metal-organic compounds
Tetra-μ2-acetato-tetraaquadi-μ3-oxido-octaoxidotetrauranium(VI) methanol disolvate tetrahydrate
aDepartment of Chemistry, Memorial University of Newfoundland, St. Johns, NL, A1B 3X7, Canada, and bDepartment of Chemistry and Centre for Chemical Analysis, Research and Training (C-CART), X-Ray Diffraction Laboratory, Memorial University of Newfoundland, St. Johns, NL, A1B 3X7, Canada
*Correspondence e-mail: louise.dawe@mun.ca
The centrosymmetric title tetramer, [U4(C2H3O2)4O10(H2O)4]·2CH4O, has a near planar core [maximum deviation from the least squares plane of 0.294 (6) Å]. It consists of two hexagonal–bipyramidally coordinated UVI atoms connected via μ2-O (acetate) and μ3-O (oxide) bridges in the equatorial plane to two pentagonal–bipyramidally coordinated UVI atoms. The equatorial plane of each UVI atom is completed by a bound water molecule, while the axial positions are occupied by uranyl (UO2)2+ O atoms. Multiple O—H⋯O hydrogen bonds are present, including a lattice methanol molecule bound to one of the pentagonal bipyramidal uranyl O atoms, as well as two different C11(6) chains orginating from a donor water molecule, via a uranyl oxygen acceptor and an acetate acceptor on different, adjacent tetramers. Finally, the contains four UVI tetramers, all connected by hydrogen bonding, forming a supramolecular R44(24) ring.
Related literature
For structurally similar tetrameric complexes with UVI, M4[(UO2)4(μ3-O)2L4] (M = NH4+, K+, Cs+; L = phthalate), see: Charushnikova et al. (2005), and with Bi, [Bi2(μ3-O)(OCH(CF3)2)2(μ-OCH(CF3)2)2(Solv)]2 (Solv = C7H8, Et2O, thf), see: Andrews et al. (2008). For a planar, mixed valent UV2UVI2 alkoxide, see: Zozulin et al. (1982). For a p-benzylcalix[7]arene complex containing a hexanuclear UVI cluster with a planar tetrameric core, see: Thuéry et al. (1999), and for dinuclear uranyl-containing salen [N,N′-ethylenebis(salicylimine)] complexes, see: Amato et al. (2007). For bond-valence-sum calculations, see: Wills (2010).
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear-SM Expert (Rigaku, 2009); cell CrystalClear-SM Expert; data reduction: CrystalClear-SM Expert; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2006); software used to prepare material for publication: publCIF (Westrip, 2010).
Supporting information
https://doi.org/10.1107/S1600536811050549/br2182sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536811050549/br2182Isup2.hkl
160 mg (0.337 mmol) of uranyl acetate dihydrate (UO2(CH3COO)2.2H2O) was dissolved in 1 ml methanol, and warmed in a hot water bath (323 K) for 5 minutes. The solution was left at room temperature (293 K) for slow evaporation. Yellow prismatic crystals, suitable for analysis by X-ray diffraction, formed after one week.
The water H-atoms, H8(A,B) and H11(A,B), were located from difference Fourier maps, and were refined with distance and angle restraints: O—H = 0.87 (2) Å, H—O—H = 104.50 (4)°. The C-bound methyl and methanolic H-atoms were included in calculated positions and treated as riding atoms: X—H = 0.98 and 0.84 Å for H-methyl and H-OMe H-atoms, respectively. For all H atoms, Uiso(H) = k × Ueq(parent atom), where k = 1.2 for H-methyl and k = 1.5 for all O-bound H-atoms. The final electron density synthesis shows the highest peak of 1.71 eÅ3 located 0.98 Å from U2 and the deepest hole of -2.85 eÅ3 located 0.72 Å from U1 and may be the result of residual absorption effects.
In connection with our on-going studies on metal-binding properties of a new series of macrocylic polyamide compounds, we were interested in determining whether such macrocycles, by analogy with analogous salen (N,N'-Ethylenebis(salicylimine)) compounds, would also form stable uranyl complexes. Using similar conditions to those which Amato et al. (2007) employed with their salens, the title compound crystallized out in the form reported herein.
Bond valence sum calculations (Wills, 2010) performed on the title compound indicate that both crystallographically independent uranium atoms are in the +6 oxidations state (U1 = 6.095, U2 = 6.074). The centrosymmetric U(VI) tetramer consists of two hexagonal bipyramids, and two pentagonal bipyramids (U1 and U2, and symmetry equivalents (-x + 1, -y, -z + 1), respectively; Figure 1), with (UO2)2+ oxygen-atoms occupying the axial positions for both U1 and U2. For U1, the equatorial plane consists of trans-bidentate acetate anions, each with one bridging µ2-O-atom (O1 and O3), and a µ3-O2- anion (O5) trans to a water molecule. The equatorial plane of U2 is therefore composed of the aforementioned µ2-O and µ3-O atoms, and their inversion-symmetry generated counter-parts, as well as water molecule (O11). Similar to the description given by Andrews et al. (2008) for [Bi2(µ3-O)(OCH(CF3)2)2(µ-OCH(CF3)2)2(Solv)]2 (Solv = C7H8, Et2O, thf) tetramers, this complex consists of a near planar, ten atom "raft", with maximum deviation from the least squares plane [U1, U2, O1–5 and symmetry equivalents (-x + 1, -y, -z + 1)] of 0.294 (6) Å for O5. Examination of longer range interactions reveals numerous hydrogen bonds, including a lattice solvent methanol molecule bound to one of the pentagonal bipyramidal uranyl oxygen atoms (O12—H12···O9; Figure 1), which further bridges to a bound water molecule of a second tetramer (O8—H8B···O12iii, (iii) x, -y+1/2, z-1/2; Figure 2, green dashed lines.) The tetramers interact via an additional hydrogen bond, wherby the aforementioned water molecule acts as a donor to one of the hexagonal bipyramidal uranyl oxygen atoms on the first assembly (O8—H8A···O7ii, (ii) -x+1, y+1/2, -z+1/2; Figure 2, black dashed lines) leading to a 24-membered H-bonded ring (graph set notation R44(24)) which spans all four tetramers present in the unit cell.
For structurally similar tetrameric complexes with U(VI), M4[(UO2)4(µ3-O)2L4] (M = NH4+, K+, Cs+; L = phthalate), see: Charushnikova et al. (2005), and with Bi, [Bi2 (µ3-O)(OCH(CF3)2)2(µ-OCH(CF3)2)2(Solv)]2 (Solv = C7H8, Et2O, thf), see: Andrews et al. (2008). For a planar, mixed valent U(V)2U(VI)2 alkoxide, see: Zozulin et al. (1982). For a p-benzylcalix[7]arene complex containing a hexanuclear U(VI) cluster with a planar tetrameric core, see: Thuéry et al. (1999), and for dinuclear uranyl-containing salen [N,N'-ethylenebis(salicylimine)] complexes, see: Amato et al. (2007). For bond-valence-sum calculations, see: Wills (2010).
Data collection: CrystalClear-SM Expert (Rigaku, 2009); cell
CrystalClear-SM Expert (Rigaku, 2009); data reduction: CrystalClear-SM Expert (Rigaku, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2006); software used to prepare material for publication: publCIF (Westrip, 2010).Fig. 1. 50% displacement ellipsoid representation of the title compound; hydrogen bonding indicated by dashed lines. Symmetry code: (i) -x + 1, -y, -z + 1. | |
Fig. 2. 50% displacement ellipsoid representation of the packed unit cell for the title compound; hydrogen bonding indicated by dashed lines. H-bonding for O11—H11A···O10iv and O11—H11B···O2v not shown. Symmetry codes: (ii)-x + 1, y + 1/2, -z + 1/2, (vi) x, -y + 1/2, z + 1/2, (vii) -x + 1, -y + 1, -z + 1, (viii)x, y + 1, z, (ix) -x + 1, y + 1/2, -z + 3/2. |
[U4(C2H3O2)4O10(H2O)4]·2CH4O | F(000) = 1296 |
Mr = 1484.44 | Dx = 3.477 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71075 Å |
Hall symbol: -P 2ybc | Cell parameters from 4946 reflections |
a = 8.334 (3) Å | θ = 1.9–29.5° |
b = 10.649 (3) Å | µ = 22.87 mm−1 |
c = 16.763 (5) Å | T = 163 K |
β = 107.632 (4)° | Prism, yellow |
V = 1417.8 (8) Å3 | 0.10 × 0.07 × 0.05 mm |
Z = 2 |
Rigaku Saturn70 CCD diffractometer | 3255 independent reflections |
Radiation source: fine-focus sealed tube | 3136 reflections with I > 2σ(I) |
Graphite - Rigaku SHINE monochromator | Rint = 0.076 |
Detector resolution: 14.63 pixels mm-1 | θmax = 27.5°, θmin = 3.1° |
ω scans | h = −10→10 |
Absorption correction: numerical (ABSCOR; Higashi, 1999) | k = −13→13 |
Tmin = 0.638, Tmax = 0.880 | l = −21→21 |
15149 measured reflections |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.034 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.088 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.09 | w = 1/[σ2(Fo2) + (0.0469P)2 + 6.6005P] where P = (Fo2 + 2Fc2)/3 |
3255 reflections | (Δ/σ)max = 0.001 |
188 parameters | Δρmax = 1.71 e Å−3 |
6 restraints | Δρmin = −2.85 e Å−3 |
[U4(C2H3O2)4O10(H2O)4]·2CH4O | V = 1417.8 (8) Å3 |
Mr = 1484.44 | Z = 2 |
Monoclinic, P21/c | Mo Kα radiation |
a = 8.334 (3) Å | µ = 22.87 mm−1 |
b = 10.649 (3) Å | T = 163 K |
c = 16.763 (5) Å | 0.10 × 0.07 × 0.05 mm |
β = 107.632 (4)° |
Rigaku Saturn70 CCD diffractometer | 3255 independent reflections |
Absorption correction: numerical (ABSCOR; Higashi, 1999) | 3136 reflections with I > 2σ(I) |
Tmin = 0.638, Tmax = 0.880 | Rint = 0.076 |
15149 measured reflections |
R[F2 > 2σ(F2)] = 0.034 | 6 restraints |
wR(F2) = 0.088 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.09 | Δρmax = 1.71 e Å−3 |
3255 reflections | Δρmin = −2.85 e Å−3 |
188 parameters |
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. |
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. |
x | y | z | Uiso*/Ueq | ||
U1 | 0.41912 (3) | 0.20869 (2) | 0.332933 (15) | 0.01529 (10) | |
U2 | 0.71490 (3) | 0.06455 (2) | 0.542406 (14) | 0.01236 (10) | |
O1 | 0.1576 (7) | 0.0796 (5) | 0.3408 (3) | 0.0247 (11) | |
O2 | 0.1274 (7) | 0.1931 (5) | 0.2295 (3) | 0.0272 (12) | |
O3 | 0.7084 (7) | 0.2370 (6) | 0.4457 (4) | 0.0296 (13) | |
O4 | 0.6738 (7) | 0.3262 (6) | 0.3266 (4) | 0.0306 (13) | |
O5 | 0.4581 (6) | 0.0936 (5) | 0.4484 (3) | 0.0217 (11) | |
O6 | 0.3486 (7) | 0.3399 (5) | 0.3788 (4) | 0.0277 (12) | |
O7 | 0.4880 (7) | 0.0816 (5) | 0.2841 (4) | 0.0277 (12) | |
O8 | 0.3755 (7) | 0.3336 (5) | 0.2040 (3) | 0.0230 (11) | |
H8A | 0.403 (12) | 0.406 (4) | 0.188 (5) | 0.034* | |
H8B | 0.367 (13) | 0.286 (6) | 0.160 (4) | 0.034* | |
O9 | 0.6588 (7) | 0.1628 (5) | 0.6159 (4) | 0.0264 (12) | |
O10 | 0.7947 (6) | −0.0283 (5) | 0.4734 (3) | 0.0236 (11) | |
O11 | 0.9960 (6) | 0.1499 (5) | 0.5992 (3) | 0.0202 (10) | |
H11A | 1.075 (7) | 0.121 (8) | 0.580 (5) | 0.030* | |
H11B | 1.047 (9) | 0.200 (7) | 0.641 (4) | 0.030* | |
O12 | 0.3208 (9) | 0.2904 (6) | 0.5615 (4) | 0.0376 (15) | |
H12 | 0.3876 | 0.2346 | 0.5557 | 0.056* | |
C1 | 0.0629 (9) | 0.1183 (7) | 0.2696 (4) | 0.0207 (14) | |
C2 | −0.1168 (10) | 0.0795 (8) | 0.2383 (6) | 0.0332 (19) | |
H2A | −0.1601 | 0.0663 | 0.2859 | 0.040* | |
H2B | −0.1261 | 0.0013 | 0.2064 | 0.040* | |
H2C | −0.1825 | 0.1454 | 0.2020 | 0.040* | |
C3 | 0.7675 (10) | 0.2993 (7) | 0.3966 (5) | 0.0239 (16) | |
C4 | 0.9472 (12) | 0.3420 (11) | 0.4242 (7) | 0.049 (3) | |
H4A | 0.9639 | 0.4053 | 0.3850 | 0.059* | |
H4B | 1.0212 | 0.2701 | 0.4252 | 0.059* | |
H4C | 0.9741 | 0.3785 | 0.4803 | 0.059* | |
C5 | 0.4006 (16) | 0.4061 (10) | 0.5715 (6) | 0.051 (3) | |
H5A | 0.4034 | 0.4418 | 0.6258 | 0.062* | |
H5B | 0.3388 | 0.4628 | 0.5267 | 0.062* | |
H5C | 0.5159 | 0.3955 | 0.5692 | 0.062* |
U11 | U22 | U33 | U12 | U13 | U23 | |
U1 | 0.01397 (15) | 0.01724 (15) | 0.01456 (16) | 0.00003 (8) | 0.00417 (11) | 0.00355 (8) |
U2 | 0.00972 (14) | 0.01612 (15) | 0.01148 (15) | −0.00104 (8) | 0.00357 (10) | 0.00029 (8) |
O1 | 0.018 (3) | 0.031 (3) | 0.021 (3) | −0.001 (2) | 0.000 (2) | 0.014 (2) |
O2 | 0.023 (3) | 0.037 (3) | 0.018 (3) | −0.006 (2) | 0.002 (2) | 0.015 (2) |
O3 | 0.020 (3) | 0.034 (3) | 0.033 (3) | −0.006 (2) | 0.005 (2) | 0.016 (3) |
O4 | 0.022 (3) | 0.043 (3) | 0.025 (3) | −0.007 (2) | 0.003 (2) | 0.005 (2) |
O5 | 0.012 (2) | 0.031 (3) | 0.019 (3) | −0.006 (2) | 0.0002 (19) | 0.010 (2) |
O6 | 0.019 (3) | 0.032 (3) | 0.029 (3) | 0.006 (2) | 0.003 (2) | −0.001 (2) |
O7 | 0.026 (3) | 0.029 (3) | 0.029 (3) | 0.002 (2) | 0.011 (2) | −0.001 (2) |
O8 | 0.023 (3) | 0.025 (3) | 0.022 (3) | 0.001 (2) | 0.008 (2) | 0.011 (2) |
O9 | 0.021 (3) | 0.029 (3) | 0.032 (3) | 0.000 (2) | 0.011 (2) | −0.008 (2) |
O10 | 0.016 (2) | 0.032 (3) | 0.022 (3) | −0.004 (2) | 0.004 (2) | −0.009 (2) |
O11 | 0.014 (2) | 0.027 (3) | 0.022 (3) | −0.006 (2) | 0.009 (2) | −0.010 (2) |
O12 | 0.042 (4) | 0.040 (4) | 0.033 (3) | 0.004 (3) | 0.014 (3) | 0.004 (3) |
C1 | 0.017 (3) | 0.020 (3) | 0.020 (3) | 0.000 (3) | −0.001 (3) | 0.006 (3) |
C2 | 0.016 (4) | 0.043 (5) | 0.036 (5) | −0.006 (3) | 0.001 (3) | 0.014 (4) |
C3 | 0.023 (4) | 0.021 (3) | 0.031 (4) | −0.005 (3) | 0.012 (3) | 0.003 (3) |
C4 | 0.028 (5) | 0.073 (7) | 0.044 (6) | −0.014 (5) | 0.006 (4) | 0.021 (5) |
C5 | 0.072 (8) | 0.041 (5) | 0.032 (5) | 0.009 (5) | 0.002 (5) | −0.005 (4) |
U1—O7 | 1.765 (6) | O4—C3 | 1.230 (10) |
U1—O6 | 1.779 (6) | O5—U2i | 2.252 (5) |
U1—O5 | 2.230 (5) | O8—H8A | 0.87 (2) |
U1—O8 | 2.469 (5) | O8—H8B | 0.87 (2) |
U1—O4 | 2.494 (6) | O11—H11A | 0.87 (2) |
U1—O2 | 2.528 (6) | O11—H11B | 0.87 (2) |
U1—O3 | 2.592 (6) | O12—C5 | 1.385 (12) |
U1—O1 | 2.614 (5) | O12—H12 | 0.8400 |
U2—O9 | 1.784 (5) | C1—C2 | 1.487 (10) |
U2—O10 | 1.795 (5) | C2—H2A | 0.9800 |
U2—O5i | 2.252 (5) | C2—H2B | 0.9800 |
U2—O5 | 2.261 (5) | C2—H2C | 0.9800 |
U2—O11 | 2.422 (5) | C3—C4 | 1.498 (12) |
U2—O3 | 2.438 (5) | C4—H4A | 0.9800 |
U2—O1i | 2.461 (5) | C4—H4B | 0.9800 |
O1—C1 | 1.284 (8) | C4—H4C | 0.9800 |
O1—U2i | 2.461 (5) | C5—H5A | 0.9800 |
O2—C1 | 1.262 (9) | C5—H5B | 0.9800 |
O3—C3 | 1.268 (9) | C5—H5C | 0.9800 |
O7—U1—O6 | 178.0 (3) | O5—U2—O1i | 136.78 (17) |
O7—U1—O5 | 89.9 (2) | O11—U2—O1i | 77.77 (18) |
O6—U1—O5 | 92.1 (2) | O3—U2—O1i | 156.28 (18) |
O7—U1—O8 | 89.4 (2) | C1—O1—U2i | 159.4 (5) |
O6—U1—O8 | 88.6 (2) | C1—O1—U1 | 94.1 (4) |
O5—U1—O8 | 179.2 (2) | U2i—O1—U1 | 101.70 (18) |
O7—U1—O4 | 88.0 (2) | C1—O2—U1 | 98.8 (4) |
O6—U1—O4 | 91.2 (2) | C3—O3—U2 | 153.0 (5) |
O5—U1—O4 | 114.24 (18) | C3—O3—U1 | 92.6 (5) |
O8—U1—O4 | 66.05 (18) | U2—O3—U1 | 103.06 (19) |
O7—U1—O2 | 90.7 (2) | C3—O4—U1 | 98.3 (5) |
O6—U1—O2 | 88.5 (2) | U1—O5—U2i | 122.8 (2) |
O5—U1—O2 | 114.60 (17) | U1—O5—U2 | 122.6 (2) |
O8—U1—O2 | 65.10 (17) | U2i—O5—U2 | 109.9 (2) |
O4—U1—O2 | 131.14 (18) | U1—O8—H8A | 140 (6) |
O7—U1—O3 | 93.8 (2) | U1—O8—H8B | 112 (5) |
O6—U1—O3 | 87.1 (2) | H8A—O8—H8B | 102 (4) |
O5—U1—O3 | 64.64 (17) | U2—O11—H11A | 118 (5) |
O8—U1—O3 | 115.72 (17) | U2—O11—H11B | 136 (5) |
O4—U1—O3 | 50.00 (18) | H11A—O11—H11B | 105 (4) |
O2—U1—O3 | 175.5 (2) | C5—O12—H12 | 109.5 |
O7—U1—O1 | 90.8 (2) | O2—C1—O1 | 117.2 (6) |
O6—U1—O1 | 90.1 (2) | O2—C1—C2 | 122.2 (7) |
O5—U1—O1 | 64.63 (17) | O1—C1—C2 | 120.5 (7) |
O8—U1—O1 | 115.07 (17) | C1—C2—H2A | 109.5 |
O4—U1—O1 | 178.31 (18) | C1—C2—H2B | 109.5 |
O2—U1—O1 | 49.97 (16) | H2A—C2—H2B | 109.5 |
O3—U1—O1 | 129.03 (16) | C1—C2—H2C | 109.5 |
O9—U2—O10 | 173.7 (2) | H2A—C2—H2C | 109.5 |
O9—U2—O5i | 94.8 (2) | H2B—C2—H2C | 109.5 |
O10—U2—O5i | 90.1 (2) | O4—C3—O3 | 118.9 (7) |
O9—U2—O5 | 90.6 (2) | O4—C3—C4 | 120.7 (7) |
O10—U2—O5 | 94.8 (2) | O3—C3—C4 | 120.4 (8) |
O5i—U2—O5 | 70.1 (2) | C3—C4—H4A | 109.5 |
O9—U2—O11 | 86.2 (2) | C3—C4—H4B | 109.5 |
O10—U2—O11 | 87.5 (2) | H4A—C4—H4B | 109.5 |
O5i—U2—O11 | 144.73 (18) | C3—C4—H4C | 109.5 |
O5—U2—O11 | 145.17 (18) | H4A—C4—H4C | 109.5 |
O9—U2—O3 | 93.4 (2) | H4B—C4—H4C | 109.5 |
O10—U2—O3 | 85.7 (2) | O12—C5—H5A | 109.5 |
O5i—U2—O3 | 136.25 (19) | O12—C5—H5B | 109.5 |
O5—U2—O3 | 66.93 (18) | H5A—C5—H5B | 109.5 |
O11—U2—O3 | 78.65 (18) | O12—C5—H5C | 109.5 |
O9—U2—O1i | 87.5 (2) | H5A—C5—H5C | 109.5 |
O10—U2—O1i | 90.8 (2) | H5B—C5—H5C | 109.5 |
O5i—U2—O1i | 67.08 (17) |
Symmetry code: (i) −x+1, −y, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
O12—H12···O9 | 0.84 | 2.31 | 3.009 (10) | 141 |
O12—H12···O5 | 0.84 | 2.54 | 3.257 (9) | 143 |
O8—H8A···O7ii | 0.87 (6) | 2.07 (6) | 2.859 (8) | 151 (7) |
O8—H8B···O12iii | 0.88 (7) | 1.78 (6) | 2.645 (8) | 170 (9) |
O11—H11A···O10iv | 0.87 (7) | 1.88 (7) | 2.736 (7) | 166 (8) |
O11—H11B···O2v | 0.88 (7) | 1.83 (7) | 2.705 (7) | 173 (7) |
Symmetry codes: (ii) −x+1, y+1/2, −z+1/2; (iii) x, −y+1/2, z−1/2; (iv) −x+2, −y, −z+1; (v) x+1, −y+1/2, z+1/2. |
Experimental details
Crystal data | |
Chemical formula | [U4(C2H3O2)4O10(H2O)4]·2CH4O |
Mr | 1484.44 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 163 |
a, b, c (Å) | 8.334 (3), 10.649 (3), 16.763 (5) |
β (°) | 107.632 (4) |
V (Å3) | 1417.8 (8) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 22.87 |
Crystal size (mm) | 0.10 × 0.07 × 0.05 |
Data collection | |
Diffractometer | Rigaku Saturn70 CCD |
Absorption correction | Numerical (ABSCOR; Higashi, 1999) |
Tmin, Tmax | 0.638, 0.880 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 15149, 3255, 3136 |
Rint | 0.076 |
(sin θ/λ)max (Å−1) | 0.650 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.034, 0.088, 1.09 |
No. of reflections | 3255 |
No. of parameters | 188 |
No. of restraints | 6 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 1.71, −2.85 |
Computer programs: CrystalClear-SM Expert (Rigaku, 2009), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), Mercury (Macrae et al., 2006), publCIF (Westrip, 2010).
D—H···A | D—H | H···A | D···A | D—H···A |
O12—H12···O9 | 0.84 | 2.31 | 3.009 (10) | 141 |
O8—H8A···O7i | 0.87 (6) | 2.07 (6) | 2.859 (8) | 151 (7) |
O8—H8B···O12ii | 0.88 (7) | 1.78 (6) | 2.645 (8) | 170 (9) |
O11—H11A···O10iii | 0.87 (7) | 1.88 (7) | 2.736 (7) | 166 (8) |
O11—H11B···O2iv | 0.88 (7) | 1.83 (7) | 2.705 (7) | 173 (7) |
Symmetry codes: (i) −x+1, y+1/2, −z+1/2; (ii) x, −y+1/2, z−1/2; (iii) −x+2, −y, −z+1; (iv) x+1, −y+1/2, z+1/2. |
Acknowledgements
The Egyptian Government is thanked for the scholarship to HS. LND would like to acknowledge Dr Amy Sarjeant, Northwestern University, for a helpful discussion about heavy atom structure refinements. Financial support from the Dean of Science and the Chemistry Department, Memorial University of Newfoundland, is acknowledged.
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
In connection with our on-going studies on metal-binding properties of a new series of macrocylic polyamide compounds, we were interested in determining whether such macrocycles, by analogy with analogous salen (N,N'-Ethylenebis(salicylimine)) compounds, would also form stable uranyl complexes. Using similar conditions to those which Amato et al. (2007) employed with their salens, the title compound crystallized out in the form reported herein.
Bond valence sum calculations (Wills, 2010) performed on the title compound indicate that both crystallographically independent uranium atoms are in the +6 oxidations state (U1 = 6.095, U2 = 6.074). The centrosymmetric U(VI) tetramer consists of two hexagonal bipyramids, and two pentagonal bipyramids (U1 and U2, and symmetry equivalents (-x + 1, -y, -z + 1), respectively; Figure 1), with (UO2)2+ oxygen-atoms occupying the axial positions for both U1 and U2. For U1, the equatorial plane consists of trans-bidentate acetate anions, each with one bridging µ2-O-atom (O1 and O3), and a µ3-O2- anion (O5) trans to a water molecule. The equatorial plane of U2 is therefore composed of the aforementioned µ2-O and µ3-O atoms, and their inversion-symmetry generated counter-parts, as well as water molecule (O11). Similar to the description given by Andrews et al. (2008) for [Bi2(µ3-O)(OCH(CF3)2)2(µ-OCH(CF3)2)2(Solv)]2 (Solv = C7H8, Et2O, thf) tetramers, this complex consists of a near planar, ten atom "raft", with maximum deviation from the least squares plane [U1, U2, O1–5 and symmetry equivalents (-x + 1, -y, -z + 1)] of 0.294 (6) Å for O5. Examination of longer range interactions reveals numerous hydrogen bonds, including a lattice solvent methanol molecule bound to one of the pentagonal bipyramidal uranyl oxygen atoms (O12—H12···O9; Figure 1), which further bridges to a bound water molecule of a second tetramer (O8—H8B···O12iii, (iii) x, -y+1/2, z-1/2; Figure 2, green dashed lines.) The tetramers interact via an additional hydrogen bond, wherby the aforementioned water molecule acts as a donor to one of the hexagonal bipyramidal uranyl oxygen atoms on the first assembly (O8—H8A···O7ii, (ii) -x+1, y+1/2, -z+1/2; Figure 2, black dashed lines) leading to a 24-membered H-bonded ring (graph set notation R44(24)) which spans all four tetramers present in the unit cell.