Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680301883X/br6112sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S160053680301883X/br6112Isup2.hkl |
CCDC reference: 222829
The starting material, K3[Cr(nta)2]·2H2O, was synthesized according to the literature (Visser et al., 1999). This complex was suspended in water and a blue–black precipitate was deposited after several days. Recrystallization of the precipitate from water afforded brown crystals of (I) suitable for X-ray analysis.
H atoms of nta3− and bridging OH− were placed geometrically, with O–H distances of 0.91 Å and C–H distances of 0.97 Å, and these atoms were refined using a riding model, Uiso(H) = Ueq(O or C). Other H atoms of hydrated water molecules were not included. In the final difference synthesis map, four rather large peaks (more than 0.65 e Å−3) were found at (a) (0.0331, 0.0000, 0.4198), (b) (0.1122, 0.3315, 0.6691), (c) (0.3252, 0.1676, 0.4900), and (d) (0.0425, 0.3444, 0.4254). Peaks a and b were close to O7 and O4 at distances of 0.666 and 1.142 Å, respectively, while peaks c and d were located around the K atom at distances of 1.283 and 1.075 Å, respectively. Thus, these peaks are not related to the H atoms of hydrated water molecules.
Data collection: MSC/AFC Diffractometer Control Software (Rigaku, 1985); cell refinement: MSC/AFC Diffractometer Control Software; data reduction: TEXSAN (Molecular Structure Cooperation and Rigaku, 2000); program(s) used to solve structure: SHELXS86 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP (Johnson, 1970); software used to prepare material for publication: SHELXL97.
Fig. 1. Perspective view of the anionic part of (I). Displacement ellipsoids are drawn at 50% probability level. [Symmetry codes: (i) x, −y, z; (ii) −x, −y, 1 − z; (iii) −x, y, 1 − z.] |
K2[Cr2(C6H6NO6)2(OH)2]·6H2O | F(000) = 716 |
Mr = 700.55 | Dx = 1.863 Mg m−3 |
Monoclinic, C2/m | Mo Kα radiation, λ = 0.71069 Å |
Hall symbol: -C 2y | Cell parameters from 25 reflections |
a = 7.311 (2) Å | θ = 14.7–15.0° |
b = 13.321 (2) Å | µ = 1.30 mm−1 |
c = 12.862 (2) Å | T = 296 K |
β = 94.45 (2)° | Block, brown |
V = 1248.8 (5) Å3 | 0.30 × 0.22 × 0.20 mm |
Z = 2 |
Rigaku AFC-5R diffractometer | 1277 reflections with I > 2σ(I) |
Radiation source: rotating anode | Rint = 0.025 |
Graphite monochromator | θmax = 30.0°, θmin = 3.1° |
ω–2θ scans | h = 0→9 |
Absorption correction: integration (Coppens et al., 1965) | k = 0→17 |
Tmin = 0.755, Tmax = 0.790 | l = −17→17 |
2000 measured reflections | 3 standard reflections every 150 reflections |
1869 independent reflections | intensity decay: 2.1% |
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)] = 0.056 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.179 | H-atom parameters constrained |
S = 1.04 | w = 1/[σ2(Fo2) + (0.1161P)2 + 0.9272P] where P = (Fo2 + 2Fc2)/3 |
1869 reflections | (Δ/σ)max = 0.001 |
99 parameters | Δρmax = 1.81 e Å−3 |
0 restraints | Δρmin = −0.71 e Å−3 |
K2[Cr2(C6H6NO6)2(OH)2]·6H2O | V = 1248.8 (5) Å3 |
Mr = 700.55 | Z = 2 |
Monoclinic, C2/m | Mo Kα radiation |
a = 7.311 (2) Å | µ = 1.30 mm−1 |
b = 13.321 (2) Å | T = 296 K |
c = 12.862 (2) Å | 0.30 × 0.22 × 0.20 mm |
β = 94.45 (2)° |
Rigaku AFC-5R diffractometer | 1277 reflections with I > 2σ(I) |
Absorption correction: integration (Coppens et al., 1965) | Rint = 0.025 |
Tmin = 0.755, Tmax = 0.790 | 3 standard reflections every 150 reflections |
2000 measured reflections | intensity decay: 2.1% |
1869 independent reflections |
R[F2 > 2σ(F2)] = 0.056 | 0 restraints |
wR(F2) = 0.179 | H-atom parameters constrained |
S = 1.04 | Δρmax = 1.81 e Å−3 |
1869 reflections | Δρmin = −0.71 e Å−3 |
99 parameters |
Experimental. none |
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 | ||
Cr | 0.14512 (10) | 0.0000 | 0.58737 (5) | 0.0176 (2) | |
K | 0.0000 | 0.32166 (9) | 0.5000 | 0.0340 (3) | |
O1 | 0.4150 (4) | 0.0000 | 0.6034 (3) | 0.0220 (7) | |
O2 | 0.6559 (5) | 0.0000 | 0.7198 (3) | 0.0335 (9) | |
O3 | 0.1490 (4) | 0.1477 (2) | 0.60712 (19) | 0.0270 (5) | |
O4 | 0.0745 (5) | 0.2649 (2) | 0.7190 (3) | 0.0468 (8) | |
O7 | 0.1218 (5) | 0.0000 | 0.4363 (3) | 0.0309 (9) | |
O8 | 0.3125 (9) | 0.5000 | 0.9839 (4) | 0.0605 (15) | |
O9 | 0.1534 (9) | 0.3207 (4) | 0.9305 (4) | 0.0926 (19) | |
N1 | 0.1642 (5) | 0.0000 | 0.7475 (3) | 0.0189 (7) | |
C1 | 0.3636 (7) | 0.0000 | 0.7860 (4) | 0.0325 (12) | |
C2 | 0.4909 (7) | 0.0000 | 0.6985 (4) | 0.0220 (9) | |
C3 | 0.0719 (5) | 0.0945 (3) | 0.7772 (3) | 0.0243 (7) | |
C4 | 0.1018 (5) | 0.1772 (3) | 0.6966 (3) | 0.0271 (7) | |
H1 | 0.3888 | −0.0588 | 0.8292 | 0.032* | |
H3A | 0.1218 | 0.1160 | 0.8457 | 0.024* | |
H3B | −0.0584 | 0.0825 | 0.7804 | 0.024* | |
H7 | 0.2097 | 0.0000 | 0.3899 | 0.031* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cr | 0.0133 (3) | 0.0250 (4) | 0.0145 (3) | 0.000 | 0.0004 (2) | 0.000 |
K | 0.0441 (7) | 0.0242 (6) | 0.0347 (6) | 0.000 | 0.0101 (5) | 0.000 |
O1 | 0.0122 (14) | 0.0345 (19) | 0.0192 (15) | 0.000 | 0.0009 (12) | 0.000 |
O2 | 0.0121 (16) | 0.057 (3) | 0.032 (2) | 0.000 | 0.0010 (14) | 0.000 |
O3 | 0.0333 (14) | 0.0255 (12) | 0.0220 (11) | 0.0008 (11) | 0.0020 (10) | 0.0017 (10) |
O4 | 0.070 (2) | 0.0262 (14) | 0.0443 (18) | 0.0056 (15) | 0.0035 (17) | −0.0016 (13) |
O7 | 0.0150 (16) | 0.062 (3) | 0.0161 (15) | 0.000 | 0.0030 (12) | 0.000 |
O8 | 0.067 (4) | 0.069 (4) | 0.044 (3) | 0.000 | −0.004 (3) | 0.000 |
O9 | 0.142 (5) | 0.064 (3) | 0.067 (3) | 0.002 (3) | −0.022 (3) | −0.013 (2) |
N1 | 0.0160 (17) | 0.0262 (19) | 0.0147 (16) | 0.000 | 0.0020 (13) | 0.000 |
C1 | 0.016 (2) | 0.064 (4) | 0.018 (2) | 0.000 | 0.0003 (16) | 0.000 |
C2 | 0.018 (2) | 0.031 (2) | 0.018 (2) | 0.000 | 0.0015 (16) | 0.000 |
C3 | 0.0246 (16) | 0.0269 (16) | 0.0220 (15) | 0.0009 (13) | 0.0059 (12) | −0.0060 (12) |
C4 | 0.0285 (18) | 0.0263 (17) | 0.0261 (16) | −0.0005 (14) | −0.0008 (13) | −0.0006 (13) |
Cr—O7 | 1.937 (4) | N1—C1 | 1.502 (6) |
Cr—O7i | 1.951 (4) | C1—C2 | 1.514 (7) |
Cr—O1 | 1.968 (3) | C1—H1 | 0.9700 |
Cr—O3 | 1.983 (3) | C3—C4 | 1.541 (5) |
Cr—N1 | 2.054 (4) | C3—H3A | 0.9700 |
O1—C2 | 1.304 (6) | C3—H3B | 0.9700 |
O2—C2 | 1.216 (6) | K—O1ii | 2.815 (2) |
O3—C4 | 1.289 (5) | K—O3 | 2.868 (3) |
O4—C4 | 1.223 (5) | K—O4 | 2.926 (3) |
O7—H7 | 0.9100 | K—O3iii | 3.033 (3) |
N1—C3 | 1.492 (4) | ||
Cr···Cri | 2.9687 (15) | ||
O7—Cr—O7i | 80.46 (16) | N1—C1—C2 | 113.1 (4) |
O7—Cr—O1 | 96.56 (15) | O2—C2—O1 | 123.6 (5) |
O7i—Cr—O1 | 177.02 (14) | O2—C2—C1 | 119.3 (4) |
O7—Cr—O3 | 97.34 (7) | O1—C2—C1 | 117.1 (4) |
O7i—Cr—O3 | 91.38 (8) | N1—C3—C4 | 109.9 (3) |
O1—Cr—O3 | 89.00 (8) | O4—C4—O3 | 124.2 (4) |
O3—Cr—O3iv | 165.32 (14) | O4—C4—C3 | 119.4 (4) |
O7—Cr—N1 | 178.84 (16) | O3—C4—C3 | 116.4 (3) |
O7i—Cr—N1 | 98.38 (15) | Cr—O7—H7 | 130.2 |
O1—Cr—N1 | 84.60 (15) | N1—C1—H1 | 109.0 |
O3—Cr—N1 | 82.67 (7) | C2—C1—H1 | 109.0 |
C2—O1—Cr | 116.6 (3) | H1—C1—H1iv | 107.8 |
C4—O3—Cr | 114.5 (2) | N1—C3—H3A | 109.7 |
Cr—O7—Cri | 99.54 (16) | C4—C3—H3A | 109.7 |
C3iv—N1—C3 | 115.1 (4) | N1—C3—H3B | 109.7 |
C3—N1—C1 | 111.2 (2) | C4—C3—H3B | 109.7 |
C3—N1—Cr | 105.1 (2) | H3A—C3—H3B | 108.2 |
C1—N1—Cr | 108.6 (3) | ||
O3—Cr—O1—C2 | 82.73 (7) | O3—Cr—N1—C3 | 29.4 (2) |
O7—Cr—O3—C4 | 157.6 (3) | O3—Cr—N1—C1 | −89.68 (8) |
O7i—Cr—O3—C4 | 77.0 (3) | C3—N1—C1—C2 | −115.1 (2) |
O1—Cr—O3—C4 | −106.0 (3) | C3iv—N1—C3—C4 | −148.0 (3) |
O3iv—Cr—O3—C4 | −23.8 (8) | C1—N1—C3—C4 | 84.3 (4) |
N1—Cr—O3—C4 | −21.3 (3) | Cr—N1—C3—C4 | −33.0 (3) |
O3—Cr—O7—Cri | −90.17 (8) | Cr—O3—C4—O4 | −170.9 (3) |
O3—Cr—N1—C3iv | 151.2 (2) | Cr—O3—C4—C3 | 6.7 (4) |
O7—Cr—N1—C3 | −60.9 (2) | N1—C3—C4—O4 | −163.2 (4) |
O1—Cr—N1—C3 | 119.1 (2) | N1—C3—C4—O3 | 19.1 (4) |
Symmetry codes: (i) −x, −y, −z+1; (ii) −x+1/2, −y+1/2, −z+1; (iii) x−1/2, −y+1/2, z; (iv) x, −y, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O7—H7···O2v | 0.91 | 1.78 | 2.680 (5) | 169 |
Symmetry code: (v) −x+1, −y, −z+1. |
Experimental details
Crystal data | |
Chemical formula | K2[Cr2(C6H6NO6)2(OH)2]·6H2O |
Mr | 700.55 |
Crystal system, space group | Monoclinic, C2/m |
Temperature (K) | 296 |
a, b, c (Å) | 7.311 (2), 13.321 (2), 12.862 (2) |
β (°) | 94.45 (2) |
V (Å3) | 1248.8 (5) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 1.30 |
Crystal size (mm) | 0.30 × 0.22 × 0.20 |
Data collection | |
Diffractometer | Rigaku AFC-5R diffractometer |
Absorption correction | Integration (Coppens et al., 1965) |
Tmin, Tmax | 0.755, 0.790 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 2000, 1869, 1277 |
Rint | 0.025 |
(sin θ/λ)max (Å−1) | 0.704 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.056, 0.179, 1.04 |
No. of reflections | 1869 |
No. of parameters | 99 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 1.81, −0.71 |
Computer programs: MSC/AFC Diffractometer Control Software (Rigaku, 1985), MSC/AFC Diffractometer Control Software, TEXSAN (Molecular Structure Cooperation and Rigaku, 2000), SHELXS86 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), ORTEP (Johnson, 1970), SHELXL97.
Cr—O7 | 1.937 (4) | K—O1ii | 2.815 (2) |
Cr—O7i | 1.951 (4) | K—O3 | 2.868 (3) |
Cr—O1 | 1.968 (3) | K—O4 | 2.926 (3) |
Cr—O3 | 1.983 (3) | K—O3iii | 3.033 (3) |
Cr—N1 | 2.054 (4) | ||
Cr···Cri | 2.9687 (15) | ||
O7—Cr—O7i | 80.46 (16) | O3—Cr—O3iv | 165.32 (14) |
O7—Cr—O1 | 96.56 (15) | O7—Cr—N1 | 178.84 (16) |
O7i—Cr—O1 | 177.02 (14) | O7i—Cr—N1 | 98.38 (15) |
O7—Cr—O3 | 97.34 (7) | O1—Cr—N1 | 84.60 (15) |
O7i—Cr—O3 | 91.38 (8) | O3—Cr—N1 | 82.67 (7) |
O1—Cr—O3 | 89.00 (8) | Cr—O7—Cri | 99.54 (16) |
Symmetry codes: (i) −x, −y, −z+1; (ii) −x+1/2, −y+1/2, −z+1; (iii) x−1/2, −y+1/2, z; (iv) x, −y, z. |
The nitrilotriacetate ion (nta3−) may coordinate to a metal ion as a tridentate or tetradentate ligand via the one N and three carboxylate O atoms. The crystal structure of di(µ-hydroxo)bis[(nitrilotriacetato)chromium(III)] with the Cs+ cation was reported previously (Visser et al., 1999). This is another example of a [Cr2(µ-OH)2(nta)2]2− complex anion with a different cation, K+. The sharp-line electronic transitions and their splittings in chromium(III) complexes are very sensitive to the exact bond angles around the metal. Thus, it may be possible to extract the structural information from the electronic spectroscopy without a full X-ray structure determination (Hoggard, 1986; Choi, 1994); the relationship between environmental changes and geometric distortion may be found in the chromium(III) complexes. In order to examine the influence of cations and water contents of the crystal on the conformations of the CrIII complexes, the title complex, (I), was prepared and its crystal structure was determined.
The structure analysis showed that the crystal of (I) consists of a [Cr2(µ-OH)2(nta)2]2− anion, two K+ cations, and six hydrated waters. Each CrIII ion displays a distorted octahedral environment, formed by two bridging hydroxo O7 atoms and one N and three O atoms of the nta ligand. It is also found that with decreasing ionic radius of the cations the water content increases from four for Cs+ to six for K+ (Golic & Bulc, 1988).