| Literature DB >> 22199770 |
Dong-Sheng Ma1, Pei-Jiang Liu, Shuai Zhang, Guang-Feng Hou.
Abstract
In the title compound, C(8)H(8)ClNO, the acetamide group is twisted out the benzene plane with a dihedral angle of 83.08 (1)°. In the crystal, mol-ecules are linked by N-H⋯O hydrogen bonds, forming layers parallel to the ab plane.Entities:
Year: 2011 PMID: 22199770 PMCID: PMC3238921 DOI: 10.1107/S1600536811046836
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| C8H8ClNO | |
| Orthorhombic, | Mo |
| Hall symbol: P 2ac 2ab | Cell parameters from 5994 reflections |
| θ = 3.1–27.4° | |
| µ = 0.42 mm−1 | |
| Block, colorless | |
| 0.29 × 0.22 × 0.07 mm |
| Rigaku R-AXIS RAPID diffractometer | 1807 independent reflections |
| Radiation source: fine-focus sealed tube | 1451 reflections with |
| graphite | |
| ω scan | θmax = 27.4°, θmin = 3.1° |
| Absorption correction: multi-scan ( | |
| 7733 measured reflections |
| Refinement on | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| H atoms treated by a mixture of independent and constrained refinement | |
| (Δ/σ)max < 0.001 | |
| 1807 reflections | Δρmax = 0.17 e Å−3 |
| 108 parameters | Δρmin = −0.17 e Å−3 |
| 2 restraints | Absolute structure: Flack (1983), 704 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: −0.12 (8) |
| 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. |
| 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 > 2sigma(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. |
| C1 | 0.3632 (4) | 0.5073 (3) | 0.79843 (7) | 0.0335 (4) | |
| C2 | 0.2527 (4) | 0.3677 (5) | 0.84087 (10) | 0.0603 (7) | |
| H2A | 0.1560 | 0.4638 | 0.8639 | 0.072* | |
| H2B | 0.1222 | 0.2633 | 0.8272 | 0.072* | |
| C3 | 0.4640 (4) | 0.2408 (4) | 0.86973 (8) | 0.0429 (5) | |
| C4 | 0.5575 (5) | 0.0374 (4) | 0.85279 (8) | 0.0487 (6) | |
| H4 | 0.4907 | −0.0195 | 0.8228 | 0.058* | |
| C5 | 0.7475 (5) | −0.0822 (3) | 0.87944 (8) | 0.0451 (5) | |
| H5 | 0.8079 | −0.2185 | 0.8676 | 0.054* | |
| C6 | 0.8470 (4) | 0.0017 (4) | 0.92375 (8) | 0.0410 (5) | |
| C7 | 0.7620 (5) | 0.2049 (4) | 0.94146 (8) | 0.0472 (6) | |
| H7 | 0.8324 | 0.2622 | 0.9711 | 0.057* | |
| C8 | 0.5697 (5) | 0.3221 (4) | 0.91430 (8) | 0.0487 (5) | |
| H8 | 0.5100 | 0.4586 | 0.9262 | 0.058* | |
| Cl1 | 1.08553 (13) | −0.14906 (11) | 0.95804 (2) | 0.0605 (2) | |
| N1 | 0.1788 (3) | 0.6234 (4) | 0.77353 (7) | 0.0441 (4) | |
| H11 | 0.004 (2) | 0.613 (4) | 0.7811 (8) | 0.046 (6)* | |
| H12 | 0.225 (5) | 0.714 (4) | 0.7485 (7) | 0.064 (8)* | |
| O1 | 0.6073 (3) | 0.5149 (3) | 0.78808 (5) | 0.0435 (4) |
| C1 | 0.0263 (9) | 0.0376 (11) | 0.0367 (10) | −0.0005 (9) | 0.0007 (8) | −0.0027 (8) |
| C2 | 0.0291 (11) | 0.0819 (19) | 0.0699 (15) | 0.0050 (12) | 0.0050 (11) | 0.0347 (15) |
| C3 | 0.0310 (11) | 0.0528 (13) | 0.0449 (11) | 0.0000 (9) | 0.0035 (9) | 0.0145 (9) |
| C4 | 0.0493 (13) | 0.0554 (14) | 0.0416 (11) | −0.0093 (12) | −0.0077 (11) | −0.0001 (10) |
| C5 | 0.0511 (13) | 0.0368 (12) | 0.0475 (12) | 0.0016 (9) | 0.0072 (11) | −0.0041 (9) |
| C6 | 0.0381 (11) | 0.0444 (12) | 0.0406 (10) | 0.0018 (10) | 0.0046 (9) | 0.0071 (9) |
| C7 | 0.0514 (13) | 0.0514 (14) | 0.0387 (11) | 0.0009 (10) | −0.0027 (10) | −0.0056 (10) |
| C8 | 0.0503 (13) | 0.0433 (13) | 0.0525 (12) | 0.0118 (12) | 0.0069 (12) | −0.0003 (10) |
| Cl1 | 0.0520 (3) | 0.0695 (4) | 0.0598 (3) | 0.0147 (3) | −0.0015 (3) | 0.0194 (3) |
| N1 | 0.0243 (8) | 0.0587 (12) | 0.0494 (10) | −0.0006 (8) | 0.0013 (8) | 0.0149 (10) |
| O1 | 0.0237 (6) | 0.0529 (9) | 0.0538 (8) | −0.0038 (7) | 0.0051 (7) | 0.0046 (7) |
| C1—O1 | 1.232 (2) | C5—C6 | 1.376 (3) |
| C1—N1 | 1.324 (3) | C5—H5 | 0.9300 |
| C1—C2 | 1.512 (3) | C6—C7 | 1.379 (3) |
| C2—C3 | 1.503 (3) | C6—Cl1 | 1.744 (2) |
| C2—H2A | 0.9700 | C7—C8 | 1.386 (3) |
| C2—H2B | 0.9700 | C7—H7 | 0.9300 |
| C3—C4 | 1.386 (3) | C8—H8 | 0.9300 |
| C3—C8 | 1.387 (3) | N1—H11 | 0.883 (10) |
| C4—C5 | 1.378 (3) | N1—H12 | 0.892 (10) |
| C4—H4 | 0.9300 | ||
| O1—C1—N1 | 122.34 (19) | C6—C5—C4 | 119.5 (2) |
| O1—C1—C2 | 122.57 (18) | C6—C5—H5 | 120.3 |
| N1—C1—C2 | 115.08 (17) | C4—C5—H5 | 120.3 |
| C3—C2—C1 | 114.78 (17) | C5—C6—C7 | 120.9 (2) |
| C3—C2—H2A | 108.6 | C5—C6—Cl1 | 119.88 (18) |
| C1—C2—H2A | 108.6 | C7—C6—Cl1 | 119.21 (17) |
| C3—C2—H2B | 108.6 | C6—C7—C8 | 118.8 (2) |
| C1—C2—H2B | 108.6 | C6—C7—H7 | 120.6 |
| H2A—C2—H2B | 107.5 | C8—C7—H7 | 120.6 |
| C4—C3—C8 | 117.9 (2) | C7—C8—C3 | 121.6 (2) |
| C4—C3—C2 | 120.9 (2) | C7—C8—H8 | 119.2 |
| C8—C3—C2 | 121.2 (2) | C3—C8—H8 | 119.2 |
| C5—C4—C3 | 121.3 (2) | C1—N1—H11 | 120.9 (16) |
| C5—C4—H4 | 119.3 | C1—N1—H12 | 121.7 (18) |
| C3—C4—H4 | 119.3 | H11—N1—H12 | 117 (2) |
| H··· | ||||
| N1—H11···O1i | 0.88 (1) | 2.05 (1) | 2.911 (2) | 165 (2) |
| N1—H12···O1ii | 0.89 (1) | 2.22 (1) | 3.064 (3) | 157 (2) |
Hydrogen-bond geometry (Å, °)
| H⋯ | ||||
|---|---|---|---|---|
| N1—H11⋯O1i | 0.88 (1) | 2.05 (1) | 2.911 (2) | 165 (2) |
| N1—H12⋯O1ii | 0.89 (1) | 2.22 (1) | 3.064 (3) | 157 (2) |
Symmetry codes: (i) ; (ii) .