Literature DB >> 23476168

(5S,11aS)-5-Hydro-per-oxy-1,5,11,11a-tetra-hydro-[1]benzothieno[3,2-f]indol-izin-3(2H)-one.

Viktor Vrábel1, Lubomír Svorc, Stefan Marchalín, Peter Safář.   

Abstract

The absolute configuration of the title compound, C14H13NO3S, was assigned from the synthesis and confirmed by the structure determination. The central six-membered ring of the indolizine moiety adopts an envelope conformation, with the greatest deviation from the mean plane of the ring being 0.661 (2) Å for the bridgehead C atom. The benzothiene ring attached to the indolizine ring system is planar to within 0.008 (2) Å. In the crystal, mol-ecules form chains parallel to the b axis via O-H⋯O hydrogen bonds.

Entities:  

Year:  2012        PMID: 23476168      PMCID: PMC3588932          DOI: 10.1107/S1600536812045394

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For background to indolizines and their biological activity, see: Malonne et al. (1998 ▶); Medda et al. (2003 ▶); Sonnet et al. (2000 ▶); Campagna et al. (1990 ▶); Pearson & Guo (2001 ▶). For their synthesis, see: Šafář et al. (2009a ▶,b ▶). For compounds with similar properties, see: Švorc et al. (2008 ▶, 2009 ▶). For IR spectroscopy on similar compounds, see: Šafář et al. (2009a ▶). For conformational analysis, see: Nardelli (1983 ▶).

Experimental

Crystal data

C14H13NO3S M = 275.31 Monoclinic, a = 7.8040 (5) Å b = 7.9800 (4) Å c = 10.2903 (5) Å β = 99.458 (5)° V = 632.13 (6) Å3 Z = 2 Mo Kα radiation μ = 0.26 mm−1 T = 295 K 0.25 × 0.20 × 0.15 mm

Data collection

Oxford Diffraction Xcalibur (Ruby, Gemi) diffractometer Absorption correction: analytical [CrysAlis RED (Oxford Diffraction, 2009 ▶), based on expressions derived by Clark & Reid (1995 ▶)] T min = 0.947, T max = 0.974 21595 measured reflections 2555 independent reflections 2162 reflections with I > 2σ(I) R int = 0.028

Refinement

R[F 2 > 2σ(F 2)] = 0.027 wR(F 2) = 0.068 S = 1.00 2555 reflections 176 parameters 2 restraints H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.13 e Å−3 Δρmin = −0.14 e Å−3 Absolute structure: Flack (1983 ▶), 1185 Friedel pairs Flack parameter: −0.05 (6) Data collection: CrysAlis CCD (Oxford Diffraction, 2009 ▶); cell refinement: CrysAlis CCD; data reduction: CrysAlis RED (Oxford Diffraction, 2009 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: DIAMOND, (Brandenburg, 2001 ▶), PLATON (Spek, 2009 ▶) and WinGX (Farrugia, 1999 ▶); software used to prepare material for publication: SHELXL97. Click here for additional data file. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812045394/bg2481sup1.cif Click here for additional data file. Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812045394/bg2481Isup2.hkl Click here for additional data file. Supplementary material file. DOI: 10.1107/S1600536812045394/bg2481Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C14H13NO3SF(000) = 288
Mr = 275.31Dx = 1.446 Mg m3
Monoclinic, P21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ybCell parameters from 10799 reflections
a = 7.8040 (5) Åθ = 3.2–29.6°
b = 7.9800 (4) ŵ = 0.26 mm1
c = 10.2903 (5) ÅT = 295 K
β = 99.458 (5)°Block, colourless
V = 632.13 (6) Å30.25 × 0.20 × 0.15 mm
Z = 2
Oxford Diffraction Xcalibur (Ruby, Gemi) diffractometer2555 independent reflections
Radiation source: fine-focus sealed tube2162 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.028
Detector resolution: 10.4340 pixels mm-1θmax = 26.4°, θmin = 4.4°
ω scansh = −9→9
Absorption correction: analytical [CrysAlis RED (Oxford Diffraction, 2009), based on expressions derived by Clark & Reid (1995)]k = −9→9
Tmin = 0.947, Tmax = 0.974l = −12→12
21595 measured reflections
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.027H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.068w = 1/[σ2(Fo2) + (0.0441P)2] where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max < 0.001
2555 reflectionsΔρmax = 0.13 e Å3
176 parametersΔρmin = −0.14 e Å3
2 restraintsAbsolute structure: Flack (1983), 1185 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: −0.05 (6)
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes.
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.
xyzUiso*/Ueq
C2−0.1152 (2)0.0934 (2)0.10939 (14)0.0487 (4)
C3−0.2994 (2)0.1556 (3)0.07868 (18)0.0625 (5)
H3B−0.37140.10140.13470.075*
H3A−0.34830.1340−0.01270.075*
C4−0.2872 (2)0.3432 (3)0.1057 (2)0.0662 (5)
H4B−0.38520.38170.14470.079*
H4A−0.28380.40540.02520.079*
C5−0.1161 (2)0.3639 (3)0.20284 (16)0.0527 (4)
H5−0.05630.46660.18340.063*
C6−0.1345 (2)0.3584 (3)0.34751 (18)0.0584 (4)
H6B−0.17500.46610.37410.070*
H6A−0.21900.27390.36130.070*
C70.0371 (2)0.31816 (19)0.42819 (16)0.0490 (4)
C80.2927 (2)0.2798 (2)0.60665 (15)0.0497 (4)
C90.4223 (3)0.2701 (3)0.71705 (16)0.0633 (5)
H90.40120.30560.79900.076*
C100.5810 (3)0.2073 (3)0.70255 (19)0.0707 (6)
H100.66910.20280.77520.085*
C110.6131 (3)0.1499 (3)0.58133 (19)0.0634 (5)
H110.72180.10640.57430.076*
C120.4862 (2)0.1569 (2)0.47181 (16)0.0511 (4)
H120.50840.11740.39120.061*
C130.3233 (2)0.22356 (19)0.48218 (15)0.0428 (4)
C140.17251 (19)0.24634 (19)0.38248 (14)0.0412 (4)
C150.15873 (19)0.1929 (2)0.24080 (14)0.0413 (4)
H150.19270.07510.23630.050*
N1−0.01704 (17)0.21547 (16)0.17396 (12)0.0447 (3)
O1−0.06189 (17)−0.04709 (17)0.08604 (12)0.0627 (3)
O20.27750 (15)0.29669 (15)0.18624 (11)0.0513 (3)
O30.28192 (17)0.23328 (18)0.05339 (11)0.0597 (3)
H30.207 (2)0.299 (3)0.013 (2)0.098 (9)*
S10.08315 (6)0.35880 (6)0.59656 (4)0.06228 (15)
U11U22U33U12U13U23
C20.0512 (10)0.0610 (11)0.0332 (7)−0.0060 (9)0.0043 (7)0.0038 (8)
C30.0518 (11)0.0782 (14)0.0546 (10)−0.0038 (10)0.0001 (8)0.0057 (9)
C40.0501 (10)0.0692 (13)0.0765 (12)0.0052 (11)0.0018 (9)0.0209 (11)
C50.0440 (9)0.0452 (9)0.0699 (10)0.0038 (9)0.0121 (8)0.0093 (9)
C60.0508 (9)0.0560 (9)0.0702 (10)0.0095 (10)0.0151 (8)−0.0066 (10)
C70.0520 (10)0.0446 (10)0.0529 (9)−0.0003 (8)0.0156 (8)−0.0048 (7)
C80.0679 (11)0.0400 (8)0.0435 (9)0.0012 (8)0.0161 (8)0.0007 (7)
C90.0933 (15)0.0563 (11)0.0402 (9)0.0050 (11)0.0102 (9)0.0006 (8)
C100.0872 (16)0.0703 (14)0.0492 (10)0.0112 (12)−0.0050 (10)0.0097 (9)
C110.0673 (12)0.0648 (12)0.0560 (10)0.0171 (10)0.0042 (9)0.0099 (9)
C120.0589 (11)0.0514 (10)0.0439 (9)0.0086 (9)0.0111 (8)0.0041 (7)
C130.0549 (9)0.0338 (8)0.0411 (7)−0.0015 (7)0.0120 (7)0.0016 (6)
C140.0467 (9)0.0354 (8)0.0433 (8)−0.0009 (7)0.0125 (7)−0.0009 (6)
C150.0405 (8)0.0433 (9)0.0408 (8)−0.0002 (7)0.0084 (6)0.0009 (6)
N10.0429 (7)0.0457 (7)0.0458 (7)0.0001 (6)0.0082 (6)0.0021 (6)
O10.0674 (9)0.0619 (8)0.0554 (7)−0.0007 (7)0.0000 (6)−0.0159 (6)
O20.0498 (6)0.0609 (7)0.0445 (6)−0.0061 (5)0.0121 (5)0.0000 (5)
O30.0607 (8)0.0756 (9)0.0452 (7)0.0118 (7)0.0163 (6)0.0007 (6)
S10.0745 (3)0.0630 (3)0.0537 (2)0.0086 (3)0.0234 (2)−0.0118 (2)
C2—O11.233 (2)C8—C131.414 (2)
C2—N11.345 (2)C8—S11.7400 (19)
C2—C31.505 (3)C9—C101.366 (3)
C3—C41.523 (3)C9—H90.9300
C3—H3B0.9700C10—C111.390 (3)
C3—H3A0.9700C10—H100.9300
C4—C51.539 (3)C11—C121.374 (3)
C4—H4B0.9700C11—H110.9300
C4—H4A0.9700C12—C131.398 (2)
C5—N11.471 (2)C12—H120.9300
C5—C61.519 (2)C13—C141.440 (2)
C5—H50.9800C14—C151.506 (2)
C6—C71.490 (2)C15—O21.4252 (19)
C6—H6B0.9700C15—N11.441 (2)
C6—H6A0.9700C15—H150.9800
C7—C141.353 (2)O2—O31.4634 (16)
C7—S11.7411 (17)O3—H30.841 (2)
C8—C91.393 (3)
O1—C2—N1124.86 (17)C13—C8—S1110.95 (13)
O1—C2—C3126.89 (16)C10—C9—C8118.72 (16)
N1—C2—C3108.17 (16)C10—C9—H9120.6
C2—C3—C4104.88 (16)C8—C9—H9120.6
C2—C3—H3B110.8C9—C10—C11121.29 (18)
C4—C3—H3B110.8C9—C10—H10119.4
C2—C3—H3A110.8C11—C10—H10119.4
C4—C3—H3A110.8C12—C11—C10120.70 (18)
H3B—C3—H3A108.8C12—C11—H11119.7
C3—C4—C5104.22 (16)C10—C11—H11119.7
C3—C4—H4B110.9C11—C12—C13119.67 (15)
C5—C4—H4B110.9C11—C12—H12120.2
C3—C4—H4A110.9C13—C12—H12120.2
C5—C4—H4A110.9C12—C13—C8118.72 (15)
H4B—C4—H4A108.9C12—C13—C14129.82 (14)
N1—C5—C6108.21 (14)C8—C13—C14111.46 (14)
N1—C5—C4102.19 (16)C7—C14—C13113.53 (14)
C6—C5—C4114.92 (14)C7—C14—C15121.41 (14)
N1—C5—H5110.4C13—C14—C15125.04 (13)
C6—C5—H5110.4O2—C15—N1111.66 (12)
C4—C5—H5110.4O2—C15—C14105.62 (12)
C7—C6—C5109.33 (13)N1—C15—C14109.74 (12)
C7—C6—H6B109.8O2—C15—H15109.9
C5—C6—H6B109.8N1—C15—H15109.9
C7—C6—H6A109.8C14—C15—H15109.9
C5—C6—H6A109.8C2—N1—C15124.42 (15)
H6B—C6—H6A108.3C2—N1—C5114.03 (14)
C14—C7—C6125.42 (15)C15—N1—C5119.65 (13)
C14—C7—S1112.32 (13)C15—O2—O3106.49 (11)
C6—C7—S1122.26 (12)O2—O3—H397.2 (18)
C9—C8—C13120.88 (17)C8—S1—C791.72 (7)
C9—C8—S1128.16 (13)
D—H···AD—HH···AD···AD—H···A
O3—H3···O1i0.84 (1)1.86 (1)2.6962 (19)173 (2)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
O3—H3⋯O1i 0.84 (1)1.86 (1)2.6962 (19)173 (2)

Symmetry code: (i) .

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  1 in total

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