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In the present work, novel salts of the multimodal antidepressant drug vortioxetine (VT) were crystallized with pharmaceutically acceptable acids, aiming to improve the solubility of VT. The acids for VT were selected based on ΔpKa being greater than 2 or 3. Salts of hydrobromic acid (HBr), hydrochloric acid (HCl), p-hydroxybenzoic acid (PHBA), saccharin (SAC) and L-aspartic acid (ASP) were reported. All salts were characterized by single-crystal X-ray diffraction, FT–IR, powder X-ray diffraction (PXRD) and differential scanning calorimetry (DSC). The acidic proton is transferred to the secondary N atom on the piperazine ring of VT, forming the charge-assisted hydrogen bond N+—H...X (X = Cl, Br, O). Solubility and intrinsic dissolution rate (IDR) experiments were carried out in distilled water (pH = 7.0) to compare the solubilities of the salts with that of VT. The VT–ASP–H2O (1:1:2) salt showed 414 times higher solubility and 1722 times faster IDR compared with VT. VT–ASP–H2O (1:1:2) is a high solubility salt that is stable in a slurry experiment at 298 K in 95% ethanol. The experimental data for the VT–ASP–H2O (1:1:2) salt identify it as a promising drug candidate.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S2052520616010556/ao5012sup1.cif
Contains datablocks 1, 2, 3, 4, 5, 6, 7, 8, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616010556/ao50121sup2.hkl
Contains datablock 1

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616010556/ao50122sup3.hkl
Contains datablock 2

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616010556/ao50123sup4.hkl
Contains datablock 3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616010556/ao50124sup5.hkl
Contains datablock 4

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616010556/ao50125sup6.hkl
Contains datablock 5

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616010556/ao50126sup7.hkl
Contains datablock 6

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616010556/ao50127sup8.hkl
Contains datablock 7

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S2052520616010556/ao50128sup9.hkl
Contains datablock 8

CCDC references: 1432151; 1432152; 1432153; 1432154; 1432185; 1432597; 1432598; 1438705

Computing details top

For all compounds, data collection: PROCESS-AUTO (Rigaku,2006); cell refinement: PROCESS-AUTO (Rigaku,2006); data reduction: CrystalStructure (Rigaku,2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia,1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

(1) top
Crystal data top
C18H23N2S·C4H6NO4·2(H2O)F(000) = 500
Mr = 467.57Dx = 1.291 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 7998 reflections
a = 8.3052 (5) Åθ = 3.1–27.4°
b = 6.1117 (3) ŵ = 0.18 mm1
c = 23.7414 (13) ÅT = 296 K
β = 93.652 (2)°Platelet, colorless
V = 1202.64 (11) Å30.41 × 0.34 × 0.08 mm
Z = 2
Data collection top
Rigaku RAXIS-RAPID/ZJUG
diffractometer
4261 independent reflections
Radiation source: rotating anode2893 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.039
Detector resolution: 10.00 pixels mm-1θmax = 26.0°, θmin = 3.1°
ω scansh = 1010
Absorption correction: multi-scan
Higashi, T. (1995)
k = 76
Tmin = 0.926, Tmax = 0.986l = 2929
10512 measured 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)] = 0.036H-atom parameters constrained
wR(F2) = 0.113 w = 1/[σ2(Fo2) + (0.0418P)2 + 0.6887P]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max < 0.001
4261 reflectionsΔρmax = 0.25 e Å3
292 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: 0.03 (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
C160.4634 (4)1.0549 (6)0.22110 (15)0.0460 (9)
H16A0.35790.99220.21150.055*
H16B0.45701.14140.25510.055*
C150.5864 (4)0.8744 (6)0.23104 (14)0.0448 (8)
H15A0.55580.78220.26180.054*
H15B0.58880.78450.19740.054*
C180.7955 (4)1.0990 (6)0.19725 (14)0.0438 (8)
H18A0.79771.00840.16380.053*
H18B0.90321.15680.20570.053*
C170.6783 (4)1.2853 (6)0.18640 (15)0.0452 (9)
H17A0.67951.37950.21930.054*
H17B0.71041.37170.15470.054*
C140.8599 (4)0.8030 (6)0.26493 (14)0.0394 (8)
C130.9738 (4)0.7096 (7)0.23220 (15)0.0521 (10)
H130.98260.75780.19540.062*
C121.0750 (5)0.5448 (7)0.25380 (17)0.0625 (11)
H121.15270.48590.23170.075*
C111.0609 (5)0.4691 (7)0.30731 (16)0.0588 (11)
H111.12590.35460.32110.071*
C100.9500 (5)0.5626 (7)0.34100 (16)0.0578 (11)
H100.94070.51030.37740.069*
C90.8523 (4)0.7333 (6)0.32116 (14)0.0431 (8)
C10.7285 (5)0.7336 (7)0.42723 (15)0.0492 (9)
C60.6453 (5)0.5371 (7)0.43226 (17)0.0536 (10)
C50.6524 (5)0.4359 (7)0.48485 (18)0.0599 (11)
H50.59670.30520.48870.072*
C40.7378 (5)0.5200 (8)0.53145 (18)0.0612 (12)
C30.8175 (5)0.7154 (8)0.52557 (16)0.0627 (11)
H30.87470.77700.55660.075*
C20.8135 (5)0.8214 (7)0.47378 (16)0.0557 (10)
H20.86850.95270.47040.067*
C80.5505 (6)0.4344 (8)0.3825 (2)0.0794 (14)
H8A0.47980.32420.39580.119*
H8B0.62360.36890.35770.119*
H8C0.48790.54490.36250.119*
C70.7446 (7)0.4050 (11)0.5877 (2)0.0961 (17)
H7A0.83800.45320.61020.144*
H7B0.75090.24980.58200.144*
H7C0.64920.43870.60690.144*
C190.6255 (3)0.8536 (6)0.05815 (13)0.0336 (7)
C200.7558 (3)0.8494 (5)0.01646 (12)0.0330 (7)
H20A0.83360.96280.02700.040*
H20B0.70690.88670.02050.040*
C210.8462 (3)0.6351 (5)0.01138 (13)0.0295 (7)
H210.91750.65340.01960.035*
C220.9541 (3)0.5725 (5)0.06368 (12)0.0314 (7)
N20.5127 (3)1.1970 (5)0.17386 (11)0.0415 (7)
H2A0.51011.11870.14170.050*
H2B0.44251.30860.16880.050*
N10.7472 (3)0.9665 (4)0.24479 (11)0.0375 (7)
N30.7366 (3)0.4491 (4)0.00443 (11)0.0348 (6)
H3A0.70350.38690.02670.052*
H3B0.78930.35100.02400.052*
H3C0.65170.49830.02540.052*
O10.5579 (3)1.0380 (4)0.06489 (10)0.0443 (6)
O20.5906 (3)0.6819 (4)0.08196 (11)0.0548 (7)
O30.9330 (2)0.3917 (4)0.08561 (9)0.0428 (5)
O41.0631 (2)0.7108 (4)0.07782 (9)0.0416 (6)
O50.3420 (3)0.5782 (4)0.14528 (10)0.0468 (6)
H5010.37630.69020.13120.070*
H5020.24380.58420.13830.070*
O61.1740 (3)0.1127 (4)0.13059 (11)0.0577 (7)
H6011.10020.19530.11990.087*
H6021.14040.01110.12290.087*
S10.72259 (14)0.88432 (18)0.36320 (4)0.0606 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C160.0387 (18)0.054 (2)0.0457 (19)0.0062 (17)0.0032 (15)0.0084 (19)
C150.0384 (18)0.045 (2)0.0498 (19)0.0051 (17)0.0056 (15)0.0065 (19)
C180.0397 (19)0.047 (2)0.0446 (19)0.0038 (17)0.0040 (15)0.0074 (17)
C170.050 (2)0.040 (2)0.0450 (19)0.0010 (17)0.0020 (16)0.0078 (16)
C140.0374 (18)0.0396 (19)0.0401 (18)0.0015 (15)0.0064 (15)0.0031 (15)
C130.051 (2)0.060 (3)0.046 (2)0.014 (2)0.0060 (17)0.007 (2)
C120.056 (2)0.071 (3)0.061 (3)0.022 (2)0.012 (2)0.006 (2)
C110.059 (2)0.063 (3)0.055 (2)0.027 (2)0.0050 (19)0.009 (2)
C100.065 (2)0.064 (3)0.043 (2)0.017 (2)0.0032 (19)0.012 (2)
C90.043 (2)0.044 (2)0.0418 (19)0.0074 (16)0.0043 (15)0.0033 (17)
C10.054 (2)0.049 (2)0.0444 (19)0.0069 (18)0.0074 (17)0.0043 (19)
C60.055 (2)0.048 (2)0.058 (2)0.0080 (19)0.0030 (18)0.004 (2)
C50.057 (2)0.047 (3)0.077 (3)0.004 (2)0.017 (2)0.014 (2)
C40.058 (2)0.071 (3)0.056 (2)0.016 (2)0.009 (2)0.017 (2)
C30.068 (3)0.080 (3)0.040 (2)0.001 (3)0.0001 (19)0.002 (2)
C20.055 (2)0.054 (3)0.058 (2)0.0058 (19)0.0060 (19)0.004 (2)
C80.079 (3)0.065 (3)0.092 (3)0.002 (2)0.013 (3)0.021 (3)
C70.107 (4)0.105 (4)0.076 (3)0.015 (4)0.011 (3)0.045 (3)
C190.0251 (15)0.039 (2)0.0360 (16)0.0059 (15)0.0023 (12)0.0029 (16)
C200.0297 (16)0.0335 (19)0.0360 (16)0.0034 (14)0.0050 (13)0.0032 (15)
C210.0219 (15)0.0319 (17)0.0345 (16)0.0014 (12)0.0009 (12)0.0004 (14)
C220.0230 (15)0.0381 (19)0.0337 (16)0.0042 (14)0.0064 (12)0.0032 (15)
N20.0450 (17)0.0435 (17)0.0359 (15)0.0106 (14)0.0014 (12)0.0015 (14)
N10.0342 (14)0.0362 (15)0.0415 (15)0.0006 (12)0.0028 (12)0.0056 (13)
N30.0287 (13)0.0344 (15)0.0408 (15)0.0002 (11)0.0011 (11)0.0020 (12)
O10.0335 (12)0.0474 (15)0.0515 (14)0.0134 (11)0.0020 (10)0.0133 (12)
O20.0551 (16)0.0457 (16)0.0667 (17)0.0017 (13)0.0278 (13)0.0059 (14)
O30.0396 (13)0.0369 (13)0.0511 (13)0.0001 (11)0.0024 (10)0.0117 (12)
O40.0313 (12)0.0421 (14)0.0501 (13)0.0074 (11)0.0065 (10)0.0035 (12)
O50.0361 (12)0.0471 (15)0.0572 (14)0.0007 (11)0.0026 (11)0.0137 (12)
O60.0513 (15)0.0496 (16)0.0698 (17)0.0013 (12)0.0156 (13)0.0016 (14)
S10.0795 (7)0.0556 (6)0.0475 (5)0.0251 (6)0.0115 (5)0.0064 (5)
Geometric parameters (Å, º) top
C16—N21.496 (4)C5—H50.9300
C16—C151.512 (5)C4—C31.377 (6)
C16—H16A0.9700C4—C71.508 (6)
C16—H16B0.9700C3—C21.388 (5)
C15—N11.467 (4)C3—H30.9300
C15—H15A0.9700C2—H20.9300
C15—H15B0.9700C8—H8A0.9600
C18—N11.466 (4)C8—H8B0.9600
C18—C171.509 (5)C8—H8C0.9600
C18—H18A0.9700C7—H7A0.9600
C18—H18B0.9700C7—H7B0.9600
C17—N21.490 (4)C7—H7C0.9600
C17—H17A0.9700C19—O21.235 (4)
C17—H17B0.9700C19—O11.274 (4)
C14—C131.385 (5)C19—C201.512 (4)
C14—C91.407 (5)C20—C211.518 (4)
C14—N11.431 (4)C20—H20A0.9700
C13—C121.389 (5)C20—H20B0.9700
C13—H130.9300C21—N31.489 (4)
C12—C111.364 (5)C21—C221.533 (4)
C12—H120.9300C21—H210.9800
C11—C101.382 (5)C22—O31.239 (4)
C11—H110.9300C22—O41.268 (4)
C10—C91.386 (5)N2—H2A0.9000
C10—H100.9300N2—H2B0.9000
C9—S11.773 (4)N3—H3A0.8900
C1—C21.381 (5)N3—H3B0.8900
C1—C61.394 (6)N3—H3C0.8900
C1—S11.776 (4)O5—H5010.8204
C6—C51.391 (5)O5—H5020.8225
C6—C81.513 (6)O6—H6010.8223
C5—C41.375 (6)O6—H6020.8234
N2—C16—C15109.0 (3)C4—C3—C2120.6 (4)
N2—C16—H16A109.9C4—C3—H3119.7
C15—C16—H16A109.9C2—C3—H3119.7
N2—C16—H16B109.9C1—C2—C3120.7 (4)
C15—C16—H16B109.9C1—C2—H2119.7
H16A—C16—H16B108.3C3—C2—H2119.7
N1—C15—C16110.6 (3)C6—C8—H8A109.5
N1—C15—H15A109.5C6—C8—H8B109.5
C16—C15—H15A109.5H8A—C8—H8B109.5
N1—C15—H15B109.5C6—C8—H8C109.5
C16—C15—H15B109.5H8A—C8—H8C109.5
H15A—C15—H15B108.1H8B—C8—H8C109.5
N1—C18—C17110.1 (3)C4—C7—H7A109.5
N1—C18—H18A109.6C4—C7—H7B109.5
C17—C18—H18A109.6H7A—C7—H7B109.5
N1—C18—H18B109.6C4—C7—H7C109.5
C17—C18—H18B109.6H7A—C7—H7C109.5
H18A—C18—H18B108.2H7B—C7—H7C109.5
N2—C17—C18109.8 (3)O2—C19—O1125.1 (3)
N2—C17—H17A109.7O2—C19—C20118.9 (3)
C18—C17—H17A109.7O1—C19—C20115.9 (3)
N2—C17—H17B109.7C19—C20—C21116.4 (3)
C18—C17—H17B109.7C19—C20—H20A108.2
H17A—C17—H17B108.2C21—C20—H20A108.2
C13—C14—C9118.8 (3)C19—C20—H20B108.2
C13—C14—N1123.8 (3)C21—C20—H20B108.2
C9—C14—N1117.4 (3)H20A—C20—H20B107.3
C14—C13—C12120.7 (3)N3—C21—C20112.4 (2)
C14—C13—H13119.7N3—C21—C22109.3 (2)
C12—C13—H13119.7C20—C21—C22114.7 (3)
C11—C12—C13120.3 (4)N3—C21—H21106.7
C11—C12—H12119.9C20—C21—H21106.7
C13—C12—H12119.9C22—C21—H21106.7
C12—C11—C10119.9 (4)O3—C22—O4126.9 (3)
C12—C11—H11120.1O3—C22—C21118.2 (3)
C10—C11—H11120.1O4—C22—C21114.8 (3)
C11—C10—C9120.8 (4)C17—N2—C16110.7 (2)
C11—C10—H10119.6C17—N2—H2A109.5
C9—C10—H10119.6C16—N2—H2A109.5
C10—C9—C14119.3 (3)C17—N2—H2B109.5
C10—C9—S1124.3 (3)C16—N2—H2B109.5
C14—C9—S1116.2 (3)H2A—N2—H2B108.1
C2—C1—C6119.8 (4)C14—N1—C18116.0 (3)
C2—C1—S1117.9 (3)C14—N1—C15111.9 (3)
C6—C1—S1122.2 (3)C18—N1—C15109.3 (2)
C5—C6—C1117.9 (4)C21—N3—H3A109.5
C5—C6—C8120.4 (4)C21—N3—H3B109.5
C1—C6—C8121.8 (4)H3A—N3—H3B109.5
C4—C5—C6123.1 (4)C21—N3—H3C109.5
C4—C5—H5118.5H3A—N3—H3C109.5
C6—C5—H5118.5H3B—N3—H3C109.5
C5—C4—C3118.0 (4)H501—O5—H502104.3
C5—C4—C7121.8 (5)H601—O6—H602105.0
C3—C4—C7120.2 (4)C9—S1—C1103.12 (17)
N2—C16—C15—N158.7 (4)S1—C1—C2—C3177.6 (3)
N1—C18—C17—N258.9 (4)C4—C3—C2—C10.4 (6)
C9—C14—C13—C122.2 (6)O2—C19—C20—C215.9 (4)
N1—C14—C13—C12177.2 (3)O1—C19—C20—C21175.4 (3)
C14—C13—C12—C111.5 (6)C19—C20—C21—N357.7 (3)
C13—C12—C11—C102.6 (7)C19—C20—C21—C2267.9 (3)
C12—C11—C10—C90.1 (7)N3—C21—C22—O32.6 (4)
C11—C10—C9—C143.8 (6)C20—C21—C22—O3124.6 (3)
C11—C10—C9—S1172.7 (3)N3—C21—C22—O4173.5 (2)
C13—C14—C9—C104.8 (5)C20—C21—C22—O459.2 (3)
N1—C14—C9—C10174.7 (3)C18—C17—N2—C1656.9 (4)
C13—C14—C9—S1171.9 (3)C15—C16—N2—C1756.5 (4)
N1—C14—C9—S18.6 (4)C13—C14—N1—C1824.8 (5)
C2—C1—C6—C50.3 (6)C9—C14—N1—C18155.8 (3)
S1—C1—C6—C5177.5 (3)C13—C14—N1—C15101.5 (4)
C2—C1—C6—C8180.0 (4)C9—C14—N1—C1577.9 (4)
S1—C1—C6—C82.8 (5)C17—C18—N1—C14171.4 (3)
C1—C6—C5—C40.4 (6)C17—C18—N1—C1561.0 (4)
C8—C6—C5—C4179.3 (4)C16—C15—N1—C14168.8 (3)
C6—C5—C4—C31.1 (6)C16—C15—N1—C1861.3 (4)
C6—C5—C4—C7179.3 (4)C10—C9—S1—C19.4 (4)
C5—C4—C3—C21.1 (6)C14—C9—S1—C1174.1 (3)
C7—C4—C3—C2179.3 (4)C2—C1—S1—C9106.8 (3)
C6—C1—C2—C30.3 (6)C6—C1—S1—C976.0 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···O10.901.952.811 (4)159
O5—H501···O20.822.192.706 (3)121
O6—H601···O30.821.972.790 (3)173
N3—H3A···O20.892.452.832 (4)106
N2—H2B···O5i0.901.912.789 (4)163
N3—H3B···O4ii0.892.022.880 (3)163
N3—H3C···O1iii0.891.942.809 (3)166
O5—H502···O4iv0.822.152.848 (3)142
O6—H602···O4v0.822.092.882 (4)162
Symmetry codes: (i) x, y+1, z; (ii) x+2, y1/2, z; (iii) x+1, y1/2, z; (iv) x1, y, z; (v) x, y1, z.
(2) top
Crystal data top
C18H23N2S·C7H5O3·H2OF(000) = 968
Mr = 454.57Dx = 1.196 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 11817 reflections
a = 16.9513 (9) Åθ = 3.1–27.5°
b = 6.9458 (5) ŵ = 0.16 mm1
c = 21.5346 (11) ÅT = 296 K
β = 95.409 (1)°Platelet, colorless
V = 2524.2 (3) Å30.53 × 0.47 × 0.16 mm
Z = 4
Data collection top
Rigaku RAXIS-RAPID/ZJUG
diffractometer
5708 independent reflections
Radiation source: rotating anode2836 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.070
Detector resolution: 10.00 pixels mm-1θmax = 27.5°, θmin = 3.1°
ω scansh = 2121
Absorption correction: multi-scan
Higashi, T. (1995)
k = 98
Tmin = 0.920, Tmax = 0.975l = 2327
23055 measured 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)] = 0.068H-atom parameters constrained
wR(F2) = 0.192 w = 1/[σ2(Fo2) + (0.070P)2 + 1.3245P]
where P = (Fo2 + 2Fc2)/3
S = 1.01(Δ/σ)max < 0.001
5708 reflectionsΔρmax = 0.30 e Å3
292 parametersΔρmin = 0.37 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.019 (2)
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
C10.9819 (2)0.3543 (7)0.63561 (16)0.0815 (11)
C21.0569 (2)0.4319 (7)0.63985 (17)0.0970 (14)
H21.06600.54570.61900.116*
C31.1188 (2)0.3419 (9)0.67488 (19)0.1155 (18)
H31.16900.39720.67770.139*
C41.1076 (3)0.1731 (10)0.70551 (18)0.118 (2)
C51.0334 (4)0.0953 (8)0.69998 (19)0.1153 (17)
H51.02550.02050.72010.138*
C60.9686 (3)0.1808 (7)0.66556 (19)0.0950 (13)
C71.1768 (3)0.0789 (10)0.7441 (2)0.179 (3)
H7A1.22550.11490.72780.268*
H7B1.17090.05850.74230.268*
H7C1.17770.12080.78670.268*
C80.8882 (3)0.0848 (8)0.6609 (3)0.1389 (19)
H8A0.84750.18140.65900.208*
H8B0.88410.00510.69690.208*
H8C0.88180.00700.62390.208*
C90.87838 (19)0.3589 (5)0.52761 (16)0.0732 (10)
C100.9202 (3)0.2033 (7)0.5071 (2)0.1177 (18)
H100.96600.16270.53070.141*
C110.8958 (3)0.1079 (7)0.4529 (2)0.1148 (17)
H110.92440.00260.44050.138*
C120.8305 (2)0.1668 (6)0.41753 (18)0.0871 (12)
H120.81420.10270.38060.104*
C130.78824 (19)0.3207 (5)0.43597 (16)0.0685 (9)
H130.74340.36070.41110.082*
C140.81071 (16)0.4179 (4)0.49056 (14)0.0572 (8)
C150.70611 (17)0.5142 (4)0.55130 (14)0.0590 (8)
H15A0.72970.43120.58420.071*
H15B0.66630.44040.52620.071*
C160.66769 (18)0.6836 (5)0.57954 (14)0.0626 (8)
H16A0.62610.63960.60410.075*
H16B0.70660.75290.60690.075*
C170.6958 (2)0.8767 (5)0.48995 (16)0.0731 (10)
H17A0.73610.94930.51490.088*
H17B0.67250.95980.45700.088*
C180.7327 (2)0.7034 (5)0.46206 (14)0.0671 (9)
H18A0.69280.63330.43600.081*
H18B0.77350.74460.43630.081*
C190.47299 (17)0.7501 (4)0.41954 (12)0.0502 (7)
C200.44314 (17)0.7460 (4)0.35223 (12)0.0511 (7)
C210.48988 (19)0.6729 (5)0.30822 (13)0.0608 (8)
H210.54000.62520.32120.073*
C220.4635 (2)0.6697 (5)0.24564 (14)0.0672 (9)
H220.49560.62050.21680.081*
C230.38943 (19)0.7396 (5)0.22611 (13)0.0667 (9)
C240.34174 (19)0.8130 (6)0.26920 (14)0.0740 (10)
H240.29150.85970.25610.089*
C250.36907 (18)0.8169 (5)0.33168 (14)0.0632 (9)
H250.33710.86790.36040.076*
N10.76746 (13)0.5781 (3)0.51217 (11)0.0541 (6)
N20.63402 (14)0.8122 (4)0.52939 (11)0.0588 (7)
H2A0.61210.91540.54630.071*
H2B0.59570.74960.50560.071*
O20.43593 (12)0.8472 (3)0.45674 (8)0.0604 (6)
O10.53378 (13)0.6534 (3)0.43715 (9)0.0679 (6)
O30.35915 (15)0.7412 (5)0.16519 (10)0.1004 (9)
H3A0.39160.69500.14350.151*
O40.46355 (14)0.7404 (3)0.58120 (9)0.0747 (7)
H410.46170.77540.54290.112*
H420.47820.60370.57470.112*
S10.90446 (6)0.49192 (16)0.59616 (5)0.0857 (4)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.073 (2)0.107 (3)0.064 (2)0.027 (2)0.0067 (17)0.003 (2)
C20.073 (2)0.149 (4)0.068 (2)0.022 (3)0.0008 (19)0.016 (2)
C30.076 (3)0.203 (6)0.067 (2)0.032 (3)0.001 (2)0.002 (3)
C40.109 (4)0.192 (6)0.053 (2)0.078 (4)0.006 (2)0.008 (3)
C50.142 (4)0.130 (4)0.076 (3)0.062 (4)0.021 (3)0.020 (3)
C60.098 (3)0.109 (4)0.079 (3)0.030 (3)0.016 (2)0.006 (2)
C70.175 (5)0.281 (8)0.076 (3)0.141 (6)0.013 (3)0.015 (4)
C80.144 (5)0.114 (4)0.163 (5)0.004 (4)0.033 (4)0.014 (4)
C90.0638 (19)0.082 (3)0.074 (2)0.0283 (18)0.0043 (16)0.0014 (18)
C100.107 (3)0.146 (4)0.095 (3)0.084 (3)0.016 (2)0.024 (3)
C110.119 (3)0.121 (4)0.101 (3)0.071 (3)0.003 (3)0.030 (3)
C120.100 (3)0.074 (3)0.086 (3)0.022 (2)0.006 (2)0.020 (2)
C130.0652 (19)0.065 (2)0.075 (2)0.0065 (17)0.0046 (16)0.0065 (18)
C140.0497 (16)0.0512 (19)0.072 (2)0.0098 (14)0.0139 (14)0.0037 (15)
C150.0569 (17)0.055 (2)0.0664 (18)0.0069 (15)0.0129 (14)0.0142 (15)
C160.0559 (17)0.073 (2)0.0595 (18)0.0133 (16)0.0070 (14)0.0071 (16)
C170.082 (2)0.057 (2)0.082 (2)0.0180 (18)0.0181 (18)0.0170 (17)
C180.076 (2)0.058 (2)0.071 (2)0.0181 (17)0.0230 (16)0.0184 (16)
C190.0613 (17)0.0432 (17)0.0458 (15)0.0029 (14)0.0038 (13)0.0041 (13)
C200.0611 (17)0.0464 (17)0.0456 (14)0.0044 (14)0.0039 (13)0.0035 (13)
C210.0680 (18)0.065 (2)0.0482 (16)0.0133 (16)0.0011 (14)0.0003 (14)
C220.079 (2)0.073 (2)0.0493 (17)0.0064 (18)0.0087 (15)0.0025 (15)
C230.071 (2)0.085 (3)0.0433 (16)0.0094 (18)0.0005 (15)0.0047 (16)
C240.0566 (18)0.108 (3)0.0557 (18)0.0008 (18)0.0053 (15)0.0134 (18)
C250.0584 (18)0.077 (2)0.0549 (17)0.0054 (16)0.0058 (14)0.0068 (16)
N10.0477 (12)0.0497 (15)0.0660 (14)0.0072 (11)0.0117 (11)0.0082 (12)
N20.0583 (14)0.0603 (17)0.0576 (14)0.0176 (12)0.0037 (11)0.0016 (12)
O20.0774 (13)0.0553 (13)0.0489 (11)0.0137 (11)0.0085 (10)0.0007 (9)
O10.0774 (14)0.0687 (15)0.0552 (12)0.0272 (12)0.0062 (10)0.0036 (10)
O30.0902 (17)0.163 (3)0.0451 (12)0.0075 (17)0.0109 (12)0.0059 (15)
O40.1038 (17)0.0709 (16)0.0495 (11)0.0150 (13)0.0078 (11)0.0026 (11)
S10.0751 (6)0.1004 (8)0.0794 (6)0.0299 (5)0.0048 (5)0.0099 (5)
Geometric parameters (Å, º) top
C1—C21.376 (5)C15—H15A0.9700
C1—C61.395 (6)C15—H15B0.9700
C1—S11.774 (4)C16—N21.474 (4)
C2—C31.383 (5)C16—H16A0.9700
C2—H20.9300C16—H16B0.9700
C3—C41.368 (7)C17—N21.479 (4)
C3—H30.9300C17—C181.507 (4)
C4—C51.363 (7)C17—H17A0.9700
C4—C71.521 (6)C17—H17B0.9700
C5—C61.398 (6)C18—N11.466 (4)
C5—H50.9300C18—H18A0.9700
C6—C81.512 (7)C18—H18B0.9700
C7—H7A0.9600C19—O11.258 (3)
C7—H7B0.9600C19—O21.259 (3)
C7—H7C0.9600C19—C201.490 (4)
C8—H8A0.9600C20—C251.382 (4)
C8—H8B0.9600C20—C211.387 (4)
C8—H8C0.9600C21—C221.380 (4)
C9—C101.387 (5)C21—H210.9300
C9—C141.396 (4)C22—C231.374 (4)
C9—S11.762 (4)C22—H220.9300
C10—C111.373 (6)C23—O31.363 (3)
C10—H100.9300C23—C241.384 (5)
C11—C121.346 (5)C24—C251.381 (4)
C11—H110.9300C24—H240.9300
C12—C131.366 (5)C25—H250.9300
C12—H120.9300N2—H2A0.9000
C13—C141.378 (4)N2—H2B0.9000
C13—H130.9300O3—H3A0.8200
C14—N11.434 (4)O4—H410.8579
C15—N11.468 (4)O4—H420.9947
C15—C161.502 (4)
C2—C1—C6119.7 (4)H15A—C15—H15B108.1
C2—C1—S1117.3 (3)N2—C16—C15109.3 (2)
C6—C1—S1122.8 (3)N2—C16—H16A109.8
C1—C2—C3120.6 (5)C15—C16—H16A109.8
C1—C2—H2119.7N2—C16—H16B109.8
C3—C2—H2119.7C15—C16—H16B109.8
C4—C3—C2121.1 (5)H16A—C16—H16B108.3
C4—C3—H3119.4N2—C17—C18109.3 (3)
C2—C3—H3119.4N2—C17—H17A109.8
C5—C4—C3117.9 (4)C18—C17—H17A109.8
C5—C4—C7122.4 (6)N2—C17—H17B109.8
C3—C4—C7119.8 (6)C18—C17—H17B109.8
C4—C5—C6123.4 (5)H17A—C17—H17B108.3
C4—C5—H5118.3N1—C18—C17109.5 (3)
C6—C5—H5118.3N1—C18—H18A109.8
C1—C6—C5117.3 (5)C17—C18—H18A109.8
C1—C6—C8122.3 (4)N1—C18—H18B109.8
C5—C6—C8120.4 (5)C17—C18—H18B109.8
C4—C7—H7A109.5H18A—C18—H18B108.2
C4—C7—H7B109.5O1—C19—O2122.5 (2)
H7A—C7—H7B109.5O1—C19—C20118.4 (3)
C4—C7—H7C109.5O2—C19—C20119.0 (3)
H7A—C7—H7C109.5C25—C20—C21118.1 (3)
H7B—C7—H7C109.5C25—C20—C19121.3 (3)
C6—C8—H8A109.5C21—C20—C19120.5 (3)
C6—C8—H8B109.5C22—C21—C20121.3 (3)
H8A—C8—H8B109.5C22—C21—H21119.4
C6—C8—H8C109.5C20—C21—H21119.4
H8A—C8—H8C109.5C23—C22—C21119.8 (3)
H8B—C8—H8C109.5C23—C22—H22120.1
C10—C9—C14117.7 (3)C21—C22—H22120.1
C10—C9—S1125.4 (3)O3—C23—C22123.2 (3)
C14—C9—S1116.9 (2)O3—C23—C24116.8 (3)
C11—C10—C9121.6 (3)C22—C23—C24119.9 (3)
C11—C10—H10119.2C25—C24—C23119.8 (3)
C9—C10—H10119.2C25—C24—H24120.1
C12—C11—C10120.1 (4)C23—C24—H24120.1
C12—C11—H11120.0C24—C25—C20121.1 (3)
C10—C11—H11120.0C24—C25—H25119.5
C11—C12—C13119.9 (4)C20—C25—H25119.5
C11—C12—H12120.0C14—N1—C18113.8 (2)
C13—C12—H12120.0C14—N1—C15111.3 (2)
C12—C13—C14121.4 (3)C18—N1—C15110.2 (2)
C12—C13—H13119.3C16—N2—C17111.0 (2)
C14—C13—H13119.3C16—N2—H2A109.4
C13—C14—C9119.4 (3)C17—N2—H2A109.4
C13—C14—N1123.3 (3)C16—N2—H2B109.4
C9—C14—N1117.4 (3)C17—N2—H2B109.4
N1—C15—C16110.7 (2)H2A—N2—H2B108.0
N1—C15—H15A109.5C23—O3—H3A109.5
C16—C15—H15A109.5H41—O4—H4297.0
N1—C15—H15B109.5C9—S1—C1103.56 (17)
C16—C15—H15B109.5
C6—C1—C2—C31.7 (6)O2—C19—C20—C2511.6 (4)
S1—C1—C2—C3173.9 (3)O1—C19—C20—C2113.7 (4)
C1—C2—C3—C40.8 (7)O2—C19—C20—C21167.4 (3)
C2—C3—C4—C50.5 (7)C25—C20—C21—C220.3 (5)
C2—C3—C4—C7179.4 (4)C19—C20—C21—C22179.4 (3)
C3—C4—C5—C61.0 (7)C20—C21—C22—C230.1 (5)
C7—C4—C5—C6179.0 (4)C21—C22—C23—O3179.9 (3)
C2—C1—C6—C51.2 (6)C21—C22—C23—C240.1 (5)
S1—C1—C6—C5174.1 (3)O3—C23—C24—C25179.6 (3)
C2—C1—C6—C8177.9 (4)C22—C23—C24—C250.4 (5)
S1—C1—C6—C86.8 (6)C23—C24—C25—C200.9 (5)
C4—C5—C6—C10.1 (7)C21—C20—C25—C240.8 (5)
C4—C5—C6—C8179.3 (5)C19—C20—C25—C24179.9 (3)
C14—C9—C10—C111.0 (7)C13—C14—N1—C1836.1 (4)
S1—C9—C10—C11179.8 (4)C9—C14—N1—C18144.4 (3)
C9—C10—C11—C121.1 (9)C13—C14—N1—C1589.2 (3)
C10—C11—C12—C130.5 (8)C9—C14—N1—C1590.3 (3)
C11—C12—C13—C140.3 (6)C17—C18—N1—C14174.4 (3)
C12—C13—C14—C90.5 (5)C17—C18—N1—C1559.7 (3)
C12—C13—C14—N1179.0 (3)C16—C15—N1—C14173.5 (2)
C10—C9—C14—C130.1 (5)C16—C15—N1—C1859.3 (3)
S1—C9—C14—C13179.1 (3)C15—C16—N2—C1757.7 (3)
C10—C9—C14—N1179.7 (4)C18—C17—N2—C1658.8 (3)
S1—C9—C14—N11.4 (4)C10—C9—S1—C19.9 (5)
N1—C15—C16—N257.5 (3)C14—C9—S1—C1171.3 (3)
N2—C17—C18—N159.2 (3)C2—C1—S1—C9111.1 (3)
O1—C19—C20—C25167.2 (3)C6—C1—S1—C973.5 (4)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2B···O10.901.852.723 (3)162
O4—H41···O20.861.932.778 (3)169
N2—H2A···O2i0.901.842.676 (3)154
O3—H3A···O4ii0.821.952.650 (3)143
O4—H42···O1iii0.991.812.765 (3)159
Symmetry codes: (i) x+1, y+2, z+1; (ii) x, y+3/2, z1/2; (iii) x+1, y+1, z+1.
(3) top
Crystal data top
C18H23N2S·C7H5O3F(000) = 928
Mr = 436.55Dx = 1.260 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 13019 reflections
a = 8.6363 (3) Åθ = 3.1–27.4°
b = 20.6504 (8) ŵ = 0.17 mm1
c = 12.9243 (6) ÅT = 296 K
β = 93.435 (1)°Chunk, colorless
V = 2300.82 (16) Å30.48 × 0.29 × 0.16 mm
Z = 4
Data collection top
Rigaku RAXIS-RAPID/ZJUG
diffractometer
5230 independent reflections
Radiation source: rotating anode3088 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.058
Detector resolution: 10.00 pixels mm-1θmax = 27.4°, θmin = 3.1°
ω scansh = 1110
Absorption correction: multi-scan
Higashi, T. (1995)
k = 2626
Tmin = 0.913, Tmax = 0.973l = 1616
22208 measured 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)] = 0.046H-atom parameters constrained
wR(F2) = 0.137 w = 1/[σ2(Fo2) + (0.0548P)2 + 0.821P]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max < 0.001
5230 reflectionsΔρmax = 0.27 e Å3
284 parametersΔρmin = 0.38 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0176 (14)
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
C10.1287 (2)0.50743 (10)0.38634 (16)0.0414 (5)
C20.0397 (2)0.54874 (10)0.32343 (18)0.0466 (5)
H20.03140.59220.34140.056*
C30.0373 (3)0.52594 (11)0.23396 (19)0.0516 (6)
H30.09620.55440.19210.062*
C40.0283 (3)0.46123 (11)0.20538 (18)0.0507 (6)
C50.0570 (3)0.42025 (11)0.27146 (18)0.0487 (6)
H50.06210.37660.25430.058*
C60.1351 (2)0.44133 (10)0.36217 (17)0.0437 (5)
C70.1097 (3)0.43717 (15)0.1064 (2)0.0786 (9)
H7A0.03710.41440.06620.118*
H7B0.15170.47330.06720.118*
H7C0.19220.40840.12260.118*
C80.2218 (3)0.39424 (11)0.4329 (2)0.0643 (7)
H8A0.19950.35080.41000.096*
H8B0.19010.39960.50230.096*
H8C0.33120.40220.43160.096*
C90.2609 (3)0.61786 (11)0.48385 (17)0.0469 (5)
C100.2192 (3)0.65766 (13)0.5644 (2)0.0662 (7)
H100.17760.63960.62250.079*
C110.2392 (4)0.72403 (14)0.5586 (3)0.0804 (9)
H110.21210.75040.61310.097*
C120.2990 (4)0.75097 (13)0.4727 (3)0.0805 (9)
H120.31120.79560.46840.097*
C130.3413 (3)0.71173 (11)0.3925 (2)0.0637 (7)
H130.38130.73050.33440.076*
C140.3253 (2)0.64496 (10)0.39680 (17)0.0440 (5)
C150.3403 (3)0.62509 (11)0.21028 (17)0.0508 (6)
H15A0.41910.65610.19300.061*
H15B0.24000.64620.20240.061*
C160.3438 (3)0.56731 (12)0.13877 (18)0.0543 (6)
H16A0.26110.53760.15380.065*
H16B0.32680.58150.06750.065*
C170.5328 (3)0.51576 (11)0.26245 (17)0.0484 (5)
H17A0.63690.49810.26980.058*
H17B0.46120.48270.28330.058*
C180.5219 (2)0.57402 (11)0.33155 (17)0.0464 (5)
H18A0.53960.56110.40350.056*
H18B0.60090.60530.31570.056*
C190.3626 (3)0.37479 (10)0.03152 (18)0.0444 (5)
C200.3017 (2)0.32396 (9)0.10119 (16)0.0402 (5)
C210.3725 (3)0.31279 (10)0.19855 (17)0.0447 (5)
H210.45790.33770.22060.054*
C220.3197 (3)0.26553 (10)0.26412 (17)0.0470 (5)
H220.37060.25830.32850.056*
C230.1905 (3)0.22923 (10)0.23279 (17)0.0459 (5)
C240.1164 (3)0.24045 (11)0.13676 (18)0.0533 (6)
H240.02850.21670.11590.064*
C250.1723 (3)0.28684 (10)0.07159 (17)0.0485 (5)
H250.12230.29340.00670.058*
N10.3690 (2)0.60334 (8)0.31585 (13)0.0419 (4)
N20.4953 (2)0.53367 (9)0.15226 (13)0.0467 (5)
H2A0.57030.55970.13030.056*
H2B0.49290.49760.11300.056*
O10.4650 (2)0.41301 (8)0.06850 (13)0.0597 (5)
O20.31152 (19)0.37677 (7)0.06250 (12)0.0540 (4)
O30.1286 (2)0.18274 (8)0.29356 (14)0.0637 (5)
H3A0.19220.17280.34060.096*
S10.23686 (7)0.53347 (3)0.50000 (4)0.0525 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0432 (11)0.0413 (11)0.0400 (12)0.0029 (9)0.0054 (9)0.0013 (9)
C20.0468 (12)0.0391 (11)0.0538 (14)0.0015 (9)0.0018 (10)0.0004 (10)
C30.0434 (12)0.0527 (13)0.0577 (15)0.0003 (10)0.0061 (11)0.0052 (11)
C40.0426 (12)0.0588 (14)0.0499 (14)0.0044 (11)0.0037 (10)0.0065 (11)
C50.0502 (13)0.0439 (12)0.0521 (15)0.0021 (10)0.0028 (11)0.0087 (10)
C60.0478 (12)0.0408 (11)0.0430 (13)0.0017 (10)0.0058 (10)0.0003 (9)
C70.0764 (19)0.086 (2)0.070 (2)0.0008 (16)0.0225 (15)0.0167 (16)
C80.094 (2)0.0454 (12)0.0526 (16)0.0110 (13)0.0056 (14)0.0018 (11)
C90.0495 (13)0.0477 (12)0.0434 (13)0.0074 (10)0.0023 (10)0.0087 (10)
C100.0744 (18)0.0700 (16)0.0556 (16)0.0159 (14)0.0158 (13)0.0249 (13)
C110.089 (2)0.0652 (17)0.089 (2)0.0172 (16)0.0225 (18)0.0388 (17)
C120.092 (2)0.0444 (14)0.106 (3)0.0156 (14)0.0140 (19)0.0253 (15)
C130.0694 (17)0.0461 (13)0.0766 (19)0.0144 (12)0.0125 (14)0.0055 (13)
C140.0442 (12)0.0411 (11)0.0468 (13)0.0042 (9)0.0025 (10)0.0074 (9)
C150.0537 (13)0.0542 (13)0.0439 (14)0.0037 (11)0.0018 (10)0.0117 (11)
C160.0498 (13)0.0752 (16)0.0372 (13)0.0050 (12)0.0043 (10)0.0043 (11)
C170.0579 (14)0.0497 (12)0.0377 (13)0.0051 (11)0.0036 (10)0.0052 (10)
C180.0463 (12)0.0555 (13)0.0367 (12)0.0024 (10)0.0042 (9)0.0023 (10)
C190.0519 (13)0.0392 (11)0.0427 (13)0.0008 (10)0.0088 (10)0.0070 (9)
C200.0463 (12)0.0350 (10)0.0399 (12)0.0008 (9)0.0076 (9)0.0029 (9)
C210.0456 (12)0.0445 (11)0.0437 (13)0.0011 (10)0.0008 (10)0.0062 (10)
C220.0547 (13)0.0461 (12)0.0398 (13)0.0052 (11)0.0015 (10)0.0002 (10)
C230.0579 (13)0.0369 (11)0.0434 (13)0.0019 (10)0.0055 (10)0.0045 (9)
C240.0609 (15)0.0510 (13)0.0473 (14)0.0132 (11)0.0043 (11)0.0060 (11)
C250.0571 (14)0.0490 (12)0.0387 (13)0.0046 (11)0.0040 (10)0.0037 (10)
N10.0439 (10)0.0452 (9)0.0363 (10)0.0020 (8)0.0003 (8)0.0003 (8)
N20.0543 (11)0.0506 (10)0.0355 (10)0.0093 (9)0.0056 (8)0.0046 (8)
O10.0734 (11)0.0547 (9)0.0511 (10)0.0214 (8)0.0062 (8)0.0085 (8)
O20.0675 (10)0.0546 (9)0.0399 (10)0.0131 (8)0.0026 (8)0.0035 (7)
O30.0808 (12)0.0545 (9)0.0549 (11)0.0114 (9)0.0031 (9)0.0194 (8)
S10.0722 (4)0.0475 (3)0.0373 (3)0.0079 (3)0.0016 (3)0.0008 (2)
Geometric parameters (Å, º) top
C1—C21.380 (3)C15—C161.510 (3)
C1—C61.402 (3)C15—H15A0.9700
C1—S11.776 (2)C15—H15B0.9700
C2—C31.381 (3)C16—N21.483 (3)
C2—H20.9300C16—H16A0.9700
C3—C41.390 (3)C16—H16B0.9700
C3—H30.9300C17—N21.488 (3)
C4—C51.383 (3)C17—C181.505 (3)
C4—C71.507 (3)C17—H17A0.9700
C5—C61.387 (3)C17—H17B0.9700
C5—H50.9300C18—N11.456 (3)
C6—C81.504 (3)C18—H18A0.9700
C7—H7A0.9600C18—H18B0.9700
C7—H7B0.9600C19—O11.258 (3)
C7—H7C0.9600C19—O21.268 (3)
C8—H8A0.9600C19—C201.499 (3)
C8—H8B0.9600C20—C211.385 (3)
C8—H8C0.9600C20—C251.390 (3)
C9—C101.391 (3)C21—C221.388 (3)
C9—C141.401 (3)C21—H210.9300
C9—S11.769 (2)C22—C231.384 (3)
C10—C111.384 (4)C22—H220.9300
C10—H100.9300C23—O31.369 (2)
C11—C121.371 (4)C23—C241.382 (3)
C11—H110.9300C24—C251.382 (3)
C12—C131.381 (4)C24—H240.9300
C12—H120.9300C25—H250.9300
C13—C141.387 (3)N2—H2A0.9000
C13—H130.9300N2—H2B0.9000
C14—N11.422 (3)O3—H3A0.8200
C15—N11.444 (3)
C2—C1—C6119.9 (2)C16—C15—H15B109.9
C2—C1—S1123.15 (16)H15A—C15—H15B108.3
C6—C1—S1116.96 (16)N2—C16—C15110.34 (18)
C1—C2—C3120.4 (2)N2—C16—H16A109.6
C1—C2—H2119.8C15—C16—H16A109.6
C3—C2—H2119.8N2—C16—H16B109.6
C2—C3—C4121.2 (2)C15—C16—H16B109.6
C2—C3—H3119.4H16A—C16—H16B108.1
C4—C3—H3119.4N2—C17—C18110.59 (17)
C5—C4—C3117.4 (2)N2—C17—H17A109.5
C5—C4—C7121.8 (2)C18—C17—H17A109.5
C3—C4—C7120.8 (2)N2—C17—H17B109.5
C4—C5—C6122.9 (2)C18—C17—H17B109.5
C4—C5—H5118.5H17A—C17—H17B108.1
C6—C5—H5118.5N1—C18—C17109.78 (17)
C5—C6—C1118.0 (2)N1—C18—H18A109.7
C5—C6—C8120.7 (2)C17—C18—H18A109.7
C1—C6—C8121.3 (2)N1—C18—H18B109.7
C4—C7—H7A109.5C17—C18—H18B109.7
C4—C7—H7B109.5H18A—C18—H18B108.2
H7A—C7—H7B109.5O1—C19—O2122.7 (2)
C4—C7—H7C109.5O1—C19—C20118.4 (2)
H7A—C7—H7C109.5O2—C19—C20118.94 (19)
H7B—C7—H7C109.5C21—C20—C25117.52 (19)
C6—C8—H8A109.5C21—C20—C19120.73 (19)
C6—C8—H8B109.5C25—C20—C19121.7 (2)
H8A—C8—H8B109.5C20—C21—C22121.9 (2)
C6—C8—H8C109.5C20—C21—H21119.0
H8A—C8—H8C109.5C22—C21—H21119.0
H8B—C8—H8C109.5C23—C22—C21119.4 (2)
C10—C9—C14119.9 (2)C23—C22—H22120.3
C10—C9—S1117.15 (19)C21—C22—H22120.3
C14—C9—S1122.90 (16)O3—C23—C24117.2 (2)
C11—C10—C9120.4 (3)O3—C23—C22123.2 (2)
C11—C10—H10119.8C24—C23—C22119.6 (2)
C9—C10—H10119.8C23—C24—C25120.3 (2)
C12—C11—C10120.0 (3)C23—C24—H24119.9
C12—C11—H11120.0C25—C24—H24119.9
C10—C11—H11120.0C24—C25—C20121.3 (2)
C11—C12—C13119.9 (2)C24—C25—H25119.4
C11—C12—H12120.0C20—C25—H25119.4
C13—C12—H12120.0C14—N1—C15117.99 (17)
C12—C13—C14121.5 (3)C14—N1—C18115.29 (17)
C12—C13—H13119.3C15—N1—C18111.33 (18)
C14—C13—H13119.3C16—N2—C17111.64 (17)
C13—C14—C9118.3 (2)C16—N2—H2A109.3
C13—C14—N1122.7 (2)C17—N2—H2A109.3
C9—C14—N1119.01 (18)C16—N2—H2B109.3
N1—C15—C16108.91 (18)C17—N2—H2B109.3
N1—C15—H15A109.9H2A—N2—H2B108.0
C16—C15—H15A109.9C23—O3—H3A109.5
N1—C15—H15B109.9C9—S1—C1105.09 (10)
C6—C1—C2—C33.2 (3)O2—C19—C20—C21168.8 (2)
S1—C1—C2—C3177.61 (17)O1—C19—C20—C25169.6 (2)
C1—C2—C3—C40.5 (4)O2—C19—C20—C2511.9 (3)
C2—C3—C4—C51.8 (4)C25—C20—C21—C221.4 (3)
C2—C3—C4—C7178.6 (2)C19—C20—C21—C22179.22 (19)
C3—C4—C5—C61.5 (4)C20—C21—C22—C231.4 (3)
C7—C4—C5—C6178.9 (2)C21—C22—C23—O3178.4 (2)
C4—C5—C6—C11.1 (3)C21—C22—C23—C240.1 (3)
C4—C5—C6—C8178.0 (2)O3—C23—C24—C25179.8 (2)
C2—C1—C6—C53.4 (3)C22—C23—C24—C251.1 (3)
S1—C1—C6—C5177.32 (16)C23—C24—C25—C201.1 (4)
C2—C1—C6—C8175.7 (2)C21—C20—C25—C240.1 (3)
S1—C1—C6—C83.6 (3)C19—C20—C25—C24179.5 (2)
C14—C9—C10—C110.8 (4)C13—C14—N1—C1537.7 (3)
S1—C9—C10—C11178.0 (2)C9—C14—N1—C15141.2 (2)
C9—C10—C11—C120.7 (5)C13—C14—N1—C1897.3 (3)
C10—C11—C12—C130.9 (5)C9—C14—N1—C1883.8 (2)
C11—C12—C13—C140.3 (5)C16—C15—N1—C14161.23 (18)
C12—C13—C14—C91.6 (4)C16—C15—N1—C1862.1 (2)
C12—C13—C14—N1179.5 (2)C17—C18—N1—C14160.91 (18)
C10—C9—C14—C131.9 (3)C17—C18—N1—C1561.2 (2)
S1—C9—C14—C13178.96 (18)C15—C16—N2—C1754.5 (2)
C10—C9—C14—N1179.2 (2)C18—C17—N2—C1653.2 (2)
S1—C9—C14—N12.1 (3)C10—C9—S1—C1128.30 (19)
N1—C15—C16—N258.0 (2)C14—C9—S1—C154.5 (2)
N2—C17—C18—N155.5 (2)C2—C1—S1—C920.8 (2)
O1—C19—C20—C219.8 (3)C6—C1—S1—C9159.94 (17)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2B···O10.901.852.723 (2)163
N2—H2A···O2i0.901.912.789 (2)166
O3—H3A···O2ii0.821.882.667 (2)161
Symmetry codes: (i) x+1, y+1, z; (ii) x, y+1/2, z+1/2.
(4) top
Crystal data top
C18H23N2S·C7H4NO3SF(000) = 1016
Mr = 481.62Dx = 1.269 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 13112 reflections
a = 6.8375 (3) Åθ = 3.1–27.4°
b = 15.8835 (7) ŵ = 0.24 mm1
c = 23.2329 (9) ÅT = 296 K
β = 92.451 (1)°Chunk, colorless
V = 2520.86 (18) Å30.46 × 0.39 × 0.20 mm
Z = 4
Data collection top
Rigaku RAXIS-RAPID/ZJUG
diffractometer
4910 independent reflections
Radiation source: rotating anode3001 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.041
Detector resolution: 10.00 pixels mm-1θmax = 26.0°, θmin = 3.1°
ω scansh = 88
Absorption correction: multi-scan
Higashi, T. (1995)
k = 1819
Tmin = 0.897, Tmax = 0.953l = 2828
20672 measured 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)] = 0.046H-atom parameters constrained
wR(F2) = 0.148 w = 1/[σ2(Fo2) + (0.0569P)2 + 1.9621P]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max = 0.001
4910 reflectionsΔρmax = 0.44 e Å3
301 parametersΔρmin = 0.39 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0212 (14)
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
C10.5606 (5)0.54205 (18)0.18239 (13)0.0556 (8)
C20.6134 (6)0.5579 (2)0.12678 (14)0.0790 (10)
H20.73770.54340.11540.095*
C30.4810 (8)0.5956 (3)0.08795 (16)0.0962 (14)
H30.51950.60640.05080.115*
C40.2963 (7)0.6173 (2)0.10225 (16)0.0765 (11)
C50.2478 (6)0.6022 (2)0.15760 (15)0.0767 (10)
H50.12330.61730.16860.092*
C60.3756 (5)0.5652 (2)0.19859 (13)0.0688 (9)
C70.1522 (7)0.6567 (3)0.0587 (2)0.1228 (19)
H7A0.10470.61440.03210.184*
H7B0.21630.70040.03810.184*
H7C0.04430.68020.07840.184*
C80.3081 (7)0.5500 (4)0.25865 (17)0.135 (2)
H8A0.33460.49270.26960.203*
H8B0.17000.56050.25960.203*
H8C0.37670.58720.28510.203*
C90.6665 (4)0.39309 (18)0.23725 (12)0.0547 (7)
C100.5292 (5)0.3557 (2)0.19991 (14)0.0716 (10)
H100.45800.38890.17350.086*
C110.4967 (6)0.2704 (2)0.20131 (17)0.0867 (12)
H110.40210.24620.17650.104*
C120.6038 (7)0.2210 (2)0.23919 (19)0.0972 (14)
H120.58700.16290.23890.117*
C130.7368 (6)0.2576 (2)0.27785 (16)0.0812 (11)
H130.80680.22360.30400.097*
C140.7683 (4)0.34304 (18)0.27861 (12)0.0545 (7)
C151.0584 (5)0.3318 (2)0.34359 (15)0.0682 (9)
H15A1.12460.30340.31300.082*
H15B1.00480.28940.36840.082*
C161.2025 (5)0.3861 (2)0.37788 (15)0.0731 (10)
H16A1.30540.35110.39510.088*
H16B1.26220.42620.35250.088*
C170.9340 (4)0.4817 (2)0.39972 (13)0.0612 (8)
H17A0.98150.52630.37540.073*
H17B0.86530.50740.43090.073*
C180.7969 (4)0.4257 (2)0.36515 (12)0.0540 (7)
H18A0.74330.38330.39010.065*
H18B0.68920.45880.34880.065*
C190.5579 (4)0.28238 (19)0.57044 (12)0.0506 (7)
C200.4306 (6)0.2354 (3)0.60181 (16)0.0822 (11)
H200.31770.25890.61600.099*
C210.4782 (7)0.1518 (3)0.61129 (19)0.0981 (14)
H210.39610.11850.63270.118*
C220.6421 (7)0.1171 (2)0.59009 (17)0.0875 (12)
H220.66900.06040.59680.105*
C230.7684 (6)0.1641 (2)0.55897 (14)0.0691 (9)
H230.88110.14030.54490.083*
C240.7236 (4)0.24800 (18)0.54898 (11)0.0497 (7)
C250.8340 (5)0.3132 (2)0.51677 (13)0.0578 (8)
N10.8998 (3)0.38451 (15)0.31881 (10)0.0531 (6)
N21.1015 (4)0.43166 (18)0.42360 (11)0.0641 (7)
H2A1.18710.46620.44230.077*
H2B1.05810.39430.44920.077*
N30.7516 (4)0.38955 (17)0.51677 (11)0.0623 (7)
O10.9866 (4)0.29579 (19)0.49223 (11)0.0882 (8)
O20.5630 (4)0.44340 (15)0.59810 (10)0.0837 (8)
O30.3857 (3)0.40264 (15)0.51036 (11)0.0791 (7)
S10.73721 (13)0.49966 (5)0.23268 (4)0.0642 (3)
S20.55065 (12)0.38844 (5)0.54906 (3)0.0567 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.068 (2)0.0444 (16)0.0539 (17)0.0083 (14)0.0055 (15)0.0048 (13)
C20.095 (3)0.084 (3)0.059 (2)0.004 (2)0.008 (2)0.0121 (18)
C30.130 (4)0.107 (3)0.051 (2)0.010 (3)0.003 (2)0.032 (2)
C40.104 (3)0.057 (2)0.066 (2)0.015 (2)0.025 (2)0.0200 (16)
C50.078 (2)0.080 (2)0.070 (2)0.0049 (19)0.0183 (19)0.0119 (18)
C60.077 (2)0.079 (2)0.0495 (17)0.0015 (18)0.0074 (17)0.0119 (16)
C70.146 (4)0.112 (4)0.104 (3)0.018 (3)0.057 (3)0.050 (3)
C80.096 (3)0.243 (7)0.068 (3)0.043 (4)0.013 (3)0.043 (3)
C90.0621 (18)0.0488 (17)0.0521 (16)0.0038 (14)0.0079 (14)0.0067 (13)
C100.087 (2)0.056 (2)0.070 (2)0.0131 (17)0.0281 (19)0.0088 (16)
C110.112 (3)0.056 (2)0.089 (3)0.024 (2)0.031 (2)0.0008 (19)
C120.137 (4)0.047 (2)0.105 (3)0.017 (2)0.031 (3)0.012 (2)
C130.109 (3)0.050 (2)0.082 (2)0.0008 (19)0.024 (2)0.0121 (17)
C140.0622 (18)0.0478 (17)0.0530 (16)0.0004 (14)0.0032 (15)0.0038 (13)
C150.065 (2)0.072 (2)0.068 (2)0.0177 (17)0.0030 (17)0.0102 (17)
C160.0518 (18)0.098 (3)0.069 (2)0.0042 (18)0.0050 (17)0.0223 (19)
C170.0643 (19)0.066 (2)0.0526 (17)0.0003 (15)0.0084 (15)0.0092 (14)
C180.0482 (16)0.0644 (19)0.0488 (16)0.0037 (14)0.0034 (14)0.0017 (14)
C190.0520 (17)0.0575 (18)0.0420 (14)0.0044 (14)0.0013 (13)0.0085 (12)
C200.074 (2)0.092 (3)0.082 (2)0.006 (2)0.021 (2)0.016 (2)
C210.117 (4)0.081 (3)0.097 (3)0.028 (3)0.013 (3)0.039 (2)
C220.126 (4)0.054 (2)0.081 (3)0.005 (2)0.015 (3)0.0229 (19)
C230.089 (2)0.060 (2)0.0575 (19)0.0133 (18)0.0089 (18)0.0055 (16)
C240.0573 (18)0.0537 (17)0.0375 (13)0.0015 (14)0.0050 (13)0.0066 (12)
C250.0517 (18)0.075 (2)0.0465 (16)0.0023 (16)0.0018 (15)0.0117 (15)
N10.0527 (14)0.0556 (15)0.0505 (13)0.0051 (11)0.0055 (12)0.0050 (11)
N20.0568 (15)0.0824 (19)0.0521 (14)0.0111 (13)0.0076 (13)0.0166 (13)
N30.0614 (16)0.0596 (17)0.0655 (16)0.0070 (13)0.0024 (13)0.0162 (13)
O10.0683 (15)0.113 (2)0.0848 (17)0.0108 (14)0.0240 (14)0.0220 (15)
O20.1069 (19)0.0666 (16)0.0760 (15)0.0170 (13)0.0153 (14)0.0216 (12)
O30.0666 (14)0.0782 (16)0.0891 (16)0.0073 (12)0.0357 (13)0.0139 (13)
S10.0708 (5)0.0482 (5)0.0719 (5)0.0099 (4)0.0184 (4)0.0103 (4)
S20.0619 (5)0.0509 (4)0.0560 (4)0.0024 (3)0.0129 (4)0.0044 (3)
Geometric parameters (Å, º) top
C1—C21.380 (4)C15—H15A0.9700
C1—C61.384 (5)C15—H15B0.9700
C1—S11.777 (3)C16—N21.481 (4)
C2—C31.386 (5)C16—H16A0.9700
C2—H20.9300C16—H16B0.9700
C3—C41.364 (6)C17—N21.482 (4)
C3—H30.9300C17—C181.501 (4)
C4—C51.363 (5)C17—H17A0.9700
C4—C71.516 (5)C17—H17B0.9700
C5—C61.395 (4)C18—N11.465 (4)
C5—H50.9300C18—H18A0.9700
C6—C81.508 (5)C18—H18B0.9700
C7—H7A0.9600C19—C241.371 (4)
C7—H7B0.9600C19—C201.378 (4)
C7—H7C0.9600C19—S21.756 (3)
C8—H8A0.9600C20—C211.383 (6)
C8—H8B0.9600C20—H200.9300
C8—H8C0.9600C21—C221.361 (6)
C9—C101.384 (4)C21—H210.9300
C9—C141.408 (4)C22—C231.371 (5)
C9—S11.765 (3)C22—H220.9300
C10—C111.375 (5)C23—C241.385 (4)
C10—H100.9300C23—H230.9300
C11—C121.367 (5)C24—C251.500 (4)
C11—H110.9300C25—O11.242 (4)
C12—C131.378 (5)C25—N31.337 (4)
C12—H120.9300N2—H2A0.9000
C13—C141.375 (4)N2—H2B0.9000
C13—H130.9300N3—S21.593 (3)
C14—N11.429 (4)O2—S21.435 (2)
C15—N11.468 (4)O3—S21.430 (2)
C15—C161.510 (5)
C2—C1—C6119.0 (3)N2—C16—H16A109.6
C2—C1—S1119.2 (3)C15—C16—H16A109.6
C6—C1—S1121.7 (2)N2—C16—H16B109.6
C1—C2—C3119.9 (4)C15—C16—H16B109.6
C1—C2—H2120.1H16A—C16—H16B108.2
C3—C2—H2120.1N2—C17—C18109.7 (3)
C4—C3—C2122.5 (4)N2—C17—H17A109.7
C4—C3—H3118.8C18—C17—H17A109.7
C2—C3—H3118.8N2—C17—H17B109.7
C3—C4—C5116.8 (3)C18—C17—H17B109.7
C3—C4—C7121.6 (4)H17A—C17—H17B108.2
C5—C4—C7121.6 (4)N1—C18—C17110.5 (2)
C4—C5—C6123.2 (4)N1—C18—H18A109.6
C4—C5—H5118.4C17—C18—H18A109.6
C6—C5—H5118.4N1—C18—H18B109.6
C1—C6—C5118.6 (3)C17—C18—H18B109.6
C1—C6—C8121.9 (3)H18A—C18—H18B108.1
C5—C6—C8119.4 (4)C24—C19—C20121.8 (3)
C4—C7—H7A109.5C24—C19—S2107.0 (2)
C4—C7—H7B109.5C20—C19—S2131.1 (3)
H7A—C7—H7B109.5C19—C20—C21117.0 (4)
C4—C7—H7C109.5C19—C20—H20121.5
H7A—C7—H7C109.5C21—C20—H20121.5
H7B—C7—H7C109.5C22—C21—C20121.6 (4)
C6—C8—H8A109.5C22—C21—H21119.2
C6—C8—H8B109.5C20—C21—H21119.2
H8A—C8—H8B109.5C21—C22—C23121.2 (4)
C6—C8—H8C109.5C21—C22—H22119.4
H8A—C8—H8C109.5C23—C22—H22119.4
H8B—C8—H8C109.5C22—C23—C24118.2 (4)
C10—C9—C14119.2 (3)C22—C23—H23120.9
C10—C9—S1123.6 (2)C24—C23—H23120.9
C14—C9—S1117.0 (2)C19—C24—C23120.2 (3)
C11—C10—C9120.9 (3)C19—C24—C25110.4 (3)
C11—C10—H10119.5C23—C24—C25129.5 (3)
C9—C10—H10119.5O1—C25—N3124.4 (3)
C12—C11—C10119.8 (3)O1—C25—C24121.7 (3)
C12—C11—H11120.1N3—C25—C24113.9 (3)
C10—C11—H11120.1C14—N1—C18112.2 (2)
C11—C12—C13119.9 (3)C14—N1—C15115.3 (2)
C11—C12—H12120.1C18—N1—C15109.7 (2)
C13—C12—H12120.1C16—N2—C17111.7 (2)
C14—C13—C12121.5 (3)C16—N2—H2A109.3
C14—C13—H13119.2C17—N2—H2A109.3
C12—C13—H13119.2C16—N2—H2B109.3
C13—C14—C9118.4 (3)C17—N2—H2B109.3
C13—C14—N1123.9 (3)H2A—N2—H2B107.9
C9—C14—N1117.7 (3)C25—N3—S2111.2 (2)
N1—C15—C16109.6 (3)C9—S1—C1102.86 (13)
N1—C15—H15A109.7O3—S2—O2114.91 (15)
C16—C15—H15A109.7O3—S2—N3112.03 (15)
N1—C15—H15B109.7O2—S2—N3110.15 (16)
C16—C15—H15B109.7O3—S2—C19109.94 (14)
H15A—C15—H15B108.2O2—S2—C19111.04 (14)
N2—C16—C15110.1 (3)N3—S2—C1997.43 (14)
C6—C1—C2—C30.8 (5)C20—C19—C24—C25180.0 (3)
S1—C1—C2—C3176.2 (3)S2—C19—C24—C250.7 (3)
C1—C2—C3—C40.7 (6)C22—C23—C24—C190.7 (4)
C2—C3—C4—C51.6 (6)C22—C23—C24—C25180.0 (3)
C2—C3—C4—C7178.6 (4)C19—C24—C25—O1178.0 (3)
C3—C4—C5—C61.0 (6)C23—C24—C25—O12.6 (5)
C7—C4—C5—C6179.2 (4)C19—C24—C25—N31.2 (3)
C2—C1—C6—C51.3 (5)C23—C24—C25—N3178.1 (3)
S1—C1—C6—C5176.6 (3)C13—C14—N1—C18102.0 (4)
C2—C1—C6—C8179.8 (4)C9—C14—N1—C1878.4 (3)
S1—C1—C6—C84.5 (5)C13—C14—N1—C1524.4 (4)
C4—C5—C6—C10.4 (6)C9—C14—N1—C15155.1 (3)
C4—C5—C6—C8179.3 (4)C17—C18—N1—C14169.2 (2)
C14—C9—C10—C112.5 (6)C17—C18—N1—C1561.3 (3)
S1—C9—C10—C11172.3 (3)C16—C15—N1—C14171.5 (3)
C9—C10—C11—C121.4 (7)C16—C15—N1—C1860.8 (3)
C10—C11—C12—C133.3 (7)C15—C16—N2—C1755.5 (3)
C11—C12—C13—C141.4 (7)C18—C17—N2—C1655.2 (3)
C12—C13—C14—C92.4 (6)O1—C25—N3—S2176.5 (3)
C12—C13—C14—N1178.0 (4)C24—C25—N3—S22.7 (3)
C10—C9—C14—C134.3 (5)C10—C9—S1—C111.1 (3)
S1—C9—C14—C13170.8 (3)C14—C9—S1—C1174.0 (2)
C10—C9—C14—N1176.1 (3)C2—C1—S1—C9104.0 (3)
S1—C9—C14—N18.8 (4)C6—C1—S1—C980.7 (3)
N1—C15—C16—N257.7 (3)C25—N3—S2—O3112.3 (2)
N2—C17—C18—N157.8 (3)C25—N3—S2—O2118.4 (2)
C24—C19—C20—C210.6 (5)C25—N3—S2—C192.7 (2)
S2—C19—C20—C21179.7 (3)C24—C19—S2—O3114.7 (2)
C19—C20—C21—C220.7 (6)C20—C19—S2—O364.4 (3)
C20—C21—C22—C230.8 (7)C24—C19—S2—O2117.0 (2)
C21—C22—C23—C240.8 (5)C20—C19—S2—O263.9 (3)
C20—C19—C24—C230.6 (4)C24—C19—S2—N32.0 (2)
S2—C19—C24—C23179.9 (2)C20—C19—S2—N3178.8 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2B···O10.901.932.815 (4)167
N2—H2A···O3i0.902.282.778 (3)115
Symmetry code: (i) x+1, y, z.
(5) top
Crystal data top
C18H23N2S·ClF(000) = 712
Mr = 334.89Dx = 1.213 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 10193 reflections
a = 16.9383 (8) Åθ = 3.1–27.4°
b = 6.5283 (3) ŵ = 0.32 mm1
c = 17.8173 (9) ÅT = 296 K
β = 111.406 (2)°Needle, colorless
V = 1834.30 (15) Å30.53 × 0.20 × 0.16 mm
Z = 4
Data collection top
Rigaku RAXIS-RAPID/ZJUG
diffractometer
4198 independent reflections
Radiation source: rotating anode2440 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.052
Detector resolution: 10.00 pixels mm-1θmax = 27.5°, θmin = 3.2°
ω scansh = 2121
Absorption correction: multi-scan
Higashi, T. (1995)
k = 88
Tmin = 0.848, Tmax = 0.951l = 2321
17262 measured 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)] = 0.049H-atom parameters constrained
wR(F2) = 0.138 w = 1/[σ2(Fo2) + (0.0414P)2 + 1.5518P]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max < 0.001
4198 reflectionsΔρmax = 0.41 e Å3
202 parametersΔρmin = 0.40 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0123 (13)
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
C10.57012 (19)0.0827 (5)0.4118 (2)0.0606 (8)
C20.5116 (2)0.1712 (6)0.3433 (2)0.0776 (10)
H20.52340.29700.32520.093*
C30.4362 (2)0.0730 (8)0.3021 (2)0.0946 (13)
H30.39730.13420.25640.113*
C40.4172 (3)0.1125 (8)0.3269 (3)0.0920 (13)
C50.4761 (2)0.1993 (6)0.3940 (3)0.0810 (11)
H50.46400.32620.41100.097*
C60.5529 (2)0.1065 (5)0.4378 (2)0.0638 (8)
C80.6149 (3)0.2103 (6)0.5111 (3)0.0982 (13)
H8A0.58660.31790.52810.147*
H8B0.63700.11210.55380.147*
H8C0.66060.26710.49810.147*
C70.3329 (3)0.2182 (10)0.2831 (3)0.161 (3)
H7A0.33830.36210.29510.241*
H7B0.31680.19870.22600.241*
H7C0.29020.16070.30040.241*
C90.74195 (17)0.1127 (4)0.43822 (17)0.0513 (7)
C100.72882 (19)0.0522 (5)0.38589 (18)0.0600 (8)
H100.67610.11580.36630.072*
C110.7935 (2)0.1231 (5)0.36255 (17)0.0587 (8)
H110.78420.23390.32760.070*
C120.8710 (2)0.0301 (5)0.39095 (18)0.0602 (8)
H120.91390.07540.37420.072*
C130.88576 (18)0.1316 (4)0.44464 (17)0.0555 (7)
H130.93900.19280.46430.067*
C140.82210 (17)0.2034 (4)0.46938 (15)0.0452 (6)
C150.89790 (19)0.5181 (4)0.52786 (18)0.0541 (7)
H15A0.88790.56490.47350.065*
H15B0.95390.45710.54940.065*
C160.89318 (19)0.6968 (4)0.57967 (18)0.0579 (7)
H16A0.93570.79790.58110.070*
H16B0.83780.76080.55700.070*
C170.8468 (2)0.4604 (4)0.66285 (19)0.0578 (7)
H17A0.78980.51610.64440.069*
H17B0.86040.40890.71720.069*
C180.85121 (19)0.2890 (4)0.60819 (16)0.0512 (7)
H18A0.90700.22660.62920.061*
H18B0.80970.18490.60650.061*
Cl10.90598 (5)0.97548 (10)0.77657 (4)0.0560 (2)
N10.83447 (13)0.3666 (3)0.52639 (12)0.0452 (5)
N20.90794 (14)0.6239 (3)0.66270 (14)0.0539 (6)
H2A0.90280.72990.69290.065*
H2B0.96110.57510.68500.065*
S10.66188 (5)0.22723 (15)0.46592 (7)0.0816 (3)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0512 (17)0.0638 (19)0.069 (2)0.0003 (15)0.0244 (16)0.0162 (16)
C20.066 (2)0.090 (2)0.080 (2)0.003 (2)0.030 (2)0.004 (2)
C30.058 (2)0.151 (4)0.068 (2)0.005 (3)0.0151 (19)0.010 (3)
C40.065 (2)0.132 (4)0.086 (3)0.028 (3)0.035 (2)0.050 (3)
C50.086 (3)0.076 (2)0.100 (3)0.023 (2)0.056 (3)0.029 (2)
C60.0653 (19)0.0641 (19)0.066 (2)0.0023 (16)0.0291 (17)0.0148 (16)
C80.124 (3)0.084 (3)0.094 (3)0.026 (3)0.047 (3)0.004 (2)
C70.081 (3)0.244 (7)0.156 (5)0.071 (4)0.043 (3)0.108 (5)
C90.0503 (15)0.0513 (15)0.0516 (16)0.0027 (13)0.0176 (13)0.0077 (13)
C100.0561 (17)0.0610 (17)0.0592 (18)0.0014 (14)0.0164 (15)0.0138 (15)
C110.070 (2)0.0585 (17)0.0477 (17)0.0087 (16)0.0219 (15)0.0063 (14)
C120.0662 (19)0.0663 (18)0.0569 (18)0.0070 (16)0.0330 (16)0.0010 (15)
C130.0534 (16)0.0589 (17)0.0589 (18)0.0013 (14)0.0262 (15)0.0025 (15)
C140.0502 (15)0.0439 (14)0.0401 (14)0.0013 (12)0.0149 (12)0.0041 (11)
C150.0628 (17)0.0478 (15)0.0540 (17)0.0067 (13)0.0241 (15)0.0078 (13)
C160.0598 (18)0.0435 (15)0.067 (2)0.0051 (13)0.0184 (15)0.0053 (14)
C170.0656 (18)0.0536 (16)0.0582 (18)0.0076 (14)0.0272 (15)0.0059 (14)
C180.0660 (18)0.0436 (14)0.0464 (16)0.0083 (13)0.0234 (14)0.0012 (12)
Cl10.0581 (4)0.0510 (4)0.0603 (5)0.0035 (3)0.0232 (3)0.0017 (3)
N10.0493 (12)0.0414 (11)0.0451 (13)0.0045 (10)0.0173 (10)0.0005 (10)
N20.0517 (13)0.0446 (12)0.0605 (15)0.0012 (11)0.0147 (12)0.0086 (11)
S10.0530 (5)0.0816 (6)0.1120 (8)0.0080 (4)0.0323 (5)0.0489 (6)
Geometric parameters (Å, º) top
C1—C61.386 (5)C11—C121.364 (4)
C1—C21.387 (5)C11—H110.9300
C1—S11.772 (3)C12—C131.385 (4)
C2—C31.378 (5)C12—H120.9300
C2—H20.9300C13—C141.387 (4)
C3—C41.367 (6)C13—H130.9300
C3—H30.9300C14—N11.434 (3)
C4—C51.369 (6)C15—N11.453 (3)
C4—C71.521 (5)C15—C161.508 (4)
C5—C61.390 (5)C15—H15A0.9700
C5—H50.9300C15—H15B0.9700
C6—C81.505 (5)C16—N21.486 (4)
C8—H8A0.9600C16—H16A0.9700
C8—H8B0.9600C16—H16B0.9700
C8—H8C0.9600C17—N21.488 (3)
C7—H7A0.9600C17—C181.503 (4)
C7—H7B0.9600C17—H17A0.9700
C7—H7C0.9600C17—H17B0.9700
C9—C101.388 (4)C18—N11.470 (3)
C9—C141.397 (4)C18—H18A0.9700
C9—S11.769 (3)C18—H18B0.9700
C10—C111.386 (4)N2—H2A0.9000
C10—H100.9300N2—H2B0.9000
C6—C1—C2119.7 (3)C13—C12—H12119.9
C6—C1—S1122.8 (3)C12—C13—C14120.8 (3)
C2—C1—S1117.4 (3)C12—C13—H13119.6
C3—C2—C1120.0 (4)C14—C13—H13119.6
C3—C2—H2120.0C13—C14—C9119.1 (2)
C1—C2—H2120.0C13—C14—N1123.1 (2)
C4—C3—C2121.4 (4)C9—C14—N1117.8 (2)
C4—C3—H3119.3N1—C15—C16109.5 (2)
C2—C3—H3119.3N1—C15—H15A109.8
C3—C4—C5117.8 (4)C16—C15—H15A109.8
C3—C4—C7121.6 (5)N1—C15—H15B109.8
C5—C4—C7120.6 (5)C16—C15—H15B109.8
C4—C5—C6123.0 (4)H15A—C15—H15B108.2
C4—C5—H5118.5N2—C16—C15109.5 (2)
C6—C5—H5118.5N2—C16—H16A109.8
C1—C6—C5117.9 (3)C15—C16—H16A109.8
C1—C6—C8121.7 (3)N2—C16—H16B109.8
C5—C6—C8120.3 (4)C15—C16—H16B109.8
C6—C8—H8A109.5H16A—C16—H16B108.2
C6—C8—H8B109.5N2—C17—C18109.5 (2)
H7A—C8—H8B109.5N2—C17—H17A109.8
C6—C8—H8C109.5C18—C17—H17A109.8
H7A—C8—H8C109.5N2—C17—H17B109.8
H7B—C8—H8C109.5C18—C17—H17B109.8
C4—C7—H7A109.5H17A—C17—H17B108.2
C4—C7—H7B109.5N1—C18—C17110.4 (2)
H8A—C7—H7B109.5N1—C18—H18A109.6
C4—C7—H7C109.5C17—C18—H18A109.6
H8A—C7—H7C109.5N1—C18—H18B109.6
H8B—C7—H7C109.5C17—C18—H18B109.6
C10—C9—C14119.3 (2)H18A—C18—H18B108.1
C10—C9—S1124.3 (2)C14—N1—C15115.7 (2)
C14—C9—S1116.3 (2)C14—N1—C18111.84 (19)
C11—C10—C9120.7 (3)C15—N1—C18110.1 (2)
C11—C10—H10119.7C16—N2—C17111.5 (2)
C9—C10—H10119.7C16—N2—H2A109.3
C12—C11—C10119.9 (3)C17—N2—H2A109.3
C12—C11—H11120.0C16—N2—H2B109.3
C10—C11—H11120.0C17—N2—H2B109.3
C11—C12—C13120.2 (3)H2A—N2—H2B108.0
C11—C12—H12119.9C9—S1—C1103.46 (13)
C6—C1—C2—C31.1 (5)C10—C9—C14—C132.6 (4)
S1—C1—C2—C3175.2 (3)S1—C9—C14—C13174.7 (2)
C1—C2—C3—C40.3 (6)C10—C9—C14—N1176.9 (2)
C2—C3—C4—C50.6 (6)S1—C9—C14—N15.8 (3)
C2—C3—C4—C7178.1 (4)N1—C15—C16—N259.1 (3)
C3—C4—C5—C60.8 (5)N2—C17—C18—N156.9 (3)
C7—C4—C5—C6177.9 (3)C13—C14—N1—C1529.4 (3)
C2—C1—C6—C50.9 (4)C9—C14—N1—C15151.1 (2)
S1—C1—C6—C5175.2 (2)C13—C14—N1—C1897.7 (3)
C2—C1—C6—C8179.1 (3)C9—C14—N1—C1881.8 (3)
S1—C1—C6—C84.8 (4)C16—C15—N1—C14170.4 (2)
C4—C5—C6—C10.0 (5)C16—C15—N1—C1861.6 (3)
C4—C5—C6—C8180.0 (3)C17—C18—N1—C14168.8 (2)
C14—C9—C10—C112.0 (4)C17—C18—N1—C1561.0 (3)
S1—C9—C10—C11175.1 (2)C15—C16—N2—C1756.5 (3)
C9—C10—C11—C120.2 (5)C18—C17—N2—C1655.3 (3)
C10—C11—C12—C131.6 (5)C10—C9—S1—C10.2 (3)
C11—C12—C13—C141.0 (4)C14—C9—S1—C1176.9 (2)
C12—C13—C14—C91.2 (4)C6—C1—S1—C980.6 (3)
C12—C13—C14—N1178.3 (2)C2—C1—S1—C9103.2 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···Cl10.902.183.072 (2)173
N2—H2B···Cl1i0.902.203.091 (2)171
Symmetry code: (i) x+2, y1/2, z+3/2.
(6) top
Crystal data top
C36H45N4S2·ClF(000) = 676
Mr = 633.33Dx = 1.223 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 9413 reflections
a = 20.9755 (12) Åθ = 3.2–27.5°
b = 7.7160 (4) ŵ = 0.26 mm1
c = 10.6432 (7) ÅT = 296 K
β = 93.067 (2)°Platelet, colorless
V = 1720.10 (17) Å30.50 × 0.38 × 0.10 mm
Z = 2
Data collection top
Rigaku RAXIS-RAPID/ZJUG
diffractometer
3028 independent reflections
Radiation source: rotating anode1917 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.047
Detector resolution: 10.00 pixels mm-1θmax = 25.0°, θmin = 3.3°
ω scansh = 2424
Absorption correction: multi-scan
Higashi, T. (1995)
k = 98
Tmin = 0.860, Tmax = 0.974l = 1212
13112 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.097Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.296H-atom parameters constrained
S = 1.00 w = 1/[σ2(Fo2) + (0.1424P)2 + 4.1586P]
where P = (Fo2 + 2Fc2)/3
3028 reflections(Δ/σ)max < 0.001
199 parametersΔρmax = 0.85 e Å3
0 restraintsΔρmin = 0.69 e Å3
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*/UeqOcc. (<1)
C10.3373 (3)0.4608 (7)0.2359 (7)0.0688 (16)
C20.3646 (3)0.4408 (10)0.1257 (8)0.090 (2)
H20.33950.44260.05090.108*
C30.4308 (4)0.4171 (10)0.1229 (9)0.093 (2)
H30.44840.40600.04500.112*
C40.4698 (3)0.4095 (8)0.2261 (9)0.089 (2)
C50.4410 (4)0.4292 (10)0.3398 (8)0.097 (2)
H50.46630.42500.41410.116*
C60.3739 (4)0.4558 (8)0.3467 (7)0.086 (2)
C70.5410 (3)0.3894 (12)0.2199 (12)0.131 (4)
H7A0.55040.33140.14320.197*
H7B0.55730.32230.29050.197*
H7C0.56080.50170.22200.197*
C80.3466 (6)0.4830 (15)0.4709 (9)0.148 (4)
H8A0.35550.59910.49910.222*
H8B0.36530.40210.53060.222*
H8C0.30120.46550.46330.222*
C90.2415 (2)0.6928 (7)0.2894 (6)0.0601 (14)
C100.2817 (3)0.8262 (7)0.2524 (7)0.0733 (18)
H100.31590.80160.20340.088*
C110.2703 (3)0.9928 (7)0.2887 (6)0.0703 (17)
H110.29881.08020.26970.084*
C120.2180 (3)1.0312 (7)0.3520 (7)0.0745 (18)
H120.20901.14600.37100.089*
C130.1777 (3)0.9010 (7)0.3887 (6)0.0671 (16)
H130.14230.92850.43400.081*
C140.1895 (2)0.7315 (6)0.3588 (5)0.0471 (11)
C150.0944 (3)0.5618 (7)0.3111 (5)0.0563 (13)
H15A0.10680.56190.22470.068*
H15B0.06380.65470.32060.068*
C160.0640 (3)0.3904 (7)0.3407 (5)0.0665 (16)
H16A0.02560.37430.28690.080*
H16B0.09320.29690.32410.080*
C170.1038 (3)0.4226 (7)0.5594 (5)0.0636 (15)
H17A0.13560.33260.55180.076*
H17B0.09120.42430.64580.076*
C180.1317 (3)0.5956 (7)0.5267 (5)0.0579 (14)
H18A0.10050.68660.53720.069*
H18B0.16890.62000.58200.069*
Cl10.00000.00000.50000.0784 (8)
N10.14994 (18)0.5905 (5)0.3953 (4)0.0473 (10)
N20.04764 (19)0.3850 (5)0.4740 (4)0.0518 (11)
H2A0.03230.27940.49180.062*
H2B0.01680.46320.48680.062*0.50
S10.25296 (8)0.4753 (2)0.2394 (2)0.0927 (8)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.070 (4)0.043 (3)0.096 (5)0.000 (3)0.021 (4)0.001 (3)
C20.079 (4)0.091 (5)0.100 (5)0.009 (4)0.023 (4)0.007 (4)
C30.070 (4)0.098 (5)0.113 (6)0.004 (4)0.033 (4)0.018 (5)
C40.069 (4)0.055 (4)0.145 (7)0.010 (3)0.022 (5)0.007 (4)
C50.103 (6)0.075 (4)0.111 (6)0.013 (4)0.006 (5)0.005 (4)
C60.125 (6)0.054 (3)0.082 (5)0.013 (4)0.037 (5)0.002 (3)
C70.064 (4)0.099 (6)0.232 (12)0.013 (4)0.019 (6)0.006 (7)
C80.206 (12)0.153 (10)0.087 (6)0.048 (8)0.028 (7)0.023 (6)
C90.044 (3)0.044 (3)0.094 (4)0.006 (2)0.015 (3)0.008 (3)
C100.052 (3)0.049 (3)0.122 (5)0.009 (3)0.028 (3)0.011 (3)
C110.057 (3)0.044 (3)0.111 (5)0.012 (2)0.015 (3)0.013 (3)
C120.078 (4)0.035 (3)0.113 (5)0.003 (3)0.027 (4)0.002 (3)
C130.063 (3)0.045 (3)0.096 (4)0.004 (3)0.023 (3)0.002 (3)
C140.040 (2)0.043 (2)0.058 (3)0.007 (2)0.001 (2)0.008 (2)
C150.061 (3)0.064 (3)0.044 (3)0.023 (3)0.002 (2)0.000 (2)
C160.069 (3)0.059 (3)0.074 (4)0.025 (3)0.017 (3)0.021 (3)
C170.062 (3)0.063 (3)0.066 (3)0.005 (3)0.003 (3)0.025 (3)
C180.054 (3)0.068 (3)0.050 (3)0.018 (3)0.009 (2)0.012 (3)
Cl10.0846 (15)0.0365 (9)0.1119 (18)0.0070 (9)0.0157 (13)0.0063 (10)
N10.043 (2)0.043 (2)0.057 (2)0.0105 (17)0.0058 (18)0.0067 (18)
N20.051 (2)0.035 (2)0.072 (3)0.0098 (17)0.017 (2)0.0039 (19)
S10.0693 (11)0.0543 (10)0.158 (2)0.0122 (7)0.0375 (11)0.0158 (10)
Geometric parameters (Å, º) top
C1—C21.341 (9)C11—C121.351 (8)
C1—C61.373 (10)C11—H110.9300
C1—S11.776 (6)C12—C131.383 (8)
C2—C31.402 (10)C12—H120.9300
C2—H20.9300C13—C141.372 (7)
C3—C41.336 (11)C13—H130.9300
C3—H30.9300C14—N11.433 (6)
C4—C51.389 (11)C15—N11.449 (6)
C4—C71.507 (10)C15—C161.509 (7)
C5—C61.428 (11)C15—H15A0.9700
C5—H50.9300C15—H15B0.9700
C6—C81.483 (11)C16—N21.478 (7)
C7—H7A0.9600C16—H16A0.9700
C7—H7B0.9600C16—H16B0.9700
C7—H7C0.9600C17—N21.477 (7)
C8—H8A0.9600C17—C181.506 (7)
C8—H8B0.9600C17—H17A0.9700
C8—H8C0.9600C17—H17B0.9700
C9—C141.383 (7)C18—N11.470 (6)
C9—C101.400 (7)C18—H18A0.9700
C9—S11.781 (6)C18—H18B0.9700
C10—C111.367 (8)N2—H2A0.9000
C10—H100.9300N2—H2B0.9000
C2—C1—C6120.2 (7)C13—C12—H12119.8
C2—C1—S1119.9 (6)C14—C13—C12120.4 (5)
C6—C1—S1119.7 (5)C14—C13—H13119.8
C1—C2—C3120.2 (8)C12—C13—H13119.8
C1—C2—H2119.9C13—C14—C9119.1 (4)
C3—C2—H2119.9C13—C14—N1123.1 (4)
C4—C3—C2123.5 (7)C9—C14—N1117.8 (4)
C4—C3—H3118.3N1—C15—C16109.9 (4)
C2—C3—H3118.3N1—C15—H15A109.7
C3—C4—C5115.8 (7)C16—C15—H15A109.7
C3—C4—C7122.2 (9)N1—C15—H15B109.7
C5—C4—C7121.9 (9)C16—C15—H15B109.7
C4—C5—C6122.5 (8)H15A—C15—H15B108.2
C4—C5—H5118.8N2—C16—C15110.3 (4)
C6—C5—H5118.8N2—C16—H16A109.6
C1—C6—C5117.8 (6)C15—C16—H16A109.6
C1—C6—C8122.5 (8)N2—C16—H16B109.6
C5—C6—C8119.7 (9)C15—C16—H16B109.6
C4—C7—H7A109.5H16A—C16—H16B108.1
C4—C7—H7B109.5N2—C17—C18109.8 (4)
H7A—C7—H7B109.5N2—C17—H17A109.7
C4—C7—H7C109.5C18—C17—H17A109.7
H7A—C7—H7C109.5N2—C17—H17B109.7
H7B—C7—H7C109.5C18—C17—H17B109.7
C6—C8—H8A109.5H17A—C17—H17B108.2
C6—C8—H8B109.5N1—C18—C17108.7 (4)
H8A—C8—H8B109.5N1—C18—H18A109.9
C6—C8—H8C109.5C17—C18—H18A109.9
H8A—C8—H8C109.5N1—C18—H18B109.9
H8B—C8—H8C109.5C17—C18—H18B109.9
C14—C9—C10119.7 (5)H18A—C18—H18B108.3
C14—C9—S1119.1 (4)C14—N1—C15114.0 (4)
C10—C9—S1121.1 (4)C14—N1—C18114.9 (4)
C11—C10—C9119.7 (5)C15—N1—C18110.5 (4)
C11—C10—H10120.1C16—N2—C17111.6 (4)
C9—C10—H10120.1C16—N2—H2A109.3
C12—C11—C10120.4 (5)C17—N2—H2A109.3
C12—C11—H11119.8C16—N2—H2B109.3
C10—C11—H11119.8C17—N2—H2B109.3
C11—C12—C13120.4 (5)H2A—N2—H2B108.0
C11—C12—H12119.8C1—S1—C9102.5 (3)
C6—C1—C2—C30.9 (10)C10—C9—C14—C130.9 (9)
S1—C1—C2—C3175.5 (6)S1—C9—C14—C13174.8 (5)
C1—C2—C3—C41.3 (12)C10—C9—C14—N1179.6 (5)
C2—C3—C4—C50.9 (11)S1—C9—C14—N14.7 (7)
C2—C3—C4—C7178.1 (7)N1—C15—C16—N256.5 (6)
C3—C4—C5—C60.1 (11)N2—C17—C18—N158.9 (6)
C7—C4—C5—C6177.3 (7)C13—C14—N1—C1583.8 (6)
C2—C1—C6—C50.1 (9)C9—C14—N1—C1595.6 (6)
S1—C1—C6—C5174.8 (5)C13—C14—N1—C1845.2 (7)
C2—C1—C6—C8177.9 (8)C9—C14—N1—C18135.3 (5)
S1—C1—C6—C87.5 (9)C16—C15—N1—C14167.9 (4)
C4—C5—C6—C10.3 (11)C16—C15—N1—C1860.9 (6)
C4—C5—C6—C8177.5 (8)C17—C18—N1—C14167.2 (4)
C14—C9—C10—C112.1 (10)C17—C18—N1—C1562.1 (5)
S1—C9—C10—C11177.7 (5)C15—C16—N2—C1754.8 (6)
C9—C10—C11—C124.9 (11)C18—C17—N2—C1656.4 (6)
C10—C11—C12—C134.6 (11)C2—C1—S1—C9113.1 (6)
C11—C12—C13—C141.5 (11)C6—C1—S1—C972.2 (5)
C12—C13—C14—C91.2 (9)C14—C9—S1—C1149.6 (5)
C12—C13—C14—N1179.3 (6)C10—C9—S1—C134.8 (6)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···Cl10.902.263.151 (4)169
(7) top
Crystal data top
C18H23N2S·BrF(000) = 784
Mr = 379.35Dx = 1.373 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 9477 reflections
a = 13.0982 (8) Åθ = 3.0–27.8°
b = 18.2551 (9) ŵ = 2.35 mm1
c = 7.8088 (4) ÅT = 296 K
β = 100.698 (2)°Platelet, colorless
V = 1834.70 (17) Å30.50 × 0.48 × 0.16 mm
Z = 4
Data collection top
Rigaku RAXIS-RAPID/ZJUG
diffractometer
4179 independent reflections
Radiation source: rotating anode2317 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.078
Detector resolution: 10.00 pixels mm-1θmax = 27.5°, θmin = 3.0°
ω scansh = 1716
Absorption correction: multi-scan
Higashi, T. (1995)
k = 2323
Tmin = 0.306, Tmax = 0.695l = 109
17291 measured 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)] = 0.049H-atom parameters constrained
wR(F2) = 0.149 w = 1/[σ2(Fo2) + (0.0579P)2 + 1.5412P]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max < 0.001
4179 reflectionsΔρmax = 0.53 e Å3
200 parametersΔρmin = 0.80 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0122 (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
C10.1502 (3)0.5710 (2)0.1072 (5)0.0510 (10)
C20.1862 (4)0.5949 (3)0.0389 (6)0.0599 (12)
H20.25410.58460.05050.072*
C30.1227 (5)0.6339 (3)0.1668 (6)0.0727 (15)
H30.14870.65000.26330.087*
C40.0220 (5)0.6496 (3)0.1550 (7)0.0726 (15)
C50.0134 (4)0.6242 (3)0.0103 (7)0.0668 (13)
H50.08200.63380.00140.080*
C60.0478 (4)0.5854 (2)0.1220 (6)0.0562 (11)
C70.0483 (6)0.6927 (4)0.2942 (9)0.125 (3)
H7A0.01120.70540.38510.188*
H7B0.07060.73660.24420.188*
H7C0.10790.66360.34180.188*
C80.0038 (4)0.5598 (3)0.2785 (7)0.0857 (17)
H8A0.05640.53380.35730.129*
H8B0.05430.52800.24030.129*
H8C0.01850.60150.33690.129*
C90.2796 (3)0.5848 (2)0.4300 (5)0.0472 (10)
C100.2591 (4)0.6596 (2)0.4136 (6)0.0534 (11)
H100.21350.67710.31650.064*
C110.3056 (4)0.7080 (2)0.5399 (6)0.0570 (11)
H110.29020.75770.52850.068*
C120.3744 (4)0.6833 (2)0.6819 (6)0.0595 (12)
H120.40800.71630.76400.071*
C130.3936 (3)0.6089 (2)0.7027 (5)0.0502 (10)
H130.43960.59230.80030.060*
C140.3453 (3)0.5590 (2)0.5807 (5)0.0448 (9)
C150.2728 (3)0.4420 (2)0.6412 (6)0.0513 (10)
H15A0.20870.46060.57240.062*
H15B0.27030.44910.76340.062*
C160.2840 (4)0.3618 (2)0.6043 (6)0.0551 (11)
H16A0.22600.33490.63440.066*
H16B0.28350.35470.48100.066*
C170.4729 (4)0.3762 (2)0.6742 (6)0.0598 (12)
H17A0.48140.36940.55440.072*
H17B0.53540.35890.75000.072*
C180.4572 (3)0.4568 (2)0.7082 (6)0.0514 (10)
H18A0.45250.46410.82950.062*
H18B0.51590.48480.68410.062*
N10.3621 (3)0.48179 (17)0.5965 (4)0.0453 (8)
N20.3821 (3)0.33361 (16)0.7066 (5)0.0516 (9)
H2A0.38990.28640.67860.062*
H2B0.37920.33570.82080.062*
S10.23556 (10)0.51918 (6)0.26458 (15)0.0617 (4)
Br10.33920 (4)0.16416 (2)0.60005 (6)0.0657 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.051 (3)0.049 (2)0.052 (2)0.0055 (19)0.008 (2)0.0034 (19)
C20.053 (3)0.073 (3)0.055 (3)0.008 (2)0.013 (2)0.006 (2)
C30.080 (4)0.085 (4)0.051 (3)0.023 (3)0.007 (3)0.003 (3)
C40.076 (4)0.064 (3)0.069 (3)0.008 (3)0.010 (3)0.003 (3)
C50.048 (3)0.066 (3)0.082 (3)0.000 (2)0.003 (3)0.006 (3)
C60.054 (3)0.054 (2)0.062 (3)0.011 (2)0.015 (2)0.006 (2)
C70.135 (7)0.122 (5)0.096 (5)0.014 (5)0.036 (5)0.030 (4)
C80.077 (4)0.103 (4)0.087 (4)0.011 (3)0.041 (3)0.009 (3)
C90.052 (3)0.042 (2)0.050 (2)0.0002 (18)0.0139 (19)0.0009 (18)
C100.060 (3)0.044 (2)0.058 (3)0.003 (2)0.016 (2)0.003 (2)
C110.070 (3)0.037 (2)0.068 (3)0.000 (2)0.023 (2)0.004 (2)
C120.066 (3)0.050 (2)0.065 (3)0.009 (2)0.016 (2)0.009 (2)
C130.055 (3)0.047 (2)0.049 (2)0.0063 (19)0.011 (2)0.0054 (19)
C140.044 (3)0.040 (2)0.053 (2)0.0010 (17)0.0167 (19)0.0017 (18)
C150.046 (3)0.044 (2)0.067 (3)0.0007 (18)0.016 (2)0.007 (2)
C160.053 (3)0.047 (2)0.065 (3)0.006 (2)0.010 (2)0.006 (2)
C170.051 (3)0.052 (2)0.079 (3)0.006 (2)0.020 (2)0.007 (2)
C180.045 (3)0.046 (2)0.064 (3)0.0002 (19)0.012 (2)0.005 (2)
N10.041 (2)0.0401 (17)0.0548 (19)0.0016 (14)0.0079 (16)0.0040 (15)
N20.058 (2)0.0383 (17)0.060 (2)0.0012 (16)0.0146 (18)0.0007 (15)
S10.0743 (9)0.0451 (6)0.0621 (7)0.0059 (5)0.0031 (6)0.0061 (5)
Br10.0868 (5)0.0515 (3)0.0608 (3)0.0061 (2)0.0191 (3)0.0025 (2)
Geometric parameters (Å, º) top
C1—C21.384 (6)C11—C121.368 (7)
C1—C61.392 (6)C11—H110.9300
C1—S11.773 (4)C12—C131.386 (6)
C2—C31.374 (7)C12—H120.9300
C2—H20.9300C13—C141.384 (6)
C3—C41.369 (8)C13—H130.9300
C3—H30.9300C14—N11.428 (5)
C4—C51.379 (7)C15—N11.474 (5)
C4—C71.510 (8)C15—C161.506 (5)
C5—C61.381 (7)C15—H15A0.9700
C5—H50.9300C15—H15B0.9700
C6—C81.518 (6)C16—N21.473 (6)
C7—H7A0.9600C16—H16A0.9700
C7—H7B0.9600C16—H16B0.9700
C7—H7C0.9600C17—N21.482 (5)
C8—H8A0.9600C17—C181.515 (6)
C8—H8B0.9600C17—H17A0.9700
C8—H8C0.9600C17—H17B0.9700
C9—C101.394 (5)C18—N11.455 (5)
C9—C141.404 (6)C18—H18A0.9700
C9—S11.777 (4)C18—H18B0.9700
C10—C111.379 (6)N2—H2A0.9000
C10—H100.9300N2—H2B0.9000
C2—C1—C6119.3 (4)C13—C12—H12120.1
C2—C1—S1118.2 (4)C14—C13—C12121.0 (4)
C6—C1—S1122.5 (3)C14—C13—H13119.5
C3—C2—C1120.7 (5)C12—C13—H13119.5
C3—C2—H2119.7C13—C14—C9119.1 (4)
C1—C2—H2119.7C13—C14—N1123.1 (4)
C4—C3—C2121.3 (5)C9—C14—N1117.7 (3)
C4—C3—H3119.4N1—C15—C16108.9 (3)
C2—C3—H3119.4N1—C15—H15A109.9
C3—C4—C5117.4 (5)C16—C15—H15A109.9
C3—C4—C7121.8 (6)N1—C15—H15B109.9
C5—C4—C7120.8 (6)C16—C15—H15B109.9
C4—C5—C6123.2 (5)H15A—C15—H15B108.3
C4—C5—H5118.4N2—C16—C15110.0 (4)
C6—C5—H5118.4N2—C16—H16A109.7
C5—C6—C1118.0 (4)C15—C16—H16A109.7
C5—C6—C8120.4 (5)N2—C16—H16B109.7
C1—C6—C8121.6 (4)C15—C16—H16B109.7
C4—C7—H7A109.5H16A—C16—H16B108.2
C4—C7—H7B109.5N2—C17—C18109.9 (3)
H7A—C7—H7B109.5N2—C17—H17A109.7
C4—C7—H7C109.5C18—C17—H17A109.7
H7A—C7—H7C109.5N2—C17—H17B109.7
H7B—C7—H7C109.5C18—C17—H17B109.7
C6—C8—H8A109.5H17A—C17—H17B108.2
C6—C8—H8B109.5N1—C18—C17109.1 (3)
H8A—C8—H8B109.5N1—C18—H18A109.9
C6—C8—H8C109.5C17—C18—H18A109.9
H8A—C8—H8C109.5N1—C18—H18B109.9
H8B—C8—H8C109.5C17—C18—H18B109.9
C10—C9—C14118.9 (4)H18A—C18—H18B108.3
C10—C9—S1124.2 (3)C14—N1—C18117.5 (3)
C14—C9—S1116.7 (3)C14—N1—C15113.0 (3)
C11—C10—C9120.7 (4)C18—N1—C15109.5 (3)
C11—C10—H10119.7C16—N2—C17111.8 (3)
C9—C10—H10119.7C16—N2—H2A109.3
C12—C11—C10120.4 (4)C17—N2—H2A109.3
C12—C11—H11119.8C16—N2—H2B109.3
C10—C11—H11119.8C17—N2—H2B109.3
C11—C12—C13119.7 (4)H2A—N2—H2B107.9
C11—C12—H12120.1C1—S1—C9102.85 (19)
C6—C1—C2—C31.4 (7)C10—C9—C14—C134.5 (6)
S1—C1—C2—C3178.6 (4)S1—C9—C14—C13171.0 (3)
C1—C2—C3—C40.7 (8)C10—C9—C14—N1177.9 (3)
C2—C3—C4—C50.4 (8)S1—C9—C14—N16.5 (5)
C2—C3—C4—C7179.6 (5)N1—C15—C16—N258.7 (5)
C3—C4—C5—C60.9 (8)N2—C17—C18—N158.1 (5)
C7—C4—C5—C6179.1 (5)C13—C14—N1—C1821.6 (5)
C4—C5—C6—C10.3 (7)C9—C14—N1—C18155.8 (4)
C4—C5—C6—C8179.4 (5)C13—C14—N1—C15107.3 (4)
C2—C1—C6—C50.9 (6)C9—C14—N1—C1575.3 (4)
S1—C1—C6—C5178.0 (3)C17—C18—N1—C14166.6 (3)
C2—C1—C6—C8179.4 (4)C17—C18—N1—C1562.8 (4)
S1—C1—C6—C82.3 (6)C16—C15—N1—C14163.7 (3)
C14—C9—C10—C112.5 (6)C16—C15—N1—C1863.2 (4)
S1—C9—C10—C11172.7 (3)C15—C16—N2—C1755.5 (5)
C9—C10—C11—C121.2 (7)C18—C17—N2—C1654.9 (5)
C10—C11—C12—C133.0 (7)C2—C1—S1—C9101.2 (4)
C11—C12—C13—C140.9 (6)C6—C1—S1—C981.7 (4)
C12—C13—C14—C92.9 (6)C10—C9—S1—C18.3 (4)
C12—C13—C14—N1179.8 (4)C14—C9—S1—C1176.4 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···Br10.902.383.225 (3)157
N2—H2B···Br1i0.902.343.224 (4)169
Symmetry code: (i) x, y+1/2, z+1/2.
(8) top
Crystal data top
C36H45N4S2·BrF(000) = 712
Mr = 677.79Dx = 1.284 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 8791 reflections
a = 21.1781 (12) Åθ = 3.2–27.4°
b = 7.8799 (4) ŵ = 1.32 mm1
c = 10.5126 (8) ÅT = 296 K
β = 87.993 (2)°Chunk, colorless
V = 1753.28 (19) Å30.50 × 0.36 × 0.30 mm
Z = 2
Data collection top
Rigaku RAXIS-RAPID/ZJUG
diffractometer
3126 independent reflections
Radiation source: rotating anode1927 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.045
Detector resolution: 10.00 pixels mm-1θmax = 25.1°, θmin = 3.2°
ω scansh = 2525
Absorption correction: multi-scan
Higashi, T. (1995)
k = 98
Tmin = 0.508, Tmax = 0.683l = 1212
13386 measured 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)] = 0.092H-atom parameters constrained
wR(F2) = 0.287 w = 1/[σ2(Fo2) + (0.1501P)2 + 4.4364P]
where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max < 0.001
3126 reflectionsΔρmax = 2.02 e Å3
199 parametersΔρmin = 0.99 e Å3
0 restraintsExtinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.023 (4)
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*/UeqOcc. (<1)
C10.3387 (4)0.4586 (10)0.2423 (10)0.083 (2)
C20.3653 (5)0.4366 (15)0.1301 (11)0.110 (3)
H20.34180.43810.05710.132*
C30.4304 (5)0.4107 (15)0.1234 (13)0.119 (4)
H30.44930.39610.04300.143*
C40.4698 (5)0.4049 (11)0.2279 (12)0.103 (3)
C50.4416 (5)0.4239 (14)0.3416 (12)0.115 (3)
H50.46490.41950.41490.139*
C60.3739 (5)0.4515 (12)0.3503 (10)0.102 (3)
C70.5398 (4)0.3808 (16)0.2170 (15)0.152 (5)
H7A0.56020.48950.21250.228*
H7B0.55050.31710.14140.228*
H7C0.55370.32020.29010.228*
C80.3465 (9)0.483 (2)0.4786 (13)0.179 (7)
H8A0.34780.60220.49660.268*
H8B0.37040.42250.54000.268*
H8C0.30350.44430.48290.268*
C90.2445 (3)0.6879 (9)0.2971 (8)0.078 (2)
C100.2838 (3)0.8175 (10)0.2569 (10)0.097 (3)
H100.31890.79130.20490.116*
C110.2736 (4)0.9829 (8)0.2899 (10)0.086 (2)
H110.30241.06640.26490.103*
C120.2217 (4)1.0228 (9)0.3585 (9)0.084 (2)
H120.21311.13540.37950.101*
C130.1810 (3)0.8971 (9)0.3977 (7)0.0728 (19)
H130.14470.92550.44510.087*
C140.1926 (3)0.7298 (7)0.3688 (6)0.0547 (14)
C150.1001 (3)0.5579 (10)0.3197 (6)0.0665 (17)
H15A0.06850.64680.32730.080*
H15B0.11660.55620.23250.080*
C160.0706 (3)0.3908 (9)0.3518 (7)0.074 (2)
H16A0.03480.37120.29870.089*
H16B0.10100.30030.33650.089*
C170.1026 (3)0.4369 (9)0.5743 (7)0.0699 (18)
H17A0.08560.44160.66120.084*
H17B0.13500.35000.56970.084*
C180.1306 (3)0.6051 (8)0.5378 (6)0.0613 (16)
H18A0.09910.69390.54760.074*
H18B0.16550.63180.59180.074*
N10.1525 (2)0.5935 (6)0.4078 (5)0.0563 (13)
N20.0500 (2)0.3922 (6)0.4846 (5)0.0640 (15)
H2A0.03440.28930.50560.077*0.50
H2B0.02380.46230.49520.077*
S10.25476 (12)0.4743 (3)0.2491 (4)0.1172 (11)
Br10.00000.00000.50000.0856 (6)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.084 (5)0.061 (4)0.103 (7)0.001 (4)0.019 (5)0.000 (4)
C20.088 (6)0.123 (8)0.117 (8)0.010 (6)0.019 (6)0.010 (6)
C30.092 (7)0.114 (8)0.148 (10)0.002 (6)0.044 (7)0.018 (7)
C40.085 (6)0.073 (5)0.147 (9)0.005 (5)0.030 (6)0.009 (6)
C50.111 (8)0.100 (7)0.136 (9)0.007 (6)0.008 (7)0.002 (6)
C60.129 (8)0.070 (5)0.104 (7)0.012 (5)0.047 (7)0.003 (5)
C70.076 (6)0.118 (9)0.260 (15)0.018 (6)0.033 (8)0.001 (9)
C80.221 (18)0.193 (17)0.118 (10)0.051 (12)0.053 (11)0.033 (9)
C90.055 (4)0.051 (4)0.126 (6)0.007 (3)0.020 (4)0.010 (4)
C100.060 (4)0.061 (4)0.166 (8)0.006 (3)0.041 (5)0.010 (5)
C110.063 (4)0.050 (4)0.144 (8)0.014 (3)0.013 (4)0.012 (4)
C120.076 (5)0.045 (4)0.129 (7)0.005 (3)0.016 (5)0.007 (4)
C130.066 (4)0.055 (4)0.096 (5)0.008 (3)0.021 (4)0.006 (3)
C140.048 (3)0.051 (3)0.065 (4)0.008 (3)0.001 (3)0.010 (3)
C150.065 (4)0.071 (4)0.062 (4)0.020 (3)0.013 (3)0.004 (3)
C160.071 (4)0.065 (4)0.085 (5)0.017 (3)0.014 (4)0.023 (4)
C170.070 (4)0.065 (4)0.074 (5)0.005 (3)0.005 (3)0.016 (3)
C180.063 (4)0.059 (4)0.062 (4)0.010 (3)0.003 (3)0.008 (3)
N10.054 (3)0.052 (3)0.063 (3)0.014 (2)0.005 (2)0.007 (2)
N20.060 (3)0.043 (3)0.088 (4)0.006 (2)0.019 (3)0.004 (2)
S10.0763 (14)0.0667 (13)0.205 (3)0.0106 (10)0.0429 (17)0.0171 (14)
Br10.0832 (8)0.0414 (6)0.1327 (12)0.0050 (4)0.0122 (6)0.0069 (5)
Geometric parameters (Å, º) top
C1—C21.300 (12)C11—C121.331 (11)
C1—C61.382 (14)C11—H110.9300
C1—S11.780 (9)C12—C131.366 (9)
C2—C31.392 (13)C12—H120.9300
C2—H20.9300C13—C141.373 (9)
C3—C41.403 (15)C13—H130.9300
C3—H30.9300C14—N11.422 (7)
C4—C51.326 (13)C15—C161.491 (10)
C4—C71.496 (12)C15—N11.496 (8)
C5—C61.451 (14)C15—H15A0.9700
C5—H50.9300C15—H15B0.9700
C6—C81.469 (15)C16—N21.448 (8)
C7—H7A0.9600C16—H16A0.9700
C7—H7B0.9600C16—H16B0.9700
C7—H7C0.9600C17—C181.498 (9)
C8—H8A0.9600C17—N21.526 (9)
C8—H8B0.9600C17—H17A0.9700
C8—H8C0.9600C17—H17B0.9700
C9—C141.352 (9)C18—N11.430 (8)
C9—C101.375 (9)C18—H18A0.9700
C9—S11.768 (7)C18—H18B0.9700
C10—C111.364 (10)N2—H2A0.9000
C10—H100.9300N2—H2B0.7888
C2—C1—C6120.7 (9)C13—C12—H12120.3
C2—C1—S1116.5 (8)C12—C13—C14121.6 (7)
C6—C1—S1122.4 (7)C12—C13—H13119.2
C1—C2—C3117.5 (11)C14—C13—H13119.2
C1—C2—H2121.2C9—C14—C13119.6 (6)
C3—C2—H2121.2C9—C14—N1116.3 (6)
C2—C3—C4125.5 (10)C13—C14—N1124.1 (5)
C2—C3—H3117.3C16—C15—N1109.9 (6)
C4—C3—H3117.3C16—C15—H15A109.7
C5—C4—C3116.1 (10)N1—C15—H15A109.7
C5—C4—C7119.8 (13)C16—C15—H15B109.7
C3—C4—C7124.0 (11)N1—C15—H15B109.7
C4—C5—C6119.1 (11)H15A—C15—H15B108.2
C4—C5—H5120.4N2—C16—C15108.8 (5)
C6—C5—H5120.4N2—C16—H16A109.9
C1—C6—C5121.0 (9)C15—C16—H16A109.9
C1—C6—C8122.7 (12)N2—C16—H16B109.9
C5—C6—C8116.1 (13)C15—C16—H16B109.9
C4—C7—H7A109.5H16A—C16—H16B108.3
C4—C7—H7B109.5C18—C17—N2109.7 (5)
H7A—C7—H7B109.5C18—C17—H17A109.7
C4—C7—H7C109.5N2—C17—H17A109.7
H7A—C7—H7C109.5C18—C17—H17B109.7
H7B—C7—H7C109.5N2—C17—H17B109.7
C6—C8—H8A109.5H17A—C17—H17B108.2
C6—C8—H8B109.5N1—C18—C17107.5 (5)
H8A—C8—H8B109.5N1—C18—H18A110.2
C6—C8—H8C109.5C17—C18—H18A110.2
H8A—C8—H8C109.5N1—C18—H18B110.2
H8B—C8—H8C109.5C17—C18—H18B110.2
C14—C9—C10117.5 (7)H18A—C18—H18B108.5
C14—C9—S1118.7 (5)C14—N1—C18113.4 (5)
C10—C9—S1123.5 (6)C14—N1—C15114.3 (5)
C11—C10—C9122.8 (7)C18—N1—C15112.5 (5)
C11—C10—H10118.6C16—N2—C17113.3 (5)
C9—C10—H10118.6C16—N2—H2A109.0
C12—C11—C10119.0 (7)C17—N2—H2A109.0
C12—C11—H11120.5C16—N2—H2B109.2
C10—C11—H11120.5C17—N2—H2B106.0
C11—C12—C13119.4 (7)H2A—N2—H2B110.3
C11—C12—H12120.3C9—S1—C1100.9 (4)
C6—C1—C2—C31.7 (15)C10—C9—C14—N1179.3 (7)
S1—C1—C2—C3175.1 (8)S1—C9—C14—N14.6 (9)
C1—C2—C3—C40.6 (18)C12—C13—C14—C91.7 (12)
C2—C3—C4—C50.8 (17)C12—C13—C14—N1179.4 (7)
C2—C3—C4—C7178.5 (11)N1—C15—C16—N255.6 (8)
C3—C4—C5—C61.0 (15)N2—C17—C18—N157.0 (7)
C7—C4—C5—C6178.4 (10)C9—C14—N1—C18137.0 (7)
C2—C1—C6—C51.6 (14)C13—C14—N1—C1844.1 (9)
S1—C1—C6—C5174.6 (8)C9—C14—N1—C1592.3 (7)
C2—C1—C6—C8177.3 (11)C13—C14—N1—C1586.6 (8)
S1—C1—C6—C89.8 (14)C17—C18—N1—C14166.7 (5)
C4—C5—C6—C10.1 (15)C17—C18—N1—C1561.6 (7)
C4—C5—C6—C8176.0 (11)C16—C15—N1—C14166.8 (5)
C14—C9—C10—C112.3 (14)C16—C15—N1—C1862.0 (7)
S1—C9—C10—C11176.7 (8)C15—C16—N2—C1754.8 (8)
C9—C10—C11—C123.6 (16)C18—C17—N2—C1656.4 (7)
C10—C11—C12—C132.1 (15)C14—C9—S1—C1149.2 (7)
C11—C12—C13—C140.4 (14)C10—C9—S1—C136.5 (9)
C10—C9—C14—C130.3 (12)C2—C1—S1—C9113.2 (8)
S1—C9—C14—C13174.4 (6)C6—C1—S1—C973.6 (8)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H21···Br10.902.393.269 (5)164
 

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