organic compounds
1,2,4,5-Tetrachloro-3,6-diiodobenzene benzene monosolvate
aDepartment of Chemistry, Missouri State University, 901 South National Avenue, Springfield MO 65804 , USA
*Correspondence e-mail: ericbosch@missouristate.edu
The title compound, C6Cl4I2·C6H6, crystallizes from benzene solution as cube-shaped crystals in the triclinic P with Z = 1. The of the contains one half of each molecule. In the crystal, the benzene ring is almost orthogonal to the perhalobenzene ring and the molecules are linked by C—I⋯π interactions, with a close contact between the iodine atom and the benzene ring of 3.412 (1) Å.
Keywords: crystal structure; solvate; C—I⋯π interactions.
CCDC reference: 1940085
Structure description
Halogen bonding, the attractive interaction between the electropositive σ-hole on a bonded halogen, commonly iodine, and a has been widely used in the supramolecular association of multi-component systems (Cavallo et al., 2016). With respect to iodobenzene, it has been established that the addition of fluorine atoms to the benzene ring enhances the σ-hole on iodine resulting in stronger attractions between the components (Präsang et al., 2009). Surprisingly, the application of iodoperchlorobenzenes had not been reported until we reported that the co-crystallization of 1,2,4,5-tetrachloro-3,6-diiodobenzene with 1,2-dipyridylethene resulted in a halogen-bonded in which the were oriented such that they underwent photo-induced 2 + 2 cycloaddition (Bosch et al., 2019). After preparation of 1,2,4,5-tetrachloro-3,6-diiodobenzene, recrystallization from benzene provided clear, colourless cube-shaped crystals that lost lustre and became opaque several hours after removal from the mother liquor. The revealed that the cube-shaped crystals represented a 1:1 benzene solvate.
The . The closest contact between the tetrachlorodiiodobenzene and the benzene is between the iodine atom and C4 with a distance of 3.434 (2) Å. Indeed the C1—I1⋯C4 bond angle is almost linear at 178.09 (6)°. This interaction is highlighted in the two Hirshfeld surface plots in Fig. 2 (Turner et al., 2017). The C—I⋯π interactions form a stepped chain of alternating tetrachlorodiiodobenzene and benzene molecules (Fig. 3) with adjacent tetrachlorodiiodobenzene molecules slip-stacked with a centroid–centroid distance of 5.4399 (10) Å and perpendicular distance between the perhalobenzene planes of 3.6607 (7) Å (Spek, 2015).
comprises one half of the tetrachlorodiodobenzene and one half of the benzene molecule with a dihedral angle between the rings of 85.89 (16)°, as shown in Fig. 1Synthesis and crystallization
1,2,4,5-Tetrachloro-3,6-diiodobenzene was prepared by the reaction of 1,2,4,5-tetrachlorobenzene with iodine and sodium metaperiodate in concentrated sulfuric acid. Cube-shaped crystals of the title solvate were obtained on recrystallization from benzene solution. Crystallization from mesitylene, chloroform or dichloromethane yielded block-shaped crystals with structures similar to that previously reported (Reddy et al., 2006).
Refinement
Crystal data, data collection and structure .
details are summarized in Table 1Structural data
CCDC reference: 1940085
https://doi.org/10.1107/S2414314619009933/zl4031sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314619009933/zl4031Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2414314619009933/zl4031Isup3.cdx
Supporting information file. DOI: https://doi.org/10.1107/S2414314619009933/zl4031Isup4.cml
Data collection: SMART (Bruker, 2014); cell
SMART (Bruker, 2014); data reduction: SAINT (Bruker, 2014); program(s) used to solve structure: SHELXT2018 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2018 (Sheldrick, 2015b); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: X-SEED (Barbour, 2001).C6Cl4I2·C6H6 | Z = 1 |
Mr = 545.77 | F(000) = 252 |
Triclinic, P1 | Dx = 2.425 Mg m−3 |
a = 5.4399 (4) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 6.3599 (4) Å | Cell parameters from 4302 reflections |
c = 11.0232 (8) Å | θ = 3.3–27.3° |
α = 96.702 (1)° | µ = 4.90 mm−1 |
β = 92.728 (1)° | T = 100 K |
γ = 98.599 (1)° | Cut cube, colourless |
V = 373.69 (5) Å3 | 0.39 × 0.12 × 0.05 mm |
Bruker APEXII CCD diffractometer | 1668 independent reflections |
Radiation source: fine-focus sealed tube | 1634 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.018 |
Detector resolution: 8.3660 pixels mm-1 | θmax = 27.3°, θmin = 1.9° |
phi and ω scans | h = −7→7 |
Absorption correction: multi-scan (SADABS; Bruker, 2014) | k = −8→8 |
Tmin = 0.611, Tmax = 1.000 | l = −14→14 |
4913 measured reflections |
Refinement on F2 | Primary atom site location: dual |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.013 | H-atom parameters constrained |
wR(F2) = 0.032 | w = 1/[σ2(Fo2) + (0.0129P)2 + 0.2107P] where P = (Fo2 + 2Fc2)/3 |
S = 1.09 | (Δ/σ)max = 0.001 |
1668 reflections | Δρmax = 0.46 e Å−3 |
82 parameters | Δρmin = −0.39 e Å−3 |
0 restraints |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
x | y | z | Uiso*/Ueq | ||
I1 | 0.63204 (2) | 0.24241 (2) | 0.70975 (2) | 0.01586 (5) | |
Cl1 | 0.70962 (8) | 0.35540 (7) | 0.42245 (4) | 0.01743 (9) | |
C1 | 0.8497 (3) | 0.0970 (3) | 0.58350 (15) | 0.0125 (3) | |
Cl2 | 1.04287 (8) | 0.14760 (7) | 0.24148 (4) | 0.01843 (9) | |
C2 | 0.8716 (3) | 0.1608 (3) | 0.46708 (16) | 0.0130 (3) | |
C3 | 1.0207 (3) | 0.0648 (3) | 0.38431 (16) | 0.0127 (3) | |
C4 | 0.2926 (4) | 0.4936 (3) | 0.92088 (17) | 0.0220 (4) | |
H4 | 0.150280 | 0.488464 | 0.866558 | 0.026* | |
C5 | 0.4738 (4) | 0.6732 (3) | 0.93667 (18) | 0.0216 (4) | |
H5 | 0.455940 | 0.791629 | 0.893655 | 0.026* | |
C6 | 0.6826 (4) | 0.6801 (3) | 1.01573 (18) | 0.0217 (4) | |
H6 | 0.808105 | 0.803023 | 1.026540 | 0.026* |
U11 | U22 | U33 | U12 | U13 | U23 | |
I1 | 0.01473 (7) | 0.01688 (7) | 0.01605 (7) | 0.00549 (4) | 0.00276 (4) | −0.00209 (4) |
Cl1 | 0.0194 (2) | 0.01586 (19) | 0.0194 (2) | 0.00981 (16) | 0.00007 (16) | 0.00377 (15) |
C1 | 0.0112 (7) | 0.0113 (7) | 0.0143 (8) | 0.0021 (6) | 0.0016 (6) | −0.0017 (6) |
Cl2 | 0.0233 (2) | 0.0205 (2) | 0.0141 (2) | 0.00780 (16) | 0.00371 (16) | 0.00617 (16) |
C2 | 0.0122 (7) | 0.0100 (7) | 0.0170 (8) | 0.0031 (6) | −0.0016 (6) | 0.0017 (6) |
C3 | 0.0129 (8) | 0.0132 (8) | 0.0117 (7) | 0.0014 (6) | −0.0004 (6) | 0.0013 (6) |
C4 | 0.0160 (8) | 0.0363 (11) | 0.0149 (8) | 0.0092 (8) | 0.0013 (7) | 0.0019 (7) |
C5 | 0.0240 (9) | 0.0251 (9) | 0.0182 (9) | 0.0086 (8) | 0.0063 (7) | 0.0052 (7) |
C6 | 0.0192 (9) | 0.0257 (10) | 0.0191 (9) | 0.0015 (7) | 0.0050 (7) | −0.0008 (7) |
I1—C1 | 2.0922 (17) | C4—C5 | 1.381 (3) |
Cl1—C2 | 1.7254 (17) | C4—C6ii | 1.394 (3) |
C1—C2 | 1.396 (2) | C4—H4 | 0.9500 |
C1—C3i | 1.400 (2) | C5—C6 | 1.390 (3) |
Cl2—C3 | 1.7215 (17) | C5—H5 | 0.9500 |
C2—C3 | 1.397 (2) | C6—H6 | 0.9500 |
C2—C1—C3i | 118.86 (15) | C5—C4—C6ii | 120.31 (18) |
C2—C1—I1 | 121.01 (12) | C5—C4—H4 | 119.8 |
C3i—C1—I1 | 120.13 (12) | C6ii—C4—H4 | 119.8 |
C1—C2—C3 | 120.44 (15) | C4—C5—C6 | 119.78 (18) |
C1—C2—Cl1 | 120.37 (13) | C4—C5—H5 | 120.1 |
C3—C2—Cl1 | 119.17 (13) | C6—C5—H5 | 120.1 |
C2—C3—C1i | 120.70 (16) | C5—C6—C4ii | 119.90 (19) |
C2—C3—Cl2 | 119.10 (13) | C5—C6—H6 | 120.0 |
C1i—C3—Cl2 | 120.21 (13) | C4ii—C6—H6 | 120.0 |
Symmetry codes: (i) −x+2, −y, −z+1; (ii) −x+1, −y+1, −z+2. |
Acknowledgements
We thank the Missouri State University Provost Incentive Fund that funded the purchase of the X-ray diffractometer.
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