Literature DB >> 21579437

2-(2-Nitro-anilino)-5,6,7,8-tetra-hydro-4H-cyclo-hepta-[b]thio-phene-3-carbonitrile.

Maria do Carmo A de Lima, Francisco J B Mendonça Junior, Suely L Galdino, Ivan R Pitta, Carlos A de Simone.   

Abstract

The title compound, C(16)H(15)N(3)O(2)S, was synthesized by the reaction of 2-amino-5,6,7,8-tetra-hydro-4H-cyclo-hepta-[b]thio-phene-3-carbonitrile and o-fluoro-nitro-benzene. The thio-phene and nitro-phenyl rings and amino and carbonitrile groups are coplanar with a maximum deviation of 0.046 (2) Å and a dihedral angle of 0.92 (6)° between the rings. The cyclo-hepta ring adopts a chair conformation. Intra-molecular N-H⋯O and C-H⋯S inter-actions occur. In the crystal, the mol-ecules form layers that are linked by π-π stacking inter-actions between the thio-phene and benzene rings [centroid-centroid distances = 3.7089 (12) and 3.6170 (12) Å].

Entities:  

Year:  2010        PMID: 21579437      PMCID: PMC2979624          DOI: 10.1107/S1600536810017149

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


Related literature

For background to 2-substituted thio­phenes, see: Campaigne (1984 ▶); Kleemann et al. (2006 ▶). For the biological activity of 2-amino thio­phene derivatives, see: Chakrabarti et al. (1982 ▶); Calligaro et al. (1997 ▶); Nikolakopoulos et al. (2006 ▶). For the synthesis of 2-amino thio­phenes, see: Gewald (1965 ▶); Gewald et al. (1966 ▶); Sridhar et al. (2007 ▶). For related structures, see: Stephenson et al. (1995 ▶); Yu (2002 ▶); Chen et al. (2005 ▶). For bond-length data, see: Allen et al. (1987 ▶). For puckering parameters, see: Cremer & Pople (1975 ▶).

Experimental

Crystal data

C16H15N3O2S M = 313.37 Monoclinic, a = 7.0273 (3) Å b = 14.4569 (6) Å c = 14.8867 (7) Å β = 97.571 (2)° V = 1499.18 (11) Å3 Z = 4 Mo Kα radiation μ = 0.23 mm−1 T = 295 K 0.35 × 0.32 × 0.27 mm

Data collection

Nonius KappaCCD diffractometer 9360 measured reflections 3147 independent reflections 2452 reflections with I > 2σ(I) R int = 0.046

Refinement

R[F 2 > 2σ(F 2)] = 0.052 wR(F 2) = 0.162 S = 1.07 3147 reflections 200 parameters H-atom parameters constrained Δρmax = 0.29 e Å−3 Δρmin = −0.31 e Å−3 Data collection: COLLECT (Nonius, 1997 ▶); cell refinement: SCALEPACK (Otwinowski & Minor, 1997 ▶); data reduction: DENZO (Otwinowski & Minor, 1997 ▶) and SCALEPACK; 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 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810017149/dn2562sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810017149/dn2562Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C16H15N3O2SF(000) = 656
Mr = 313.37Dx = 1.388 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 6392 reflections
a = 7.0273 (3) Åθ = 2.9–26.7°
b = 14.4569 (6) ŵ = 0.23 mm1
c = 14.8867 (7) ÅT = 295 K
β = 97.571 (2)°Prism, colorless
V = 1499.18 (11) Å30.35 × 0.32 × 0.27 mm
Z = 4
Nonius KappaCCD diffractometer2452 reflections with I > 2σ(I)
Radiation source: Enraf Nonius FR590Rint = 0.046
horizonally mounted graphite crystalθmax = 26.6°, θmin = 3.1°
Detector resolution: 9 pixels mm-1h = −8→8
CCD rotation images,thick slices scansk = −15→18
9360 measured reflectionsl = −18→18
3147 independent reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.052Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.162H-atom parameters constrained
S = 1.07w = 1/[σ2(Fo2) + (0.1026P)2 + 0.1476P] where P = (Fo2 + 2Fc2)/3
3147 reflections(Δ/σ)max = 0.001
200 parametersΔρmax = 0.29 e Å3
0 restraintsΔρmin = −0.30 e Å3
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 > 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
S10.29875 (7)0.33887 (3)0.05524 (3)0.0529 (2)
O10.1864 (3)0.64817 (11)−0.14472 (10)0.0763 (5)
O20.1729 (3)0.78484 (12)−0.09126 (12)0.0887 (6)
N10.2433 (2)0.50661 (11)−0.03762 (10)0.0531 (4)
H10.22770.5305−0.09100.064*
N20.1906 (2)0.70191 (13)−0.07994 (12)0.0594 (4)
N30.2128 (4)0.44432 (17)−0.26828 (13)0.0871 (7)
C10.2620 (2)0.41167 (13)−0.03697 (12)0.0474 (4)
C20.2544 (3)0.36042 (14)−0.11578 (12)0.0501 (4)
C30.2772 (3)0.26261 (14)−0.10156 (13)0.0527 (5)
C40.2731 (4)0.19525 (16)−0.17935 (14)0.0673 (6)
H4A0.40410.1775−0.18500.081*
H4B0.22210.2269−0.23480.081*
C50.1554 (3)0.10721 (16)−0.17147 (15)0.0688 (6)
H5A0.02710.1251−0.16090.083*
H5B0.14380.0750−0.22910.083*
C60.2345 (4)0.04019 (15)−0.09784 (16)0.0707 (6)
H6A0.36880.0293−0.10310.085*
H6B0.1677−0.0183−0.10860.085*
C70.2190 (4)0.07060 (16)−0.00136 (16)0.0710 (6)
H7A0.08720.08880.00210.085*
H7B0.24710.01790.03850.085*
C80.3487 (4)0.14916 (15)0.03367 (16)0.0669 (6)
H8A0.47980.13240.02700.080*
H8B0.34180.15640.09790.080*
C90.3044 (3)0.24118 (14)−0.01205 (13)0.0551 (5)
C100.2447 (2)0.57016 (13)0.03089 (12)0.0473 (4)
C110.2192 (3)0.66561 (13)0.01206 (13)0.0491 (4)
C120.2185 (3)0.73041 (15)0.08074 (14)0.0587 (5)
H120.20120.79270.06630.070*
C130.2430 (3)0.70360 (16)0.16918 (15)0.0635 (5)
H130.24270.74720.21510.076*
C140.2683 (3)0.61106 (16)0.18993 (14)0.0636 (5)
H140.28450.59240.25030.076*
C150.2700 (3)0.54584 (15)0.12264 (13)0.0594 (5)
H150.28840.48400.13860.071*
C160.2285 (3)0.40474 (15)−0.20159 (13)0.0594 (5)
U11U22U33U12U13U23
S10.0672 (3)0.0504 (3)0.0413 (3)−0.00605 (19)0.0074 (2)0.00132 (18)
O10.1190 (14)0.0599 (10)0.0478 (8)−0.0002 (8)0.0034 (8)0.0025 (7)
O20.1394 (16)0.0503 (10)0.0753 (11)0.0042 (9)0.0103 (10)0.0123 (8)
N10.0707 (10)0.0480 (9)0.0407 (8)−0.0010 (7)0.0077 (7)0.0000 (7)
N20.0684 (10)0.0538 (10)0.0558 (10)−0.0019 (7)0.0072 (8)0.0042 (8)
N30.1274 (18)0.0861 (15)0.0481 (11)0.0209 (13)0.0123 (10)0.0112 (10)
C10.0508 (9)0.0485 (10)0.0427 (9)−0.0040 (7)0.0061 (7)0.0005 (7)
C20.0563 (10)0.0523 (10)0.0422 (9)−0.0028 (8)0.0078 (7)0.0000 (8)
C30.0604 (10)0.0505 (10)0.0475 (10)−0.0033 (8)0.0084 (8)−0.0032 (8)
C40.0929 (15)0.0587 (12)0.0513 (11)−0.0070 (11)0.0131 (10)−0.0077 (10)
C50.0836 (14)0.0569 (12)0.0647 (13)0.0012 (10)0.0048 (11)−0.0140 (10)
C60.0909 (16)0.0494 (12)0.0705 (14)−0.0006 (11)0.0057 (11)−0.0047 (10)
C70.0915 (15)0.0502 (12)0.0715 (14)−0.0034 (10)0.0116 (11)0.0040 (11)
C80.0859 (14)0.0559 (13)0.0566 (12)−0.0038 (10)0.0010 (10)0.0049 (9)
C90.0650 (11)0.0505 (11)0.0497 (10)−0.0063 (8)0.0069 (8)−0.0009 (8)
C100.0481 (9)0.0511 (10)0.0432 (9)−0.0042 (7)0.0081 (7)−0.0011 (8)
C110.0493 (9)0.0508 (11)0.0474 (10)−0.0045 (7)0.0071 (7)0.0001 (7)
C120.0653 (11)0.0520 (11)0.0597 (12)0.0000 (9)0.0120 (9)−0.0070 (9)
C130.0725 (13)0.0632 (13)0.0569 (11)−0.0048 (10)0.0169 (9)−0.0144 (10)
C140.0811 (13)0.0665 (13)0.0448 (11)−0.0042 (10)0.0147 (9)−0.0043 (9)
C150.0786 (13)0.0532 (11)0.0478 (11)−0.0023 (10)0.0134 (9)0.0008 (9)
C160.0750 (12)0.0587 (12)0.0442 (10)0.0058 (9)0.0066 (8)−0.0043 (9)
S1—C11.7220 (18)C6—C71.520 (3)
S1—C91.735 (2)C6—H6A0.9700
O1—N21.236 (2)C6—H6B0.9700
O2—N21.215 (2)C7—C81.506 (3)
N1—C101.372 (2)C7—H7A0.9700
N1—C11.379 (2)C7—H7B0.9700
N1—H10.8600C8—C91.508 (3)
N2—C111.456 (2)C8—H8A0.9700
N3—C161.139 (3)C8—H8B0.9700
C1—C21.383 (2)C10—C151.399 (3)
C2—C161.419 (3)C10—C111.415 (3)
C2—C31.436 (3)C11—C121.387 (3)
C3—C91.357 (3)C12—C131.361 (3)
C3—C41.510 (3)C12—H120.9300
C4—C51.531 (3)C13—C141.379 (3)
C4—H4A0.9700C13—H130.9300
C4—H4B0.9700C14—C151.377 (3)
C5—C61.513 (3)C14—H140.9300
C5—H5A0.9700C15—H150.9300
C5—H5B0.9700
C1—S1—C992.84 (9)C8—C7—C6115.5 (2)
C10—N1—C1132.09 (16)C8—C7—H7A108.4
C10—N1—H1114.0C6—C7—H7A108.4
C1—N1—H1114.0C8—C7—H7B108.4
O2—N2—O1121.38 (19)C6—C7—H7B108.4
O2—N2—C11119.03 (18)H7A—C7—H7B107.5
O1—N2—C11119.59 (17)C7—C8—C9115.43 (19)
N1—C1—C2122.32 (17)C7—C8—H8A108.4
N1—C1—S1128.18 (14)C9—C8—H8A108.4
C2—C1—S1109.50 (14)C7—C8—H8B108.4
C1—C2—C16120.52 (18)C9—C8—H8B108.4
C1—C2—C3114.31 (17)H8A—C8—H8B107.5
C16—C2—C3125.17 (18)C3—C9—C8129.69 (19)
C9—C3—C2111.61 (17)C3—C9—S1111.73 (15)
C9—C3—C4126.28 (19)C8—C9—S1118.46 (15)
C2—C3—C4122.11 (18)N1—C10—C15123.03 (18)
C3—C4—C5115.66 (17)N1—C10—C11121.17 (16)
C3—C4—H4A108.4C15—C10—C11115.79 (17)
C5—C4—H4A108.4C12—C11—C10121.68 (18)
C3—C4—H4B108.4C12—C11—N2115.89 (18)
C5—C4—H4B108.4C10—C11—N2122.43 (16)
H4A—C4—H4B107.4C13—C12—C11120.6 (2)
C6—C5—C4115.93 (19)C13—C12—H12119.7
C6—C5—H5A108.3C11—C12—H12119.7
C4—C5—H5A108.3C12—C13—C14119.26 (19)
C6—C5—H5B108.3C12—C13—H13120.4
C4—C5—H5B108.3C14—C13—H13120.4
H5A—C5—H5B107.4C15—C14—C13120.97 (19)
C5—C6—C7115.73 (19)C15—C14—H14119.5
C5—C6—H6A108.3C13—C14—H14119.5
C7—C6—H6A108.3C14—C15—C10121.7 (2)
C5—C6—H6B108.3C14—C15—H15119.1
C7—C6—H6B108.3C10—C15—H15119.1
H6A—C6—H6B107.4N3—C16—C2176.3 (2)
D—H···AD—HH···AD···AD—H···A
N1—H1···O10.861.892.593 (2)138
C12—H12···O20.932.332.657 (3)100
C15—H15···S10.932.443.171 (2)135
Cg1···Cg2Cg1 to plane 2Cg2 to plane 1Offset
Cg1···Cg2i3.7089 (12)-3.5039 (9)-3.5021 (9)19.4
Cg1···Cg2ii3.6170 (12)3.4761 (9)3.4878 (9)16.0
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H1⋯O10.861.892.593 (2)138
C15—H15⋯S10.932.443.171 (2)135
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