metal-organic compounds
Di-μ-azido-bis({N′-[1-(2-pyridyl-κN)ethylidene]acetohydrazidato-κ2N′,O}dicopper(II))
aNational Changhua University of Education, Department of Chemistry, Changhua, Taiwan 50058
*Correspondence e-mail: leehm@cc.ncue.edu.tw
The dimeric title compound, [Cu2(C9H10N3O)2(N3)2], is located on a crystallographic inversion center. The Cu atom is coordinated by a tridentate anionic hydrazone ligand and two bridging azide ligands in a distorted square-pyramidal coordination geometry. The non-bonding Cu⋯Cu distance is 3.238 (1) Å. Non-classical intermolecular C—H⋯N hydrogen bonds link the dimers into chains along the c axis.
Related literature
For related dimeric copper(II) complexes with similar tridentate ligands, see: Recio Despaigne et al. (2009); Sen et al. (2007); Patole et al. (2003).
Experimental
Crystal data
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Refinement
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Data collection: APEX2 (Bruker, 2007); cell 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: DIAMOND (Brandenburg, 2006).
Supporting information
10.1107/S1600536810034860/pv2324sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536810034860/pv2324Isup2.hkl
The tridentate ligand precursor, 2-benzoylpyridine-methyl hydrazone, was prepared according to the literature procedure (Recio Despaigne et al., 2009). To the tridentate ligand precursor (1.0 mmol), methanolic solution (20 ml) of copper nitrate trihydrate (0.241 g, 1.0 mmol), was added, followed by the addition, with constant stirring of a solution of sodium azide (0.065 g, 1.0 mmol) in minimum volume of water/methanol mixture. The final solution was kept at room temperature yielding brown square-shaped crystals suitable for X-ray diffraction after few days. Crystals were isolated by filtration and were air-dried.
All the hydrogen atoms were located in the difference Fourier map, nevertheless, all the H atoms were positioned geometrically and refined as riding atoms, with Caryl—H = 0.95, Cmethyl—H = 0.98 Å while Uiso(H) = 1.2Ueq(Caryl) and 1.5Ueq(Cmethyl) H atoms. Although the residual electron in the final difference map is high, the
model appears to be reliable since the largest peak and hole are located near the heavy Cu atom at distances of 0.70 and 0.03 Å, respectively.Data collection: APEX2 (Bruker, 2007); cell
SAINT (Bruker, 2007); data reduction: SAINT (Bruker, 2007); 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: DIAMOND (Brandenburg, 2006).[Cu2(C9H10N3O)2(N3)2] | Z = 1 |
Mr = 563.54 | F(000) = 286 |
Triclinic, P1 | Dx = 1.654 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 7.589 (3) Å | Cell parameters from 3185 reflections |
b = 8.955 (3) Å | θ = 2.9–28.5° |
c = 9.693 (4) Å | µ = 1.92 mm−1 |
α = 66.534 (15)° | T = 150 K |
β = 69.461 (13)° | Prism, brown |
γ = 81.468 (16)° | 0.25 × 0.20 × 0.20 mm |
V = 565.8 (4) Å3 |
Bruker SMART APEXII diffractometer | 2358 independent reflections |
Radiation source: fine-focus sealed tube | 1591 reflections with I > 2σ |
Graphite monochromator | Rint = 0.040 |
ω scans | θmax = 27.0°, θmin = 3.1° |
Absorption correction: multi-scan (SADABS; Sheldrick, 2003) | h = −9→9 |
Tmin = 0.645, Tmax = 0.700 | k = −11→10 |
3858 measured reflections | l = −12→12 |
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)] = 0.027 | Hydrogen site location: difference Fourier map |
wR(F2) = 0.093 | H-atom parameters constrained |
S = 1.08 | w = 1/[σ2(Fo2) + (0.0597P)2] where P = (Fo2 + 2Fc2)/3 |
2358 reflections | (Δ/σ)max = 0.001 |
156 parameters | Δρmax = 2.08 e Å−3 |
0 restraints | Δρmin = −2.81 e Å−3 |
[Cu2(C9H10N3O)2(N3)2] | γ = 81.468 (16)° |
Mr = 563.54 | V = 565.8 (4) Å3 |
Triclinic, P1 | Z = 1 |
a = 7.589 (3) Å | Mo Kα radiation |
b = 8.955 (3) Å | µ = 1.92 mm−1 |
c = 9.693 (4) Å | T = 150 K |
α = 66.534 (15)° | 0.25 × 0.20 × 0.20 mm |
β = 69.461 (13)° |
Bruker SMART APEXII diffractometer | 2358 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 2003) | 1591 reflections with I > 2σ |
Tmin = 0.645, Tmax = 0.700 | Rint = 0.040 |
3858 measured reflections |
R[F2 > 2σ(F2)] = 0.027 | 0 restraints |
wR(F2) = 0.093 | H-atom parameters constrained |
S = 1.08 | Δρmax = 2.08 e Å−3 |
2358 reflections | Δρmin = −2.81 e Å−3 |
156 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Cu1 | 0.34274 (3) | 0.93665 (3) | 0.95880 (3) | 0.02989 (14) | |
N5 | 0.2011 (2) | 0.7390 (2) | 1.0402 (2) | 0.0307 (5) | |
O1 | 0.4938 (2) | 0.8357 (2) | 0.8052 (2) | 0.0380 (5) | |
N1 | 0.4648 (3) | 1.1498 (2) | 0.8642 (2) | 0.0329 (5) | |
N6 | 0.2719 (3) | 0.6294 (3) | 0.9663 (2) | 0.0367 (6) | |
C8 | 0.4270 (3) | 0.6937 (3) | 0.8443 (3) | 0.0314 (6) | |
N2 | 0.5605 (3) | 1.2073 (2) | 0.7250 (2) | 0.0358 (6) | |
N4 | 0.1206 (2) | 0.9791 (2) | 1.1350 (2) | 0.0315 (5) | |
C1 | −0.0012 (3) | 0.8504 (3) | 1.2187 (3) | 0.0341 (6) | |
C2 | −0.1553 (3) | 0.8504 (4) | 1.3488 (3) | 0.0438 (8) | |
H2 | −0.2404 | 0.7619 | 1.4036 | 0.053* | |
C9 | 0.5264 (3) | 0.5944 (3) | 0.7465 (3) | 0.0436 (7) | |
H9A | 0.4938 | 0.6357 | 0.6483 | 0.065* | |
H9B | 0.4881 | 0.4806 | 0.8067 | 0.065* | |
H9C | 0.6627 | 0.6019 | 0.7202 | 0.065* | |
C5 | 0.0911 (3) | 1.1048 (3) | 1.1831 (3) | 0.0390 (7) | |
H5 | 0.1758 | 1.1935 | 1.1254 | 0.047* | |
C6 | 0.0467 (3) | 0.7153 (3) | 1.1593 (3) | 0.0351 (7) | |
C3 | −0.1850 (3) | 0.9815 (4) | 1.3992 (3) | 0.0470 (9) | |
H3 | −0.2888 | 0.9825 | 1.4891 | 0.056* | |
C4 | −0.0596 (4) | 1.1095 (4) | 1.3148 (3) | 0.0449 (7) | |
H4 | −0.0761 | 1.1997 | 1.3465 | 0.054* | |
N3 | 0.6520 (4) | 1.2683 (4) | 0.5959 (3) | 0.0644 (10) | |
C7 | −0.0748 (4) | 0.5681 (4) | 1.2321 (4) | 0.0564 (10) | |
H7A | −0.0411 | 0.5099 | 1.1594 | 0.085* | |
H7B | −0.2073 | 0.6022 | 1.2516 | 0.085* | |
H7C | −0.0556 | 0.4962 | 1.3328 | 0.085* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cu1 | 0.03078 (16) | 0.0297 (2) | 0.02843 (18) | −0.00779 (10) | −0.00486 (12) | −0.01154 (14) |
N5 | 0.0319 (7) | 0.0317 (10) | 0.0289 (9) | −0.0042 (7) | −0.0062 (7) | −0.0133 (8) |
O1 | 0.0400 (8) | 0.0382 (10) | 0.0350 (9) | −0.0100 (6) | −0.0044 (7) | −0.0163 (8) |
N1 | 0.0386 (8) | 0.0306 (10) | 0.0287 (9) | −0.0063 (7) | −0.0068 (8) | −0.0117 (9) |
N6 | 0.0383 (9) | 0.0368 (11) | 0.0351 (10) | −0.0048 (8) | −0.0079 (9) | −0.0154 (9) |
C8 | 0.0389 (9) | 0.0296 (11) | 0.0318 (10) | −0.0017 (8) | −0.0140 (9) | −0.0148 (9) |
N2 | 0.0404 (9) | 0.0327 (10) | 0.0316 (10) | −0.0034 (7) | −0.0105 (8) | −0.0091 (9) |
N4 | 0.0303 (7) | 0.0331 (10) | 0.0310 (9) | −0.0027 (6) | −0.0079 (7) | −0.0126 (8) |
C1 | 0.0286 (8) | 0.0403 (12) | 0.0295 (11) | −0.0040 (7) | −0.0073 (8) | −0.0098 (10) |
C2 | 0.0346 (10) | 0.0535 (16) | 0.0353 (12) | −0.0070 (9) | −0.0012 (9) | −0.0150 (13) |
C9 | 0.0495 (12) | 0.0421 (15) | 0.0402 (13) | −0.0022 (10) | −0.0097 (11) | −0.0200 (12) |
C5 | 0.0395 (10) | 0.0399 (14) | 0.0386 (12) | −0.0032 (9) | −0.0109 (10) | −0.0162 (12) |
C6 | 0.0323 (9) | 0.0352 (12) | 0.0343 (11) | −0.0074 (8) | −0.0070 (9) | −0.0102 (10) |
C3 | 0.0388 (10) | 0.0623 (19) | 0.0358 (13) | 0.0030 (10) | −0.0028 (10) | −0.0234 (14) |
C4 | 0.0484 (12) | 0.0489 (16) | 0.0437 (14) | 0.0071 (10) | −0.0130 (11) | −0.0277 (12) |
N3 | 0.0746 (16) | 0.0654 (19) | 0.0323 (12) | −0.0125 (13) | −0.0042 (12) | −0.0045 (14) |
C7 | 0.0493 (13) | 0.0495 (18) | 0.0599 (19) | −0.0198 (12) | 0.0053 (13) | −0.0229 (16) |
Cu1—N5 | 1.941 (2) | C1—C6 | 1.484 (4) |
Cu1—N1 | 1.969 (2) | C2—C3 | 1.403 (5) |
Cu1—O1 | 1.979 (2) | C2—H2 | 0.9500 |
Cu1—N4 | 2.051 (2) | C9—H9A | 0.9800 |
Cu1—N1i | 2.4574 (18) | C9—H9B | 0.9800 |
N5—C6 | 1.297 (3) | C9—H9C | 0.9800 |
N5—N6 | 1.377 (4) | C5—C4 | 1.394 (4) |
O1—C8 | 1.300 (3) | C5—H5 | 0.9500 |
N1—N2 | 1.218 (3) | C6—C7 | 1.500 (3) |
N1—Cu1i | 2.4574 (18) | C3—C4 | 1.386 (4) |
N6—C8 | 1.341 (3) | C3—H3 | 0.9500 |
C8—C9 | 1.493 (5) | C4—H4 | 0.9500 |
N2—N3 | 1.142 (3) | C7—H7A | 0.9800 |
N4—C5 | 1.343 (4) | C7—H7B | 0.9800 |
N4—C1 | 1.374 (3) | C7—H7C | 0.9800 |
C1—C2 | 1.387 (4) | ||
N5—Cu1—N1 | 173.44 (6) | C1—C2—C3 | 119.8 (2) |
N5—Cu1—O1 | 79.78 (9) | C1—C2—H2 | 120.1 |
N1—Cu1—O1 | 101.14 (9) | C3—C2—H2 | 120.1 |
N5—Cu1—N4 | 80.27 (9) | C8—C9—H9A | 109.5 |
N1—Cu1—N4 | 98.12 (10) | C8—C9—H9B | 109.5 |
O1—Cu1—N4 | 159.42 (8) | H9A—C9—H9B | 109.5 |
N5—Cu1—N1i | 99.67 (7) | C8—C9—H9C | 109.5 |
N1—Cu1—N1i | 86.64 (6) | H9A—C9—H9C | 109.5 |
O1—Cu1—N1i | 98.75 (8) | H9B—C9—H9C | 109.5 |
N4—Cu1—N1i | 89.51 (8) | N4—C5—C4 | 122.3 (2) |
C6—N5—N6 | 123.0 (2) | N4—C5—H5 | 118.9 |
C6—N5—Cu1 | 119.7 (2) | C4—C5—H5 | 118.9 |
N6—N5—Cu1 | 117.28 (14) | N5—C6—C1 | 113.21 (19) |
C8—O1—Cu1 | 110.27 (16) | N5—C6—C7 | 124.6 (3) |
N2—N1—Cu1 | 122.4 (2) | C1—C6—C7 | 122.2 (3) |
N2—N1—Cu1i | 111.79 (13) | C4—C3—C2 | 118.5 (3) |
Cu1—N1—Cu1i | 93.36 (6) | C4—C3—H3 | 120.7 |
C8—N6—N5 | 107.9 (2) | C2—C3—H3 | 120.7 |
O1—C8—N6 | 124.6 (3) | C3—C4—C5 | 119.4 (3) |
O1—C8—C9 | 118.6 (2) | C3—C4—H4 | 120.3 |
N6—C8—C9 | 116.8 (2) | C5—C4—H4 | 120.3 |
N3—N2—N1 | 176.3 (3) | C6—C7—H7A | 109.5 |
C5—N4—C1 | 119.0 (2) | C6—C7—H7B | 109.5 |
C5—N4—Cu1 | 128.98 (15) | H7A—C7—H7B | 109.5 |
C1—N4—Cu1 | 111.8 (2) | C6—C7—H7C | 109.5 |
N4—C1—C2 | 121.1 (3) | H7A—C7—H7C | 109.5 |
N4—C1—C6 | 114.9 (2) | H7B—C7—H7C | 109.5 |
C2—C1—C6 | 124.0 (2) |
Symmetry code: (i) −x+1, −y+2, −z+2. |
D—H···A | D—H | H···A | D···A | D—H···A |
C9—H9A···N3ii | 0.98 | 2.74 | 3.710 (4) | 171 |
Symmetry code: (ii) −x+1, −y+2, −z+1. |
Experimental details
Crystal data | |
Chemical formula | [Cu2(C9H10N3O)2(N3)2] |
Mr | 563.54 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 150 |
a, b, c (Å) | 7.589 (3), 8.955 (3), 9.693 (4) |
α, β, γ (°) | 66.534 (15), 69.461 (13), 81.468 (16) |
V (Å3) | 565.8 (4) |
Z | 1 |
Radiation type | Mo Kα |
µ (mm−1) | 1.92 |
Crystal size (mm) | 0.25 × 0.20 × 0.20 |
Data collection | |
Diffractometer | Bruker SMART APEXII diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 2003) |
Tmin, Tmax | 0.645, 0.700 |
No. of measured, independent and observed (I > 2σ) reflections | 3858, 2358, 1591 |
Rint | 0.040 |
(sin θ/λ)max (Å−1) | 0.639 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.027, 0.093, 1.08 |
No. of reflections | 2358 |
No. of parameters | 156 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 2.08, −2.81 |
Computer programs: APEX2 (Bruker, 2007), SAINT (Bruker, 2007), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008), DIAMOND (Brandenburg, 2006).
D—H···A | D—H | H···A | D···A | D—H···A |
C9—H9A···N3i | 0.98 | 2.74 | 3.710 (4) | 171 |
Symmetry code: (i) −x+1, −y+2, −z+1. |
Acknowledgements
We are grateful to the National Science Council of Taiwan for financial support of this work.
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
The title compound is a dimeric copper(II) complex. Each copper atom is coordinated by a tridentate, anionic hydrazone ligand and two bridging azide ligands. The non-bonding Cu···Cu distance is 3.238 (1) Å, which is slightly longer than that in a related dicopper azido complex (Sen et al.., 2007).
The dimer is located on a crystallographic inversion center. The non-classical intermolecular hydrogen bonds of the type C—H···N link the dimeric compounds into one dimensional chains along the c axis.
Dimeric copper(II) complexes with similar tridentate ligands have been reported in the literature (Recio Despaigne et al., 2009; Sen et al. 2007; Patole et al. 2003).