Acta Crystallogr E Crystallogr CommunActa Crystallogr E Crystallogr CommunActa Cryst. EActa Crystallographica Section E: Crystallographic Communications2056-9890International Union of Crystallography292503495730286zs238710.1107/S2056989017012488ACSECIS2056989017012488Research CommunicationsCrystal structure of (1S,2S,5R)-5-acetyl­amino-4-oxo-2,3-diphenyl-1,3-thia­zinan-1-ium-1-olateC18H18N2O3SYennawarHemant P.aNobleDuncan J.bhttps://orcid.org/0000-0002-7353-1289SilverbergLee J.b* Department of Biochemistry and Molecular Biology, Pennsylvania State University, University Park, PA 16802, USA Pennsylvania State University, Schuylkill Campus, 200 University Drive, Schuylkill Haven, PA 17972, USA Correspondence e-mail: ljs43@psu.edu011020170592017059201773Pt 10e1710001417142004820172982017© Yennawar et al. 20172017This 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.http://creativecommons.org/licenses/by/2.0/uk/A full version of this article is available from Crystallography Journals Online.

The crystal structure of the enanti­opure sulfoxide of a 2,3,5,6-tetra­hydro-1,3-thia­zin-4-one exhibits a twisted half-chair pucker for the thia­zine ring. Inter­molecular N—H ⋯O hydrogen-bonding inter­actions form a two-dimensional layered structure lying parallel to (001).

The asymmetric unit of the enanti­omerically pure title compound, C18H18N2O3S, comprises two independent mol­ecules (A and B) having almost identical conformations. When overlayed, the alignment–r.m.s. deviation value is 0.30 Å. The six-membered heterocycle has a twisted half-chair conformation in both mol­ecules. The O atom on the S atom of the ring is pseudo-axial on the thia­zine ring and trans to both a phenyl group substituent and the acetamide group in each case. The two benzene rings in each mol­ecule are almost orthogonal to each other, with inter­planar dihedral angles of 83.79 (17) and 86.95 (16)°. The acetamide group is pseudo-equatorial and a phenyl ring is pseudo-axial on the thia­zine ring. Both mol­ecules show a weak intra­molecular C—H⋯O inter­action between H-atom donors of one of the phenyl rings and the acetamide group. In the crystal, an inter­molecular N—H⋯O(thia­zine) hydrogen bond links B mol­ecules along the 21 (b) screw axis and, in addition, an N—H⋯O(acetamide) hydrogen bond links A and B mol­ecules across a. A two-dimensional layered structure lying parallel to (001) is generated, also involving weak inter­molecular C—H⋯O inter­actions.

1,3-thia­zin-4-onetwisted half-chair puckerN—H⋯O and C—H⋯O inter­actionscrystal structureNational Science FoundationCHEM-0131112Penn State SchuylkillThis work was funded by National Science Foundation grant CHEM-0131112. Penn State Schuylkill grant .
Chemical context  

The 1,3-thia­zin-4-ones are a group of six-membered heterocycles with a wide range of biological activity (Ryabukhin et al., 1996). Surrey’s research (Surrey et al., 1958; Surrey, 1963a ,b ) resulted in the discovery of two drugs, the anti-anxiety and muscle relaxant chlormezanone [2-(4-chloro­phen­yl)-3-methyl-2,3,5,6-tetra­hydro-4H-1,3-thia­zin-4-one 1,1-dioxide] (O’Neil, 2006; Tanaka & Horayama, 2005) and muscle relaxant di­chloro­mezanone [2-(3,4-di­chloro­phen­yl)-3-methyl-2,3,5,6-tetra­hydro-4H-1,3-thia­zin-4-one 1,1-dioxide] (Elks & Ganellin, 1990). These sulfones showed greater activity than the sulfides from which they were synthesized (Surrey et al., 1958). Surrey also prepared a variety of other sulfoxides and sulfones of 3-alkyl-2-aryl-2,3,5,6-tetra­hydro-4H-1,3-thia­zin-4-ones (Surrey, 1963a ,b ). We have reported previously the crystal structure of the first N-aryl sulfoxide in this family, racemic 2,3-diphenyl-2,3,5,6-tetra­hydro-4H-1,3-thia­zin-4-one 1-oxide (Yennawar et al., 2016).

A sulfoxide typically has an S—O bond that is between a double bond and a single bond, with one of the lone pairs that was on the sulfide coordinating to the O atom, while O atom contributes electrons from a lone pair to a d orbital of the S atom. The geometry of a sulfoxide is pyramidal, with a high energy barrier for inversion, making it possible to isolate stable enanti­omers (Bentley, 2005). Herein, we report the crystal structure of the sulfoxide of N-[(2S,5R)-4-oxo-2,3-diphenyl-1,3-thia­zinan-5-yl]acetamide (Yennawar, Singh & Silverberg, 2015), C18H18N2O3S, prepared using the method we have reported previously for the oxidation of other 2,3-diphenyl-1,3-thia­zin-4-ones (Yennawar et al., 2016; Yennawar, Noble et al., 2017) and 1,3-thia­zolidinones (Yennawar, Hullihen et al., 2015; Cannon et al., 2015). The oxidation of the confirmed enanti­opure sulfide N-[(2S,5R)-4-oxo-2,3-diphenyl-1,3-thia­zinan-5-yl]acetamide 0.375-hydrate (Yennawar, Singh & Silverberg, 2015), derived from N-acetyl-l-cysteine, yielded a single stereoisomer as the only product.

Structural commentary  

The crystal structure of the title compound has two independent homochiral mol­ecules (A and B) in the asymmetric unit (Fig. 1), which have almost identical conformational features, having an alignment–r.m.s. deviation value of 0.3 Å. Both have the thia­zine rings in a twisted half-chair configuration, with puckering amplitudes = 0.6753 (19)/0.653 (2) Å and θ = 131.05 (17)/135.66 (18)° in mol­ecules A/B, respectively (Cremer & Pople, 1975). The O atom on the S atom of the ring is pseudo-axial on the thia­zine ring and trans to both the 2-phenyl group and the acetamide group in each case. The two phenyl rings in each mol­ecule are almost orthogonal to one another, with dihedral angles of 83.79 (17) and 86.95 (16)° in mol­ecules A and B, respectively. The acetamide group is pseudo-equatorial and the 2-phenyl group is pseudo-axial on the thia­zine ring. A weak intra­molecular C—H⋯O hydrogen bond between the 2-phenyl ring and the O atom of the acetamide group is seen in both mol­ecules (C10A—H⋯O3A and C10B—H⋯O3B), as detailed in Table 1.

We reported previously the crystal structure of the starting sulfide, N-[(2S,5R)-4-oxo-2,3-diphenyl-1,3-thia­zinan-5-yl]ace­t­amide 0.375-hydrate (Yennawar, Singh & Silverberg, 2015), which also had two independent homochiral mol­ecules in the asymmetric unit. However, they were not identical: in one mol­ecule, the thia­zine ring was in a half-chair conformation in which the 2-phenyl ring was nearly pseudo-axial and the acetamide group was nearly pseudo-equatorial. The other mol­ecule had the thia­zine ring in a boat conformation in which both substituents were pseudo-equatorial.

Supra­molecular features  

In the crystal, the B mol­ecule and its 21-related symmetry neighbours form a continuous hydrogen-bonded chain along the b-cell direction through N—H⋯O inter­actions involving the acetamide N atom and the thia­zin-1-ium-1-olate O atoms [N2B—H⋯O1B ii; symmetry code: (ii) −x, y + , −z; Table 1] (Fig. 2). Mol­ecules A and B inter­act, wherein the O atom in the 4-position of mol­ecule B accepts a proton from the acetamide N atom of mol­ecule A [N2A—H⋯O1B i; symmetry code: (i) x + 1, y, z]. The sulfoxide O atom of mol­ecule A does not participate in any hydrogen bonding. A two-dimensional sheet structure lying parallel to (001) is generated. No benzene ring in either of the mol­ecules participates in face-to-face π–π stacking inter­actions.

Database survey  

Crystal structures of a number of 1,3-thia­zolidin-4-one 1-oxides have been reported (Wang et al., 2010; Johnson et al., 1983; Chen et al., 2011; Colombo et al., 2008; Yennawar, Hullihen et al., 2015) and the structure of chlormezanone [2-(4-chloro­phen­yl)-3-methyl-2,3,5,6-tetra­hydro-4H-1,3-thia­zin-4-one 1,1-dioxide] has also been reported (Tanaka & Horayama, 2005). We have reported previously the crystal structure of 2,3-diphenyl-2,3,5,6-tetra­hydro-4H-1,3-thia­zin-4-one 1-oxide (Yennawar et al., 2016). We have also reported recently the crystal structures of 2,3-diphenyl-2,3-di­hydro-4H-1,3-benzo­thia­zin-4-one 1-oxide (Yennawar, Fox et al., 2017) and 2,3-diphenyl-2,3-di­hydro-4H-pyrido[3,2-e][1,3]thia­zin-4-one 1-oxide (Yennawar, Noble et al., 2017).

Synthesis and crystallization  

A 5 ml round-bottomed flask was charged with 53.9 mg of N-[(2S,5R)-4-oxo-2,3-diphenyl-1,3-thia­zinan-5-yl]acetamide 0.375-hydrate, whose configuration was established previously (Yennawar, Singh & Silverberg, 2015), and 1.4 ml of methanol and stirred. A solution of 79.5 mg of Oxone® and 1 ml of distilled water was added dropwise and the mixture was stirred until the reaction was complete, as determined by thin-layer chromatography (TLC). The solids were dissolved by the addition of 5 ml of distilled water. The solution was extracted with 10 ml of di­chloro­methane. The organic layer was washed with 5 ml of distilled water and then with 5 ml of saturated sodium chloride. The solution was dried over Na2SO4 and concentrated under vacuum giving a crude solid. This was chromatographed on flash silica gel, eluting with a gradient of 0–60% acetone in ethyl acetate, giving 55.8 mg of product [98.6% yield; m.p. 449–452 K; R F = 0.20 (30% acetone/70% ethyl acetate)]. Crystals suitable for X-ray crystallography were grown by slow evaporation from propan-2-ol.

Refinement  

Crystal data, data collection and structure refinement details are summarized in Table 2. The H atoms, excepting those on N atoms, were placed geometrically and allowed to ride on their parent C atoms during refinement, with C—H distances of 0.93 (aromatic), 0.96 (meth­yl), 0.97 or (methyl­ene) and 0.98 Å (meth­yl), and with U iso(H) = 1.2U eq(aromatic or methyl­ene C) or 1.5U eq(methyl C). H atoms on N atoms were located in a difference Fourier map and were refined isotropically. The absolute configuration for the chiral centres in the mol­ecule was determined as (1S,2S,5R) (for the arbitrarily numbered atoms C1A/B,C3A/B), with a Flack absolute structure parameter (Flack, 1983) of 0.07 (6) for 4160 Friedel pairs.

Supplementary Material

Crystal structure: contains datablock(s) I. DOI: 10.1107/S2056989017012488/zs2387sup1.cif

Structure factors: contains datablock(s) I. DOI: 10.1107/S2056989017012488/zs2387Isup2.hkl

Click here for additional data file.

Supporting information file. DOI: 10.1107/S2056989017012488/zs2387Isup3.mol

Analysis of short ring interactions.. DOI: 10.1107/S2056989017012488/zs2387sup4.pdf

CCDC reference: 1571357

Additional supporting information: crystallographic information; 3D view; checkCIF report

supplementary crystallographic informationCrystal data
C18H18N2O3SDx = 1.329 Mg m3
Mr = 342.40Melting point = 449–452 K
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
a = 12.872 (6) ÅCell parameters from 7433 reflections
b = 10.139 (5) Åθ = 2.5–28.2°
c = 13.460 (6) ŵ = 0.21 mm1
β = 103.104 (9)°T = 298 K
V = 1710.8 (14) Å3Block, colorless
Z = 40.23 × 0.20 × 0.19 mm
F(000) = 720
Data collection
Bruker SCD area detector diffractometer8079 independent reflections
Radiation source: fine-focus sealed tube6949 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.031
φ and ω scansθmax = 28.2°, θmin = 2.0°
Absorption correction: multi-scan (SADABS; Bruker, 2016)h = −16→17
Tmin = 0.309, Tmax = 0.900k = −13→13
15296 measured reflectionsl = −17→17
Refinement
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.049H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.128w = 1/[σ2(Fo2) + (0.0745P)2] where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max = 0.001
8079 reflectionsΔρmax = 0.37 e Å3
443 parametersΔρmin = −0.27 e Å3
1 restraintAbsolute structure: Flack (1983), 4160 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.07 (6)
Special details
Experimental. The data collection nominally covered a full sphere of reciprocal space by a combination of 4 sets of ω scans each set at different φ and/or 2θ angles and each scan (10 s exposure) covering -0.300° degrees in ω. The crystal to detector distance was 5.82 cm.
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 > 2sigma(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 (Å<sup>2</sup>)
xyzUiso*/Ueq
C1A0.79355 (19)0.2939 (3)0.48969 (16)0.0397 (5)
H1A0.78930.20950.52410.048*
C2A0.86711 (19)0.3246 (3)0.33058 (17)0.0393 (5)
C3A0.93950 (18)0.4386 (2)0.37719 (15)0.0344 (5)
H3A1.01090.40090.40100.041*
C4A0.91189 (19)0.5047 (2)0.46957 (15)0.0356 (5)
H4AA0.84260.54680.44990.043*
H4AB0.96450.57180.49640.043*
C5A0.69426 (19)0.3706 (3)0.49564 (17)0.0431 (5)
C6A0.6572 (2)0.3596 (4)0.5857 (2)0.0598 (8)
H6A0.68950.30110.63650.072*
C7A0.5723 (3)0.4365 (5)0.5981 (2)0.0759 (11)
H7A0.54790.42970.65790.091*
C8A0.5243 (3)0.5217 (5)0.5243 (3)0.0763 (10)
H8A0.46740.57280.53400.092*
C9A0.5592 (2)0.5335 (4)0.4343 (2)0.0636 (8)
H9A0.52620.59260.38410.076*
C10A0.6433 (2)0.4567 (3)0.4200 (2)0.0497 (6)
H10A0.66580.46270.35920.060*
C11A0.7454 (2)0.1476 (2)0.34101 (17)0.0398 (5)
C16A0.7794 (2)0.0238 (3)0.3750 (2)0.0563 (7)
H16A0.84000.01360.42730.068*
C15A0.7227 (3)−0.0862 (3)0.3309 (3)0.0719 (10)
H15A0.7447−0.17010.35460.086*
C14A0.6350 (3)−0.0716 (4)0.2531 (3)0.0709 (10)
H14A0.5983−0.14550.22280.085*
C13A0.6014 (3)0.0507 (4)0.2197 (3)0.0734 (10)
H13A0.54110.06020.16710.088*
C12A0.6561 (2)0.1616 (4)0.2634 (2)0.0588 (7)
H12A0.63250.24530.24030.071*
C17A0.8618 (2)0.5983 (3)0.2465 (2)0.0487 (6)
C18A0.8817 (3)0.7020 (4)0.1734 (3)0.0784 (11)
H18A0.94970.74270.19990.118*
H18B0.82660.76760.16480.118*
H18C0.88140.66210.10870.118*
N1A0.80481 (17)0.26229 (19)0.38641 (14)0.0384 (4)
N2A0.94797 (16)0.5352 (2)0.29910 (14)0.0392 (4)
H2A1.014 (2)0.561 (3)0.2912 (19)0.036 (7)*
O1A1.00529 (16)0.2968 (2)0.56800 (15)0.0581 (5)
O2A0.87065 (18)0.2840 (2)0.24629 (13)0.0615 (6)
O3A0.77158 (16)0.5727 (3)0.25622 (17)0.0702 (7)
S1A0.91010 (5)0.38151 (6)0.56562 (4)0.04051 (15)
C1B0.22990 (19)0.4488 (2)0.06076 (17)0.0389 (5)
H1B0.20750.35620.05840.047*
C2B0.16558 (17)0.6316 (2)0.16162 (17)0.0357 (5)
C3B0.13964 (19)0.7241 (3)0.06778 (18)0.0410 (5)
H3B0.06250.71640.04070.049*
C4B0.1904 (2)0.6890 (3)−0.02038 (17)0.0418 (5)
H4BA0.26720.69830.00090.050*
H4BB0.16490.7488−0.07690.050*
C5B0.34898 (18)0.4469 (3)0.06755 (16)0.0377 (5)
C6B0.3913 (2)0.3500 (3)0.0150 (2)0.0528 (7)
H6B0.34680.2870−0.02290.063*
C7B0.4994 (3)0.3473 (3)0.0189 (2)0.0615 (8)
H7B0.52690.2836−0.01770.074*
C8B0.5669 (2)0.4381 (4)0.0764 (2)0.0578 (7)
H8B0.63970.43500.07910.069*
C9B0.5264 (2)0.5332 (3)0.1298 (2)0.0499 (6)
H9B0.57210.59410.16920.060*
C10B0.4174 (2)0.5390 (3)0.12537 (18)0.0424 (5)
H10B0.39030.60430.16090.051*
C11B0.2058 (2)0.4150 (2)0.23392 (18)0.0419 (5)
C12B0.2934 (3)0.4162 (4)0.3126 (2)0.0722 (10)
H12B0.34660.47870.31430.087*
C13B0.3032 (4)0.3236 (5)0.3903 (3)0.0893 (13)
H13B0.36350.32320.44360.107*
C14B0.2239 (3)0.2330 (4)0.3880 (3)0.0775 (11)
H14B0.23070.17050.43970.093*
C15B0.1358 (3)0.2339 (3)0.3110 (3)0.0669 (9)
H15B0.08180.17290.31070.080*
C16B0.1249 (2)0.3260 (3)0.2317 (2)0.0505 (6)
H16B0.06440.32680.17870.061*
C17B0.2575 (2)0.9072 (3)0.13509 (19)0.0458 (6)
C18B0.2671 (4)1.0542 (3)0.1506 (3)0.0763 (10)
H18D0.30071.07270.22040.114*
H18E0.19741.09320.13420.114*
H18F0.30951.09030.10690.114*
N1B0.19754 (16)0.5070 (2)0.14898 (14)0.0381 (4)
N2B0.15836 (19)0.8610 (2)0.09612 (17)0.0469 (5)
H2B0.110 (2)0.910 (3)0.089 (2)0.042 (8)*
O1B0.04145 (15)0.5076 (3)−0.06247 (17)0.0666 (6)
O2B0.14719 (15)0.66808 (19)0.24289 (14)0.0484 (4)
O3B0.33503 (15)0.83467 (19)0.15418 (15)0.0530 (5)
S1B0.15756 (5)0.52300 (7)−0.06050 (4)0.04663 (17)
Atomic displacement parameters (Å<sup>2</sup>)
U11U22U33U12U13U23
C1A0.0472 (13)0.0435 (13)0.0292 (10)−0.0069 (11)0.0101 (9)−0.0013 (9)
C2A0.0442 (12)0.0432 (13)0.0316 (10)−0.0011 (10)0.0108 (9)−0.0049 (9)
C3A0.0338 (11)0.0389 (12)0.0300 (10)−0.0003 (9)0.0065 (8)−0.0027 (9)
C4A0.0397 (11)0.0343 (12)0.0319 (9)0.0014 (9)0.0062 (9)−0.0056 (8)
C5A0.0441 (12)0.0518 (14)0.0355 (11)−0.0110 (12)0.0135 (10)−0.0064 (11)
C6A0.0595 (16)0.083 (2)0.0409 (13)−0.0101 (16)0.0195 (12)−0.0040 (14)
C7A0.0571 (18)0.125 (3)0.0529 (16)−0.0064 (19)0.0280 (15)−0.0207 (19)
C8A0.0464 (17)0.110 (3)0.073 (2)0.0079 (19)0.0156 (15)−0.025 (2)
C9A0.0417 (14)0.084 (2)0.0621 (16)0.0076 (16)0.0050 (12)−0.0074 (17)
C10A0.0429 (13)0.0638 (18)0.0428 (12)−0.0026 (13)0.0106 (10)−0.0038 (12)
C11A0.0426 (13)0.0425 (13)0.0367 (11)−0.0081 (11)0.0137 (9)−0.0063 (10)
C16A0.0598 (17)0.0445 (15)0.0607 (16)−0.0018 (14)0.0055 (13)−0.0077 (13)
C15A0.100 (3)0.0442 (18)0.076 (2)−0.0166 (17)0.029 (2)−0.0106 (14)
C14A0.084 (2)0.070 (2)0.0665 (19)−0.0399 (19)0.0320 (19)−0.0292 (17)
C13A0.062 (2)0.094 (3)0.0601 (18)−0.0213 (19)0.0051 (15)−0.0221 (18)
C12A0.0604 (18)0.0622 (19)0.0468 (14)−0.0062 (14)−0.0028 (13)−0.0074 (13)
C17A0.0390 (13)0.0625 (18)0.0442 (13)−0.0003 (12)0.0085 (11)0.0123 (12)
C18A0.0573 (18)0.097 (3)0.081 (2)0.0043 (19)0.0149 (17)0.050 (2)
N1A0.0482 (11)0.0372 (11)0.0311 (9)−0.0086 (9)0.0115 (8)−0.0076 (7)
N2A0.0349 (10)0.0446 (12)0.0388 (9)−0.0033 (9)0.0102 (8)0.0027 (9)
O1A0.0572 (11)0.0548 (12)0.0561 (11)0.0131 (10)−0.0005 (9)0.0087 (9)
O2A0.0785 (14)0.0743 (14)0.0388 (9)−0.0276 (12)0.0280 (10)−0.0233 (9)
O3A0.0353 (10)0.103 (2)0.0692 (13)−0.0017 (10)0.0059 (9)0.0341 (13)
S1A0.0493 (3)0.0405 (3)0.0289 (2)0.0010 (3)0.0029 (2)−0.0018 (2)
C1B0.0428 (12)0.0363 (12)0.0386 (11)−0.0073 (10)0.0114 (10)−0.0046 (9)
C2B0.0284 (10)0.0408 (12)0.0396 (11)−0.0031 (9)0.0111 (9)0.0040 (9)
C3B0.0320 (11)0.0487 (14)0.0423 (12)0.0031 (10)0.0083 (9)0.0088 (10)
C4B0.0400 (12)0.0535 (15)0.0296 (10)−0.0044 (11)0.0030 (9)0.0073 (10)
C5B0.0390 (12)0.0417 (13)0.0334 (10)0.0012 (10)0.0099 (9)0.0018 (9)
C6B0.0530 (15)0.0572 (18)0.0474 (14)0.0036 (13)0.0099 (11)−0.0136 (12)
C7B0.0560 (16)0.070 (2)0.0626 (17)0.0151 (15)0.0223 (14)−0.0136 (15)
C8B0.0397 (14)0.074 (2)0.0604 (16)0.0124 (14)0.0134 (12)0.0068 (15)
C9B0.0410 (13)0.0488 (15)0.0568 (14)−0.0004 (12)0.0047 (11)0.0037 (13)
C10B0.0423 (12)0.0381 (13)0.0465 (12)0.0000 (10)0.0093 (10)−0.0022 (10)
C11B0.0459 (13)0.0422 (14)0.0414 (12)0.0020 (10)0.0178 (10)0.0077 (9)
C12B0.070 (2)0.082 (3)0.0588 (17)−0.0207 (17)0.0013 (15)0.0301 (17)
C13B0.096 (3)0.104 (3)0.061 (2)−0.010 (2)0.0021 (19)0.040 (2)
C14B0.090 (3)0.075 (2)0.075 (2)0.011 (2)0.034 (2)0.0384 (19)
C15B0.067 (2)0.0498 (18)0.097 (2)0.0029 (15)0.046 (2)0.0232 (17)
C16B0.0485 (14)0.0436 (15)0.0639 (17)0.0020 (12)0.0224 (13)0.0070 (12)
C17B0.0572 (16)0.0417 (15)0.0410 (12)0.0062 (12)0.0160 (11)0.0010 (10)
C18B0.098 (3)0.0469 (19)0.084 (2)0.0031 (17)0.021 (2)−0.0066 (16)
N1B0.0428 (10)0.0384 (11)0.0360 (9)−0.0021 (8)0.0148 (8)0.0055 (8)
N2B0.0459 (12)0.0432 (13)0.0541 (12)0.0160 (11)0.0163 (10)0.0089 (10)
O1B0.0388 (10)0.0814 (16)0.0722 (13)−0.0158 (11)−0.0029 (9)−0.0075 (12)
O2B0.0558 (11)0.0522 (11)0.0435 (9)0.0023 (8)0.0246 (8)0.0015 (8)
O3B0.0478 (10)0.0490 (11)0.0607 (11)0.0041 (8)0.0093 (9)−0.0076 (8)
S1B0.0416 (3)0.0590 (4)0.0362 (3)−0.0103 (3)0.0023 (2)−0.0070 (3)
Geometric parameters (Å, º)
C1A—H1A0.9800C1B—H1B0.9800
C1A—C5A1.514 (4)C1B—C5B1.515 (3)
C1A—N1A1.465 (3)C1B—N1B1.468 (3)
C1A—S1A1.841 (3)C1B—S1B1.846 (3)
C2A—C3A1.527 (3)C2B—C3B1.547 (3)
C2A—N1A1.371 (3)C2B—N1B1.351 (3)
C2A—O2A1.217 (3)C2B—O2B1.227 (3)
C3A—H3A0.9800C3B—H3B0.9800
C3A—C4A1.524 (3)C3B—C4B1.521 (3)
C3A—N2A1.459 (3)C3B—N2B1.445 (4)
C4A—H4AA0.9700C4B—H4BA0.9700
C4A—H4AB0.9700C4B—H4BB0.9700
C4A—S1A1.801 (2)C4B—S1B1.788 (3)
C5A—C6A1.404 (3)C5B—C6B1.392 (4)
C5A—C10A1.388 (4)C5B—C10B1.394 (4)
C6A—H6A0.9300C6B—H6B0.9300
C6A—C7A1.383 (5)C6B—C7B1.380 (4)
C7A—H7A0.9300C7B—H7B0.9300
C7A—C8A1.355 (6)C7B—C8B1.377 (5)
C8A—H8A0.9300C8B—H8B0.9300
C8A—C9A1.389 (5)C8B—C9B1.374 (4)
C9A—H9A0.9300C9B—H9B0.9300
C9A—C10A1.382 (4)C9B—C10B1.392 (4)
C10A—H10A0.9300C10B—H10B0.9300
C11A—C16A1.372 (4)C11B—C12B1.361 (4)
C11A—C12A1.375 (4)C11B—C16B1.372 (4)
C11A—N1A1.449 (3)C11B—N1B1.460 (3)
C16A—H16A0.9300C12B—H12B0.9300
C16A—C15A1.390 (5)C12B—C13B1.389 (5)
C15A—H15A0.9300C13B—H13B0.9300
C15A—C14A1.362 (6)C13B—C14B1.369 (6)
C14A—H14A0.9300C14B—H14B0.9300
C14A—C13A1.356 (6)C14B—C15B1.353 (5)
C13A—H13A0.9300C15B—H15B0.9300
C13A—C12A1.385 (5)C15B—C16B1.401 (4)
C12A—H12A0.9300C16B—H16B0.9300
C17A—C18A1.502 (4)C17B—C18B1.505 (4)
C17A—N2A1.336 (3)C17B—N2B1.350 (4)
C17A—O3A1.226 (3)C17B—O3B1.219 (3)
C18A—H18A0.9600C18B—H18D0.9600
C18A—H18B0.9600C18B—H18E0.9600
C18A—H18C0.9600C18B—H18F0.9600
N2A—H2A0.91 (3)N2B—H2B0.79 (3)
O1A—S1A1.491 (2)O1B—S1B1.497 (2)
C5A—C1A—H1A106.6C5B—C1B—H1B106.0
C5A—C1A—S1A108.30 (17)C5B—C1B—S1B111.05 (15)
N1A—C1A—H1A106.6N1B—C1B—H1B106.0
N1A—C1A—C5A115.4 (2)N1B—C1B—C5B115.16 (19)
N1A—C1A—S1A112.87 (15)N1B—C1B—S1B111.87 (17)
S1A—C1A—H1A106.6S1B—C1B—H1B106.0
N1A—C2A—C3A120.12 (19)N1B—C2B—C3B118.6 (2)
O2A—C2A—C3A119.4 (2)O2B—C2B—C3B119.7 (2)
O2A—C2A—N1A120.3 (2)O2B—C2B—N1B121.3 (2)
C2A—C3A—H3A106.2C2B—C3B—H3B105.6
C4A—C3A—C2A115.76 (18)C4B—C3B—C2B116.3 (2)
C4A—C3A—H3A106.2C4B—C3B—H3B105.6
N2A—C3A—C2A110.52 (18)N2B—C3B—C2B112.0 (2)
N2A—C3A—H3A106.2N2B—C3B—H3B105.6
N2A—C3A—C4A111.2 (2)N2B—C3B—C4B110.8 (2)
C3A—C4A—H4AA109.9C3B—C4B—H4BA109.7
C3A—C4A—H4AB109.9C3B—C4B—H4BB109.7
C3A—C4A—S1A108.90 (16)C3B—C4B—S1B109.99 (17)
H4AA—C4A—H4AB108.3H4BA—C4B—H4BB108.2
S1A—C4A—H4AA109.9S1B—C4B—H4BA109.7
S1A—C4A—H4AB109.9S1B—C4B—H4BB109.7
C6A—C5A—C1A117.5 (3)C6B—C5B—C1B119.1 (2)
C10A—C5A—C1A123.3 (2)C6B—C5B—C10B119.1 (2)
C10A—C5A—C6A119.1 (3)C10B—C5B—C1B121.8 (2)
C5A—C6A—H6A120.2C5B—C6B—H6B119.9
C7A—C6A—C5A119.5 (3)C7B—C6B—C5B120.1 (3)
C7A—C6A—H6A120.2C7B—C6B—H6B119.9
C6A—C7A—H7A119.6C6B—C7B—H7B119.6
C8A—C7A—C6A120.8 (3)C8B—C7B—C6B120.7 (3)
C8A—C7A—H7A119.6C8B—C7B—H7B119.6
C7A—C8A—H8A119.6C7B—C8B—H8B120.1
C7A—C8A—C9A120.7 (3)C9B—C8B—C7B119.8 (3)
C9A—C8A—H8A119.6C9B—C8B—H8B120.1
C8A—C9A—H9A120.3C8B—C9B—H9B119.8
C10A—C9A—C8A119.4 (3)C8B—C9B—C10B120.4 (3)
C10A—C9A—H9A120.3C10B—C9B—H9B119.8
C5A—C10A—H10A119.8C5B—C10B—H10B120.0
C9A—C10A—C5A120.5 (3)C9B—C10B—C5B119.9 (2)
C9A—C10A—H10A119.8C9B—C10B—H10B120.0
C16A—C11A—C12A119.8 (3)C12B—C11B—C16B120.9 (3)
C16A—C11A—N1A119.7 (2)C12B—C11B—N1B120.3 (2)
C12A—C11A—N1A120.5 (3)C16B—C11B—N1B118.8 (2)
C11A—C16A—H16A120.2C11B—C12B—H12B120.1
C11A—C16A—C15A119.6 (3)C11B—C12B—C13B119.9 (3)
C15A—C16A—H16A120.2C13B—C12B—H12B120.1
C16A—C15A—H15A119.9C12B—C13B—H13B120.1
C14A—C15A—C16A120.3 (3)C14B—C13B—C12B119.8 (4)
C14A—C15A—H15A119.9C14B—C13B—H13B120.1
C15A—C14A—H14A120.0C13B—C14B—H14B119.9
C13A—C14A—C15A120.0 (3)C15B—C14B—C13B120.3 (3)
C13A—C14A—H14A120.0C15B—C14B—H14B119.9
C14A—C13A—H13A119.7C14B—C15B—H15B119.7
C14A—C13A—C12A120.6 (3)C14B—C15B—C16B120.7 (3)
C12A—C13A—H13A119.7C16B—C15B—H15B119.7
C11A—C12A—C13A119.7 (3)C11B—C16B—C15B118.5 (3)
C11A—C12A—H12A120.2C11B—C16B—H16B120.7
C13A—C12A—H12A120.2C15B—C16B—H16B120.7
N2A—C17A—C18A116.0 (2)N2B—C17B—C18B116.0 (3)
O3A—C17A—C18A121.6 (3)O3B—C17B—C18B122.0 (3)
O3A—C17A—N2A122.4 (2)O3B—C17B—N2B121.9 (2)
C17A—C18A—H18A109.5C17B—C18B—H18D109.5
C17A—C18A—H18B109.5C17B—C18B—H18E109.5
C17A—C18A—H18C109.5C17B—C18B—H18F109.5
H18A—C18A—H18B109.5H18D—C18B—H18E109.5
H18A—C18A—H18C109.5H18D—C18B—H18F109.5
H18B—C18A—H18C109.5H18E—C18B—H18F109.5
C2A—N1A—C1A127.96 (19)C2B—N1B—C1B128.89 (19)
C2A—N1A—C11A117.19 (18)C2B—N1B—C11B117.93 (19)
C11A—N1A—C1A114.79 (18)C11B—N1B—C1B113.1 (2)
C3A—N2A—H2A120.0 (16)C3B—N2B—H2B120 (2)
C17A—N2A—C3A121.0 (2)C17B—N2B—C3B121.5 (2)
C17A—N2A—H2A118.6 (16)C17B—N2B—H2B119 (2)
C4A—S1A—C1A94.46 (11)C4B—S1B—C1B94.54 (11)
O1A—S1A—C1A107.22 (13)O1B—S1B—C1B105.93 (12)
O1A—S1A—C4A105.71 (11)O1B—S1B—C4B105.70 (14)
Hydrogen-bond geometry (Å, º)
D—H···AD—HH···AD···AD—H···A
N2A—H2A···O2Bi0.91 (3)2.25 (3)3.137 (3)164 (2)
N2B—H2B···O1Bii0.79 (3)2.14 (3)2.916 (3)168 (3)
C10A—H10A···O3A0.932.423.259 (3)149
C10B—H10B···O3B0.932.443.232 (4)143
C4B—H4BB···O2Aiii0.972.253.116 (3)148

Symmetry codes: (i) x+1, y, z; (ii) −x, y+1/2, −z; (iii) −x+1, y+1/2, −z.

ReferencesBentley, R. (2005). Chem. Soc. Rev. 34, 609–624.Bruker (2016). SMART, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.Cannon, K., Gandla, D., Lauro, S., Silverberg, L., Tierney, J. & Lagalante, A. (2015). Int. J. Chem. 7(2), 73–84.Chen, H., Zai-Hong, G., Qing-Mei, Y. & Xiao-Liu, L. (2011). Chin. J. Org. Chem. 31, 249–255.Colombo, A., Fernàndez, J. C., Fernández-Forner, D., de la Figuera, N., Albericio, F. & Forns, P. (2008). Tetrahedron Lett. 49, 1569–1572.Cremer, D. & Pople, J. A. (1975). J. Am. Chem. Soc. 97, 1354–1358.Dolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339–341.Elks, J. & Ganellin, C. R. (1990). Editors. Dictionary of Drugs, p. 382. Cambridge, UK: Chapman and Hall.Flack, H. D. (1983). Acta Cryst. A39, 876–881.Johnson, M. R., Fazio, M. J., Ward, D. L. & Sousa, L. R. (1983). J. Org. Chem. 48, 494–499.O’Neil, M. J. (2006). Editor. The Merck Index, 14th ed., p. 349, Whitehouse Station, NJ: Merck & Co. Inc.Ryabukhin, Y. I., Korzhavina, O. B. & Suzdalev, K. F. (1996). Adv. Heterocycl. Chem. 66, 131–190.Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.Surrey, A. R. (1963a). US Patent 3082209.Surrey, A. R. (1963b). US Patent 3093639.Surrey, A. R., Webb, W. G. & Gesler, R. M. (1958). J. Am. Chem. Soc. 80, 3469–3471.Tanaka, R. & Horayama, N. (2005). X-Ray Struct. Anal. Online, 21, x57–x58.Wang, Q., Xu, Z. & Sun, Y. (2010). Acta Cryst. E66, o1422.Yennawar, H. P., Fox, R., Moyer, Q. J., Yang, Z. & Silverberg, L. J. (2017). Acta Cryst. E73, 1189–1191.Yennawar, H. P., Noble, D. J., Yang, Z. & Silverberg, L. J. (2017). IUCrData, 2, x171112.Yennawar, H. P., Singh, H. & Silverberg, L. J. (2015). Acta Cryst. E71, 62–64.Yennawar, H. P., Tierney, J., Hullihen, P. D. & Silverberg, L. J. (2015). Acta Cryst. E71, 264–267.Yennawar, H. P., Yang, Z. & Silverberg, L. J. (2016). Acta Cryst. E72, 1541–1543.

The mol­ecular structures of the two independent mol­ecules (A and B) in the asymmetric unit of the title compound, with displacement ellipsoids drawn at the 50% probability level. Dashed lines indicate intra­molecular C—H⋯O inter­actions.

Crystal packing diagram with red dotted lines for inter­molecular N—H⋯O contacts between 21-related mol­ecules, forming helical chains along the b-axis direction, as well as the inter­action with an independent mol­ecule. Blue dotted lines represent the intra­molecular C—H⋯O contacts.

Hydrogen-bond geometry (Å, °)
D—H⋯A D—HH⋯A DA D—H⋯A
N2A—H2A⋯O2B i 0.91 (3)2.25 (3)3.137 (3)164 (2)
N2B—H2B⋯O1B ii 0.79 (3)2.14 (3)2.916 (3)168 (3)
C10A—H10A⋯O3A 0.932.423.259 (3)149
C10B—H10B⋯O3B 0.932.443.232 (4)143
C4B—H4BB⋯O2A iii 0.972.253.116 (3)148

Symmetry codes: (i) ; (ii) ; (iii) .

Experimental details
Crystal data
Chemical formulaC18H18N2O3S
M r 342.40
Crystal system, space groupMonoclinic, P21
Temperature (K)298
a, b, c (Å)12.872 (6), 10.139 (5), 13.460 (6)
β (°)103.104 (9)
V3)1710.8 (14)
Z 4
Radiation typeMo Kα
μ (mm−1)0.21
Crystal size (mm)0.23 × 0.20 × 0.19
 
Data collection
DiffractometerBruker SCD area detector
Absorption correctionMulti-scan (SADABS; Bruker, 2016)
T min, T max 0.309, 0.900
No. of measured, independent and observed [I > 2σ(I)] reflections15296, 8079, 6949
R int 0.031
(sin θ/λ)max−1)0.666
 
Refinement
R[F 2 > 2σ(F 2)], wR(F 2), S 0.049, 0.128, 1.02
No. of reflections8079
No. of parameters443
No. of restraints1
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å−3)0.37, −0.27
Absolute structureFlack (1983), 4160 Friedel pairs
Absolute structure parameter0.07 (6)

Computer programs: SMART (Bruker, 2016), SAINT (Bruker, 2016), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008) and OLEX2 (Dolomanov et al., 2009).