| Literature DB >> 23284543 |
Abstract
The asymmetric unit of the title compound, C(4)H(4)Br(2)O(2), contains one half-mol-ecule, being located about a centre of inversion. In the crystal, there are no significant inter-molecular inter-actions.Entities:
Year: 2012 PMID: 23284543 PMCID: PMC3515323 DOI: 10.1107/S1600536812044200
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| C4H4Br2O2 | |
| Melting point < 395 K | |
| Orthorhombic, | Mo |
| Hall symbol: -P 2ac 2ab | Cell parameters from 25 reflections |
| θ = 9–14° | |
| µ = 12.13 mm−1 | |
| Cube, yellow | |
| 0.10 × 0.10 × 0.10 mm | |
| Enraf–Nonius CAD-4 diffractometer | 319 reflections with |
| Radiation source: fine-focus sealed tube | |
| Graphite monochromator | θmax = 25.4°, θmin = 2.4° |
| ω/2θ scans | |
| Absorption correction: ψ scan (North | |
| 614 measured reflections | 3 standard reflections every 120 min |
| 614 independent reflections | intensity decay: 1% |
| 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 | |
| H-atom parameters constrained | |
| 614 reflections | (Δ/σ)max < 0.001 |
| 37 parameters | Δρmax = 0.65 e Å−3 |
| 1 restraint | Δρmin = −0.60 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 |
| Br | 0.96430 (19) | 0.17863 (19) | 0.67746 (8) | 0.0634 (5) | |
| O | 0.8640 (13) | 0.2368 (15) | 0.5056 (4) | 0.062 (2) | |
| C1 | 1.0276 (16) | 0.4425 (18) | 0.6134 (6) | 0.055 (3) | |
| H1A | 0.9689 | 0.5875 | 0.6342 | 0.066* | |
| H1B | 1.1661 | 0.4652 | 0.6138 | 0.066* | |
| C2 | 0.9577 (15) | 0.4056 (11) | 0.5267 (6) | 0.039 (2) |
| Br | 0.0755 (7) | 0.0501 (7) | 0.0647 (9) | −0.0027 (7) | 0.0041 (7) | 0.0097 (6) |
| O | 0.076 (5) | 0.036 (3) | 0.073 (6) | −0.026 (5) | −0.019 (5) | 0.007 (3) |
| C1 | 0.045 (6) | 0.068 (7) | 0.052 (7) | 0.000 (6) | 0.009 (6) | −0.016 (7) |
| C2 | 0.033 (5) | 0.028 (4) | 0.057 (7) | 0.013 (6) | 0.023 (5) | 0.007 (5) |
| Br—C1 | 1.885 (10) | C1—H1A | 0.9700 |
| O—C2 | 1.196 (11) | C1—H1B | 0.9700 |
| C1—C2 | 1.585 (9) | C2—C2i | 1.512 (16) |
| C2—C1—Br | 112.4 (6) | H1A—C1—H1B | 107.9 |
| C2—C1—H1A | 109.1 | O—C2—C2i | 124.6 (12) |
| Br—C1—H1A | 109.1 | O—C2—C1 | 123.7 (8) |
| C2—C1—H1B | 109.1 | C2i—C2—C1 | 111.4 (10) |
| Br—C1—H1B | 109.1 | ||
| Br—C1—C2—O | 4.7 (13) | Br—C1—C2—C2i | −169.0 (8) |