Download citation
Download citation
link to html
In the title compound, [VOCl2(C9H21N3)], the V atom is at the center of a distorted octahedral coordination sphere and is coordinated by the three N atoms of the N,N′,N′′-tri­methyl-1,4,7-tri­aza­cyclo­nonane (Me3tacn) ligand, and by two chlorides and an oxo ligand.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S160053680201053X/ob6133sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S160053680201053X/ob6133Isup2.hkl
Contains datablock I

CCDC reference: 189870

Key indicators

  • Single-crystal X-ray study
  • T = 141 K
  • Mean [sigma](C-C) = 0.007 Å
  • R factor = 0.038
  • wR factor = 0.108
  • Data-to-parameter ratio = 14.8

checkCIF results

No syntax errors found

ADDSYM reports no extra symmetry


Amber Alert Alert Level B:
ABSTM_02 Alert B The ratio of expected to reported Tmax/Tmin(RR') is < 0.75 Tmin and Tmax reported: 0.480 0.920 Tmin' and Tmax expected: 0.832 0.894 RR' = 0.560 Please check that your absorption correction is appropriate.
Author response: The absorption corrections were applied using SADABS.
REFLT_03
         From the CIF: _diffrn_reflns_theta_max           25.44
         From the CIF: _reflns_number_total               2167
         TEST2: Reflns within _diffrn_reflns_theta_max
         Count of symmetry unique reflns         2478
         Completeness (_total/calc)             87.45%
          Alert B: < 90% complete (theta max?)
Author response: High angle data were lost due to the twinning within the crystal. Perhaps a resolution cutoff at 0.9 \%A should have been applied.
SYMMS_02  Alert B All angles should not be 90 for a monoclinic cell
Cell      13.6069    7.7759   12.6586
Angles    90.0000   90.0000   90.0000
Author response: We believe that the real \b is somewhere between 89.9 and 90.1\%. However, due to twinning, the angle is indistinguishable from 90\%.

Yellow Alert Alert Level C:
GOODF_01 Alert C The least squares goodness of fit parameter lies outside the range 0.80 <> 2.00 Goodness of fit given = 0.718
0 Alert Level A = Potentially serious problem
3 Alert Level B = Potential problem
1 Alert Level C = Please check

Computing details top

Data collection: SMART (Bruker, 1999); cell refinement: SAINT (Bruker, 1995); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997).

(I) top
Crystal data top
[VCl2O(C9H21N3)]F(000) = 644
Mr = 309.13Dx = 1.533 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 13.6069 (15) ÅCell parameters from 5166 reflections
b = 7.7759 (8) Åθ = 1.7–25.4°
c = 12.6586 (14) ŵ = 1.12 mm1
β = 90.000 (2)°T = 141 K
V = 1339.4 (3) Å3Plate, blue
Z = 40.16 × 0.12 × 0.10 mm
Data collection top
Siemens SMART CCD
diffractometer
2167 independent reflections
Radiation source: fine-focus sealed tube1929 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.046
ω scansθmax = 25.4°, θmin = 1.6°
Absorption correction: empirical (using intensity measurements)
(Blessing, 1995)
h = 1516
Tmin = 0.48, Tmax = 0.92k = 69
5156 measured reflectionsl = 1413
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)] = 0.038Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.108H-atom parameters constrained
S = 0.76 w = 1/[σ2(Fo2) + (0.XXXXP)2 + 0.XXXXP]
where P = (Fo2 + 2Fc2)/3
2167 reflections(Δ/σ)max = 0.002
146 parametersΔρmax = 0.30 e Å3
0 restraintsΔρmin = 0.53 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 on F2 for ALL reflections except for 0 with very negative F2 or flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating _R_factor_obs 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
V10.25222 (5)0.00902 (8)0.39124 (5)0.0157 (2)
Cl10.11854 (8)0.19963 (14)0.40875 (10)0.0260 (3)
Cl20.36795 (7)0.23401 (13)0.40500 (10)0.0226 (3)
O10.2600 (2)0.0728 (3)0.5101 (2)0.0226 (7)
N10.3651 (3)0.1634 (4)0.3269 (3)0.0202 (8)
N20.1595 (3)0.2037 (5)0.3376 (3)0.0248 (9)
N30.2414 (3)0.0524 (4)0.2080 (3)0.0206 (8)
C10.3226 (3)0.3362 (6)0.3040 (4)0.0269 (11)
H1A0.3687 (3)0.4265 (6)0.3283 (4)0.032*
H1B0.3137 (3)0.3495 (6)0.2268 (4)0.032*
C20.2251 (4)0.3582 (6)0.3587 (4)0.0311 (11)
H2A0.2357 (4)0.3705 (6)0.4357 (4)0.037*
H2B0.1926 (4)0.4640 (6)0.3328 (4)0.037*
C30.1306 (4)0.1977 (6)0.2241 (4)0.0303 (11)
H3A0.0611 (4)0.2334 (6)0.2168 (4)0.036*
H3B0.1716 (4)0.2791 (6)0.1833 (4)0.036*
C40.1433 (4)0.0183 (6)0.1803 (4)0.0282 (12)
H4A0.1360 (4)0.0211 (6)0.1025 (4)0.034*
H4B0.0914 (4)0.0576 (6)0.2092 (4)0.034*
C50.3221 (3)0.0412 (6)0.1517 (4)0.0242 (11)
H5A0.3476 (3)0.0312 (6)0.0935 (4)0.029*
H5B0.2959 (3)0.1487 (6)0.1207 (4)0.029*
C60.4042 (3)0.0833 (6)0.2271 (4)0.0264 (10)
H6A0.4406 (3)0.0231 (6)0.2448 (4)0.032*
H6B0.4506 (3)0.1639 (6)0.1927 (4)0.032*
C80.0703 (3)0.2201 (7)0.4053 (5)0.0361 (13)
H7A0.0899 (3)0.2240 (7)0.4798 (5)0.054*
H7B0.0351 (3)0.3260 (7)0.3870 (5)0.054*
H7C0.0271 (3)0.1209 (7)0.3936 (5)0.054*
C90.2433 (4)0.2367 (5)0.1748 (4)0.0304 (11)
H8A0.3074 (4)0.2867 (5)0.1922 (4)0.046*
H8B0.1915 (4)0.2999 (5)0.2119 (4)0.046*
H8C0.2323 (4)0.2443 (5)0.0984 (4)0.046*
C70.4481 (3)0.1820 (6)0.4022 (5)0.0299 (11)
H9A0.4761 (3)0.0685 (6)0.4174 (5)0.045*
H9B0.4987 (3)0.2559 (6)0.3711 (5)0.045*
H9C0.4242 (3)0.2338 (6)0.4680 (5)0.045*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
V10.0149 (4)0.0153 (4)0.0168 (4)0.0008 (3)0.0010 (6)0.0010 (2)
Cl10.0190 (5)0.0320 (6)0.0271 (7)0.0077 (4)0.0012 (5)0.0048 (5)
Cl20.0202 (5)0.0197 (5)0.0279 (7)0.0061 (4)0.0005 (5)0.0021 (4)
O10.028 (2)0.0153 (13)0.025 (2)0.0027 (14)0.005 (2)0.0032 (11)
N10.023 (2)0.017 (2)0.021 (2)0.004 (2)0.000 (2)0.0011 (15)
N20.026 (2)0.028 (2)0.021 (2)0.009 (2)0.004 (2)0.001 (2)
N30.022 (2)0.019 (2)0.021 (2)0.006 (2)0.004 (2)0.0027 (13)
C10.036 (3)0.014 (2)0.031 (3)0.007 (2)0.004 (2)0.002 (2)
C20.041 (3)0.020 (2)0.033 (3)0.006 (2)0.001 (2)0.000 (2)
C30.028 (3)0.041 (3)0.022 (3)0.011 (2)0.002 (2)0.008 (2)
C40.029 (3)0.036 (3)0.020 (3)0.006 (2)0.011 (2)0.004 (2)
C50.031 (3)0.022 (2)0.020 (3)0.006 (2)0.009 (2)0.002 (2)
C60.024 (2)0.025 (3)0.031 (3)0.002 (2)0.007 (2)0.006 (2)
C80.030 (3)0.050 (3)0.028 (3)0.017 (2)0.005 (3)0.007 (3)
C90.050 (3)0.019 (2)0.023 (2)0.002 (3)0.002 (3)0.003 (2)
C70.028 (2)0.027 (2)0.035 (3)0.011 (2)0.009 (3)0.006 (2)
Geometric parameters (Å, º) top
V1—O11.637 (3)C3—C41.511 (7)
V1—N22.189 (4)C3—H3A0.99
V1—N12.195 (4)C3—H3B0.99
V1—N32.349 (4)C4—H4A0.99
V1—Cl12.3569 (12)C4—H4B0.99
V1—Cl22.3603 (12)C5—C61.505 (7)
N1—C71.486 (6)C5—H5A0.99
N1—C11.491 (5)C5—H5B0.99
N1—C61.505 (6)C6—H6A0.99
N2—C31.491 (6)C6—H6B0.99
N2—C81.491 (6)C8—H7A0.98
N2—C21.520 (6)C8—H7B0.98
N3—C41.486 (6)C8—H7C0.98
N3—C91.493 (5)C9—H8A0.98
N3—C51.498 (5)C9—H8B0.98
C1—C21.507 (7)C9—H8C0.98
C1—H1A0.99C7—H9A0.98
C1—H1B0.99C7—H9B0.98
C2—H2A0.99C7—H9C0.98
C2—H2B0.99
O1—V1—N291.63 (15)H2A—C2—H2B108.1
O1—V1—N193.34 (14)N2—C3—C4110.7 (4)
N2—V1—N180.02 (13)N2—C3—H3A109.5 (2)
O1—V1—N3165.38 (13)C4—C3—H3A109.5 (3)
N2—V1—N376.49 (14)N2—C3—H3B109.5 (2)
N1—V1—N376.41 (13)C4—C3—H3B109.5 (3)
O1—V1—Cl1102.02 (11)H3A—C3—H3B108.1
N2—V1—Cl193.41 (11)N3—C4—C3111.0 (4)
N1—V1—Cl1163.50 (11)N3—C4—H4A109.4 (3)
N3—V1—Cl187.36 (9)C3—C4—H4A109.4 (3)
O1—V1—Cl2100.19 (11)N3—C4—H4B109.4 (2)
N2—V1—Cl2165.44 (11)C3—C4—H4B109.4 (3)
N1—V1—Cl290.76 (10)H4A—C4—H4B108.0
N3—V1—Cl290.47 (10)N3—C5—C6110.4 (4)
Cl1—V1—Cl292.40 (4)N3—C5—H5A109.6 (2)
C7—N1—C1109.4 (4)C6—C5—H5A109.6 (3)
C7—N1—C6108.1 (3)N3—C5—H5B109.6 (2)
C1—N1—C6110.3 (4)C6—C5—H5B109.6 (2)
C7—N1—V1110.7 (3)H5A—C5—H5B108.1
C1—N1—V1110.6 (3)C5—C6—N1111.0 (4)
C6—N1—V1107.8 (3)C5—C6—H6A109.4 (2)
C3—N2—C8110.0 (4)N1—C6—H6A109.4 (2)
C3—N2—C2110.5 (4)C5—C6—H6B109.4 (2)
C8—N2—C2108.1 (4)N1—C6—H6B109.4 (2)
C3—N2—V1115.3 (3)H6A—C6—H6B108.0
C8—N2—V1110.8 (3)N2—C8—H7A109.5 (3)
C2—N2—V1101.8 (3)N2—C8—H7B109.5 (2)
C4—N3—C9107.7 (4)H7A—C8—H7B109.5
C4—N3—C5111.5 (4)N2—C8—H7C109.5 (3)
C9—N3—C5108.6 (3)H7A—C8—H7C109.5
C4—N3—V1103.7 (3)H7B—C8—H7C109.5
C9—N3—V1114.5 (3)N3—C9—H8A109.5 (2)
C5—N3—V1110.7 (3)N3—C9—H8B109.5 (2)
N1—C1—C2110.7 (3)H8A—C9—H8B109.5
N1—C1—H1A109.5 (2)N3—C9—H8C109.5 (2)
C2—C1—H1A109.5 (2)H8A—C9—H8C109.5
N1—C1—H1B109.5 (2)H8B—C9—H8C109.5
C2—C1—H1B109.5 (3)N1—C7—H9A109.5 (2)
H1A—C1—H1B108.1N1—C7—H9B109.5 (2)
C1—C2—N2110.3 (4)H9A—C7—H9B109.5
C1—C2—H2A109.6 (3)N1—C7—H9C109.5 (3)
N2—C2—H2A109.6 (3)H9A—C7—H9C109.5
C1—C2—H2B109.6 (2)H9B—C7—H9C109.5
N2—C2—H2B109.6 (2)
 

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds