Abstract
In the title complex, [HgI2(C12H12N2)], the HgII atom has a distorted tetrahedral coordination formed by two N atoms of the 6,6′-dimethyl-2,2′-bipyridine ligand and two terminal I atoms [N—Hg—N = 70.1 (2) and I—Hg—I = 130.59 (3)°]. The crystal packing features π–π contacts between the pyridine rings of adjacent molecules [centroid–centroid distance = 3.773 (5) Å] and also between a pyridine ring of one molecule and the five-membered chelate ring of an adjacent molecule [centroid–centroid distance = 3.668 (4) Å].
Related literature
For the structures of metal complexes with a 6,6′-dimethyl-2,2′-bipyridine ligand, see: Akbarzadeh Torbati et al. (2010 ▶); Alizadeh et al. (2010 ▶); Alizadeh, Kalateh, Ebadi et al. (2009 ▶); Alizadeh, Kalateh, Khoshtarkib et al. (2009 ▶); Alizadeh, Khoshtarkib et al. (2009 ▶); Itoh et al. (2005 ▶); Kou et al. (2008 ▶); Onggo et al. (2005 ▶).
Experimental
Crystal data
[HgI2(C12H12N2)]
M r = 638.63
Monoclinic,
a = 8.8096 (18) Å
b = 12.025 (2) Å
c = 14.693 (3) Å
β = 101.88 (3)°
V = 1523.2 (5) Å3
Z = 4
Mo Kα radiation
μ = 14.14 mm−1
T = 298 K
0.16 × 0.15 × 0.12 mm
Data collection
Bruker APEXII CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2001 ▶) T min = 0.128, T max = 0.186
9361 measured reflections
4057 independent reflections
3409 reflections with I > 2σ(I)
R int = 0.051
Refinement
R[F 2 > 2σ(F 2)] = 0.040
wR(F 2) = 0.095
S = 1.10
4057 reflections
154 parameters
H-atom parameters constrained
Δρmax = 1.22 e Å−3
Δρmin = −1.23 e Å−3
Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811004041/ya2136sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811004041/ya2136Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected bond lengths (Å).
| N1—Hg1 | 2.380 (5) |
| N2—Hg1 | 2.381 (6) |
| I1—Hg1 | 2.6503 (10) |
| I2—Hg1 | 2.6876 (7) |
Acknowledgments
The authors are grateful to Damghan University for financial support.
supplementary crystallographic information
Comment
6,6'-Dimethyl-2,2'-bipyridine (6,6'-dmbipy) is a rather widely used bidentate ligand, and complexes of different metals with 6,6'-dmbipy have been prepared, e.g. those of cobalt (Akbarzadeh Torbati et al., 2010),cadmium (Alizadeh et al., 2010),zinc (Alizadeh, Kalateh, Ebadi et al., 2009; Alizadeh, Kalateh, Khoshtarkib et al., 2009; Alizadeh, Khoshtarkib et al., 2009), copper (Itoh et al., 2005), nickel (Kou et al., 2008), and ruthenium (Onggo et al., 2005). We report herein the synthesis and first crystal structure of the mercury complex of this ligand (Fig. 1).
The Hg1 atom has a distorted tetrahedral coordination formed by atoms N1 and N2 of the 6,6'-dimethyl-2,2'-bipyridine ligand and terminal I1 and I2 atoms [N—Hg—N 70.1 (2)°; I—Hg—I 130.59 (3)°; see Table 1 for bond lengths involving Hg1].
In the crystal structure, intermolecular /p-/p contacts (Fig. 2) between the pyridine rings and also between pyridine ring and chelate ring of the adjacent molecules may stabilize the structure: the centroid-centroid distances Cg1—Cg2i and Cg2—Cg3i are equal to 3.668 (4) and 3.773 (5)Å respectively [Cg1, Cg2 and Cg3 represent centroids of the rings (Hg1/N1/C6/C7/N2), (N1/C2—C6), and (N2/C7—C11); symmetry code (i): 2 - x,1 - y,-z].
Experimental
For the preparation of the title compound, a solution of 6,6'-dimethyl-2,2'-bipyridine (0.28 g, 1.50 mmol) in acetonitrile (10 ml) was added to a solution of HgI2 (0.68 g, 1.50 mmol) in methanol (10 ml), and the resulting colorless mixture was stirred for 30 min at 313 K. It was then left to evaporate slowly at room temperature. After six days, colorless prismatic crystals of the title compound, suitable for X-ray diffraction experiment, were isolated (yield 0.71 g; 74.1%).
Refinement
All H atoms were positioned geometrically, with C—H 0.93 and 0.96 Å for aromatics and methyl hydrogen atoms, respectively, and constrained to ride on their parent atoms, with Uiso(H)=1.2Ueq. The highest residual density peak and the deepest hole (1.22 and -1.23 e A°-3) are located at distances of 0.83 and 0.82 Å from the Hg1 atom respectively.
Figures
Fig. 1.
Molecular structure of the title compound;. displacement ellipsoids are drawn at the 30% probability level.
Fig. 2.
Packing diagram for the crystal of the title compound viewed along the a axis.
Crystal data
| [HgI2(C12H12N2)] | F(000) = 1136 |
| Mr = 638.63 | Dx = 2.785 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2yn | Cell parameters from 1223 reflections |
| a = 8.8096 (18) Å | θ = 2.2–29.2° |
| b = 12.025 (2) Å | µ = 14.14 mm−1 |
| c = 14.693 (3) Å | T = 298 K |
| β = 101.88 (3)° | Prism, colorless |
| V = 1523.2 (5) Å3 | 0.16 × 0.15 × 0.12 mm |
| Z = 4 |
Data collection
| Bruker APEXII CCD area-detector diffractometer | 4057 independent reflections |
| Radiation source: fine-focus sealed tube | 3409 reflections with I > 2σ(I) |
| graphite | Rint = 0.051 |
| φ and ω scans | θmax = 29.2°, θmin = 2.2° |
| Absorption correction: multi-scan (SADABS; Bruker, 2001) | h = −11→12 |
| Tmin = 0.128, Tmax = 0.186 | k = −16→13 |
| 9361 measured reflections | l = −20→17 |
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)] = 0.040 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.095 | H-atom parameters constrained |
| S = 1.10 | w = 1/[σ2(Fo2) + (0.0397P)2 + 3.5854P] where P = (Fo2 + 2Fc2)/3 |
| 4057 reflections | (Δ/σ)max = 0.001 |
| 154 parameters | Δρmax = 1.22 e Å−3 |
| 0 restraints | Δρmin = −1.23 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 | ||
| C1 | 0.6805 (9) | 0.4904 (8) | 0.1498 (7) | 0.065 (2) | |
| H1A | 0.6238 | 0.5560 | 0.1595 | 0.077* | |
| H1B | 0.7749 | 0.4868 | 0.1960 | 0.077* | |
| H1C | 0.6186 | 0.4258 | 0.1547 | 0.077* | |
| C2 | 0.7174 (7) | 0.4943 (6) | 0.0569 (5) | 0.0493 (16) | |
| C3 | 0.6678 (9) | 0.4111 (7) | −0.0091 (6) | 0.061 (2) | |
| H3 | 0.6079 | 0.3520 | 0.0042 | 0.073* | |
| C4 | 0.7097 (10) | 0.4188 (7) | −0.0941 (7) | 0.069 (2) | |
| H4 | 0.6773 | 0.3644 | −0.1388 | 0.083* | |
| C5 | 0.7983 (9) | 0.5055 (7) | −0.1137 (6) | 0.060 (2) | |
| H5 | 0.8272 | 0.5100 | −0.1710 | 0.072* | |
| C6 | 0.8444 (7) | 0.5869 (6) | −0.0461 (5) | 0.0478 (15) | |
| C7 | 0.9441 (7) | 0.6807 (6) | −0.0608 (4) | 0.0445 (14) | |
| C8 | 0.9964 (10) | 0.6955 (9) | −0.1438 (6) | 0.066 (2) | |
| H8 | 0.9628 | 0.6477 | −0.1936 | 0.079* | |
| C9 | 1.0961 (13) | 0.7794 (10) | −0.1518 (8) | 0.080 (3) | |
| H9 | 1.1294 | 0.7900 | −0.2073 | 0.096* | |
| C10 | 1.1474 (10) | 0.8489 (8) | −0.0772 (8) | 0.074 (3) | |
| H10 | 1.2190 | 0.9046 | −0.0812 | 0.089* | |
| C11 | 1.0915 (9) | 0.8353 (7) | 0.0045 (7) | 0.0592 (19) | |
| C12 | 1.1391 (11) | 0.9092 (8) | 0.0862 (8) | 0.079 (3) | |
| H12A | 1.1882 | 0.8659 | 0.1389 | 0.094* | |
| H12B | 1.0493 | 0.9456 | 0.0998 | 0.094* | |
| H12C | 1.2106 | 0.9640 | 0.0728 | 0.094* | |
| N1 | 0.8032 (6) | 0.5792 (4) | 0.0366 (4) | 0.0399 (11) | |
| N2 | 0.9903 (6) | 0.7526 (5) | 0.0104 (4) | 0.0452 (12) | |
| I1 | 1.05284 (6) | 0.68838 (5) | 0.30203 (4) | 0.06506 (16) | |
| I2 | 0.61128 (6) | 0.85868 (4) | 0.09788 (4) | 0.05659 (14) | |
| Hg1 | 0.86805 (3) | 0.73253 (2) | 0.139654 (19) | 0.04718 (9) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.051 (4) | 0.060 (5) | 0.081 (6) | −0.010 (3) | 0.009 (4) | 0.019 (4) |
| C2 | 0.041 (3) | 0.037 (3) | 0.066 (4) | 0.003 (2) | 0.003 (3) | 0.005 (3) |
| C3 | 0.047 (3) | 0.045 (4) | 0.082 (6) | 0.004 (3) | −0.005 (4) | −0.010 (4) |
| C4 | 0.062 (4) | 0.056 (5) | 0.077 (6) | 0.008 (4) | −0.012 (4) | −0.027 (4) |
| C5 | 0.057 (4) | 0.068 (5) | 0.051 (4) | 0.014 (4) | 0.004 (3) | −0.018 (4) |
| C6 | 0.041 (3) | 0.058 (4) | 0.042 (3) | 0.019 (3) | 0.002 (2) | −0.005 (3) |
| C7 | 0.045 (3) | 0.051 (4) | 0.039 (3) | 0.014 (3) | 0.012 (2) | 0.006 (3) |
| C8 | 0.066 (5) | 0.088 (6) | 0.047 (4) | 0.020 (4) | 0.020 (4) | 0.009 (4) |
| C9 | 0.087 (6) | 0.094 (8) | 0.070 (6) | 0.019 (6) | 0.041 (5) | 0.034 (6) |
| C10 | 0.062 (5) | 0.065 (6) | 0.107 (8) | 0.009 (4) | 0.046 (5) | 0.028 (5) |
| C11 | 0.050 (4) | 0.045 (4) | 0.088 (6) | 0.003 (3) | 0.026 (4) | 0.017 (4) |
| C12 | 0.074 (6) | 0.053 (5) | 0.116 (8) | −0.016 (4) | 0.034 (6) | −0.012 (5) |
| N1 | 0.038 (2) | 0.036 (3) | 0.045 (3) | 0.005 (2) | 0.006 (2) | −0.002 (2) |
| N2 | 0.045 (3) | 0.040 (3) | 0.054 (3) | 0.006 (2) | 0.021 (2) | 0.006 (2) |
| I1 | 0.0656 (3) | 0.0743 (4) | 0.0493 (3) | 0.0076 (3) | −0.0020 (2) | −0.0064 (2) |
| I2 | 0.0534 (2) | 0.0536 (3) | 0.0609 (3) | 0.0024 (2) | 0.0073 (2) | −0.0054 (2) |
| Hg1 | 0.05023 (14) | 0.04953 (15) | 0.04286 (13) | −0.00229 (11) | 0.01209 (10) | −0.00399 (11) |
Geometric parameters (Å, °)
| C1—C2 | 1.468 (12) | C8—C9 | 1.359 (15) |
| C1—H1A | 0.9600 | C8—H8 | 0.9300 |
| C1—H1B | 0.9600 | C9—C10 | 1.379 (16) |
| C1—H1C | 0.9600 | C9—H9 | 0.9300 |
| C2—N1 | 1.340 (9) | C10—C11 | 1.398 (13) |
| C2—C3 | 1.399 (10) | C10—H10 | 0.9300 |
| C3—C4 | 1.377 (14) | C11—N2 | 1.351 (9) |
| C3—H3 | 0.9300 | C11—C12 | 1.483 (14) |
| C4—C5 | 1.367 (13) | C12—H12A | 0.9600 |
| C4—H4 | 0.9300 | C12—H12B | 0.9600 |
| C5—C6 | 1.394 (10) | C12—H12C | 0.9600 |
| C5—H5 | 0.9300 | N1—Hg1 | 2.380 (5) |
| C6—N1 | 1.341 (9) | N2—Hg1 | 2.381 (6) |
| C6—C7 | 1.473 (11) | I1—Hg1 | 2.6503 (10) |
| C7—N2 | 1.354 (9) | I2—Hg1 | 2.6876 (7) |
| C7—C8 | 1.401 (10) | ||
| C2—C1—H1A | 109.5 | C8—C9—C10 | 119.5 (9) |
| C2—C1—H1B | 109.5 | C8—C9—H9 | 120.2 |
| H1A—C1—H1B | 109.5 | C10—C9—H9 | 120.2 |
| C2—C1—H1C | 109.5 | C9—C10—C11 | 119.8 (9) |
| H1A—C1—H1C | 109.5 | C9—C10—H10 | 120.1 |
| H1B—C1—H1C | 109.5 | C11—C10—H10 | 120.1 |
| N1—C2—C3 | 120.0 (8) | N2—C11—C10 | 119.7 (9) |
| N1—C2—C1 | 118.4 (7) | N2—C11—C12 | 118.1 (8) |
| C3—C2—C1 | 121.6 (7) | C10—C11—C12 | 122.3 (8) |
| C4—C3—C2 | 118.5 (8) | C11—C12—H12A | 109.5 |
| C4—C3—H3 | 120.8 | C11—C12—H12B | 109.5 |
| C2—C3—H3 | 120.8 | H12A—C12—H12B | 109.5 |
| C5—C4—C3 | 120.9 (8) | C11—C12—H12C | 109.5 |
| C5—C4—H4 | 119.5 | H12A—C12—H12C | 109.5 |
| C3—C4—H4 | 119.5 | H12B—C12—H12C | 109.5 |
| C4—C5—C6 | 118.7 (8) | C2—N1—C6 | 121.6 (6) |
| C4—C5—H5 | 120.6 | C2—N1—Hg1 | 121.4 (5) |
| C6—C5—H5 | 120.6 | C6—N1—Hg1 | 116.7 (5) |
| N1—C6—C5 | 120.2 (8) | C11—N2—C7 | 121.2 (7) |
| N1—C6—C7 | 117.8 (6) | C11—N2—Hg1 | 122.6 (6) |
| C5—C6—C7 | 121.9 (7) | C7—N2—Hg1 | 116.0 (4) |
| N2—C7—C8 | 119.4 (7) | N1—Hg1—N2 | 70.1 (2) |
| N2—C7—C6 | 118.0 (6) | N1—Hg1—I1 | 116.12 (12) |
| C8—C7—C6 | 122.6 (7) | N2—Hg1—I1 | 116.33 (14) |
| C9—C8—C7 | 120.3 (9) | N1—Hg1—I2 | 102.20 (12) |
| C9—C8—H8 | 119.8 | N2—Hg1—I2 | 104.98 (13) |
| C7—C8—H8 | 119.8 | I1—Hg1—I2 | 130.59 (3) |
| N1—C2—C3—C4 | 0.3 (10) | C5—C6—N1—Hg1 | −174.1 (5) |
| C1—C2—C3—C4 | −178.5 (7) | C7—C6—N1—Hg1 | 8.4 (7) |
| C2—C3—C4—C5 | 0.2 (12) | C10—C11—N2—C7 | 1.4 (11) |
| C3—C4—C5—C6 | −0.7 (12) | C12—C11—N2—C7 | −178.7 (7) |
| C4—C5—C6—N1 | 0.6 (10) | C10—C11—N2—Hg1 | −173.7 (6) |
| C4—C5—C6—C7 | 177.9 (6) | C12—C11—N2—Hg1 | 6.2 (10) |
| N1—C6—C7—N2 | 1.0 (8) | C8—C7—N2—C11 | −3.1 (10) |
| C5—C6—C7—N2 | −176.4 (6) | C6—C7—N2—C11 | 174.8 (6) |
| N1—C6—C7—C8 | 178.7 (6) | C8—C7—N2—Hg1 | 172.3 (5) |
| C5—C6—C7—C8 | 1.3 (10) | C6—C7—N2—Hg1 | −9.8 (7) |
| N2—C7—C8—C9 | 1.8 (11) | C2—N1—Hg1—N2 | 176.3 (5) |
| C6—C7—C8—C9 | −175.9 (8) | C6—N1—Hg1—N2 | −9.7 (4) |
| C7—C8—C9—C10 | 1.1 (14) | C2—N1—Hg1—I1 | 65.9 (5) |
| C8—C9—C10—C11 | −2.7 (15) | C6—N1—Hg1—I1 | −120.0 (4) |
| C9—C10—C11—N2 | 1.5 (13) | C2—N1—Hg1—I2 | −82.0 (4) |
| C9—C10—C11—C12 | −178.4 (9) | C6—N1—Hg1—I2 | 92.1 (4) |
| C3—C2—N1—C6 | −0.4 (9) | C11—N2—Hg1—N1 | −174.6 (6) |
| C1—C2—N1—C6 | 178.5 (6) | C7—N2—Hg1—N1 | 10.1 (4) |
| C3—C2—N1—Hg1 | 173.4 (5) | C11—N2—Hg1—I1 | −64.5 (6) |
| C1—C2—N1—Hg1 | −7.8 (8) | C7—N2—Hg1—I1 | 120.2 (4) |
| C5—C6—N1—C2 | −0.1 (9) | C11—N2—Hg1—I2 | 87.6 (5) |
| C7—C6—N1—C2 | −177.5 (5) | C7—N2—Hg1—I2 | −87.7 (4) |
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: YA2136).
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 I, global. DOI: 10.1107/S1600536811004041/ya2136sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811004041/ya2136Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


