organic compounds
3-(1-Phenylethyl)-1,3-thiazinane-2-thione
aProvincial Key Laboratory of Surface & Interface Science, Zhengzhou University of Light Industry, Zhengzhou 450002, People's Republic of China, and bHenan Sports School, Zhengzhou 450044, People's Republic of China
*Correspondence e-mail: yanfufeng@yahoo.cn
In the title molecule, C12H15NS2, the 1,3-thiazinane ring has a half-boat conformation; the C atom at position 5 deviates by 0.715 (2) Å from the mean plane (P) of the remaining five atoms. Plane P and the phenyl ring form a dihedral angle of 83.62 (3)°. In the weak intermolecular C—H⋯S hydrogen bonds link molecules related by translation along the axis a into chains.
Related literature
For the crystal structures of related thiazinane derivatives, see: Kálmán et al. (1977); Peng & Wu (2009); Amir et al. (2006). For the biological activity of thiazinane-containing compounds, see: Soloway et al. (1978); Tomizawa et al. (1995).
Experimental
Crystal data
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Refinement
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Data collection: CrystalClear (Rigaku, 2005); cell 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 .
Supporting information
10.1107/S1600536809046248/cv2647sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536809046248/cv2647Isup2.hkl
A solution of 1,3-thiazinane-2-thione (1.33 g, 10 mmol) and sodium hydride (0.3 g) dissolved in anhydrous acetonitrile (20 ml), and dropwise added over a period of 10 min to a solution of 1-(1-chloroethyl)benzene (1.41g, 10 mmol) in acetonitrile (10 ml) at 273 K. The mixture was stirred at 353 K for 2 h. The solvent was removed and the residue was purified by flash
(3:1 Cyclohexane:Dichloromethane) to give title compound as a white solid (1.90 g, 80%). Single crystals suitable for X-ray measurements were obtained by recrystallization from ethanol at room temperature.C-bound H atoms were placed in calculated positions (C—H = 0.95–1.00 Å), and included in the final cycles of
using a riding model, with Uiso(H) = 1.2Ueq(C) for the aryl and methylene H atoms and 1.5Ueq(C) for the methyl H atoms.Data collection: CrystalClear (Rigaku, 2005); cell
CrystalClear (Rigaku, 2005); data reduction: CrystalClear (Rigaku, 2005); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).Fig. 1. The molecular structure of (I) with displacement ellipsoids drawn at the 40% probability level. |
C12H15NS2 | F(000) = 504 |
Mr = 237.37 | Dx = 1.344 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71070 Å |
Hall symbol: -P 2yn | Cell parameters from 3792 reflections |
a = 7.0169 (4) Å | θ = 2.3–27.9° |
b = 15.5107 (9) Å | µ = 0.42 mm−1 |
c = 11.0349 (7) Å | T = 113 K |
β = 102.391 (3)° | Prism, colourless |
V = 1173.03 (12) Å3 | 0.26 × 0.10 × 0.08 mm |
Z = 4 |
Rigaku Saturn diffractometer | 2798 independent reflections |
Radiation source: rotating anode | 2631 reflections with I > 2σ(I) |
Confocal monochromator | Rint = 0.040 |
Detector resolution: 14.63 pixels mm-1 | θmax = 27.9°, θmin = 2.3° |
ω scans | h = −9→9 |
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | k = −19→20 |
Tmin = 0.899, Tmax = 0.967 | l = −14→14 |
14476 measured reflections |
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.041 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.087 | H-atom parameters constrained |
S = 1.13 | w = 1/[σ2(Fo2) + (0.034P)2 + 0.4071P] where P = (Fo2 + 2Fc2)/3 |
2798 reflections | (Δ/σ)max < 0.001 |
137 parameters | Δρmax = 0.27 e Å−3 |
0 restraints | Δρmin = −0.32 e Å−3 |
C12H15NS2 | V = 1173.03 (12) Å3 |
Mr = 237.37 | Z = 4 |
Monoclinic, P21/n | Mo Kα radiation |
a = 7.0169 (4) Å | µ = 0.42 mm−1 |
b = 15.5107 (9) Å | T = 113 K |
c = 11.0349 (7) Å | 0.26 × 0.10 × 0.08 mm |
β = 102.391 (3)° |
Rigaku Saturn diffractometer | 2798 independent reflections |
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005) | 2631 reflections with I > 2σ(I) |
Tmin = 0.899, Tmax = 0.967 | Rint = 0.040 |
14476 measured reflections |
R[F2 > 2σ(F2)] = 0.041 | 0 restraints |
wR(F2) = 0.087 | H-atom parameters constrained |
S = 1.13 | Δρmax = 0.27 e Å−3 |
2798 reflections | Δρmin = −0.32 e Å−3 |
137 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
S1 | 1.23060 (6) | 0.17662 (3) | 0.70183 (4) | 0.03009 (13) | |
S2 | 1.02102 (6) | 0.13716 (3) | 0.45696 (4) | 0.02633 (12) | |
N1 | 0.86777 (18) | 0.11187 (8) | 0.65929 (12) | 0.0193 (3) | |
C1 | 1.0203 (2) | 0.13813 (10) | 0.61536 (15) | 0.0208 (3) | |
C2 | 0.6824 (2) | 0.08125 (10) | 0.58027 (14) | 0.0215 (3) | |
H2A | 0.5755 | 0.0905 | 0.6247 | 0.026* | |
H2B | 0.6923 | 0.0185 | 0.5663 | 0.026* | |
C3 | 0.6315 (2) | 0.12648 (10) | 0.45586 (15) | 0.0225 (3) | |
H3A | 0.4993 | 0.1088 | 0.4115 | 0.027* | |
H3B | 0.6302 | 0.1896 | 0.4690 | 0.027* | |
C4 | 0.7771 (2) | 0.10468 (11) | 0.37795 (15) | 0.0262 (4) | |
H4A | 0.7410 | 0.1346 | 0.2970 | 0.031* | |
H4B | 0.7749 | 0.0418 | 0.3621 | 0.031* | |
C5 | 0.8766 (2) | 0.11054 (10) | 0.79582 (14) | 0.0207 (3) | |
H5 | 1.0167 | 0.1176 | 0.8383 | 0.025* | |
C6 | 0.7662 (2) | 0.18756 (10) | 0.83194 (15) | 0.0245 (3) | |
H6A | 0.8277 | 0.2410 | 0.8124 | 0.037* | |
H6B | 0.7692 | 0.1854 | 0.9211 | 0.037* | |
H6C | 0.6305 | 0.1858 | 0.7855 | 0.037* | |
C7 | 0.8115 (2) | 0.02299 (10) | 0.83270 (14) | 0.0203 (3) | |
C8 | 0.9420 (3) | −0.04584 (11) | 0.84269 (15) | 0.0250 (4) | |
H8 | 1.0682 | −0.0366 | 0.8268 | 0.030* | |
C9 | 0.8901 (3) | −0.12754 (11) | 0.87548 (16) | 0.0316 (4) | |
H9 | 0.9796 | −0.1740 | 0.8804 | 0.038* | |
C10 | 0.7074 (3) | −0.14124 (11) | 0.90105 (16) | 0.0316 (4) | |
H10 | 0.6718 | −0.1970 | 0.9243 | 0.038* | |
C11 | 0.5777 (3) | −0.07356 (11) | 0.89258 (15) | 0.0283 (4) | |
H11 | 0.4528 | −0.0828 | 0.9105 | 0.034* | |
C12 | 0.6284 (2) | 0.00820 (10) | 0.85792 (14) | 0.0235 (3) | |
H12 | 0.5373 | 0.0542 | 0.8515 | 0.028* |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0166 (2) | 0.0355 (3) | 0.0367 (3) | −0.00502 (17) | 0.00244 (18) | −0.00113 (19) |
S2 | 0.0240 (2) | 0.0303 (2) | 0.0266 (2) | −0.00098 (17) | 0.00950 (17) | 0.00309 (17) |
N1 | 0.0157 (6) | 0.0211 (6) | 0.0203 (6) | −0.0016 (5) | 0.0020 (5) | −0.0005 (5) |
C1 | 0.0177 (7) | 0.0165 (7) | 0.0282 (8) | 0.0027 (6) | 0.0048 (6) | 0.0007 (6) |
C2 | 0.0181 (7) | 0.0238 (8) | 0.0217 (8) | −0.0045 (6) | 0.0022 (6) | −0.0013 (6) |
C3 | 0.0214 (8) | 0.0218 (8) | 0.0225 (8) | −0.0018 (6) | 0.0009 (6) | 0.0000 (6) |
C4 | 0.0290 (9) | 0.0280 (9) | 0.0211 (8) | −0.0021 (7) | 0.0043 (7) | 0.0007 (7) |
C5 | 0.0178 (7) | 0.0244 (8) | 0.0188 (7) | 0.0005 (6) | 0.0015 (6) | −0.0017 (6) |
C6 | 0.0259 (8) | 0.0218 (8) | 0.0245 (8) | 0.0006 (7) | 0.0025 (7) | −0.0032 (6) |
C7 | 0.0224 (8) | 0.0226 (8) | 0.0149 (7) | 0.0008 (6) | 0.0016 (6) | −0.0019 (6) |
C8 | 0.0257 (8) | 0.0275 (8) | 0.0204 (8) | 0.0067 (7) | 0.0019 (6) | −0.0023 (6) |
C9 | 0.0421 (11) | 0.0241 (8) | 0.0249 (8) | 0.0105 (8) | −0.0008 (8) | −0.0027 (7) |
C10 | 0.0484 (11) | 0.0207 (8) | 0.0227 (8) | −0.0016 (8) | 0.0012 (8) | 0.0016 (7) |
C11 | 0.0328 (9) | 0.0301 (9) | 0.0225 (8) | −0.0051 (7) | 0.0071 (7) | 0.0019 (7) |
C12 | 0.0251 (8) | 0.0241 (8) | 0.0210 (8) | 0.0033 (7) | 0.0043 (6) | 0.0002 (6) |
S1—C1 | 1.6851 (16) | C5—H5 | 1.0000 |
S2—C1 | 1.7491 (17) | C6—H6A | 0.9800 |
S2—C4 | 1.8172 (17) | C6—H6B | 0.9800 |
N1—C1 | 1.330 (2) | C6—H6C | 0.9800 |
N1—C2 | 1.4803 (19) | C7—C12 | 1.390 (2) |
N1—C5 | 1.495 (2) | C7—C8 | 1.395 (2) |
C2—C3 | 1.515 (2) | C8—C9 | 1.388 (2) |
C2—H2A | 0.9900 | C8—H8 | 0.9500 |
C2—H2B | 0.9900 | C9—C10 | 1.387 (3) |
C3—C4 | 1.508 (2) | C9—H9 | 0.9500 |
C3—H3A | 0.9900 | C10—C11 | 1.379 (3) |
C3—H3B | 0.9900 | C10—H10 | 0.9500 |
C4—H4A | 0.9900 | C11—C12 | 1.393 (2) |
C4—H4B | 0.9900 | C11—H11 | 0.9500 |
C5—C7 | 1.516 (2) | C12—H12 | 0.9500 |
C5—C6 | 1.523 (2) | ||
C1—S2—C4 | 106.11 (8) | N1—C5—H5 | 107.2 |
C1—N1—C2 | 123.90 (13) | C7—C5—H5 | 107.2 |
C1—N1—C5 | 120.59 (13) | C6—C5—H5 | 107.2 |
C2—N1—C5 | 115.50 (12) | C5—C6—H6A | 109.5 |
N1—C1—S1 | 125.27 (13) | C5—C6—H6B | 109.5 |
N1—C1—S2 | 122.45 (12) | H6A—C6—H6B | 109.5 |
S1—C1—S2 | 112.27 (9) | C5—C6—H6C | 109.5 |
N1—C2—C3 | 113.06 (13) | H6A—C6—H6C | 109.5 |
N1—C2—H2A | 109.0 | H6B—C6—H6C | 109.5 |
C3—C2—H2A | 109.0 | C12—C7—C8 | 118.47 (15) |
N1—C2—H2B | 109.0 | C12—C7—C5 | 123.11 (14) |
C3—C2—H2B | 109.0 | C8—C7—C5 | 118.42 (14) |
H2A—C2—H2B | 107.8 | C9—C8—C7 | 120.99 (16) |
C4—C3—C2 | 110.86 (13) | C9—C8—H8 | 119.5 |
C4—C3—H3A | 109.5 | C7—C8—H8 | 119.5 |
C2—C3—H3A | 109.5 | C10—C9—C8 | 119.90 (16) |
C4—C3—H3B | 109.5 | C10—C9—H9 | 120.0 |
C2—C3—H3B | 109.5 | C8—C9—H9 | 120.0 |
H3A—C3—H3B | 108.1 | C11—C10—C9 | 119.66 (16) |
C3—C4—S2 | 110.36 (11) | C11—C10—H10 | 120.2 |
C3—C4—H4A | 109.6 | C9—C10—H10 | 120.2 |
S2—C4—H4A | 109.6 | C10—C11—C12 | 120.52 (17) |
C3—C4—H4B | 109.6 | C10—C11—H11 | 119.7 |
S2—C4—H4B | 109.6 | C12—C11—H11 | 119.7 |
H4A—C4—H4B | 108.1 | C7—C12—C11 | 120.44 (15) |
N1—C5—C7 | 109.47 (12) | C7—C12—H12 | 119.8 |
N1—C5—C6 | 109.85 (13) | C11—C12—H12 | 119.8 |
C7—C5—C6 | 115.64 (13) | ||
C2—N1—C1—S1 | 177.75 (11) | C2—N1—C5—C6 | −78.27 (16) |
C5—N1—C1—S1 | −3.2 (2) | N1—C5—C7—C12 | −103.30 (16) |
C2—N1—C1—S2 | −1.5 (2) | C6—C5—C7—C12 | 21.4 (2) |
C5—N1—C1—S2 | 177.55 (11) | N1—C5—C7—C8 | 77.19 (17) |
C4—S2—C1—N1 | 4.98 (15) | C6—C5—C7—C8 | −158.12 (14) |
C4—S2—C1—S1 | −174.33 (8) | C12—C7—C8—C9 | 0.8 (2) |
C1—N1—C2—C3 | −33.2 (2) | C5—C7—C8—C9 | −179.67 (15) |
C5—N1—C2—C3 | 147.72 (13) | C7—C8—C9—C10 | −1.2 (3) |
N1—C2—C3—C4 | 66.05 (17) | C8—C9—C10—C11 | 0.6 (3) |
C2—C3—C4—S2 | −59.48 (16) | C9—C10—C11—C12 | 0.4 (3) |
C1—S2—C4—C3 | 25.10 (14) | C8—C7—C12—C11 | 0.2 (2) |
C1—N1—C5—C7 | −129.39 (14) | C5—C7—C12—C11 | −179.36 (15) |
C2—N1—C5—C7 | 49.72 (17) | C10—C11—C12—C7 | −0.7 (2) |
C1—N1—C5—C6 | 102.62 (16) |
D—H···A | D—H | H···A | D···A | D—H···A |
C6—H6C···S1i | 0.98 | 2.76 | 3.7279 (17) | 168 |
Symmetry code: (i) x−1, y, z. |
Experimental details
Crystal data | |
Chemical formula | C12H15NS2 |
Mr | 237.37 |
Crystal system, space group | Monoclinic, P21/n |
Temperature (K) | 113 |
a, b, c (Å) | 7.0169 (4), 15.5107 (9), 11.0349 (7) |
β (°) | 102.391 (3) |
V (Å3) | 1173.03 (12) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.42 |
Crystal size (mm) | 0.26 × 0.10 × 0.08 |
Data collection | |
Diffractometer | Rigaku Saturn diffractometer |
Absorption correction | Multi-scan (CrystalClear; Rigaku, 2005) |
Tmin, Tmax | 0.899, 0.967 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 14476, 2798, 2631 |
Rint | 0.040 |
(sin θ/λ)max (Å−1) | 0.658 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.041, 0.087, 1.13 |
No. of reflections | 2798 |
No. of parameters | 137 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.27, −0.32 |
Computer programs: CrystalClear (Rigaku, 2005), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
C6—H6C···S1i | 0.98 | 2.76 | 3.7279 (17) | 168.3 |
Symmetry code: (i) x−1, y, z. |
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
Many compounds containing thiazinane groups possess a broad spectrum of biological activities (Soloway et al., 1978; Tomizawa et al., 1995). Herein we report the crystal structure of the title compound, (I).
In (I) (Fig. 1), all bond lengths and angles are in a good agreement with those reported previously (Kálmán et al., 1977; Peng & Wu, 2009; Amir et al., 2006). The thiazinane ring shows a conformation near to a half boat with the carbon atom at position 5 (C3) deviating 0.715 (2) Å above the plane p1 formed by S2, N1, C1, C2 and C4 [maximum least squares plane deviation for S2 0.038 (3) Å]. The dihedral angle between the benzene ring C7-C12 and plane p1 is 83.62 (3) °. In the crystal structure, weak intermolecular C—H···S hydrogen bonds link molecules related by translation along axis a into chains.