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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Jun 11;67(Pt 7):m882. doi: 10.1107/S1600536811021179

Bis{μ-1-[(2-ethyl-1H-imidazol-1-yl)meth­yl]-1H-benzotriazole}bis­(iodido­cadmium)

Xia Wang a,*, Jun-long Niu b
PMCID: PMC3152091  PMID: 21836875

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).graphic file with name e-67-0m882-scheme1.jpg

Experimental

Crystal data

  • [Cd2I4(C12H13N5)2]

  • M r = 1186.95

  • Triclinic, Inline graphic

  • 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

e-67-0m882-sup1.cif (18.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021179/zq2107Isup2.hkl

e-67-0m882-Isup2.hkl (169.8KB, 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.

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.

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 m3
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 mm1
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 Å3
0 restraints Δρmin = −1.05 e Å3

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

  1. Agilent (2010). CrysAlis PRO Agilent Technologies, Yarnton, Oxfordshire, England.
  2. Dolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339–341.
  3. Huang, M.-H., Liu, P., Wang, J., Chen, Y. & Liu, Q.-Y. (2006). Inorg. Chem. Commun. 9, 952–954.
  4. Meng, X.-R., Jin, S.-Z., Hou, H.-W., Du, C.-X. & Ng, S. W. (2009). Inorg. Chim. Acta, 362, 1519–1527.
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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

e-67-0m882-sup1.cif (18.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811021179/zq2107Isup2.hkl

e-67-0m882-Isup2.hkl (169.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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