supplementary materials


im2064 scheme

Acta Cryst. (2008). E64, m828    [ doi:10.1107/S1600536808014748 ]

Chlorido(pyridine-2-carbaldehyde oximato-[kappa]2N,N')(pyridine-2-carbaldehyde oxime-[kappa]2N,N')copper(II)

G. Wu and D. Wu

Abstract top

In the title compound, [Cu(C6H5N2O)Cl(C6H6N2O)], the Cu atom is coordinated by one neutral and one deprotonated pyridine-2-carboxaldehyde oxime (pco) ligand, resulting in the formation of two five-membered CuN2C2 rings. Together with the additional coordinating chloride anion, the coordination polyhedron of copper is best described as a distorted square-pyramid, the distortion parameter being 0.288. The two organic ligands are linked by an intramolecular O-H...O hydrogen bond.

Comment top

Pyridine-2-carbaldehyde oxime ligands usually bind to metals in a bidentate fashion, either chelating one metal center or bridging two metals. Their complexes find application in diverse areas such as functional supramolecular design, magnetic materials and catalysis (Korpi et al., 2005; Pearse et al., 1989; Afrati et al., 2005; Stamatatos et al., 2006). The title compound is a new copper complex from the reaction of CuCl2 with pyridine-2-carbaldehyde oxime (pco). The compound consists of two N,N-chelating ligands and one chloride anion. The two pco ligands are coordinated to copper to form two five-membered CuC2N2 rings. The copper atom adopts a distorted 4 + 1 square-pyramidal coordination mode with the distortion parameter being 0.288 (Addison et al., 1984) and the angles around copper ion ranging from 79.07 (1)° for N3—Cu1—N4 to 168.37 (1)° for N2—Cu1—N3. From the viewpoint of charge balance, it is presumed there exists one deprotonated and one protonated oxime ligand with a strong intramolecular hydrogen bond between the OH group and the negatively charged oxygen of the other ligand (O1···O2 = 2.488 Å) which would also give an explanation for the rather unusal cis-arrangement of the ligands (Scheme 1, Figure 1. ).

Related literature top

For related literature, see: Addison et al. (1984); Afrati et al. (2005); Korpi et al. (2005); Pearse et al. (1989); Stamatatos et al. (2006).

Experimental top

A methanolic solution (15 ml) containing pco (0.1 mmol, 0.012 g) was added to an methanolic solution (10 ml) containing CuCl2 × 2 H2O (0.1 mmol, 0.017 g). After stirring for 2 h, the solution was filtered. Dark green needle-like crystals suitable for single-crystal X-ray diffraction were obtained by evaporating the resulting filtrate in air for several days (yield 65.6% based on the ligand).

Refinement top

H atoms were placed geometrically and allowed to ride during refinement with C—H = 0.93–0.96 Å and O—H = 0.82 Å with Uiso(H) = 1.2 or 1.5Ueq(C or O).

Computing details top

Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT (Bruker, 1997); 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 molecular structure of the title compound with the atom-numbering scheme. Displacement ellipsoids were drawn at the 50% probability level.
Chlorido(pyridine-2-carbaldehyde oximato-κ2N,N')(pyridine-2- carbaldehyde oxime-κ2N,N')copper(II) top
Crystal data top
[Cu(C6H5N2O)Cl(C6H6N2O)]F000 = 1384
Mr = 342.24Dx = 1.730 Mg m3
Monoclinic, C2/cMo Kα radiation
λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 2343 reflections
a = 16.686 (2) Åθ = 2.4–26.6º
b = 12.064 (2) ŵ = 1.87 mm1
c = 13.805 (1) ÅT = 293 (2) K
β = 109.02 (1)ºBlock, dark green
V = 2627.3 (5) Å30.22 × 0.18 × 0.15 mm
Z = 8
Data collection top
Bruker SMART CCD area-detector
diffractometer
2318 independent reflections
Radiation source: fine-focus sealed tube1788 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.034
T = 293(2) Kθmax = 25.0º
φ and ω scansθmin = 2.1º
Absorption correction: multi-scan
(SHELXTL; Sheldrick, 2008)
h = 14→19
Tmin = 0.488, Tmax = 0.594k = 14→13
6487 measured reflectionsl = 16→16
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)] = 0.029H-atom parameters constrained
wR(F2) = 0.110  w = 1/[σ2(Fo2) + (0.065P)2 + 1.2P]
where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max = 0.001
2318 reflectionsΔρmax = 0.40 e Å3
181 parametersΔρmin = 0.39 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
[Cu(C6H5N2O)Cl(C6H6N2O)]V = 2627.3 (5) Å3
Mr = 342.24Z = 8
Monoclinic, C2/cMo Kα
a = 16.686 (2) ŵ = 1.87 mm1
b = 12.064 (2) ÅT = 293 (2) K
c = 13.805 (1) Å0.22 × 0.18 × 0.15 mm
β = 109.02 (1)º
Data collection top
Bruker SMART CCD area-detector
diffractometer
2318 independent reflections
Absorption correction: multi-scan
(SHELXTL; Sheldrick, 2008)
1788 reflections with I > 2σ(I)
Tmin = 0.488, Tmax = 0.594Rint = 0.034
6487 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.029181 parameters
wR(F2) = 0.110H-atom parameters constrained
S = 1.01Δρmax = 0.40 e Å3
2318 reflectionsΔρmin = 0.39 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 > 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
Cu10.45583 (2)0.75857 (3)0.08754 (3)0.03490 (18)
Cl10.39133 (6)0.74459 (6)0.09737 (7)0.0452 (3)
N20.39301 (17)0.8985 (2)0.1014 (2)0.0365 (6)
N30.53622 (18)0.6345 (2)0.0978 (2)0.0432 (7)
N40.39418 (17)0.6311 (2)0.1352 (2)0.0386 (7)
O20.60997 (16)0.6484 (2)0.0801 (2)0.0594 (7)
C10.3107 (2)0.9115 (3)0.0892 (3)0.0445 (9)
H1A0.27610.84910.07640.053*
N10.54953 (17)0.8713 (2)0.1156 (2)0.0431 (7)
C110.4316 (2)0.5328 (3)0.1314 (3)0.0427 (9)
C50.4419 (2)0.9892 (3)0.1166 (3)0.0433 (8)
O10.63020 (15)0.8491 (3)0.1224 (2)0.0666 (8)
H1B0.63460.78340.11000.100*
C20.2750 (3)1.0126 (4)0.0946 (3)0.0585 (11)
H2A0.21771.01870.08660.070*
C90.3236 (3)0.4362 (4)0.1762 (3)0.0647 (12)
H9A0.30020.37070.19030.078*
C70.3232 (2)0.6295 (3)0.1599 (3)0.0457 (9)
H7A0.29730.69680.16380.055*
C120.5115 (2)0.5390 (3)0.1109 (3)0.0463 (9)
H12A0.54260.47600.10760.056*
C60.5299 (2)0.9703 (3)0.1257 (3)0.0483 (9)
H6A0.56921.02760.13810.058*
C100.3975 (3)0.4349 (3)0.1509 (3)0.0579 (11)
H10A0.42390.36800.14710.069*
C80.2865 (3)0.5352 (4)0.1798 (3)0.0593 (11)
H8A0.23650.53880.19570.071*
C40.4094 (3)1.0927 (3)0.1215 (3)0.0636 (12)
H4A0.44401.15500.13130.076*
C30.3253 (3)1.1034 (3)0.1118 (4)0.0718 (13)
H3A0.30291.17290.11710.086*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cu10.0277 (3)0.0340 (3)0.0441 (3)0.00547 (15)0.0132 (2)0.00158 (17)
Cl10.0482 (6)0.0432 (5)0.0407 (5)0.0035 (4)0.0094 (4)0.0023 (4)
N20.0355 (16)0.0317 (15)0.0418 (16)0.0041 (12)0.0118 (13)0.0026 (12)
N30.0398 (17)0.0480 (19)0.0432 (17)0.0156 (14)0.0152 (14)0.0003 (14)
N40.0385 (16)0.0366 (16)0.0392 (16)0.0031 (12)0.0107 (13)0.0023 (12)
O20.0440 (16)0.0712 (19)0.0731 (19)0.0207 (14)0.0327 (14)0.0047 (15)
C10.040 (2)0.044 (2)0.049 (2)0.0096 (16)0.0142 (17)0.0009 (16)
N10.0286 (16)0.0516 (19)0.0505 (18)0.0040 (13)0.0147 (14)0.0005 (14)
C110.052 (2)0.0372 (19)0.032 (2)0.0057 (16)0.0044 (17)0.0001 (15)
C50.052 (2)0.038 (2)0.040 (2)0.0022 (16)0.0157 (18)0.0024 (16)
O10.0326 (15)0.077 (2)0.092 (2)0.0025 (13)0.0241 (15)0.0042 (17)
C20.051 (2)0.066 (3)0.059 (3)0.029 (2)0.019 (2)0.002 (2)
C90.069 (3)0.058 (3)0.058 (3)0.024 (2)0.009 (2)0.009 (2)
C70.041 (2)0.051 (2)0.047 (2)0.0006 (17)0.0166 (17)0.0022 (17)
C120.052 (2)0.044 (2)0.040 (2)0.0195 (18)0.0113 (18)0.0006 (17)
C60.045 (2)0.045 (2)0.056 (2)0.0115 (17)0.0177 (18)0.0050 (18)
C100.071 (3)0.036 (2)0.053 (2)0.0020 (19)0.002 (2)0.0001 (18)
C80.052 (3)0.067 (3)0.057 (3)0.014 (2)0.016 (2)0.006 (2)
C40.080 (3)0.031 (2)0.079 (3)0.0027 (19)0.025 (3)0.0044 (19)
C30.088 (4)0.044 (3)0.084 (3)0.033 (2)0.029 (3)0.004 (2)
Geometric parameters (Å, °) top
Cu1—N31.984 (3)C5—C41.371 (5)
Cu1—N12.012 (3)C5—C61.451 (5)
Cu1—N22.029 (3)O1—H1B0.8200
Cu1—N42.072 (3)C2—C31.352 (6)
Cu1—Cl12.4316 (10)C2—H2A0.9300
N2—C11.338 (4)C9—C81.354 (6)
N2—C51.340 (4)C9—C101.385 (6)
N3—C121.256 (5)C9—H9A0.9300
N3—O21.341 (3)C7—C81.361 (5)
N4—C71.335 (4)C7—H7A0.9300
N4—C111.350 (4)C12—H12A0.9300
C1—C21.370 (5)C6—H6A0.9300
C1—H1A0.9300C10—H10A0.9300
N1—C61.258 (4)C8—H8A0.9300
N1—O11.345 (3)C4—C31.371 (6)
C11—C101.375 (5)C4—H4A0.9300
C11—C121.453 (5)C3—H3A0.9300
N3—Cu1—N191.79 (14)C4—C5—C6123.0 (4)
N3—Cu1—N2168.29 (12)N1—O1—H1B109.5
N1—Cu1—N279.19 (11)C3—C2—C1118.4 (4)
N3—Cu1—N479.15 (12)C3—C2—H2A120.8
N1—Cu1—N4151.07 (12)C1—C2—H2A120.8
N2—Cu1—N4105.21 (11)C8—C9—C10118.3 (4)
N3—Cu1—Cl194.60 (9)C8—C9—H9A120.9
N1—Cu1—Cl1107.40 (9)C10—C9—H9A120.9
N2—Cu1—Cl195.22 (8)N4—C7—C8124.0 (4)
N4—Cu1—Cl1100.71 (8)N4—C7—H7A118.0
C1—N2—C5118.1 (3)C8—C7—H7A118.0
C1—N2—Cu1128.8 (2)N3—C12—C11116.1 (3)
C5—N2—Cu1112.8 (2)N3—C12—H12A121.9
C12—N3—O2120.3 (3)C11—C12—H12A121.9
C12—N3—Cu1117.1 (2)N1—C6—C5115.7 (3)
O2—N3—Cu1122.1 (2)N1—C6—H6A122.2
C7—N4—C11117.2 (3)C5—C6—H6A122.2
C7—N4—Cu1131.7 (2)C11—C10—C9119.9 (4)
C11—N4—Cu1110.9 (2)C11—C10—H10A120.0
N2—C1—C2122.9 (4)C9—C10—H10A120.0
N2—C1—H1A118.5C9—C8—C7119.2 (4)
C2—C1—H1A118.5C9—C8—H8A120.4
C6—N1—O1118.2 (3)C7—C8—H8A120.4
C6—N1—Cu1116.6 (2)C5—C4—C3119.3 (4)
O1—N1—Cu1125.2 (2)C5—C4—H4A120.4
N4—C11—C10121.4 (4)C3—C4—H4A120.4
N4—C11—C12115.3 (3)C2—C3—C4119.8 (4)
C10—C11—C12123.2 (3)C2—C3—H3A120.1
N2—C5—C4121.4 (4)C4—C3—H3A120.1
N2—C5—C6115.6 (3)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O1—H1B···O20.821.702.488 (5)162
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O1—H1B···O20.821.702.488 (5)162
Acknowledgements top

DW thanks Anqing Teachers College for financial support.

references
References top

Addison, A. W., Rao, T. N., Reedijk, J., van Rijn, J. & Verschoor, G. C. (1984). J. Chem. Soc. Dalton Trans. pp. 1349–1356.

Afrati, T., Dendrinou-Samara, C., Zaleski, C. M., Kampf, J. W., Pecoraro, V. L. & Kessissoglou, D. P. (2005). Inorg. Chem. Commun. 8, 1173–1176.

Bruker (1997). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.

Korpi, H., Polamo, M., Leskela, M. & Repo, T. (2005). Inorg. Chem. Commun. 8, 1181–1184.

Pearse, G. A., Raithby, P. R. & Lewis, J. (1989). Polyhedron, 8, 301–304.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Stamatatos, T. C., Vlahopoulou, J. C., Sanakis, Y., Raptopoulou, C. P., Psycharis, V., Boudalis, A. K. & Perlepes, S. P. (2006). Inorg. Chem. Commun. 9, 814–818.