supplementary materials


Acta Cryst. (2007). E63, m2422    [ doi:10.1107/S1600536807039323 ]

Redetermination of bis(acetylacetonato)oxidopyridinevanadium(IV)

R. M. S. da Silva, C. C. Spiazzi, R. Bortolotto and R. A. Burrow

Abstract top

The crystal structure of the title compound, [VO(C5H7O2)2(C5H5N)], has been reported previously [Meicheng, Lifeng & Youqi (1984). Kexue Tongbao, 29, 759-764], with an R value of 0.13. The current redetermination shows a significant improvement in the precision of the geometric parameters. The V atom binds five O atoms and one N atom from the pyridine ligand in a distorted octahedral configuration; the acetylacetonate anions act as bidentate ligands. A crystallographic twofold axis passes through the V, vanadyl O, and pyridine N and para-C atoms.

Comment top

The crystal structure of the title compound, VO(C5H7O)2C5H5N, was determined previously by (Meicheng et al., 1984). The original structure refinement converged with R1 = 0.13 [CUCWUS; Cambridge Structural Database (CSD, Version 5.28, update of January 2007; Allen, 2002)]. The current redetermination shows a significant improvement in the precision of the geometric parameters. A low temperature experiment was attempted, but the crystal quickly powders under a cold nitrogen stream. One half-molecule is found in the asymmetric unit; the complete molecule is generated by a crystallographic 2 fold axis which passes through atoms O1, V1, N1 and C8. The geometry of the hexacoordinate V atom can be regarded as distorted octahedral with the two acetylacetonato ligands chelating in the equatorial plane, and the vandyl O and the pyridinal N atoms in axial positions (Fig. 1). The V1 atom is centered 0.3160 (10) Å out of the plane formed by four coordinated oxygen atoms, in the direction of the apical O1 atom. The V=O distance is 1.5976 (18) Å in good agreement with ranges observed for other VO5N octahedral found in the Cambridge Structural Database (CSD, Version 5.28, update of January 2007; Allen, 2002)] (V=O 1.598 (11) Å for 21 observations), the cisoid angles (O–V–O and O–V–N) being 80.08 (4) – 99.92 (4)°, and transoid angles (O–V–O and O–V–N) being 160.16 (8) – 180° (Table 1). The molecules packs around a crystallographic twofold screw axis, parallel to the crystallographic b-axis (Fig. 2).

The thermal gravimetric analysis (TGA) of 1 shows a loss of one molecule of pyridine (exp. 22.03%, calc. 22.97%) at 334.98 K, followed by the loss of C10H16O5(exp. 64.41%, calc. 62.23%)at 438.45 K. The residual weight for the whole process (exp. 13.56%, calc. 14.80%) is in good agreement assuming V as the final end product.

Related literature top

For a related structure, see: Meicheng et al. (1984).

For related literature, see: Allen (2002).

Experimental top

The title compound was synthesized by refluxing VO(acac)2 (1.00 g, 3.68 mmol) dissolved pyridine (15 ml) for 2 h. After cooling to room temperature, 80 ml of diethyl ether was added. Light green single crystals of the compound were obtained by slow evaporation of the solution at room temperature over several days in a dessecator. Yield (crystals): 0.13 g (10.15%).

Refinement top

All H atoms on were refined using a riding model, with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C) for the methine C atoms and C—H = 0.96 Å and Uiso = 1.5Ueq(C) for the methyl C atoms.

Computing details top

Data collection: APEX2, COSMO and BIS (Bruker, 2006); cell refinement: SAINT (Bruker, 2006); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: DIAMOND (Brandenburg, 2007); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. The molecular structure with 30% probability ellipsoids. [Symmetry code: (i) 1 − x, y, 1.5 − z.]
[Figure 2] Fig. 2. Part of the crytal structure viewed perpendicular to the bc plane. The phenyl groups are represented as solid grey lines. Hydrogen atoms omitted for sake of clarity.
bis(acetylacetonato)oxidopyridinevanadium(IV) top
Crystal data top
[V(C5H7O2)2O(C5H5N)]F000 = 716
Mr = 344.25Dx = 1.344 Mg m3
Monoclinic, C2/cMo Kα radiation
λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 2628 reflections
a = 7.9121 (3) Åθ = 2.9–24.1º
b = 15.5258 (7) ŵ = 0.60 mm1
c = 14.2523 (6) ÅT = 296 (2) K
β = 103.621 (3)ºTrapezoid, blue–green
V = 1701.54 (12) Å30.35 × 0.35 × 0.25 mm
Z = 4
Data collection top
Bruker APEX II area-detector
diffractometer
1837 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.032
T = 296(2) Kθmax = 30.4º
φ and ω scansθmin = 2.9º
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
h = 11→11
Tmin = 0.903, Tmax = 1k = 22→20
11650 measured reflectionsl = 20→20
2595 independent reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039H-atom parameters constrained
wR(F2) = 0.116  w = 1/[σ2(Fo2) + (0.0608P)2 + 0.0762P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
2595 reflectionsΔρmax = 0.23 e Å3
104 parametersΔρmin = 0.31 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
[V(C5H7O2)2O(C5H5N)]V = 1701.54 (12) Å3
Mr = 344.25Z = 4
Monoclinic, C2/cMo Kα
a = 7.9121 (3) ŵ = 0.60 mm1
b = 15.5258 (7) ÅT = 296 (2) K
c = 14.2523 (6) Å0.35 × 0.35 × 0.25 mm
β = 103.621 (3)º
Data collection top
Bruker APEX II area-detector
diffractometer
2595 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2006)
1837 reflections with I > 2σ(I)
Tmin = 0.903, Tmax = 1Rint = 0.032
11650 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.039104 parameters
wR(F2) = 0.116H-atom parameters constrained
S = 1.05Δρmax = 0.23 e Å3
2595 reflectionsΔρmin = 0.31 e Å3
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 > 2sigma(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
C10.8337 (2)0.61290 (12)0.88998 (13)0.0543 (4)
C20.7518 (2)0.62217 (15)0.96641 (14)0.0663 (5)
H20.82260.63221.02750.08*
C30.5742 (2)0.61768 (12)0.95867 (12)0.0525 (4)
C41.0287 (2)0.61760 (18)0.91047 (17)0.0838 (7)
H4A1.07530.56070.90860.126*
H4B1.07310.64210.97330.126*
H4C1.06230.65290.86270.126*
C50.5044 (3)0.62994 (17)1.04695 (13)0.0761 (6)
H5A0.41640.67381.03480.114*
H5B0.59720.6471.10010.114*
H5C0.45510.57681.06240.114*
C60.6215 (2)0.78243 (13)0.71999 (13)0.0592 (5)
H60.7070.75250.69850.071*
C70.6260 (3)0.87100 (15)0.71941 (14)0.0755 (6)
H70.71330.90.69850.091*
C80.50.91579 (19)0.750.0835 (10)
H80.50.97570.750.1*
N10.50.73721 (13)0.750.0495 (4)
O10.50.47833 (11)0.750.0607 (4)
O20.46038 (14)0.60333 (8)0.88081 (8)0.0530 (3)
O30.75487 (14)0.59983 (9)0.80249 (9)0.0544 (3)
V10.50.58123 (3)0.750.04534 (15)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0421 (8)0.0563 (10)0.0592 (11)0.0013 (7)0.0014 (7)0.0033 (8)
C20.0509 (10)0.0910 (15)0.0500 (10)0.0003 (10)0.0018 (8)0.0085 (10)
C30.0576 (9)0.0538 (10)0.0444 (9)0.0013 (8)0.0087 (7)0.0035 (7)
C40.0411 (9)0.115 (2)0.0879 (16)0.0009 (11)0.0001 (9)0.0218 (14)
C50.0798 (14)0.1023 (18)0.0470 (10)0.0041 (13)0.0163 (9)0.0046 (10)
C60.0488 (9)0.0674 (12)0.0609 (11)0.0088 (8)0.0119 (8)0.0019 (9)
C70.0876 (15)0.0694 (15)0.0654 (13)0.0281 (12)0.0101 (10)0.0034 (10)
C80.126 (3)0.0495 (17)0.0649 (19)00.0016 (19)0
N10.0413 (9)0.0547 (12)0.0520 (11)00.0101 (8)0
O10.0631 (10)0.0560 (11)0.0623 (11)00.0133 (8)0
O20.0448 (6)0.0710 (8)0.0430 (6)0.0021 (5)0.0095 (5)0.0021 (5)
O30.0360 (6)0.0735 (8)0.0519 (7)0.0035 (5)0.0069 (5)0.0015 (5)
V10.0375 (2)0.0560 (3)0.0412 (2)00.00648 (15)0
Geometric parameters (Å, °) top
C1—O31.272 (2)C6—C71.376 (3)
C1—C21.400 (2)C6—H60.93
C1—C41.503 (2)C7—C81.368 (3)
C2—C31.386 (2)C7—H70.93
C2—H20.93C8—C7i1.368 (3)
C3—O21.273 (2)C8—H80.93
C3—C51.500 (2)N1—C6i1.339 (2)
C4—H4A0.96N1—V12.422 (2)
C4—H4B0.96O1—V11.5976 (18)
C4—H4C0.96O2—V11.9918 (11)
C5—H5A0.96O3—V11.9997 (11)
C5—H5B0.96V1—O2i1.9918 (11)
C5—H5C0.96V1—O3i1.9997 (11)
C6—N11.339 (2)
O3—C1—C2124.71 (15)C8—C7—H7120.5
O3—C1—C4116.22 (16)C6—C7—H7120.5
C2—C1—C4119.06 (17)C7i—C8—C7118.9 (3)
C3—C2—C1125.41 (17)C7i—C8—H8120.6
C3—C2—H2117.3C7—C8—H8120.6
C1—C2—H2117.3C6—N1—C6i116.8 (2)
O2—C3—C2125.04 (16)C6—N1—V1121.61 (11)
O2—C3—C5115.39 (15)C6i—N1—V1121.61 (11)
C2—C3—C5119.57 (16)C3—O2—V1127.66 (11)
C1—C4—H4A109.5C1—O3—V1127.44 (11)
C1—C4—H4B109.5O1—V1—O299.92 (4)
H4A—C4—H4B109.5O1—V1—O2i99.92 (4)
C1—C4—H4C109.5O2—V1—O2i160.16 (8)
H4A—C4—H4C109.5O1—V1—O398.30 (4)
H4B—C4—H4C109.5O2—V1—O389.55 (5)
C3—C5—H5A109.5O2i—V1—O387.60 (5)
C3—C5—H5B109.5O1—V1—O3i98.30 (4)
H5A—C5—H5B109.5O2—V1—O3i87.60 (5)
C3—C5—H5C109.5O2i—V1—O3i89.55 (5)
H5A—C5—H5C109.5O3—V1—O3i163.39 (8)
H5B—C5—H5C109.5O1—V1—N1180
N1—C6—C7123.16 (19)O2—V1—N180.08 (4)
N1—C6—H6118.4O2i—V1—N180.08 (4)
C7—C6—H6118.4O3—V1—N181.70 (4)
C8—C7—C6119.0 (2)O3i—V1—N181.70 (4)
O3—C1—C2—C30.7 (4)C3—O2—V1—O3i166.86 (15)
C4—C1—C2—C3178.7 (2)C3—O2—V1—N184.87 (15)
C1—C2—C3—O21.0 (4)C1—O3—V1—O195.23 (15)
C1—C2—C3—C5179.3 (2)C1—O3—V1—O24.73 (15)
N1—C6—C7—C80.6 (3)C1—O3—V1—O2i165.09 (15)
C6—C7—C8—C7i0.28 (12)C1—O3—V1—O3i84.77 (15)
C7—C6—N1—C6i0.30 (13)C1—O3—V1—N184.77 (15)
C7—C6—N1—V1179.70 (13)C6—N1—V1—O2133.93 (10)
C2—C3—O2—V11.2 (3)C6i—N1—V1—O246.07 (10)
C5—C3—O2—V1178.52 (13)C6—N1—V1—O2i46.07 (10)
C2—C1—O3—V14.3 (3)C6i—N1—V1—O2i133.93 (10)
C4—C1—O3—V1175.11 (14)C6—N1—V1—O342.93 (10)
C3—O2—V1—O195.13 (15)C6i—N1—V1—O3137.07 (10)
C3—O2—V1—O2i84.87 (15)C6—N1—V1—O3i137.07 (10)
C3—O2—V1—O33.22 (15)C6i—N1—V1—O3i42.93 (10)
Symmetry codes: (i) −x+1, y, −z+3/2.
Selected geometric parameters (Å, °) top
C1—O31.272 (2)C3—C51.500 (2)
C1—C21.400 (2)N1—V12.422 (2)
C1—C41.503 (2)O1—V11.5976 (18)
C2—C31.386 (2)O2—V11.9918 (11)
C3—O21.273 (2)O3—V11.9997 (11)
O3—C1—C2124.71 (15)C1—O3—V1127.44 (11)
O3—C1—C4116.22 (16)O1—V1—O299.92 (4)
C2—C1—C4119.06 (17)O2—V1—O2i160.16 (8)
C3—C2—C1125.41 (17)O1—V1—O398.30 (4)
O2—C3—C2125.04 (16)O2—V1—O389.55 (5)
O2—C3—C5115.39 (15)O2i—V1—O387.60 (5)
C2—C3—C5119.57 (16)O1—V1—N1180
C3—O2—V1127.66 (11)
Symmetry codes: (i) −x+1, y, −z+3/2.
Acknowledgements top

RMSS thanks CAPES for a PhD schlolarship. The diffractomer was funded by a CT–INFRA grant from the Financiadora de Estudos e Projetos (FINEP), Brazil.

references
References top

Allen, F. H. (2002). Acta Cryst. B58, 380–388.

Brandenburg, K. (2007). DIAMOND. Version 3.1e. Crystal Impact Gbr, Bonn, Germany.

Bruker (2006). APEX2 (Version 2.1), COSMO (Version 1.56), BIS (Version 2.0.1.9), SAINT (Version 7.34A) and SADABS (Version 2004/1). Bruker AXS Inc., Madison, Wisconsin, USA.

Meicheng, S., Lifeng, W. & Yougi, T. (1984). Kexue Tongbao, 29, 759–764.

Sheldrick, G. M. (1997). SHELXL97 and SHELXS97. University of Göttingen, Germany.