metal-organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890

Bis[4-chloro-2-(imino­meth­yl)phenolato]copper(II)

aDepartment of Chemistry, Jiaying University, Meizhou 514015, People's Republic of China
*Correspondence e-mail: chunbao_tang@126.com

(Received 25 February 2009; accepted 2 March 2009; online 6 March 2009)

In the title mononuclear copper(II) complex, [Cu(C7H5ClNO)2], the Cu atom, situated on an inversion center, is four-coordinated, in a slightly distorted square-planar geometry, by the N- and O-donor atoms of two symmetry-related 4-chloro-2-(imino­meth­yl)phenolate Schiff base ligands.

Related literature

For the isotypic Ni(II) complex, see: Hong (2009[Hong, Z. (2009). Acta Cryst. E65, m273.]). For bio-inorganic chemistry and the coordination chemistry of copper(II) complexes, see: Datta et al. (2008[Datta, A., Huang, J.-H. & Lee, H. M. (2008). Acta Cryst. E64, m1497.]); Diallo et al. (2008[Diallo, M., Tamboura, F. B., Gaye, M., Barry, A. H. & Bah, Y. (2008). Acta Cryst. E64, m1124-m1125.]); Khalaji et al. (2009[Khalaji, A. D., Hadadzadeh, H., Gotoh, K. & Ishida, H. (2009). Acta Cryst. E65, m70.]).

[Scheme 1]

Experimental

Crystal data
  • [Cu(C7H5ClNO)2]

  • Mr = 372.68

  • Monoclinic, P 21 /c

  • a = 15.775 (4) Å

  • b = 5.6949 (14) Å

  • c = 7.886 (2) Å

  • β = 93.932 (3)°

  • V = 706.8 (3) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 1.93 mm−1

  • T = 298 K

  • 0.18 × 0.17 × 0.17 mm

Data collection
  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996[Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.]) Tmin = 0.723, Tmax = 0.735

  • 3835 measured reflections

  • 1488 independent reflections

  • 1025 reflections with I > 2σ(I)

  • Rint = 0.038

Refinement
  • R[F2 > 2σ(F2)] = 0.047

  • wR(F2) = 0.139

  • S = 1.01

  • 1488 reflections

  • 97 parameters

  • H-atom parameters constrained

  • Δρmax = 0.48 e Å−3

  • Δρmin = −0.57 e Å−3

Data collection: SMART (Bruker, 2002[Bruker (2002). SAINT and SMART. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2002[Bruker (2002). SAINT and SMART. Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); software used to prepare material for publication: SHELXTL.

Supporting information


Comment top

Copper(II) complexes have been widely investigated in both bioinorganic chemistry and coordination chemistry (Diallo et al., 2008; Datta et al., 2008; Khalaji et al., 2009). As a further study of the structures of such complexes, the crystal structure of the title mononuclear copper(II) complex is reported here. The title complex is isostructural with the nickel(II) complex of the same ligand, 4-Chloro-2-(iminomethyl)phenolate, reported on recently by (Hong, 2009).

The molecular structure of the title complex is illustrated in Fig. 1, and geometrical parameters are given in the archived CIF. The CuII atom lies on an inversion center and is four-coordinated in a square-planar geometry by the N-and O-donor atoms of two Schiff base ligands. The whole molecule of the complex is approximately coplanar with mean deviation from the least-squares plane of 0.021 (2) Å.

Related literature top

For the isostructural nickel(II) complex of the same ligand, see: Hong (2009). For bio-inorganic chemistry and the coordination chemistry of copper(II) complexes, see: Datta et al. (2008); Diallo et al. (2008); Khalaji et al. (2009).

Experimental top

5-Chloro-2-hydroxybenzaldehyde (0.2 mmol, 31.3 mg), copper(II) acetate monohydrate (0.1 mmol, 20.0 mg) and three drops of ammonia (30%) were mixed in 10 ml of methanol. The final solution was stirred for 10 min and allowed to stand in air for two days, yielding blue needle-like crystals of the title compound.

Refinement top

The H-atoms were included in calculated positions and treated as riding: C-H = 0.93 Å, N-H = 0.86 Å, and Uiso(H) = 1.2Ueq(C,N).

Computing details top

Data collection: SMART (Bruker, 2002); cell refinement: SAINT (Bruker, 2002); data reduction: SAINT (Bruker, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The structure of the title compound, showing the atom-numbering scheme and displacement ellipsoids drawn at the 30% probability level.
(I) top
Crystal data top
[Cu(C7H5ClNO)2]F(000) = 374
Mr = 372.68Dx = 1.751 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
a = 15.775 (4) ÅCell parameters from 811 reflections
b = 5.6949 (14) Åθ = 2.5–24.3°
c = 7.886 (2) ŵ = 1.93 mm1
β = 93.932 (3)°T = 298 K
V = 706.8 (3) Å3Cut from needle, blue
Z = 20.18 × 0.17 × 0.17 mm
Data collection top
Bruker SMART CCD area-detector
diffractometer
1488 independent reflections
Radiation source: fine-focus sealed tube1025 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.038
ω scansθmax = 26.7°, θmin = 2.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1919
Tmin = 0.723, Tmax = 0.735k = 74
3835 measured reflectionsl = 99
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)] = 0.047Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.139H-atom parameters constrained
S = 1.01 w = 1/[σ2(Fo2) + (0.0757P)2 + 0.0803P]
where P = (Fo2 + 2Fc2)/3
1488 reflections(Δ/σ)max < 0.001
97 parametersΔρmax = 0.48 e Å3
0 restraintsΔρmin = 0.57 e Å3
Crystal data top
[Cu(C7H5ClNO)2]V = 706.8 (3) Å3
Mr = 372.68Z = 2
Monoclinic, P21/cMo Kα radiation
a = 15.775 (4) ŵ = 1.93 mm1
b = 5.6949 (14) ÅT = 298 K
c = 7.886 (2) Å0.18 × 0.17 × 0.17 mm
β = 93.932 (3)°
Data collection top
Bruker SMART CCD area-detector
diffractometer
1488 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
1025 reflections with I > 2σ(I)
Tmin = 0.723, Tmax = 0.735Rint = 0.038
3835 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0470 restraints
wR(F2) = 0.139H-atom parameters constrained
S = 1.01Δρmax = 0.48 e Å3
1488 reflectionsΔρmin = 0.57 e Å3
97 parameters
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 > 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) top
xyzUiso*/Ueq
Cu10.50001.00001.00000.0394 (3)
Cl10.93518 (8)0.8488 (3)0.8060 (2)0.0767 (5)
N10.5411 (2)0.7404 (6)0.8909 (4)0.0407 (8)
H10.50430.63360.86310.049*
O10.60283 (17)1.1520 (5)1.0157 (4)0.0418 (7)
C10.6875 (3)0.8577 (7)0.8857 (5)0.0361 (9)
C20.6766 (3)1.0747 (7)0.9685 (5)0.0369 (9)
C30.7494 (3)1.2131 (8)1.0047 (5)0.0446 (11)
H30.74441.35431.06240.053*
C40.8280 (3)1.1444 (8)0.9568 (6)0.0506 (12)
H40.87511.23970.98170.061*
C50.8372 (3)0.9355 (8)0.8721 (6)0.0468 (11)
C60.7682 (3)0.7904 (8)0.8369 (6)0.0460 (11)
H60.77490.64850.78110.055*
C70.6171 (3)0.6979 (7)0.8509 (5)0.0411 (10)
H70.62740.55680.79670.049*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.0443 (5)0.0320 (4)0.0413 (5)0.0014 (3)0.0013 (3)0.0036 (3)
Cl10.0436 (7)0.0892 (11)0.0988 (12)0.0013 (7)0.0152 (7)0.0162 (9)
N10.041 (2)0.0338 (19)0.047 (2)0.0048 (15)0.0007 (16)0.0067 (15)
O10.0398 (17)0.0346 (17)0.0509 (18)0.0019 (12)0.0033 (13)0.0081 (13)
C10.041 (2)0.031 (2)0.036 (2)0.0007 (17)0.0005 (17)0.0020 (17)
C20.046 (3)0.031 (2)0.033 (2)0.0010 (18)0.0024 (18)0.0008 (16)
C30.051 (3)0.034 (2)0.048 (3)0.0038 (19)0.003 (2)0.0040 (18)
C40.042 (3)0.052 (3)0.057 (3)0.008 (2)0.001 (2)0.002 (2)
C50.037 (2)0.052 (3)0.051 (3)0.003 (2)0.004 (2)0.001 (2)
C60.051 (3)0.040 (3)0.048 (3)0.006 (2)0.004 (2)0.0001 (19)
C70.050 (3)0.030 (2)0.042 (2)0.0008 (18)0.0004 (19)0.0048 (18)
Geometric parameters (Å, º) top
Cu1—O1i1.835 (3)C1—C71.447 (6)
Cu1—O11.835 (3)C2—C31.406 (6)
Cu1—N1i1.850 (3)C3—C41.378 (6)
Cu1—N11.850 (3)C3—H30.9300
Cl1—C51.736 (5)C4—C51.377 (7)
N1—C71.282 (5)C4—H40.9300
N1—H10.8600C5—C61.380 (6)
O1—C21.321 (5)C6—H60.9300
C1—C61.408 (6)C7—H70.9300
C1—C21.413 (6)
O1i—Cu1—O1180.00 (8)C4—C3—C2121.6 (4)
O1i—Cu1—N1i94.10 (14)C4—C3—H3119.2
O1—Cu1—N1i85.90 (14)C2—C3—H3119.2
O1i—Cu1—N185.90 (14)C5—C4—C3120.3 (4)
O1—Cu1—N194.10 (14)C5—C4—H4119.8
N1i—Cu1—N1180.000 (1)C3—C4—H4119.8
C7—N1—Cu1128.9 (3)C4—C5—C6120.5 (4)
C7—N1—H1115.5C4—C5—Cl1121.1 (4)
Cu1—N1—H1115.5C6—C5—Cl1118.4 (4)
C2—O1—Cu1128.0 (3)C5—C6—C1119.9 (4)
C6—C1—C2120.3 (4)C5—C6—H6120.1
C6—C1—C7118.3 (4)C1—C6—H6120.1
C2—C1—C7121.4 (4)N1—C7—C1123.5 (4)
O1—C2—C3118.6 (4)N1—C7—H7118.2
O1—C2—C1124.0 (4)C1—C7—H7118.2
C3—C2—C1117.4 (4)
Symmetry code: (i) x+1, y+2, z+2.

Experimental details

Crystal data
Chemical formula[Cu(C7H5ClNO)2]
Mr372.68
Crystal system, space groupMonoclinic, P21/c
Temperature (K)298
a, b, c (Å)15.775 (4), 5.6949 (14), 7.886 (2)
β (°) 93.932 (3)
V3)706.8 (3)
Z2
Radiation typeMo Kα
µ (mm1)1.93
Crystal size (mm)0.18 × 0.17 × 0.17
Data collection
DiffractometerBruker SMART CCD area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.723, 0.735
No. of measured, independent and
observed [I > 2σ(I)] reflections
3835, 1488, 1025
Rint0.038
(sin θ/λ)max1)0.633
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.047, 0.139, 1.01
No. of reflections1488
No. of parameters97
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.48, 0.57

Computer programs: SMART (Bruker, 2002), SAINT (Bruker, 2002), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

 

Acknowledgements

Financial support from Jiaying University Research Fund is gratefully acknowledged.

References

First citationBruker (2002). SAINT and SMART. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationDatta, A., Huang, J.-H. & Lee, H. M. (2008). Acta Cryst. E64, m1497.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationDiallo, M., Tamboura, F. B., Gaye, M., Barry, A. H. & Bah, Y. (2008). Acta Cryst. E64, m1124–m1125.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationHong, Z. (2009). Acta Cryst. E65, m273.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationKhalaji, A. D., Hadadzadeh, H., Gotoh, K. & Ishida, H. (2009). Acta Cryst. E65, m70.  Web of Science CSD CrossRef IUCr Journals Google Scholar
First citationSheldrick, G. M. (1996). SADABS. University of Göttingen, Germany.  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar

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ISSN: 2056-9890
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