Abstract
The molecule of the title compound, C13H9NO2, is slightly twisted with a dihedral angle of 4.85 (9)° between the nine-membered ring system and the phenyl ring. The nine non-H atoms of the 1H-pyrrolo[2,1-c][1,4]oxazin-1-one system are coplanar [r.m.s. deviation = 0.0122 (2) Å]. In the crystal, weak intermolecular C—H⋯O interactions link molecules into chains along [1
0]. The crystal studied was an inversion twin with a 0.48624 (9):0.51376 (9) domain ratio.
Related literature
For the biological activity and applications of pyrrolo[1,2-a]pyrazine derivatives, see: Bélanger et al. (1983 ▶); Fu et al. (2002 ▶); Micheli et al. (2008 ▶). For a related structure, see: Khan et al. (2010 ▶). For standard bond-length data, see: Allen et al. (1987 ▶).
Experimental
Crystal data
C13H9NO2
M r = 211.21
Monoclinic,
a = 5.870 (1) Å
b = 3.8345 (7) Å
c = 21.733 (4) Å
β = 91.059 (7)°
V = 489.09 (15) Å3
Z = 2
Mo Kα radiation
μ = 0.10 mm−1
T = 113 K
0.22 × 0.18 × 0.08 mm
Data collection
Rigaku Saturn CCD area-detector diffractometer
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.979, T max = 0.992
4358 measured reflections
1222 independent reflections
1092 reflections with I > 2σ(I)
R int = 0.032
Refinement
R[F 2 > 2σ(F 2)] = 0.031
wR(F 2) = 0.085
S = 1.10
1222 reflections
147 parameters
1 restraint
H-atom parameters constrained
Δρmax = 0.20 e Å−3
Δρmin = −0.19 e Å−3
Data collection: CrystalClear (Rigaku, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810017940/rz2449sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810017940/rz2449Isup2.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 |
|---|---|---|---|---|
| C7—H7⋯O2i | 0.95 | 2.27 | 3.109 (2) | 147 |
Symmetry code: (i)
.
Acknowledgments
STK acknowledges funding from the Industrial Linkage Programme of Pakistan Council of Scientific and Industrial Research (PCSIR) Laboratories, Pakistan. He also thanks Dr Song Haibin of the State Key Laboratory of Elemento-Organic Chemistry, Nankai University, for the X-ray data collection. PY is grateful to Tianjin University of Science & Technology for a research grant (No. 2009 0431).
supplementary crystallographic information
Comment
A series of pyrrolo[1,2-a]pyrazine compounds show potent and selective non-competitive mGluR5 antagonists properties (Micheli et al., 2008). We previously reported the synthesis and crystal structure of 3-methyl-1H-pyrrolo[2,1-c][1,4]oxazin-1-one (I) (Khan et al., 2010). The title compound (II), which was designed by changing the methyl substituent in (I) to phenyl, is a new key intermediate which can be used as a precursor for the syntheses of muscle relaxant agents (Bélanger et al., 1983) and other biological active compounds (Fu et al., 2002).
The molecule of title compound (Fig. 1) is slightly twisted, the dihedral angle between this nine membered ring system and phenyl ring being 4.85 (9)° and the O1–C6–C8–C9 torsion angle 5.0 (3)°. The nine non-hydrogen atoms of the 1H-pyrrolo[2,1-c][1,4]oxazin-1-one ring system are coplanar with a r.m.s. of 0.0122 (2) Å. The bond lengths are in normal ranges (Allen et al., 1987) and comparable with the related structure (Khan et al., 2010). In the crystal structure (Fig. 2), weak intermolecular C—H···O interactions (Table 1) link the molecules into chains along [110]. These chains are stacked along the b axis.
Experimental
A solution of α-bromo acetophenone (2.37 g, 11.91 mmol) in acetone (25 ml) was dropwise added through a dropping funnel to a slurry of 2,2,2-trichloro-1-(lH-pyrrol-2-yl)ethanone (1.69 g, 7.95 mmol), potassium carbonate (1.98 g, 14.31 mmol) and acetone (20 ml) at room temperature in a 100 ml reaction flask. The reaction mixture was refluxed for 4 h. The solid was then removed by filtration and washed with acetone. The filtrate was concentrated under reduced pressure by rotary evaporator, the residue was partitioned between water (20 ml) and ethyl acetate (40 ml) in a separatory funnel (100 ml). The organic layer was separated and the aqueous phase was washed with ethyl acetate (30 ml x 2). The combined organic layers were washed successively with water (20 ml x 3) and brine solution and dried over anhydrous MgSO4. After filtration, the solvent was removed by rotary evaporator to obtain the oily residue (1.90 g) which was purified by flash column chromatography (petroleum ether:ethyl acetate, 4:1 v/v) to afford the desired compound as white solid (1.05 g, yield 62.5 %). Colourless needle-shaped single crystals of the title compound suitable for X-ray structure determination were recrystalized from ethyl acetate by slow evaporation of the solvent at room temperature after several days.
Refinement
H atoms were placed in calculated positions with C—H = 0.95 Å, and were included in the refinement in a riding-model approximation, with Uiso(H) = 1.2 Ueq(C). The highest residual electron density peak and the deepest hole are located at 0.69 Å and 0.93 Å from atom C4. The crystal studied was an inversion twin, with a refined BASF ratio of 0.48624 (9)/0.51376 (9). The final refinement was carried out with Friedel pairs merged.
Figures
Fig. 1.
The molecular structure of the title compound, showing 50% probability displacement ellipsoids and the atom-numbering scheme.
Fig. 2.
The crystal packing of the title compound viewd along the b axis. Intermoilecular C—H···O interactions are drawn as dashed lines.
Crystal data
| C13H9NO2 | F(000) = 220 |
| Mr = 211.21 | Dx = 1.434 Mg m−3 |
| Monoclinic, P21 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2yb | Cell parameters from 1222 reflections |
| a = 5.870 (1) Å | θ = 2.8–27.0° |
| b = 3.8345 (7) Å | µ = 0.10 mm−1 |
| c = 21.733 (4) Å | T = 113 K |
| β = 91.059 (7)° | Needle, colourless |
| V = 489.09 (15) Å3 | 0.22 × 0.18 × 0.08 mm |
| Z = 2 |
Data collection
| Rigaku Saturn CCD area-detector diffractometer | 1222 independent reflections |
| Radiation source: rotating anode | 1092 reflections with I > 2σ(I) |
| multilayer | Rint = 0.032 |
| Detector resolution: 14.63 pixels mm-1 | θmax = 27.0°, θmin = 2.8° |
| ω and φ scans | h = −7→7 |
| Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −4→4 |
| Tmin = 0.979, Tmax = 0.992 | l = −26→27 |
| 4358 measured reflections |
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)] = 0.031 | H-atom parameters constrained |
| wR(F2) = 0.085 | w = 1/[σ2(Fo2) + (0.050P)2] where P = (Fo2 + 2Fc2)/3 |
| S = 1.10 | (Δ/σ)max < 0.001 |
| 1222 reflections | Δρmax = 0.20 e Å−3 |
| 147 parameters | Δρmin = −0.19 e Å−3 |
| 1 restraint | Extinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.037 (9) |
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 | ||
| O1 | 0.4797 (2) | 0.4846 (4) | 0.25405 (5) | 0.0201 (4) | |
| O2 | 0.7147 (2) | 0.7726 (4) | 0.31664 (6) | 0.0273 (4) | |
| N1 | 0.1877 (2) | 0.3508 (4) | 0.34783 (7) | 0.0181 (4) | |
| C1 | 0.0686 (3) | 0.3143 (6) | 0.40070 (8) | 0.0219 (5) | |
| H1 | −0.0763 | 0.2067 | 0.4044 | 0.026* | |
| C2 | 0.1959 (3) | 0.4614 (6) | 0.44782 (8) | 0.0232 (5) | |
| H2 | 0.1546 | 0.4700 | 0.4899 | 0.028* | |
| C3 | 0.3965 (3) | 0.5960 (6) | 0.42329 (9) | 0.0230 (5) | |
| H3 | 0.5148 | 0.7140 | 0.4453 | 0.028* | |
| C4 | 0.3895 (3) | 0.5244 (5) | 0.36106 (8) | 0.0186 (4) | |
| C5 | 0.5406 (3) | 0.6064 (6) | 0.31182 (8) | 0.0198 (4) | |
| C6 | 0.2775 (3) | 0.3039 (6) | 0.24323 (8) | 0.0177 (4) | |
| C7 | 0.1330 (3) | 0.2396 (6) | 0.28844 (8) | 0.0189 (4) | |
| H7 | −0.0057 | 0.1192 | 0.2802 | 0.023* | |
| C8 | 0.2448 (3) | 0.1991 (6) | 0.17857 (8) | 0.0186 (4) | |
| C9 | 0.4150 (3) | 0.2573 (6) | 0.13567 (8) | 0.0223 (5) | |
| H9 | 0.5540 | 0.3651 | 0.1483 | 0.027* | |
| C10 | 0.3819 (4) | 0.1584 (6) | 0.07468 (9) | 0.0258 (5) | |
| H10 | 0.4987 | 0.1992 | 0.0459 | 0.031* | |
| C11 | 0.1813 (4) | 0.0015 (6) | 0.05544 (8) | 0.0242 (5) | |
| H11 | 0.1596 | −0.0651 | 0.0136 | 0.029* | |
| C12 | 0.0115 (3) | −0.0580 (6) | 0.09787 (8) | 0.0248 (5) | |
| H12 | −0.1273 | −0.1651 | 0.0849 | 0.030* | |
| C13 | 0.0429 (3) | 0.0377 (6) | 0.15879 (8) | 0.0220 (5) | |
| H13 | −0.0738 | −0.0068 | 0.1875 | 0.026* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| O1 | 0.0165 (7) | 0.0229 (8) | 0.0210 (6) | −0.0045 (6) | 0.0017 (5) | 0.0005 (7) |
| O2 | 0.0190 (7) | 0.0308 (9) | 0.0321 (8) | −0.0093 (7) | −0.0014 (5) | 0.0000 (7) |
| N1 | 0.0163 (8) | 0.0198 (10) | 0.0183 (8) | −0.0017 (7) | 0.0007 (6) | 0.0014 (7) |
| C1 | 0.0206 (10) | 0.0251 (12) | 0.0202 (9) | 0.0008 (9) | 0.0047 (7) | 0.0043 (9) |
| C2 | 0.0263 (10) | 0.0249 (12) | 0.0185 (9) | 0.0048 (10) | 0.0025 (7) | 0.0021 (9) |
| C3 | 0.0233 (10) | 0.0222 (12) | 0.0234 (9) | 0.0015 (9) | −0.0033 (7) | −0.0017 (9) |
| C4 | 0.0161 (9) | 0.0173 (12) | 0.0224 (9) | 0.0000 (8) | −0.0019 (7) | 0.0001 (9) |
| C5 | 0.0183 (10) | 0.0170 (11) | 0.0240 (9) | 0.0002 (9) | −0.0017 (7) | 0.0007 (9) |
| C6 | 0.0146 (9) | 0.0166 (11) | 0.0220 (9) | −0.0019 (8) | −0.0010 (7) | 0.0017 (8) |
| C7 | 0.0172 (9) | 0.0207 (11) | 0.0187 (8) | −0.0025 (8) | −0.0012 (7) | 0.0002 (9) |
| C8 | 0.0193 (9) | 0.0168 (11) | 0.0197 (9) | 0.0027 (8) | 0.0009 (7) | 0.0020 (8) |
| C9 | 0.0202 (10) | 0.0237 (12) | 0.0229 (9) | 0.0017 (9) | 0.0011 (7) | 0.0015 (10) |
| C10 | 0.0289 (11) | 0.0275 (13) | 0.0211 (9) | 0.0049 (10) | 0.0064 (8) | 0.0034 (9) |
| C11 | 0.0310 (11) | 0.0237 (12) | 0.0178 (9) | 0.0066 (9) | −0.0020 (7) | −0.0001 (9) |
| C12 | 0.0239 (10) | 0.0248 (12) | 0.0255 (10) | 0.0016 (10) | −0.0042 (7) | −0.0020 (10) |
| C13 | 0.0199 (10) | 0.0243 (13) | 0.0219 (9) | 0.0000 (9) | 0.0030 (7) | 0.0003 (10) |
Geometric parameters (Å, °)
| O1—C5 | 1.380 (2) | C6—C8 | 1.471 (2) |
| O1—C6 | 1.391 (2) | C7—H7 | 0.9500 |
| O2—C5 | 1.207 (2) | C8—C9 | 1.397 (2) |
| N1—C1 | 1.363 (2) | C8—C13 | 1.397 (3) |
| N1—C4 | 1.384 (2) | C9—C10 | 1.389 (3) |
| N1—C7 | 1.391 (2) | C9—H9 | 0.9500 |
| C1—C2 | 1.377 (3) | C10—C11 | 1.380 (3) |
| C1—H1 | 0.9500 | C10—H10 | 0.9500 |
| C2—C3 | 1.400 (3) | C11—C12 | 1.389 (3) |
| C2—H2 | 0.9500 | C11—H11 | 0.9500 |
| C3—C4 | 1.380 (3) | C12—C13 | 1.383 (3) |
| C3—H3 | 0.9500 | C12—H12 | 0.9500 |
| C4—C5 | 1.438 (2) | C13—H13 | 0.9500 |
| C6—C7 | 1.333 (2) | ||
| C5—O1—C6 | 121.88 (14) | C6—C7—N1 | 119.21 (18) |
| C1—N1—C4 | 108.95 (15) | C6—C7—H7 | 120.4 |
| C1—N1—C7 | 129.57 (17) | N1—C7—H7 | 120.4 |
| C4—N1—C7 | 121.48 (15) | C9—C8—C13 | 118.58 (17) |
| N1—C1—C2 | 107.74 (17) | C9—C8—C6 | 120.77 (17) |
| N1—C1—H1 | 126.1 | C13—C8—C6 | 120.65 (16) |
| C2—C1—H1 | 126.1 | C10—C9—C8 | 120.26 (19) |
| C1—C2—C3 | 108.45 (17) | C10—C9—H9 | 119.9 |
| C1—C2—H2 | 125.8 | C8—C9—H9 | 119.9 |
| C3—C2—H2 | 125.8 | C11—C10—C9 | 120.78 (17) |
| C4—C3—C2 | 106.83 (18) | C11—C10—H10 | 119.6 |
| C4—C3—H3 | 126.6 | C9—C10—H10 | 119.6 |
| C2—C3—H3 | 126.6 | C10—C11—C12 | 119.29 (18) |
| C3—C4—N1 | 108.03 (16) | C10—C11—H11 | 120.4 |
| C3—C4—C5 | 132.71 (19) | C12—C11—H11 | 120.4 |
| N1—C4—C5 | 119.21 (16) | C13—C12—C11 | 120.47 (19) |
| O2—C5—O1 | 117.52 (16) | C13—C12—H12 | 119.8 |
| O2—C5—C4 | 125.73 (18) | C11—C12—H12 | 119.8 |
| O1—C5—C4 | 116.75 (16) | C12—C13—C8 | 120.62 (17) |
| C7—C6—O1 | 121.35 (17) | C12—C13—H13 | 119.7 |
| C7—C6—C8 | 125.48 (18) | C8—C13—H13 | 119.7 |
| O1—C6—C8 | 113.17 (15) | ||
| C4—N1—C1—C2 | −0.7 (2) | C5—O1—C6—C8 | 179.70 (17) |
| C7—N1—C1—C2 | 178.7 (2) | O1—C6—C7—N1 | −1.1 (3) |
| N1—C1—C2—C3 | 0.9 (2) | C8—C6—C7—N1 | 179.16 (18) |
| C1—C2—C3—C4 | −0.7 (2) | C1—N1—C7—C6 | −179.8 (2) |
| C2—C3—C4—N1 | 0.3 (2) | C4—N1—C7—C6 | −0.5 (3) |
| C2—C3—C4—C5 | 177.6 (2) | C7—C6—C8—C9 | −175.2 (2) |
| C1—N1—C4—C3 | 0.2 (2) | O1—C6—C8—C9 | 5.0 (3) |
| C7—N1—C4—C3 | −179.20 (19) | C7—C6—C8—C13 | 4.5 (3) |
| C1—N1—C4—C5 | −177.49 (18) | O1—C6—C8—C13 | −175.29 (19) |
| C7—N1—C4—C5 | 3.1 (3) | C13—C8—C9—C10 | 0.5 (3) |
| C6—O1—C5—O2 | −177.16 (18) | C6—C8—C9—C10 | −179.8 (2) |
| C6—O1—C5—C4 | 2.6 (3) | C8—C9—C10—C11 | 0.0 (3) |
| C3—C4—C5—O2 | −1.3 (4) | C9—C10—C11—C12 | −0.1 (4) |
| N1—C4—C5—O2 | 175.7 (2) | C10—C11—C12—C13 | −0.2 (4) |
| C3—C4—C5—O1 | 178.9 (2) | C11—C12—C13—C8 | 0.7 (4) |
| N1—C4—C5—O1 | −4.0 (3) | C9—C8—C13—C12 | −0.8 (3) |
| C5—O1—C6—C7 | −0.1 (3) | C6—C8—C13—C12 | 179.4 (2) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C7—H7···O2i | 0.95 | 2.27 | 3.109 (2) | 147 |
Symmetry codes: (i) x−1, y−1, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ2449).
References
- Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19.
- Bélanger, P. C., Atkinson, J. G., Rooney, C. S., Britcher, S. F. & Remy, D. C. (1983). J. Org. Chem 48, 3234–3241.
- Fu, D.-C., Yu, H. & Zhang, S.-F. (2002). Chin. Chem. Lett 13, 1051–1054.
- Khan, S. T., Yu, P., Hua, E., Ali, S. N. & Nisa, M. (2010). Acta Cryst. E66, o711. [DOI] [PMC free article] [PubMed]
- Micheli, F., Bertani, B., Bozzoli, A., Crippa, L., Cavanni, P., Di Fabio, R., Donati, D., Marzorati, P., Merlo, G., Paio, A., Perugini, L. & Zarantonello, P. (2008). Bioorg. Med. Chem. Lett 18, 1804–1809. [DOI] [PubMed]
- Rigaku (2005). CrystalClear Rigaku Corporation, Tokyo, Japan.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810017940/rz2449sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810017940/rz2449Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


