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The coordination polyhedron of the U atom in the title compound, [U(C2H3O2)2O2(H2O)2]·2CH3COOH, is a distorted hexa­gonal bipyramid, with the equatorial positions occupied by four O atoms of two bidentate-chelating acetate anions and two O atoms of coordinated water mol­ecules. The complex lies on an inversion centre. A two-dimensional network of hydrogen bonds is present in the crystal structure.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805029922/bh6027sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805029922/bh6027Isup2.hkl
Contains datablock I

CCDC reference: 287446

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.007 Å
  • R factor = 0.022
  • wR factor = 0.051
  • Data-to-parameter ratio = 20.9

checkCIF/PLATON results

No syntax errors found



Alert level C ABSTM02_ALERT_3_C The ratio of expected to reported Tmax/Tmin(RR) is > 1.10 Tmin and Tmax reported: 0.168 0.289 Tmin and Tmax expected: 0.121 0.289 RR = 1.391 Please check that your absorption correction is appropriate. PLAT060_ALERT_3_C Ratio Tmax/Tmin (Exp-to-Rep) (too) Large ....... 1.36 PLAT199_ALERT_1_C Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_C Check the Reported _diffrn_ambient_temperature . 293 K PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 2.26 PLAT790_ALERT_4_C Centre of Gravity not Within Unit Cell: Resd. # 2 C2 H4 O2
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 6 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 2 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion

Comment top

Carboxylate compounds of the actinides play a significant role in laboratory practice and radiochemical industry. Several uranyl compounds are known, in which both acetate anions and acetic acid molecules are present (Ramos Silva et al., 1999; Grigor'ev et al., 2004). Here, we present a further example of a uranyl acetate compound, (I), containing acetic acid as solvate.

The U atom in compound (I) lies on an inversion centre. Itscoordination polyhedron is a distorted hexagonal bipyramid, with the equatorial positions occupied by four O atoms of two bidentate-chelating acetate anions and two O atoms of coordination water molecules (Fig. 1). Crystallographically independent bond lengths in the U-atom environment are given in Table 1.

The coordination water and solvate acetic acid molecules act as H donors in several types of hydrogen bonds (Table 2). The acceptors in these bonds are O atoms of acetate anions and acetic acid. The hydrogen bonding results in the formation of infinite chains in the [100] direction (Fig. 2) and these chains are combined into layers parallel to the (011) plane (Fig. 3).

Experimental top

Crystals of (I) were obtained as an admixture in an attempt to recrystallize anhydrous uranyl acetate in glacial acetic acid at 413 K.

Refinement top

All H atoms were initially located in a difference Fourier map. The methyl H atoms were then constrained to an ideal geometry, with C—H distances of 0.96 Å and Uiso(H) = 1.5Ueq(C), but each group was allowed to rotate freely about its C—C bond. The positions of H atoms bonded to O atoms were refined freely along with isotropic displacement parameters.

Computing details top

Data collection: P3/PC (Siemens, 1989); cell refinement: P3/PC; data reduction: P3/PC; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: SHELXTL (Sheldrick, 1998); software used to prepare material for publication: SHELXTL.

Figures top
[Figure 1] Fig. 1. A view of (I), showing the atom-labelling scheme for the asymmetric unit. Displacement ellipsoids are drawn at the 50% probability level and H atoms are represented by circles of arbitrary size. Dashed lines indicate the hydrogen-bonding interactions.
[Figure 2] Fig. 2. Part of an infinite chain in the crystal structure of (I).
[Figure 3] Fig. 3. A layer in the crystal structure of (I), viewed along the direction of the chains.
Bis(acetato)diaquadioxouranium(VI) acetic acid disolvate top
Crystal data top
[UO2(C2H3O2)2(H2O)2]·2C2H4O2Z = 1
Mr = 544.25F(000) = 254
Triclinic, P1Dx = 2.291 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 6.914 (2) ÅCell parameters from 24 reflections
b = 7.822 (2) Åθ = 13.1–14.0°
c = 8.211 (2) ŵ = 10.34 mm1
α = 95.00 (2)°T = 293 K
β = 113.74 (2)°Irregular, yellow
γ = 99.79 (2)°0.24 × 0.18 × 0.12 mm
V = 394.6 (2) Å3
Data collection top
Siemens P3/PC
diffractometer
2316 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.021
Graphite monochromatorθmax = 30.1°, θmin = 2.7°
ω/2θ scansh = 09
Absorption correction: ψ scan
(North et al., 1968)
k = 1110
Tmin = 0.168, Tmax = 0.289l = 1110
2494 measured reflections2 standard reflections every 98 reflections
2316 independent reflections intensity decay: 0.0%
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.022Hydrogen site location: difference Fourier map
wR(F2) = 0.051H atoms treated by a mixture of independent and constrained refinement
S = 1.05 w = 1/[σ2(Fo2) + (0.0313P)2]
where P = (Fo2 + 2Fc2)/3
2316 reflections(Δ/σ)max < 0.001
111 parametersΔρmax = 1.36 e Å3
0 restraintsΔρmin = 1.55 e Å3
Crystal data top
[UO2(C2H3O2)2(H2O)2]·2C2H4O2γ = 99.79 (2)°
Mr = 544.25V = 394.6 (2) Å3
Triclinic, P1Z = 1
a = 6.914 (2) ÅMo Kα radiation
b = 7.822 (2) ŵ = 10.34 mm1
c = 8.211 (2) ÅT = 293 K
α = 95.00 (2)°0.24 × 0.18 × 0.12 mm
β = 113.74 (2)°
Data collection top
Siemens P3/PC
diffractometer
2316 reflections with I > 2σ(I)
Absorption correction: ψ scan
(North et al., 1968)
Rint = 0.021
Tmin = 0.168, Tmax = 0.2892 standard reflections every 98 reflections
2494 measured reflections intensity decay: 0.0%
2316 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0220 restraints
wR(F2) = 0.051H atoms treated by a mixture of independent and constrained refinement
S = 1.05Δρmax = 1.36 e Å3
2316 reflectionsΔρmin = 1.55 e Å3
111 parameters
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
U0.50000.50000.50000.02319 (6)
O10.8816 (4)0.6529 (4)0.6462 (4)0.0421 (7)
H1A0.936 (10)0.717 (8)0.754 (9)0.052 (15)*
H1B0.964 (14)0.638 (11)0.613 (12)0.09 (3)*
O20.5474 (5)0.4010 (4)0.6929 (4)0.0388 (6)
O30.4226 (4)0.2003 (3)0.3289 (4)0.0388 (6)
O40.7500 (4)0.3501 (3)0.4119 (4)0.0347 (5)
C10.6119 (6)0.2055 (4)0.3420 (5)0.0284 (6)
C20.6669 (7)0.0461 (5)0.2752 (7)0.0422 (9)
H2A0.54880.05380.24370.063*
H2B0.79520.02520.36810.063*
H2C0.69230.06390.17060.063*
O50.0829 (6)0.1835 (5)0.0019 (4)0.0480 (7)
O60.1202 (5)0.0887 (4)0.2740 (4)0.0405 (6)
H60.217 (10)0.006 (8)0.272 (8)0.049 (15)*
C30.0257 (6)0.1988 (5)0.1181 (5)0.0332 (7)
C40.1547 (9)0.3402 (6)0.1096 (7)0.0507 (11)
H4A0.16050.44710.03910.076*
H4B0.28970.30480.05450.076*
H4C0.13000.35940.22950.076*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
U0.01944 (8)0.02120 (8)0.02777 (9)0.00096 (5)0.01174 (6)0.00310 (5)
O10.0222 (12)0.0482 (16)0.0470 (16)0.0042 (11)0.0164 (11)0.0211 (13)
O20.0422 (15)0.0369 (13)0.0379 (14)0.0070 (11)0.0185 (12)0.0062 (11)
O30.0248 (12)0.0300 (12)0.0569 (17)0.0010 (9)0.0184 (12)0.0119 (11)
O40.0266 (11)0.0294 (11)0.0466 (15)0.0003 (9)0.0195 (11)0.0085 (10)
C10.0284 (15)0.0292 (14)0.0294 (15)0.0051 (12)0.0159 (13)0.0014 (12)
C20.044 (2)0.0322 (17)0.057 (2)0.0092 (15)0.0303 (19)0.0053 (16)
O50.0474 (17)0.0554 (18)0.0382 (15)0.0018 (14)0.0213 (13)0.0047 (13)
O60.0463 (16)0.0355 (13)0.0344 (14)0.0029 (12)0.0186 (12)0.0038 (11)
C30.0358 (17)0.0293 (15)0.0328 (17)0.0087 (13)0.0130 (14)0.0015 (13)
C40.054 (3)0.040 (2)0.050 (2)0.0085 (19)0.023 (2)0.0008 (18)
Geometric parameters (Å, º) top
U—O2i1.760 (3)C1—C21.487 (5)
U—O21.760 (3)C2—H2A0.9600
U—O12.441 (3)C2—H2B0.9600
U—O1i2.441 (3)C2—H2C0.9600
U—O3i2.480 (3)O5—C31.208 (5)
U—O32.480 (3)O6—C31.323 (4)
U—O42.536 (3)O6—H60.86 (6)
U—O4i2.536 (3)C3—C41.493 (6)
O1—H1A0.88 (7)C4—H4A0.9600
O1—H1B0.75 (9)C4—H4B0.9600
O3—C11.262 (4)C4—H4C0.9600
O4—C11.265 (4)
O2i—U—O2180.000 (1)O3—U—O4i128.94 (8)
O2i—U—O192.61 (14)O4—U—O4i180.000 (1)
O2—U—O187.39 (14)U—O1—H1A121 (4)
O2i—U—O1i87.39 (13)U—O1—H1B124 (7)
O2—U—O1i92.61 (14)H1A—O1—H1B114 (7)
O1—U—O1i180.0C1—O3—U96.8 (2)
O2i—U—O3i86.98 (13)C1—O4—U94.0 (2)
O2—U—O3i93.02 (13)O3—C1—O4117.7 (3)
O1—U—O3i64.58 (10)O3—C1—C2120.4 (3)
O1i—U—O3i115.42 (10)O4—C1—C2121.9 (3)
O2i—U—O393.02 (13)C1—C2—H2A109.5
O2—U—O386.98 (13)C1—C2—H2B109.5
O1—U—O3115.42 (10)H2A—C2—H2B109.5
O1i—U—O364.58 (10)C1—C2—H2C109.5
O3i—U—O3180.0H2A—C2—H2C109.5
O2i—U—O486.50 (12)H2B—C2—H2C109.5
O2—U—O493.50 (12)C3—O6—H6110 (4)
O1—U—O465.22 (9)O5—C3—O6122.3 (4)
O1i—U—O4114.78 (9)O5—C3—C4125.0 (4)
O3i—U—O4128.94 (8)O6—C3—C4112.7 (4)
O3—U—O451.06 (8)C3—C4—H4A109.5
O2i—U—O4i93.50 (12)C3—C4—H4B109.5
O2—U—O4i86.50 (12)H4A—C4—H4B109.5
O1—U—O4i114.78 (9)C3—C4—H4C109.5
O1i—U—O4i65.22 (9)H4A—C4—H4C109.5
O3i—U—O4i51.06 (8)H4B—C4—H4C109.5
Symmetry code: (i) x+1, y+1, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O6—H6···O30.86 (6)1.84 (6)2.672 (4)163 (6)
O1—H1A···O5ii0.88 (7)1.86 (7)2.727 (4)168 (6)
O1—H1B···O4iii0.75 (9)2.05 (9)2.778 (4)163 (9)
Symmetry codes: (ii) x+1, y+1, z+1; (iii) x+2, y+1, z+1.

Experimental details

Crystal data
Chemical formula[UO2(C2H3O2)2(H2O)2]·2C2H4O2
Mr544.25
Crystal system, space groupTriclinic, P1
Temperature (K)293
a, b, c (Å)6.914 (2), 7.822 (2), 8.211 (2)
α, β, γ (°)95.00 (2), 113.74 (2), 99.79 (2)
V3)394.6 (2)
Z1
Radiation typeMo Kα
µ (mm1)10.34
Crystal size (mm)0.24 × 0.18 × 0.12
Data collection
DiffractometerSiemens P3/PC
diffractometer
Absorption correctionψ scan
(North et al., 1968)
Tmin, Tmax0.168, 0.289
No. of measured, independent and
observed [I > 2σ(I)] reflections
2494, 2316, 2316
Rint0.021
(sin θ/λ)max1)0.705
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.022, 0.051, 1.05
No. of reflections2316
No. of parameters111
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)1.36, 1.55

Computer programs: P3/PC (Siemens, 1989), P3/PC, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), SHELXTL (Sheldrick, 1998), SHELXTL.

Selected bond lengths (Å) top
U—O21.760 (3)U—O32.480 (3)
U—O12.441 (3)U—O42.536 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O6—H6···O30.86 (6)1.84 (6)2.672 (4)163 (6)
O1—H1A···O5i0.88 (7)1.86 (7)2.727 (4)168 (6)
O1—H1B···O4ii0.75 (9)2.05 (9)2.778 (4)163 (9)
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+2, y+1, z+1.
 

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