Abstract
The TeIV atom in the title compound, [Te(C4H9)(C8H10Br)Cl2] or C12H19BrCl2Te, is in a distorted ψ-trigonal–bipyramidal geometry, with the lone pair of electrons projected to occupy a position in the equatorial plane, and with the Cl atoms being mutually trans [172.48 (4)°]. Close intramolecular [Te⋯Br = 3.3444 (18) Å] and intermolecular [Te⋯Cl = 3.675 (3) Å] interactions are observed. The latter lead to centrosymmetric dimers which assemble into layers in the bc plane. The primary connections between layers are of the type C—H⋯Cl.
Related literature
For background to the synthesis, see: Guadagnin et al. (2008 ▶). For related X-ray structures, see: Zukerman-Schpector et al. (1998 ▶, 2008 ▶). For coordination polyhedra around TeIV atoms, see: Zukerman-Schpector & Haiduc (2002 ▶); Tiekink & Zukerman-Schpector (2010 ▶). For ring conformational analysis, see: Cremer & Pople (1975 ▶).
Experimental
Crystal data
C12H19BrCl2Te
M r = 441.67
Triclinic,
a = 6.311 (3) Å
b = 10.243 (6) Å
c = 12.334 (9) Å
α = 103.34 (2)°
β = 91.53 (2)°
γ = 91.411 (14)°
V = 775.1 (8) Å3
Z = 2
Mo Kα radiation
μ = 4.82 mm−1
T = 98 K
0.22 × 0.20 × 0.15 mm
Data collection
Rigaku Saturn724 diffractometer
Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.360, T max = 0.486
7151 measured reflections
3012 independent reflections
2898 reflections with I > 2σ(I)
R int = 0.033
Refinement
R[F 2 > 2σ(F 2)] = 0.032
wR(F 2) = 0.086
S = 1.12
3012 reflections
146 parameters
H-atom parameters constrained
Δρmax = 0.89 e Å−3
Δρmin = −0.59 e Å−3
Data collection: CrystalClear (Molecular Structure Corporation & Rigaku, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SIR97 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶) and DIAMOND (Brandenburg, 2006 ▶); software used to prepare material for publication: MarvinSketch (Chemaxon, 2010 ▶) and publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811023142/hg5055sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811023142/hg5055Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811023142/hg5055Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Selected geometric parameters (Å, °).
| Te—Cl1 | 2.5381 (15) |
| Te—Cl2 | 2.4859 (15) |
| Te—C1 | 2.092 (4) |
| Te—C3 | 2.143 (4) |
| Cl1—Te—Cl2 | 172.48 (4) |
Table 2. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C3—H3a⋯Cl2i | 0.97 | 2.80 | 3.576 (5) | 138 |
Symmetry code: (i)
.
Acknowledgments
We thank the Brazilian agencies FAPESP (07/59404–2 to HAS), CNPq (306532/2009–3 to JZ-S, 308116/2010–0 to IC) and CAPES (808/2009 to JZ-S and IC) for financial support.
supplementary crystallographic information
Comment
The title compound, (I), was synthesized using a palladium-catalyzed cross-coupling reaction of a potassium aryltrifluoroborate salt with various (Z)-2-chloro vinylic tellurides (Guadagnin et al., 2008). Complementing these studies are crystallographic studies (Zukerman-Schpector et al. 1998; Zukerman-Schpector et al., 2008) focused upon determining coordination polyhedra and supramolecular aggregation patterns (Zukerman-Schpector & Haiduc, 2002; Tiekink & Zukerman-Schpector, 2010) which lead to the crystallographic characterization of (I).
The immediate coordination geometry about the TeIV atom in (I) is defined by two Cl atoms and two C atoms which, along with a stereochemically active lone pair of electrons, define a ψ-trigonal bi-pyramidal geometry, Table 1. In this description the lone pair is assumed to occupy a position in the equatorial plane, and the Cl atoms to be mutually trans. Additional Te···X interactions are evident and contribute to the distortion of the coordination geometry. Thus, an intramolecular Te···Br interaction [3.3444 (18) Å] is noted. In addition, there is an intermolecular Te···Cl contact [Te···Cl1i = 3.675 (3) Å, symmetry operation i: 1 - x, 1 - y, 1 - z]. The latter interaction explains the elongation of the Te—Cl1 bond compared to the Te—Cl2 bond, Table 1. Within the substituted ligand, the configuration about the C1═C2 bond [1.327 (6) Å] is Z. The cyclohexene ring adopts a half-chair conformation with puckering parameters: q2 = 0.364 (5) Å and q3 = -0.278 (5) Å, and amplitudes: Q = 0.458 (6) Å, θ = 127.4 (6) ° and φ2 = 30.2 (8) ° (Cremer & Pople, 1975).
The most prominent feature of the crystal packing are the aforementioned Te···Cl1 interactions. These lead to centrosymmetric dimers that assemble into chains along the b axis. These partially inter-digitate along the c axis. The layers thus formed in the bc plane, Fig. 2, are connected via C—H···Cl interactions, Table 2, along the a axis, Fig. 3.
Experimental
The starting (Z)-(2-bromo-2-cyclohexenylvinyl)(butyl)tellane was prepared as described in previous work (Guadagnin et al., 2008) and a solution of it (1 mmol, 0.370 g) in hexane (5 ml) at 273 K was poured into a two-necked round-bottomed flask under a nitrogen atmosphere and then SO2Cl2 (1 mmol, 1.37 g) added drop wise. A white solid formed immediately. The mixture was warmed to room temperature. The resulting solid was filtered and dried. Crystals of (I) were obatined by slow evaporation from its CHCl3 solution held at room temperature.
Refinement
C-bound H-atoms were placed in calculated positions (C—H 0.93–0.97 Å) and were included in the refinement in the riding model approximation with Uiso(H) set to 1.2–1.5Ueq(C).
Figures
Fig. 1.
Molecular structure of (I) showing atom-labelling scheme and displacement ellipsoids at the 50% probability level.
Fig. 2.
A view of the assembly of centrosymmetric molecules in the bc plane in (I). The intermolecular Te···Cl interactions are indicated by dashed lines.
Fig. 3.
Unit-cell contents in (I) viewed in projection down the b axis showing C—H···Cl interactions (orange dashed lines) occurring between the layers shown in Fig. 2.
Crystal data
| C12H19BrCl2Te | Z = 2 |
| Mr = 441.67 | F(000) = 424 |
| Triclinic, P1 | Dx = 1.893 Mg m−3 |
| Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
| a = 6.311 (3) Å | Cell parameters from 2823 reflections |
| b = 10.243 (6) Å | θ = 2.3–30.3° |
| c = 12.334 (9) Å | µ = 4.82 mm−1 |
| α = 103.34 (2)° | T = 98 K |
| β = 91.53 (2)° | Block, colourless |
| γ = 91.411 (14)° | 0.22 × 0.20 × 0.15 mm |
| V = 775.1 (8) Å3 |
Data collection
| Rigaku Saturn724 diffractometer | 3012 independent reflections |
| Radiation source: fine-focus sealed tube | 2898 reflections with I > 2σ(I) |
| graphite | Rint = 0.033 |
| Detector resolution: 28.5714 pixels mm-1 | θmax = 26.0°, θmin = 3.0° |
| dtprofit.ref scans | h = −7→7 |
| Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | k = −12→12 |
| Tmin = 0.360, Tmax = 0.486 | l = −15→14 |
| 7151 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)] = 0.032 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.086 | H-atom parameters constrained |
| S = 1.12 | w = 1/[σ2(Fo2) + (0.0328P)2 + 2.7479P] where P = (Fo2 + 2Fc2)/3 |
| 3012 reflections | (Δ/σ)max < 0.001 |
| 146 parameters | Δρmax = 0.89 e Å−3 |
| 0 restraints | Δρmin = −0.59 e Å−3 |
Special details
| Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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 | ||
| Te | 0.54785 (4) | 0.72646 (3) | 0.54317 (2) | 0.02297 (11) | |
| Cl1 | 0.28881 (18) | 0.59324 (11) | 0.63286 (10) | 0.0303 (2) | |
| Cl2 | 0.76717 (17) | 0.88070 (11) | 0.46001 (9) | 0.0270 (2) | |
| Br | 0.88870 (7) | 0.84752 (4) | 0.75713 (4) | 0.02781 (13) | |
| C1 | 0.4888 (7) | 0.8911 (4) | 0.6734 (4) | 0.0243 (9) | |
| H1 | 0.3606 | 0.9336 | 0.6721 | 0.029* | |
| C2 | 0.6258 (6) | 0.9377 (4) | 0.7578 (4) | 0.0210 (8) | |
| C3 | 0.2891 (7) | 0.7512 (5) | 0.4343 (4) | 0.0272 (10) | |
| H3A | 0.1601 | 0.7647 | 0.4760 | 0.033* | |
| H3B | 0.3167 | 0.8303 | 0.4056 | 0.033* | |
| C4 | 0.2579 (7) | 0.6278 (4) | 0.3363 (4) | 0.0254 (9) | |
| H4A | 0.3884 | 0.6127 | 0.2960 | 0.031* | |
| H4B | 0.2263 | 0.5491 | 0.3649 | 0.031* | |
| C5 | 0.0798 (7) | 0.6463 (5) | 0.2574 (4) | 0.0275 (9) | |
| H5A | 0.1144 | 0.7224 | 0.2260 | 0.033* | |
| H5B | −0.0492 | 0.6655 | 0.2983 | 0.033* | |
| C6 | 0.0426 (8) | 0.5215 (5) | 0.1634 (4) | 0.0327 (11) | |
| H6A | 0.1697 | 0.5029 | 0.1223 | 0.049* | |
| H6B | −0.0705 | 0.5363 | 0.1145 | 0.049* | |
| H6C | 0.0051 | 0.4465 | 0.1942 | 0.049* | |
| C7 | 0.5937 (7) | 1.0547 (4) | 0.8505 (4) | 0.0218 (9) | |
| C8 | 0.7386 (8) | 1.0984 (5) | 0.9333 (4) | 0.0278 (10) | |
| H8 | 0.8617 | 1.0502 | 0.9330 | 0.033* | |
| C9 | 0.7148 (8) | 1.2201 (5) | 1.0265 (4) | 0.0339 (11) | |
| H9A | 0.8450 | 1.2744 | 1.0361 | 0.041* | |
| H9B | 0.6925 | 1.1917 | 1.0952 | 0.041* | |
| C10 | 0.5313 (8) | 1.3048 (5) | 1.0050 (5) | 0.0390 (12) | |
| H10A | 0.4959 | 1.3655 | 1.0744 | 0.047* | |
| H10B | 0.5742 | 1.3585 | 0.9536 | 0.047* | |
| C11 | 0.3404 (8) | 1.2207 (5) | 0.9576 (4) | 0.0358 (11) | |
| H11A | 0.2274 | 1.2786 | 0.9452 | 0.043* | |
| H11B | 0.2927 | 1.1710 | 1.0110 | 0.043* | |
| C12 | 0.3841 (7) | 1.1224 (5) | 0.8482 (4) | 0.0280 (10) | |
| H12A | 0.2710 | 1.0542 | 0.8316 | 0.034* | |
| H12B | 0.3833 | 1.1700 | 0.7888 | 0.034* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Te | 0.02153 (17) | 0.01990 (16) | 0.02365 (17) | 0.00270 (11) | −0.00238 (11) | −0.00268 (11) |
| Cl1 | 0.0311 (6) | 0.0213 (5) | 0.0360 (6) | −0.0017 (4) | 0.0052 (5) | 0.0010 (4) |
| Cl2 | 0.0254 (5) | 0.0286 (5) | 0.0260 (5) | 0.0036 (4) | 0.0036 (4) | 0.0034 (4) |
| Br | 0.0224 (2) | 0.0283 (2) | 0.0286 (2) | 0.00692 (18) | −0.00469 (18) | −0.00199 (18) |
| C1 | 0.023 (2) | 0.023 (2) | 0.025 (2) | 0.0068 (17) | 0.0015 (17) | −0.0014 (17) |
| C2 | 0.0174 (19) | 0.0191 (19) | 0.026 (2) | 0.0021 (16) | 0.0012 (16) | 0.0042 (17) |
| C3 | 0.023 (2) | 0.024 (2) | 0.030 (2) | 0.0023 (17) | −0.0078 (18) | −0.0023 (19) |
| C4 | 0.032 (2) | 0.021 (2) | 0.021 (2) | 0.0082 (18) | −0.0013 (18) | 0.0000 (17) |
| C5 | 0.031 (2) | 0.024 (2) | 0.025 (2) | 0.0000 (18) | −0.0044 (18) | 0.0004 (18) |
| C6 | 0.042 (3) | 0.028 (2) | 0.025 (2) | 0.000 (2) | −0.004 (2) | 0.0016 (19) |
| C7 | 0.026 (2) | 0.0157 (19) | 0.024 (2) | −0.0026 (16) | 0.0001 (17) | 0.0042 (16) |
| C8 | 0.028 (2) | 0.025 (2) | 0.028 (2) | 0.0017 (18) | −0.0027 (19) | 0.0029 (19) |
| C9 | 0.031 (3) | 0.033 (3) | 0.030 (2) | 0.000 (2) | −0.003 (2) | −0.009 (2) |
| C10 | 0.040 (3) | 0.032 (3) | 0.037 (3) | 0.005 (2) | 0.000 (2) | −0.008 (2) |
| C11 | 0.034 (3) | 0.034 (3) | 0.034 (3) | 0.010 (2) | 0.000 (2) | −0.001 (2) |
| C12 | 0.026 (2) | 0.027 (2) | 0.027 (2) | 0.0040 (18) | −0.0047 (18) | 0.0000 (19) |
Geometric parameters (Å, °)
| Te—Cl1 | 2.5381 (15) | C6—H6B | 0.9600 |
| Te—Cl2 | 2.4859 (15) | C6—H6C | 0.9600 |
| Te—C1 | 2.092 (4) | C7—C8 | 1.341 (6) |
| Te—C3 | 2.143 (4) | C7—C12 | 1.511 (6) |
| Br—C2 | 1.918 (4) | C8—C9 | 1.502 (6) |
| C1—C2 | 1.327 (6) | C8—H8 | 0.9300 |
| C1—H1 | 0.9300 | C9—C10 | 1.518 (7) |
| C2—C7 | 1.475 (6) | C9—H9A | 0.9700 |
| C3—C4 | 1.539 (6) | C9—H9B | 0.9700 |
| C3—H3A | 0.9700 | C10—C11 | 1.488 (7) |
| C3—H3B | 0.9700 | C10—H10A | 0.9700 |
| C4—C5 | 1.511 (6) | C10—H10B | 0.9700 |
| C4—H4A | 0.9700 | C11—C12 | 1.522 (7) |
| C4—H4B | 0.9700 | C11—H11A | 0.9700 |
| C5—C6 | 1.524 (6) | C11—H11B | 0.9700 |
| C5—H5A | 0.9700 | C12—H12A | 0.9700 |
| C5—H5B | 0.9700 | C12—H12B | 0.9700 |
| C6—H6A | 0.9600 | ||
| C1—Te—C3 | 97.25 (17) | H6A—C6—H6C | 109.5 |
| C1—Te—Cl2 | 87.77 (14) | H6B—C6—H6C | 109.5 |
| C3—Te—Cl2 | 88.63 (14) | C8—C7—C2 | 122.8 (4) |
| C1—Te—Cl1 | 86.80 (14) | C8—C7—C12 | 121.3 (4) |
| Cl1—Te—Cl2 | 172.48 (4) | C2—C7—C12 | 115.9 (4) |
| C2—C1—Te | 123.1 (3) | C7—C8—C9 | 124.2 (4) |
| C2—C1—H1 | 118.5 | C7—C8—H8 | 117.9 |
| Te—C1—H1 | 118.5 | C9—C8—H8 | 117.9 |
| C1—C2—C7 | 125.3 (4) | C8—C9—C10 | 112.4 (4) |
| C1—C2—Br | 117.1 (3) | C8—C9—H9A | 109.1 |
| C7—C2—Br | 117.6 (3) | C10—C9—H9A | 109.1 |
| C4—C3—Te | 111.2 (3) | C8—C9—H9B | 109.1 |
| C4—C3—H3A | 109.4 | C10—C9—H9B | 109.1 |
| Te—C3—H3A | 109.4 | H9A—C9—H9B | 107.9 |
| C4—C3—H3B | 109.4 | C11—C10—C9 | 111.9 (4) |
| Te—C3—H3B | 109.4 | C11—C10—H10A | 109.2 |
| H3A—C3—H3B | 108.0 | C9—C10—H10A | 109.2 |
| C5—C4—C3 | 111.5 (4) | C11—C10—H10B | 109.2 |
| C5—C4—H4A | 109.3 | C9—C10—H10B | 109.2 |
| C3—C4—H4A | 109.3 | H10A—C10—H10B | 107.9 |
| C5—C4—H4B | 109.3 | C10—C11—C12 | 112.2 (4) |
| C3—C4—H4B | 109.3 | C10—C11—H11A | 109.2 |
| H4A—C4—H4B | 108.0 | C12—C11—H11A | 109.2 |
| C4—C5—C6 | 111.3 (4) | C10—C11—H11B | 109.2 |
| C4—C5—H5A | 109.4 | C12—C11—H11B | 109.2 |
| C6—C5—H5A | 109.4 | H11A—C11—H11B | 107.9 |
| C4—C5—H5B | 109.4 | C7—C12—C11 | 113.1 (4) |
| C6—C5—H5B | 109.4 | C7—C12—H12A | 109.0 |
| H5A—C5—H5B | 108.0 | C11—C12—H12A | 109.0 |
| C5—C6—H6A | 109.5 | C7—C12—H12B | 109.0 |
| C5—C6—H6B | 109.5 | C11—C12—H12B | 109.0 |
| H6A—C6—H6B | 109.5 | H12A—C12—H12B | 107.8 |
| C5—C6—H6C | 109.5 | ||
| C3—Te—C1—C2 | −168.3 (4) | Br—C2—C7—C8 | −0.7 (6) |
| Cl2—Te—C1—C2 | −80.0 (4) | C1—C2—C7—C12 | 1.7 (6) |
| Cl1—Te—C1—C2 | 105.2 (4) | Br—C2—C7—C12 | −179.7 (3) |
| Te—C1—C2—C7 | 178.8 (3) | C2—C7—C8—C9 | 177.6 (4) |
| Te—C1—C2—Br | 0.2 (5) | C12—C7—C8—C9 | −3.5 (7) |
| C1—Te—C3—C4 | −168.9 (3) | C7—C8—C9—C10 | −11.7 (7) |
| Cl2—Te—C3—C4 | 103.5 (3) | C8—C9—C10—C11 | 42.3 (6) |
| Cl1—Te—C3—C4 | −82.6 (3) | C9—C10—C11—C12 | −58.9 (6) |
| Te—C3—C4—C5 | −178.3 (3) | C8—C7—C12—C11 | −12.0 (6) |
| C3—C4—C5—C6 | −177.4 (4) | C2—C7—C12—C11 | 167.0 (4) |
| C1—C2—C7—C8 | −179.3 (5) | C10—C11—C12—C7 | 42.8 (6) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C3—H3a···Cl2i | 0.97 | 2.80 | 3.576 (5) | 138 |
Symmetry codes: (i) x−1, y, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG5055).
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 datablock(s) I, global. DOI: 10.1107/S1600536811023142/hg5055sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811023142/hg5055Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536811023142/hg5055Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



