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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Jun 16;66(Pt 7):m801–m802. doi: 10.1107/S1600536810021719

(Acetyl­acetonato-κ2 O,O′)chlorido­trimethano­latoniobium(V)

Leandra Herbst a,*, Renier Koen a, Andreas Roodt a, Hendrik G Visser a
PMCID: PMC3006950  PMID: 21587722

Abstract

In the title compound, [Nb(CH3O)3(C5H7O2)Cl], the NbV atom is coordinated by two O atoms from the chelating acetyl­acetonate ligand, three O atoms from the methano­late groups and one chloride ligand. The octa­hedral environment around niobium is slightly distorted with Nb—O distances in the range 1.8603 (15)–2.1083 (15) Å and an Nb—Cl distance of 2.4693 (9) Å. The O—Nb—O angles vary between 80.74 (6) and 100.82 (7)°, while the trans Cl—Nb—O angle is 167.60 (5)°. There are no hydrogen bonds observed, only an inter­molecular C—H⋯O inter­action.

Related literature

For synthetic background, see: Davies et al. (1999). For applications of acetyl­acetone in industry, see: Steyn et al. (1992, 1997); Otto et al. (1998); Roodt & Steyn (2000); Brink et al. (2010); Viljoen et al. (2008, 2009a ,b , 2010); Steyn et al. (2008). For related niobium complexes, see: Sokolov et al. (1999, 2005); Anti­nolo et al. (2000); Dahan et al. (1976).graphic file with name e-66-0m801-scheme1.jpg

Experimental

Crystal data

  • [Nb(CH3O)3(C5H7O2)Cl]

  • M r = 320.57

  • Orthorhombic, Inline graphic

  • a = 12.296 (5) Å

  • b = 12.915 (4) Å

  • c = 15.470 (5) Å

  • V = 2456.7 (16) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 1.20 mm−1

  • T = 100 K

  • 0.36 × 0.30 × 0.19 mm

Data collection

  • Bruker X8 APEXII 4K Kappa CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2004) T min = 0.673, T max = 0.805

  • 28601 measured reflections

  • 3083 independent reflections

  • 2757 reflections with I > 2σ(I)

  • R int = 0.030

Refinement

  • R[F 2 > 2σ(F 2)] = 0.023

  • wR(F 2) = 0.068

  • S = 1.16

  • 3083 reflections

  • 141 parameters

  • H-atom parameters constrained

  • Δρmax = 1.06 e Å−3

  • Δρmin = −0.87 e Å−3

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT-Plus (Bruker, 2004); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg & Putz, 2005); software used to prepare material for publication: WinGX (Farrugia, 1999).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810021719/pv2289sup1.cif

e-66-0m801-sup1.cif (17KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810021719/pv2289Isup2.hkl

e-66-0m801-Isup2.hkl (148.3KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected geometric parameters (Å, °).

O1—Nb1 1.8640 (15)
O2—Nb1 1.8811 (16)
O3—Nb1 1.8603 (15)
O4—Nb1 2.1083 (15)
O5—Nb1 2.0842 (15)
Cl1—Nb1 2.4693 (9)
O3—Nb1—O1 100.82 (7)
O3—Nb1—O2 99.96 (7)
O1—Nb1—O2 99.45 (7)
O3—Nb1—O5 163.63 (6)
O1—Nb1—O5 91.53 (7)
O2—Nb1—O5 88.43 (7)
O3—Nb1—O4 85.71 (7)
O2—Nb1—Cl1 167.60 (5)

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C8—H8C⋯O4i 0.98 2.46 3.442 (3) 176

Symmetry code: (i) Inline graphic.

Acknowledgments

Financial assistance from the Advanced Metals Initiative (AMI) and the Department of Science and Technology (DST) of South Africa, the New Metals Development Network (NMDN), the South African Nuclear Energy Corporation Limited (Necsa) and the University of the Free State is gratefully acknowledged.

supplementary crystallographic information

Comment

Acetylacetone and its analogues find applications in homogenous catalysis and the separations industry (Steyn et al., 1992; 1997; Otto et al., 1998; Roodt & Steyn, 2000; Brink et al., 2010). This study forms part of ongoing research to investigate the intimate mechanism of the reactions of O,O'- and N,O -bidentate ligands with transition metals used in the nuclear industry, specifically hafnium, zirconium, niobium and tantalum (Viljoen et al., 2008; 2009a,b; 2010; Steyn et al., 2008).

Pale-yellow cubic crystals of the title complex crystallize from a methanol reaction solution containing niobium(V) chloride and acetylacetone after several days (Davies et al., 1999). The asymmetric unit consists of a niobium(V) atom surrounded by three methanolate groups, a chloride ligand and a O,O'- bonded acetylacetonato ligand (Figure 1). The octahedral environment around niobium is slightly distorted with Nb–O distances varying between 1.8603 (15) and 2.1083 (15) Å, while the Nb–Cl distance is 2.4693 (9) Å. The O–Nb–O angles vary between 80.74 (6) and 100.82 (7) ° while the trans Cl–Nb–O angle is 167.60 (5) °. All the bond distances and angles are similar to other relevant niobium(V) structures (Sokolov et al., 1999; 2005; Antinolo et al., 2000 and Dahan et al., 1976). The niobium compounds pack in a head-to-tail fashion along the bc plain.

There are no classical hydrogen bonds observed in this structure. However, the structure is stabilized by C8–H8C..O4* (* = -1/2+x,1/2-y,1-z) intermolecular interactions with C—H = 0.98, H···O = 2.46 and C···O = 3.442 (3) Å and C—H···O angle = 176°.

Experimental

The reaction was performed under modified Schlenk conditions under an argon atmosphere. NbCl5 (0.3134 g, 1.16 mmol) was carefully dissolved in absolute methanol (5 ml) (Care: exothermic reaction). Acetylacetone (0.119 ml, 1.16 mmol) was added to the solution. The colourless solution was stirred for 1 h at room temperature and the solution was left to stand at 252 K for a few days after which pale-yellow crystals, suitable for X-ray diffraction were obtained.

Refinement

The methyl and aromatic H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms, with C—H = 0.95 and 0.98Å and Uiso(H) = 1.5Ueq(C) and 1.2Ueq(C), respectively. The highest residual electron-density peak is 0.93 Å from Cl1.

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound. Displacement ellipsoids are drawn at the 50% probability displacement level.

Crystal data

[Nb(CH3O)3(C5H7O2)Cl] F(000) = 1296
Mr = 320.57 Dx = 1.733 Mg m3
Orthorhombic, Pbca Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ac 2ab Cell parameters from 9878 reflections
a = 12.296 (5) Å θ = 2.6–28.4°
b = 12.915 (4) Å µ = 1.20 mm1
c = 15.470 (5) Å T = 100 K
V = 2456.7 (16) Å3 Cuboid, pale-yellow
Z = 8 0.36 × 0.3 × 0.19 mm

Data collection

Bruker X8 APEXII 4K Kappa CCD diffractometer 3083 independent reflections
Radiation source: fine-focus sealed tube 2757 reflections with I > 2σ(I)
graphite Rint = 0.030
ω and φ scans θmax = 28.4°, θmin = 2.6°
Absorption correction: multi-scan (SADABS; Bruker, 2004) h = −12→16
Tmin = 0.673, Tmax = 0.805 k = −14→17
28601 measured reflections l = −18→20

Refinement

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)] = 0.023 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.068 H-atom parameters constrained
S = 1.16 w = 1/[σ2(Fo2) + (0.0273P)2 + 3.5334P] where P = (Fo2 + 2Fc2)/3
3083 reflections (Δ/σ)max = 0.001
141 parameters Δρmax = 1.06 e Å3
0 restraints Δρmin = −0.87 e Å3
0 constraints

Special details

Experimental. The intensity data were collected on a Bruker X8 ApexII 4 K Kappa CCD diffractometer using an exposure time of 60 s/frame. A total of 688 frames were collected with a frame width of 0.5° covering up to θ = 28.24° with 99.1% completeness accomplished.
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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)

x y z Uiso*/Ueq
C1 0.00363 (19) 0.09540 (17) 0.76165 (14) 0.0195 (4)
H1A −0.0385 0.1594 0.7676 0.029*
H1B 0.0228 0.0692 0.8191 0.029*
H1C −0.04 0.0435 0.7311 0.029*
C2 0.3610 (2) 0.07674 (19) 0.54112 (15) 0.0217 (5)
H2A 0.3222 0.0834 0.4861 0.033*
H2B 0.3847 0.0049 0.5488 0.033*
H2C 0.4247 0.1224 0.5409 0.033*
C3 0.26952 (19) 0.38799 (16) 0.74055 (15) 0.0195 (4)
H3A 0.2855 0.43 0.6894 0.029*
H3B 0.3309 0.3915 0.7809 0.029*
H3C 0.2039 0.4145 0.7689 0.029*
C4 0.2957 (2) 0.37805 (19) 0.41139 (16) 0.0231 (5)
H4A 0.3083 0.44 0.4466 0.035*
H4B 0.2605 0.3978 0.357 0.035*
H4C 0.3654 0.3443 0.399 0.035*
C5 0.22378 (18) 0.30466 (16) 0.45973 (14) 0.0158 (4)
C6 0.14339 (18) 0.24919 (17) 0.41581 (14) 0.0174 (4)
H6 0.1304 0.2657 0.3569 0.021*
C7 0.08152 (17) 0.17147 (16) 0.45334 (13) 0.0148 (4)
O1 0.09963 (13) 0.11572 (11) 0.71426 (9) 0.0162 (3)
O2 0.29097 (12) 0.10497 (12) 0.60982 (10) 0.0161 (3)
O3 0.25251 (13) 0.28363 (11) 0.71528 (9) 0.0158 (3)
O4 0.24286 (13) 0.29502 (11) 0.54083 (10) 0.0155 (3)
O5 0.09160 (13) 0.14211 (11) 0.53257 (9) 0.0158 (3)
Cl1 0.02912 (4) 0.32547 (4) 0.64105 (3) 0.01788 (11)
Nb1 0.178955 (15) 0.198214 (14) 0.638103 (11) 0.01144 (7)
C8 −0.00329 (19) 0.11656 (18) 0.40125 (14) 0.0200 (4)
H8A −0.0015 0.0424 0.4147 0.03*
H8B 0.0113 0.1268 0.3396 0.03*
H8C −0.0752 0.1445 0.4154 0.03*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0207 (11) 0.0218 (10) 0.0160 (10) −0.0056 (9) 0.0046 (8) −0.0002 (8)
C2 0.0221 (11) 0.0254 (11) 0.0175 (10) 0.0029 (9) 0.0043 (9) −0.0018 (8)
C3 0.0185 (11) 0.0155 (9) 0.0245 (11) −0.0016 (8) −0.0015 (9) −0.0023 (8)
C4 0.0237 (12) 0.0247 (12) 0.0209 (11) −0.0011 (9) 0.0053 (9) 0.0094 (9)
C5 0.0175 (10) 0.0160 (10) 0.0139 (10) 0.0040 (8) 0.0042 (8) 0.0037 (7)
C6 0.0192 (10) 0.0226 (10) 0.0105 (9) 0.0033 (9) 0.0009 (8) 0.0023 (8)
C7 0.0155 (10) 0.0178 (9) 0.0112 (9) 0.0054 (8) −0.0003 (8) −0.0029 (7)
O1 0.0187 (8) 0.0174 (7) 0.0125 (7) −0.0016 (6) 0.0030 (6) 0.0022 (6)
O2 0.0161 (7) 0.0180 (7) 0.0140 (7) 0.0021 (6) 0.0020 (6) 0.0010 (6)
O3 0.0194 (8) 0.0148 (7) 0.0132 (7) −0.0018 (6) −0.0011 (6) −0.0007 (5)
O4 0.0173 (7) 0.0170 (7) 0.0123 (7) −0.0024 (6) 0.0009 (6) 0.0025 (5)
O5 0.0198 (8) 0.0165 (7) 0.0112 (7) −0.0032 (6) −0.0013 (6) −0.0006 (5)
Cl1 0.0170 (2) 0.0169 (2) 0.0198 (3) 0.00236 (19) 0.00092 (19) 0.00026 (18)
Nb1 0.01376 (11) 0.01214 (10) 0.00841 (10) −0.00081 (6) 0.00045 (6) 0.00115 (6)
C8 0.0199 (11) 0.0250 (11) 0.0150 (10) 0.0007 (9) −0.0035 (8) −0.0043 (8)

Geometric parameters (Å, °)

C1—O1 1.414 (3) C5—O4 1.282 (3)
C1—H1A 0.98 C5—C6 1.397 (3)
C1—H1B 0.98 C6—C7 1.387 (3)
C1—H1C 0.98 C6—H6 0.95
C2—O2 1.416 (3) C7—O5 1.289 (3)
C2—H2A 0.98 C7—C8 1.497 (3)
C2—H2B 0.98 O1—Nb1 1.8640 (15)
C2—H2C 0.98 O2—Nb1 1.8811 (16)
C3—O3 1.419 (2) O3—Nb1 1.8603 (15)
C3—H3A 0.98 O4—Nb1 2.1083 (15)
C3—H3B 0.98 O5—Nb1 2.0842 (15)
C3—H3C 0.98 Cl1—Nb1 2.4693 (9)
C4—C5 1.497 (3) C8—H8A 0.98
C4—H4A 0.98 C8—H8B 0.98
C4—H4B 0.98 C8—H8C 0.98
C4—H4C 0.98
O1—C1—H1A 109.5 O5—C7—C6 123.9 (2)
O1—C1—H1B 109.5 O5—C7—C8 116.1 (2)
H1A—C1—H1B 109.5 C6—C7—C8 120.0 (2)
O1—C1—H1C 109.5 C1—O1—Nb1 150.52 (14)
H1A—C1—H1C 109.5 C2—O2—Nb1 141.71 (14)
H1B—C1—H1C 109.5 C3—O3—Nb1 144.27 (14)
O2—C2—H2A 109.5 C5—O4—Nb1 133.45 (14)
O2—C2—H2B 109.5 C7—O5—Nb1 133.79 (14)
H2A—C2—H2B 109.5 O3—Nb1—O1 100.82 (7)
O2—C2—H2C 109.5 O3—Nb1—O2 99.96 (7)
H2A—C2—H2C 109.5 O1—Nb1—O2 99.45 (7)
H2B—C2—H2C 109.5 O3—Nb1—O5 163.63 (6)
O3—C3—H3A 109.5 O1—Nb1—O5 91.53 (7)
O3—C3—H3B 109.5 O2—Nb1—O5 88.43 (7)
H3A—C3—H3B 109.5 O3—Nb1—O4 85.71 (7)
O3—C3—H3C 109.5 O1—Nb1—O4 170.09 (6)
H3A—C3—H3C 109.5 O2—Nb1—O4 86.60 (7)
H3B—C3—H3C 109.5 O5—Nb1—O4 80.74 (6)
C5—C4—H4A 109.5 O3—Nb1—Cl1 87.49 (6)
C5—C4—H4B 109.5 O1—Nb1—Cl1 88.76 (5)
H4A—C4—H4B 109.5 O2—Nb1—Cl1 167.60 (5)
C5—C4—H4C 109.5 O5—Nb1—Cl1 82.03 (5)
H4A—C4—H4C 109.5 O4—Nb1—Cl1 84.06 (5)
H4B—C4—H4C 109.5 C7—C8—H8A 109.5
O4—C5—C6 123.7 (2) C7—C8—H8B 109.5
O4—C5—C4 116.2 (2) H8A—C8—H8B 109.5
C6—C5—C4 120.0 (2) C7—C8—H8C 109.5
C7—C6—C5 123.8 (2) H8A—C8—H8C 109.5
C7—C6—H6 118.1 H8B—C8—H8C 109.5
C5—C6—H6 118.1
O4—C5—C6—C7 −5.6 (3) C1—O1—Nb1—Cl1 5.1 (3)
C4—C5—C6—C7 172.5 (2) C2—O2—Nb1—O3 −109.4 (2)
C5—C6—C7—O5 0.0 (3) C2—O2—Nb1—O1 147.7 (2)
C5—C6—C7—C8 179.7 (2) C2—O2—Nb1—O5 56.4 (2)
C6—C5—O4—Nb1 3.5 (3) C2—O2—Nb1—O4 −24.4 (2)
C4—C5—O4—Nb1 −174.66 (15) C2—O2—Nb1—Cl1 16.8 (4)
C6—C7—O5—Nb1 8.1 (3) C7—O5—Nb1—O3 26.9 (3)
C8—C7—O5—Nb1 −171.59 (14) C7—O5—Nb1—O1 166.10 (19)
C3—O3—Nb1—O1 −120.8 (2) C7—O5—Nb1—O2 −94.49 (19)
C3—O3—Nb1—O2 137.5 (2) C7—O5—Nb1—O4 −7.67 (19)
C3—O3—Nb1—O5 17.5 (4) C7—O5—Nb1—Cl1 77.56 (19)
C3—O3—Nb1—O4 51.7 (2) C5—O4—Nb1—O3 −169.00 (19)
C3—O3—Nb1—Cl1 −32.5 (2) C5—O4—Nb1—O2 90.7 (2)
C1—O1—Nb1—O3 92.3 (3) C5—O4—Nb1—O5 1.77 (19)
C1—O1—Nb1—O2 −165.5 (3) C5—O4—Nb1—Cl1 −81.08 (19)
C1—O1—Nb1—O5 −76.9 (3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C8—H8C···O4i 0.98 2.46 3.442 (3) 176

Symmetry codes: (i) x−1/2, −y+1/2, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PV2289).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810021719/pv2289sup1.cif

e-66-0m801-sup1.cif (17KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810021719/pv2289Isup2.hkl

e-66-0m801-Isup2.hkl (148.3KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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