Abstract
In the title molecule, C17H13NO2, the allyl group is almost perpendicular to the carbazole mean plane, with a dihedral angle of 89.0 (2)°. In the crystal, nonclassical C—H⋯O hydrogen bonds link the molecules into corrugated sheets parallel to the bc plane. Weak intermolecular π–π interactions are observed between the benzene rings [centroid–centroid distance = 3.874 (4) Å] from neighbouring sheets.
Related literature
For applications of carbazole derivatives, see: Hong et al. (2012 ▶); Samanta et al. (2001 ▶); Koyuncua et al. (2011 ▶); Zhang et al. (2010 ▶). For related structures, see: Wang et al. (2008 ▶); Zhao et al. (2012 ▶).
Experimental
Crystal data
C17H13NO2
M r = 263.28
Monoclinic,
a = 8.4062 (8) Å
b = 10.3279 (10) Å
c = 15.2432 (19) Å
β = 94.958 (9)°
V = 1318.4 (2) Å3
Z = 4
Mo Kα radiation
μ = 0.09 mm−1
T = 293 K
0.44 × 0.28 × 0.26 mm
Data collection
Oxford Gemini S Ultra area-detector diffractometer
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010 ▶) T min = 0.963, T max = 0.978
5464 measured reflections
2835 independent reflections
1909 reflections with I > 2σ(I)
R int = 0.024
Refinement
R[F 2 > 2σ(F 2)] = 0.045
wR(F 2) = 0.118
S = 1.02
2835 reflections
182 parameters
H-atom parameters constrained
Δρmax = 0.16 e Å−3
Δρmin = −0.15 e Å−3
Data collection: CrysAlis PRO (Oxford Diffraction, 2010 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; 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 datablock(s) I, global. DOI: 10.1107/S160053681203190X/cv5316sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681203190X/cv5316Isup2.hkl
Supplementary material file. DOI: 10.1107/S160053681203190X/cv5316Isup3.cml
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 |
|---|---|---|---|---|
| C2—H2⋯O1i | 0.93 | 2.58 | 3.489 (3) | 166 |
| C5—H5⋯O2ii | 0.93 | 2.54 | 3.332 (2) | 143 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
This work has been supported by the Natural Science Foundation of Guangdong Province, China (grant No. 06300581).
supplementary crystallographic information
Comment
The carbazole ring has a highly conjugated π system with desirable optical and charge-transport properties, and these characteristics make carozole derivatives the excellent candidates to yield materials for applications in different areas of science, such as dye-sensitized solar cell (Hong et al., 2012), electroluminescent (Samanta et al., 2001), electrochromic displays (Koyuncua et al., 2011) and antibacterial and antitumor agents (Zhang et al., 2010). These are the reasons why they have attracted our interest. Here we report the crystal structure of the title compound which consists of a carbazole skeleton with a allyl group and two formacyls (Fig. 1).
In the title molecule, the bond lengths and angles are unexceptional, and generally agree with those observed in the related compounds (Wang et al., 2008; Zhao et al., 2012). The non-H atoms of the carbazole ring and the two formacyls are approximately coplanar with r.m.s. deviation from the best fit plane of 0.006 (3) °, the allyl group is almost perpendicular to the carbazole mean plane with a dihedral angle of 89.0 (2)°. In the crystal, C2—H···O1 and C5—H···O2 non-classical H-bonds (Table 1) link the molecules into corrugated sheets parallel to bc plane (Fig. 2). Weak intermolecular π–π interactions between the benzene rings [centroid-centroid distance = 3.874 (4) Å] from the neighbouring sheets stabilize further the crystal packing.
Experimental
Phosphorus oxychloride (2.0 ml, 20 mmol) was added dropwise to the mixture of dry dimethylformamide (DMF, 3.0 ml, 40 mmol) and 9-allylcarbazole (2.07 g, 10 mmol) in chlorobenzene (20 ml) at 273 K under stirring. This solution was warmed up slowly to the room temperature in 0.5 h and stirred for another 0.5 h. After standing for 18 h at 343 K, more 3 ml DMF and 2 ml phosphorus oxychloride were added and stirred for 18 h continuously at the same temperature. After cooling, the resulting mixture was neutralized with saturated sodium bicarbonate solution until pH reached a value of 6 - 7, then the chlorobenzene was removed by water steam distillation, and the product was extracted with chloroform. After washing three times with water, the organic layer was dried over magnesium sulfate and evaporated in vacuo. The residue was separated by silica-gel column chromatography using petroleum ether-ethyl acetate (10:1) as eluting solvent and the title compound (I) was obtained (55.2% yield). Light brown crystals suitable for X-ray analysis (m.p. 429 K) grew over a period of one week when the ethyl acetate solution of I was exposed to the air at room temperature.
Refinement
All H atoms were positioned geometrically [C—H = 0.97 Å for CH2, 0.93 Å for CH2(alkene), 0.93 Å for CH] and refined using a riding model, with Uiso = 1.2Ueq of the parent atom.
Figures
Fig. 1.
The molecular structure of the title compound, with the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.
Fig. 2.
A portion of the crystal packing showing the sheet formed by the weak C—H···O hydrogen bonds (dashed lines).
Crystal data
| C17H13NO2 | Dx = 1.326 Mg m−3 |
| Mr = 263.28 | Melting point: 429 K |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
| a = 8.4062 (8) Å | Cell parameters from 1300 reflections |
| b = 10.3279 (10) Å | θ = 3.3–29.4° |
| c = 15.2432 (19) Å | µ = 0.09 mm−1 |
| β = 94.958 (9)° | T = 293 K |
| V = 1318.4 (2) Å3 | Block, light brown |
| Z = 4 | 0.44 × 0.28 × 0.26 mm |
| F(000) = 552 |
Data collection
| Oxford Gemini S Ultra area-detector diffractometer | 2835 independent reflections |
| Radiation source: fine-focus sealed tube | 1909 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.024 |
| φ and ω scans | θmax = 27.0°, θmin = 3.3° |
| Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) | h = −6→10 |
| Tmin = 0.963, Tmax = 0.978 | k = −12→12 |
| 5464 measured reflections | l = −19→18 |
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)] = 0.045 | H-atom parameters constrained |
| wR(F2) = 0.118 | w = 1/[σ2(Fo2) + (0.0432P)2 + 0.2427P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.02 | (Δ/σ)max < 0.001 |
| 2835 reflections | Δρmax = 0.16 e Å−3 |
| 182 parameters | Δρmin = −0.15 e Å−3 |
| 0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.047 (4) |
Special details
| 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 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 | ||
| N1 | 0.59424 (16) | 0.67631 (13) | 1.01449 (10) | 0.0497 (4) | |
| C7 | 0.69533 (17) | 0.55686 (15) | 0.90689 (11) | 0.0421 (4) | |
| C5 | 0.84834 (18) | 0.39928 (15) | 1.01791 (11) | 0.0451 (4) | |
| H5 | 0.8926 | 0.3478 | 0.9763 | 0.054* | |
| C1 | 0.68710 (19) | 0.58033 (16) | 1.05593 (12) | 0.0461 (4) | |
| C12 | 0.59952 (19) | 0.66450 (16) | 0.92455 (12) | 0.0461 (4) | |
| C9 | 0.64340 (19) | 0.59883 (17) | 0.75251 (12) | 0.0483 (4) | |
| C6 | 0.75183 (18) | 0.50343 (15) | 0.99146 (11) | 0.0422 (4) | |
| C4 | 0.87835 (19) | 0.37238 (17) | 1.10679 (12) | 0.0483 (4) | |
| C8 | 0.71472 (19) | 0.52431 (16) | 0.82040 (11) | 0.0455 (4) | |
| H8 | 0.7756 | 0.4525 | 0.8079 | 0.055* | |
| C2 | 0.7177 (2) | 0.55521 (19) | 1.14551 (12) | 0.0552 (5) | |
| H2 | 0.6753 | 0.6072 | 1.1875 | 0.066* | |
| O1 | 1.00518 (18) | 0.22217 (15) | 1.20823 (10) | 0.0826 (5) | |
| C11 | 0.5259 (2) | 0.73978 (17) | 0.85642 (13) | 0.0537 (5) | |
| H11 | 0.4626 | 0.8105 | 0.8682 | 0.064* | |
| O2 | 0.62394 (17) | 0.62669 (15) | 0.59663 (10) | 0.0806 (5) | |
| C17 | 0.6687 (2) | 0.5651 (2) | 0.66156 (13) | 0.0587 (5) | |
| H17 | 0.7245 | 0.4891 | 0.6529 | 0.070* | |
| C3 | 0.8126 (2) | 0.45114 (19) | 1.16965 (12) | 0.0555 (5) | |
| H3 | 0.8340 | 0.4321 | 1.2291 | 0.067* | |
| C14 | 0.5887 (2) | 0.89280 (17) | 1.08156 (13) | 0.0592 (5) | |
| H14 | 0.5316 | 0.9572 | 1.1077 | 0.071* | |
| C10 | 0.5500 (2) | 0.70602 (17) | 0.77173 (13) | 0.0546 (5) | |
| H10 | 0.5031 | 0.7556 | 0.7256 | 0.066* | |
| C13 | 0.5018 (2) | 0.77164 (17) | 1.05870 (13) | 0.0573 (5) | |
| H13A | 0.4682 | 0.7335 | 1.1122 | 0.069* | |
| H13B | 0.4064 | 0.7923 | 1.0209 | 0.069* | |
| C16 | 0.9756 (2) | 0.26040 (19) | 1.13370 (14) | 0.0601 (5) | |
| H16 | 1.0191 | 0.2138 | 1.0893 | 0.072* | |
| C15 | 0.7349 (3) | 0.9192 (2) | 1.06934 (15) | 0.0763 (7) | |
| H15A | 0.7975 | 0.8582 | 1.0435 | 0.092* | |
| H15B | 0.7778 | 0.9992 | 1.0864 | 0.092* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| N1 | 0.0457 (8) | 0.0427 (8) | 0.0613 (10) | 0.0001 (7) | 0.0086 (7) | −0.0127 (7) |
| C7 | 0.0380 (8) | 0.0360 (8) | 0.0528 (11) | −0.0056 (7) | 0.0068 (7) | −0.0053 (7) |
| C5 | 0.0409 (8) | 0.0425 (9) | 0.0527 (11) | −0.0054 (8) | 0.0089 (7) | −0.0038 (8) |
| C1 | 0.0413 (8) | 0.0424 (9) | 0.0554 (11) | −0.0082 (8) | 0.0087 (8) | −0.0086 (8) |
| C12 | 0.0397 (8) | 0.0384 (9) | 0.0605 (12) | −0.0079 (8) | 0.0065 (7) | −0.0081 (8) |
| C9 | 0.0441 (9) | 0.0470 (10) | 0.0539 (11) | −0.0096 (9) | 0.0047 (8) | 0.0030 (8) |
| C6 | 0.0382 (8) | 0.0398 (9) | 0.0490 (10) | −0.0058 (8) | 0.0069 (7) | −0.0058 (8) |
| C4 | 0.0445 (9) | 0.0484 (9) | 0.0524 (11) | −0.0071 (8) | 0.0059 (8) | 0.0036 (8) |
| C8 | 0.0432 (8) | 0.0403 (9) | 0.0541 (11) | −0.0025 (8) | 0.0098 (7) | −0.0031 (8) |
| C2 | 0.0542 (10) | 0.0593 (11) | 0.0536 (12) | −0.0077 (10) | 0.0141 (8) | −0.0134 (9) |
| O1 | 0.0964 (11) | 0.0819 (10) | 0.0701 (10) | 0.0061 (9) | 0.0108 (8) | 0.0289 (9) |
| C11 | 0.0467 (9) | 0.0379 (9) | 0.0762 (13) | 0.0018 (8) | 0.0045 (9) | −0.0026 (9) |
| O2 | 0.0836 (10) | 0.0966 (11) | 0.0625 (10) | 0.0006 (9) | 0.0108 (8) | 0.0236 (9) |
| C17 | 0.0551 (10) | 0.0630 (12) | 0.0588 (13) | −0.0077 (10) | 0.0090 (9) | 0.0089 (10) |
| C3 | 0.0556 (10) | 0.0632 (12) | 0.0481 (11) | −0.0115 (10) | 0.0070 (8) | −0.0009 (9) |
| C14 | 0.0607 (11) | 0.0458 (10) | 0.0705 (14) | 0.0025 (10) | 0.0025 (10) | −0.0154 (9) |
| C10 | 0.0494 (10) | 0.0454 (10) | 0.0681 (13) | −0.0051 (9) | 0.0000 (9) | 0.0081 (9) |
| C13 | 0.0501 (10) | 0.0510 (10) | 0.0725 (13) | 0.0022 (9) | 0.0144 (9) | −0.0166 (10) |
| C16 | 0.0610 (11) | 0.0576 (11) | 0.0627 (13) | −0.0049 (10) | 0.0105 (9) | 0.0114 (10) |
| C15 | 0.0719 (14) | 0.0600 (13) | 0.0958 (18) | −0.0142 (12) | 0.0002 (12) | −0.0126 (12) |
Geometric parameters (Å, º)
| N1—C1 | 1.380 (2) | C2—C3 | 1.370 (3) |
| N1—C12 | 1.381 (2) | C2—H2 | 0.9300 |
| N1—C13 | 1.455 (2) | O1—C16 | 1.208 (2) |
| C7—C8 | 1.384 (2) | C11—C10 | 1.369 (2) |
| C7—C12 | 1.412 (2) | C11—H11 | 0.9300 |
| C7—C6 | 1.444 (2) | O2—C17 | 1.209 (2) |
| C5—C4 | 1.385 (2) | C17—H17 | 0.9300 |
| C5—C6 | 1.386 (2) | C3—H3 | 0.9300 |
| C5—H5 | 0.9300 | C14—C15 | 1.288 (3) |
| C1—C2 | 1.392 (2) | C14—C13 | 1.475 (2) |
| C1—C6 | 1.409 (2) | C14—H14 | 0.9300 |
| C12—C11 | 1.398 (2) | C10—H10 | 0.9300 |
| C9—C8 | 1.384 (2) | C13—H13A | 0.9700 |
| C9—C10 | 1.403 (2) | C13—H13B | 0.9700 |
| C9—C17 | 1.463 (3) | C16—H16 | 0.9300 |
| C4—C3 | 1.406 (3) | C15—H15A | 0.9300 |
| C4—C16 | 1.455 (3) | C15—H15B | 0.9300 |
| C8—H8 | 0.9300 | ||
| C1—N1—C12 | 108.99 (13) | C1—C2—H2 | 121.2 |
| C1—N1—C13 | 125.26 (16) | C10—C11—C12 | 117.82 (16) |
| C12—N1—C13 | 125.72 (15) | C10—C11—H11 | 121.1 |
| C8—C7—C12 | 119.27 (16) | C12—C11—H11 | 121.1 |
| C8—C7—C6 | 134.49 (15) | O2—C17—C9 | 126.2 (2) |
| C12—C7—C6 | 106.23 (15) | O2—C17—H17 | 116.9 |
| C4—C5—C6 | 119.54 (16) | C9—C17—H17 | 116.9 |
| C4—C5—H5 | 120.2 | C2—C3—C4 | 121.67 (17) |
| C6—C5—H5 | 120.2 | C2—C3—H3 | 119.2 |
| N1—C1—C2 | 129.20 (16) | C4—C3—H3 | 119.2 |
| N1—C1—C6 | 108.83 (15) | C15—C14—C13 | 127.18 (19) |
| C2—C1—C6 | 121.96 (17) | C15—C14—H14 | 116.4 |
| N1—C12—C11 | 129.66 (16) | C13—C14—H14 | 116.4 |
| N1—C12—C7 | 109.06 (15) | C11—C10—C9 | 121.94 (17) |
| C11—C12—C7 | 121.27 (17) | C11—C10—H10 | 119.0 |
| C8—C9—C10 | 119.79 (17) | C9—C10—H10 | 119.0 |
| C8—C9—C17 | 119.17 (17) | N1—C13—C14 | 114.22 (14) |
| C10—C9—C17 | 121.04 (17) | N1—C13—H13A | 108.7 |
| C5—C6—C1 | 119.09 (16) | C14—C13—H13A | 108.7 |
| C5—C6—C7 | 134.05 (15) | N1—C13—H13B | 108.7 |
| C1—C6—C7 | 106.87 (14) | C14—C13—H13B | 108.7 |
| C5—C4—C3 | 120.10 (17) | H13A—C13—H13B | 107.6 |
| C5—C4—C16 | 119.06 (17) | O1—C16—C4 | 126.1 (2) |
| C3—C4—C16 | 120.82 (17) | O1—C16—H16 | 116.9 |
| C7—C8—C9 | 119.89 (16) | C4—C16—H16 | 116.9 |
| C7—C8—H8 | 120.1 | C14—C15—H15A | 120.0 |
| C9—C8—H8 | 120.1 | C14—C15—H15B | 120.0 |
| C3—C2—C1 | 117.63 (17) | H15A—C15—H15B | 120.0 |
| C3—C2—H2 | 121.2 | ||
| C12—N1—C1—C2 | 179.57 (16) | C6—C5—C4—C16 | 178.05 (14) |
| C13—N1—C1—C2 | −2.3 (3) | C12—C7—C8—C9 | 1.4 (2) |
| C12—N1—C1—C6 | −0.97 (17) | C6—C7—C8—C9 | −179.34 (16) |
| C13—N1—C1—C6 | 177.21 (14) | C10—C9—C8—C7 | −0.8 (2) |
| C1—N1—C12—C11 | −179.46 (16) | C17—C9—C8—C7 | 178.34 (15) |
| C13—N1—C12—C11 | 2.4 (3) | N1—C1—C2—C3 | 178.68 (15) |
| C1—N1—C12—C7 | 1.20 (17) | C6—C1—C2—C3 | −0.7 (2) |
| C13—N1—C12—C7 | −176.96 (14) | N1—C12—C11—C10 | −179.46 (16) |
| C8—C7—C12—N1 | 178.47 (13) | C7—C12—C11—C10 | −0.2 (2) |
| C6—C7—C12—N1 | −0.95 (17) | C8—C9—C17—O2 | −174.17 (17) |
| C8—C7—C12—C11 | −0.9 (2) | C10—C9—C17—O2 | 5.0 (3) |
| C6—C7—C12—C11 | 179.64 (14) | C1—C2—C3—C4 | 0.5 (3) |
| C4—C5—C6—C1 | 0.4 (2) | C5—C4—C3—C2 | 0.2 (3) |
| C4—C5—C6—C7 | −179.03 (16) | C16—C4—C3—C2 | −178.48 (16) |
| N1—C1—C6—C5 | −179.23 (13) | C12—C11—C10—C9 | 0.8 (2) |
| C2—C1—C6—C5 | 0.3 (2) | C8—C9—C10—C11 | −0.3 (3) |
| N1—C1—C6—C7 | 0.36 (17) | C17—C9—C10—C11 | −179.48 (16) |
| C2—C1—C6—C7 | 179.87 (14) | C1—N1—C13—C14 | 91.2 (2) |
| C8—C7—C6—C5 | 0.6 (3) | C12—N1—C13—C14 | −90.9 (2) |
| C12—C7—C6—C5 | 179.86 (16) | C15—C14—C13—N1 | −2.6 (3) |
| C8—C7—C6—C1 | −178.93 (16) | C5—C4—C16—O1 | −176.38 (18) |
| C12—C7—C6—C1 | 0.36 (17) | C3—C4—C16—O1 | 2.3 (3) |
| C6—C5—C4—C3 | −0.7 (2) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C2—H2···O1i | 0.93 | 2.58 | 3.489 (3) | 166 |
| C5—H5···O2ii | 0.93 | 2.54 | 3.332 (2) | 143 |
Symmetry codes: (i) −x+3/2, y+1/2, −z+5/2; (ii) −x+3/2, y−1/2, −z+3/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CV5316).
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 datablock(s) I, global. DOI: 10.1107/S160053681203190X/cv5316sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681203190X/cv5316Isup2.hkl
Supplementary material file. DOI: 10.1107/S160053681203190X/cv5316Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


