Abstract
The crystal structure of the title compound, C12H11NS, features parallel chains of alternating N—H⋯S hydrogen-bonded mirror-image conformers along [10
]. The molecular conformation is that of an envelope, with all of the framework atoms except one close to a mean plane (rms deviation 0.054 Å); one C atom of the cyclohexenethione ring forms the envelope flap, which makes a dihedral angle of 48.6 (1)° with the rest of the molecule. There is a π–π* interaction between pairs of enantiomers in adjacent chains; the distance between parallel planes is 3.466 (1) Å.
Related literature
For related structures, see: Hökelek et al. (1998 ▶); Ianelli et al. (1994 ▶); Çaylak et al. (2007 ▶); Rodriguez et al. (1989 ▶). Hückel calculations were performed using Chem3DPro (Cambridgesoft, 2009 ▶).
Experimental
Crystal data
C12H11NS
M r = 201.28
Monoclinic,
a = 8.6353 (14) Å
b = 12.1395 (15) Å
c = 9.5808 (14) Å
β = 104.599 (10)°
V = 971.9 (2) Å3
Z = 4
Mo Kα radiation
μ = 0.29 mm−1
T = 90 K
0.38 × 0.33 × 0.15 mm
Data collection
Nonius KappaCCD diffractometer
Absorption correction: multi-scan (SCALEPACK; Otwinowski & Minor, 1997 ▶) T min = 0.900, T max = 0.958
6145 measured reflections
3305 independent reflections
2915 reflections with I > 2σ(I)
R int = 0.018
Refinement
R[F 2 > 2σ(F 2)] = 0.033
wR(F 2) = 0.087
S = 1.04
3305 reflections
128 parameters
H-atom parameters constrained
Δρmax = 0.42 e Å−3
Δρmin = −0.30 e Å−3
Data collection: COLLECT (Nonius, 2000 ▶); cell refinement: SCALEPACK (Otwinowski & Minor, 1997 ▶); data reduction: DENZO (Otwinowski & Minor, 1997 ▶) and SCALEPACK; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536811006623/fl2336sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811006623/fl2336Isup2.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 |
|---|---|---|---|---|
| N9—H9⋯S1i | 0.88 | 2.45 | 3.3187 (9) | 172 |
Symmetry code: (i)
.
Acknowledgments
The purchase of the diffractometer was made possible by grant No. LEQSF(1999–2000)-ENH-TR-13, administered by the Louisiana Board of Regents.
supplementary crystallographic information
Comment
The title compound (1, Fig.1) is the sulfur analog of substituted carbazole 1,2,3-trihydrocarbazol-4(9H)-one (2) (Rodriguez et al., 1989). Both 1 and 2 show the same molecular conformation (envelope, with flap angles 48.6 (1)° for 1 and 48.2 (1)° for 2) and similar H-bonded chains (Table 1) of alternating enantiomers (N···S = 3.319 (1) Å, N—H···S = 172.0 (1)°, and N···S═C = 98.0 (1)° for 1, N···O = 2.829 (1) Å, N—H···O = 162.3 (1)° and H···O═C = 117.5 (1)° for 2).
In 1, all H-bonded chains are parallel, extending along the [101] crystallographic direction, and adjacent chains 5.583 (1) Å apart are arranged in corrugated sheets parallel to the (010) crystallographic plane (Fig. 22)). The mean planes of adjacent sheets are 5.099 (1) Å apart, but enantiomers in adjacent sheets have parallel π-nodal planes and are only 3.466 (1) Å apart, indicative of a π-π* interaction. Extended Hückel calculations (Chem3DPro, Cambridgesoft, 2009) suggest that the π-HOMO and π*-LUMO orbitals in 1 are larger and closer in energy than those in 2. This may explain why molecules of 2 show no π-type interaction and are thus packed in a different pattern: H-bonded chains 5.359 (1) Å apart extend along the [011] and [011] directions in alternating sheets, so adjacent sheets are rotated by 76.5 (1)°. The distance between adjacent sheets is 4.979 (1) Å and the only interactions between them are C—H···C van der Waals and C—H···O contacts.
Experimental
A solution of 1,2-dihydrocarbazol-4(3H)-one (5.4 mmol) in anhydrous 1,2-dimethoxyethane (30 ml) was stirred at room temperature for 15 min. Upon dissolution, the solution was chilled in an ice-water bath. Lawesson reagent, 2,4-bis(4-methoxyphenyl)-1,3,2,4-dithiadiphosphetane 2,4-disulfide, (2.9 mmol) was added to the vigorously stirred cold solution. The resulting mixture was stirred for 5 min and then allowed to warm to room temperature. After stirring for an additional 10 min, the white suspension dissolved, and the reaction mixture turned deep orange. The reaction mixture was poured into 150 ml of chilled water and the orange suspension was extracted with CHCl3 (3 x 80 ml). Evaporation under reduced pressure left a deep orange residue, which was purified on a silica column (100 g). The orange band was eluted with ethyl acetate. Evaporation of the solvent in vacuo gave the title compound as a yellow powder (92%). Recrystallization from dichloromethane yielded yellow needles, m.p. 173–175°C.
Refinement
All H atoms were placed in calculated positions, guided by difference maps, with C—H bond distances 0.95–0.99 Å, N—H 0.88 Å, Uiso=1.2Ueq, and thereafter refined as riding.
Figures
Fig. 1.
View of 1 (50% probability displacement ellipsoids).
Fig. 2.
The unit cell, illustrating hydrogen bonds.
Crystal data
| C12H11NS | F(000) = 424 |
| Mr = 201.28 | Dx = 1.376 Mg m−3 |
| Monoclinic, P21/n | Melting point: 447(1) K |
| Hall symbol: -P 2yn | Mo Kα radiation, λ = 0.71073 Å |
| a = 8.6353 (14) Å | Cell parameters from 3145 reflections |
| b = 12.1395 (15) Å | θ = 2.8–31.8° |
| c = 9.5808 (14) Å | µ = 0.29 mm−1 |
| β = 104.599 (10)° | T = 90 K |
| V = 971.9 (2) Å3 | Prism, yellow |
| Z = 4 | 0.38 × 0.33 × 0.15 mm |
Data collection
| Nonius KappaCCD diffractometer | 2915 reflections with I > 2σ(I) |
| ω and φ scans | Rint = 0.018 |
| Absorption correction: multi-scan (SCALEPACK; Otwinowski & Minor, 1997) | θmax = 31.8°, θmin = 2.8° |
| Tmin = 0.900, Tmax = 0.958 | h = −12→12 |
| 6145 measured reflections | k = −17→15 |
| 3305 independent reflections | l = −14→14 |
Refinement
| Refinement on F2 | H-atom parameters constrained |
| Least-squares matrix: full | w = 1/[σ2(Fo2) + (0.0381P)2 + 0.4607P] where P = (Fo2 + 2Fc2)/3 |
| R[F2 > 2σ(F2)] = 0.033 | (Δ/σ)max = 0.001 |
| wR(F2) = 0.087 | Δρmax = 0.42 e Å−3 |
| S = 1.03 | Δρmin = −0.30 e Å−3 |
| 3305 reflections | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
| 128 parameters | Extinction coefficient: 0.007 (2) |
| 0 restraints |
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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
| x | y | z | Uiso*/Ueq | ||
| S1 | 0.73572 (3) | 0.09251 (2) | 0.17793 (3) | 0.01632 (8) | |
| N9 | 0.40190 (10) | 0.23264 (7) | 0.49231 (9) | 0.01459 (16) | |
| H9 | 0.3596 | 0.2739 | 0.5486 | 0.018* | |
| C1 | 0.64126 (13) | 0.35282 (8) | 0.50486 (11) | 0.01640 (19) | |
| H1A | 0.6442 | 0.3693 | 0.6067 | 0.02* | |
| H1B | 0.5975 | 0.4178 | 0.4456 | 0.02* | |
| C2 | 0.81014 (12) | 0.32729 (9) | 0.49014 (11) | 0.01613 (19) | |
| H2A | 0.8612 | 0.2724 | 0.5639 | 0.019* | |
| H2B | 0.8756 | 0.3953 | 0.5072 | 0.019* | |
| C3 | 0.80512 (12) | 0.28219 (8) | 0.33970 (11) | 0.01504 (18) | |
| H3A | 0.766 | 0.3409 | 0.2677 | 0.018* | |
| H3B | 0.9153 | 0.2631 | 0.3355 | 0.018* | |
| C4 | 0.69952 (12) | 0.18152 (8) | 0.29869 (10) | 0.01239 (17) | |
| C5 | 0.40380 (12) | −0.00895 (8) | 0.27655 (10) | 0.01451 (18) | |
| H5 | 0.4724 | −0.0398 | 0.2234 | 0.017* | |
| C6 | 0.26491 (13) | −0.06343 (9) | 0.28577 (11) | 0.0179 (2) | |
| H6 | 0.2394 | −0.1325 | 0.2389 | 0.021* | |
| C7 | 0.16174 (13) | −0.01841 (9) | 0.36297 (12) | 0.0196 (2) | |
| H7 | 0.0665 | −0.0567 | 0.3655 | 0.024* | |
| C8 | 0.19647 (13) | 0.08102 (9) | 0.43570 (11) | 0.0181 (2) | |
| H8 | 0.1273 | 0.1116 | 0.4885 | 0.022* | |
| C10 | 0.53890 (12) | 0.25494 (8) | 0.45510 (10) | 0.01313 (17) | |
| C11 | 0.56930 (11) | 0.17216 (8) | 0.36283 (10) | 0.01191 (17) | |
| C12 | 0.44039 (11) | 0.09230 (8) | 0.34726 (10) | 0.01234 (17) | |
| C13 | 0.33703 (12) | 0.13394 (8) | 0.42784 (10) | 0.01382 (18) |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.01819 (13) | 0.01449 (12) | 0.01981 (13) | −0.00184 (8) | 0.01132 (9) | −0.00327 (8) |
| N9 | 0.0156 (4) | 0.0158 (4) | 0.0144 (4) | 0.0018 (3) | 0.0077 (3) | −0.0002 (3) |
| C1 | 0.0194 (5) | 0.0149 (4) | 0.0159 (4) | −0.0014 (4) | 0.0063 (4) | −0.0029 (3) |
| C2 | 0.0162 (4) | 0.0168 (4) | 0.0150 (4) | −0.0032 (4) | 0.0031 (3) | −0.0016 (3) |
| C3 | 0.0149 (4) | 0.0145 (4) | 0.0167 (4) | −0.0031 (3) | 0.0059 (3) | −0.0012 (3) |
| C4 | 0.0128 (4) | 0.0125 (4) | 0.0123 (4) | 0.0008 (3) | 0.0041 (3) | 0.0011 (3) |
| C5 | 0.0149 (4) | 0.0145 (4) | 0.0141 (4) | −0.0005 (3) | 0.0035 (3) | 0.0017 (3) |
| C6 | 0.0182 (5) | 0.0169 (5) | 0.0175 (4) | −0.0039 (4) | 0.0027 (4) | 0.0026 (4) |
| C7 | 0.0156 (5) | 0.0230 (5) | 0.0204 (5) | −0.0045 (4) | 0.0049 (4) | 0.0056 (4) |
| C8 | 0.0140 (4) | 0.0235 (5) | 0.0182 (4) | 0.0001 (4) | 0.0068 (4) | 0.0046 (4) |
| C10 | 0.0140 (4) | 0.0142 (4) | 0.0115 (4) | 0.0012 (3) | 0.0039 (3) | 0.0012 (3) |
| C11 | 0.0120 (4) | 0.0126 (4) | 0.0115 (4) | 0.0001 (3) | 0.0037 (3) | 0.0005 (3) |
| C12 | 0.0117 (4) | 0.0142 (4) | 0.0115 (4) | 0.0006 (3) | 0.0035 (3) | 0.0026 (3) |
| C13 | 0.0136 (4) | 0.0160 (4) | 0.0126 (4) | 0.0011 (3) | 0.0046 (3) | 0.0026 (3) |
Geometric parameters (Å, °)
| C1—C10 | 1.4860 (14) | C5—H5 | 0.95 |
| C1—C2 | 1.5318 (14) | C6—C7 | 1.4042 (16) |
| C1—H1A | 0.99 | C6—H6 | 0.95 |
| C1—H1B | 0.99 | C7—C8 | 1.3882 (16) |
| C2—C3 | 1.5322 (14) | C7—H7 | 0.95 |
| C2—H2A | 0.99 | C8—C13 | 1.3920 (14) |
| C2—H2B | 0.99 | C8—H8 | 0.95 |
| C3—C4 | 1.5162 (14) | C10—N9 | 1.3463 (12) |
| C3—H3A | 0.99 | C10—C11 | 1.4061 (13) |
| C3—H3B | 0.99 | C11—C12 | 1.4553 (13) |
| C4—C11 | 1.4154 (13) | C12—C13 | 1.4127 (13) |
| C4—S1 | 1.6692 (10) | C13—N9 | 1.3988 (13) |
| C5—C6 | 1.3917 (14) | N9—H9 | 0.88 |
| C5—C12 | 1.4006 (13) | ||
| C10—C1—C2 | 108.17 (8) | C5—C6—C7 | 121.32 (10) |
| C10—C1—H1A | 110.1 | C5—C6—H6 | 119.3 |
| C2—C1—H1A | 110.1 | C7—C6—H6 | 119.3 |
| C10—C1—H1B | 110.1 | C8—C7—C6 | 121.15 (10) |
| C2—C1—H1B | 110.1 | C8—C7—H7 | 119.4 |
| H1A—C1—H1B | 108.4 | C6—C7—H7 | 119.4 |
| C1—C2—C3 | 110.92 (8) | C7—C8—C13 | 117.08 (10) |
| C1—C2—H2A | 109.5 | C7—C8—H8 | 121.5 |
| C3—C2—H2A | 109.5 | C13—C8—H8 | 121.5 |
| C1—C2—H2B | 109.5 | N9—C10—C11 | 109.79 (9) |
| C3—C2—H2B | 109.5 | N9—C10—C1 | 124.55 (9) |
| H2A—C2—H2B | 108 | C11—C10—C1 | 125.66 (9) |
| C4—C3—C2 | 113.85 (8) | C10—C11—C4 | 120.68 (9) |
| C4—C3—H3A | 108.8 | C10—C11—C12 | 106.34 (8) |
| C2—C3—H3A | 108.8 | C4—C11—C12 | 132.83 (9) |
| C4—C3—H3B | 108.8 | C5—C12—C13 | 118.80 (9) |
| C2—C3—H3B | 108.8 | C5—C12—C11 | 135.05 (9) |
| H3A—C3—H3B | 107.7 | C13—C12—C11 | 106.14 (8) |
| C11—C4—C3 | 116.35 (8) | C8—C13—N9 | 128.98 (9) |
| C11—C4—S1 | 123.85 (7) | C8—C13—C12 | 122.96 (10) |
| C3—C4—S1 | 119.73 (7) | N9—C13—C12 | 108.06 (8) |
| C6—C5—C12 | 118.64 (9) | C10—N9—C13 | 109.64 (8) |
| C6—C5—H5 | 120.7 | C10—N9—H9 | 125.2 |
| C12—C5—H5 | 120.7 | C13—N9—H9 | 125.2 |
| C10—C1—C2—C3 | 49.84 (11) | C6—C5—C12—C13 | 1.45 (14) |
| C1—C2—C3—C4 | −55.67 (11) | C6—C5—C12—C11 | −179.79 (10) |
| C2—C3—C4—C11 | 28.23 (12) | C10—C11—C12—C5 | −177.03 (10) |
| C2—C3—C4—S1 | −154.52 (8) | C4—C11—C12—C5 | 7.46 (19) |
| C12—C5—C6—C7 | 0.52 (15) | C10—C11—C12—C13 | 1.84 (10) |
| C5—C6—C7—C8 | −1.47 (16) | C4—C11—C12—C13 | −173.67 (10) |
| C6—C7—C8—C13 | 0.35 (15) | C7—C8—C13—N9 | −178.60 (10) |
| C2—C1—C10—N9 | 158.35 (9) | C7—C8—C13—C12 | 1.70 (15) |
| C2—C1—C10—C11 | −21.72 (13) | C5—C12—C13—C8 | −2.64 (14) |
| N9—C10—C11—C4 | 174.61 (9) | C11—C12—C13—C8 | 178.27 (9) |
| C1—C10—C11—C4 | −5.33 (15) | C5—C12—C13—N9 | 177.61 (8) |
| N9—C10—C11—C12 | −1.56 (11) | C11—C12—C13—N9 | −1.47 (10) |
| C1—C10—C11—C12 | 178.50 (9) | C11—C10—N9—C13 | 0.66 (11) |
| C3—C4—C11—C10 | 2.22 (13) | C1—C10—N9—C13 | −179.40 (9) |
| S1—C4—C11—C10 | −174.91 (7) | C8—C13—N9—C10 | −179.18 (10) |
| C3—C4—C11—C12 | 177.20 (10) | C12—C13—N9—C10 | 0.55 (11) |
| S1—C4—C11—C12 | 0.08 (16) |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N9—H9···S1i | 0.88 | 2.45 | 3.3187 (9) | 172 |
Symmetry codes: (i) x−1/2, −y+1/2, z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FL2336).
References
- Cambridgesoft (2009). Chem3DPro Cambridgesoft Corporation, Cambridge, MA, USA.
- Çaylak, N., Hökelek, T., Uludağ, N. & Patır, S. (2007). Acta Cryst. E63, o3913–o3914.
- Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
- Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838.
- Hökelek, T., Gündüz, H., Patir, S. & Uludaug, N. (1998). Acta Cryst. C54, 1297–1299.
- Ianelli, S., Nardelli, M., Belletti, D., Caubère, C., Caubère, P. & Jamart-Grégoire, B. (1994). Acta Cryst. C50, 1919–1922. [DOI] [PubMed]
- Nonius (2000). COLLECT Nonius BV, Delft, The Netherlands.
- Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276, Macromolecular Crystallography, Part A, edited by C. W. Carter Jr & R. M. Sweet, pp. 307–326. New York: Academic Press.
- Rodriguez, J. G., Temprano, F., Esteban-Calderon, C. & Martinez-Ripoll, M. (1989). J. Chem. Soc. Perkin Trans. 1, pp. 2117–2122.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [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 global, I. DOI: 10.1107/S1600536811006623/fl2336sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536811006623/fl2336Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


