Abstract
In the asymmetric unit of the title polymeric complex, {[CuI(C11H9N3)]·0.5CH3CN}n, there are two CuI atoms, two N-[(pyridin-2-yl-κN)methylidene]pyridin-3-amine (PyPy) ligands and two I atoms. Both CuI atoms have a distorted tetrahedral geometry, each being coordinated by one I atom, two N atoms of one PyPy ligand and one N atom from an adjacent PyPy ligand. In the crystal, infinite helical chains of [Cu2(PyPy)2]n are formed propagating along the b axis. These chains are linked via weak C—H⋯I hydrogen bonds and π–π stacking interactions [shortest centroid–centroid distance = 3.2727 (14) Å]. During the refinement, electron-density peaks were located that were believed to be highly disordered solvent molecules (possibly acetonitrile). The SQUEEZE option in PLATON [Spek (2009 ▶). Acta Cryst. D65, 148–155] indicated there were solvent cavities with a total volume of 196 Å3 containing approximately 60 electrons per unit cell, which equated to one molecule of acetonitrile per asymmetric unit.
Related literature
For related structures and applications of coordination polymers, see: Moulton & Zaworotko (2001 ▶); Fei et al. (2000 ▶). For the synthesis of the title ligand, see: Dehghanpour et al. (2009 ▶).
Experimental
Crystal data
[CuI(C11H9N3)]·0.5C2H3N
M r = 394.18
Monoclinic,
a = 7.1800 (2) Å
b = 13.2303 (7) Å
c = 27.9383 (13) Å
β = 90.741 (3)°
V = 2653.7 (2) Å3
Z = 8
Mo Kα radiation
μ = 3.96 mm−1
T = 150 K
0.17 × 0.12 × 0.10 mm
Data collection
Nonius KappaCCD diffractometer
Absorption correction: multi-scan (SORTAV; Blessing, 1995 ▶) T min = 0.569, T max = 0.733
19063 measured reflections
4676 independent reflections
2627 reflections with I > 2σ(I)
R int = 0.104
Refinement
R[F 2 > 2σ(F 2)] = 0.060
wR(F 2) = 0.178
S = 1.02
4676 reflections
289 parameters
H-atom parameters constrained
Δρmax = 1.39 e Å−3
Δρmin = −1.24 e Å−3
Data collection: COLLECT (Nonius, 2002 ▶); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997 ▶); data reduction: DENZO-SMN; program(s) used to solve structure: SIR92 (Altomare et al., 1994 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812037270/su2480sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812037270/su2480Isup2.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 |
|---|---|---|---|---|
| C22—H22A⋯I1i | 0.95 | 3.03 | 3.789 (12) | 138 |
| C20—H20A⋯I1ii | 0.95 | 3.14 | 4.025 (12) | 156 |
| C17—H17A⋯I2iii | 0.95 | 3.16 | 4.011 (11) | 149 |
Symmetry codes: (i)
; (ii)
; (iii)
.
Acknowledgments
The authors are grateful to the Islamic Azad University, University Research Councils for partial support of this work. The crystal structure analysis was carried out by Dr A. J. Lough of the Department of Chemistry of the University of Toronto, Canada.
supplementary crystallographic information
Comment
In recent years, coordination polymers have received much attention due to their variety of architectures and the potential applications as functional materials (Moulton & Zaworotko, 2001). Early reports have shown that nitrogen heterocyclic ligands have been employed in the synthesis of many novel structures (Fei et al., 2000). Here, we report on the synthetic and crystal structure of a novel copper iodide complex based on the ligand pyridin-3-ylpyridin-2-ylmethyleneamine (PyPy).
The asymmetric unit of the title compound, Fig. 1, contains two CuI atoms, two pyridin-3-ylpyridin-2-ylmethyleneamine (Dehghanpour et al., 2009) ligands, and two I atoms, Each Cu+ atom is four-coordinated in a distorted tetrahedral configuration by two N atoms from one PyPy ligand, one N atom from an adjacent PyPy ligand and one I atom. Each PyPy ligand chelates the Cu atom (via N, N' atoms) and also bridges to another Cu atom (with N" atom), resulting in the formation of chains propagating along the b axis.
The two ligands in the asymmetric unit are nearly planar. In ligand A the interplanar angles between chelate ring (N2/C6/C7/N3) and pyridine ring (lN3/C7-C11) is 2.11 (3)°, while for ligand B [chelate ring N5/C17/C18/N6 and pyridine ring N6/C18-C22] the same angle is 5.82 (4)°. In ligand A the two pyridine rings (N1/C1-C5 and N3/C7-C11) are inclined to one another by 12.11 (4)°. In ligand B the two pyridine rings (N6/C18-C22 and N4/C12-5C16) are inclined to one another by 7.49 (3)°. However, the interplanar angle between two ligand mean planes (A and B) is 52.82 (1)°.
In the crystal, these chains interact viaπ–π interactions between adjacent, inversion replated PyPy ligands The shortest distance of 3.2727 (14) Å [C15-C19 ring, symmetry code: (iii) = -x + 3, -y - 1, -z + 1] is observed between two inversion related ligands. These chains are further connected through C—H···I interactions (Table 1 and Fig 2.).
Experimental
The title complex was prepared by the reaction of CuI (19.1 mg, 0.1 mmol) and pyridin-3-ylpyridin-2-ylmethyleneamine (18.3 mg, 0.1 mmol) in 20 ml of acetonitrile at room temperature. Crystals of the title compound, suitable for X-ray analysis, were obtained by slow evaporation of the solvent at rt.
Refinement
H atoms were placed in calculated positions and included in the refinement in a riding-motion approximation: C—H = 0.95 Å with Uiso(H)= 1.2Ueq(C). During the refinement of the structure, electron density peaks were located that were believed to be highly disordered solvent molecules (possibly acetonitrile). Attempts to model the solvent molecule were not successful. The SQUEEZE option in PLATON (Spek, A. L. (2009). Acta Cryst. D65, 148-155) indicated there were solvent cavities with a total volume of 196 Å3 containing approximately 60 electrons per unit cell. This was equated to one molecule of acetonitrile per asymmetric unit. The density, the F(000) value, the molecular weight and the formula are given taking into account the results obtained with the SQUEEZE option in PLATON.
Figures
Fig. 1.
A view of the molecular structure of the title complex, with atom numbering. Displacement ellipsoids are drawn at the 50% probability level [Symmetry codes: (ix) 5/2 - x, -1/2 + y, 1/2 - z; (x) x, -1 + y, z; (xiii) 5/2 - x, 1/2 + y, 1/2 - z].
Fig. 2.
A view of the π–π interactions and C—H···I hydrogen bonds (dotted lines) in the crystal structure of the title compound.
Crystal data
| [CuI(C11H9N3)]·0.5C2H3N | F(000) = 1512 |
| Mr = 394.18 | Dx = 1.973 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2yn | Cell parameters from 19063 reflections |
| a = 7.1800 (2) Å | θ = 2.5–25.0° |
| b = 13.2303 (7) Å | µ = 3.96 mm−1 |
| c = 27.9383 (13) Å | T = 150 K |
| β = 90.741 (3)° | Block, brown |
| V = 2653.7 (2) Å3 | 0.17 × 0.12 × 0.10 mm |
| Z = 8 |
Data collection
| Nonius KappaCCD diffractometer | 4676 independent reflections |
| Radiation source: fine-focus sealed tube | 2627 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.104 |
| Detector resolution: 9 pixels mm-1 | θmax = 25.0°, θmin = 2.7° |
| φ scans and ω scans with κ offsets | h = −8→8 |
| Absorption correction: multi-scan (SORTAV; Blessing, 1995) | k = −15→15 |
| Tmin = 0.569, Tmax = 0.733 | l = −33→33 |
| 19063 measured reflections |
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)] = 0.060 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.178 | H-atom parameters constrained |
| S = 1.02 | w = 1/[σ2(Fo2) + (0.0943P)2] where P = (Fo2 + 2Fc2)/3 |
| 4676 reflections | (Δ/σ)max = 0.002 |
| 289 parameters | Δρmax = 1.39 e Å−3 |
| 0 restraints | Δρmin = −1.24 e Å−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 | ||
| I1 | 1.60988 (13) | −0.00459 (7) | 0.36787 (3) | 0.0589 (3) | |
| I2 | 0.61501 (9) | −0.05499 (6) | 0.10018 (2) | 0.0389 (3) | |
| Cu1 | 1.50363 (18) | −0.17127 (11) | 0.32943 (4) | 0.0400 (4) | |
| Cu2 | 0.97229 (16) | −0.07450 (11) | 0.10723 (4) | 0.0365 (4) | |
| N1 | 1.0526 (12) | −0.0684 (7) | 0.1767 (3) | 0.039 (2) | |
| N2 | 1.4312 (11) | −0.1559 (6) | 0.2576 (3) | 0.032 (2) | |
| N3 | 1.7228 (11) | −0.2492 (7) | 0.2989 (3) | 0.039 (2) | |
| N4 | 1.3514 (11) | −0.2392 (7) | 0.3785 (3) | 0.036 (2) | |
| N5 | 1.3643 (10) | −0.4852 (7) | 0.4384 (3) | 0.029 (2) | |
| N6 | 1.4522 (11) | −0.6811 (7) | 0.4423 (3) | 0.037 (2) | |
| C1 | 0.9411 (16) | −0.0224 (9) | 0.2091 (4) | 0.042 (3) | |
| H1A | 0.8262 | 0.0063 | 0.1987 | 0.051* | |
| C2 | 0.9913 (15) | −0.0165 (9) | 0.2567 (4) | 0.044 (3) | |
| H2A | 0.9147 | 0.0176 | 0.2790 | 0.053* | |
| C3 | 1.1567 (14) | −0.0616 (8) | 0.2713 (4) | 0.038 (3) | |
| H3A | 1.1948 | −0.0593 | 0.3040 | 0.045* | |
| C4 | 1.2640 (14) | −0.1092 (8) | 0.2385 (4) | 0.037 (3) | |
| C5 | 1.2109 (13) | −0.1129 (8) | 0.1925 (3) | 0.030 (2) | |
| H5A | 1.2867 | −0.1478 | 0.1703 | 0.036* | |
| C6 | 1.5589 (15) | −0.1921 (8) | 0.2304 (4) | 0.036 (3) | |
| H6A | 1.5464 | −0.1853 | 0.1966 | 0.043* | |
| C7 | 1.7202 (14) | −0.2428 (8) | 0.2502 (3) | 0.034 (3) | |
| C8 | 1.8553 (15) | −0.2858 (9) | 0.2230 (4) | 0.042 (3) | |
| H8A | 1.8478 | −0.2806 | 0.1891 | 0.050* | |
| C9 | 2.0017 (16) | −0.3364 (9) | 0.2440 (4) | 0.044 (3) | |
| H9A | 2.0955 | −0.3666 | 0.2250 | 0.053* | |
| C10 | 2.0096 (15) | −0.3424 (9) | 0.2930 (4) | 0.049 (3) | |
| H10A | 2.1101 | −0.3757 | 0.3088 | 0.059* | |
| C11 | 1.8675 (14) | −0.2987 (9) | 0.3186 (4) | 0.045 (3) | |
| H11A | 1.8725 | −0.3041 | 0.3525 | 0.054* | |
| C12 | 1.2362 (14) | −0.1885 (9) | 0.4062 (4) | 0.040 (3) | |
| H12A | 1.2122 | −0.1196 | 0.3988 | 0.049* | |
| C13 | 1.1467 (14) | −0.2310 (9) | 0.4462 (4) | 0.045 (3) | |
| H13A | 1.0588 | −0.1928 | 0.4638 | 0.054* | |
| C14 | 1.1884 (13) | −0.3277 (9) | 0.4593 (4) | 0.040 (3) | |
| H14A | 1.1356 | −0.3570 | 0.4870 | 0.048* | |
| C15 | 1.3101 (13) | −0.3826 (9) | 0.4310 (3) | 0.033 (3) | |
| C16 | 1.3879 (12) | −0.3373 (8) | 0.3914 (3) | 0.031 (3) | |
| H16A | 1.4704 | −0.3758 | 0.3724 | 0.037* | |
| C17 | 1.2990 (12) | −0.5374 (8) | 0.4725 (4) | 0.033 (3) | |
| H17A | 1.2150 | −0.5068 | 0.4941 | 0.040* | |
| C18 | 1.3492 (14) | −0.6418 (8) | 0.4791 (4) | 0.035 (3) | |
| C19 | 1.3045 (14) | −0.6992 (9) | 0.5186 (4) | 0.042 (3) | |
| H19A | 1.2341 | −0.6695 | 0.5435 | 0.051* | |
| C20 | 1.3595 (14) | −0.7977 (10) | 0.5228 (4) | 0.043 (3) | |
| H20A | 1.3260 | −0.8378 | 0.5496 | 0.052* | |
| C21 | 1.4685 (16) | −0.8371 (9) | 0.4854 (4) | 0.050 (3) | |
| H21A | 1.5134 | −0.9045 | 0.4872 | 0.060* | |
| C22 | 1.5098 (16) | −0.7777 (9) | 0.4462 (4) | 0.049 (3) | |
| H22A | 1.5814 | −0.8060 | 0.4212 | 0.058* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| I1 | 0.0911 (7) | 0.0473 (6) | 0.0383 (5) | −0.0199 (5) | −0.0001 (4) | −0.0023 (4) |
| I2 | 0.0311 (4) | 0.0564 (6) | 0.0292 (4) | 0.0023 (3) | −0.0015 (3) | 0.0035 (4) |
| Cu1 | 0.0506 (8) | 0.0436 (9) | 0.0259 (7) | 0.0010 (6) | 0.0002 (6) | 0.0026 (6) |
| Cu2 | 0.0346 (7) | 0.0508 (10) | 0.0241 (7) | 0.0002 (6) | 0.0001 (5) | 0.0010 (6) |
| N1 | 0.048 (6) | 0.047 (6) | 0.023 (5) | 0.004 (5) | −0.001 (4) | −0.002 (4) |
| N2 | 0.037 (5) | 0.034 (6) | 0.024 (5) | 0.001 (4) | −0.005 (4) | 0.007 (4) |
| N3 | 0.031 (5) | 0.039 (6) | 0.046 (6) | −0.005 (4) | −0.009 (4) | 0.003 (5) |
| N4 | 0.033 (5) | 0.040 (6) | 0.034 (5) | 0.006 (4) | 0.000 (4) | −0.012 (5) |
| N5 | 0.029 (4) | 0.041 (6) | 0.019 (4) | 0.004 (4) | −0.005 (3) | −0.003 (4) |
| N6 | 0.035 (5) | 0.036 (6) | 0.038 (5) | −0.010 (4) | −0.007 (4) | −0.008 (5) |
| C1 | 0.051 (7) | 0.046 (8) | 0.030 (6) | 0.006 (6) | 0.004 (5) | −0.003 (5) |
| C2 | 0.044 (7) | 0.065 (9) | 0.024 (6) | 0.006 (6) | 0.004 (5) | 0.001 (6) |
| C3 | 0.047 (7) | 0.037 (7) | 0.029 (6) | 0.013 (5) | −0.009 (5) | 0.005 (5) |
| C4 | 0.036 (6) | 0.037 (7) | 0.037 (7) | 0.005 (5) | −0.003 (5) | 0.000 (6) |
| C5 | 0.030 (6) | 0.036 (7) | 0.025 (6) | 0.000 (5) | −0.004 (4) | −0.003 (5) |
| C6 | 0.055 (7) | 0.034 (7) | 0.019 (5) | −0.003 (5) | −0.001 (5) | 0.002 (5) |
| C7 | 0.042 (6) | 0.038 (7) | 0.022 (6) | −0.005 (5) | −0.004 (5) | −0.001 (5) |
| C8 | 0.044 (7) | 0.047 (8) | 0.034 (6) | −0.009 (6) | 0.005 (5) | −0.007 (6) |
| C9 | 0.049 (7) | 0.037 (7) | 0.046 (8) | 0.003 (6) | −0.017 (6) | −0.014 (6) |
| C10 | 0.040 (7) | 0.052 (9) | 0.054 (8) | 0.018 (6) | −0.004 (6) | −0.007 (7) |
| C11 | 0.040 (7) | 0.048 (8) | 0.045 (7) | −0.006 (6) | −0.004 (5) | 0.005 (6) |
| C12 | 0.037 (6) | 0.031 (7) | 0.053 (8) | 0.006 (5) | −0.008 (5) | −0.005 (6) |
| C13 | 0.031 (6) | 0.043 (8) | 0.061 (8) | −0.003 (5) | 0.008 (5) | −0.007 (6) |
| C14 | 0.036 (6) | 0.047 (8) | 0.037 (6) | −0.005 (5) | 0.006 (5) | −0.009 (6) |
| C15 | 0.028 (5) | 0.047 (8) | 0.025 (6) | −0.001 (5) | −0.008 (4) | 0.002 (5) |
| C16 | 0.025 (5) | 0.039 (7) | 0.030 (6) | −0.011 (5) | −0.005 (4) | −0.008 (5) |
| C17 | 0.020 (5) | 0.048 (8) | 0.031 (6) | −0.005 (5) | −0.006 (4) | 0.013 (5) |
| C18 | 0.038 (6) | 0.038 (7) | 0.028 (6) | −0.008 (5) | −0.014 (5) | 0.000 (5) |
| C19 | 0.042 (6) | 0.055 (9) | 0.030 (6) | −0.010 (6) | 0.004 (5) | 0.011 (6) |
| C20 | 0.043 (7) | 0.052 (9) | 0.035 (7) | −0.006 (6) | −0.008 (5) | 0.008 (6) |
| C21 | 0.062 (8) | 0.033 (8) | 0.054 (8) | −0.008 (6) | −0.019 (6) | −0.002 (6) |
| C22 | 0.068 (8) | 0.038 (8) | 0.040 (7) | −0.010 (6) | 0.004 (6) | −0.008 (6) |
Geometric parameters (Å, º)
| I1—Cu1 | 2.5645 (16) | C5—H5A | 0.9500 |
| I2—Cu2 | 2.5832 (14) | C6—C7 | 1.443 (14) |
| Cu1—N4 | 1.980 (9) | C6—H6A | 0.9500 |
| Cu1—N3 | 2.074 (9) | C7—C8 | 1.365 (14) |
| Cu1—N2 | 2.078 (8) | C8—C9 | 1.372 (15) |
| Cu2—N1 | 2.018 (8) | C8—H8A | 0.9500 |
| Cu2—N6i | 2.053 (9) | C9—C10 | 1.371 (15) |
| Cu2—N5i | 2.107 (8) | C9—H9A | 0.9500 |
| N1—C5 | 1.350 (12) | C10—C11 | 1.382 (14) |
| N1—C1 | 1.361 (13) | C10—H10A | 0.9500 |
| N2—C6 | 1.291 (12) | C11—H11A | 0.9500 |
| N2—C4 | 1.445 (12) | C12—C13 | 1.415 (15) |
| N3—C11 | 1.341 (13) | C12—H12A | 0.9500 |
| N3—C7 | 1.362 (12) | C13—C14 | 1.362 (15) |
| N4—C12 | 1.323 (12) | C13—H13A | 0.9500 |
| N4—C16 | 1.372 (13) | C14—C15 | 1.390 (14) |
| N5—C17 | 1.270 (12) | C14—H14A | 0.9500 |
| N5—C15 | 1.426 (13) | C15—C16 | 1.381 (13) |
| N5—Cu2ii | 2.107 (8) | C16—H16A | 0.9500 |
| N6—C22 | 1.347 (14) | C17—C18 | 1.439 (15) |
| N6—C18 | 1.376 (13) | C17—H17A | 0.9500 |
| N6—Cu2ii | 2.053 (9) | C18—C19 | 1.382 (14) |
| C1—C2 | 1.376 (14) | C19—C20 | 1.366 (16) |
| C1—H1A | 0.9500 | C19—H19A | 0.9500 |
| C2—C3 | 1.386 (14) | C20—C21 | 1.413 (15) |
| C2—H2A | 0.9500 | C20—H20A | 0.9500 |
| C3—C4 | 1.358 (14) | C21—C22 | 1.382 (16) |
| C3—H3A | 0.9500 | C21—H21A | 0.9500 |
| C4—C5 | 1.339 (13) | C22—H22A | 0.9500 |
| N4—Cu1—N3 | 119.2 (4) | N3—C7—C8 | 122.0 (10) |
| N4—Cu1—N2 | 125.5 (3) | N3—C7—C6 | 114.4 (9) |
| N3—Cu1—N2 | 80.4 (3) | C8—C7—C6 | 123.5 (10) |
| N4—Cu1—I1 | 105.3 (3) | C7—C8—C9 | 120.7 (11) |
| N3—Cu1—I1 | 112.1 (2) | C7—C8—H8A | 119.6 |
| N2—Cu1—I1 | 112.9 (2) | C9—C8—H8A | 119.6 |
| N1—Cu2—N6i | 126.9 (3) | C10—C9—C8 | 118.5 (11) |
| N1—Cu2—N5i | 113.9 (3) | C10—C9—H9A | 120.8 |
| N6i—Cu2—N5i | 79.8 (3) | C8—C9—H9A | 120.8 |
| N1—Cu2—I2 | 109.9 (2) | C9—C10—C11 | 118.2 (11) |
| N6i—Cu2—I2 | 106.7 (2) | C9—C10—H10A | 120.9 |
| N5i—Cu2—I2 | 117.3 (2) | C11—C10—H10A | 120.9 |
| C5—N1—C1 | 118.5 (9) | N3—C11—C10 | 124.3 (11) |
| C5—N1—Cu2 | 121.7 (7) | N3—C11—H11A | 117.8 |
| C1—N1—Cu2 | 119.7 (7) | C10—C11—H11A | 117.8 |
| C6—N2—C4 | 122.4 (9) | N4—C12—C13 | 123.7 (11) |
| C6—N2—Cu1 | 111.2 (7) | N4—C12—H12A | 118.2 |
| C4—N2—Cu1 | 126.4 (6) | C13—C12—H12A | 118.2 |
| C11—N3—C7 | 116.3 (9) | C14—C13—C12 | 119.0 (10) |
| C11—N3—Cu1 | 131.4 (8) | C14—C13—H13A | 120.5 |
| C7—N3—Cu1 | 112.3 (7) | C12—C13—H13A | 120.5 |
| C12—N4—C16 | 116.4 (9) | C13—C14—C15 | 118.5 (10) |
| C12—N4—Cu1 | 122.0 (8) | C13—C14—H14A | 120.8 |
| C16—N4—Cu1 | 120.5 (6) | C15—C14—H14A | 120.8 |
| C17—N5—C15 | 121.6 (9) | C16—C15—C14 | 119.4 (11) |
| C17—N5—Cu2ii | 111.3 (7) | C16—C15—N5 | 114.6 (9) |
| C15—N5—Cu2ii | 126.8 (6) | C14—C15—N5 | 125.9 (9) |
| C22—N6—C18 | 117.7 (9) | N4—C16—C15 | 122.9 (9) |
| C22—N6—Cu2ii | 128.6 (7) | N4—C16—H16A | 118.5 |
| C18—N6—Cu2ii | 113.1 (7) | C15—C16—H16A | 118.5 |
| N1—C1—C2 | 121.3 (10) | N5—C17—C18 | 121.6 (10) |
| N1—C1—H1A | 119.3 | N5—C17—H17A | 119.2 |
| C2—C1—H1A | 119.3 | C18—C17—H17A | 119.2 |
| C1—C2—C3 | 118.2 (10) | N6—C18—C19 | 121.5 (10) |
| C1—C2—H2A | 120.9 | N6—C18—C17 | 113.8 (9) |
| C3—C2—H2A | 120.9 | C19—C18—C17 | 124.7 (10) |
| C4—C3—C2 | 119.5 (10) | C20—C19—C18 | 121.5 (11) |
| C4—C3—H3A | 120.2 | C20—C19—H19A | 119.3 |
| C2—C3—H3A | 120.2 | C18—C19—H19A | 119.3 |
| C5—C4—C3 | 120.5 (10) | C19—C20—C21 | 116.8 (11) |
| C5—C4—N2 | 124.3 (9) | C19—C20—H20A | 121.6 |
| C3—C4—N2 | 115.2 (9) | C21—C20—H20A | 121.6 |
| C4—C5—N1 | 121.8 (9) | C22—C21—C20 | 120.1 (11) |
| C4—C5—H5A | 119.1 | C22—C21—H21A | 119.9 |
| N1—C5—H5A | 119.1 | C20—C21—H21A | 119.9 |
| N2—C6—C7 | 121.3 (9) | N6—C22—C21 | 122.4 (11) |
| N2—C6—H6A | 119.4 | N6—C22—H22A | 118.8 |
| C7—C6—H6A | 119.4 | C21—C22—H22A | 118.8 |
Symmetry codes: (i) −x+5/2, y+1/2, −z+1/2; (ii) −x+5/2, y−1/2, −z+1/2.
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C22—H22A···I1iii | 0.95 | 3.03 | 3.789 (12) | 138 |
| C20—H20A···I1iv | 0.95 | 3.14 | 4.025 (12) | 156 |
| C17—H17A···I2v | 0.95 | 3.16 | 4.011 (11) | 149 |
Symmetry codes: (iii) x, y−1, z; (iv) −x+3, −y−1, −z+1; (v) x+1/2, −y−1/2, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SU2480).
References
- Altomare, A., Cascarano, G., Giacovazzo, C., Guagliardi, A., Burla, M. C., Polidori, G. & Camalli, M. (1994). J. Appl. Cryst 27, 435.
- Blessing, R. H. (1995). Acta Cryst. A51, 33–38. [DOI] [PubMed]
- Dehghanpour, S., Khalaj, M. & Mahmoudi, A. (2009). Polyhedron, 28, 1205–1210.
- Fei, B. L., Sun, W. Y., Yu, K. B. & Tang, W. X. (2000). J. Chem. Soc. Dalton Trans. pp. 805–811.
- Moulton, B. & Zaworotko, M. J. (2001). Chem. Rev. 101, 1629–1658. [DOI] [PubMed]
- Nonius (2002). COLLECT Nonius BV, Delft, The Netherlands.
- Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276, Macromolecular Crystallography, Part A, edited by C. W. Carter Jr & R. M. Sweet, pp. 307–326. New York: Academic Press.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812037270/su2480sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812037270/su2480Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


