| Literature DB >> 21578279 |
Michael T Kirchner, Dieter Bläser, Roland Boese, Tejender S Thakur, Gautam R Desiraju.
Abstract
In the title compound, C(6)H(3)F(3), weak electrostatic and dispersive forces between C(δ+)-F(δ-) and H(δ+)-C(δ-) groups are at the borderline of the hydrogen-bond phenomenon and are poorly directional and further deformed in the presence of π-π stacking inter-actions. The mol-ecule lies on a twofold rotation axis. In the crystal structure, one-dimensional tapes are formed via two anti-dromic C-H⋯F hydrogen bonds. These tapes are, in turn, connected into corrugated two-dimensional sheets by bifurcated C-H⋯F hydrogen bonds. Packing in the third dimension is furnished by π-π stacking inter-actions with a centroid-centroid distance of 3.6362 (14) Å.Entities:
Year: 2009 PMID: 21578279 PMCID: PMC2971369 DOI: 10.1107/S1600536809038975
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| C6H3F3 | |
| Monoclinic, | Mo |
| Hall symbol: -C 2yc | Cell parameters from 376 reflections |
| θ = 3.8–22.7° | |
| µ = 0.16 mm−1 | |
| β = 112.783 (4)° | Cylindric, colourless |
| 0.30 × 0.30 × 0.30 mm | |
| Siemens SMART three-axis goniometer with an APEXII area-detector system diffractometer | 634 independent reflections |
| Radiation source: fine-focus sealed tube | 413 reflections with |
| graphite | |
| Detector resolution: 512 pixels mm-1 | θmax = 28.2°, θmin = 3.5° |
| in ω at 0.3° scan width one run with 740 frames, phi = 0°, chi = 0° | |
| Absorption correction: multi-scan ( | |
| 1074 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 | |
| H-atom parameters constrained | |
| 634 reflections | (Δ/σ)max = 0.017 |
| 44 parameters | Δρmax = 0.20 e Å−3 |
| 0 restraints | Δρmin = −0.18 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 |
| F1 | 1.0000 | 0.30558 (17) | 0.2500 | 0.1156 (10) | |
| F2 | 0.6666 (2) | 0.4183 (2) | 0.1576 (3) | 0.1354 (10) | |
| C1 | 1.0000 | 0.4213 (3) | 0.2500 | 0.0769 (9) | |
| C2 | 0.8308 (3) | 0.4803 (2) | 0.2036 (3) | 0.0824 (8) | |
| C3 | 0.8265 (4) | 0.5973 (3) | 0.2023 (3) | 0.0942 (9) | |
| H3 | 0.6833 | 0.6388 | 0.1585 | 0.113* | |
| C4 | 1.0000 | 0.6558 (3) | 0.2500 | 0.1006 (13) | |
| H4 | 1.0000 | 0.7422 | 0.2500 | 0.121* |
| F1 | 0.161 (2) | 0.0623 (13) | 0.1249 (16) | 0.000 | 0.0563 (14) | 0.000 |
| F2 | 0.0959 (12) | 0.157 (2) | 0.1484 (16) | −0.0341 (10) | 0.0415 (10) | 0.0067 (12) |
| C1 | 0.1030 (19) | 0.0573 (16) | 0.0725 (15) | 0.000 | 0.0364 (13) | 0.000 |
| C2 | 0.0830 (14) | 0.0890 (17) | 0.0770 (13) | −0.0101 (9) | 0.0327 (10) | 0.0013 (9) |
| C3 | 0.1073 (17) | 0.0935 (18) | 0.0858 (15) | 0.0277 (12) | 0.0419 (12) | 0.0094 (10) |
| C4 | 0.163 (4) | 0.0605 (17) | 0.0848 (19) | 0.000 | 0.056 (2) | 0.000 |
| F1—C1 | 1.341 (4) | C3—C4 | 1.377 (3) |
| F2—C2 | 1.342 (3) | C3—H3 | 1.0973 |
| C1—C2 | 1.354 (3) | C4—H4 | 1.0018 |
| C2—C3 | 1.357 (4) | ||
| F1—C1—C2 | 120.30 (15) | C2—C3—H3 | 117.3 |
| C2i—C1—C2 | 119.4 (3) | C4—C3—H3 | 124.4 |
| F2—C2—C3 | 121.1 (2) | C3—C4—C3i | 121.0 (3) |
| F2—C2—C1 | 117.3 (3) | C3—C4—H4 | 119.5 |
| C3—C2—C1 | 121.5 (2) | C3i—C4—H4 | 119.5 |
| C2—C3—C4 | 118.3 (2) |
| H··· | ||||
| C3—H3···F2ii | 1.10 | 2.77 | 3.560 (3) | 129 |
| C3—H3···F1iii | 1.10 | 2.59 | 3.528 (4) | 144 |
| C4—H4···F2iv | 1.00 | 2.60 | 3.440 (4) | 142 |
Hydrogen-bond geometry (Å, °)
| H⋯ | ||||
|---|---|---|---|---|
| C3—H3⋯F2i | 1.10 | 2.77 | 3.560 (3) | 129 |
| C3—H3⋯F1ii | 1.10 | 2.59 | 3.528 (4) | 144 |
| C4—H4⋯F2iii | 1.00 | 2.60 | 3.440 (4) | 142 |
Symmetry codes: (i) ; (ii) ; (iii) .