Acta Cryst. (2009). E65, m525 [ doi:10.1107/S1600536809013427 ]
2N,N']bis(thiocyanato-
N)copper(II)In the title complex, [Cu(NCS)2(C6H8N2)2], the CuII atom, lying on an inversion center, adopts a Jahn-Teller distorted octahedral CuN6 coordination geometry. The two bidentate 2-aminomethylpyridine ligands are coordinated in a trans fashion, while the two thiocyanate ligands are at the axial positions and coordinate to the Cu atom in a bent mode with a C-N-Cu angle of 127.49 (10)°. Intermolecular N-H
N and N-H
S hydrogen bonds link the copper complex molecules into an infinite two-dimensional network.
To a methanolic solution (10 ml) of Cu(O2CCH3)2.H2O (1.0 mmol, 0.199 g), a methanolic solution (10.0 ml) of 2-aminomethylpyridine (2.0 mmol, 0.207 ml) was added dropwise with stirring. Then to this mixture of solution, NaSCN (2.0 mmol, 0.162 g) in methanol (5.0 ml) was added and the mixture was stirred for 5 min. The solution was kept undisturbed. Blue crystals suitable for X-ray crystallography were obtained after one week by slow evaporation of the solvent.
All the H atoms were positioned geometrically and refined as riding atoms, with N—H = 0.92, Caryl—H = 0.95, Cmethylene—H = 0.99 Å while Uiso(H) = 1.2Ueq(C or N) for all H atoms.
Data collection: APEX2 (Bruker, 2004); cell refinement: SAINT (Bruker, 2004); data reduction: SAINT (Bruker, 2004); 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).
| [Cu(NCS)2(C6H8N2)2] | F(000) = 406 |
| Mr = 395.99 | Dx = 1.626 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 3360 reflections |
| a = 9.1023 (4) Å | θ = 3.1–28.0° |
| b = 9.1740 (4) Å | µ = 1.62 mm−1 |
| c = 9.6895 (4) Å | T = 150 K |
| β = 91.872 (3)° | Plate, blue |
| V = 808.69 (6) Å3 | 0.46 × 0.38 × 0.31 mm |
| Z = 2 |
| Bruker SMART APEXII diffractometer | 2086 independent reflections |
| Radiation source: fine-focus sealed tube | 1776 reflections with I > 2σ |
| graphite | Rint = 0.031 |
| ω scans | θmax = 28.7°, θmin = 2.2° |
| Absorption correction: multi-scan (SADABS; Sheldrick, 2003) | h = −12→12 |
| Tmin = 0.497, Tmax = 0.603 | k = −12→12 |
| 11419 measured reflections | l = −13→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)] = 0.023 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.063 | H-atom parameters constrained |
| S = 1.13 | w = 1/[σ2(Fo2) + (0.0308P)2 + 0.2097P] where P = (Fo2 + 2Fc2)/3 |
| 2086 reflections | (Δ/σ)max < 0.001 |
| 106 parameters | Δρmax = 0.35 e Å−3 |
| 0 restraints | Δρmin = −0.40 e Å−3 |
| [Cu(NCS)2(C6H8N2)2] | V = 808.69 (6) Å3 |
| Mr = 395.99 | Z = 2 |
| Monoclinic, P21/c | Mo Kα radiation |
| a = 9.1023 (4) Å | µ = 1.62 mm−1 |
| b = 9.1740 (4) Å | T = 150 K |
| c = 9.6895 (4) Å | 0.46 × 0.38 × 0.31 mm |
| β = 91.872 (3)° |
| Bruker SMART APEXII diffractometer | 2086 independent reflections |
| Absorption correction: multi-scan (SADABS; Sheldrick, 2003) | 1776 reflections with I > 2σ |
| Tmin = 0.497, Tmax = 0.603 | Rint = 0.031 |
| 11419 measured reflections | θmax = 28.7° |
| R[F2 > 2σ(F2)] = 0.023 | H-atom parameters constrained |
| wR(F2) = 0.063 | Δρmax = 0.35 e Å−3 |
| S = 1.13 | Δρmin = −0.40 e Å−3 |
| 2086 reflections | Absolute structure: ? |
| 106 parameters | Flack parameter: ? |
| 0 restraints | Rogers parameter: ? |
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 | ||
| C1 | 0.27555 (16) | 0.35413 (16) | 0.48964 (15) | 0.0151 (3) | |
| C2 | 0.41671 (16) | 0.30420 (16) | 0.52349 (17) | 0.0187 (3) | |
| H2 | 0.4607 | 0.2302 | 0.4701 | 0.022* | |
| C3 | 0.49184 (16) | 0.36421 (17) | 0.63614 (17) | 0.0199 (3) | |
| H3 | 0.5878 | 0.3311 | 0.6618 | 0.024* | |
| C4 | 0.42557 (17) | 0.47314 (17) | 0.71109 (17) | 0.0190 (3) | |
| H4 | 0.4759 | 0.5170 | 0.7878 | 0.023* | |
| C5 | 0.28491 (17) | 0.51688 (16) | 0.67232 (16) | 0.0170 (3) | |
| H5 | 0.2395 | 0.5917 | 0.7236 | 0.020* | |
| C6 | 0.18680 (17) | 0.29582 (17) | 0.36793 (16) | 0.0188 (3) | |
| H6A | 0.2513 | 0.2813 | 0.2888 | 0.023* | |
| H6B | 0.1435 | 0.2005 | 0.3918 | 0.023* | |
| C7 | −0.15576 (16) | 0.17946 (16) | 0.52438 (16) | 0.0175 (3) | |
| Cu1 | 0.0000 | 0.5000 | 0.5000 | 0.01369 (8) | |
| N1 | 0.20991 (13) | 0.45719 (14) | 0.56437 (13) | 0.0142 (2) | |
| N2 | 0.06857 (13) | 0.39999 (14) | 0.32960 (13) | 0.0161 (3) | |
| H2A | −0.0087 | 0.3513 | 0.2869 | 0.019* | |
| H2B | 0.1030 | 0.4680 | 0.2688 | 0.019* | |
| N3 | −0.08726 (15) | 0.26276 (15) | 0.58955 (15) | 0.0244 (3) | |
| S1 | −0.25589 (5) | 0.06047 (5) | 0.43612 (4) | 0.02601 (11) |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0159 (7) | 0.0142 (6) | 0.0154 (7) | 0.0005 (5) | 0.0020 (5) | 0.0008 (5) |
| C2 | 0.0166 (7) | 0.0171 (7) | 0.0225 (8) | 0.0036 (6) | 0.0032 (6) | 0.0011 (6) |
| C3 | 0.0140 (7) | 0.0215 (7) | 0.0243 (8) | 0.0029 (6) | 0.0003 (6) | 0.0069 (6) |
| C4 | 0.0167 (7) | 0.0224 (8) | 0.0177 (8) | −0.0027 (6) | −0.0030 (6) | 0.0016 (6) |
| C5 | 0.0164 (7) | 0.0187 (7) | 0.0159 (7) | −0.0008 (6) | 0.0001 (6) | −0.0009 (5) |
| C6 | 0.0187 (7) | 0.0201 (7) | 0.0176 (8) | 0.0052 (6) | −0.0015 (6) | −0.0049 (6) |
| C7 | 0.0168 (7) | 0.0183 (7) | 0.0175 (8) | 0.0037 (6) | 0.0027 (6) | 0.0057 (6) |
| Cu1 | 0.01194 (13) | 0.01631 (13) | 0.01273 (14) | 0.00240 (9) | −0.00107 (9) | −0.00347 (9) |
| N1 | 0.0130 (6) | 0.0152 (5) | 0.0143 (6) | 0.0009 (5) | 0.0004 (5) | 0.0000 (5) |
| N2 | 0.0154 (6) | 0.0190 (6) | 0.0140 (6) | 0.0017 (5) | −0.0006 (5) | −0.0019 (5) |
| N3 | 0.0261 (7) | 0.0213 (7) | 0.0255 (8) | −0.0016 (6) | −0.0033 (6) | 0.0040 (6) |
| S1 | 0.0235 (2) | 0.0293 (2) | 0.0251 (2) | −0.00253 (17) | −0.00159 (16) | −0.00652 (17) |
| C1—N1 | 1.3430 (19) | C6—N2 | 1.4775 (18) |
| C1—C2 | 1.393 (2) | C6—H6A | 0.9900 |
| C1—C6 | 1.506 (2) | C6—H6B | 0.9900 |
| C2—C3 | 1.383 (2) | C7—N3 | 1.160 (2) |
| C2—H2 | 0.9500 | C7—S1 | 1.6440 (16) |
| C3—C4 | 1.385 (2) | Cu1—N2 | 2.0062 (12) |
| C3—H3 | 0.9500 | Cu1—N2i | 2.0062 (12) |
| C4—C5 | 1.382 (2) | Cu1—N1 | 2.0288 (12) |
| C4—H4 | 0.9500 | Cu1—N1i | 2.0288 (12) |
| C5—N1 | 1.3466 (19) | N2—H2A | 0.9200 |
| C5—H5 | 0.9500 | N2—H2B | 0.9200 |
| N1—C1—C2 | 121.85 (14) | C1—C6—H6B | 109.8 |
| N1—C1—C6 | 115.83 (12) | H6A—C6—H6B | 108.2 |
| C2—C1—C6 | 122.32 (13) | N3—C7—S1 | 178.26 (15) |
| C3—C2—C1 | 118.90 (14) | N2—Cu1—N2i | 180.0 |
| C3—C2—H2 | 120.5 | N2—Cu1—N1 | 81.33 (5) |
| C1—C2—H2 | 120.5 | N2i—Cu1—N1 | 98.67 (5) |
| C2—C3—C4 | 119.23 (14) | N2—Cu1—N1i | 98.67 (5) |
| C2—C3—H3 | 120.4 | N2i—Cu1—N1i | 81.33 (5) |
| C4—C3—H3 | 120.4 | N1—Cu1—N1i | 180.0 |
| C5—C4—C3 | 118.84 (14) | C1—N1—C5 | 118.81 (13) |
| C5—C4—H4 | 120.6 | C1—N1—Cu1 | 113.68 (10) |
| C3—C4—H4 | 120.6 | C5—N1—Cu1 | 127.49 (10) |
| N1—C5—C4 | 122.33 (14) | C6—N2—Cu1 | 109.43 (9) |
| N1—C5—H5 | 118.8 | C6—N2—H2A | 109.8 |
| C4—C5—H5 | 118.8 | Cu1—N2—H2A | 109.8 |
| N2—C6—C1 | 109.56 (12) | C6—N2—H2B | 109.8 |
| N2—C6—H6A | 109.8 | Cu1—N2—H2B | 109.8 |
| C1—C6—H6A | 109.8 | H2A—N2—H2B | 108.2 |
| N2—C6—H6B | 109.8 | ||
| N1—C1—C2—C3 | −0.9 (2) | C6—C1—N1—Cu1 | 3.52 (16) |
| C6—C1—C2—C3 | 179.38 (14) | C4—C5—N1—C1 | −1.7 (2) |
| C1—C2—C3—C4 | −0.7 (2) | C4—C5—N1—Cu1 | 176.34 (11) |
| C2—C3—C4—C5 | 1.1 (2) | N2—Cu1—N1—C1 | −17.99 (10) |
| C3—C4—C5—N1 | 0.1 (2) | N2i—Cu1—N1—C1 | 162.01 (10) |
| N1—C1—C6—N2 | 19.63 (18) | N2—Cu1—N1—C5 | 163.84 (13) |
| C2—C1—C6—N2 | −160.67 (14) | N2i—Cu1—N1—C5 | −16.16 (13) |
| C2—C1—N1—C5 | 2.2 (2) | C1—C6—N2—Cu1 | −33.03 (14) |
| C6—C1—N1—C5 | −178.14 (13) | N1—Cu1—N2—C6 | 27.99 (10) |
| C2—C1—N1—Cu1 | −176.18 (11) | N1i—Cu1—N2—C6 | −152.01 (10) |
| Symmetry codes: (i) −x, −y+1, −z+1. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| N2—H2A···N3ii | 0.92 | 2.27 | 3.0717 (19) | 145 |
| N2—H2B···S1iii | 0.92 | 2.60 | 3.4628 (13) | 156 |
| Symmetry codes: (ii) x, −y+1/2, z−1/2; (iii) −x, y+1/2, −z+1/2. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| N2—H2A···N3i | 0.92 | 2.27 | 3.0717 (19) | 145 |
| N2—H2B···S1ii | 0.92 | 2.60 | 3.4628 (13) | 156 |
| Symmetry codes: (i) x, −y+1/2, z−1/2; (ii) −x, y+1/2, −z+1/2. |
We thank the National Science Council of Taiwan for financial support of this work.
Bruker (2004). APEX2 andSAINT. Bruker AXS Inc., Madison, Wisconsin, USA.
Ferrer, S., Haasnoot, J. G., Reedijk, J., Muller, E., Biagini-Cingi, M., Manotti-Lanfredi, A. M., Ugozzoli, F. & Foglia, C. (1992). J. Chem. Soc. Dalton Trans. pp. 3029–3034.
Gary, J. B., Kautz, J. A., Klausmeyer, K. K. & Wong, C.-W. (2004). Acta Cryst. E60, m328–m329.
Gorji, A., Mahmoudkhani, A. H. M. & Amirnasr, M. (2001). Inorg. Chim. Acta, 315, 133–138
Kozlowski, D. L. & Hodgson, D. L. (1975). J. Chem. Soc. Dalton Trans. pp. 55–58.
Li, Z.-X. & Zhang, X.-L. (2004). Acta Cryst. E60, m1597–m1598.
Sheldrick, G. M. (2003). SADABS. University of Göttingen, Germany.
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.
The tilte complex was readily obtained from the reaction between copper(II) acetate, 2-aminomethylpyridine, and sodium thiocyanate. The complex consists of two trans bidentate ligands and two trans thiocyanate ligands (Fig. 1). It exhibits an octahedron coordination geometry at the Cu atom which is located on the inversion center. The bent coordination of thiocyanate results in the C5—N1—Cu1 bond angle of 127.49 (10)°. The pyridine ring is twisted from the equatorial plane defined by the Cu and the four N atoms; the interplanar angle is 17.86 (8)°. Intermolecular H-bonds of the type N—H···N and N—H···S exist, linking the complex into a into a two-dimensional hydrogen bonded network (Table 1).
Six-coordinate trans-dithiocyanato Cu(II) complexes similar to the title complex have been reported in the literature (Gary et al., 2004; Ferrer et al., 1992; Gorji et al., 2001; Kozlowski & Hodgson, 1975; Li & Zhang, 2004).