Acta Cryst. (2009). E65, m1250 [ doi:10.1107/S1600536809038215 ]
2N,N')zinc(II)In the title compound, [ZnCl2(C12H12N2)], the complete molecule is generated by crystallographic mirror symmetry, with the Zn atom and both chloride ions lying on the reflecting plane, yielding a distorted ZnN2Cl2 tetrahedral coordination for the metal ion. In the crystal, there are
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contacts between the pyridine rings [centroid-centroid distance = 3.7857 (17) Å].
A solution of 6,6'-dimethyl-2,2'-bipyridine (0.20 g, 1.10 mmol) in methanol (10 ml) was added to a solution of ZnCl2 (0.15 g, 0.88 mmol) in acetonitrile (10 ml) and the resulting colourless solution was stirred for 20 min at at 313 K. This solution was left to evaporate slowly at room temperature. After one week, colorless prisms of (I) were isolated (yield 0.26 g, 73.7%).
All H atoms were positioned geometrically, with C—H = 0.93–0.96Å and constrained to ride on their parent atoms, with Uiso(H)=1.2Ueq(C) or 1.5Ueq(methyl C).
Data collection: SMART (Bruker, 1998); cell refinement: SAINT (Bruker, 1998); data reduction: SAINT (Bruker, 1998); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).
| Fig. 1. The molecular structure of (I). Displacement ellipsoids are drawn at the 50% probability level. [Symmetry codes: (a) x,-y + 3/2,z] |
| Fig. 2. Tha unit-cell packing of (I). |
| [ZnCl2(C12H12N2)] | F(000) = 324 |
| Mr = 320.53 | Dx = 1.611 Mg m−3 |
| Monoclinic, P21/m | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2yb | Cell parameters from 1170 reflections |
| a = 7.6957 (15) Å | θ = 2.8–30.6° |
| b = 11.266 (2) Å | µ = 2.24 mm−1 |
| c = 8.1431 (16) Å | T = 298 K |
| β = 110.61 (3)° | Prism, colourless |
| V = 660.8 (3) Å3 | 0.40 × 0.33 × 0.30 mm |
| Z = 2 |
| Bruker SMART CCD diffractometer | 2075 independent reflections |
| Radiation source: fine-focus sealed tube | 1972 reflections with I > 2σ(I) |
| graphite | Rint = 0.043 |
| ω scans | θmax = 30.6°, θmin = 2.8° |
| Absorption correction: multi-scan (SADABS; Sheldrick, 1998) | h = −10→10 |
| Tmin = 0.421, Tmax = 0.512 | k = −16→16 |
| 8852 measured reflections | l = −11→10 |
| 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)] = 0.034 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.101 | H-atom parameters constrained |
| S = 1.26 | w = 1/[σ2(Fo2) + (0.036P)2 + 0.4143P] where P = (Fo2 + 2Fc2)/3 |
| 2075 reflections | (Δ/σ)max < 0.001 |
| 83 parameters | Δρmax = 0.70 e Å−3 |
| 0 restraints | Δρmin = −0.55 e Å−3 |
| [ZnCl2(C12H12N2)] | V = 660.8 (3) Å3 |
| Mr = 320.53 | Z = 2 |
| Monoclinic, P21/m | Mo Kα radiation |
| a = 7.6957 (15) Å | µ = 2.24 mm−1 |
| b = 11.266 (2) Å | T = 298 K |
| c = 8.1431 (16) Å | 0.40 × 0.33 × 0.30 mm |
| β = 110.61 (3)° |
| Bruker SMART CCD diffractometer | 2075 independent reflections |
| Absorption correction: multi-scan (SADABS; Sheldrick, 1998) | 1972 reflections with I > 2σ(I) |
| Tmin = 0.421, Tmax = 0.512 | Rint = 0.043 |
| 8852 measured reflections | θmax = 30.6° |
| R[F2 > 2σ(F2)] = 0.034 | H-atom parameters constrained |
| wR(F2) = 0.101 | Δρmax = 0.70 e Å−3 |
| S = 1.26 | Δρmin = −0.55 e Å−3 |
| 2075 reflections | Absolute structure: ? |
| 83 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 | 0.9103 (5) | 1.0397 (3) | 0.7493 (4) | 0.0605 (7) | |
| H1A | 0.8626 | 1.0161 | 0.8386 | 0.091* | |
| H1B | 0.9085 | 1.1247 | 0.7405 | 0.091* | |
| H1C | 1.0355 | 1.0117 | 0.7793 | 0.091* | |
| C2 | 0.7921 (3) | 0.9875 (2) | 0.5768 (3) | 0.0415 (5) | |
| C3 | 0.6959 (4) | 1.0566 (2) | 0.4331 (4) | 0.0525 (6) | |
| H3 | 0.7041 | 1.1389 | 0.4413 | 0.063* | |
| C4 | 0.5891 (4) | 1.0046 (3) | 0.2791 (4) | 0.0524 (6) | |
| H4 | 0.5246 | 1.0512 | 0.1825 | 0.063* | |
| C5 | 0.5776 (3) | 0.8820 (2) | 0.2679 (3) | 0.0424 (5) | |
| H5 | 0.5053 | 0.8449 | 0.1644 | 0.051* | |
| C6 | 0.6762 (3) | 0.81599 (18) | 0.4143 (3) | 0.0317 (4) | |
| N1 | 0.7813 (2) | 0.86822 (16) | 0.5661 (2) | 0.0330 (3) | |
| Cl1 | 1.20088 (11) | 0.7500 | 0.88188 (13) | 0.0521 (2) | |
| Cl2 | 0.74082 (14) | 0.7500 | 0.94980 (13) | 0.0511 (2) | |
| Zn1 | 0.89560 (5) | 0.7500 | 0.76788 (4) | 0.03392 (12) |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.0688 (19) | 0.0401 (13) | 0.0625 (17) | −0.0094 (12) | 0.0104 (15) | −0.0154 (12) |
| C2 | 0.0457 (12) | 0.0306 (10) | 0.0480 (12) | −0.0039 (8) | 0.0162 (10) | −0.0032 (8) |
| C3 | 0.0694 (17) | 0.0281 (10) | 0.0616 (16) | 0.0033 (10) | 0.0249 (14) | 0.0063 (10) |
| C4 | 0.0641 (16) | 0.0434 (13) | 0.0473 (13) | 0.0122 (12) | 0.0168 (12) | 0.0161 (11) |
| C5 | 0.0453 (12) | 0.0424 (12) | 0.0342 (10) | 0.0048 (9) | 0.0074 (9) | 0.0057 (9) |
| C6 | 0.0326 (9) | 0.0308 (9) | 0.0300 (8) | 0.0014 (7) | 0.0091 (7) | 0.0016 (7) |
| N1 | 0.0341 (8) | 0.0288 (8) | 0.0328 (8) | −0.0010 (6) | 0.0075 (6) | −0.0002 (6) |
| Cl1 | 0.0325 (4) | 0.0642 (6) | 0.0492 (5) | 0.000 | 0.0014 (3) | 0.000 |
| Cl2 | 0.0548 (5) | 0.0567 (5) | 0.0479 (4) | 0.000 | 0.0255 (4) | 0.000 |
| Zn1 | 0.03172 (18) | 0.03621 (19) | 0.02830 (18) | 0.000 | 0.00368 (12) | 0.000 |
| C1—C2 | 1.499 (4) | C4—H4 | 0.9300 |
| C1—H1A | 0.9600 | C5—C6 | 1.383 (3) |
| C1—H1B | 0.9600 | C5—H5 | 0.9300 |
| C1—H1C | 0.9600 | C6—N1 | 1.350 (3) |
| C2—N1 | 1.347 (3) | C6—C6i | 1.487 (4) |
| C2—C3 | 1.384 (4) | Zn1—N1 | 2.0569 (18) |
| C3—C4 | 1.366 (4) | Zn1—Cl1 | 2.2013 (11) |
| C3—H3 | 0.9300 | Zn1—Cl2 | 2.2035 (10) |
| C4—C5 | 1.386 (4) | Zn1—N1i | 2.0569 (18) |
| C2—C1—H1A | 109.5 | C6—C5—C4 | 118.4 (2) |
| C2—C1—H1B | 109.5 | C6—C5—H5 | 120.8 |
| H1A—C1—H1B | 109.5 | C4—C5—H5 | 120.8 |
| C2—C1—H1C | 109.5 | N1—C6—C5 | 121.6 (2) |
| H1A—C1—H1C | 109.5 | N1—C6—C6i | 115.83 (11) |
| H1B—C1—H1C | 109.5 | C5—C6—C6i | 122.51 (14) |
| N1—C2—C3 | 120.3 (2) | C2—N1—C6 | 119.82 (19) |
| N1—C2—C1 | 117.1 (2) | C2—N1—Zn1 | 126.50 (16) |
| C3—C2—C1 | 122.6 (2) | C6—N1—Zn1 | 113.51 (13) |
| C4—C3—C2 | 120.3 (2) | N1i—Zn1—N1 | 80.71 (10) |
| C4—C3—H3 | 119.8 | N1i—Zn1—Cl1 | 115.45 (6) |
| C2—C3—H3 | 119.8 | N1—Zn1—Cl1 | 115.45 (6) |
| C3—C4—C5 | 119.5 (2) | N1i—Zn1—Cl2 | 110.90 (6) |
| C3—C4—H4 | 120.3 | N1—Zn1—Cl2 | 110.90 (6) |
| C5—C4—H4 | 120.3 | Cl1—Zn1—Cl2 | 117.76 (5) |
| N1—C2—C3—C4 | 0.0 (4) | C5—C6—N1—C2 | −0.2 (3) |
| C1—C2—C3—C4 | −179.6 (3) | C6i—C6—N1—C2 | 178.78 (16) |
| C2—C3—C4—C5 | 0.1 (5) | C5—C6—N1—Zn1 | 175.34 (17) |
| C3—C4—C5—C6 | −0.2 (4) | C6i—C6—N1—Zn1 | −5.7 (3) |
| C4—C5—C6—N1 | 0.3 (4) | C2—N1—Zn1—N1i | −178.10 (16) |
| C4—C5—C6—C6i | −178.63 (19) | C6—N1—Zn1—N1i | 6.69 (17) |
| C3—C2—N1—C6 | 0.0 (4) | C2—N1—Zn1—Cl1 | −64.2 (2) |
| C1—C2—N1—C6 | 179.7 (2) | C6—N1—Zn1—Cl1 | 120.55 (13) |
| C3—C2—N1—Zn1 | −174.88 (19) | C2—N1—Zn1—Cl2 | 73.0 (2) |
| C1—C2—N1—Zn1 | 4.7 (3) | C6—N1—Zn1—Cl2 | −102.24 (14) |
| Symmetry codes: (i) x, −y+3/2, z. |
| Zn1—N1 | 2.0569 (18) | Zn1—Cl2 | 2.2035 (10) |
| Zn1—Cl1 | 2.2013 (11) | ||
| N1i—Zn1—N1 | 80.71 (10) |
| Symmetry codes: (i) x, −y+3/2, z. |
We are grateful to the Damghan University of Basic Sciences and Islamic Azad University, Shahr-e-Rey Branch, for financial support.
Ahmadi, R., Kalateh, K., Alizadeh, R., Khoshtarkib, Z. & Amani, V. (2009a). Acta Cryst. E65, m848–m849.
Ahmadi, R., Kalateh, K., Alizadeh, R., Khoshtarkib, Z. & Amani, V. (2009b). Acta Cryst. E65, m1169–m1170.
Ahmadi, R., Kalateh, K., Ebadi, A., Amani, V. & Khavasi, H. R. (2008). Acta Cryst. E64, m1266.
Alizadeh, R., Heidari, A., Ahmadi, R. & Amani, V. (2009). Acta Cryst. E65, m483–m484.
Bruker (2003). or (1998). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA. Please check date; 2003 in CIF
Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838.
Gruia, L. M., Rochon, F. D. & Beauchamp, A. L. (2007). Inorg. Chim. Acta, 360, 1825–1840.
Khalighi, A., Ahmadi, R., Amani, V. & Khavasi, H. R. (2008). Acta Cryst. E64, m1211–m1212.
Khan, M. A. & Tuck, D. G. (1984). Acta Cryst. C40, 60–62.
Khavasi, H. R., Abedi, A., Amani, V., Notash, B. & Safari, N. (2008). Polyhedron, 27, 1848–1854.
Khoshtarkib, Z., Ebadi, A., Alizadeh, R., Ahmadi, R. & Amani, V. (2009). Acta Cryst. E65, m739–m740.
Kozhevnikov, D. N., Shabunina, O. V., Kopchuk, D. S., Slepukhin, P. A. & Kozhevnikov, V. N. (2006). Tetrahedron Lett. 47, 7025–7029.
Liu, Q. D., Wang, R. & Wang, S. (2004). Dalton Trans. pp. 2073-2079.
Preston, H. S. & Kennard, C. H. L. (1969). J. Chem. Soc. A, pp. 1965–1968.
Reimann, C. W., Block, S. & Perloff, A. (1966). Inorg. Chem. 5, 1185–1189.
Sheldrick, G. M. (1998). SADABS. University of Göttingen, Germany.
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.
Recently, we reported the synthes and crystal structure of [ZnCl2(phend)], (II), (Khoshtarkib et al., 2009), [HgBr2(2,9-dmphen)], (III), (Alizadeh et al., 2009), [HgCl2(2,9-dmPh2phen)].0.5 CH3CN, (IV) (Ahmadi, et al., 2009a) and [Pb4(NO3)8(6-mbpy)4], (V), (Ahmadi, et al., 2009b) [where phend is phenanthridine, 2,9-dmphen is 2,9-dimethyl-1,10-phenanthroline, 2,9-dmPh2phen is 2,9-dimethyl-4,7-diphenyl-1,10-phenanthroline and 6-mbpy is 6-methyl-2,2'-bipyridine].
There are several ZnII complexes, with formula, [ZnCl2(N—N)], such as [ZnCl2(bipy)], (VI), (Khan & Tuck, 1984), [ZnCl2(biim)], (VII), (Gruia et al., 2007), [ZnCl2(phbipy)], (IIX), (Kozhevnikov et al., 2006), [ZnCl2(phen)], (IX), (Reimann et al., 1966), [ZnCl2(dmphen)], (X), (Preston & Kennard, 1969), [ZnCl2(dpdmbip)], (XI), (Liu et al., 2004), [ZnCl2(dm4bt)], (XII), (Khavasi et al., 2008), [ZnCl2(5,5'-dmbpy)], (XIII), (Khalighi et al., 2008) and [ZnCl2(6-mbpy)], (XIV), (Ahmadi, Kalateh, Ebadi et al., 2008) [where bipy is 2,2'-bipyridine, biim is 2,2'-biimidazole, phbipy is 5-phenyl-2,2'-bipyridine, phen is 1,10-phenanthroline, dmphen is 2,9-dimethyl-1,10-phenanthroline, dpdmbip is 4,4'-diphenyl-6,6'-dimethyl-2,2'-bipyrimidine, dm4bt is 2,2'-dimethyl-4,4'-bithiazole and 5,5'-dmbpy 5,5'-dimethyl-2,2'-bipyridine] have been synthesized and characterized by single-crystal X-ray diffraction methods. We report herein the synthesis and crystal structure of the title compound (I).
The asymmetric unit of the title compound, (I), (Fig. 1), contains half molecule. The ZnII atom is four-coordinated in distorted tetrahedral configurations by two N atoms from one 6,6'-dimethyl-2,2'-bipyridine and two terminal Cl atoms. The Zn—Cl and Zn—N bond lengths and angles are collected in Table 1.
In the crystal structure, the π-π contacts between the rings A (N1/C2—C6) and rings A, Cg2···Cg2i [distance = 3.7857 (17) Å, symmetry cods: 1-X,2-Y,1-Z]. It seems this π-π stacking is effective in the stabilization of the crystal structure (Fig. 2).