Abstract
The asymmetric unit of the title coordination polymer, [Cu(C18H16Cl2N2O2)]n, consists of a Schiff base complex in which the CuII atom adopts a square-pyramidal coordination geometry, being coordinated by two N and two O atoms of symmetry-related ligands and by a third O atom from a complex related by an inversion center. In the structure, a crystallographic twofold rotation axis bisects the central C—C bonds of the n-butyl spacers of the designated Schiff base ligands, making symmetry-related dimeric units, which are twisted around CuII atoms in a bis-bidentate coordination mode. In the crystal, these dimeric units are connected through the third bridging Cu—O bonds [2.3951 (13) Å], forming one-dimensional coordination polymers, which propagate along [001]. Furthermore, intermolecular π–π interactions [centroid–centroid distance = 3.811 (1) Å] stabilize the crystal packing.
Related literature
For van der Waals radii, see: Bondi (1964 ▶). For background to coordination polymers, see: Kido & Okamoto (2002 ▶); Li et al. (2006 ▶); Eddaoudi et al. (2001 ▶); Dietzel et al. (2005 ▶). For background to bis-bidentate Schiff base complexes, see: Hannon et al. (1999 ▶); Lavalette et al. (2003 ▶). For the synthesis and structural variations of Schiff base complexes, see: Granovski et al. (1993 ▶); Elmali et al. (2000 ▶).
Experimental
Crystal data
[Cu(C18H16Cl2N2O2)]
M r = 426.77
Monoclinic,
a = 23.7249 (5) Å
b = 10.5067 (2) Å
c = 15.2460 (3) Å
β = 116.988 (1)°
V = 3386.52 (12) Å3
Z = 8
Mo Kα radiation
μ = 1.62 mm−1
T = 100 K
0.42 × 0.23 × 0.17 mm
Data collection
Bruker SMART APEXII CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2001 ▶) T min = 0.547, T max = 0.768
30759 measured reflections
7465 independent reflections
5511 reflections with I > 2σ(I)
R int = 0.048
Refinement
R[F 2 > 2σ(F 2)] = 0.041
wR(F 2) = 0.108
S = 1.03
7465 reflections
226 parameters
H-atom parameters constrained
Δρmax = 1.07 e Å−3
Δρmin = −0.70 e Å−3
Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; 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 and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811009974/su2262sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811009974/su2262Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C18—H18A⋯O1 | 0.97 | 2.28 | 2.973 (2) | 127 |
Acknowledgments
HK thanks PNU for support of this work. RK thanks the Science and Research Branch, Islamic Azad University.
supplementary crystallographic information
Comment
The design and construction of metal-organic coordination polymers (MOCPs) have attracted considerable attention, not only for their novel topologies but also for their potential in the area of magnetic applications and functional materials (Kido & Okamoto, 2002; Li et al., 2006; Eddaoudi et al., 2001; Dietzel et al., 2005). One of the key strategies in the construction of metal-organic coordination polymers is to select suitable bi- or multi-dentate bridging ligands. Among these, bis-bidentate NN- or NO-donor Schiff base ligands with aliphatic and aromatic spacers (Hannon et al., 1999; Lavalette et al., 2003) have attracted much attention because of the flexibility in their coordination modes and the resulting intermolecular interactions. The long chain aliphatic spacers or rigid aromatic spacers with large bite angles in these ligands favour the bis-bidentate coordination mode and allow the ligands to accomodate metal centers in one unit of the ligand. On the other hand, Schiff bases are one of the most prevalent ligands in coordination chemistry and their complexes are some of the most important stereochemical models in transition metal-organic chemistry, with their ease of preparation and structural variations (Granovski et al., 1993; Elmali et al., 2000).
The molecular structure of the title complex (Fig. 1) consists of symmetry-related dimers in which the Schiff base ligands are twisted around CuII centers in a bis-bidentate coordination mode, having a crystallographic twofold rotation axis which passes through the central C—C bonds of the n-butyl spacers [C9—C9Ai and C18—C18Ai; symmetry code: (i) -x, y, -z + 1/2 ].
In the crystal the dimer units are connected through Cu—O bonds, forming one-diensional coordination polymer running along the c axis (Fig. 2), in which the CuII atom adopts a square-based pyramidal coordination geometry. The CuII atoms are supported by the two nitrogen and oxygen atoms of the symmetry-related ligands and a third oxygen atom of neighboring complexes. The lengths of the intermolecular Cu1—O2i bonds [2.3951 (13) Å; symetry code (i) -x, -y+1, -z] is significantly shorter than the sum of the van der Waals (vdW) radii of these atoms [Cu, 1.43Å and O, 1.52 Å; Bondi, 1964]. There are different non-bonded internuclear Cu···Cu distances. The longer one is separated by the butyl spacers [4.672 Å], and the shorter one is in the centrosymmetric Cu2O2 rectangular unit [3.299 Å]. Furthermore, intermolecular π-π interactions stabilize the crystal packings with centroid to centroid distances of 3.811 (1)Å [Cg1 and Cg2 are the centroids of the rings (C1–C6) and (C10–C15)]. There are also C—H···O interactions present (Table 1).
Experimental
The title complex was synthesized by the template method of mixing an ethanolic solution (50 ml) of 5-chlorosalicylaldeyde (4 mmol), 1,4-butanediamine (2 mmol), and CuCl2.4H2O (2.1 mmol). After stirring at reflux conditions for 2 h, the solution was filtered and the resulting green solid was crystallized from ethanol, giving single crystals suitable for X-ray diffraction. Spectoscopic and analytical data are given in the archived CIF.
Refinement
All H atoms were positioned geometrically and constrained to refine with the parents atoms using the riding-model approximation, with C—H = 0.93 - 0.97Å and Uiso(H) = 1.2 Ueq(C).
Figures
Fig. 1.
The molecular structure of the title complex, showing 40% probability displacement ellipsoids and the atomic numbering [H-atoms have been omitted for clarity; symmetry code: (A) -x, -y+1, -z].
Fig. 2.
The crystal packing, viewed down the b-axis, of the title complex, showing the one-dimensional coordination chain propagating along the c-axis [H-atoms have been omitted for clarity].
Crystal data
| [Cu(C18H16Cl2N2O2)] | F(000) = 1736 |
| Mr = 426.77 | Dx = 1.674 Mg m−3 |
| Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -C 2yc | Cell parameters from 7283 reflections |
| a = 23.7249 (5) Å | θ = 2.4–34.8° |
| b = 10.5067 (2) Å | µ = 1.62 mm−1 |
| c = 15.2460 (3) Å | T = 100 K |
| β = 116.988 (1)° | Block, green |
| V = 3386.52 (12) Å3 | 0.42 × 0.23 × 0.17 mm |
| Z = 8 |
Data collection
| Bruker SMART APEXII CCD area-detector diffractometer | 7465 independent reflections |
| Radiation source: fine-focus sealed tube | 5511 reflections with I > 2σ(I) |
| graphite | Rint = 0.048 |
| φ and ω scans | θmax = 35.2°, θmin = 2.4° |
| Absorption correction: multi-scan (SADABS; Bruker, 2001) | h = −38→38 |
| Tmin = 0.547, Tmax = 0.768 | k = −15→16 |
| 30759 measured reflections | l = −24→23 |
Refinement
| Refinement on F2 | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Secondary atom site location: difference Fourier map |
| R[F2 > 2σ(F2)] = 0.041 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.108 | H-atom parameters constrained |
| S = 1.03 | w = 1/[σ2(Fo2) + (0.0534P)2 + 2.3966P] where P = (Fo2 + 2Fc2)/3 |
| 7465 reflections | (Δ/σ)max = 0.001 |
| 226 parameters | Δρmax = 1.07 e Å−3 |
| 0 restraints | Δρmin = −0.69 e Å−3 |
Special details
| Experimental. Spectoscopic and analytical data:FTIR (KBr, cm-1): νmax 1622 (versus), 1533 (s), 1465 (s), 1386 (s), 1317 (s), 1195 (m), 1176 (m), 821 (s), 705 (s). Anal. Calc. for C18H16Cl2CuN2O2: 50.66; H, 3.78; N, 6.56 %. Found: C, 50.70; H, 3.66; N, 6.57 %. |
| 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 | ||
| Cu1 | 0.022690 (9) | 0.53850 (2) | 0.116076 (15) | 0.01452 (6) | |
| Cl1 | 0.362651 (19) | 0.48963 (5) | 0.38428 (4) | 0.02231 (9) | |
| Cl2 | −0.31688 (2) | 0.50558 (5) | −0.08067 (4) | 0.02457 (10) | |
| O1 | 0.09481 (6) | 0.63334 (13) | 0.20125 (10) | 0.0197 (2) | |
| O2 | −0.04854 (6) | 0.44838 (12) | 0.01836 (9) | 0.0169 (2) | |
| N1 | 0.06650 (7) | 0.37212 (14) | 0.17172 (10) | 0.0158 (3) | |
| N2 | −0.03106 (6) | 0.69745 (15) | 0.09189 (10) | 0.0151 (3) | |
| C1 | 0.15334 (8) | 0.59527 (17) | 0.24600 (12) | 0.0160 (3) | |
| C2 | 0.20162 (8) | 0.68856 (17) | 0.28841 (13) | 0.0177 (3) | |
| H2A | 0.1904 | 0.7735 | 0.2877 | 0.021* | |
| C3 | 0.26477 (8) | 0.65589 (18) | 0.33059 (13) | 0.0178 (3) | |
| H3A | 0.2956 | 0.7187 | 0.3563 | 0.021* | |
| C4 | 0.28228 (8) | 0.52825 (17) | 0.33464 (13) | 0.0170 (3) | |
| C5 | 0.23719 (8) | 0.43461 (18) | 0.30031 (13) | 0.0173 (3) | |
| H5A | 0.2495 | 0.3497 | 0.3064 | 0.021* | |
| C6 | 0.17232 (8) | 0.46601 (17) | 0.25576 (12) | 0.0157 (3) | |
| C7 | 0.12726 (8) | 0.36225 (17) | 0.22349 (12) | 0.0169 (3) | |
| H7A | 0.1435 | 0.2806 | 0.2417 | 0.020* | |
| C8 | 0.02982 (8) | 0.25245 (18) | 0.14935 (13) | 0.0175 (3) | |
| H8A | 0.0587 | 0.1812 | 0.1749 | 0.021* | |
| H8B | 0.0064 | 0.2424 | 0.0785 | 0.021* | |
| C9 | −0.01643 (8) | 0.25036 (18) | 0.19396 (12) | 0.0176 (3) | |
| H9A | −0.0438 | 0.3242 | 0.1709 | 0.021* | |
| H9B | −0.0428 | 0.1751 | 0.1709 | 0.021* | |
| C10 | −0.10753 (8) | 0.46309 (17) | 0.00258 (12) | 0.0150 (3) | |
| C11 | −0.14972 (8) | 0.35895 (18) | −0.03223 (13) | 0.0189 (3) | |
| H11A | −0.1347 | 0.2802 | −0.0402 | 0.023* | |
| C12 | −0.21273 (8) | 0.37172 (19) | −0.05460 (13) | 0.0197 (3) | |
| H12A | −0.2396 | 0.3018 | −0.0766 | 0.024* | |
| C13 | −0.23591 (8) | 0.48954 (19) | −0.04415 (13) | 0.0180 (3) | |
| C14 | −0.19608 (8) | 0.59274 (18) | −0.00739 (12) | 0.0170 (3) | |
| H14A | −0.2119 | 0.6704 | 0.0009 | 0.020* | |
| C15 | −0.13129 (7) | 0.58023 (17) | 0.01757 (12) | 0.0151 (3) | |
| C16 | −0.09196 (8) | 0.69309 (17) | 0.05320 (12) | 0.0155 (3) | |
| H16A | −0.1128 | 0.7699 | 0.0475 | 0.019* | |
| C17 | −0.00209 (8) | 0.82531 (17) | 0.12060 (12) | 0.0167 (3) | |
| H17A | −0.0338 | 0.8894 | 0.0852 | 0.020* | |
| H17B | 0.0315 | 0.8335 | 0.1015 | 0.020* | |
| C18 | 0.02494 (8) | 0.85016 (17) | 0.23129 (12) | 0.0161 (3) | |
| H18A | 0.0563 | 0.7854 | 0.2665 | 0.019* | |
| H18B | 0.0463 | 0.9319 | 0.2462 | 0.019* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Cu1 | 0.01204 (9) | 0.01378 (10) | 0.01660 (10) | 0.00038 (7) | 0.00551 (7) | −0.00146 (7) |
| Cl1 | 0.01324 (16) | 0.0221 (2) | 0.0287 (2) | 0.00137 (15) | 0.00701 (15) | 0.00028 (16) |
| Cl2 | 0.01322 (17) | 0.0314 (3) | 0.0279 (2) | −0.00119 (16) | 0.00826 (16) | −0.00369 (18) |
| O1 | 0.0139 (5) | 0.0149 (6) | 0.0256 (6) | 0.0014 (4) | 0.0048 (5) | −0.0040 (5) |
| O2 | 0.0132 (5) | 0.0174 (6) | 0.0205 (5) | −0.0002 (4) | 0.0079 (4) | −0.0032 (4) |
| N1 | 0.0160 (6) | 0.0149 (7) | 0.0179 (6) | 0.0002 (5) | 0.0089 (5) | −0.0007 (5) |
| N2 | 0.0155 (6) | 0.0150 (7) | 0.0148 (6) | −0.0003 (5) | 0.0068 (5) | −0.0005 (5) |
| C1 | 0.0149 (7) | 0.0162 (8) | 0.0169 (7) | 0.0012 (6) | 0.0074 (6) | −0.0015 (6) |
| C2 | 0.0167 (7) | 0.0139 (8) | 0.0205 (7) | 0.0006 (6) | 0.0066 (6) | −0.0014 (6) |
| C3 | 0.0165 (7) | 0.0171 (8) | 0.0184 (7) | −0.0019 (6) | 0.0066 (6) | −0.0016 (6) |
| C4 | 0.0133 (6) | 0.0179 (8) | 0.0180 (7) | 0.0010 (6) | 0.0055 (6) | −0.0005 (6) |
| C5 | 0.0158 (7) | 0.0158 (8) | 0.0197 (7) | 0.0014 (6) | 0.0075 (6) | 0.0011 (6) |
| C6 | 0.0161 (7) | 0.0148 (8) | 0.0168 (7) | −0.0003 (6) | 0.0079 (6) | −0.0002 (6) |
| C7 | 0.0165 (7) | 0.0159 (8) | 0.0187 (7) | 0.0018 (6) | 0.0084 (6) | −0.0001 (6) |
| C8 | 0.0173 (7) | 0.0164 (8) | 0.0213 (7) | −0.0021 (6) | 0.0108 (6) | −0.0024 (6) |
| C9 | 0.0170 (7) | 0.0177 (8) | 0.0191 (7) | −0.0019 (6) | 0.0090 (6) | −0.0008 (6) |
| C10 | 0.0144 (6) | 0.0158 (8) | 0.0150 (6) | 0.0008 (5) | 0.0067 (5) | −0.0004 (6) |
| C11 | 0.0165 (7) | 0.0176 (8) | 0.0218 (8) | −0.0010 (6) | 0.0080 (6) | −0.0034 (6) |
| C12 | 0.0176 (7) | 0.0208 (9) | 0.0205 (7) | −0.0044 (6) | 0.0085 (6) | −0.0032 (6) |
| C13 | 0.0133 (7) | 0.0234 (9) | 0.0171 (7) | −0.0011 (6) | 0.0066 (6) | −0.0007 (6) |
| C14 | 0.0142 (7) | 0.0190 (8) | 0.0172 (7) | 0.0028 (6) | 0.0065 (6) | 0.0000 (6) |
| C15 | 0.0137 (6) | 0.0161 (8) | 0.0146 (6) | −0.0004 (5) | 0.0057 (5) | −0.0007 (6) |
| C16 | 0.0147 (7) | 0.0150 (8) | 0.0154 (7) | 0.0019 (5) | 0.0057 (5) | −0.0005 (5) |
| C17 | 0.0177 (7) | 0.0142 (8) | 0.0174 (7) | −0.0012 (6) | 0.0075 (6) | 0.0008 (6) |
| C18 | 0.0143 (7) | 0.0151 (8) | 0.0178 (7) | −0.0013 (6) | 0.0063 (5) | −0.0012 (6) |
Geometric parameters (Å, °)
| Cu1—O1 | 1.8948 (13) | C7—H7A | 0.9300 |
| Cu1—O2 | 1.9201 (12) | C8—C9 | 1.531 (2) |
| Cu1—N1 | 2.0139 (15) | C8—H8A | 0.9700 |
| Cu1—N2 | 2.0308 (15) | C8—H8B | 0.9700 |
| Cu1—O2i | 2.3951 (13) | C9—C9ii | 1.523 (3) |
| Cl1—C4 | 1.7503 (17) | C9—H9A | 0.9700 |
| Cl2—C13 | 1.7488 (17) | C9—H9B | 0.9700 |
| O1—C1 | 1.301 (2) | C10—C11 | 1.414 (2) |
| O2—C10 | 1.3172 (19) | C10—C15 | 1.415 (2) |
| O2—Cu1i | 2.3951 (13) | C11—C12 | 1.381 (2) |
| N1—C7 | 1.296 (2) | C11—H11A | 0.9300 |
| N1—C8 | 1.478 (2) | C12—C13 | 1.393 (3) |
| N2—C16 | 1.290 (2) | C12—H12A | 0.9300 |
| N2—C17 | 1.482 (2) | C13—C14 | 1.379 (3) |
| C1—C6 | 1.417 (3) | C14—C15 | 1.412 (2) |
| C1—C2 | 1.421 (2) | C14—H14A | 0.9300 |
| C2—C3 | 1.379 (2) | C15—C16 | 1.453 (2) |
| C2—H2A | 0.9300 | C16—H16A | 0.9300 |
| C3—C4 | 1.397 (3) | C17—C18 | 1.531 (2) |
| C3—H3A | 0.9300 | C17—H17A | 0.9700 |
| C4—C5 | 1.370 (2) | C17—H17B | 0.9700 |
| C5—C6 | 1.411 (2) | C18—C18ii | 1.529 (3) |
| C5—H5A | 0.9300 | C18—H18A | 0.9700 |
| C6—C7 | 1.448 (2) | C18—H18B | 0.9700 |
| O1—Cu1—O2 | 173.80 (6) | C9—C8—H8A | 109.2 |
| O1—Cu1—N1 | 92.00 (6) | N1—C8—H8B | 109.2 |
| O2—Cu1—N1 | 90.18 (6) | C9—C8—H8B | 109.2 |
| O1—Cu1—N2 | 89.39 (6) | H8A—C8—H8B | 107.9 |
| O2—Cu1—N2 | 90.32 (6) | C9ii—C9—C8 | 113.17 (17) |
| N1—Cu1—N2 | 162.14 (6) | C9ii—C9—H9A | 108.9 |
| O1—Cu1—O2i | 93.09 (5) | C8—C9—H9A | 108.9 |
| O2—Cu1—O2i | 80.87 (5) | C9ii—C9—H9B | 108.9 |
| N1—Cu1—O2i | 97.28 (5) | C8—C9—H9B | 108.9 |
| N2—Cu1—O2i | 100.42 (5) | H9A—C9—H9B | 107.8 |
| C1—O1—Cu1 | 127.92 (12) | O2—C10—C11 | 119.37 (15) |
| C10—O2—Cu1 | 124.88 (11) | O2—C10—C15 | 122.73 (15) |
| C10—O2—Cu1i | 120.03 (10) | C11—C10—C15 | 117.89 (15) |
| Cu1—O2—Cu1i | 99.13 (5) | C12—C11—C10 | 121.35 (17) |
| C7—N1—C8 | 116.63 (15) | C12—C11—H11A | 119.3 |
| C7—N1—Cu1 | 123.02 (13) | C10—C11—H11A | 119.3 |
| C8—N1—Cu1 | 120.25 (11) | C11—C12—C13 | 119.84 (17) |
| C16—N2—C17 | 116.13 (15) | C11—C12—H12A | 120.1 |
| C16—N2—Cu1 | 122.32 (12) | C13—C12—H12A | 120.1 |
| C17—N2—Cu1 | 121.53 (10) | C14—C13—C12 | 120.80 (15) |
| O1—C1—C6 | 124.21 (16) | C14—C13—Cl2 | 120.31 (14) |
| O1—C1—C2 | 118.33 (16) | C12—C13—Cl2 | 118.88 (14) |
| C6—C1—C2 | 117.46 (15) | C13—C14—C15 | 119.85 (16) |
| C3—C2—C1 | 121.43 (17) | C13—C14—H14A | 120.1 |
| C3—C2—H2A | 119.3 | C15—C14—H14A | 120.1 |
| C1—C2—H2A | 119.3 | C14—C15—C10 | 120.14 (16) |
| C2—C3—C4 | 119.86 (16) | C14—C15—C16 | 117.42 (16) |
| C2—C3—H3A | 120.1 | C10—C15—C16 | 122.34 (14) |
| C4—C3—H3A | 120.1 | N2—C16—C15 | 126.57 (16) |
| C5—C4—C3 | 120.49 (16) | N2—C16—H16A | 116.7 |
| C5—C4—Cl1 | 120.47 (14) | C15—C16—H16A | 116.7 |
| C3—C4—Cl1 | 119.04 (13) | N2—C17—C18 | 112.71 (14) |
| C4—C5—C6 | 120.53 (17) | N2—C17—H17A | 109.0 |
| C4—C5—H5A | 119.7 | C18—C17—H17A | 109.0 |
| C6—C5—H5A | 119.7 | N2—C17—H17B | 109.0 |
| C5—C6—C1 | 120.00 (16) | C18—C17—H17B | 109.0 |
| C5—C6—C7 | 117.61 (16) | H17A—C17—H17B | 107.8 |
| C1—C6—C7 | 122.37 (15) | C18ii—C18—C17 | 113.78 (17) |
| N1—C7—C6 | 126.34 (17) | C18ii—C18—H18A | 108.8 |
| N1—C7—H7A | 116.8 | C17—C18—H18A | 108.8 |
| C6—C7—H7A | 116.8 | C18ii—C18—H18B | 108.8 |
| N1—C8—C9 | 112.04 (14) | C17—C18—H18B | 108.8 |
| N1—C8—H8A | 109.2 | H18A—C18—H18B | 107.7 |
| N1—Cu1—O1—C1 | 21.62 (15) | O1—C1—C6—C5 | 176.08 (16) |
| N2—Cu1—O1—C1 | −176.19 (15) | C2—C1—C6—C5 | −4.2 (2) |
| O2i—Cu1—O1—C1 | −75.79 (15) | O1—C1—C6—C7 | −5.4 (3) |
| N1—Cu1—O2—C10 | 125.77 (14) | C2—C1—C6—C7 | 174.30 (16) |
| N2—Cu1—O2—C10 | −36.38 (14) | C8—N1—C7—C6 | −178.71 (15) |
| O2i—Cu1—O2—C10 | −136.88 (16) | Cu1—N1—C7—C6 | 4.9 (2) |
| N1—Cu1—O2—Cu1i | −97.35 (5) | C5—C6—C7—N1 | −171.74 (16) |
| N2—Cu1—O2—Cu1i | 100.50 (5) | C1—C6—C7—N1 | 9.7 (3) |
| O2i—Cu1—O2—Cu1i | 0.0 | C7—N1—C8—C9 | 117.57 (17) |
| O1—Cu1—N1—C7 | −16.53 (14) | Cu1—N1—C8—C9 | −65.94 (17) |
| O2—Cu1—N1—C7 | 157.66 (14) | N1—C8—C9—C9ii | −65.42 (14) |
| N2—Cu1—N1—C7 | −110.7 (2) | Cu1—O2—C10—C11 | −149.56 (13) |
| O2i—Cu1—N1—C7 | 76.84 (14) | Cu1i—O2—C10—C11 | 81.66 (18) |
| O1—Cu1—N1—C8 | 167.21 (12) | Cu1—O2—C10—C15 | 31.4 (2) |
| O2—Cu1—N1—C8 | −18.60 (12) | Cu1i—O2—C10—C15 | −97.34 (16) |
| N2—Cu1—N1—C8 | 73.0 (2) | O2—C10—C11—C12 | −176.62 (16) |
| O2i—Cu1—N1—C8 | −99.42 (12) | C15—C10—C11—C12 | 2.4 (3) |
| O1—Cu1—N2—C16 | −164.27 (14) | C10—C11—C12—C13 | 0.8 (3) |
| O2—Cu1—N2—C16 | 21.92 (14) | C11—C12—C13—C14 | −3.0 (3) |
| N1—Cu1—N2—C16 | −69.7 (2) | C11—C12—C13—Cl2 | 175.83 (14) |
| O2i—Cu1—N2—C16 | 102.69 (13) | C12—C13—C14—C15 | 1.7 (3) |
| O1—Cu1—N2—C17 | 13.94 (12) | Cl2—C13—C14—C15 | −177.05 (13) |
| O2—Cu1—N2—C17 | −159.87 (12) | C13—C14—C15—C10 | 1.6 (2) |
| N1—Cu1—N2—C17 | 108.6 (2) | C13—C14—C15—C16 | 178.22 (16) |
| O2i—Cu1—N2—C17 | −79.09 (12) | O2—C10—C15—C14 | 175.38 (15) |
| Cu1—O1—C1—C6 | −14.3 (2) | C11—C10—C15—C14 | −3.6 (2) |
| Cu1—O1—C1—C2 | 166.02 (12) | O2—C10—C15—C16 | −1.0 (3) |
| O1—C1—C2—C3 | −175.20 (16) | C11—C10—C15—C16 | 179.95 (16) |
| C6—C1—C2—C3 | 5.1 (2) | C17—N2—C16—C15 | 178.78 (15) |
| C1—C2—C3—C4 | −1.8 (3) | Cu1—N2—C16—C15 | −2.9 (2) |
| C2—C3—C4—C5 | −2.4 (3) | C14—C15—C16—N2 | 169.93 (16) |
| C2—C3—C4—Cl1 | 177.60 (14) | C10—C15—C16—N2 | −13.6 (3) |
| C3—C4—C5—C6 | 3.3 (3) | C16—N2—C17—C18 | 101.27 (17) |
| Cl1—C4—C5—C6 | −176.79 (13) | Cu1—N2—C17—C18 | −77.05 (16) |
| C4—C5—C6—C1 | 0.2 (3) | N2—C17—C18—C18ii | −63.30 (14) |
| C4—C5—C6—C7 | −178.41 (16) |
Symmetry codes: (i) −x, −y+1, −z; (ii) −x, y, −z+1/2.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C18—H18A···O1 | 0.97 | 2.28 | 2.973 (2) | 127 |
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SU2262).
References
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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/S1600536811009974/su2262sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811009974/su2262Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


