (UO2)(3)(CO3)(6)(6-) (2). EXAFS data fr
om solid [C(NH2)(3)](6)[(UO2)(3)(CO3)(6)] and a solution of (UO2)(3)(C
O3)(6)(6-) suggest that the same uranium species is present in both th
e solid and solution states. Fourier transforms of the EXAFS spectra o
f both solid and solution samples revealed five well-resolved peaks co
rresponding to nearly identical near-neighbor distances for solid and
solution- samples of 2. Fitting of these peaks yields U-O(uranyl) = 1.
79, U-O(carbonate) = 2.45, U- -C = 2.90, U- -O(terminal carbonate) = 4
.16, and U- -U = 4.91 Angstrom for the solid and similar distances for
the solution sample. A peak at 4.75 Angstrom in both Fourier transfor
ms (uncorrected for phase shift) corresponds to a U- -U interaction at
4.91 Angstrom, a conclusion which is supported by the absence of this
peak in the Fourier transform of the crystalline monomeric K-4[UO2(CO
3)(3)] Multiple scattering along the uranyl vector is believed to play
a significant role in the EXAFS of all three systems. The EXAFS data
are consistent with the trimeric uranyl carbonate species indicated by
NMR spectroscopy. Single crystals of [C(NH2)(3)](6)[(UO2)(3)(CO3)(6)]
. 6.5H(2)O were obtained from a solution that contained stoichiometric
amounts of uranyl nitrate and guanidinium carbonate and an excess of
guanidinium nitrate at pH 6.5 under a CO2 atmosphere. The solid state
molecular structure of [C(NH2)(3)](6)[(UO2)(3)(CO3)6]. 6.5H(2)O contai
ns a planar D-3h trimetallic (UO2)(3)(CO3)(6)(6-) anion, the structure
that Aberg and co-workers originally proposed for the trimeric soluti
on species. The trimetallic anion contains three uranium atoms and all
six carbonate ligands in the molecular plane with three uranyl oxygen
atoms above and three below the plane. Uranyl U=O distances average 1
.78(1) Angstrom, while U-O distances to the carbonate oxygen atoms ave
rage 2.41(1) Angstrom for terminal and 2.48(1) Angstrom for bridging l
igands. Particularly significant is the average nonbonding U- -U dista
nce of 4. 97 Angstrom which compares favorably to the 4.91 Angstrom di
stance seen in the EXAFS analysis. The molecule crystallizes in the tr
iclinic space group P ($) over bar 1, with a = 6.941(2) Angstrom, b =
14.488(2) Angstrom, c = 22.374(2) Angstrom, alpha = 95.63(2)degrees, b
eta = 98.47(2)degrees, gamma = 101.88(2)degrees, R = 0.0555, R(w), = 0
.0607, V = 2158.5 Angstrom(3),d(cal), = 2.551 g cm(-3), and Z = 2.