| Literature DB >> 21582852 |
C John McAdam1, Lyall R Hanton, Stephen C Moratti, Jim Simpson.
Abstract
The centrosymmetric title compound, C(8)H(8)I(2), was prepared by metathesis from the dibromo analogue. In the crystal structure, weak C-H⋯I inter-actions link the mol-ecules into stacks down the b axis. The structure is further stabilized by short I⋯I contacts [3.8433 (2) Å], forming undulating sheets in the (101) plane.Entities:
Year: 2009 PMID: 21582852 PMCID: PMC2969495 DOI: 10.1107/S1600536809021151
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| C8H8I2 | |
| Monoclinic, | Mo |
| Hall symbol: -P 2ybc | Cell parameters from 5590 reflections |
| θ = 2.3–33.0° | |
| µ = 6.69 mm−1 | |
| β = 99.808 (1)° | Rectangular plate, pale yellow |
| 0.21 × 0.15 × 0.03 mm | |
| Bruker APEXII CCD area-detector diffractometer | 1674 independent reflections |
| Radiation source: fine-focus sealed tube | 1538 reflections with |
| graphite | |
| ω scans | θmax = 33.4°, θmin = 3.7° |
| Absorption correction: multi-scan ( | |
| 8198 measured reflections |
| Refinement on | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Secondary atom site location: difference Fourier map |
| Hydrogen site location: inferred from neighbouring sites | |
| All H-atom parameters refined | |
| 1674 reflections | (Δ/σ)max = 0.001 |
| 62 parameters | Δρmax = 0.51 e Å−3 |
| 0 restraints | Δρmin = −0.51 e Å−3 |
| 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 |
| C1 | 0.62504 (16) | 0.1521 (3) | 0.47504 (13) | 0.0138 (2) | |
| C2 | 0.63784 (17) | −0.0405 (3) | 0.57245 (14) | 0.0154 (3) | |
| C3 | 0.51429 (17) | −0.1903 (3) | 0.59710 (14) | 0.0154 (3) | |
| C4 | 0.75717 (18) | 0.3189 (4) | 0.45106 (15) | 0.0190 (3) | |
| I1 | 0.880515 (9) | 0.07951 (2) | 0.331669 (8) | 0.01438 (4) | |
| H2 | 0.729 (3) | −0.073 (4) | 0.620 (2) | 0.021 (6)* | |
| H41 | 0.841 (3) | 0.354 (5) | 0.524 (2) | 0.031 (6)* | |
| H3 | 0.523 (2) | −0.330 (5) | 0.6678 (19) | 0.022 (5)* | |
| H42 | 0.733 (3) | 0.509 (5) | 0.405 (2) | 0.021 (5)* |
| C1 | 0.0142 (6) | 0.0109 (6) | 0.0180 (6) | −0.0017 (5) | 0.0078 (5) | −0.0032 (5) |
| C2 | 0.0133 (6) | 0.0159 (7) | 0.0174 (7) | 0.0007 (5) | 0.0038 (5) | −0.0010 (5) |
| C3 | 0.0175 (6) | 0.0126 (6) | 0.0175 (6) | 0.0006 (5) | 0.0070 (5) | 0.0012 (5) |
| C4 | 0.0191 (7) | 0.0150 (7) | 0.0258 (8) | −0.0039 (5) | 0.0124 (6) | −0.0051 (6) |
| I1 | 0.01367 (5) | 0.01628 (6) | 0.01473 (5) | −0.00037 (3) | 0.00680 (3) | 0.00092 (3) |
| C1—C3i | 1.396 (2) | C3—C1i | 1.396 (2) |
| C1—C2 | 1.401 (2) | C3—H3 | 1.01 (2) |
| C1—C4 | 1.489 (2) | C4—I1 | 2.1907 (15) |
| C2—C3 | 1.386 (2) | C4—H41 | 1.04 (2) |
| C2—H2 | 0.92 (2) | C4—H42 | 1.02 (2) |
| C3i—C1—C2 | 118.88 (13) | C1i—C3—H3 | 118.7 (12) |
| C3i—C1—C4 | 120.68 (14) | C1—C4—I1 | 111.52 (10) |
| C2—C1—C4 | 120.42 (14) | C1—C4—H41 | 116.4 (13) |
| C3—C2—C1 | 120.64 (14) | I1—C4—H41 | 100.5 (13) |
| C3—C2—H2 | 119.1 (14) | C1—C4—H42 | 114.9 (13) |
| C1—C2—H2 | 120.3 (14) | I1—C4—H42 | 101.8 (13) |
| C2—C3—C1i | 120.48 (14) | H41—C4—H42 | 109.8 (19) |
| C2—C3—H3 | 120.9 (12) | ||
| C3i—C1—C2—C3 | −0.1 (2) | C3i—C1—C4—I1 | −91.95 (15) |
| C4—C1—C2—C3 | 178.24 (14) | C2—C1—C4—I1 | 89.71 (15) |
| C1—C2—C3—C1i | 0.1 (2) |
| H··· | ||||
| C4—H42···I1ii | 1.02 (2) | 3.12 (2) | 3.9774 (16) | 141.8 (16) |
Hydrogen-bond geometry (Å, °)
| H⋯ | ||||
|---|---|---|---|---|
| C4—H42⋯I1i | 1.02 (2) | 3.12 (2) | 3.9774 (16) | 141.8 (16) |
Symmetry code: (i) .