Abstract
In the title compound, C11H19Cl2NO2, the oxazolidine ring is in an envelope conformation with the O atom forming the flap. In the crystal structure, molecules are linked by weak intermolecular C—H⋯O hydrogen bonds, forming chains.
Related literature
For general background to N-dichloroacetyl oxazolidine, see: Agami & Couty (2004 ▶); Abu-Qare & Duncan (2002 ▶); Guirado et al. (2003 ▶); Davies & Caseley (1999 ▶). For the bioactivity of related compounds, see: Del Buono et al. (2007 ▶); Hatzios & Burgos (2004 ▶). For details of the synthesis, see: Fu et al. (2009 ▶).
Experimental
Crystal data
C11H19Cl2NO2
M r = 268.17
Orthorhombic,
a = 6.4834 (12) Å
b = 10.795 (2) Å
c = 20.030 (4) Å
V = 1401.8 (5) Å3
Z = 4
Mo Kα radiation
μ = 0.45 mm−1
T = 293 K
0.32 × 0.24 × 0.20 mm
Data collection
Bruker SMART CCD diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.869, T max = 0.915
14134 measured reflections
3499 independent reflections
2117 reflections with I > 2σ(I)
R int = 0.058
Refinement
R[F 2 > 2σ(F 2)] = 0.084
wR(F 2) = 0.258
S = 1.02
3499 reflections
148 parameters
H-atom parameters constrained
Δρmax = 0.58 e Å−3
Δρmin = −0.39 e Å−3
Absolute structure: Flack (1983 ▶) 1468 Friedels
Flack parameter: 0.02 (15)
Data collection: SMART (Bruker, 1998 ▶); cell refinement: SAINT (Bruker, 1998 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810016090/lh5034sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810016090/lh5034Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| C1—H1⋯O2i | 0.98 | 2.38 | 3.327 (5) | 163 |
Symmetry code: (i)
.
Acknowledgments
We thank the Heilongjiang Province Foundation for Young Scholars (QC2009C44), the Innovation Foundation for Young Scholars of Harbin (No.2007RFQXN017),the China Postdoctoral Science Foundation (20080430951), the Heilongjiang Province Postdoctoral Science Foundation and the Northeast Agricultural University Doctoral Foundation for generously supporting this study.
supplementary crystallographic information
Comment
N-dichloroacetyl oxazolidines are becoming increasingly important with their excellent biological activity (Agami & Couty, 2004; Abu-Qare & Duncan, 2002; Guirado et al., 2003; Davies & Caseley, 1999). The discovery of N-dichloroacetyl oxazolidine as a herbicide safener has drawn widespread attention in agricultural biochemistry (Del Buono et al., 2007; Hatzios & Burgos, 2004). As a part of our ongoing investigation of oxazolidine derivatives (Fu et al., 2009) we prepared the title compound.
The molecular structure of the title compound is shown in Fig. 1. In the crystal structure, molecules are linked by weak intermolecular C—H···O hydrogen bonds to form one-dimensional chains (Fig. 2).
Experimental
The title compound was prepared according to the literature procedure (Fu et al., 2009). The single crystal suitable for X-ray structural analysis was obtained by slow evaporation in petroleum ether and ethyl acetate at room temperature. The title enantiomer spontaneously resolved from a racemic mixture during the crystallization.
Refinement
All H atoms were initially located in a different Fourier map. The C—H atoms were then constrained to an ideal geometry, with C—H = 0.96-0.98 Å and Uiso(H) = 1.2Ueq(C) or 1.5Ueq(C) for methyl H atoms.
Figures
Fig. 1.
The molecular structure of the title compound, with the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level.
Fig. 2.
A packing diagram for (I), showing weak hydrogen bonds as dashed lines.
Crystal data
| C11H19Cl2NO2 | F(000) = 568.0 |
| Mr = 268.17 | Dx = 1.271 Mg m−3Dm = 1.271 Mg m−3Dm measured by not measured |
| Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2ac 2ab | Cell parameters from 3142 reflections |
| a = 6.4834 (12) Å | θ = 2.8–20.6° |
| b = 10.795 (2) Å | µ = 0.45 mm−1 |
| c = 20.030 (4) Å | T = 293 K |
| V = 1401.8 (5) Å3 | Block, colourless |
| Z = 4 | 0.32 × 0.24 × 0.20 mm |
Data collection
| Bruker SMART CCD diffractometer | 3499 independent reflections |
| Radiation source: fine-focus sealed tube | 2117 reflections with I > 2σ(I) |
| graphite | Rint = 0.058 |
| φ and ω scans | θmax = 28.4°, θmin = 2.8° |
| Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −8→8 |
| Tmin = 0.869, Tmax = 0.915 | k = −14→14 |
| 14134 measured reflections | l = −25→26 |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.084 | H-atom parameters constrained |
| wR(F2) = 0.258 | w = 1/[σ2(Fo2) + (0.165P)2] where P = (Fo2 + 2Fc2)/3 |
| S = 1.02 | (Δ/σ)max < 0.001 |
| 3499 reflections | Δρmax = 0.58 e Å−3 |
| 148 parameters | Δρmin = −0.39 e Å−3 |
| 0 restraints | Absolute structure: Flack (1983) 1468 Friedels |
| Primary atom site location: structure-invariant direct methods | Flack parameter: 0.02 (15) |
Special details
| 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 > σ(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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| C1 | 0.5074 (7) | 0.9192 (4) | 0.2071 (2) | 0.0675 (11) | |
| H1 | 0.4966 | 0.8365 | 0.2270 | 0.081* | |
| C2 | 0.5889 (7) | 1.0103 (3) | 0.2598 (2) | 0.0638 (10) | |
| C3 | 0.7886 (9) | 0.8326 (4) | 0.3065 (3) | 0.0789 (13) | |
| H3A | 0.6784 | 0.7758 | 0.3181 | 0.095* | |
| H3B | 0.8454 | 0.8089 | 0.2636 | 0.095* | |
| C4 | 0.9470 (13) | 0.8334 (4) | 0.3575 (3) | 0.105 (2) | |
| H4 | 1.0627 | 0.8594 | 0.3293 | 0.126* | |
| C5 | 1.0407 (13) | 0.7301 (5) | 0.3866 (4) | 0.122 (3) | |
| H5A | 1.0922 | 0.6801 | 0.3500 | 0.147* | |
| H5B | 0.9306 | 0.6828 | 0.4072 | 0.147* | |
| C6 | 1.2052 (13) | 0.7357 (6) | 0.4353 (3) | 0.111 (2) | |
| H6A | 1.3358 | 0.7362 | 0.4127 | 0.166* | |
| H6B | 1.1976 | 0.6647 | 0.4640 | 0.166* | |
| H6C | 1.1915 | 0.8098 | 0.4614 | 0.166* | |
| C7 | 0.8170 (7) | 1.0342 (4) | 0.3589 (2) | 0.0680 (10) | |
| C8 | 0.9703 (10) | 1.1251 (5) | 0.3287 (3) | 0.0925 (16) | |
| H8A | 1.0635 | 1.1533 | 0.3627 | 0.139* | |
| H8B | 0.8973 | 1.1946 | 0.3104 | 0.139* | |
| H8C | 1.0470 | 1.0847 | 0.2939 | 0.139* | |
| C9 | 0.6750 (10) | 1.1009 (5) | 0.4051 (3) | 0.0875 (14) | |
| H9A | 0.7550 | 1.1310 | 0.4427 | 0.105* | |
| H9B | 0.6205 | 1.1727 | 0.3819 | 0.105* | |
| C10 | 0.4982 (11) | 1.0277 (6) | 0.4315 (3) | 0.1013 (18) | |
| H10A | 0.5481 | 0.9494 | 0.4488 | 0.122* | |
| H10B | 0.4023 | 1.0103 | 0.3955 | 0.122* | |
| C11 | 0.3855 (15) | 1.0989 (8) | 0.4874 (4) | 0.127 (3) | |
| H11A | 0.4781 | 1.1119 | 0.5242 | 0.190* | |
| H11B | 0.2688 | 1.0516 | 0.5023 | 0.190* | |
| H11C | 0.3396 | 1.1775 | 0.4707 | 0.190* | |
| Cl1 | 0.6885 (3) | 0.91462 (14) | 0.14073 (7) | 0.0996 (5) | |
| Cl2 | 0.2642 (2) | 0.96549 (13) | 0.17873 (9) | 0.1008 (5) | |
| N1 | 0.7143 (5) | 0.9597 (3) | 0.30507 (18) | 0.0629 (8) | |
| O1 | 0.9265 (6) | 0.9417 (3) | 0.39428 (17) | 0.0793 (9) | |
| O2 | 0.5407 (6) | 1.1193 (3) | 0.2580 (2) | 0.0859 (10) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| C1 | 0.072 (2) | 0.0401 (18) | 0.090 (3) | 0.0031 (17) | −0.013 (2) | 0.0002 (18) |
| C2 | 0.071 (2) | 0.0396 (17) | 0.081 (3) | 0.0077 (17) | 0.000 (2) | −0.0023 (17) |
| C3 | 0.093 (3) | 0.0354 (18) | 0.108 (3) | 0.014 (2) | −0.021 (3) | −0.0090 (18) |
| C4 | 0.154 (5) | 0.046 (2) | 0.114 (4) | 0.033 (3) | −0.043 (4) | −0.013 (3) |
| C5 | 0.149 (6) | 0.059 (3) | 0.160 (6) | 0.031 (4) | −0.071 (5) | −0.020 (3) |
| C6 | 0.127 (5) | 0.070 (3) | 0.134 (5) | 0.010 (4) | −0.031 (4) | 0.013 (3) |
| C7 | 0.084 (3) | 0.0379 (17) | 0.082 (3) | 0.0039 (18) | −0.010 (2) | −0.0029 (16) |
| C8 | 0.101 (4) | 0.052 (2) | 0.124 (4) | −0.020 (3) | −0.013 (3) | 0.003 (3) |
| C9 | 0.109 (4) | 0.060 (3) | 0.093 (3) | 0.006 (3) | 0.003 (3) | −0.010 (2) |
| C10 | 0.105 (4) | 0.075 (3) | 0.124 (5) | 0.010 (3) | 0.006 (3) | 0.000 (3) |
| C11 | 0.149 (6) | 0.124 (6) | 0.107 (4) | 0.021 (5) | 0.035 (4) | −0.005 (4) |
| Cl1 | 0.1169 (11) | 0.0780 (8) | 0.1038 (9) | −0.0063 (8) | 0.0152 (9) | −0.0185 (7) |
| Cl2 | 0.0899 (8) | 0.0761 (8) | 0.1365 (12) | 0.0154 (7) | −0.0350 (8) | −0.0093 (7) |
| N1 | 0.0715 (19) | 0.0298 (13) | 0.087 (2) | 0.0036 (14) | −0.0060 (17) | −0.0042 (13) |
| O1 | 0.102 (2) | 0.0413 (14) | 0.095 (2) | 0.0055 (15) | −0.0232 (19) | −0.0079 (14) |
| O2 | 0.114 (3) | 0.0338 (13) | 0.110 (2) | 0.0152 (16) | −0.023 (2) | −0.0013 (14) |
Geometric parameters (Å, °)
| C1—C2 | 1.536 (6) | C6—H6C | 0.9600 |
| C1—Cl2 | 1.750 (4) | C7—O1 | 1.416 (5) |
| C1—Cl1 | 1.775 (5) | C7—C9 | 1.491 (7) |
| C1—H1 | 0.9800 | C7—N1 | 1.501 (5) |
| C2—O2 | 1.218 (5) | C7—C8 | 1.523 (7) |
| C2—N1 | 1.335 (6) | C8—H8A | 0.9600 |
| C3—C4 | 1.448 (8) | C8—H8B | 0.9600 |
| C3—N1 | 1.454 (5) | C8—H8C | 0.9600 |
| C3—H3A | 0.9700 | C9—C10 | 1.490 (9) |
| C3—H3B | 0.9700 | C9—H9A | 0.9700 |
| C4—O1 | 1.388 (6) | C9—H9B | 0.9700 |
| C4—C5 | 1.397 (7) | C10—C11 | 1.542 (9) |
| C4—H4 | 0.9800 | C10—H10A | 0.9700 |
| C5—C6 | 1.446 (10) | C10—H10B | 0.9700 |
| C5—H5A | 0.9700 | C11—H11A | 0.9600 |
| C5—H5B | 0.9700 | C11—H11B | 0.9600 |
| C6—H6A | 0.9600 | C11—H11C | 0.9600 |
| C6—H6B | 0.9600 | ||
| C2—C1—Cl2 | 110.5 (3) | O1—C7—N1 | 101.8 (3) |
| C2—C1—Cl1 | 107.8 (3) | C9—C7—N1 | 115.5 (4) |
| Cl2—C1—Cl1 | 111.1 (3) | O1—C7—C8 | 109.0 (4) |
| C2—C1—H1 | 109.1 | C9—C7—C8 | 109.8 (4) |
| Cl2—C1—H1 | 109.1 | N1—C7—C8 | 110.5 (4) |
| Cl1—C1—H1 | 109.1 | C7—C8—H8A | 109.5 |
| O2—C2—N1 | 124.9 (4) | C7—C8—H8B | 109.5 |
| O2—C2—C1 | 120.7 (4) | H8A—C8—H8B | 109.5 |
| N1—C2—C1 | 114.5 (3) | C7—C8—H8C | 109.5 |
| C4—C3—N1 | 104.1 (4) | H8A—C8—H8C | 109.5 |
| C4—C3—H3A | 110.9 | H8B—C8—H8C | 109.5 |
| N1—C3—H3A | 110.9 | C10—C9—C7 | 116.0 (5) |
| C4—C3—H3B | 110.9 | C10—C9—H9A | 108.3 |
| N1—C3—H3B | 110.9 | C7—C9—H9A | 108.3 |
| H3A—C3—H3B | 108.9 | C10—C9—H9B | 108.3 |
| O1—C4—C5 | 119.5 (5) | C7—C9—H9B | 108.3 |
| O1—C4—C3 | 108.1 (4) | H9A—C9—H9B | 107.4 |
| C5—C4—C3 | 126.8 (5) | C9—C10—C11 | 111.0 (6) |
| O1—C4—H4 | 97.9 | C9—C10—H10A | 109.4 |
| C5—C4—H4 | 97.9 | C11—C10—H10A | 109.4 |
| C3—C4—H4 | 97.9 | C9—C10—H10B | 109.4 |
| C4—C5—C6 | 124.7 (6) | C11—C10—H10B | 109.4 |
| C4—C5—H5A | 106.2 | H10A—C10—H10B | 108.0 |
| C6—C5—H5A | 106.2 | C10—C11—H11A | 109.5 |
| C4—C5—H5B | 106.2 | C10—C11—H11B | 109.5 |
| C6—C5—H5B | 106.2 | H11A—C11—H11B | 109.5 |
| H5A—C5—H5B | 106.3 | C10—C11—H11C | 109.5 |
| C5—C6—H6A | 109.5 | H11A—C11—H11C | 109.5 |
| C5—C6—H6B | 109.5 | H11B—C11—H11C | 109.5 |
| H6A—C6—H6B | 109.5 | C2—N1—C3 | 127.0 (3) |
| C5—C6—H6C | 109.5 | C2—N1—C7 | 122.6 (3) |
| H6A—C6—H6C | 109.5 | C3—N1—C7 | 110.1 (3) |
| H6B—C6—H6C | 109.5 | C4—O1—C7 | 112.1 (3) |
| O1—C7—C9 | 109.9 (4) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C1—H1···O2i | 0.98 | 2.38 | 3.327 (5) | 163 |
Symmetry codes: (i) −x+1, y−1/2, −z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH5034).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810016090/lh5034sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810016090/lh5034Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


