Abstract
The dinuclear title complex, [Cd2I4(C12H13N5)2], lies on a crystallographic center of inversion. The CdII atom is four-coordinated by two N atoms from two 1-[(2-ethyl-1H-imidazol-1-yl)methyl]-1H-benzotriazole (bmei) ligands and two terminal I atoms in a distorted tetrahedral coordination environment. The CdII atoms are connected to each other by two bridging bmei ligands. The benzotriazole rings in adjacent molecules are almost parallel, with an average interplanar distance of 3.3400 (2) Å and a centroid–centroid distance of 4.852 (2) Å.
Related literature
For related structures, see: Meng et al. (2009 ▶); Huang et al. (2006 ▶); Zhai et al. (2006 ▶); Wang et al. (2010 ▶).
Experimental
Crystal data
[Cd2I4(C12H13N5)2]
M r = 1186.95
Triclinic,
a = 7.8323 (4) Å
b = 10.0657 (6) Å
c = 11.2335 (7) Å
α = 78.849 (5)°
β = 86.020 (5)°
γ = 77.538 (5)°
V = 848.08 (9) Å3
Z = 1
Mo Kα radiation
μ = 4.93 mm−1
T = 290 K
0.25 × 0.21 × 0.15 mm
Data collection
Agilent Xcalibur Eos Gemini diffractometer
Absorption correction: Gaussian [numerical absorption correction based on Gaussian integration over a multifaceted crystal model (CrysAlis PRO; Agilent, 2010 ▶)] T min = 0.287, T max = 0.487
13998 measured reflections
3462 independent reflections
2961 reflections with I > 2σ(I)
R int = 0.031
Refinement
R[F 2 > 2σ(F 2)] = 0.027
wR(F 2) = 0.061
S = 1.08
3462 reflections
182 parameters
H-atom parameters constrained
Δρmax = 0.82 e Å−3
Δρmin = −1.05 e Å−3
Data collection: CrysAlis PRO (Agilent, 2010 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: OLEX2 (Dolomanov et al., 2009 ▶); software used to prepare material for publication: OLEX2 and publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811021179/zq2107sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021179/zq2107Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Acknowledgments
The authors thank Professor Hong-Wei Hou and Yu Zhu of Zhengzhou University for their help.
supplementary crystallographic information
Comment
Imidazole and benzotriazole derivatives have been widely used in the construction of complexes since they can act as polydentate ligands and function as bridging ligands (Meng et al., 2009; Huang et al., 2006). The CdII atom is a good model atom to construct complexes owing to its property to form bonds with different donors simultaneously, and to its various modes (Zhai et al., 2006; Wang et al., 2010). In this work, through the reaction of 1-[(2-ethyl-1H-imidazol-1-yl)methyl]-1H-benzotriazole (bmei) with cadmium iodide at room temperature, we obtained the title complex [Cd2(C12H13N5)2I2], which is reported here.
The dinuclear title complex, [Cd2(C12H13N5)2I2], lies on a crystallographic center of inversion. The CdII atom is four-coordinated by two N atoms from two 1-[(2-ethyl-1H-imidazol-1-yl)methyl]-1H-benzotriazole (bmei) ligands and two terminal I atoms in a distorted tetrahedral coordination environment. The CdII atoms are connected by two bridging bmei ligands (Fig. 1). The distance between two Cd atoms bridged by two bmei ligands is 8.4983 (7) Å. In addition, the benzotriazole rings in adjacent molecules are almost parallel with an average interplanar distance of 3.3400 (2) Å and a centroid-centroid distance of 4.852 (2) Å.
Experimental
The ligand 1-[(2-ethyl-1H-imidazol-1-yl)methyl]-1H-benzotriazole (0.04 mmol, 0.0096 g) in methanol (6 ml) was added dropwise to a methanol solution (6 ml) of CdI2 (0.04 mmol, 0.0146 g) in methanol. The resulting solution was allowed to stand at room temperature. After two weeks good quality colourless crystals were obtained from the dried in air.
Refinement
H atoms were generated geometrically and refined as riding atoms with C—H = 0.93 Å and Uiso(H) = 1.2Ueq(C) for aromatic H atoms, with C—H = 0.97 Å and Uiso(H) = 1.2Ueq(C) for methylene H atoms, and with C—H = 0.96 Å and Uiso(H) = 1.5Ueq(C) for methyl H atoms.
Figures
Fig. 1.
View of the title complex, showing the labeling of the 30% probability ellipsolids (all H atoms have been omitted for clarity). Symmetry code: (A) -x + 1, -y + 2, -z.
Fig. 2.
A view of the crystal packing along the a axis. All H atoms are omitted for clarity.
Crystal data
| [Cd2I4(C12H13N5)2] | Z = 1 |
| Mr = 1186.95 | F(000) = 548 |
| Triclinic, P1 | Dx = 2.324 Mg m−3 |
| a = 7.8323 (4) Å | Mo Kα radiation, λ = 0.7107 Å |
| b = 10.0657 (6) Å | Cell parameters from 6849 reflections |
| c = 11.2335 (7) Å | θ = 3.0–26.3° |
| α = 78.849 (5)° | µ = 4.93 mm−1 |
| β = 86.020 (5)° | T = 290 K |
| γ = 77.538 (5)° | Prismatic, colourless |
| V = 848.08 (9) Å3 | 0.25 × 0.21 × 0.15 mm |
Data collection
| Agilent Xcalibur Eos Gemini diffractometer | 3462 independent reflections |
| Radiation source: Enhance (Mo) X-ray Source | 2961 reflections with I > 2σ(I) |
| graphite | Rint = 0.031 |
| Detector resolution: 16.2312 pixels mm-1 | θmax = 26.3°, θmin = 3.0° |
| ω scans | h = −9→9 |
| Absorption correction: gaussian [numerical absorption correction based on Gaussian integration over a multifaceted crystal model (CrysAlis PRO; Agilent, 2010)] | k = −12→12 |
| Tmin = 0.287, Tmax = 0.487 | l = −14→14 |
| 13998 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)] = 0.027 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.061 | H-atom parameters constrained |
| S = 1.08 | w = 1/[σ2(Fo2) + (0.026P)2 + 0.3471P] where P = (Fo2 + 2Fc2)/3 |
| 3462 reflections | (Δ/σ)max = 0.002 |
| 182 parameters | Δρmax = 0.82 e Å−3 |
| 0 restraints | Δρmin = −1.05 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 | 0.49488 (4) | 1.31204 (3) | 0.40337 (2) | 0.04897 (9) | |
| I2 | −0.04748 (4) | 1.42680 (3) | 0.22432 (3) | 0.06153 (11) | |
| Cd1 | 0.27758 (4) | 1.26989 (3) | 0.24333 (2) | 0.03657 (9) | |
| N1 | 0.2561 (4) | 1.0409 (3) | 0.2834 (3) | 0.0385 (7) | |
| N2 | 0.4017 (4) | 0.9559 (3) | 0.2627 (3) | 0.0389 (7) | |
| N3 | 0.3713 (4) | 0.8276 (3) | 0.2862 (3) | 0.0350 (7) | |
| N4 | 0.5058 (4) | 0.7062 (3) | 0.1294 (3) | 0.0354 (7) | |
| N5 | 0.5744 (4) | 0.7249 (3) | −0.0641 (3) | 0.0370 (7) | |
| C1 | 0.2006 (5) | 0.8280 (4) | 0.3244 (3) | 0.0343 (8) | |
| C2 | 0.1274 (5) | 0.9679 (4) | 0.3215 (3) | 0.0356 (8) | |
| C3 | −0.0491 (5) | 1.0113 (4) | 0.3544 (4) | 0.0451 (10) | |
| H3 | −0.1003 | 1.1043 | 0.3512 | 0.054* | |
| C4 | −0.1422 (6) | 0.9082 (5) | 0.3916 (4) | 0.0514 (11) | |
| H4 | −0.2598 | 0.9322 | 0.4139 | 0.062* | |
| C5 | −0.0643 (6) | 0.7676 (5) | 0.3966 (4) | 0.0525 (11) | |
| H5 | −0.1322 | 0.7018 | 0.4236 | 0.063* | |
| C6 | 0.1076 (6) | 0.7234 (4) | 0.3635 (4) | 0.0469 (10) | |
| H6 | 0.1583 | 0.6303 | 0.3670 | 0.056* | |
| C7 | 0.5056 (5) | 0.7136 (4) | 0.2573 (3) | 0.0421 (9) | |
| H7A | 0.4851 | 0.6274 | 0.3059 | 0.051* | |
| H7B | 0.6192 | 0.7258 | 0.2772 | 0.051* | |
| C8 | 0.3756 (5) | 0.6688 (4) | 0.0752 (4) | 0.0432 (9) | |
| H8 | 0.2762 | 0.6414 | 0.1132 | 0.052* | |
| C9 | 0.4206 (5) | 0.6798 (4) | −0.0435 (4) | 0.0440 (9) | |
| H9 | 0.3570 | 0.6598 | −0.1023 | 0.053* | |
| C10 | 0.6246 (5) | 0.7411 (3) | 0.0414 (3) | 0.0330 (8) | |
| C11 | 0.7851 (5) | 0.7927 (4) | 0.0590 (4) | 0.0442 (9) | |
| H11B | 0.8741 | 0.7642 | −0.0007 | 0.053* | |
| H11A | 0.8297 | 0.7494 | 0.1388 | 0.053* | |
| C12 | 0.7549 (6) | 0.9494 (4) | 0.0479 (4) | 0.0564 (11) | |
| H12B | 0.7143 | 0.9933 | −0.0316 | 0.085* | |
| H12C | 0.8626 | 0.9748 | 0.0607 | 0.085* | |
| H12A | 0.6687 | 0.9786 | 0.1078 | 0.085* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| I1 | 0.04834 (17) | 0.06438 (19) | 0.03873 (15) | −0.02051 (14) | −0.00434 (12) | −0.00950 (13) |
| I2 | 0.04034 (16) | 0.04634 (17) | 0.0956 (3) | −0.00025 (13) | −0.00964 (16) | −0.01437 (16) |
| Cd1 | 0.03734 (16) | 0.03522 (15) | 0.03821 (16) | −0.00826 (12) | 0.00067 (12) | −0.00907 (12) |
| N1 | 0.0398 (18) | 0.0340 (17) | 0.0428 (18) | −0.0096 (14) | 0.0045 (15) | −0.0097 (14) |
| N2 | 0.0433 (18) | 0.0328 (17) | 0.0398 (17) | −0.0086 (14) | 0.0052 (15) | −0.0065 (14) |
| N3 | 0.0410 (17) | 0.0326 (16) | 0.0298 (15) | −0.0068 (14) | 0.0026 (13) | −0.0037 (12) |
| N4 | 0.0390 (17) | 0.0341 (16) | 0.0343 (16) | −0.0070 (14) | 0.0003 (14) | −0.0103 (13) |
| N5 | 0.0422 (18) | 0.0361 (17) | 0.0344 (17) | −0.0120 (14) | 0.0013 (14) | −0.0074 (13) |
| C1 | 0.039 (2) | 0.038 (2) | 0.0278 (18) | −0.0134 (17) | −0.0008 (16) | −0.0064 (15) |
| C2 | 0.039 (2) | 0.040 (2) | 0.0297 (18) | −0.0114 (17) | 0.0007 (16) | −0.0074 (16) |
| C3 | 0.040 (2) | 0.050 (2) | 0.047 (2) | −0.0078 (19) | 0.0020 (19) | −0.0138 (19) |
| C4 | 0.038 (2) | 0.071 (3) | 0.049 (2) | −0.019 (2) | 0.0026 (19) | −0.015 (2) |
| C5 | 0.053 (3) | 0.061 (3) | 0.053 (3) | −0.036 (2) | 0.004 (2) | −0.007 (2) |
| C6 | 0.058 (3) | 0.042 (2) | 0.045 (2) | −0.020 (2) | 0.003 (2) | −0.0083 (18) |
| C7 | 0.046 (2) | 0.038 (2) | 0.038 (2) | 0.0005 (18) | −0.0032 (18) | −0.0041 (17) |
| C8 | 0.042 (2) | 0.042 (2) | 0.050 (2) | −0.0147 (18) | 0.0083 (19) | −0.0142 (19) |
| C9 | 0.044 (2) | 0.047 (2) | 0.049 (2) | −0.0176 (19) | 0.0011 (19) | −0.0195 (19) |
| C10 | 0.0353 (19) | 0.0265 (17) | 0.037 (2) | −0.0068 (15) | 0.0012 (16) | −0.0058 (15) |
| C11 | 0.039 (2) | 0.051 (2) | 0.046 (2) | −0.0116 (19) | −0.0028 (18) | −0.0127 (19) |
| C12 | 0.055 (3) | 0.059 (3) | 0.062 (3) | −0.028 (2) | −0.001 (2) | −0.011 (2) |
Geometric parameters (Å, °)
| I1—Cd1 | 2.7094 (4) | C3—C4 | 1.379 (6) |
| I2—Cd1 | 2.6892 (4) | C4—H4 | 0.9300 |
| Cd1—N1 | 2.302 (3) | C4—C5 | 1.406 (6) |
| Cd1—N5i | 2.250 (3) | C5—H5 | 0.9300 |
| N1—N2 | 1.306 (4) | C5—C6 | 1.373 (6) |
| N1—C2 | 1.371 (5) | C6—H6 | 0.9300 |
| N2—N3 | 1.337 (4) | C7—H7A | 0.9700 |
| N3—C1 | 1.375 (5) | C7—H7B | 0.9700 |
| N3—C7 | 1.451 (5) | C8—H8 | 0.9300 |
| N4—C7 | 1.452 (5) | C8—C9 | 1.345 (5) |
| N4—C8 | 1.376 (5) | C9—H9 | 0.9300 |
| N4—C10 | 1.359 (5) | C10—C11 | 1.499 (5) |
| N5—Cd1i | 2.250 (3) | C11—H11B | 0.9700 |
| N5—C9 | 1.367 (5) | C11—H11A | 0.9700 |
| N5—C10 | 1.323 (4) | C11—C12 | 1.525 (6) |
| C1—C2 | 1.396 (5) | C12—H12B | 0.9600 |
| C1—C6 | 1.393 (5) | C12—H12C | 0.9600 |
| C2—C3 | 1.403 (5) | C12—H12A | 0.9600 |
| C3—H3 | 0.9300 | ||
| I2—Cd1—I1 | 118.809 (14) | C4—C3—C2 | 116.1 (4) |
| N1—Cd1—I1 | 109.18 (8) | C4—C3—H3 | 121.9 |
| N1—Cd1—I2 | 108.30 (8) | C4—C5—H5 | 118.6 |
| N1—N2—N3 | 107.9 (3) | C5—C4—H4 | 119.1 |
| N1—C2—C1 | 107.6 (3) | C5—C6—C1 | 115.2 (4) |
| N1—C2—C3 | 131.4 (4) | C5—C6—H6 | 122.4 |
| N2—N1—Cd1 | 113.7 (2) | C6—C1—C2 | 123.0 (4) |
| N2—N1—C2 | 109.7 (3) | C6—C5—C4 | 122.8 (4) |
| N2—N3—C1 | 111.1 (3) | C6—C5—H5 | 118.6 |
| N2—N3—C7 | 119.6 (3) | H7A—C7—H7B | 108.0 |
| N3—C1—C2 | 103.7 (3) | C8—N4—C7 | 124.5 (3) |
| N3—C1—C6 | 133.2 (4) | C8—C9—N5 | 109.3 (4) |
| N3—C7—N4 | 110.9 (3) | C8—C9—H9 | 125.4 |
| N3—C7—H7A | 109.5 | C9—N5—Cd1i | 122.4 (3) |
| N3—C7—H7B | 109.5 | C9—C8—N4 | 106.4 (4) |
| N4—C7—H7A | 109.5 | C9—C8—H8 | 126.8 |
| N4—C7—H7B | 109.5 | C10—N4—C7 | 127.6 (3) |
| N4—C8—H8 | 126.8 | C10—N4—C8 | 107.8 (3) |
| N4—C10—C11 | 126.0 (3) | C10—N5—Cd1i | 129.4 (3) |
| N5i—Cd1—I1 | 106.59 (8) | C10—N5—C9 | 107.5 (3) |
| N5i—Cd1—I2 | 112.86 (8) | C10—C11—H11B | 108.7 |
| N5i—Cd1—N1 | 99.31 (11) | C10—C11—H11A | 108.7 |
| N5—C9—H9 | 125.4 | C10—C11—C12 | 114.1 (3) |
| N5—C10—N4 | 109.1 (3) | C11—C12—H12B | 109.5 |
| N5—C10—C11 | 124.9 (3) | C11—C12—H12C | 109.5 |
| C1—N3—C7 | 128.9 (3) | C11—C12—H12A | 109.5 |
| C1—C2—C3 | 121.0 (4) | H11B—C11—H11A | 107.6 |
| C1—C6—H6 | 122.4 | C12—C11—H11B | 108.7 |
| C2—N1—Cd1 | 136.6 (2) | C12—C11—H11A | 108.7 |
| C2—C3—H3 | 121.9 | H12B—C12—H12C | 109.5 |
| C3—C4—H4 | 119.1 | H12B—C12—H12A | 109.5 |
| C3—C4—C5 | 121.9 (4) | H12C—C12—H12A | 109.5 |
| I1—Cd1—N1—N2 | −66.6 (2) | N5i—Cd1—N1—C2 | −133.4 (4) |
| I1—Cd1—N1—C2 | 115.3 (3) | N5—C10—C11—C12 | 90.2 (5) |
| I2—Cd1—N1—N2 | 162.7 (2) | C1—N3—C7—N4 | 90.9 (4) |
| I2—Cd1—N1—C2 | −15.4 (4) | C1—C2—C3—C4 | 1.4 (6) |
| Cd1—N1—N2—N3 | −178.4 (2) | C2—N1—N2—N3 | 0.2 (4) |
| Cd1—N1—C2—C1 | 178.3 (3) | C2—C1—C6—C5 | 1.6 (6) |
| Cd1—N1—C2—C3 | −1.7 (6) | C2—C3—C4—C5 | 0.2 (6) |
| Cd1i—N5—C9—C8 | 171.0 (2) | C3—C4—C5—C6 | −1.0 (7) |
| Cd1i—N5—C10—N4 | −169.5 (2) | C4—C5—C6—C1 | 0.1 (6) |
| Cd1i—N5—C10—C11 | 11.7 (5) | C6—C1—C2—N1 | 177.6 (3) |
| N1—N2—N3—C1 | −0.5 (4) | C6—C1—C2—C3 | −2.4 (6) |
| N1—N2—N3—C7 | 172.9 (3) | C7—N3—C1—C2 | −172.0 (3) |
| N1—C2—C3—C4 | −178.6 (4) | C7—N3—C1—C6 | 10.3 (7) |
| N2—N1—C2—C1 | 0.1 (4) | C7—N4—C8—C9 | 177.7 (3) |
| N2—N1—C2—C3 | −179.9 (4) | C7—N4—C10—N5 | −177.4 (3) |
| N2—N3—C1—C2 | 0.5 (4) | C7—N4—C10—C11 | 1.3 (6) |
| N2—N3—C1—C6 | −177.1 (4) | C8—N4—C7—N3 | −69.3 (5) |
| N2—N3—C7—N4 | −81.1 (4) | C8—N4—C10—N5 | −0.9 (4) |
| N3—C1—C2—N1 | −0.4 (4) | C8—N4—C10—C11 | 177.9 (3) |
| N3—C1—C2—C3 | 179.6 (3) | C9—N5—C10—N4 | 0.4 (4) |
| N3—C1—C6—C5 | 178.9 (4) | C9—N5—C10—C11 | −178.4 (3) |
| N4—C8—C9—N5 | −0.8 (4) | C10—N4—C7—N3 | 106.8 (4) |
| N4—C10—C11—C12 | −88.4 (5) | C10—N4—C8—C9 | 1.0 (4) |
| N5i—Cd1—N1—N2 | 44.7 (3) | C10—N5—C9—C8 | 0.3 (4) |
Symmetry codes: (i) −x+1, −y+2, −z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ZQ2107).
References
- Agilent (2010). CrysAlis PRO Agilent Technologies, Yarnton, Oxfordshire, England.
- Dolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339–341.
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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 datablock(s) global, I. DOI: 10.1107/S1600536811021179/zq2107sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021179/zq2107Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


