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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 22;67(Pt 5):m626–m627. doi: 10.1107/S1600536811014280

Aqua­chloridobis(diphenyl­glyoximato-κ2 N,N′)cobalt(III) dihydrate

Parthasarathy Meera a, Madhavan Amutha Selvi a, Arunachalam Dayalan a,*
PMCID: PMC3089102  PMID: 21754336

Abstract

The asymmetric unit of the title complex, [Co(C14H11N2O2)2Cl(H2O)]·2H2O or [Co(dpgH)2Cl(H2O)]·2H2O, where dpgH− is diphenyl glyoximate, consists of one-half of a [Co(dpgH)2Cl(H2O)] complex and one solvent water mol­ecule. The complex is completed through inversion symmetry, with the CoIII atom situated at the centre of symmetry. The coordination geometry around the CoIII atom is distorted octa­hedral with the four N atoms of the two dpgH− ligands forming an approximate square plane with N—Co—N bite angles of 81.13 (14) and 98.87 (14)°. The Cl− ligand and the water mol­ecule are disordered in a 1:1 ratio and are in the axial positions, almost perpendicular to the plane of the glyoximate ligands [O—Co—Cl = 175.3 (10)°]. The two glyoximate ligands are linked by strong intra­molecular O—H⋯O hydrogen bonds. In addition, O—H⋯O inter­actions involving the solvent water mol­ecules and O—H⋯N hydrogen-bonding inter­actions are also observed. The solvent water mol­ecule is disordered over five positions with different occupancies.

Related literature

For related complexes, see: Gupta et al. (2003 ▶); Randaccio (1999 ▶); Brown & Satyanarayana (1992 ▶); Gilaberte et al. (1988 ▶). For the nature of equatorial ligands, see: Varhelyi et al. (1999 ▶). For similar structures, see: Meera et al. (2009 ▶). For details of the synthesis, see: Toscano et al. (1983 ▶); Gupta et al. (2001 ▶). For spectroscopic studies related to the complex, see: Gupta et al. (2004 ▶); Lopez et al. (1992 ▶); Silverstein & Bassler (1984 ▶); Mandal & Gupta (2005 ▶).graphic file with name e-67-0m626-scheme1.jpg

Experimental

Crystal data

  • [Co(C14H11N2O2)2Cl(H2O)]·2H2O

  • M r = 626.92

  • Monoclinic, Inline graphic

  • a = 12.0709 (4) Å

  • b = 5.9689 (2) Å

  • c = 21.9224 (5) Å

  • β = 104.770 (1)°

  • V = 1527.32 (8) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.70 mm−1

  • T = 293 K

  • 0.30 × 0.20 × 0.20 mm

Data collection

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 1999 ▶) T min = 0.761, T max = 0.861

  • 13610 measured reflections

  • 2682 independent reflections

  • 2431 reflections with I > 2σ(I)

  • R int = 0.030

Refinement

  • R[F 2 > 2σ(F 2)] = 0.062

  • wR(F 2) = 0.199

  • S = 1.25

  • 2682 reflections

  • 215 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.92 e Å−3

  • Δρmin = −0.53 e Å−3

Data collection: APEX2 (Bruker, 2004 ▶); cell refinement: SAINT (Bruker, 2004 ▶); data reduction: SAINT; program(s) used to solve structure: SIR92 (Altomare et al., 1993 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶) and Mercury (Macrae et al., 2008 ▶); software used to prepare material for publication: PLATON (Spek, 2009 ▶).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811014280/wm2477sup1.cif

e-67-0m626-sup1.cif (20.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014280/wm2477Isup2.hkl

e-67-0m626-Isup2.hkl (131.7KB, hkl)

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

Table 1. Selected bond lengths (Å).

Co1—N2i 1.891 (3)
Co1—N1i 1.894 (3)
Co1—O3 1.95 (3)
Co1—Cl1 2.214 (11)

Symmetry code: (i) Inline graphic.

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

D—H⋯A D—H H⋯A D⋯A D—H⋯A
O2—H2A⋯O1i 0.82 1.68 2.477 (4) 162
O2—H2A⋯N1i 0.82 2.40 2.999 (4) 130
O4A⋯O3ii     2.592 (4)  

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

The authors are thankful to Rev. Dr B. Jeyaraj, S. J., Principal, Loyola College (Autonomous), Chennai 34, India, for providing the necessary facilities, the Head, SAIF, CDRI, Lucknow, India, for supplying elemental data, and the Head, SAIF, IIT Madras, Chennai 36, India, for recording NMR spectra and for X-ray data collection.

supplementary crystallographic information

Comment

The dioxime complexes of cobalt(III), known as cobaloximes, and their derivatives have been found to mimic vitamin-B12 coenzyme. The studies on steric and electronic effects of cobaloximes helped in the successful design of novel derivatives with desired properties (Gupta et al., 2003; Randaccio, 1999; Brown & Satyanarayana, 1992; Gilaberte et al., 1988). Among the stereoisomeric benzildioximes (syn, amphi, anti), only the anti isomer shows chelation properties towards transition metal ions (Varhelyi et al., 1999).

In the structure of the title compound, [Co(C14H11N2O2)2Cl(H2O)].2H2O, or [Co(dpgH)2Cl(H2O)].2H2O, where dpgH- = diphenyl glyoximate, two halves of the complex molecule are related through inversion symmetry with CoIII situated at the centre of symmetry. The coordination geometry around CoIII is a slightly distorted octahedron (Fig. 1) with the four N atoms of the dpgH- ligand forming an approximate square plane. The bite angles N1—Co—N2 of the equatorial ligands are 81.13 (14) and 98.87 (14)°, respectively. The Cl- ligand and the water molecule are in axial positions and are disordered in a 1:1 ratio. They are almost perpendicular to the plane containing the equatorial dpgH- ligand (O3—Co1—Cl1 = 175.3 (10)°). The two glyoximate ligands are linked by strong intramolecular O—H···O hydrogen bonds. In addition, O1—H1···N2 hydrogen bonding interaction is also observed (Fig. 2). A similar interaction was observed for a related complex (Meera et al., 2009). The lattice water molecule (O4) is disordered over five positions with different occupancies. Although the H positions of the disordered water molecules could not be located, close O···O interactions suggest likewise an involvement in hydrogen bonding (Table 2).

Experimental

Cobalt(II) chloride hexahydrate was thoroughly ground and mixed with diphenylglyoxime in a 1:2 molar ratio in an aqueous solution of acetone. The reaction mixture was stirred for five hours at an elevated temperature (Toscano et al., 1983; Gupta et al., 2001). The resulting brown mass was filtered, washed with acetone, ether and dried in a desiccator. Brown coloured crystals appeared in two to three days on slow evaporation of the saturated solution of the complex in ethanol. Elemental analysis, obtained by analytical method, agreed well with the theoretical data expected for the formula of the complex, C28H28N4O7ClCo. Anal., % (calc., %): C 53.97 (53.58); H 4.94 (4.47); N 9.05 (8.93). The C═N stretching vibration of oxime in its complex was observed at 1385 cm-1 and the intramolecular hydrogen bonded –OH around 3140 cm-1. A moderate peak around 1090 cm-1 may be assigned to the C=N—O stretching of the oxime. The band around 540 cm-1 could be attributed to cobalt(III)-nitrogen stretching. The 1H NMR spectrum of the complex in acetone-d6 shows three different signals corresponding to the three different aromatic protons of the diphenylglyoximate (Gupta et al., 2004; Lopez et al., 1992). The H atoms in the second and the sixth position of the benzene ring of the diphenylglyoximate show a doublet at 7.2 p.p.m., while the third and fifth H atoms show a triplet at 7.4 p.p.m.. Similarly, the fourth one gives a triplet at 7.3 p.p.m..The oxime –OH protons resonate at 9.1 p.p.m.. A singlet around 8.5 p.p.m. represents the protons of the –OH group of the aqua ligand (Silverstein & Bassler, 1984; Mandal & Gupta, 2005).

Refinement

The O atom of the solvent water molecule in the lattice is disordered over five positions O4A, O4B, O4C, O4D, O4E with different site occupancy factor. The refinement of occupancy by means of free variable in each case is 0.302, 0.250, 0.131, 0.198 and 0.119 for O4A, O4B, O4C, O4D and O4E, respectively. The O atoms of water were refined anisotropically with equal anisotropic displacement parameters. The disordered chloride (Cl1) and oxygen (O3) atom sharing the axial position were refined with equal site occupancies of 1:1. The H atoms bound to aromatic carbon were constrained to ride on their parent atom with d(C—H) = 0.93Å and Uiso(H) =1.2Uequ(C). The position of the H atom bound to the hydroxyl group was identified from the difference in the electron density map and constrained to a distance of d(O2—H2) = 0.92 (1) Å. H positions of the positionally disordered lattice water molecules could not be found from difference maps and were eventually omitted from refinement.

Figures

Fig. 1.

Fig. 1.

ORTEP representation of the complex drawn at the 30% probability level with the atom labelling scheme. [Symmetry Code: (i) 1-x, -y, -z].

Fig. 2.

Fig. 2.

Packing of the complex in the unit cell with the disordered water occupying the intermolecular voids. The hydrogen atoms bound to aromatic carbons have been omitted for clarity.

Crystal data

[Co(C14H11N2O2)2Cl(H2O)]·2H2O F(000) = 648
Mr = 626.92 Dx = 1.363 Mg m−3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 2441 reflections
a = 12.0709 (4) Å θ = 2.8–25.0°
b = 5.9689 (2) Å µ = 0.70 mm−1
c = 21.9224 (5) Å T = 293 K
β = 104.770 (1)° Block, brown
V = 1527.32 (8) Å3 0.30 × 0.20 × 0.20 mm
Z = 2

Data collection

Bruker APEXII CCD diffractometer 2682 independent reflections
Radiation source: fine-focus sealed tube 2431 reflections with I > 2σ(I)
graphite Rint = 0.030
ω and φ scan θmax = 25.0°, θmin = 1.8°
Absorption correction: multi-scan (SADABS; Bruker, 1999) h = −14→14
Tmin = 0.761, Tmax = 0.861 k = −7→7
13610 measured reflections l = −25→26

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.062 H-atom parameters constrained
wR(F2) = 0.199 w = 1/[σ2(Fo2) + (0.1021P)2 + 2.2574P] where P = (Fo2 + 2Fc2)/3
S = 1.25 (Δ/σ)max < 0.001
2682 reflections Δρmax = 0.92 e Å−3
215 parameters Δρmin = −0.53 e Å−3
1 restraint Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods Extinction coefficient: 0.025 (3)

Special details

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)

x y z Uiso*/Ueq Occ. (<1)
C1 0.3917 (4) 0.0079 (7) 0.0955 (2) 0.0349 (9)
C2 0.5064 (3) 0.0989 (7) 0.12232 (19) 0.0342 (9)
C3 0.3003 (4) 0.0027 (8) 0.1290 (2) 0.0404 (11)
C4 0.2296 (4) −0.1819 (9) 0.1254 (2) 0.0519 (12)
H4 0.2423 −0.3092 0.1037 0.062*
C5 0.1405 (5) −0.1770 (12) 0.1539 (3) 0.0668 (16)
H5 0.0927 −0.3009 0.1508 0.080*
C6 0.1215 (5) 0.0054 (12) 0.1864 (3) 0.0677 (18)
H6 0.0610 0.0062 0.2055 0.081*
C7 0.1911 (5) 0.1880 (11) 0.1913 (3) 0.0619 (15)
H7 0.1784 0.3131 0.2139 0.074*
C8 0.2809 (4) 0.1867 (9) 0.1625 (2) 0.0482 (11)
H8 0.3284 0.3112 0.1660 0.058*
C9 0.5534 (3) 0.1512 (8) 0.19009 (18) 0.0353 (9)
C10 0.5471 (4) −0.0079 (8) 0.2349 (2) 0.0457 (11)
H10 0.5078 −0.1412 0.2227 0.055*
C11 0.5994 (5) 0.0313 (11) 0.2977 (2) 0.0576 (14)
H11 0.5969 −0.0767 0.3279 0.069*
C12 0.6550 (4) 0.2299 (11) 0.3153 (2) 0.0604 (16)
H12 0.6900 0.2559 0.3576 0.073*
C13 0.6600 (4) 0.3909 (10) 0.2718 (2) 0.0519 (13)
H13 0.6972 0.5259 0.2844 0.062*
C14 0.6092 (4) 0.3513 (8) 0.2090 (2) 0.0432 (11)
H14 0.6125 0.4599 0.1791 0.052*
N1 0.3780 (3) −0.0578 (6) 0.03761 (16) 0.0335 (8)
N2 0.5663 (3) 0.1165 (6) 0.08134 (15) 0.0325 (8)
O1 0.2790 (2) −0.1374 (6) 0.00398 (14) 0.0455 (8)
O2 0.6748 (2) 0.1866 (6) 0.09899 (14) 0.0416 (8)
H2A 0.7025 0.1849 0.0685 0.10 (3)*
Co1 0.5000 0.0000 0.0000 0.0294 (3)
Cl1 0.5813 (10) −0.3227 (16) 0.0360 (5) 0.0429 (13) 0.50
O3 0.564 (2) −0.296 (4) 0.0254 (12) 0.044 (7) 0.50
O4A 0.7645 (12) 0.624 (3) 0.0072 (7) 0.084 (3) 0.302 (9)
O4B 0.9669 (16) 0.417 (4) 0.0424 (9) 0.084 (3) 0.250 (10)
O4C 0.875 (3) 0.618 (7) 0.0176 (17) 0.084 (3) 0.131 (9)
O4D 1.023 (2) 0.437 (5) −0.0007 (13) 0.084 (3) 0.198 (9)
O4E 1.002 (3) 0.295 (9) 0.028 (2) 0.084 (3) 0.119 (10)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.033 (2) 0.038 (2) 0.034 (2) −0.0038 (17) 0.0086 (17) −0.0021 (16)
C2 0.031 (2) 0.037 (2) 0.034 (2) −0.0015 (17) 0.0082 (17) 0.0000 (17)
C3 0.033 (2) 0.054 (3) 0.033 (2) −0.0056 (19) 0.0075 (18) −0.0005 (18)
C4 0.054 (3) 0.059 (3) 0.046 (3) −0.016 (2) 0.019 (2) −0.004 (2)
C5 0.054 (3) 0.087 (4) 0.064 (3) −0.030 (3) 0.023 (3) 0.003 (3)
C6 0.045 (3) 0.109 (5) 0.057 (3) −0.008 (3) 0.027 (3) −0.003 (3)
C7 0.049 (3) 0.083 (4) 0.058 (3) 0.010 (3) 0.022 (2) −0.009 (3)
C8 0.039 (2) 0.058 (3) 0.050 (3) −0.002 (2) 0.015 (2) −0.005 (2)
C9 0.0275 (19) 0.046 (2) 0.033 (2) 0.0019 (18) 0.0090 (16) −0.0058 (18)
C10 0.041 (3) 0.057 (3) 0.041 (2) 0.002 (2) 0.013 (2) −0.001 (2)
C11 0.053 (3) 0.083 (4) 0.036 (3) 0.013 (3) 0.011 (2) 0.009 (2)
C12 0.038 (3) 0.104 (5) 0.035 (2) 0.008 (3) 0.002 (2) −0.020 (3)
C13 0.038 (2) 0.067 (3) 0.050 (3) −0.003 (2) 0.011 (2) −0.023 (3)
C14 0.035 (2) 0.053 (3) 0.043 (2) −0.005 (2) 0.0112 (18) −0.008 (2)
N1 0.0282 (17) 0.0370 (18) 0.0344 (18) −0.0050 (14) 0.0061 (14) −0.0023 (15)
N2 0.0278 (17) 0.0378 (19) 0.0312 (16) −0.0044 (14) 0.0061 (13) −0.0015 (14)
O1 0.0311 (15) 0.065 (2) 0.0411 (16) −0.0167 (15) 0.0101 (13) −0.0096 (15)
O2 0.0272 (15) 0.060 (2) 0.0369 (15) −0.0128 (14) 0.0064 (12) −0.0088 (14)
Co1 0.0256 (5) 0.0331 (5) 0.0286 (5) −0.0046 (3) 0.0054 (3) −0.0011 (3)
Cl1 0.044 (3) 0.0374 (18) 0.041 (3) 0.0015 (18) −0.001 (3) 0.004 (2)
O3 0.027 (8) 0.064 (12) 0.031 (8) −0.003 (7) −0.012 (5) 0.016 (5)
O4A 0.062 (6) 0.103 (9) 0.087 (7) 0.019 (6) 0.021 (5) 0.004 (6)
O4B 0.062 (6) 0.103 (9) 0.087 (7) 0.019 (6) 0.021 (5) 0.004 (6)
O4C 0.062 (6) 0.103 (9) 0.087 (7) 0.019 (6) 0.021 (5) 0.004 (6)
O4D 0.062 (6) 0.103 (9) 0.087 (7) 0.019 (6) 0.021 (5) 0.004 (6)
O4E 0.062 (6) 0.103 (9) 0.087 (7) 0.019 (6) 0.021 (5) 0.004 (6)

Geometric parameters (Å, °)

C1—N1 1.298 (6) C11—C12 1.368 (9)
C1—C2 1.463 (6) C11—H11 0.9300
C1—C3 1.473 (6) C12—C13 1.366 (8)
C2—N2 1.294 (5) C12—H12 0.9300
C2—C9 1.482 (6) C13—C14 1.377 (6)
C3—C8 1.375 (7) C13—H13 0.9300
C3—C4 1.383 (7) C14—H14 0.9300
C4—C5 1.375 (7) N1—O1 1.323 (4)
C4—H4 0.9300 N1—Co1 1.894 (3)
C5—C6 1.353 (9) N2—O2 1.334 (4)
C5—H5 0.9300 N2—Co1 1.891 (3)
C6—C7 1.363 (9) O2—H2A 0.8200
C6—H6 0.9300 Co1—N2i 1.891 (3)
C7—C8 1.386 (7) Co1—N1i 1.894 (3)
C7—H7 0.9300 Co1—O3 1.95 (3)
C8—H8 0.9300 Co1—O3i 1.95 (3)
C9—C14 1.382 (6) Co1—Cl1 2.214 (11)
C9—C10 1.382 (6) Co1—Cl1i 2.214 (11)
C10—C11 1.381 (7) O4D—O4Dii 0.94 (4)
C10—H10 0.9300
O4A···O3iii 2.592 (4) O4A···CL1iii 2.470 (2)
O4A···O1i 2.951 (2)
N1—C1—C2 112.1 (4) C13—C14—C9 120.5 (5)
N1—C1—C3 123.8 (4) C13—C14—H14 119.8
C2—C1—C3 124.0 (4) C9—C14—H14 119.8
N2—C2—C1 113.0 (4) C1—N1—O1 121.7 (3)
N2—C2—C9 122.6 (4) C1—N1—Co1 116.8 (3)
C1—C2—C9 124.2 (4) O1—N1—Co1 121.0 (3)
C8—C3—C4 118.7 (4) C2—N2—O2 120.4 (3)
C8—C3—C1 120.1 (4) C2—N2—Co1 116.6 (3)
C4—C3—C1 121.2 (4) O2—N2—Co1 122.5 (2)
C5—C4—C3 120.0 (5) N2—O2—H2A 109.5
C5—C4—H4 120.0 N2—Co1—N2i 179.998 (1)
C3—C4—H4 120.0 N2—Co1—N1 81.13 (14)
C6—C5—C4 120.9 (5) N2i—Co1—N1 98.87 (14)
C6—C5—H5 119.5 N2—Co1—N1i 98.87 (14)
C4—C5—H5 119.5 N2i—Co1—N1i 81.13 (14)
C5—C6—C7 120.1 (5) N1—Co1—N1i 180.00 (17)
C5—C6—H6 120.0 N2—Co1—O3 91.3 (7)
C7—C6—H6 120.0 N2i—Co1—O3 88.7 (7)
C6—C7—C8 119.8 (5) N1—Co1—O3 90.4 (9)
C6—C7—H7 120.1 N1i—Co1—O3 89.6 (9)
C8—C7—H7 120.1 N2—Co1—O3i 88.7 (7)
C3—C8—C7 120.5 (5) N2i—Co1—O3i 91.3 (7)
C3—C8—H8 119.7 N1—Co1—O3i 89.6 (9)
C7—C8—H8 119.7 N1i—Co1—O3i 90.4 (9)
C14—C9—C10 119.5 (4) O3—Co1—O3i 179.999 (2)
C14—C9—C2 121.0 (4) N2—Co1—Cl1 86.6 (3)
C10—C9—C2 119.4 (4) N2i—Co1—Cl1 93.4 (3)
C11—C10—C9 119.9 (5) N1—Co1—Cl1 90.6 (3)
C11—C10—H10 120.1 N1i—Co1—Cl1 89.4 (3)
C9—C10—H10 120.1 O3—Co1—Cl1 4.7 (10)
C12—C11—C10 119.6 (5) O3i—Co1—Cl1 175.3 (10)
C12—C11—H11 120.2 N2—Co1—Cl1i 93.4 (3)
C10—C11—H11 120.2 N2i—Co1—Cl1i 86.6 (3)
C13—C12—C11 121.3 (4) N1—Co1—Cl1i 89.4 (3)
C13—C12—H12 119.4 N1i—Co1—Cl1i 90.6 (3)
C11—C12—H12 119.4 O3—Co1—Cl1i 175.3 (10)
C12—C13—C14 119.3 (5) O3i—Co1—Cl1i 4.7 (10)
C12—C13—H13 120.3 Cl1—Co1—Cl1i 179.999 (1)
C14—C13—H13 120.3
N1—C1—C2—N2 6.6 (5) C1—C2—N2—O2 −176.8 (3)
C3—C1—C2—N2 −170.3 (4) C9—C2—N2—O2 −0.8 (6)
N1—C1—C2—C9 −169.3 (4) C1—C2—N2—Co1 −5.3 (5)
C3—C1—C2—C9 13.8 (7) C9—C2—N2—Co1 170.7 (3)
N1—C1—C3—C8 −132.9 (5) C2—N2—Co1—N2i 164 (6)
C2—C1—C3—C8 43.6 (6) O2—N2—Co1—N2i −25 (6)
N1—C1—C3—C4 44.5 (7) C2—N2—Co1—N1 2.1 (3)
C2—C1—C3—C4 −139.0 (5) O2—N2—Co1—N1 173.5 (3)
C8—C3—C4—C5 1.4 (7) C2—N2—Co1—N1i −177.9 (3)
C1—C3—C4—C5 −176.0 (5) O2—N2—Co1—N1i −6.5 (3)
C3—C4—C5—C6 −0.9 (8) C2—N2—Co1—O3 −88.1 (10)
C4—C5—C6—C7 0.0 (9) O2—N2—Co1—O3 83.2 (10)
C5—C6—C7—C8 0.4 (9) C2—N2—Co1—O3i 91.9 (10)
C4—C3—C8—C7 −1.0 (7) O2—N2—Co1—O3i −96.8 (10)
C1—C3—C8—C7 176.4 (4) C2—N2—Co1—Cl1 −89.0 (4)
C6—C7—C8—C3 0.1 (8) O2—N2—Co1—Cl1 82.4 (4)
N2—C2—C9—C14 50.7 (6) C2—N2—Co1—Cl1i 91.0 (4)
C1—C2—C9—C14 −133.8 (4) O2—N2—Co1—Cl1i −97.6 (4)
N2—C2—C9—C10 −125.5 (5) C1—N1—Co1—N2 2.0 (3)
C1—C2—C9—C10 50.0 (6) O1—N1—Co1—N2 174.3 (3)
C14—C9—C10—C11 −1.9 (7) C1—N1—Co1—N2i −178.0 (3)
C2—C9—C10—C11 174.4 (4) O1—N1—Co1—N2i −5.7 (3)
C9—C10—C11—C12 1.4 (7) C1—N1—Co1—N1i −133 (100)
C10—C11—C12—C13 −0.1 (8) O1—N1—Co1—N1i 39 (100)
C11—C12—C13—C14 −0.8 (7) C1—N1—Co1—O3 93.2 (8)
C12—C13—C14—C9 0.2 (7) O1—N1—Co1—O3 −94.5 (8)
C10—C9—C14—C13 1.1 (6) C1—N1—Co1—O3i −86.8 (8)
C2—C9—C14—C13 −175.1 (4) O1—N1—Co1—O3i 85.5 (8)
C2—C1—N1—O1 −177.4 (4) C1—N1—Co1—Cl1 88.4 (4)
C3—C1—N1—O1 −0.5 (6) O1—N1—Co1—Cl1 −99.2 (4)
C2—C1—N1—Co1 −5.1 (5) C1—N1—Co1—Cl1i −91.6 (4)
C3—C1—N1—Co1 171.8 (3) O1—N1—Co1—Cl1i 80.8 (4)

Symmetry codes: (i) −x+1, −y, −z; (ii) −x+2, −y+1, −z; (iii) x, y+1, z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O2—H2A···O1i 0.82 1.68 2.477 (4) 162.
O2—H2A···N1i 0.82 2.40 2.999 (4) 130.
O4A—···.O3iii . . 2.592 (4) .

Symmetry codes: (i) −x+1, −y, −z; (iii) x, y+1, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: WM2477).

References

  1. Altomare, A., Cascarano, G., Giacovazzo, C. & Guagliardi, A. (1993). J. Appl. Cryst. 26, 343–350.
  2. Brown, K. L. & Satyanarayana, S. (1992). J. Am. Chem. Soc. 114, 5674–5684.
  3. Bruker (1999). SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
  4. Bruker (2004). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  5. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  6. Gilaberte, J. M., Lopez, C. & Alvarez, S. (1988). J. Organomet. Chem. 342, C13–C14.
  7. Gupta, B. D., Tiwari, U., Barley, T. & Cordes, W. (2001). J. Organomet. Chem. 629, 83–92.
  8. Gupta, B. D., Vijayaikanth, V. & Sing, V. (2004). Organometallics, 23, 2067–2079.
  9. Gupta, B. D., Yamuna, R., Veena, S. & Tiwari, U. (2003). Organometallics, 22, 226–232.
  10. Lopez, C., Alavarez, S., Solans, X. & Font-Bardia, M. (1992). Polyhedron, 11, 1637.
  11. Macrae, C. F., Bruno, I. J., Chisholm, J. A., Edgington, P. R., McCabe, P., Pidcock, E., Rodriguez-Monge, L., Taylor, R., van de Streek, J. & Wood, P. A. (2008). J. Appl. Cryst. 41, 466–470.
  12. Mandal, D. & Gupta, B. D. (2005). J. Organomet. Chem. 690, 3746–3754.
  13. Meera, P., Revathi, C. & Dayalan, A. (2009). Acta Cryst. E65, m140–m141. [DOI] [PMC free article] [PubMed]
  14. Randaccio, L. (1999). Comments Inorg. Chem. 21, 327–376.
  15. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  16. Silverstein, R. M. & Bassler, G. C. (1984). Spectrometric Identification of Organic Compounds, 2nd ed., pp. 459–460. New York: John Wiley & Sons
  17. Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
  18. Toscano, P. J., Swider, S., Marzilli, L. G., Phor, N. B. & Randaccio, L. (1983). Inorg. Chem. 22, 3416–3421.
  19. Varhelyi, C. S., Zsako, J., Megyes, T. J., Majdik, K. & Liptay, G. (1999). Periodica Polytech. Ser. Chem. Eng. 43, 41–49.

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/S1600536811014280/wm2477sup1.cif

e-67-0m626-sup1.cif (20.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014280/wm2477Isup2.hkl

e-67-0m626-Isup2.hkl (131.7KB, hkl)

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


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