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Ten new crystal structures of cis and trans bicyclic diketopiperazines (DKPs) of thia-pipecolic acid (with sulfur in the β, γ or δ position) or thia-proline (with sulfur in the β or γ position) and N-methyl phenyl­alanine [(NMe)Phe]: cyclo[(β-S)Pip-(NMe)Phe], cyclo[(γ-S)Pip-(NMe)Phe], cyclo[(δ-S)Pip-(NMe)Phe], cyclo[(β-S)Pro-(NMe)Phe] and cyclo[(γ-S)Pro-(NMe)Phe] were determined with X-ray crystallography. Density functional theory calculations of these molecules in the gas phase succeed in reproducing the observed molecular conformations in the crystal remarkably well. This illustrates the weak to moderate impact of intermolecular packing forces in the absence of classical N—H...O hydrogen bonds. The effect of sulfur on the geometry of the DKP ring and details of amide bond non-planarity are discussed. Molecular flexibility of the DKP ring, as estimated from the calculated deformation energies of its endocyclic ring torsion angles, is not in general the decisive factor for the occurrence of multiple symmetry independent molecules in the unit cell (Z′ > 1), though in some cases a correlation is observed.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520617014731/dk5056sup1.cif
Contains datablocks 4a, 4b, 6a, 6b, 8a, 8b, 12a, 12b, 14a, 14b

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Structure factor file (CIF format) https://doi.org/10.1107/S2052520617014731/dk50564asup2.hkl
Contains datablock 4a

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Structure factor file (CIF format) https://doi.org/10.1107/S2052520617014731/dk50564bsup3.hkl
Contains datablock 4b

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Structure factor file (CIF format) https://doi.org/10.1107/S2052520617014731/dk50566asup4.hkl
Contains datablock 6a

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Structure factor file (CIF format) https://doi.org/10.1107/S2052520617014731/dk50566bsup5.hkl
Contains datablock 6b

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Structure factor file (CIF format) https://doi.org/10.1107/S2052520617014731/dk50568asup6.hkl
Contains datablock 8a

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Structure factor file (CIF format) https://doi.org/10.1107/S2052520617014731/dk50568bsup7.hkl
Contains datablock 8b

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Structure factor file (CIF format) https://doi.org/10.1107/S2052520617014731/dk505612asup8.hkl
Contains datablock 12a

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Structure factor file (CIF format) https://doi.org/10.1107/S2052520617014731/dk505612bsup9.hkl
Contains datablock 12b

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Structure factor file (CIF format) https://doi.org/10.1107/S2052520617014731/dk505614asup10.hkl
Contains datablock 14a

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Structure factor file (CIF format) https://doi.org/10.1107/S2052520617014731/dk505614bsup11.hkl
Contains datablock 14b

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S2052520617014731/dk5056sup12.pdf
Fig. S1, Tables S1-S2

CCDC references: 1400449; 1400450; 1400451; 1400452; 1400453; 1400454; 1400455; 1400456; 1400457; 1400458

Computing details top

Data collection: COLLECT (Hooft, 1998) and DENZO (Otwinowski & Minor, 1997) for (4a), (4b), (6a), (6b), (8a), (8b); Bruker APEX2 for (12a), (12b), (14a), (14b). Cell refinement: COLLECT and DENZO for (4a), (4b), (6a), (6b), (8a), (8b); Bruker SAINT for (12a), (12b), (14a), (14b). Data reduction: COLLECT and DENZO for (4a), (4b), (6a), (6b), (8a), (8b); Bruker SAINT for (12a), (12b), (14a), (14b). Program(s) used to solve structure: SIR92 (Altomare et al., 1994) for (4a), (4b), (6a), (6b), (8a), (8b); SHELXS97 (Sheldrick, 2008) for (12a), (12b), (14a), (14b). For all structures, program(s) used to refine structure: SHELXL2014/7 (Sheldrick, 2014).

(4a) top
Crystal data top
2(C15H18N2O2S)·H2ODx = 1.332 Mg m3
Mr = 598.76Mo Kα radiation, λ = 0.71070 Å
Trigonal, P31Cell parameters from 54195 reflections
Hall symbol: P 31θ = 1–27.8°
a = 8.4102 (2) ŵ = 0.22 mm1
c = 36.562 (1) ÅT = 150 K
V = 2239.61 (10) Å3Plate, colourless
Z = 30.5 × 0.5 × 0.2 mm
F(000) = 954
Data collection top
Nonius KappaCCD area detector
diffractometer
5051 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.051
Graphite monochromatorθmax = 26.0°, θmin = 4.0°
Detector resolution: 9.091 pixels mm-1h = 1010
φ and ω scans to fill the Ewald spherek = 88
15456 measured reflectionsl = 4444
5110 independent reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.045H-atom parameters constrained
wR(F2) = 0.113 w = 1/[σ2(Fo2) + (0.0502P)2 + 1.5374P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
5110 reflectionsΔρmax = 0.37 e Å3
373 parametersΔρmin = 0.28 e Å3
1 restraintAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.01 (12)
Special details top

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 (Å2) top
xyzUiso*/Ueq
N110.3901 (5)0.5157 (6)0.13434 (10)0.0365 (9)
C120.5655 (7)0.6501 (6)0.13601 (12)0.0341 (10)
O120.6366 (5)0.7696 (5)0.11261 (10)0.0466 (9)
C130.6815 (7)0.6559 (7)0.16871 (13)0.0402 (10)
H130.72530.77500.18060.048*
N140.5804 (6)0.5150 (6)0.19644 (10)0.0386 (9)
C140.6782 (9)0.5387 (9)0.23141 (13)0.0539 (14)
H14A0.59090.48970.25100.081*
H14B0.76130.66690.23560.081*
H14C0.74600.47480.23030.081*
C150.4104 (7)0.3733 (7)0.19289 (12)0.0393 (11)
O150.3273 (6)0.2514 (6)0.21654 (10)0.0548 (10)
C160.3100 (7)0.3562 (7)0.15723 (12)0.0392 (11)
H160.18580.32980.16350.047*
S170.28769 (18)0.1535 (2)0.13302 (4)0.0487 (3)
C180.1582 (7)0.1636 (8)0.09461 (17)0.0515 (13)
H18A0.14340.07240.07660.062*
H18B0.03700.13490.10280.062*
C190.2546 (8)0.3543 (9)0.07682 (13)0.0519 (14)
H19A0.37490.38170.06830.062*
H19B0.18430.35330.05570.062*
C1100.2756 (8)0.5003 (8)0.10224 (14)0.0475 (12)
H11A0.15540.47390.11060.057*
H11B0.33170.61670.08940.057*
C1110.8543 (7)0.6530 (7)0.15442 (13)0.0389 (10)
H11C0.92840.76380.14030.047*
H11D0.92690.65530.17520.047*
C1120.8127 (5)0.4905 (6)0.13119 (12)0.0293 (9)
C1130.7797 (6)0.3272 (7)0.14774 (14)0.0346 (10)
H1130.78820.32140.17300.041*
C1140.7342 (6)0.1734 (6)0.12650 (14)0.0376 (10)
H1140.71380.06510.13750.045*
C1150.7190 (7)0.1818 (8)0.08865 (15)0.0465 (12)
H1150.68510.07770.07450.056*
C1160.7538 (7)0.3434 (7)0.07204 (13)0.0420 (12)
H1160.74660.34910.04670.050*
C1170.8005 (6)0.4996 (6)0.09355 (13)0.0374 (10)
H1170.82300.60860.08250.045*
N210.3464 (5)0.5511 (5)0.29836 (10)0.0334 (8)
C220.4839 (6)0.7289 (6)0.29613 (11)0.0318 (9)
O220.6062 (4)0.7998 (5)0.31883 (10)0.0426 (8)
C230.4884 (6)0.8361 (6)0.26299 (12)0.0331 (9)
H230.60590.87410.25080.040*
N240.3462 (5)0.7350 (5)0.23596 (9)0.0335 (8)
C240.3699 (9)0.8292 (8)0.20022 (13)0.0484 (12)
H24A0.31130.73920.18130.073*
H24B0.49840.90360.19490.073*
H24C0.31520.90560.20150.073*
C250.2004 (6)0.5682 (6)0.24092 (12)0.0349 (10)
O250.0815 (5)0.4888 (5)0.21737 (9)0.0453 (8)
C260.1824 (6)0.4705 (6)0.27707 (12)0.0323 (9)
H260.15210.34460.27130.039*
S270.01290 (17)0.45711 (18)0.30100 (4)0.0396 (3)
C280.0017 (7)0.3327 (7)0.34046 (14)0.0422 (11)
H28A0.08910.31940.35840.051*
H28B0.02750.21050.33280.051*
C290.1901 (7)0.4276 (7)0.35825 (14)0.0461 (12)
H29A0.18920.35880.37960.055*
H29B0.22040.54970.36610.055*
C2100.3357 (7)0.4411 (7)0.33090 (13)0.0431 (11)
H21A0.45450.49730.34280.052*
H21B0.30520.31870.32320.052*
C2110.4930 (6)1.0149 (7)0.27509 (12)0.0360 (9)
H21C0.60371.08900.28920.043*
H21D0.49821.08450.25350.043*
C2120.3296 (6)0.9802 (6)0.29763 (11)0.0277 (9)
C2130.3308 (6)0.9645 (6)0.33568 (12)0.0315 (9)
H2130.43620.98170.34750.038*
C2140.1767 (7)0.9236 (6)0.35570 (12)0.0354 (10)
H2140.17920.91480.38100.042*
C2150.0169 (6)0.8953 (6)0.33857 (12)0.0329 (9)
H2150.08830.86280.35220.040*
C2160.0161 (6)0.9160 (6)0.30082 (12)0.0354 (10)
H2160.08750.90450.28920.042*
C2170.1693 (6)0.9534 (6)0.28075 (12)0.0307 (9)
H2170.16600.96100.25540.037*
O1W0.0873 (5)1.0814 (5)0.21503 (12)0.0500 (9)
H1W0.06151.19880.21960.060*
H2W0.01741.10170.20990.060*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N110.042 (2)0.046 (2)0.0288 (17)0.027 (2)0.0031 (16)0.0087 (16)
C120.051 (3)0.031 (2)0.029 (2)0.027 (2)0.0001 (19)0.0031 (18)
O120.066 (2)0.041 (2)0.0378 (18)0.0298 (19)0.0025 (17)0.0056 (15)
C130.056 (3)0.043 (3)0.032 (2)0.033 (2)0.006 (2)0.008 (2)
N140.055 (3)0.049 (2)0.0265 (18)0.037 (2)0.0031 (17)0.0053 (17)
C140.076 (4)0.085 (4)0.027 (2)0.060 (4)0.015 (2)0.015 (3)
C150.046 (3)0.056 (3)0.028 (2)0.035 (3)0.0117 (19)0.011 (2)
O150.062 (2)0.079 (3)0.0377 (19)0.045 (2)0.0034 (17)0.0206 (19)
C160.045 (3)0.049 (3)0.038 (2)0.035 (2)0.012 (2)0.021 (2)
S170.0398 (7)0.0447 (7)0.0619 (8)0.0213 (6)0.0128 (6)0.0003 (6)
C180.032 (2)0.053 (3)0.068 (4)0.021 (2)0.006 (2)0.003 (3)
C190.051 (3)0.079 (4)0.031 (2)0.037 (3)0.002 (2)0.011 (2)
C1100.046 (3)0.056 (3)0.041 (2)0.026 (2)0.007 (2)0.010 (2)
C1110.042 (2)0.031 (2)0.042 (3)0.018 (2)0.002 (2)0.003 (2)
C1120.025 (2)0.025 (2)0.039 (2)0.0139 (17)0.0039 (17)0.0022 (17)
C1130.026 (2)0.042 (3)0.041 (2)0.021 (2)0.0013 (18)0.002 (2)
C1140.034 (2)0.030 (2)0.047 (3)0.016 (2)0.0045 (19)0.0024 (19)
C1150.045 (3)0.049 (3)0.051 (3)0.028 (2)0.003 (2)0.008 (2)
C1160.045 (3)0.057 (3)0.032 (2)0.032 (2)0.001 (2)0.009 (2)
C1170.036 (2)0.033 (2)0.045 (3)0.019 (2)0.004 (2)0.0062 (19)
N210.034 (2)0.035 (2)0.0365 (19)0.0214 (18)0.0015 (16)0.0008 (15)
C220.026 (2)0.044 (3)0.029 (2)0.019 (2)0.0039 (17)0.0017 (18)
O220.0287 (17)0.052 (2)0.049 (2)0.0214 (16)0.0089 (15)0.0032 (16)
C230.028 (2)0.044 (3)0.036 (2)0.024 (2)0.0051 (17)0.0015 (19)
N240.0333 (19)0.044 (2)0.0278 (18)0.0225 (18)0.0014 (15)0.0003 (16)
C240.074 (4)0.054 (3)0.031 (2)0.043 (3)0.009 (2)0.004 (2)
C250.040 (3)0.036 (2)0.038 (2)0.026 (2)0.0013 (19)0.0061 (19)
O250.053 (2)0.049 (2)0.0373 (18)0.0278 (17)0.0153 (15)0.0084 (14)
C260.038 (2)0.030 (2)0.034 (2)0.0203 (19)0.0046 (19)0.0099 (18)
S270.0367 (6)0.0407 (7)0.0454 (6)0.0224 (5)0.0034 (5)0.0045 (5)
C280.044 (3)0.045 (3)0.041 (2)0.026 (2)0.008 (2)0.011 (2)
C290.063 (3)0.040 (3)0.035 (2)0.025 (3)0.009 (2)0.003 (2)
C2100.046 (3)0.045 (3)0.042 (3)0.025 (2)0.010 (2)0.001 (2)
C2110.036 (2)0.038 (2)0.038 (2)0.022 (2)0.0040 (19)0.0088 (19)
C2120.030 (2)0.030 (2)0.0268 (19)0.0176 (18)0.0022 (16)0.0043 (16)
C2130.033 (2)0.037 (2)0.030 (2)0.022 (2)0.0065 (17)0.0038 (18)
C2140.046 (3)0.031 (2)0.027 (2)0.018 (2)0.0025 (19)0.0060 (18)
C2150.035 (2)0.037 (2)0.032 (2)0.0213 (19)0.0063 (18)0.0047 (18)
C2160.033 (2)0.035 (2)0.034 (2)0.0132 (19)0.0074 (18)0.0122 (17)
C2170.031 (2)0.030 (2)0.034 (2)0.0182 (18)0.0021 (18)0.0016 (17)
O1W0.044 (2)0.0407 (19)0.056 (2)0.0145 (16)0.0004 (17)0.0040 (17)
Geometric parameters (Å, º) top
N11—C121.338 (6)N21—C261.426 (6)
N11—C161.431 (6)N21—C2101.482 (6)
N11—C1101.482 (6)C22—O221.220 (6)
C12—O121.224 (6)C22—C231.500 (6)
C12—C131.528 (7)C23—N241.454 (6)
C13—N141.465 (7)C23—C2111.549 (6)
C13—C1111.556 (7)C23—H230.9800
C13—H130.9800N24—C251.336 (6)
N14—C151.333 (7)N24—C241.489 (6)
N14—C141.479 (6)C24—H24A0.9600
C14—H14A0.9600C24—H24B0.9600
C14—H14B0.9600C24—H24C0.9600
C14—H14C0.9600C25—O251.233 (6)
C15—O151.253 (6)C25—C261.524 (6)
C15—C161.521 (6)C26—S271.814 (5)
C16—S171.845 (5)C26—H260.9800
C16—H160.9800S27—C281.822 (5)
S17—C181.805 (6)C28—C291.518 (7)
C18—C191.534 (8)C28—H28A0.9700
C18—H18A0.9700C28—H28B0.9700
C18—H18B0.9700C29—C2101.540 (8)
C19—C1101.478 (8)C29—H29A0.9700
C19—H19A0.9700C29—H29B0.9700
C19—H19B0.9700C210—H21A0.9700
C110—H11A0.9700C210—H21B0.9700
C110—H11B0.9700C211—C2121.500 (6)
C111—C1121.495 (6)C211—H21C0.9700
C111—H11C0.9700C211—H21D0.9700
C111—H11D0.9700C212—C2171.394 (6)
C112—C1171.385 (6)C212—C2131.398 (6)
C112—C1131.395 (6)C213—C2141.374 (6)
C113—C1141.388 (7)C213—H2130.9300
C113—H1130.9300C214—C2151.391 (7)
C114—C1151.395 (7)C214—H2140.9300
C114—H1140.9300C215—C2161.392 (6)
C115—C1161.380 (7)C215—H2150.9300
C115—H1150.9300C216—C2171.376 (6)
C116—C1171.408 (7)C216—H2160.9300
C116—H1160.9300C217—H2170.9300
C117—H1170.9300O1W—H1W0.9138
N21—C221.360 (6)O1W—H2W0.8308
C12—N11—C16124.6 (4)C22—N21—C210119.2 (4)
C12—N11—C110120.2 (4)C26—N21—C210113.5 (4)
C16—N11—C110113.6 (4)O22—C22—N21122.8 (4)
O12—C12—N11122.8 (4)O22—C22—C23119.6 (4)
O12—C12—C13118.6 (5)N21—C22—C23117.5 (4)
N11—C12—C13118.6 (4)N24—C23—C22115.6 (4)
N14—C13—C12114.4 (4)N24—C23—C211112.0 (4)
N14—C13—C111112.9 (4)C22—C23—C211109.5 (3)
C12—C13—C111108.8 (4)N24—C23—H23106.4
N14—C13—H13106.8C22—C23—H23106.4
C12—C13—H13106.8C211—C23—H23106.4
C111—C13—H13106.8C25—N24—C23125.2 (4)
C15—N14—C13125.8 (4)C25—N24—C24119.1 (4)
C15—N14—C14118.7 (4)C23—N24—C24115.7 (4)
C13—N14—C14115.5 (5)N24—C24—H24A109.5
N14—C14—H14A109.5N24—C24—H24B109.5
N14—C14—H14B109.5H24A—C24—H24B109.5
H14A—C14—H14B109.5N24—C24—H24C109.5
N14—C14—H14C109.5H24A—C24—H24C109.5
H14A—C14—H14C109.5H24B—C24—H24C109.5
H14B—C14—H14C109.5O25—C25—N24123.0 (4)
O15—C15—N14125.0 (4)O25—C25—C26118.6 (4)
O15—C15—C16117.2 (5)N24—C25—C26118.4 (4)
N14—C15—C16117.7 (4)N21—C26—C25113.9 (4)
N11—C16—C15115.7 (4)N21—C26—S27113.4 (3)
N11—C16—S17111.6 (3)C25—C26—S27107.1 (3)
C15—C16—S17107.1 (3)N21—C26—H26107.3
N11—C16—H16107.4C25—C26—H26107.3
C15—C16—H16107.4S27—C26—H26107.3
S17—C16—H16107.4C26—S27—C2895.7 (2)
C18—S17—C1696.6 (2)C29—C28—S27112.9 (4)
C19—C18—S17111.3 (4)C29—C28—H28A109.0
C19—C18—H18A109.4S27—C28—H28A109.0
S17—C18—H18A109.4C29—C28—H28B109.0
C19—C18—H18B109.4S27—C28—H28B109.0
S17—C18—H18B109.4H28A—C28—H28B107.8
H18A—C18—H18B108.0C28—C29—C210110.0 (4)
C110—C19—C18112.5 (4)C28—C29—H29A109.7
C110—C19—H19A109.1C210—C29—H29A109.7
C18—C19—H19A109.1C28—C29—H29B109.7
C110—C19—H19B109.1C210—C29—H29B109.7
C18—C19—H19B109.1H29A—C29—H29B108.2
H19A—C19—H19B107.8N21—C210—C29111.4 (4)
C19—C110—N11111.9 (4)N21—C210—H21A109.3
C19—C110—H11A109.2C29—C210—H21A109.3
N11—C110—H11A109.2N21—C210—H21B109.3
C19—C110—H11B109.2C29—C210—H21B109.3
N11—C110—H11B109.2H21A—C210—H21B108.0
H11A—C110—H11B107.9C212—C211—C23113.1 (4)
C112—C111—C13114.3 (4)C212—C211—H21C109.0
C112—C111—H11C108.7C23—C211—H21C109.0
C13—C111—H11C108.7C212—C211—H21D109.0
C112—C111—H11D108.7C23—C211—H21D109.0
C13—C111—H11D108.7H21C—C211—H21D107.8
H11C—C111—H11D107.6C217—C212—C213118.5 (4)
C117—C112—C113120.1 (4)C217—C212—C211120.4 (4)
C117—C112—C111120.2 (4)C213—C212—C211121.0 (4)
C113—C112—C111119.6 (4)C214—C213—C212120.2 (4)
C114—C113—C112120.0 (4)C214—C213—H213119.9
C114—C113—H113120.0C212—C213—H213119.9
C112—C113—H113120.0C213—C214—C215120.8 (4)
C113—C114—C115119.8 (5)C213—C214—H214119.6
C113—C114—H114120.1C215—C214—H214119.6
C115—C114—H114120.1C214—C215—C216119.3 (4)
C116—C115—C114120.4 (5)C214—C215—H215120.3
C116—C115—H115119.8C216—C215—H215120.3
C114—C115—H115119.8C217—C216—C215119.7 (4)
C115—C116—C117119.7 (4)C217—C216—H216120.2
C115—C116—H116120.1C215—C216—H216120.2
C117—C116—H116120.1C216—C217—C212121.3 (4)
C112—C117—C116119.8 (4)C216—C217—H217119.3
C112—C117—H117120.1C212—C217—H217119.3
C116—C117—H117120.1H1W—O1W—H2W99.5
C22—N21—C26125.4 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1W—H1W···O25i0.912.112.983 (5)159
O1W—H2W···O15i0.832.273.037 (5)154
Symmetry code: (i) x, y+1, z.
(4b) top
Crystal data top
C15H18N2O2SF(000) = 616
Mr = 290.37Dx = 1.329 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71070 Å
Hall symbol: P 2ac 2abCell parameters from 10583 reflections
a = 6.2287 (1) Åθ = 1–27.5°
b = 8.9737 (3) ŵ = 0.23 mm1
c = 25.9694 (7) ÅT = 150 K
V = 1451.55 (7) Å3Bar, colourless
Z = 40.4 × 0.25 × 0.25 mm
Data collection top
Nonius KappaCCD area detector
diffractometer
2975 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.035
Graphite monochromatorθmax = 27.5°, θmin = 3.1°
Detector resolution: 9.091 pixels mm-1h = 88
φ and ω scans to fill the Ewald spherek = 1111
11349 measured reflectionsl = 3333
3296 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.032 w = 1/[σ2(Fo2) + (0.0234P)2 + 0.431P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.073(Δ/σ)max = 0.002
S = 1.04Δρmax = 0.18 e Å3
3296 reflectionsΔρmin = 0.23 e Å3
183 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.036 (2)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Secondary atom site location: difference Fourier mapAbsolute structure parameter: 0.01 (6)
Special details top

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 (Å2) top
xyzUiso*/Ueq
N10.4052 (2)0.92175 (15)0.68106 (5)0.0206 (3)
C20.6083 (2)0.91855 (18)0.66408 (6)0.0209 (3)
C30.6519 (3)0.85243 (18)0.61181 (6)0.0231 (3)
H30.78070.79030.61470.028*
N40.4801 (2)0.75947 (16)0.59111 (5)0.0226 (3)
C40.5337 (3)0.6728 (2)0.54519 (6)0.0311 (4)
H4A0.43790.58940.54240.047*
H4B0.67880.63750.54780.047*
H4C0.51960.73460.51520.047*
C50.2757 (2)0.76196 (18)0.60745 (6)0.0217 (3)
C60.2306 (2)0.83673 (19)0.65878 (6)0.0202 (3)
H60.10720.90330.65440.024*
S70.15137 (7)0.68411 (5)0.702119 (16)0.02814 (12)
C80.1114 (3)0.7946 (2)0.76006 (6)0.0290 (4)
H8A0.01530.85620.75570.035*
H8B0.08560.72820.78890.035*
O20.75784 (18)0.97884 (13)0.68699 (4)0.0280 (3)
O50.12814 (18)0.69978 (14)0.58448 (4)0.0292 (3)
C90.3017 (3)0.8936 (2)0.77244 (6)0.0268 (4)
H9A0.42640.83180.77910.032*
H9B0.27120.95000.80350.032*
C100.3527 (3)1.00125 (18)0.72882 (6)0.0242 (3)
H10A0.22991.06550.72290.029*
H10B0.47311.06360.73870.029*
C110.7055 (3)0.9840 (2)0.57508 (6)0.0291 (4)
H11A0.83631.03200.58670.035*
H11B0.73110.94520.54080.035*
C120.5283 (3)1.0979 (2)0.57273 (6)0.0271 (4)
C130.3553 (3)1.0807 (2)0.53912 (7)0.0322 (4)
H130.35180.99930.51690.039*
C140.1895 (3)1.1825 (2)0.53832 (7)0.0402 (5)
H140.07591.16960.51550.048*
C150.1910 (3)1.3029 (2)0.57103 (8)0.0438 (5)
H150.07861.37100.57050.053*
C160.3615 (4)1.3220 (2)0.60485 (7)0.0445 (5)
H160.36321.40290.62730.053*
C170.5288 (3)1.2207 (2)0.60510 (7)0.0350 (4)
H170.64371.23520.62740.042*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0207 (6)0.0218 (7)0.0195 (6)0.0001 (6)0.0012 (5)0.0019 (6)
C20.0176 (7)0.0217 (8)0.0234 (8)0.0032 (6)0.0029 (6)0.0012 (7)
C30.0161 (7)0.0278 (9)0.0253 (8)0.0008 (7)0.0011 (7)0.0032 (6)
N40.0202 (6)0.0252 (7)0.0223 (7)0.0002 (6)0.0005 (5)0.0040 (6)
C40.0292 (9)0.0361 (10)0.0281 (8)0.0005 (8)0.0032 (7)0.0104 (8)
C50.0214 (7)0.0215 (8)0.0223 (8)0.0010 (6)0.0015 (6)0.0010 (7)
C60.0158 (7)0.0228 (8)0.0219 (7)0.0009 (6)0.0005 (6)0.0015 (7)
S70.0314 (2)0.0253 (2)0.0278 (2)0.00572 (19)0.00419 (18)0.00170 (18)
C80.0310 (9)0.0327 (10)0.0233 (8)0.0001 (8)0.0044 (7)0.0046 (7)
O20.0206 (6)0.0328 (7)0.0306 (6)0.0003 (5)0.0043 (5)0.0053 (5)
O50.0226 (6)0.0347 (7)0.0302 (6)0.0026 (6)0.0042 (5)0.0067 (5)
C90.0299 (9)0.0295 (9)0.0211 (8)0.0051 (7)0.0000 (7)0.0013 (7)
C100.0259 (8)0.0234 (8)0.0232 (7)0.0001 (7)0.0032 (7)0.0049 (7)
C110.0248 (8)0.0381 (10)0.0245 (8)0.0082 (8)0.0068 (7)0.0027 (8)
C120.0322 (9)0.0287 (10)0.0205 (8)0.0078 (8)0.0035 (7)0.0057 (7)
C130.0381 (10)0.0299 (9)0.0286 (9)0.0114 (9)0.0043 (8)0.0076 (7)
C140.0400 (10)0.0381 (11)0.0425 (10)0.0099 (10)0.0112 (8)0.0165 (10)
C150.0470 (11)0.0366 (11)0.0478 (11)0.0072 (10)0.0025 (9)0.0144 (10)
C160.0671 (13)0.0327 (10)0.0339 (9)0.0075 (12)0.0062 (10)0.0000 (9)
C170.0460 (11)0.0327 (11)0.0263 (9)0.0024 (9)0.0077 (8)0.0021 (8)
Geometric parameters (Å, º) top
N1—C21.340 (2)C8—H8B0.9700
N1—C61.449 (2)C9—C101.522 (2)
N1—C101.468 (2)C9—H9A0.9700
C2—O21.2305 (19)C9—H9B0.9700
C2—C31.506 (2)C10—H10A0.9700
C3—N41.459 (2)C10—H10B0.9700
C3—C111.554 (2)C11—C121.505 (3)
C3—H30.9800C11—H11A0.9700
N4—C51.342 (2)C11—H11B0.9700
N4—C41.462 (2)C12—C171.386 (3)
C4—H4A0.9600C12—C131.395 (2)
C4—H4B0.9600C13—C141.379 (3)
C4—H4C0.9600C13—H130.9300
C5—O51.2297 (19)C14—C151.374 (3)
C5—C61.519 (2)C14—H140.9300
C6—S71.8400 (16)C15—C161.389 (3)
C6—H60.9800C15—H150.9300
S7—C81.8189 (17)C16—C171.383 (3)
C8—C91.516 (2)C16—H160.9300
C8—H8A0.9700C17—H170.9300
C2—N1—C6124.48 (13)C8—C9—C10112.15 (14)
C2—N1—C10119.92 (13)C8—C9—H9A109.2
C6—N1—C10115.21 (12)C10—C9—H9A109.2
O2—C2—N1123.10 (15)C8—C9—H9B109.2
O2—C2—C3118.20 (14)C10—C9—H9B109.2
N1—C2—C3118.36 (13)H9A—C9—H9B107.9
N4—C3—C2115.15 (13)N1—C10—C9111.54 (13)
N4—C3—C11111.44 (13)N1—C10—H10A109.3
C2—C3—C11107.02 (13)C9—C10—H10A109.3
N4—C3—H3107.6N1—C10—H10B109.3
C2—C3—H3107.6C9—C10—H10B109.3
C11—C3—H3107.6H10A—C10—H10B108.0
C5—N4—C3124.71 (13)C12—C11—C3112.54 (13)
C5—N4—C4118.89 (14)C12—C11—H11A109.1
C3—N4—C4115.93 (13)C3—C11—H11A109.1
N4—C4—H4A109.5C12—C11—H11B109.1
N4—C4—H4B109.5C3—C11—H11B109.1
H4A—C4—H4B109.5H11A—C11—H11B107.8
N4—C4—H4C109.5C17—C12—C13117.97 (17)
H4A—C4—H4C109.5C17—C12—C11120.90 (16)
H4B—C4—H4C109.5C13—C12—C11121.10 (16)
O5—C5—N4123.24 (15)C14—C13—C12120.98 (18)
O5—C5—C6119.20 (13)C14—C13—H13119.5
N4—C5—C6117.42 (13)C12—C13—H13119.5
N1—C6—C5116.37 (12)C15—C14—C13120.40 (18)
N1—C6—S7110.43 (10)C15—C14—H14119.8
C5—C6—S7104.93 (11)C13—C14—H14119.8
N1—C6—H6108.3C14—C15—C16119.6 (2)
C5—C6—H6108.3C14—C15—H15120.2
S7—C6—H6108.3C16—C15—H15120.2
C8—S7—C697.88 (8)C17—C16—C15119.84 (19)
C9—C8—S7112.82 (12)C17—C16—H16120.1
C9—C8—H8A109.0C15—C16—H16120.1
S7—C8—H8A109.0C16—C17—C12121.22 (18)
C9—C8—H8B109.0C16—C17—H17119.4
S7—C8—H8B109.0C12—C17—H17119.4
H8A—C8—H8B107.8
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3···O5i0.982.443.3435 (19)153
C6—H6···O2ii0.982.433.2916 (19)146
C8—H8A···O2ii0.972.533.344 (2)142
C8—H8B···O2iii0.972.523.253 (2)132
Symmetry codes: (i) x+1, y, z; (ii) x1, y, z; (iii) x+1, y1/2, z+3/2.
(6a) top
Crystal data top
C15H18N2O2SF(000) = 616
Mr = 290.37Dx = 1.373 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71070 Å
Hall symbol: P 2ybCell parameters from 28687 reflections
a = 7.3126 (1) Åθ = 1–27.5°
b = 27.1077 (5) ŵ = 0.23 mm1
c = 7.3745 (1) ÅT = 150 K
β = 106.0640 (11)°Plate, colourless
V = 1404.75 (4) Å30.42 × 0.42 × 0.08 mm
Z = 4
Data collection top
Nonius KappaCCD area detector
diffractometer
5572 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.032
Graphite monochromatorθmax = 27.4°, θmin = 2.9°
Detector resolution: 9.091 pixels mm-1h = 99
φ and ω scans to fill the Ewald spherek = 3534
22183 measured reflectionsl = 99
6211 independent reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.034H-atom parameters constrained
wR(F2) = 0.083 w = 1/[σ2(Fo2) + (0.0376P)2 + 0.3225P]
where P = (Fo2 + 2Fc2)/3
S = 1.05(Δ/σ)max = 0.001
6211 reflectionsΔρmax = 0.16 e Å3
363 parametersΔρmin = 0.22 e Å3
1 restraintAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.03 (6)
Special details top

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 (Å2) top
xyzUiso*/Ueq
N10.6695 (2)0.82534 (6)0.2140 (2)0.0204 (3)
C20.8202 (2)0.85551 (7)0.2369 (2)0.0210 (4)
O20.91482 (19)0.85832 (5)0.12241 (18)0.0309 (3)
C30.8767 (2)0.88835 (6)0.4094 (2)0.0199 (4)
H30.88860.92190.36410.024*
N40.7370 (2)0.89062 (5)0.5170 (2)0.0208 (3)
C40.7637 (3)0.92884 (7)0.6628 (3)0.0290 (4)
H4A0.64200.93920.67460.044*
H4B0.82840.95660.62810.044*
H4C0.83840.91580.78120.044*
C50.6088 (2)0.85508 (7)0.5159 (2)0.0213 (4)
O50.51521 (18)0.85330 (6)0.63010 (19)0.0315 (3)
C60.5693 (2)0.81742 (7)0.3573 (2)0.0208 (4)
H60.43320.81980.29240.025*
C70.6024 (3)0.76511 (7)0.4384 (3)0.0249 (4)
H7A0.53750.76130.53580.030*
H7B0.73740.76020.49600.030*
S80.51661 (8)0.71900 (2)0.25788 (7)0.03646 (13)
C90.6426 (3)0.74036 (8)0.0920 (3)0.0343 (5)
H9A0.77800.73510.14580.041*
H9B0.60210.72110.02300.041*
C100.6069 (3)0.79455 (7)0.0445 (3)0.0274 (4)
H10A0.67500.80420.04570.033*
H10B0.47220.79980.01360.033*
C111.0765 (2)0.87324 (7)0.5329 (3)0.0241 (4)
H11A1.16650.87620.45840.029*
H11B1.11550.89600.63800.029*
C121.0851 (2)0.82146 (7)0.6089 (3)0.0219 (4)
C131.1236 (2)0.78173 (7)0.5059 (3)0.0268 (4)
H131.14370.78720.38840.032*
C141.1325 (3)0.73414 (8)0.5757 (3)0.0370 (5)
H141.15850.70790.50540.044*
C151.1026 (3)0.72561 (8)0.7511 (4)0.0426 (6)
H151.10960.69370.79880.051*
C161.0626 (3)0.76446 (9)0.8540 (3)0.0393 (5)
H161.04160.75880.97100.047*
C171.0536 (3)0.81206 (8)0.7832 (3)0.0285 (4)
H171.02600.83810.85340.034*
N211.0345 (2)0.52543 (5)1.0909 (2)0.0205 (3)
C221.0110 (2)0.49609 (7)0.9391 (2)0.0211 (3)
O221.12701 (18)0.49369 (5)0.84587 (19)0.0306 (3)
C230.8353 (2)0.46406 (7)0.8797 (2)0.0203 (4)
H230.87920.43050.86520.024*
N240.7251 (2)0.46122 (6)1.0170 (2)0.0211 (3)
C240.5776 (3)0.42313 (7)0.9868 (3)0.0287 (4)
H24A0.56870.41111.10650.043*
H24B0.61000.39640.91610.043*
H24C0.45760.43690.91790.043*
C250.7300 (2)0.49543 (7)1.1490 (2)0.0210 (4)
O250.61701 (19)0.49628 (5)1.24486 (18)0.0313 (3)
C260.8884 (3)0.53334 (7)1.1898 (2)0.0211 (4)
H260.95290.53101.32500.025*
C270.8058 (3)0.58555 (7)1.1555 (3)0.0266 (4)
H27A0.70820.58951.22060.032*
H27B0.74670.59011.02160.032*
S280.98609 (8)0.632028 (19)1.23693 (8)0.03969 (15)
C291.1537 (3)0.61042 (8)1.1143 (3)0.0380 (5)
H29A1.09930.61500.97970.046*
H29B1.26880.63011.15290.046*
C2101.2044 (3)0.55644 (7)1.1538 (3)0.0298 (4)
H21A1.29700.54671.08850.036*
H21B1.26120.55181.28800.036*
C2110.7127 (3)0.48051 (7)0.6822 (2)0.0256 (4)
H21C0.78730.47690.59280.031*
H21D0.60370.45870.64250.031*
C2120.6428 (3)0.53313 (7)0.6757 (2)0.0228 (4)
C2130.7540 (3)0.57185 (7)0.6387 (3)0.0270 (4)
H2130.87120.56490.61780.032*
C2140.6922 (3)0.62023 (8)0.6327 (3)0.0334 (5)
H2140.76750.64560.60800.040*
C2150.5181 (3)0.63075 (9)0.6635 (3)0.0381 (5)
H2150.47590.66320.65940.046*
C2160.4071 (3)0.59288 (9)0.7004 (3)0.0373 (5)
H2160.28990.59990.72070.045*
C2170.4696 (3)0.54443 (8)0.7073 (3)0.0287 (4)
H2170.39430.51930.73340.034*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0234 (7)0.0190 (7)0.0191 (7)0.0015 (6)0.0063 (6)0.0008 (6)
C20.0228 (8)0.0184 (9)0.0217 (8)0.0007 (7)0.0062 (7)0.0019 (7)
O20.0368 (7)0.0333 (8)0.0284 (7)0.0069 (6)0.0191 (6)0.0027 (6)
C30.0193 (8)0.0179 (9)0.0241 (9)0.0027 (7)0.0084 (7)0.0012 (7)
N40.0199 (7)0.0198 (8)0.0241 (8)0.0008 (6)0.0083 (6)0.0033 (6)
C40.0310 (10)0.0252 (10)0.0313 (10)0.0022 (8)0.0094 (8)0.0084 (8)
C50.0165 (7)0.0239 (9)0.0231 (8)0.0020 (7)0.0047 (7)0.0014 (7)
O50.0248 (6)0.0415 (8)0.0327 (7)0.0019 (6)0.0154 (6)0.0017 (6)
C60.0170 (8)0.0205 (9)0.0235 (9)0.0004 (7)0.0036 (7)0.0021 (7)
C70.0243 (9)0.0241 (10)0.0251 (9)0.0023 (7)0.0046 (7)0.0035 (8)
S80.0470 (3)0.0228 (3)0.0361 (3)0.0120 (2)0.0056 (2)0.0013 (2)
C90.0483 (12)0.0237 (10)0.0310 (11)0.0027 (9)0.0113 (10)0.0046 (8)
C100.0335 (10)0.0256 (10)0.0207 (9)0.0033 (8)0.0036 (8)0.0026 (8)
C110.0189 (8)0.0232 (9)0.0300 (9)0.0029 (7)0.0065 (8)0.0010 (7)
C120.0134 (7)0.0242 (9)0.0266 (9)0.0009 (7)0.0028 (7)0.0008 (7)
C130.0174 (8)0.0305 (11)0.0315 (10)0.0002 (7)0.0052 (8)0.0046 (8)
C140.0252 (9)0.0259 (11)0.0543 (14)0.0037 (8)0.0018 (9)0.0065 (9)
C150.0311 (11)0.0302 (12)0.0584 (15)0.0021 (9)0.0009 (10)0.0160 (11)
C160.0319 (11)0.0508 (14)0.0336 (11)0.0017 (10)0.0066 (9)0.0171 (10)
C170.0214 (9)0.0360 (12)0.0268 (10)0.0021 (8)0.0046 (8)0.0010 (8)
N210.0188 (7)0.0191 (7)0.0236 (7)0.0020 (6)0.0060 (6)0.0021 (6)
C220.0215 (8)0.0182 (9)0.0241 (8)0.0004 (7)0.0071 (7)0.0016 (7)
O220.0267 (7)0.0326 (8)0.0381 (7)0.0030 (6)0.0184 (6)0.0050 (6)
C230.0218 (8)0.0187 (9)0.0213 (8)0.0002 (7)0.0079 (7)0.0029 (7)
N240.0229 (7)0.0200 (8)0.0211 (7)0.0042 (6)0.0074 (6)0.0007 (6)
C240.0268 (9)0.0270 (10)0.0329 (10)0.0082 (8)0.0090 (8)0.0004 (8)
C250.0235 (8)0.0222 (9)0.0173 (8)0.0021 (7)0.0055 (7)0.0030 (7)
O250.0331 (7)0.0396 (8)0.0260 (7)0.0021 (6)0.0162 (6)0.0015 (6)
C260.0245 (9)0.0211 (9)0.0169 (8)0.0017 (7)0.0044 (7)0.0013 (7)
C270.0288 (10)0.0225 (10)0.0268 (9)0.0040 (7)0.0048 (8)0.0021 (8)
S280.0426 (3)0.0207 (3)0.0504 (3)0.0008 (2)0.0039 (3)0.0115 (2)
C290.0370 (12)0.0255 (11)0.0501 (13)0.0110 (9)0.0093 (10)0.0016 (10)
C2100.0224 (9)0.0285 (11)0.0364 (11)0.0058 (8)0.0045 (8)0.0025 (8)
C2110.0312 (10)0.0280 (10)0.0175 (8)0.0028 (8)0.0064 (8)0.0042 (7)
C2120.0262 (9)0.0265 (10)0.0143 (8)0.0008 (7)0.0035 (7)0.0005 (7)
C2130.0293 (10)0.0319 (11)0.0216 (9)0.0024 (8)0.0101 (8)0.0032 (8)
C2140.0416 (12)0.0298 (12)0.0285 (10)0.0007 (9)0.0091 (9)0.0064 (8)
C2150.0462 (12)0.0328 (12)0.0323 (11)0.0135 (10)0.0057 (10)0.0049 (9)
C2160.0282 (11)0.0507 (14)0.0326 (11)0.0141 (10)0.0078 (9)0.0051 (10)
C2170.0241 (9)0.0384 (12)0.0224 (9)0.0006 (8)0.0045 (8)0.0034 (8)
Geometric parameters (Å, º) top
N1—C21.345 (2)N21—C221.345 (2)
N1—C61.459 (2)N21—C2101.465 (2)
N1—C101.467 (2)N21—C261.467 (2)
C2—O21.233 (2)C22—O221.233 (2)
C2—C31.514 (2)C22—C231.512 (2)
C3—N41.459 (2)C23—N241.461 (2)
C3—C111.547 (3)C23—C2111.549 (2)
C3—H30.9800C23—H230.9800
N4—C51.343 (2)N24—C251.338 (2)
N4—C41.467 (2)N24—C241.465 (2)
C4—H4A0.9600C24—H24A0.9600
C4—H4B0.9600C24—H24B0.9600
C4—H4C0.9600C24—H24C0.9600
C5—O51.224 (2)C25—O251.227 (2)
C5—C61.519 (3)C25—C261.515 (3)
C6—C71.532 (3)C26—C271.532 (3)
C6—H60.9800C26—H260.9800
C7—S81.8072 (19)C27—S281.802 (2)
C7—H7A0.9700C27—H27A0.9700
C7—H7B0.9700C27—H27B0.9700
S8—C91.817 (2)S28—C291.810 (2)
C9—C101.516 (3)C29—C2101.518 (3)
C9—H9A0.9700C29—H29A0.9700
C9—H9B0.9700C29—H29B0.9700
C10—H10A0.9700C210—H21A0.9700
C10—H10B0.9700C210—H21B0.9700
C11—C121.506 (3)C211—C2121.512 (3)
C11—H11A0.9700C211—H21C0.9700
C11—H11B0.9700C211—H21D0.9700
C12—C171.391 (3)C212—C2171.384 (3)
C12—C131.391 (3)C212—C2131.400 (3)
C13—C141.384 (3)C213—C2141.384 (3)
C13—H130.9300C213—H2130.9300
C14—C151.389 (4)C214—C2151.384 (3)
C14—H140.9300C214—H2140.9300
C15—C161.376 (4)C215—C2161.381 (3)
C15—H150.9300C215—H2150.9300
C16—C171.387 (3)C216—C2171.387 (3)
C16—H160.9300C216—H2160.9300
C17—H170.9300C217—H2170.9300
C2—N1—C6123.85 (14)C22—N21—C210120.33 (15)
C2—N1—C10120.27 (15)C22—N21—C26123.87 (14)
C6—N1—C10115.66 (14)C210—N21—C26115.43 (14)
O2—C2—N1123.18 (16)O22—C22—N21123.10 (16)
O2—C2—C3117.70 (15)O22—C22—C23117.95 (15)
N1—C2—C3119.12 (14)N21—C22—C23118.94 (14)
N4—C3—C2114.38 (14)N24—C23—C22114.64 (14)
N4—C3—C11112.35 (14)N24—C23—C211112.34 (14)
C2—C3—C11109.43 (14)C22—C23—C211109.38 (15)
N4—C3—H3106.7N24—C23—H23106.7
C2—C3—H3106.7C22—C23—H23106.7
C11—C3—H3106.7C211—C23—H23106.7
C5—N4—C3124.02 (14)C25—N24—C23124.01 (14)
C5—N4—C4117.57 (15)C25—N24—C24118.03 (15)
C3—N4—C4117.21 (14)C23—N24—C24117.11 (14)
N4—C4—H4A109.5N24—C24—H24A109.5
N4—C4—H4B109.5N24—C24—H24B109.5
H4A—C4—H4B109.5H24A—C24—H24B109.5
N4—C4—H4C109.5N24—C24—H24C109.5
H4A—C4—H4C109.5H24A—C24—H24C109.5
H4B—C4—H4C109.5H24B—C24—H24C109.5
O5—C5—N4123.10 (17)O25—C25—N24123.05 (16)
O5—C5—C6118.68 (15)O25—C25—C26118.20 (15)
N4—C5—C6118.10 (14)N24—C25—C26118.67 (14)
N1—C6—C5115.62 (14)N21—C26—C25115.12 (14)
N1—C6—C7111.25 (14)N21—C26—C27111.14 (15)
C5—C6—C7110.23 (14)C25—C26—C27110.45 (14)
N1—C6—H6106.4N21—C26—H26106.5
C5—C6—H6106.4C25—C26—H26106.5
C7—C6—H6106.4C27—C26—H26106.5
C6—C7—S8111.56 (12)C26—C27—S28111.88 (13)
C6—C7—H7A109.3C26—C27—H27A109.2
S8—C7—H7A109.3S28—C27—H27A109.2
C6—C7—H7B109.3C26—C27—H27B109.2
S8—C7—H7B109.3S28—C27—H27B109.2
H7A—C7—H7B108.0H27A—C27—H27B107.9
C7—S8—C997.94 (9)C27—S28—C2998.12 (9)
C10—C9—S8112.20 (15)C210—C29—S28112.30 (16)
C10—C9—H9A109.2C210—C29—H29A109.1
S8—C9—H9A109.2S28—C29—H29A109.1
C10—C9—H9B109.2C210—C29—H29B109.1
S8—C9—H9B109.2S28—C29—H29B109.1
H9A—C9—H9B107.9H29A—C29—H29B107.9
N1—C10—C9111.16 (16)N21—C210—C29110.59 (16)
N1—C10—H10A109.4N21—C210—H21A109.5
C9—C10—H10A109.4C29—C210—H21A109.5
N1—C10—H10B109.4N21—C210—H21B109.5
C9—C10—H10B109.4C29—C210—H21B109.5
H10A—C10—H10B108.0H21A—C210—H21B108.1
C12—C11—C3113.65 (14)C212—C211—C23113.86 (14)
C12—C11—H11A108.8C212—C211—H21C108.8
C3—C11—H11A108.8C23—C211—H21C108.8
C12—C11—H11B108.8C212—C211—H21D108.8
C3—C11—H11B108.8C23—C211—H21D108.8
H11A—C11—H11B107.7H21C—C211—H21D107.7
C17—C12—C13118.23 (18)C217—C212—C213118.36 (18)
C17—C12—C11120.96 (17)C217—C212—C211121.38 (18)
C13—C12—C11120.80 (17)C213—C212—C211120.25 (17)
C14—C13—C12120.97 (19)C214—C213—C212120.95 (18)
C14—C13—H13119.5C214—C213—H213119.5
C12—C13—H13119.5C212—C213—H213119.5
C13—C14—C15119.9 (2)C215—C214—C213119.8 (2)
C13—C14—H14120.1C215—C214—H214120.1
C15—C14—H14120.1C213—C214—H214120.1
C16—C15—C14119.9 (2)C216—C215—C214119.8 (2)
C16—C15—H15120.1C216—C215—H215120.1
C14—C15—H15120.1C214—C215—H215120.1
C15—C16—C17120.0 (2)C215—C216—C217120.37 (19)
C15—C16—H16120.0C215—C216—H216119.8
C17—C16—H16120.0C217—C216—H216119.8
C16—C17—C12121.0 (2)C212—C217—C216120.7 (2)
C16—C17—H17119.5C212—C217—H217119.6
C12—C17—H17119.5C216—C217—H217119.6
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3···O22i0.982.473.416 (2)162
C11—H11A···O5ii0.972.593.135 (2)116
C17—H17···O2iii0.932.413.204 (2)144
C211—H21C···O25iv0.972.583.135 (2)117
C23—H23···O2v0.982.463.402 (2)162
C217—H217···O22vi0.932.433.260 (2)149
Symmetry codes: (i) x+2, y+1/2, z+1; (ii) x+1, y, z; (iii) x, y, z+1; (iv) x, y, z1; (v) x+2, y1/2, z+1; (vi) x1, y, z.
(6b) top
Crystal data top
C15H18N2O2SF(000) = 616
Mr = 290.37Dx = 1.325 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71070 Å
Hall symbol: P 2ybCell parameters from 16855 reflections
a = 9.8928 (2) Åθ = 1–27.5°
b = 9.0312 (2) ŵ = 0.23 mm1
c = 16.4470 (5) ÅT = 150 K
β = 97.8246 (15)°Bar, colourless
V = 1455.76 (6) Å30.5 × 0.15 × 0.1 mm
Z = 4
Data collection top
Nonius KappaCCD area detector
diffractometer
5781 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.045
Graphite monochromatorθmax = 27.5°, θmin = 3.2°
Detector resolution: 9.091 pixels mm-1h = 1212
φ and ω scans to fill the Ewald spherek = 1111
23095 measured reflectionsl = 2121
6621 independent reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039H-atom parameters constrained
wR(F2) = 0.082 w = 1/[σ2(Fo2) + (0.0316P)2 + 0.3753P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.001
6621 reflectionsΔρmax = 0.22 e Å3
363 parametersΔρmin = 0.22 e Å3
1 restraintAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.06 (5)
Special details top

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 (Å2) top
xyzUiso*/Ueq
N10.26974 (15)0.09585 (17)0.37766 (9)0.0226 (3)
C20.36775 (19)0.04534 (19)0.33489 (11)0.0231 (4)
O20.34415 (14)0.03944 (14)0.27615 (8)0.0323 (3)
C30.51233 (19)0.0982 (2)0.35878 (12)0.0248 (4)
H30.57200.01120.36100.030*
N40.53693 (14)0.17062 (17)0.43830 (9)0.0237 (3)
C40.67909 (19)0.1838 (3)0.47573 (13)0.0359 (5)
H4A0.72040.26710.45250.054*
H4B0.72760.09510.46550.054*
H4C0.68270.19790.53380.054*
C50.44075 (19)0.24650 (19)0.47023 (11)0.0236 (4)
O50.46557 (13)0.33206 (15)0.52862 (8)0.0319 (3)
C60.29172 (18)0.21877 (19)0.43574 (11)0.0222 (4)
H60.25520.30900.40790.027*
C70.21595 (18)0.1919 (2)0.50931 (12)0.0302 (4)
H7A0.23400.27370.54740.036*
H7B0.25130.10260.53730.036*
S80.03443 (5)0.17300 (7)0.48181 (3)0.03746 (13)
C90.0414 (2)0.0221 (2)0.41060 (13)0.0341 (5)
H9A0.07910.06460.44020.041*
H9B0.05040.00180.38530.041*
C100.12734 (19)0.0608 (2)0.34480 (12)0.0303 (4)
H10A0.12640.02180.30700.036*
H10B0.08720.14530.31410.036*
C110.54995 (19)0.2002 (2)0.28941 (12)0.0281 (4)
H11A0.64600.22510.30080.034*
H11B0.53600.14620.23800.034*
C120.46810 (18)0.3411 (2)0.27977 (11)0.0258 (4)
C130.5105 (2)0.4683 (2)0.32414 (12)0.0290 (4)
H130.59080.46600.36090.035*
C140.4355 (2)0.5978 (2)0.31452 (13)0.0319 (4)
H140.46600.68180.34420.038*
C150.3155 (2)0.6026 (2)0.26090 (13)0.0328 (5)
H150.26490.68960.25440.039*
C160.2707 (2)0.4774 (2)0.21691 (14)0.0354 (5)
H160.18910.47970.18140.042*
C170.34728 (19)0.3483 (2)0.22556 (12)0.0298 (4)
H170.31750.26540.19470.036*
N210.79215 (15)0.66563 (17)0.22461 (9)0.0244 (3)
C220.73000 (18)0.7944 (2)0.23921 (11)0.0229 (4)
O220.76346 (13)0.87162 (14)0.29992 (8)0.0300 (3)
C230.61717 (17)0.8489 (2)0.17468 (10)0.0225 (4)
H230.54580.89110.20350.027*
N240.55451 (16)0.73322 (16)0.12097 (9)0.0253 (3)
C240.4176 (2)0.7611 (2)0.07789 (14)0.0361 (5)
H24A0.42440.80410.02520.054*
H24B0.37030.82800.10950.054*
H24C0.36830.66940.07060.054*
C250.6247 (2)0.6169 (2)0.09895 (12)0.0305 (4)
O250.57947 (18)0.53368 (18)0.04268 (10)0.0502 (4)
C260.76157 (19)0.5811 (2)0.14838 (11)0.0250 (4)
H260.83340.60010.11420.030*
C270.7582 (2)0.4150 (2)0.16631 (13)0.0292 (4)
H27A0.73850.36230.11470.035*
H27B0.68410.39540.19790.035*
S280.91319 (6)0.34311 (6)0.22139 (3)0.03858 (14)
C290.9283 (2)0.4728 (2)0.30545 (13)0.0379 (5)
H29A0.85500.45580.33800.046*
H29B1.01410.45630.34040.046*
C2100.9224 (2)0.6310 (2)0.27577 (13)0.0318 (5)
H21A0.93450.69690.32280.038*
H21B0.99680.64840.24420.038*
C2110.67422 (19)0.9770 (2)0.12559 (12)0.0257 (4)
H21C0.60331.01060.08300.031*
H21D0.69921.05960.16230.031*
C2120.7969 (2)0.9300 (2)0.08679 (12)0.0271 (4)
C2130.7833 (2)0.8635 (2)0.00970 (12)0.0344 (5)
H2130.69760.85640.02130.041*
C2140.8968 (3)0.8079 (3)0.02118 (14)0.0482 (6)
H2140.88650.76090.07200.058*
C2151.0254 (3)0.8222 (3)0.02349 (15)0.0580 (7)
H2151.10140.78530.00260.070*
C2161.0402 (2)0.8911 (3)0.09866 (15)0.0495 (7)
H2161.12650.90150.12850.059*
C2170.9277 (2)0.9447 (2)0.12983 (13)0.0359 (5)
H2170.93900.99160.18060.043*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0204 (7)0.0213 (7)0.0257 (8)0.0002 (6)0.0012 (6)0.0042 (6)
C20.0299 (10)0.0158 (8)0.0240 (9)0.0038 (7)0.0053 (8)0.0024 (7)
O20.0402 (8)0.0252 (7)0.0327 (7)0.0007 (6)0.0095 (6)0.0085 (6)
C30.0262 (9)0.0177 (8)0.0318 (10)0.0035 (8)0.0083 (8)0.0018 (8)
N40.0182 (7)0.0239 (7)0.0286 (8)0.0015 (7)0.0018 (6)0.0003 (7)
C40.0207 (9)0.0415 (11)0.0450 (12)0.0004 (9)0.0020 (9)0.0040 (11)
C50.0258 (9)0.0193 (9)0.0254 (9)0.0004 (7)0.0030 (8)0.0015 (8)
O50.0317 (7)0.0316 (7)0.0311 (7)0.0041 (6)0.0002 (6)0.0095 (6)
C60.0227 (9)0.0195 (9)0.0240 (9)0.0024 (7)0.0017 (7)0.0013 (7)
C70.0244 (9)0.0397 (11)0.0261 (9)0.0019 (9)0.0022 (8)0.0048 (9)
S80.0222 (2)0.0525 (3)0.0387 (3)0.0000 (2)0.0078 (2)0.0081 (3)
C90.0221 (10)0.0367 (11)0.0426 (12)0.0052 (9)0.0013 (9)0.0015 (10)
C100.0245 (10)0.0338 (11)0.0307 (11)0.0006 (8)0.0037 (8)0.0057 (9)
C110.0289 (10)0.0236 (9)0.0343 (11)0.0002 (8)0.0128 (8)0.0012 (8)
C120.0299 (10)0.0225 (8)0.0274 (9)0.0021 (8)0.0125 (8)0.0029 (8)
C130.0288 (10)0.0257 (10)0.0317 (10)0.0031 (8)0.0016 (8)0.0000 (8)
C140.0385 (12)0.0217 (9)0.0369 (11)0.0029 (9)0.0096 (9)0.0035 (9)
C150.0366 (11)0.0221 (9)0.0408 (12)0.0054 (9)0.0089 (9)0.0027 (9)
C160.0317 (11)0.0312 (11)0.0413 (12)0.0014 (9)0.0024 (9)0.0012 (9)
C170.0365 (11)0.0218 (9)0.0305 (10)0.0045 (9)0.0026 (8)0.0038 (9)
N210.0256 (8)0.0240 (8)0.0227 (8)0.0044 (7)0.0002 (6)0.0000 (7)
C220.0228 (9)0.0235 (9)0.0232 (10)0.0017 (7)0.0057 (8)0.0006 (7)
O220.0350 (7)0.0298 (7)0.0249 (7)0.0010 (6)0.0030 (6)0.0064 (6)
C230.0231 (9)0.0220 (8)0.0226 (9)0.0023 (8)0.0035 (7)0.0037 (8)
N240.0229 (8)0.0252 (8)0.0264 (8)0.0000 (6)0.0013 (6)0.0012 (7)
C240.0279 (11)0.0348 (11)0.0421 (12)0.0006 (9)0.0085 (9)0.0054 (10)
C250.0362 (11)0.0246 (10)0.0287 (10)0.0011 (9)0.0026 (9)0.0016 (8)
O250.0594 (11)0.0387 (9)0.0449 (9)0.0107 (8)0.0198 (8)0.0166 (8)
C260.0297 (10)0.0223 (9)0.0231 (9)0.0024 (8)0.0041 (8)0.0028 (7)
C270.0301 (11)0.0236 (9)0.0342 (11)0.0033 (8)0.0060 (9)0.0016 (8)
S280.0402 (3)0.0279 (3)0.0460 (3)0.0122 (2)0.0001 (2)0.0018 (2)
C290.0387 (12)0.0391 (12)0.0336 (11)0.0105 (10)0.0036 (9)0.0036 (10)
C2100.0294 (10)0.0343 (11)0.0294 (10)0.0036 (8)0.0047 (8)0.0006 (9)
C2110.0264 (10)0.0218 (9)0.0288 (10)0.0024 (8)0.0034 (8)0.0016 (8)
C2120.0279 (10)0.0257 (10)0.0280 (10)0.0018 (8)0.0049 (8)0.0063 (8)
C2130.0359 (11)0.0400 (12)0.0277 (10)0.0054 (10)0.0060 (9)0.0076 (9)
C2140.0573 (15)0.0616 (16)0.0282 (11)0.0189 (12)0.0152 (11)0.0072 (11)
C2150.0452 (14)0.087 (2)0.0476 (15)0.0241 (14)0.0260 (12)0.0161 (14)
C2160.0277 (12)0.0770 (18)0.0451 (14)0.0060 (11)0.0094 (10)0.0129 (13)
C2170.0317 (11)0.0435 (12)0.0333 (11)0.0028 (9)0.0066 (9)0.0048 (10)
Geometric parameters (Å, º) top
N1—C21.352 (2)N21—C221.352 (2)
N1—C61.461 (2)N21—C261.464 (2)
N1—C101.473 (2)N21—C2101.473 (2)
C2—O21.230 (2)C22—O221.226 (2)
C2—C31.508 (3)C22—C231.514 (2)
C3—N41.453 (2)C23—N241.452 (2)
C3—C111.551 (3)C23—C2111.560 (3)
C3—H30.9800C23—H230.9800
N4—C51.337 (2)N24—C251.336 (2)
N4—C41.461 (2)N24—C241.462 (2)
C4—H4A0.9600C24—H24A0.9600
C4—H4B0.9600C24—H24B0.9600
C4—H4C0.9600C24—H24C0.9600
C5—O51.231 (2)C25—O251.228 (2)
C5—C61.527 (2)C25—C261.517 (3)
C6—C71.527 (3)C26—C271.530 (3)
C6—H60.9800C26—H260.9800
C7—S81.7992 (18)C27—S281.793 (2)
C7—H7A0.9700C27—H27A0.9700
C7—H7B0.9700C27—H27B0.9700
S8—C91.804 (2)S28—C291.803 (2)
C9—C101.506 (3)C29—C2101.508 (3)
C9—H9A0.9700C29—H29A0.9700
C9—H9B0.9700C29—H29B0.9700
C10—H10A0.9700C210—H21A0.9700
C10—H10B0.9700C210—H21B0.9700
C11—C121.505 (3)C211—C2121.507 (3)
C11—H11A0.9700C211—H21C0.9700
C11—H11B0.9700C211—H21D0.9700
C12—C171.392 (3)C212—C2131.393 (3)
C12—C131.395 (3)C212—C2171.394 (3)
C13—C141.382 (3)C213—C2141.388 (3)
C13—H130.9300C213—H2130.9300
C14—C151.380 (3)C214—C2151.385 (4)
C14—H140.9300C214—H2140.9300
C15—C161.382 (3)C215—C2161.374 (4)
C15—H150.9300C215—H2150.9300
C16—C171.387 (3)C216—C2171.376 (3)
C16—H160.9300C216—H2160.9300
C17—H170.9300C217—H2170.9300
C2—N1—C6122.88 (15)C22—N21—C26123.69 (15)
C2—N1—C10117.02 (15)C22—N21—C210117.69 (15)
C6—N1—C10116.93 (14)C26—N21—C210116.17 (15)
O2—C2—N1123.08 (17)O22—C22—N21123.71 (16)
O2—C2—C3118.27 (16)O22—C22—C23118.54 (16)
N1—C2—C3118.64 (15)N21—C22—C23117.69 (15)
N4—C3—C2114.44 (15)N24—C23—C22113.92 (15)
N4—C3—C11111.56 (15)N24—C23—C211111.94 (14)
C2—C3—C11108.08 (15)C22—C23—C211108.65 (15)
N4—C3—H3107.5N24—C23—H23107.3
C2—C3—H3107.5C22—C23—H23107.3
C11—C3—H3107.5C211—C23—H23107.3
C5—N4—C3122.92 (14)C25—N24—C23122.44 (15)
C5—N4—C4119.24 (16)C25—N24—C24119.01 (16)
C3—N4—C4116.72 (15)C23—N24—C24117.49 (15)
N4—C4—H4A109.5N24—C24—H24A109.5
N4—C4—H4B109.5N24—C24—H24B109.5
H4A—C4—H4B109.5H24A—C24—H24B109.5
N4—C4—H4C109.5N24—C24—H24C109.5
H4A—C4—H4C109.5H24A—C24—H24C109.5
H4B—C4—H4C109.5H24B—C24—H24C109.5
O5—C5—N4123.45 (17)O25—C25—N24122.42 (18)
O5—C5—C6118.22 (16)O25—C25—C26118.71 (17)
N4—C5—C6118.23 (15)N24—C25—C26118.77 (16)
N1—C6—C5114.69 (14)N21—C26—C25114.41 (15)
N1—C6—C7110.59 (15)N21—C26—C27110.71 (15)
C5—C6—C7106.56 (14)C25—C26—C27105.71 (15)
N1—C6—H6108.3N21—C26—H26108.6
C5—C6—H6108.3C25—C26—H26108.6
C7—C6—H6108.3C27—C26—H26108.6
C6—C7—S8113.37 (13)C26—C27—S28114.37 (14)
C6—C7—H7A108.9C26—C27—H27A108.7
S8—C7—H7A108.9S28—C27—H27A108.7
C6—C7—H7B108.9C26—C27—H27B108.7
S8—C7—H7B108.9S28—C27—H27B108.7
H7A—C7—H7B107.7H27A—C27—H27B107.6
C7—S8—C996.30 (9)C27—S28—C2997.35 (9)
C10—C9—S8111.52 (14)C210—C29—S28111.83 (15)
C10—C9—H9A109.3C210—C29—H29A109.3
S8—C9—H9A109.3S28—C29—H29A109.3
C10—C9—H9B109.3C210—C29—H29B109.3
S8—C9—H9B109.3S28—C29—H29B109.3
H9A—C9—H9B108.0H29A—C29—H29B107.9
N1—C10—C9113.06 (16)N21—C210—C29112.23 (17)
N1—C10—H10A109.0N21—C210—H21A109.2
C9—C10—H10A109.0C29—C210—H21A109.2
N1—C10—H10B109.0N21—C210—H21B109.2
C9—C10—H10B109.0C29—C210—H21B109.2
H10A—C10—H10B107.8H21A—C210—H21B107.9
C12—C11—C3113.59 (15)C212—C211—C23112.29 (15)
C12—C11—H11A108.8C212—C211—H21C109.1
C3—C11—H11A108.8C23—C211—H21C109.1
C12—C11—H11B108.8C212—C211—H21D109.1
C3—C11—H11B108.8C23—C211—H21D109.1
H11A—C11—H11B107.7H21C—C211—H21D107.9
C17—C12—C13117.87 (18)C213—C212—C217118.12 (19)
C17—C12—C11120.65 (18)C213—C212—C211121.54 (17)
C13—C12—C11121.48 (17)C217—C212—C211120.24 (18)
C14—C13—C12121.23 (18)C214—C213—C212120.4 (2)
C14—C13—H13119.4C214—C213—H213119.8
C12—C13—H13119.4C212—C213—H213119.8
C15—C14—C13120.08 (19)C215—C214—C213120.2 (2)
C15—C14—H14120.0C215—C214—H214119.9
C13—C14—H14120.0C213—C214—H214119.9
C14—C15—C16119.70 (19)C216—C215—C214119.8 (2)
C14—C15—H15120.2C216—C215—H215120.1
C16—C15—H15120.2C214—C215—H215120.1
C15—C16—C17120.14 (18)C215—C216—C217120.1 (2)
C15—C16—H16119.9C215—C216—H216120.0
C17—C16—H16119.9C217—C216—H216120.0
C16—C17—C12120.96 (18)C216—C217—C212121.3 (2)
C16—C17—H17119.5C216—C217—H217119.3
C12—C17—H17119.5C212—C217—H217119.3
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3···O22i0.982.593.457 (2)148
C3—H3···O5ii0.982.503.024 (2)114
C9—H9B···O22iii0.972.443.370 (2)160
C10—H10B···S28iv0.972.793.733 (2)166
C15—H15···O2v0.932.583.252 (2)130
C211—H21C···O25vi0.972.563.511 (2)166
C23—H23···O2v0.982.543.511 (2)171
C24—H24A···O25vi0.962.353.164 (3)142
C14—H14···O5vii0.932.513.377 (2)156
Symmetry codes: (i) x, y1, z; (ii) x+1, y1/2, z+1; (iii) x1, y1, z; (iv) x1, y, z; (v) x, y+1, z; (vi) x+1, y+1/2, z; (vii) x+1, y+1/2, z+1.
(8a) top
Crystal data top
C15H18N2O2SZ = 2
Mr = 290.37F(000) = 308
Triclinic, P1Dx = 1.387 Mg m3
a = 7.4536 (1) ÅMo Kα radiation, λ = 0.7107 Å
b = 7.4603 (2) ÅCell parameters from 11838 reflections
c = 13.6011 (3) Åθ = 1–27.5°
α = 79.6877 (12)°µ = 0.24 mm1
β = 89.2981 (14)°T = 150 K
γ = 69.3688 (12)°Plate, colourless
V = 695.31 (3) Å30.45 × 0.32 × 0.2 mm
Data collection top
Nonius KappaCCD area detector
diffractometer
Rint = 0.031
Radiation source: fine-focus sealed tubeθmax = 27.4°, θmin = 3.0°
φ and ω scans to fill the Ewald sphereh = 99
17028 measured reflectionsk = 99
6242 independent reflectionsl = 1717
6027 reflections with I > 2σ(I)
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.029 w = 1/[σ2(Fo2) + (0.0468P)2 + 0.0971P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.079(Δ/σ)max < 0.001
S = 1.04Δρmax = 0.22 e Å3
6242 reflectionsΔρmin = 0.20 e Å3
363 parametersAbsolute structure: Flack x determined using 2865 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259).
3 restraintsAbsolute structure parameter: 0.022 (19)
Secondary atom site location: difference Fourier map
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
N10.1876 (3)0.2874 (3)0.04004 (13)0.0175 (4)
C20.2259 (3)0.1522 (3)0.01870 (15)0.0182 (4)
O20.1243 (2)0.0558 (3)0.02513 (13)0.0280 (4)
C30.3987 (3)0.1223 (3)0.08201 (16)0.0171 (4)
H30.35180.13680.15100.020*
N40.4902 (3)0.2669 (3)0.08300 (14)0.0178 (4)
C40.6324 (3)0.2706 (4)0.15787 (18)0.0243 (5)
H4A0.63400.40040.17580.037*
H4B0.59920.23070.21630.037*
H4C0.75710.18300.13060.037*
C50.4782 (3)0.3689 (3)0.00977 (17)0.0190 (4)
O50.5825 (3)0.4630 (2)0.00267 (14)0.0290 (4)
C60.3232 (3)0.3770 (3)0.06461 (16)0.0182 (4)
H60.24820.51540.06210.022*
C70.4106 (3)0.2946 (3)0.17251 (17)0.0217 (4)
H7A0.48600.15710.17850.026*
H7B0.49610.36040.18660.026*
C80.2572 (4)0.3202 (4)0.24932 (19)0.0263 (5)
H8A0.18590.45820.24550.032*
H8B0.31900.26810.31590.032*
S90.09101 (7)0.19901 (8)0.23000 (4)0.02701 (15)
C100.0216 (3)0.3201 (4)0.10145 (17)0.0228 (5)
H10A0.06860.27160.07470.027*
H10B0.04210.45890.09900.027*
C110.5430 (3)0.0889 (3)0.05250 (17)0.0205 (4)
H11A0.47700.17810.05810.025*
H11B0.64350.10950.09970.025*
C120.6340 (3)0.1376 (3)0.05179 (17)0.0195 (4)
C130.5541 (3)0.2198 (3)0.13250 (18)0.0222 (5)
H130.44240.24420.12200.027*
C140.6392 (4)0.2661 (4)0.22882 (19)0.0276 (5)
H140.58500.32230.28190.033*
C150.8044 (4)0.2287 (3)0.24563 (19)0.0284 (5)
H150.86120.25890.30990.034*
C160.8843 (4)0.1455 (4)0.1655 (2)0.0282 (5)
H160.99490.11950.17640.034*
C170.8008 (3)0.1011 (3)0.06986 (19)0.0240 (5)
H170.85640.04620.01690.029*
N210.1328 (3)0.1550 (3)0.35899 (13)0.0182 (4)
C220.0295 (3)0.0907 (3)0.30047 (16)0.0184 (4)
O220.1282 (3)0.1905 (2)0.29408 (13)0.0279 (4)
C230.0905 (3)0.1113 (3)0.23659 (16)0.0172 (4)
H230.10880.09620.16770.021*
N240.0528 (3)0.2046 (3)0.23505 (14)0.0179 (4)
C240.0188 (3)0.3823 (3)0.16022 (18)0.0241 (5)
H24A0.13960.39390.14180.036*
H24B0.04880.37600.10210.036*
H24C0.05650.49350.18770.036*
C250.1903 (3)0.1596 (3)0.30785 (17)0.0196 (4)
O250.2873 (2)0.2605 (3)0.31402 (14)0.0292 (4)
C260.2338 (3)0.0303 (3)0.38275 (16)0.0186 (4)
H260.37110.10380.38030.022*
C270.2020 (3)0.0090 (3)0.49018 (16)0.0211 (4)
H27A0.06710.08190.49590.025*
H27B0.27440.08840.50350.025*
C280.2637 (4)0.1794 (4)0.56857 (18)0.0259 (5)
H28A0.40020.24870.56540.031*
H28B0.24160.14690.63470.031*
S290.13449 (8)0.33726 (8)0.55012 (4)0.02691 (14)
C2100.1954 (3)0.3488 (3)0.42137 (17)0.0235 (5)
H21A0.13500.42770.39530.028*
H21B0.33330.41070.41890.028*
C2110.2882 (3)0.2410 (3)0.26655 (17)0.0218 (4)
H21C0.38070.17890.25970.026*
H21D0.33040.36510.22040.026*
C2120.2875 (3)0.2782 (3)0.37139 (17)0.0192 (4)
C2130.2435 (3)0.4345 (3)0.39265 (19)0.0251 (5)
H2130.21660.51930.34080.030*
C2140.2394 (4)0.4652 (4)0.4906 (2)0.0315 (6)
H2140.20850.56920.50380.038*
C2150.2811 (4)0.3415 (4)0.56785 (19)0.0312 (6)
H2150.27940.36270.63310.037*
C2160.3258 (4)0.1852 (4)0.54826 (19)0.0276 (5)
H2160.35390.10150.60030.033*
C2170.3283 (3)0.1546 (3)0.45085 (18)0.0221 (5)
H2170.35770.04930.43820.027*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0174 (9)0.0208 (9)0.0150 (9)0.0072 (7)0.0008 (7)0.0048 (7)
C20.0182 (10)0.0206 (10)0.0157 (10)0.0067 (8)0.0000 (8)0.0033 (8)
O20.0271 (9)0.0370 (9)0.0298 (9)0.0196 (8)0.0068 (7)0.0150 (8)
C30.0198 (11)0.0187 (10)0.0158 (10)0.0093 (8)0.0014 (8)0.0057 (8)
N40.0179 (9)0.0179 (8)0.0179 (9)0.0076 (7)0.0036 (7)0.0015 (7)
C40.0226 (11)0.0240 (11)0.0234 (12)0.0067 (9)0.0073 (9)0.0007 (9)
C50.0177 (10)0.0145 (9)0.0225 (11)0.0037 (8)0.0010 (8)0.0018 (8)
O50.0310 (9)0.0252 (9)0.0382 (10)0.0175 (7)0.0042 (7)0.0089 (7)
C60.0194 (10)0.0153 (9)0.0197 (10)0.0052 (8)0.0011 (8)0.0052 (8)
C70.0241 (11)0.0199 (10)0.0208 (11)0.0068 (9)0.0040 (9)0.0053 (8)
C80.0322 (13)0.0273 (12)0.0193 (11)0.0086 (10)0.0014 (9)0.0081 (9)
S90.0292 (3)0.0359 (3)0.0174 (3)0.0132 (3)0.0048 (2)0.0058 (2)
C100.0182 (10)0.0284 (12)0.0210 (11)0.0057 (9)0.0030 (8)0.0079 (9)
C110.0252 (11)0.0169 (10)0.0208 (11)0.0076 (9)0.0042 (9)0.0067 (8)
C120.0202 (11)0.0121 (9)0.0246 (11)0.0031 (8)0.0032 (9)0.0050 (8)
C130.0214 (11)0.0189 (11)0.0268 (12)0.0074 (9)0.0031 (9)0.0051 (9)
C140.0316 (14)0.0224 (12)0.0236 (12)0.0052 (10)0.0049 (10)0.0005 (9)
C150.0328 (13)0.0216 (11)0.0238 (12)0.0022 (10)0.0075 (10)0.0014 (9)
C160.0230 (11)0.0225 (11)0.0381 (14)0.0078 (9)0.0051 (10)0.0035 (10)
C170.0216 (11)0.0183 (11)0.0305 (13)0.0075 (9)0.0020 (9)0.0001 (9)
N210.0202 (9)0.0165 (8)0.0165 (9)0.0055 (7)0.0004 (7)0.0016 (7)
C220.0215 (10)0.0181 (10)0.0159 (10)0.0072 (8)0.0018 (8)0.0041 (8)
O220.0336 (9)0.0248 (8)0.0297 (9)0.0173 (7)0.0056 (7)0.0013 (7)
C230.0176 (10)0.0195 (10)0.0142 (10)0.0071 (8)0.0017 (7)0.0014 (8)
N240.0186 (9)0.0168 (8)0.0176 (9)0.0070 (7)0.0010 (7)0.0005 (7)
C240.0253 (11)0.0195 (10)0.0232 (11)0.0059 (9)0.0028 (9)0.0026 (9)
C250.0150 (10)0.0216 (10)0.0218 (11)0.0054 (8)0.0037 (8)0.0060 (9)
O250.0230 (8)0.0317 (9)0.0371 (10)0.0162 (7)0.0000 (7)0.0036 (8)
C260.0135 (10)0.0225 (11)0.0190 (10)0.0052 (8)0.0004 (8)0.0039 (8)
C270.0184 (10)0.0263 (11)0.0192 (11)0.0074 (9)0.0000 (8)0.0069 (9)
C280.0243 (12)0.0345 (13)0.0162 (11)0.0078 (10)0.0013 (9)0.0034 (9)
S290.0321 (3)0.0273 (3)0.0182 (3)0.0099 (2)0.0001 (2)0.0021 (2)
C2100.0276 (12)0.0177 (10)0.0213 (11)0.0045 (9)0.0008 (9)0.0012 (9)
C2110.0167 (10)0.0238 (11)0.0219 (11)0.0053 (9)0.0025 (8)0.0003 (9)
C2120.0119 (10)0.0214 (10)0.0215 (11)0.0027 (8)0.0006 (8)0.0038 (9)
C2130.0197 (11)0.0207 (11)0.0344 (13)0.0058 (9)0.0066 (9)0.0070 (10)
C2140.0231 (12)0.0312 (13)0.0453 (15)0.0097 (10)0.0061 (11)0.0206 (12)
C2150.0240 (12)0.0431 (15)0.0291 (13)0.0098 (11)0.0039 (10)0.0182 (11)
C2160.0237 (13)0.0344 (14)0.0240 (12)0.0095 (10)0.0038 (10)0.0051 (11)
C2170.0183 (11)0.0230 (11)0.0258 (11)0.0080 (9)0.0008 (8)0.0049 (9)
Geometric parameters (Å, º) top
N1—C21.348 (3)N21—C221.343 (3)
N1—C101.457 (3)N21—C2101.457 (3)
N1—C61.464 (3)N21—C261.464 (3)
C2—O21.228 (3)C22—O221.231 (3)
C2—C31.513 (3)C22—C231.514 (3)
C3—N41.463 (3)C23—N241.464 (3)
C3—C111.546 (3)C23—C2111.548 (3)
C3—H30.9800C23—H230.9800
N4—C51.342 (3)N24—C251.344 (3)
N4—C41.464 (3)N24—C241.464 (3)
C4—H4A0.9600C24—H24A0.9600
C4—H4B0.9600C24—H24B0.9600
C4—H4C0.9600C24—H24C0.9600
C5—O51.232 (3)C25—O251.227 (3)
C5—C61.519 (3)C25—C261.522 (3)
C6—C71.541 (3)C26—C271.540 (3)
C6—H60.9800C26—H260.9800
C7—C81.524 (3)C27—C281.531 (3)
C7—H7A0.9700C27—H27A0.9700
C7—H7B0.9700C27—H27B0.9700
C8—S91.817 (3)C28—S291.814 (3)
C8—H8A0.9700C28—H28A0.9700
C8—H8B0.9700C28—H28B0.9700
S9—C101.808 (2)S29—C2101.813 (2)
C10—H10A0.9700C210—H21A0.9700
C10—H10B0.9700C210—H21B0.9700
C11—C121.507 (3)C211—C2121.501 (3)
C11—H11A0.9700C211—H21C0.9700
C11—H11B0.9700C211—H21D0.9700
C12—C131.392 (3)C212—C2131.393 (3)
C12—C171.397 (3)C212—C2171.395 (3)
C13—C141.394 (4)C213—C2141.394 (4)
C13—H130.9300C213—H2130.9300
C14—C151.385 (4)C214—C2151.378 (4)
C14—H140.9300C214—H2140.9300
C15—C161.389 (4)C215—C2161.388 (4)
C15—H150.9300C215—H2150.9300
C16—C171.382 (4)C216—C2171.386 (4)
C16—H160.9300C216—H2160.9300
C17—H170.9300C217—H2170.9300
C2—N1—C10119.68 (18)C22—N21—C210119.92 (18)
C2—N1—C6124.19 (18)C22—N21—C26124.30 (17)
C10—N1—C6114.75 (18)C210—N21—C26114.44 (18)
O2—C2—N1123.0 (2)O22—C22—N21123.10 (19)
O2—C2—C3118.52 (19)O22—C22—C23118.28 (19)
N1—C2—C3118.44 (18)N21—C22—C23118.58 (18)
N4—C3—C2114.36 (17)N24—C23—C22114.30 (17)
N4—C3—C11112.27 (17)N24—C23—C211112.13 (18)
C2—C3—C11110.31 (17)C22—C23—C211110.22 (18)
N4—C3—H3106.4N24—C23—H23106.6
C2—C3—H3106.4C22—C23—H23106.6
C11—C3—H3106.4C211—C23—H23106.6
C5—N4—C3123.86 (18)C25—N24—C24117.99 (18)
C5—N4—C4118.07 (19)C25—N24—C23124.06 (18)
C3—N4—C4116.92 (18)C24—N24—C23116.76 (17)
N4—C4—H4A109.5N24—C24—H24A109.5
N4—C4—H4B109.5N24—C24—H24B109.5
H4A—C4—H4B109.5H24A—C24—H24B109.5
N4—C4—H4C109.5N24—C24—H24C109.5
H4A—C4—H4C109.5H24A—C24—H24C109.5
H4B—C4—H4C109.5H24B—C24—H24C109.5
O5—C5—N4122.8 (2)O25—C25—N24122.9 (2)
O5—C5—C6118.5 (2)O25—C25—C26118.7 (2)
N4—C5—C6118.68 (19)N24—C25—C26118.34 (19)
N1—C6—C5114.10 (18)N21—C26—C25114.26 (18)
N1—C6—C7111.66 (18)N21—C26—C27111.84 (17)
C5—C6—C7111.32 (18)C25—C26—C27110.85 (18)
N1—C6—H6106.4N21—C26—H26106.4
C5—C6—H6106.4C25—C26—H26106.4
C7—C6—H6106.4C27—C26—H26106.4
C8—C7—C6112.16 (19)C28—C27—C26112.33 (19)
C8—C7—H7A109.2C28—C27—H27A109.1
C6—C7—H7A109.2C26—C27—H27A109.1
C8—C7—H7B109.2C28—C27—H27B109.1
C6—C7—H7B109.2C26—C27—H27B109.1
H7A—C7—H7B107.9H27A—C27—H27B107.9
C7—C8—S9112.48 (16)C27—C28—S29112.34 (16)
C7—C8—H8A109.1C27—C28—H28A109.1
S9—C8—H8A109.1S29—C28—H28A109.1
C7—C8—H8B109.1C27—C28—H28B109.1
S9—C8—H8B109.1S29—C28—H28B109.1
H8A—C8—H8B107.8H28A—C28—H28B107.9
C10—S9—C895.64 (11)C210—S29—C2895.87 (11)
N1—C10—S9111.34 (15)N21—C210—S29111.30 (15)
N1—C10—H10A109.4N21—C210—H21A109.4
S9—C10—H10A109.4S29—C210—H21A109.4
N1—C10—H10B109.4N21—C210—H21B109.4
S9—C10—H10B109.4S29—C210—H21B109.4
H10A—C10—H10B108.0H21A—C210—H21B108.0
C12—C11—C3114.16 (17)C212—C211—C23113.88 (17)
C12—C11—H11A108.7C212—C211—H21C108.8
C3—C11—H11A108.7C23—C211—H21C108.8
C12—C11—H11B108.7C212—C211—H21D108.8
C3—C11—H11B108.7C23—C211—H21D108.8
H11A—C11—H11B107.6H21C—C211—H21D107.7
C13—C12—C17118.3 (2)C213—C212—C217118.0 (2)
C13—C12—C11120.9 (2)C213—C212—C211121.4 (2)
C17—C12—C11120.8 (2)C217—C212—C211120.6 (2)
C12—C13—C14120.8 (2)C212—C213—C214120.9 (2)
C12—C13—H13119.6C212—C213—H213119.6
C14—C13—H13119.6C214—C213—H213119.6
C15—C14—C13120.2 (2)C215—C214—C213120.0 (2)
C15—C14—H14119.9C215—C214—H214120.0
C13—C14—H14119.9C213—C214—H214120.0
C14—C15—C16119.3 (2)C214—C215—C216120.0 (2)
C14—C15—H15120.3C214—C215—H215120.0
C16—C15—H15120.3C216—C215—H215120.0
C17—C16—C15120.5 (2)C217—C216—C215119.7 (2)
C17—C16—H16119.7C217—C216—H216120.1
C15—C16—H16119.7C215—C216—H216120.1
C16—C17—C12120.8 (2)C216—C217—C212121.3 (2)
C16—C17—H17119.6C216—C217—H217119.3
C12—C17—H17119.6C212—C217—H217119.3
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3···O220.982.463.397 (3)160
C11—H11A···O5i0.972.483.197 (3)130
C17—H17···O2ii0.932.403.197 (3)143
C211—H21C···O25ii0.972.473.179 (3)130
C23—H23···O20.982.443.378 (3)161
C213—H213···O22i0.932.453.269 (3)146
Symmetry codes: (i) x, y1, z; (ii) x+1, y, z.
(8b) top
Crystal data top
C15H18N2O2SF(000) = 616
Mr = 290.37Dx = 1.341 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71070 Å
Hall symbol: P 2ac 2abCell parameters from 14664 reflections
a = 9.8689 (2) Åθ = 1–27.5°
b = 10.6838 (2) ŵ = 0.23 mm1
c = 13.6421 (2) ÅT = 150 K
V = 1438.39 (4) Å3Prism, colourles
Z = 40.4 × 0.25 × 0.25 mm
Data collection top
Nonius KappaCCD area detector
diffractometer
3045 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.035
Graphite monochromatorθmax = 27.5°, θmin = 2.8°
Detector resolution: 9.091 pixels mm-1h = 012
φ and ω scans to fill the Ewald spherek = 013
25952 measured reflectionsl = 1717
3291 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.031 w = 1/[σ2(Fo2) + (0.0369P)2 + 0.3211P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.077(Δ/σ)max < 0.001
S = 1.06Δρmax = 0.20 e Å3
3291 reflectionsΔρmin = 0.18 e Å3
183 parametersExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.044 (2)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Secondary atom site location: difference Fourier mapAbsolute structure parameter: 0.01 (7)
Special details top

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 (Å2) top
xyzUiso*/Ueq
N10.28236 (13)0.78426 (11)0.10568 (8)0.0256 (3)
C20.21533 (15)0.88543 (13)0.13948 (11)0.0260 (3)
C30.13535 (14)0.87245 (12)0.23322 (10)0.0247 (3)
H30.05100.91980.22520.030*
N40.09891 (11)0.74383 (11)0.25736 (9)0.0230 (3)
C40.00986 (16)0.72775 (15)0.32923 (11)0.0325 (3)
H4A0.05880.65220.31510.049*
H4B0.07050.79790.32590.049*
H4C0.02840.72260.39380.049*
C50.16656 (13)0.64327 (13)0.22624 (10)0.0215 (3)
C60.27321 (14)0.65846 (13)0.14681 (10)0.0225 (3)
H60.36140.63790.17560.027*
C70.24381 (16)0.56212 (14)0.06594 (11)0.0295 (3)
H7A0.24030.47940.09510.035*
H7B0.15540.57960.03810.035*
C80.3480 (2)0.56163 (17)0.01575 (12)0.0403 (4)
H8A0.32570.49640.06250.048*
H8B0.43660.54310.01140.048*
S90.35366 (5)0.71083 (4)0.07809 (3)0.04405 (14)
C100.38512 (16)0.80154 (17)0.03036 (11)0.0352 (4)
H10A0.47280.77840.05700.042*
H10B0.38890.88940.01270.042*
C110.21673 (16)0.93424 (15)0.31800 (12)0.0300 (3)
H11A0.23381.02130.30210.036*
H11B0.16310.93180.37760.036*
C120.34986 (16)0.86860 (13)0.33545 (10)0.0267 (3)
C130.46417 (15)0.90170 (15)0.28157 (12)0.0319 (3)
H130.46050.97020.23960.038*
C140.58348 (16)0.83375 (16)0.28969 (14)0.0377 (4)
H140.65920.85710.25350.045*
C150.58988 (17)0.73134 (16)0.35165 (13)0.0383 (4)
H150.66930.68500.35650.046*
C160.47739 (18)0.69845 (16)0.40622 (12)0.0377 (4)
H160.48140.63000.44830.045*
C170.35842 (17)0.76714 (15)0.39854 (11)0.0322 (3)
H170.28360.74480.43610.039*
O20.22419 (12)0.98925 (10)0.10066 (9)0.0373 (3)
O50.14323 (11)0.53662 (9)0.25671 (8)0.0301 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0293 (6)0.0238 (6)0.0236 (6)0.0026 (5)0.0033 (5)0.0010 (5)
C20.0270 (7)0.0232 (7)0.0278 (7)0.0025 (6)0.0062 (6)0.0008 (6)
C30.0235 (6)0.0196 (6)0.0311 (7)0.0022 (6)0.0011 (6)0.0018 (5)
N40.0210 (5)0.0230 (6)0.0250 (6)0.0004 (4)0.0015 (5)0.0008 (5)
C40.0292 (7)0.0359 (8)0.0325 (8)0.0002 (7)0.0092 (6)0.0026 (7)
C50.0203 (6)0.0231 (7)0.0211 (6)0.0009 (5)0.0020 (5)0.0012 (5)
C60.0221 (6)0.0241 (7)0.0214 (6)0.0012 (5)0.0001 (5)0.0000 (5)
C70.0369 (8)0.0261 (7)0.0256 (7)0.0009 (6)0.0010 (6)0.0027 (6)
C80.0528 (10)0.0406 (9)0.0275 (7)0.0073 (9)0.0095 (8)0.0070 (7)
S90.0579 (3)0.0510 (3)0.02326 (19)0.0009 (2)0.01065 (19)0.00207 (18)
C100.0364 (8)0.0381 (9)0.0312 (8)0.0074 (7)0.0091 (6)0.0032 (7)
C110.0313 (8)0.0267 (7)0.0319 (8)0.0021 (6)0.0021 (6)0.0070 (6)
C120.0301 (7)0.0249 (7)0.0251 (7)0.0012 (6)0.0053 (6)0.0075 (5)
C130.0317 (8)0.0293 (8)0.0348 (8)0.0066 (6)0.0059 (7)0.0003 (6)
C140.0272 (7)0.0418 (10)0.0441 (9)0.0059 (7)0.0016 (7)0.0068 (8)
C150.0314 (8)0.0355 (9)0.0478 (10)0.0062 (7)0.0110 (7)0.0115 (7)
C160.0454 (9)0.0318 (8)0.0360 (9)0.0030 (7)0.0128 (7)0.0017 (7)
C170.0354 (8)0.0360 (8)0.0251 (7)0.0035 (7)0.0024 (6)0.0009 (6)
O20.0445 (6)0.0241 (5)0.0432 (7)0.0029 (5)0.0011 (5)0.0079 (5)
O50.0345 (5)0.0227 (5)0.0332 (5)0.0008 (4)0.0069 (5)0.0038 (4)
Geometric parameters (Å, º) top
N1—C21.3486 (19)C8—S91.8076 (18)
N1—C101.4554 (18)C8—H8A0.9700
N1—C61.4593 (18)C8—H8B0.9700
C2—O21.2322 (18)S9—C101.7956 (18)
C2—C31.509 (2)C10—H10A0.9700
C3—N41.4581 (18)C10—H10B0.9700
C3—C111.555 (2)C11—C121.508 (2)
C3—H30.9800C11—H11A0.9700
N4—C51.3342 (18)C11—H11B0.9700
N4—C41.4638 (18)C12—C171.387 (2)
C4—H4A0.9600C12—C131.392 (2)
C4—H4B0.9600C13—C141.388 (2)
C4—H4C0.9600C13—H130.9300
C5—O51.2346 (17)C14—C151.384 (3)
C5—C61.5193 (19)C14—H140.9300
C6—C71.5365 (19)C15—C161.382 (3)
C6—H60.9800C15—H150.9300
C7—C81.516 (2)C16—C171.388 (2)
C7—H7A0.9700C16—H160.9300
C7—H7B0.9700C17—H170.9300
C2—N1—C10118.79 (13)C7—C8—H8A109.4
C2—N1—C6125.19 (12)S9—C8—H8A109.4
C10—N1—C6115.56 (12)C7—C8—H8B109.4
O2—C2—N1122.66 (14)S9—C8—H8B109.4
O2—C2—C3118.95 (13)H8A—C8—H8B108.0
N1—C2—C3118.21 (12)C10—S9—C895.38 (8)
N4—C3—C2114.02 (11)N1—C10—S9113.12 (11)
N4—C3—C11111.06 (12)N1—C10—H10A109.0
C2—C3—C11108.72 (12)S9—C10—H10A109.0
N4—C3—H3107.6N1—C10—H10B109.0
C2—C3—H3107.6S9—C10—H10B109.0
C11—C3—H3107.6H10A—C10—H10B107.8
C5—N4—C3124.30 (11)C12—C11—C3111.71 (12)
C5—N4—C4119.05 (12)C12—C11—H11A109.3
C3—N4—C4116.28 (11)C3—C11—H11A109.3
N4—C4—H4A109.5C12—C11—H11B109.3
N4—C4—H4B109.5C3—C11—H11B109.3
H4A—C4—H4B109.5H11A—C11—H11B107.9
N4—C4—H4C109.5C17—C12—C13118.48 (14)
H4A—C4—H4C109.5C17—C12—C11120.97 (14)
H4B—C4—H4C109.5C13—C12—C11120.29 (13)
O5—C5—N4122.86 (12)C14—C13—C12120.83 (15)
O5—C5—C6117.90 (12)C14—C13—H13119.6
N4—C5—C6119.19 (12)C12—C13—H13119.6
N1—C6—C5114.55 (11)C15—C14—C13120.07 (16)
N1—C6—C7110.64 (11)C15—C14—H14120.0
C5—C6—C7108.04 (11)C13—C14—H14120.0
N1—C6—H6107.8C16—C15—C14119.56 (15)
C5—C6—H6107.8C16—C15—H15120.2
C7—C6—H6107.8C14—C15—H15120.2
C8—C7—C6113.71 (13)C15—C16—C17120.28 (15)
C8—C7—H7A108.8C15—C16—H16119.9
C6—C7—H7A108.8C17—C16—H16119.9
C8—C7—H7B108.8C12—C17—C16120.76 (15)
C6—C7—H7B108.8C12—C17—H17119.6
H7A—C7—H7B107.7C16—C17—H17119.6
C7—C8—S9111.33 (11)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3···O5i0.982.303.2641 (17)167
C8—H8A···O5ii0.972.513.2779 (19)136
C15—H15···O2iii0.932.413.237 (2)148
Symmetry codes: (i) x, y+1/2, z+1/2; (ii) x+1/2, y+1, z1/2; (iii) x+1, y1/2, z+1/2.
(12a) top
Crystal data top
C14H16N2O2SDx = 1.407 Mg m3
Mr = 276.35Mo Kα radiation, λ = 0.71073 Å
Tetragonal, P43212Cell parameters from 6416 reflections
Hall symbol: P 4nw 2abwθ = 3.2–27.5°
a = 7.7430 (2) ŵ = 0.25 mm1
c = 43.5343 (14) ÅT = 150 K
V = 2610.06 (13) Å3Bar, colourless
Z = 80.46 × 0.18 × 0.18 mm
F(000) = 1168
Data collection top
Bruker APEX-II CCD
diffractometer
2992 independent reflections
Radiation source: fine-focus sealed tube2800 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.026
φ and ω scansθmax = 27.5°, θmin = 1.9°
Absorption correction: multi-scan
SADABS-2014/5 - Bruker AXS area detector scaling and absorption correction
h = 710
Tmin = 0.894, Tmax = 0.957k = 810
15598 measured reflectionsl = 5256
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.030H-atom parameters constrained
wR(F2) = 0.075 w = 1/[σ2(Fo2) + (0.0398P)2 + 0.4448P]
where P = (Fo2 + 2Fc2)/3
S = 1.11(Δ/σ)max = 0.001
2992 reflectionsΔρmax = 0.21 e Å3
173 parametersΔρmin = 0.21 e Å3
0 restraintsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.06 (7)
Special details top

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 (Å2) top
xyzUiso*/Ueq
N10.38721 (17)0.01940 (16)0.73082 (3)0.0197 (3)
C20.4236 (2)0.14453 (19)0.72231 (3)0.0182 (3)
C30.28391 (19)0.24774 (18)0.70624 (3)0.0174 (3)
H30.26940.35760.71800.021*
N40.11398 (16)0.16492 (16)0.70493 (3)0.0180 (3)
C50.0860 (2)0.0049 (2)0.70881 (3)0.0204 (3)
C60.2319 (2)0.11047 (18)0.72197 (3)0.0197 (3)
H60.18690.17110.74060.024*
S70.30515 (6)0.27642 (5)0.694748 (9)0.02662 (11)
C80.5216 (2)0.2738 (3)0.71089 (4)0.0377 (5)
H8A0.60630.23950.69500.045*
H8B0.55280.39020.71850.045*
C90.5242 (2)0.1450 (2)0.73721 (4)0.0280 (4)
H9A0.63780.08660.73830.034*
H9B0.50240.20420.75700.034*
C100.0291 (2)0.2728 (2)0.69390 (4)0.0254 (3)
H10A0.13670.23640.70380.038*
H10B0.00590.39400.69890.038*
H10C0.04030.26000.67160.038*
C110.3505 (2)0.29767 (19)0.67383 (3)0.0197 (3)
H11A0.46020.36220.67610.024*
H11B0.26570.37640.66420.024*
C120.3810 (2)0.14716 (19)0.65245 (3)0.0193 (3)
C130.2488 (2)0.08414 (19)0.63401 (3)0.0221 (3)
H130.13650.13280.63560.027*
C140.2785 (3)0.0489 (2)0.61329 (4)0.0303 (4)
H140.18690.09020.60080.036*
C150.4409 (3)0.1214 (2)0.61085 (4)0.0346 (4)
H150.46130.21210.59660.042*
C160.5740 (3)0.0614 (2)0.62924 (4)0.0330 (4)
H160.68570.11120.62760.040*
C170.5444 (2)0.0718 (2)0.65010 (4)0.0248 (3)
H170.63590.11170.66280.030*
O20.56338 (14)0.21299 (15)0.72714 (3)0.0270 (3)
O50.05266 (15)0.07533 (16)0.70351 (3)0.0334 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0219 (7)0.0169 (6)0.0202 (6)0.0028 (5)0.0043 (5)0.0001 (5)
C20.0226 (8)0.0182 (7)0.0138 (6)0.0008 (6)0.0007 (6)0.0038 (6)
C30.0201 (7)0.0143 (7)0.0178 (6)0.0005 (5)0.0002 (6)0.0015 (5)
N40.0159 (6)0.0198 (6)0.0183 (6)0.0018 (5)0.0002 (5)0.0011 (5)
C50.0210 (8)0.0209 (8)0.0193 (7)0.0013 (6)0.0016 (6)0.0028 (6)
C60.0248 (8)0.0142 (7)0.0201 (7)0.0009 (6)0.0008 (6)0.0005 (6)
S70.0361 (2)0.01715 (18)0.02665 (19)0.00488 (15)0.00655 (17)0.00451 (15)
C80.0351 (10)0.0368 (11)0.0412 (10)0.0176 (8)0.0097 (8)0.0117 (9)
C90.0296 (9)0.0260 (9)0.0284 (8)0.0107 (7)0.0083 (7)0.0002 (7)
C100.0214 (8)0.0286 (8)0.0262 (7)0.0088 (6)0.0001 (6)0.0020 (7)
C110.0252 (7)0.0146 (7)0.0192 (7)0.0006 (6)0.0013 (6)0.0019 (5)
C120.0255 (8)0.0146 (7)0.0177 (7)0.0002 (6)0.0047 (6)0.0043 (6)
C130.0290 (9)0.0186 (7)0.0188 (7)0.0004 (6)0.0006 (6)0.0038 (6)
C140.0498 (11)0.0219 (8)0.0192 (7)0.0069 (8)0.0002 (8)0.0005 (6)
C150.0596 (13)0.0173 (8)0.0269 (8)0.0008 (8)0.0183 (9)0.0006 (7)
C160.0376 (10)0.0218 (8)0.0396 (10)0.0082 (7)0.0199 (8)0.0075 (7)
C170.0236 (8)0.0210 (8)0.0297 (8)0.0011 (6)0.0064 (7)0.0048 (6)
O20.0228 (6)0.0277 (6)0.0306 (6)0.0039 (5)0.0069 (5)0.0024 (5)
O50.0213 (6)0.0290 (7)0.0499 (8)0.0056 (5)0.0027 (6)0.0018 (6)
Geometric parameters (Å, º) top
N1—C21.352 (2)C9—H9B0.9900
N1—C61.4464 (19)C10—H10A0.9800
N1—C91.4658 (19)C10—H10B0.9800
C2—O21.2236 (19)C10—H10C0.9800
C2—C31.516 (2)C11—C121.510 (2)
C3—N41.4648 (18)C11—H11A0.9900
C3—C111.5515 (19)C11—H11B0.9900
C3—H31.0000C12—C131.390 (2)
N4—C51.343 (2)C12—C171.397 (2)
N4—C101.4684 (19)C13—C141.389 (2)
C5—O51.2262 (19)C13—H130.9500
C5—C61.507 (2)C14—C151.381 (3)
C6—S71.8378 (15)C14—H140.9500
C6—H61.0000C15—C161.385 (3)
S7—C81.8178 (19)C15—H150.9500
C8—C91.519 (2)C16—C171.393 (2)
C8—H8A0.9900C16—H160.9500
C8—H8B0.9900C17—H170.9500
C9—H9A0.9900
C2—N1—C6123.92 (13)N1—C9—H9B110.4
C2—N1—C9121.61 (14)C8—C9—H9B110.4
C6—N1—C9109.21 (12)H9A—C9—H9B108.6
O2—C2—N1122.95 (14)N4—C10—H10A109.5
O2—C2—C3118.82 (14)N4—C10—H10B109.5
N1—C2—C3118.22 (13)H10A—C10—H10B109.5
N4—C3—C2115.34 (12)N4—C10—H10C109.5
N4—C3—C11111.86 (12)H10A—C10—H10C109.5
C2—C3—C11108.29 (12)H10B—C10—H10C109.5
N4—C3—H3107.0C12—C11—C3114.85 (12)
C2—C3—H3107.0C12—C11—H11A108.6
C11—C3—H3107.0C3—C11—H11A108.6
C5—N4—C3124.65 (12)C12—C11—H11B108.6
C5—N4—C10118.44 (13)C3—C11—H11B108.6
C3—N4—C10116.21 (12)H11A—C11—H11B107.5
O5—C5—N4123.57 (15)C13—C12—C17118.58 (15)
O5—C5—C6119.11 (14)C13—C12—C11120.79 (14)
N4—C5—C6117.25 (13)C17—C12—C11120.60 (14)
N1—C6—C5117.38 (12)C14—C13—C12120.93 (16)
N1—C6—S7104.82 (10)C14—C13—H13119.5
C5—C6—S7111.43 (10)C12—C13—H13119.5
N1—C6—H6107.6C15—C14—C13120.14 (17)
C5—C6—H6107.6C15—C14—H14119.9
S7—C6—H6107.6C13—C14—H14119.9
C8—S7—C691.57 (8)C14—C15—C16119.76 (16)
C9—C8—S7108.13 (12)C14—C15—H15120.1
C9—C8—H8A110.1C16—C15—H15120.1
S7—C8—H8A110.1C15—C16—C17120.21 (17)
C9—C8—H8B110.1C15—C16—H16119.9
S7—C8—H8B110.1C17—C16—H16119.9
H8A—C8—H8B108.4C16—C17—C12120.37 (16)
N1—C9—C8106.42 (13)C16—C17—H17119.8
N1—C9—H9A110.4C12—C17—H17119.8
C8—C9—H9A110.4
C6—N1—C2—O2171.76 (14)N4—C5—C6—N13.0 (2)
C9—N1—C2—O220.2 (2)O5—C5—C6—S765.32 (17)
C6—N1—C2—C38.6 (2)N4—C5—C6—S7117.83 (13)
C9—N1—C2—C3160.19 (13)N1—C6—S7—C824.08 (12)
O2—C2—C3—N4172.33 (13)C5—C6—S7—C8152.02 (12)
N1—C2—C3—N47.31 (18)C6—S7—C8—C91.01 (15)
O2—C2—C3—C1161.48 (16)C2—N1—C9—C8108.88 (17)
N1—C2—C3—C11118.88 (14)C6—N1—C9—C846.39 (18)
C2—C3—N4—C519.1 (2)S7—C8—C9—N125.71 (19)
C11—C3—N4—C5105.20 (16)N4—C3—C11—C1263.34 (16)
C2—C3—N4—C10170.70 (12)C2—C3—C11—C1264.85 (16)
C11—C3—N4—C1064.96 (16)C3—C11—C12—C1388.38 (17)
C3—N4—C5—O5169.62 (15)C3—C11—C12—C1793.65 (17)
C10—N4—C5—O50.3 (2)C17—C12—C13—C141.0 (2)
C3—N4—C5—C613.7 (2)C11—C12—C13—C14176.96 (13)
C10—N4—C5—C6176.37 (13)C12—C13—C14—C150.3 (2)
C2—N1—C6—C514.4 (2)C13—C14—C15—C160.3 (2)
C9—N1—C6—C5168.93 (13)C14—C15—C16—C170.1 (2)
C2—N1—C6—S7109.88 (14)C15—C16—C17—C120.6 (2)
C9—N1—C6—S744.70 (13)C13—C12—C17—C161.2 (2)
O5—C5—C6—N1173.84 (14)C11—C12—C17—C16176.81 (14)
(12b) top
Crystal data top
C14H16N2O2SF(000) = 584
Mr = 276.35Dx = 1.357 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 4807 reflections
a = 10.0987 (4) Åθ = 2.6–27.4°
b = 11.0883 (4) ŵ = 0.24 mm1
c = 12.0825 (5) ÅT = 150 K
V = 1352.97 (9) Å3Prism, colourless
Z = 40.54 × 0.41 × 0.26 mm
Data collection top
Bruker APEX-II CCD
diffractometer
3096 independent reflections
Radiation source: fine-focus sealed tube2931 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.020
φ and ω scansθmax = 27.5°, θmin = 2.5°
Absorption correction: multi-scan
SADABS-2014/5 - Bruker AXS area detector scaling and absorption correction
h = 1312
Tmin = 0.863, Tmax = 0.941k = 1410
8542 measured reflectionsl = 1513
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.028H-atom parameters constrained
wR(F2) = 0.069 w = 1/[σ2(Fo2) + (0.0351P)2 + 0.2268P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max = 0.001
3096 reflectionsΔρmax = 0.18 e Å3
173 parametersΔρmin = 0.22 e Å3
0 restraintsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.01 (6)
Special details top

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 (Å2) top
xyzUiso*/Ueq
N10.22369 (12)0.77660 (10)0.41260 (9)0.0210 (2)
C20.28328 (13)0.87153 (12)0.36511 (11)0.0197 (3)
C30.35435 (12)0.84942 (11)0.25659 (11)0.0180 (2)
H30.43530.90130.25740.022*
N40.40000 (11)0.72480 (10)0.24390 (9)0.0184 (2)
C50.34087 (13)0.62907 (12)0.29054 (11)0.0188 (3)
C60.22785 (13)0.65444 (11)0.36909 (10)0.0181 (3)
H60.14230.63680.33070.022*
S70.23985 (4)0.56073 (3)0.49162 (3)0.03100 (10)
C80.12233 (18)0.66080 (15)0.55673 (13)0.0343 (4)
H8A0.03120.64240.53160.041*
H8B0.12600.65230.63820.041*
C90.16183 (18)0.78775 (14)0.52223 (13)0.0347 (4)
H9A0.08300.84060.51840.042*
H9B0.22520.82250.57600.042*
C100.50501 (15)0.70247 (15)0.16278 (13)0.0295 (3)
H10A0.46540.67760.09230.044*
H10B0.56340.63840.19000.044*
H10C0.55650.77640.15170.044*
C110.26820 (14)0.89321 (12)0.15834 (11)0.0221 (3)
H11A0.25310.98110.16570.026*
H11B0.31700.87940.08840.026*
C120.13645 (14)0.83005 (11)0.15212 (11)0.0198 (3)
C130.02472 (15)0.88075 (14)0.20006 (13)0.0289 (3)
H130.03060.95810.23350.035*
C140.09570 (16)0.82002 (17)0.19984 (16)0.0376 (4)
H140.17160.85620.23230.045*
C150.10488 (15)0.70704 (15)0.15234 (14)0.0329 (4)
H150.18670.66480.15300.040*
C160.00535 (15)0.65563 (13)0.10387 (13)0.0278 (3)
H160.00080.57790.07120.033*
C170.12537 (14)0.71713 (12)0.10266 (11)0.0226 (3)
H170.20030.68180.06790.027*
O20.28006 (11)0.97279 (9)0.40579 (9)0.0306 (2)
O50.37353 (11)0.52417 (9)0.27289 (9)0.0301 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0259 (6)0.0164 (5)0.0208 (5)0.0033 (5)0.0063 (5)0.0013 (4)
C20.0182 (6)0.0176 (6)0.0234 (6)0.0024 (5)0.0022 (5)0.0008 (5)
C30.0157 (6)0.0158 (6)0.0225 (6)0.0022 (5)0.0001 (5)0.0035 (5)
N40.0153 (5)0.0191 (5)0.0209 (5)0.0013 (4)0.0027 (4)0.0024 (4)
C50.0177 (6)0.0182 (6)0.0206 (6)0.0002 (5)0.0006 (5)0.0004 (5)
C60.0179 (6)0.0158 (6)0.0207 (6)0.0003 (5)0.0016 (5)0.0028 (4)
S70.0407 (2)0.02351 (17)0.02876 (18)0.00466 (15)0.00626 (17)0.01102 (13)
C80.0350 (9)0.0396 (9)0.0284 (7)0.0016 (7)0.0120 (7)0.0067 (7)
C90.0461 (9)0.0297 (8)0.0282 (8)0.0073 (7)0.0175 (7)0.0015 (6)
C100.0237 (8)0.0325 (8)0.0323 (8)0.0010 (6)0.0118 (6)0.0017 (7)
C110.0222 (7)0.0206 (6)0.0234 (6)0.0015 (5)0.0015 (6)0.0078 (5)
C120.0212 (6)0.0183 (6)0.0198 (6)0.0014 (5)0.0042 (5)0.0052 (5)
C130.0248 (7)0.0219 (7)0.0398 (8)0.0041 (6)0.0025 (6)0.0045 (6)
C140.0214 (7)0.0387 (9)0.0529 (10)0.0044 (7)0.0044 (7)0.0047 (8)
C150.0222 (8)0.0319 (8)0.0447 (9)0.0048 (6)0.0064 (7)0.0062 (7)
C160.0315 (8)0.0222 (7)0.0297 (7)0.0008 (6)0.0102 (6)0.0009 (6)
C170.0240 (7)0.0231 (7)0.0206 (6)0.0034 (6)0.0025 (6)0.0002 (5)
O20.0380 (6)0.0174 (5)0.0363 (5)0.0019 (4)0.0033 (5)0.0043 (4)
O50.0313 (6)0.0168 (5)0.0423 (6)0.0033 (4)0.0092 (5)0.0022 (4)
Geometric parameters (Å, º) top
N1—C21.3414 (17)C9—H9B0.9900
N1—C61.4536 (16)C10—H10A0.9800
N1—C91.4697 (18)C10—H10B0.9800
C2—O21.2260 (16)C10—H10C0.9800
C2—C31.5149 (18)C11—C121.5054 (19)
C3—N41.4647 (17)C11—H11A0.9900
C3—C111.5498 (18)C11—H11B0.9900
C3—H31.0000C12—C131.387 (2)
N4—C51.3420 (17)C12—C171.3919 (19)
N4—C101.4651 (18)C13—C141.390 (2)
C5—O51.2278 (16)C13—H130.9500
C5—C61.5108 (18)C14—C151.381 (2)
C6—S71.8128 (12)C14—H140.9500
C6—H61.0000C15—C161.381 (2)
S7—C81.8051 (17)C15—H150.9500
C8—C91.521 (2)C16—C171.391 (2)
C8—H8A0.9900C16—H160.9500
C8—H8B0.9900C17—H170.9500
C9—H9A0.9900
C2—N1—C6124.31 (11)N1—C9—H9B110.5
C2—N1—C9120.67 (11)C8—C9—H9B110.5
C6—N1—C9114.62 (11)H9A—C9—H9B108.7
O2—C2—N1122.36 (12)N4—C10—H10A109.5
O2—C2—C3120.52 (12)N4—C10—H10B109.5
N1—C2—C3117.11 (11)H10A—C10—H10B109.5
N4—C3—C2113.11 (10)N4—C10—H10C109.5
N4—C3—C11113.08 (11)H10A—C10—H10C109.5
C2—C3—C11110.26 (11)H10B—C10—H10C109.5
N4—C3—H3106.6C12—C11—C3112.87 (10)
C2—C3—H3106.6C12—C11—H11A109.0
C11—C3—H3106.6C3—C11—H11A109.0
C5—N4—C3124.21 (11)C12—C11—H11B109.0
C5—N4—C10117.99 (11)C3—C11—H11B109.0
C3—N4—C10117.21 (11)H11A—C11—H11B107.8
O5—C5—N4123.84 (13)C13—C12—C17118.58 (13)
O5—C5—C6119.24 (12)C13—C12—C11120.63 (12)
N4—C5—C6116.92 (11)C17—C12—C11120.72 (13)
N1—C6—C5114.99 (11)C12—C13—C14120.96 (14)
N1—C6—S7103.93 (8)C12—C13—H13119.5
C5—C6—S7110.85 (9)C14—C13—H13119.5
N1—C6—H6109.0C15—C14—C13119.93 (15)
C5—C6—H6109.0C15—C14—H14120.0
S7—C6—H6109.0C13—C14—H14120.0
C8—S7—C687.69 (6)C16—C15—C14119.77 (14)
C9—C8—S7106.08 (11)C16—C15—H15120.1
C9—C8—H8A110.5C14—C15—H15120.1
S7—C8—H8A110.5C15—C16—C17120.30 (14)
C9—C8—H8B110.5C15—C16—H16119.9
S7—C8—H8B110.5C17—C16—H16119.9
H8A—C8—H8B108.7C16—C17—C12120.44 (13)
N1—C9—C8106.29 (12)C16—C17—H17119.8
N1—C9—H9A110.5C12—C17—H17119.8
C8—C9—H9A110.5
(14a) top
Crystal data top
C14H16N2O2SDx = 1.378 Mg m3
Mr = 276.35Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, P212121Cell parameters from 3930 reflections
a = 7.7112 (7) Åθ = 2.8–27.4°
b = 11.6576 (12) ŵ = 0.24 mm1
c = 14.8171 (14) ÅT = 150 K
V = 1332.0 (2) Å3Prism, colourless
Z = 40.47 × 0.32 × 0.22 mm
F(000) = 584
Data collection top
Bruker APEX-II CCD
diffractometer
2789 reflections with I > 2σ(I)
Radiation source: fine-focus sealed tubeRint = 0.047
φ and ω scansθmax = 27.5°, θmin = 2.2°
Absorption correction: multi-scan
SADABS-2014/5 - Bruker AXS area detector scaling and absorption correction
h = 106
Tmin = 0.895, Tmax = 0.948k = 1514
8310 measured reflectionsl = 1917
3051 independent reflections
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.035 w = 1/[σ2(Fo2) + (0.0393P)2 + 0.0987P]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.082(Δ/σ)max = 0.005
S = 1.04Δρmax = 0.28 e Å3
3051 reflectionsΔρmin = 0.22 e Å3
173 parametersAbsolute structure: Flack x determined using 1085 quotients [(I+)-(I-)]/[(I+)+(I-)] (Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259).
0 restraintsAbsolute structure parameter: 0.03 (5)
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
N10.7342 (2)0.91146 (15)0.95285 (12)0.0172 (4)
C20.6237 (3)0.87146 (18)0.89056 (15)0.0171 (5)
C30.4971 (3)0.95500 (18)0.84832 (15)0.0173 (4)
H30.37830.92200.85620.021*
N40.4954 (2)1.06933 (16)0.88879 (12)0.0179 (4)
C50.6271 (3)1.11390 (19)0.93647 (15)0.0206 (5)
C60.7600 (3)1.03238 (18)0.97499 (15)0.0181 (4)
H60.75511.03951.04220.022*
C70.9456 (3)1.05934 (19)0.94594 (16)0.0211 (5)
H7A0.98771.13070.97480.025*
H7B0.95361.06760.87960.025*
S81.06830 (7)0.93579 (5)0.98469 (5)0.02899 (17)
C90.8777 (3)0.84158 (19)0.98550 (16)0.0211 (5)
H9A0.89630.77470.94550.025*
H9B0.85400.81351.04730.025*
C100.3559 (3)1.1466 (2)0.86001 (18)0.0249 (5)
H10A0.39481.19170.80800.037*
H10B0.32591.19840.90970.037*
H10C0.25381.10140.84310.037*
C110.5332 (2)0.96046 (19)0.74573 (15)0.0182 (5)
H11A0.51540.88330.71940.022*
H11B0.44861.01310.71730.022*
C120.7149 (3)1.00079 (19)0.72346 (14)0.0169 (5)
C130.8497 (3)0.9231 (2)0.71145 (14)0.0212 (5)
H130.82860.84350.71970.025*
C141.0150 (3)0.9601 (2)0.68745 (18)0.0260 (5)
H141.10550.90590.67870.031*
C151.0474 (3)1.0762 (2)0.67630 (15)0.0256 (5)
H151.15951.10170.65900.031*
C160.9155 (3)1.1546 (2)0.69046 (16)0.0256 (5)
H160.93831.23430.68460.031*
C170.7492 (3)1.1174 (2)0.71336 (15)0.0217 (5)
H170.65911.17190.72210.026*
O20.6208 (2)0.77031 (12)0.86597 (11)0.0235 (4)
O50.6384 (2)1.21630 (14)0.95518 (13)0.0335 (5)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0156 (8)0.0167 (9)0.0194 (9)0.0033 (7)0.0011 (7)0.0001 (7)
C20.0132 (10)0.0188 (11)0.0194 (12)0.0035 (8)0.0058 (8)0.0033 (9)
C30.0122 (9)0.0162 (10)0.0234 (11)0.0028 (8)0.0002 (9)0.0001 (9)
N40.0139 (8)0.0156 (9)0.0242 (10)0.0036 (7)0.0008 (7)0.0004 (8)
C50.0165 (10)0.0232 (12)0.0221 (12)0.0040 (9)0.0029 (9)0.0054 (9)
C60.0186 (10)0.0194 (11)0.0164 (10)0.0022 (8)0.0002 (8)0.0052 (9)
C70.0165 (9)0.0194 (11)0.0273 (12)0.0029 (9)0.0036 (9)0.0002 (9)
S80.0153 (2)0.0309 (3)0.0408 (4)0.0034 (2)0.0051 (2)0.0057 (3)
C90.0195 (10)0.0223 (11)0.0213 (11)0.0054 (9)0.0012 (9)0.0023 (10)
C100.0159 (10)0.0229 (12)0.0358 (14)0.0077 (9)0.0002 (10)0.0007 (11)
C110.0134 (10)0.0206 (11)0.0205 (11)0.0017 (8)0.0036 (8)0.0015 (9)
C120.0170 (10)0.0216 (11)0.0120 (10)0.0005 (9)0.0019 (9)0.0004 (9)
C130.0183 (10)0.0236 (12)0.0218 (12)0.0001 (10)0.0015 (9)0.0001 (10)
C140.0166 (11)0.0320 (14)0.0292 (13)0.0016 (10)0.0001 (10)0.0030 (10)
C150.0168 (10)0.0361 (13)0.0238 (12)0.0065 (11)0.0004 (9)0.0070 (11)
C160.0278 (13)0.0243 (12)0.0245 (12)0.0071 (10)0.0025 (10)0.0060 (10)
C170.0226 (11)0.0230 (12)0.0196 (12)0.0011 (9)0.0004 (9)0.0031 (9)
O20.0223 (8)0.0147 (8)0.0335 (9)0.0035 (6)0.0011 (7)0.0001 (7)
O50.0285 (9)0.0200 (9)0.0521 (12)0.0071 (7)0.0072 (9)0.0141 (8)
Geometric parameters (Å, º) top
N1—C21.340 (3)C9—H9B0.9900
N1—C91.457 (3)C10—H10A0.9800
N1—C61.461 (3)C10—H10B0.9800
C2—O21.234 (3)C10—H10C0.9800
C2—C31.514 (3)C11—C121.514 (3)
C3—N41.462 (3)C11—H11A0.9900
C3—C111.547 (3)C11—H11B0.9900
C3—H31.0000C12—C131.390 (3)
N4—C51.342 (3)C12—C171.394 (3)
N4—C101.467 (3)C13—C141.392 (3)
C5—O51.229 (3)C13—H130.9500
C5—C61.509 (3)C14—C151.385 (3)
C6—C71.527 (3)C14—H140.9500
C6—H61.0000C15—C161.384 (3)
C7—S81.817 (2)C15—H150.9500
C7—H7A0.9900C16—C171.395 (3)
C7—H7B0.9900C16—H160.9500
S8—C91.835 (2)C17—H170.9500
C9—H9A0.9900
C2—N1—C9121.15 (18)N1—C9—H9B110.6
C2—N1—C6125.23 (17)S8—C9—H9B110.6
C9—N1—C6111.21 (17)H9A—C9—H9B108.7
O2—C2—N1123.2 (2)N4—C10—H10A109.5
O2—C2—C3118.7 (2)N4—C10—H10B109.5
N1—C2—C3118.10 (18)H10A—C10—H10B109.5
N4—C3—C2115.00 (18)N4—C10—H10C109.5
N4—C3—C11111.56 (17)H10A—C10—H10C109.5
C2—C3—C11108.45 (18)H10B—C10—H10C109.5
N4—C3—H3107.2C12—C11—C3113.18 (18)
C2—C3—H3107.2C12—C11—H11A108.9
C11—C3—H3107.2C3—C11—H11A108.9
C5—N4—C3124.22 (18)C12—C11—H11B108.9
C5—N4—C10118.06 (18)C3—C11—H11B108.9
C3—N4—C10116.58 (18)H11A—C11—H11B107.8
O5—C5—N4123.3 (2)C13—C12—C17118.7 (2)
O5—C5—C6118.6 (2)C13—C12—C11121.2 (2)
N4—C5—C6117.97 (19)C17—C12—C11120.2 (2)
N1—C6—C5115.49 (18)C12—C13—C14121.0 (2)
N1—C6—C7105.23 (17)C12—C13—H13119.5
C5—C6—C7113.57 (18)C14—C13—H13119.5
N1—C6—H6107.4C15—C14—C13119.9 (2)
C5—C6—H6107.4C15—C14—H14120.1
C7—C6—H6107.4C13—C14—H14120.1
C6—C7—S8103.65 (15)C16—C15—C14119.7 (2)
C6—C7—H7A111.0C16—C15—H15120.2
S8—C7—H7A111.0C14—C15—H15120.2
C6—C7—H7B111.0C15—C16—C17120.5 (2)
S8—C7—H7B111.0C15—C16—H16119.8
H7A—C7—H7B109.0C17—C16—H16119.8
C7—S8—C993.40 (10)C12—C17—C16120.2 (2)
N1—C9—S8105.75 (14)C12—C17—H17119.9
N1—C9—H9A110.6C16—C17—H17119.9
S8—C9—H9A110.6
(14b) top
Crystal data top
C14H16N2O2SF(000) = 1752
Mr = 276.35Dx = 1.361 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 9979 reflections
a = 13.4996 (5) Åθ = 2.3–26.9°
b = 14.5841 (5) ŵ = 0.24 mm1
c = 20.5461 (8) ÅT = 150 K
V = 4045.1 (3) Å3Prism, colourless
Z = 120.56 × 0.39 × 0.37 mm
Data collection top
Bruker APEX-II CCD
diffractometer
8811 independent reflections
Radiation source: fine-focus sealed tube7668 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.030
φ and ω scansθmax = 27.0°, θmin = 1.7°
Absorption correction: multi-scan
SADABS-2014/5 - Bruker AXS area detector scaling and absorption correction
h = 1317
Tmin = 0.839, Tmax = 0.917k = 1816
23583 measured reflectionsl = 2625
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.039H-atom parameters constrained
wR(F2) = 0.102 w = 1/[σ2(Fo2) + (0.0533P)2 + 0.9427P]
where P = (Fo2 + 2Fc2)/3
S = 1.06(Δ/σ)max = 0.003
8811 reflectionsΔρmax = 0.39 e Å3
517 parametersΔρmin = 0.26 e Å3
0 restraintsAbsolute structure: Flack H D (1983), Acta Cryst. A39, 876-881
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.06 (5)
Special details top

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 (Å2) top
xyzUiso*/Ueq
N110.60480 (14)0.32716 (12)0.07200 (9)0.0262 (4)
C210.58491 (17)0.30207 (14)0.13301 (10)0.0251 (4)
C310.48098 (17)0.26865 (15)0.14798 (10)0.0258 (4)
H310.46020.29850.18960.031*
N410.40698 (13)0.29299 (12)0.09876 (9)0.0264 (4)
C510.42813 (17)0.31012 (14)0.03634 (10)0.0269 (4)
C610.53587 (15)0.32280 (14)0.01736 (10)0.0244 (4)
H610.55600.27160.01220.029*
C710.54925 (16)0.41394 (14)0.01833 (11)0.0280 (4)
H71A0.52620.40900.06390.034*
H71B0.51160.46330.00360.034*
S810.68112 (5)0.43720 (4)0.01543 (3)0.03865 (15)
C910.70182 (17)0.36268 (17)0.05501 (12)0.0333 (5)
H91A0.73030.39790.09170.040*
H91B0.74760.31210.04380.040*
C1010.30269 (17)0.28412 (17)0.11739 (12)0.0352 (5)
H10A0.27930.22220.10690.053*
H10B0.29580.29490.16420.053*
H10C0.26310.32920.09350.053*
C1110.48490 (18)0.16381 (15)0.16082 (11)0.0299 (5)
H11A0.41940.14290.17650.036*
H11B0.53410.15110.19540.036*
C1210.51231 (17)0.11065 (14)0.10070 (11)0.0280 (5)
C1310.61036 (19)0.10116 (17)0.08142 (12)0.0366 (5)
H1310.66160.12520.10810.044*
C1410.63450 (19)0.05691 (19)0.02363 (13)0.0419 (6)
H1410.70190.05160.01090.050*
C1510.5611 (2)0.02076 (17)0.01526 (13)0.0419 (6)
H1510.57770.01000.05450.050*
C1610.4630 (2)0.02974 (18)0.00344 (12)0.0402 (6)
H1610.41200.00530.02330.048*
C1710.43891 (18)0.07419 (15)0.06084 (11)0.0319 (5)
H1710.37140.07990.07320.038*
O210.64754 (12)0.30304 (11)0.17623 (7)0.0326 (4)
O510.36396 (12)0.31954 (12)0.00598 (8)0.0363 (4)
N120.35662 (15)0.17699 (13)0.08737 (9)0.0293 (4)
C220.40428 (19)0.19563 (15)0.03202 (10)0.0316 (5)
C320.5139 (2)0.21435 (18)0.03580 (11)0.0379 (6)
H320.54580.18010.00080.045*
N420.56056 (15)0.18232 (14)0.09646 (10)0.0363 (5)
C520.51233 (19)0.16795 (17)0.15212 (11)0.0341 (5)
C620.40045 (18)0.17579 (15)0.15235 (10)0.0290 (5)
H620.38130.23330.17570.035*
C720.35293 (18)0.09420 (16)0.18677 (11)0.0346 (5)
H72A0.35780.10100.23460.041*
H72B0.38570.03620.17380.041*
S820.22375 (5)0.09506 (4)0.16072 (3)0.03748 (14)
C920.25013 (18)0.16048 (17)0.08686 (12)0.0349 (5)
H92A0.23080.12510.04770.042*
H92B0.21340.21920.08700.042*
C1020.6689 (2)0.1749 (2)0.09628 (15)0.0508 (7)
H10D0.69790.23210.11250.076*
H10E0.69210.16350.05180.076*
H10F0.68920.12400.12440.076*
C1120.5330 (2)0.31743 (18)0.02376 (13)0.0416 (6)
H11C0.60520.32880.02450.050*
H11D0.50840.33380.02010.050*
C1220.48358 (18)0.37890 (16)0.07339 (11)0.0333 (5)
C1320.38367 (18)0.40155 (16)0.06889 (11)0.0326 (5)
H1320.34530.37850.03380.039*
C1420.3395 (2)0.45759 (16)0.11535 (12)0.0369 (5)
H1420.27140.47310.11150.044*
C1520.3944 (2)0.49074 (17)0.16709 (12)0.0422 (6)
H1520.36420.52860.19910.051*
C1620.4932 (2)0.46846 (18)0.17187 (13)0.0468 (7)
H1620.53130.49120.20720.056*
C1720.5377 (2)0.41291 (18)0.12535 (13)0.0424 (6)
H1720.60600.39810.12920.051*
O220.36184 (14)0.20075 (13)0.02087 (8)0.0428 (4)
O520.55408 (14)0.14734 (15)0.20364 (9)0.0491 (5)
N130.53199 (13)0.37714 (12)0.29698 (8)0.0255 (4)
C230.44281 (17)0.34175 (14)0.31160 (10)0.0268 (4)
C330.38564 (17)0.29795 (14)0.25687 (10)0.0268 (4)
H330.35480.24120.27510.032*
N430.44733 (13)0.26897 (12)0.20248 (9)0.0256 (4)
C530.53506 (16)0.30643 (14)0.18708 (10)0.0248 (4)
C630.57306 (15)0.38195 (14)0.23116 (10)0.0245 (4)
H630.55570.44270.21160.029*
C730.68418 (17)0.37675 (15)0.23994 (12)0.0319 (5)
H73A0.71910.39870.20050.038*
H73B0.70550.31320.24940.038*
S830.70814 (5)0.45137 (5)0.30873 (3)0.04241 (16)
C930.59071 (18)0.42212 (16)0.34718 (11)0.0335 (5)
H93A0.60150.38040.38450.040*
H93B0.55680.47810.36300.040*
C1030.40747 (19)0.19818 (17)0.15918 (12)0.0371 (5)
H10G0.39710.22420.11570.056*
H10H0.34420.17590.17650.056*
H10I0.45450.14710.15640.056*
C1130.29966 (16)0.36076 (15)0.23529 (11)0.0293 (5)
H11E0.26060.32910.20120.035*
H11F0.25540.37190.27290.035*
C1230.33569 (15)0.45208 (14)0.20894 (11)0.0261 (4)
C1330.35170 (18)0.52535 (16)0.25129 (12)0.0333 (5)
H1330.33770.51850.29630.040*
C1430.3879 (2)0.60818 (16)0.22804 (13)0.0413 (6)
H1430.39840.65760.25730.050*
C1530.4086 (2)0.61926 (17)0.16313 (14)0.0418 (6)
H1530.43330.67610.14740.050*
C1630.39291 (18)0.54662 (17)0.12048 (12)0.0364 (5)
H1630.40720.55370.07550.044*
C1730.35638 (16)0.46356 (15)0.14363 (11)0.0294 (5)
H1730.34560.41430.11420.035*
O230.40791 (14)0.34572 (12)0.36696 (8)0.0392 (4)
O530.58457 (12)0.28290 (11)0.14017 (7)0.0326 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N110.0215 (9)0.0263 (9)0.0307 (9)0.0007 (7)0.0025 (7)0.0001 (7)
C210.0289 (12)0.0178 (9)0.0287 (10)0.0038 (8)0.0051 (9)0.0038 (8)
C310.0294 (12)0.0239 (10)0.0241 (10)0.0023 (9)0.0004 (8)0.0021 (8)
N410.0228 (9)0.0243 (9)0.0320 (9)0.0000 (7)0.0007 (7)0.0003 (7)
C510.0272 (12)0.0214 (10)0.0320 (11)0.0007 (8)0.0024 (9)0.0010 (8)
C610.0238 (11)0.0237 (10)0.0259 (10)0.0016 (8)0.0020 (8)0.0016 (8)
C710.0265 (11)0.0249 (10)0.0325 (11)0.0032 (8)0.0003 (9)0.0015 (8)
S810.0301 (3)0.0359 (3)0.0499 (4)0.0037 (3)0.0030 (3)0.0115 (3)
C910.0240 (12)0.0365 (12)0.0395 (13)0.0029 (9)0.0020 (9)0.0074 (10)
C1010.0256 (12)0.0377 (13)0.0424 (13)0.0010 (10)0.0053 (10)0.0020 (10)
C1110.0375 (13)0.0235 (11)0.0288 (10)0.0023 (9)0.0022 (9)0.0027 (8)
C1210.0329 (12)0.0207 (10)0.0306 (11)0.0005 (9)0.0051 (9)0.0038 (8)
C1310.0341 (13)0.0300 (12)0.0456 (13)0.0042 (10)0.0119 (11)0.0090 (10)
C1410.0295 (12)0.0424 (14)0.0538 (15)0.0061 (11)0.0006 (11)0.0132 (12)
C1510.0467 (15)0.0364 (13)0.0426 (13)0.0027 (11)0.0002 (12)0.0129 (11)
C1610.0415 (15)0.0381 (13)0.0408 (13)0.0027 (11)0.0076 (11)0.0091 (10)
C1710.0291 (12)0.0294 (12)0.0373 (12)0.0044 (9)0.0024 (9)0.0015 (9)
O210.0319 (9)0.0330 (8)0.0328 (8)0.0044 (7)0.0084 (7)0.0043 (6)
O510.0280 (9)0.0445 (10)0.0364 (9)0.0017 (7)0.0080 (7)0.0071 (7)
N120.0326 (10)0.0283 (9)0.0270 (9)0.0047 (8)0.0047 (8)0.0016 (7)
C220.0453 (14)0.0248 (11)0.0247 (11)0.0095 (10)0.0014 (9)0.0022 (8)
C320.0433 (15)0.0434 (14)0.0270 (11)0.0121 (12)0.0058 (10)0.0012 (10)
N420.0315 (11)0.0405 (12)0.0369 (11)0.0109 (9)0.0014 (9)0.0023 (8)
C520.0371 (13)0.0390 (13)0.0261 (11)0.0085 (11)0.0033 (10)0.0040 (9)
C620.0329 (12)0.0290 (11)0.0252 (10)0.0067 (9)0.0019 (9)0.0038 (8)
C720.0434 (14)0.0280 (11)0.0323 (11)0.0069 (10)0.0003 (10)0.0008 (9)
S820.0400 (3)0.0305 (3)0.0419 (3)0.0015 (3)0.0029 (3)0.0031 (2)
C920.0365 (13)0.0319 (12)0.0364 (13)0.0007 (10)0.0051 (10)0.0019 (9)
C1020.0315 (14)0.0625 (19)0.0584 (17)0.0129 (13)0.0045 (13)0.0036 (14)
C1120.0373 (14)0.0443 (14)0.0431 (14)0.0034 (11)0.0127 (11)0.0103 (11)
C1220.0350 (13)0.0278 (12)0.0369 (12)0.0042 (10)0.0066 (10)0.0097 (9)
C1320.0340 (13)0.0298 (11)0.0341 (11)0.0020 (10)0.0009 (9)0.0046 (9)
C1420.0380 (14)0.0309 (12)0.0419 (13)0.0021 (11)0.0047 (10)0.0028 (10)
C1520.0574 (17)0.0274 (12)0.0419 (13)0.0052 (12)0.0009 (12)0.0010 (10)
C1620.0579 (18)0.0351 (14)0.0475 (15)0.0149 (12)0.0140 (13)0.0003 (11)
C1720.0338 (14)0.0396 (14)0.0538 (15)0.0083 (11)0.0090 (11)0.0070 (12)
O220.0560 (12)0.0462 (10)0.0262 (8)0.0116 (9)0.0059 (8)0.0037 (7)
O520.0411 (10)0.0729 (13)0.0333 (9)0.0158 (10)0.0074 (8)0.0012 (9)
N130.0259 (9)0.0244 (9)0.0262 (9)0.0027 (7)0.0032 (7)0.0007 (7)
C230.0313 (11)0.0234 (10)0.0258 (10)0.0006 (9)0.0013 (9)0.0025 (8)
C330.0279 (11)0.0194 (10)0.0331 (11)0.0055 (8)0.0020 (9)0.0011 (8)
N430.0257 (9)0.0195 (8)0.0315 (9)0.0016 (7)0.0013 (8)0.0041 (7)
C530.0269 (11)0.0215 (10)0.0261 (10)0.0031 (8)0.0047 (8)0.0044 (8)
C630.0229 (10)0.0212 (10)0.0294 (10)0.0002 (8)0.0005 (8)0.0018 (8)
C730.0258 (11)0.0274 (11)0.0424 (13)0.0008 (9)0.0014 (10)0.0059 (9)
S830.0290 (3)0.0448 (4)0.0534 (4)0.0071 (3)0.0060 (3)0.0126 (3)
C930.0377 (13)0.0319 (12)0.0308 (11)0.0049 (10)0.0053 (10)0.0021 (9)
C1030.0356 (13)0.0297 (12)0.0459 (13)0.0033 (10)0.0026 (11)0.0130 (10)
C1130.0232 (11)0.0263 (10)0.0386 (12)0.0039 (9)0.0015 (9)0.0034 (9)
C1230.0180 (10)0.0216 (10)0.0387 (11)0.0021 (8)0.0018 (8)0.0040 (8)
C1330.0327 (13)0.0296 (12)0.0377 (12)0.0005 (10)0.0004 (10)0.0069 (9)
C1430.0408 (14)0.0244 (12)0.0586 (16)0.0016 (10)0.0051 (12)0.0125 (11)
C1530.0367 (14)0.0259 (12)0.0628 (16)0.0003 (10)0.0040 (12)0.0050 (11)
C1630.0339 (13)0.0339 (12)0.0415 (13)0.0079 (11)0.0025 (10)0.0063 (10)
C1730.0235 (11)0.0300 (11)0.0346 (12)0.0063 (9)0.0023 (9)0.0050 (9)
O230.0445 (11)0.0421 (10)0.0309 (8)0.0064 (8)0.0079 (8)0.0000 (7)
O530.0312 (9)0.0349 (9)0.0316 (8)0.0012 (7)0.0028 (7)0.0029 (6)
Geometric parameters (Å, º) top
N11—C211.333 (3)C92—H92B0.9900
N11—C911.451 (3)C102—H10D0.9800
N11—C611.460 (3)C102—H10E0.9800
C21—O211.226 (3)C102—H10F0.9800
C21—C311.517 (3)C112—C1221.513 (3)
C31—N411.465 (3)C112—H11C0.9900
C31—C1111.553 (3)C112—H11D0.9900
C31—H311.0000C122—C1721.385 (3)
N41—C511.337 (3)C122—C1321.392 (3)
N41—C1011.465 (3)C132—C1421.391 (3)
C51—O511.235 (3)C132—H1320.9500
C51—C611.517 (3)C142—C1521.383 (4)
C61—C711.529 (3)C142—H1420.9500
C61—H611.0000C152—C1621.376 (4)
C71—S811.813 (2)C152—H1520.9500
C71—H71A0.9900C162—C1721.390 (4)
C71—H71B0.9900C162—H1620.9500
S81—C911.831 (2)C172—H1720.9500
C91—H91A0.9900N13—C231.344 (3)
C91—H91B0.9900N13—C931.457 (3)
C101—H10A0.9800N13—C631.463 (3)
C101—H10B0.9800C23—O231.232 (3)
C101—H10C0.9800C23—C331.506 (3)
C111—C1211.505 (3)C33—N431.456 (3)
C111—H11A0.9900C33—C1131.544 (3)
C111—H11B0.9900C33—H331.0000
C121—C1311.389 (3)N43—C531.342 (3)
C121—C1711.391 (3)N43—C1031.465 (3)
C131—C1411.390 (3)C53—O531.222 (3)
C131—H1310.9500C53—C631.516 (3)
C141—C1511.377 (4)C63—C731.513 (3)
C141—H1410.9500C63—H631.0000
C151—C1611.386 (4)C73—S831.813 (2)
C151—H1510.9500C73—H73A0.9900
C161—C1711.384 (3)C73—H73B0.9900
C161—H1610.9500S83—C931.822 (3)
C171—H1710.9500C93—H93A0.9900
N12—C221.335 (3)C93—H93B0.9900
N12—C921.458 (3)C103—H10G0.9800
N12—C621.460 (3)C103—H10H0.9800
C22—O221.231 (3)C103—H10I0.9800
C22—C321.507 (4)C113—C1231.518 (3)
C32—N421.472 (3)C113—H11E0.9900
C32—C1121.545 (4)C113—H11F0.9900
C32—H321.0000C123—C1731.381 (3)
N42—C521.333 (3)C123—C1331.395 (3)
N42—C1021.467 (3)C133—C1431.388 (3)
C52—O521.236 (3)C133—H1330.9500
C52—C621.515 (3)C143—C1531.372 (4)
C62—C721.526 (3)C143—H1430.9500
C62—H621.0000C153—C1631.391 (4)
C72—S821.824 (3)C153—H1530.9500
C72—H72A0.9900C163—C1731.392 (3)
C72—H72B0.9900C163—H1630.9500
S82—C921.828 (2)C173—H1730.9500
C92—H92A0.9900
C21—N11—C91120.39 (18)N12—C92—H92B110.6
C21—N11—C61125.65 (18)S82—C92—H92B110.6
C91—N11—C61113.96 (17)H92A—C92—H92B108.7
O21—C21—N11122.6 (2)N42—C102—H10D109.5
O21—C21—C31119.65 (19)N42—C102—H10E109.5
N11—C21—C31117.72 (18)H10D—C102—H10E109.5
N41—C31—C21114.38 (17)N42—C102—H10F109.5
N41—C31—C111112.29 (18)H10D—C102—H10F109.5
C21—C31—C111108.63 (18)H10E—C102—H10F109.5
N41—C31—H31107.1C122—C112—C32113.29 (19)
C21—C31—H31107.1C122—C112—H11C108.9
C111—C31—H31107.1C32—C112—H11C108.9
C51—N41—C101118.18 (18)C122—C112—H11D108.9
C51—N41—C31124.17 (18)C32—C112—H11D108.9
C101—N41—C31116.97 (18)H11C—C112—H11D107.7
O51—C51—N41123.1 (2)C172—C122—C132118.5 (2)
O51—C51—C61118.54 (19)C172—C122—C112120.0 (2)
N41—C51—C61118.29 (18)C132—C122—C112121.5 (2)
N11—C61—C51114.75 (17)C142—C132—C122120.6 (2)
N11—C61—C71104.82 (17)C142—C132—H132119.7
C51—C61—C71110.03 (17)C122—C132—H132119.7
N11—C61—H61109.0C152—C142—C132120.2 (3)
C51—C61—H61109.0C152—C142—H142119.9
C71—C61—H61109.0C132—C142—H142119.9
C61—C71—S81105.24 (14)C162—C152—C142119.5 (3)
C61—C71—H71A110.7C162—C152—H152120.3
S81—C71—H71A110.7C142—C152—H152120.3
C61—C71—H71B110.7C152—C162—C172120.5 (2)
S81—C71—H71B110.7C152—C162—H162119.8
H71A—C71—H71B108.8C172—C162—H162119.8
C71—S81—C9193.71 (10)C122—C172—C162120.7 (3)
N11—C91—S81105.32 (15)C122—C172—H172119.6
N11—C91—H91A110.7C162—C172—H172119.6
S81—C91—H91A110.7C23—N13—C93120.15 (18)
N11—C91—H91B110.7C23—N13—C63124.36 (17)
S81—C91—H91B110.7C93—N13—C63115.24 (17)
H91A—C91—H91B108.8O23—C23—N13122.0 (2)
N41—C101—H10A109.5O23—C23—C33120.9 (2)
N41—C101—H10B109.5N13—C23—C33117.07 (18)
H10A—C101—H10B109.5N43—C33—C23113.77 (18)
N41—C101—H10C109.5N43—C33—C113112.44 (17)
H10A—C101—H10C109.5C23—C33—C113110.38 (18)
H10B—C101—H10C109.5N43—C33—H33106.6
C121—C111—C31112.10 (18)C23—C33—H33106.6
C121—C111—H11A109.2C113—C33—H33106.6
C31—C111—H11A109.2C53—N43—C33124.57 (18)
C121—C111—H11B109.2C53—N43—C103117.88 (19)
C31—C111—H11B109.2C33—N43—C103117.41 (18)
H11A—C111—H11B107.9O53—C53—N43123.7 (2)
C131—C121—C171118.2 (2)O53—C53—C63119.36 (19)
C131—C121—C111121.3 (2)N43—C53—C63116.98 (18)
C171—C121—C111120.3 (2)N13—C63—C73105.26 (17)
C121—C131—C141120.9 (2)N13—C63—C53112.90 (17)
C121—C131—H131119.6C73—C63—C53111.75 (17)
C141—C131—H131119.6N13—C63—H63108.9
C151—C141—C131120.3 (2)C73—C63—H63108.9
C151—C141—H141119.8C53—C63—H63108.9
C131—C141—H141119.8C63—C73—S83103.87 (15)
C141—C151—C161119.4 (2)C63—C73—H73A111.0
C141—C151—H151120.3S83—C73—H73A111.0
C161—C151—H151120.3C63—C73—H73B111.0
C171—C161—C151120.3 (2)S83—C73—H73B111.0
C171—C161—H161119.8H73A—C73—H73B109.0
C151—C161—H161119.8C73—S83—C9392.42 (10)
C161—C171—C121120.9 (2)N13—C93—S83105.79 (15)
C161—C171—H171119.6N13—C93—H93A110.6
C121—C171—H171119.6S83—C93—H93A110.6
C22—N12—C92120.20 (19)N13—C93—H93B110.6
C22—N12—C62125.9 (2)S83—C93—H93B110.6
C92—N12—C62113.85 (19)H93A—C93—H93B108.7
O22—C22—N12122.7 (2)N43—C103—H10G109.5
O22—C22—C32119.4 (2)N43—C103—H10H109.5
N12—C22—C32117.8 (2)H10G—C103—H10H109.5
N42—C32—C22114.0 (2)N43—C103—H10I109.5
N42—C32—C112111.9 (2)H10G—C103—H10I109.5
C22—C32—C112109.3 (2)H10H—C103—H10I109.5
N42—C32—H32107.1C123—C113—C33112.47 (17)
C22—C32—H32107.1C123—C113—H11E109.1
C112—C32—H32107.1C33—C113—H11E109.1
C52—N42—C102118.5 (2)C123—C113—H11F109.1
C52—N42—C32124.6 (2)C33—C113—H11F109.1
C102—N42—C32116.6 (2)H11E—C113—H11F107.8
O52—C52—N42123.4 (2)C173—C123—C133118.8 (2)
O52—C52—C62118.1 (2)C173—C123—C113121.19 (19)
N42—C52—C62118.5 (2)C133—C123—C113120.0 (2)
N12—C62—C52113.72 (19)C143—C133—C123120.4 (2)
N12—C62—C72105.23 (18)C143—C133—H133119.8
C52—C62—C72111.21 (19)C123—C133—H133119.8
N12—C62—H62108.8C153—C143—C133120.6 (2)
C52—C62—H62108.8C153—C143—H143119.7
C72—C62—H62108.8C133—C143—H143119.7
C62—C72—S82105.10 (15)C143—C153—C163119.5 (2)
C62—C72—H72A110.7C143—C153—H153120.3
S82—C72—H72A110.7C163—C153—H153120.3
C62—C72—H72B110.7C153—C163—C173120.1 (2)
S82—C72—H72B110.7C153—C163—H163120.0
H72A—C72—H72B108.8C173—C163—H163120.0
C72—S82—C9293.49 (11)C123—C173—C163120.6 (2)
N12—C92—S82105.81 (16)C123—C173—H173119.7
N12—C92—H92A110.6C163—C173—H173119.7
S82—C92—H92A110.6
 

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