Literature DB >> 22904931

N-[(E)-Thio-phen-2-yl-methyl-idene]-1,3-benzothia-zol-2-amine.

Irvin N Booysen1, Muhammed B Ismail, Matthew P Akerman.   

Abstract

In the title thio-phene-derived Schiff base compound, C(12)H(8)N(2)S(2), the thio-phene ring is slighty rotated from the benzothia-zole group mean plane, giving a dihedral angle of 12.87 (6)°. The largest displacement of an atom in the mol-ecule from the nine-atom mean plane defined by the non-H atoms of the benzothia-zole ring system is 0.572 (1) Å, exhibited by the C atom at the 3-position of the thio-phene ring. In the crystal, weak C-H⋯S hydrogen bonds involving the thio-phene group S atom and the 4-position thio-phene C-H group of a symmetry-related mol-ecule lead to an infinite one-dimensional chain colinear with the c axis. The structure is further stabilized by π-π inter-actions; the distance between the thia-zole ring centroid and the centroid of an adjacent benzene ring is 3.686 (1) Å. The crystal studied was an inversion twin with the ratio of components 0.73 (3):0.27 (3).

Entities:  

Year:  2012        PMID: 22904931      PMCID: PMC3414944          DOI: 10.1107/S1600536812030498

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


Related literature

For the synthesis and crystal structure of 2-amino­benzothia­zole, see: Ding et al. (2009 ▶). For crystal structures containing 2-amino­benzothia­zole derivatives, see: Garcia-Hernandez et al. (2006 ▶). For inhibitory properties against human cancer cell lines and general anti­tumor properties of benzothia­zole derivatives, see: Racane et al. (2001 ▶); O’Brien et al. (2003 ▶). For anti­bacterial, anti­fungal, anti­tumor and anti­viral activites of benzthia­zoles, see: Yadav & Malipatil (2011 ▶); Singh & Seghal (1988 ▶); Pattan et al. (2005 ▶).

Experimental

Crystal data

C12H8N2S2 M = 244.32 Monoclinic, a = 10.7244 (5) Å b = 4.6021 (2) Å c = 11.1280 (5) Å β = 100.367 (2)° V = 540.25 (4) Å3 Z = 2 Mo Kα radiation μ = 0.46 mm−1 T = 100 K 0.45 × 0.20 × 0.12 mm

Data collection

Bruker APEXII CCD diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2010 ▶) T min = 0.625, T max = 0.749 14476 measured reflections 7768 independent reflections 7126 reflections with I > 2σ(I) R int = 0.033

Refinement

R[F 2 > 2σ(F 2)] = 0.033 wR(F 2) = 0.085 S = 1.04 7768 reflections 145 parameters 2 restraints H-atom parameters constrained Δρmax = 0.62 e Å−3 Δρmin = −0.36 e Å−3 Absolute structure: Flack (1983 ▶), 2974 Friedel pairs Flack parameter: 0.27 (3) Data collection: APEX2 (Bruker, 2010 ▶); cell refinement: SAINT (Bruker, 2010 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: WinGX (Farrugia, 1999 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶). Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812030498/lh5495sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812030498/lh5495Isup2.hkl Supplementary material file. DOI: 10.1107/S1600536812030498/lh5495Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C12H8N2S2F(000) = 252
Mr = 244.32Dx = 1.502 Mg m3
Monoclinic, PcMo Kα radiation, λ = 0.71073 Å
Hall symbol: P -2ycCell parameters from 7126 reflections
a = 10.7244 (5) Åθ = 1.9–46.7°
b = 4.6021 (2) ŵ = 0.46 mm1
c = 11.1280 (5) ÅT = 100 K
β = 100.367 (2)°Neelde, yellow
V = 540.25 (4) Å30.45 × 0.20 × 0.12 mm
Z = 2
Bruker APEXII CCD diffractometer7768 independent reflections
Radiation source: fine-focus sealed tube7126 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.033
φ and ω scansθmax = 46.7°, θmin = 2.0°
Absorption correction: multi-scan (SADABS; Bruker, 2010)h = −21→21
Tmin = 0.625, Tmax = 0.749k = −9→9
14476 measured reflectionsl = −21→22
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.033H-atom parameters constrained
wR(F2) = 0.085w = 1/[σ2(Fo2) + (0.0462P)2 + 0.0113P] where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max = 0.001
7768 reflectionsΔρmax = 0.62 e Å3
145 parametersΔρmin = −0.36 e Å3
2 restraintsAbsolute structure: Flack (1983), 2974 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.27 (3)
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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
S10.784499 (18)0.45575 (5)0.332022 (16)0.01350 (4)
S20.443816 (19)−0.29395 (6)0.120085 (18)0.01726 (4)
N10.84951 (6)0.36879 (17)0.11966 (6)0.01280 (9)
N20.66346 (7)0.11200 (17)0.15758 (6)0.01375 (10)
C41.11614 (8)0.8815 (2)0.21064 (8)0.01636 (12)
H41.18520.96700.18080.020*
C51.03822 (8)0.68618 (19)0.13798 (7)0.01428 (11)
H51.05370.63640.05910.017*
C60.93578 (7)0.56279 (17)0.18281 (7)0.01178 (10)
C70.76580 (7)0.29951 (17)0.18671 (7)0.01226 (10)
C80.63195 (8)0.02760 (18)0.04564 (7)0.01376 (11)
H80.67830.0935−0.01420.017*
C90.52640 (7)−0.16652 (18)0.01185 (7)0.01283 (10)
C100.47648 (8)−0.2709 (2)−0.10331 (8)0.01632 (12)
H100.5091−0.2242−0.17490.020*
C110.37091 (9)−0.4557 (2)−0.10202 (9)0.01923 (14)
H110.3248−0.5476−0.17270.023*
C31.09458 (8)0.9554 (2)0.32807 (9)0.01656 (12)
H31.14941.09010.37610.020*
C20.99466 (8)0.83477 (19)0.37474 (7)0.01491 (11)
H20.98030.88410.45400.018*
C10.91594 (7)0.63843 (17)0.30119 (7)0.01210 (10)
C120.34282 (9)−0.4870 (2)0.01255 (10)0.01891 (14)
H120.2750−0.60260.03030.023*
U11U22U33U12U13U23
S10.01409 (7)0.01617 (8)0.01111 (6)−0.00243 (6)0.00462 (5)−0.00251 (6)
S20.01686 (8)0.02164 (9)0.01432 (7)−0.00281 (7)0.00559 (6)0.00148 (6)
N10.0128 (2)0.0148 (2)0.0111 (2)−0.00094 (18)0.00313 (16)−0.00076 (18)
N20.0137 (2)0.0151 (3)0.0127 (2)−0.00233 (19)0.00298 (17)−0.00149 (18)
C40.0137 (3)0.0163 (3)0.0195 (3)−0.0015 (2)0.0040 (2)0.0025 (2)
C50.0129 (2)0.0164 (3)0.0143 (2)−0.0002 (2)0.0044 (2)0.0016 (2)
C60.0117 (2)0.0121 (3)0.0117 (2)0.00034 (18)0.00274 (18)0.00046 (18)
C70.0132 (2)0.0131 (3)0.0107 (2)−0.0009 (2)0.00263 (18)−0.00112 (19)
C80.0142 (3)0.0150 (3)0.0125 (2)−0.0025 (2)0.0037 (2)−0.0016 (2)
C90.0126 (2)0.0142 (3)0.0122 (2)−0.0008 (2)0.00370 (19)−0.00131 (19)
C100.0152 (3)0.0208 (3)0.0138 (3)−0.0033 (2)0.0047 (2)−0.0044 (2)
C110.0140 (3)0.0229 (4)0.0211 (3)−0.0032 (3)0.0041 (2)−0.0073 (3)
C30.0140 (3)0.0156 (3)0.0195 (3)−0.0028 (2)0.0012 (2)−0.0005 (2)
C20.0147 (3)0.0147 (3)0.0151 (3)−0.0013 (2)0.0020 (2)−0.0022 (2)
C10.0119 (2)0.0123 (3)0.0122 (2)−0.00014 (19)0.00249 (18)−0.00036 (19)
C120.0143 (3)0.0185 (3)0.0249 (4)−0.0031 (2)0.0062 (3)−0.0015 (3)
S1—C11.7279 (8)C6—C11.4152 (10)
S1—C71.7480 (7)C8—C91.4379 (11)
S2—C121.7111 (10)C8—H80.9500
S2—C91.7213 (8)C9—C101.3830 (11)
N1—C71.3058 (10)C10—C111.4183 (13)
N1—C61.3831 (10)C10—H100.9500
N2—C81.2904 (10)C11—C121.3694 (15)
N2—C71.3879 (10)C11—H110.9500
C4—C51.3844 (12)C3—C21.3880 (12)
C4—C31.4091 (13)C3—H30.9500
C4—H40.9500C2—C11.3966 (11)
C5—C61.4055 (11)C2—H20.9500
C5—H50.9500C12—H120.9500
C1—S1—C788.76 (4)C10—C9—S2111.59 (6)
C12—S2—C991.61 (4)C8—C9—S2120.57 (6)
C7—N1—C6109.46 (6)C9—C10—C11112.06 (8)
C8—N2—C7118.12 (7)C9—C10—H10124.0
C5—C4—C3121.06 (8)C11—C10—H10124.0
C5—C4—H4119.5C12—C11—C10112.47 (8)
C3—C4—H4119.5C12—C11—H11123.8
C4—C5—C6118.89 (7)C10—C11—H11123.8
C4—C5—H5120.6C2—C3—C4121.13 (8)
C6—C5—H5120.6C2—C3—H3119.4
N1—C6—C5125.08 (7)C4—C3—H3119.4
N1—C6—C1115.64 (7)C3—C2—C1117.74 (8)
C5—C6—C1119.28 (7)C3—C2—H2121.1
N1—C7—N2127.91 (7)C1—C2—H2121.1
N1—C7—S1116.87 (6)C2—C1—C6121.90 (7)
N2—C7—S1115.22 (6)C2—C1—S1128.84 (6)
N2—C8—C9119.77 (7)C6—C1—S1109.26 (6)
N2—C8—H8120.1C11—C12—S2112.27 (7)
C9—C8—H8120.1C11—C12—H12123.9
C10—C9—C8127.83 (7)S2—C12—H12123.9
C3—C4—C5—C60.46 (13)C8—C9—C10—C11−179.24 (9)
C7—N1—C6—C5−179.28 (8)S2—C9—C10—C11−0.19 (11)
C7—N1—C6—C10.46 (10)C9—C10—C11—C120.20 (13)
C4—C5—C6—N1178.98 (8)C5—C4—C3—C20.04 (14)
C4—C5—C6—C1−0.76 (12)C4—C3—C2—C1−0.22 (13)
C6—N1—C7—N2179.97 (8)C3—C2—C1—C6−0.10 (12)
C6—N1—C7—S1−1.01 (9)C3—C2—C1—S1−179.40 (7)
C8—N2—C7—N1−12.23 (13)N1—C6—C1—C2−179.17 (7)
C8—N2—C7—S1168.73 (7)C5—C6—C1—C20.60 (12)
C1—S1—C7—N11.00 (7)N1—C6—C1—S10.26 (9)
C1—S1—C7—N2−179.84 (6)C5—C6—C1—S1−179.98 (6)
C7—N2—C8—C9−179.96 (7)C7—S1—C1—C2178.73 (8)
N2—C8—C9—C10177.50 (9)C7—S1—C1—C6−0.64 (6)
N2—C8—C9—S2−1.47 (12)C10—C11—C12—S2−0.12 (12)
C12—S2—C9—C100.10 (8)C9—S2—C12—C110.01 (8)
C12—S2—C9—C8179.23 (7)
D—H···AD—HH···AD···AD—H···A
C11—H11···S2i0.952.923.517 (1)122 (1)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
C11—H11⋯S2i 0.952.923.517 (1)122 (1)

Symmetry code: (i) .

  3 in total

1.  Antitumor benzothiazoles. Frontier molecular orbital analysis predicts bioactivation of 2-(4-aminophenyl)benzothiazoles to reactive intermediates by cytochrome P4501A1.

Authors:  Sean E O'Brien; Helen L Browne; Tracey D Bradshaw; Andrew D Westwell; Malcolm F Stevens; Charles A Laughton
Journal:  Org Biomol Chem       Date:  2003-02-07       Impact factor: 3.876

2.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

3.  Synthesis of 2-aminobenzothiazole via copper(I)-catalyzed tandem reaction of 2-iodobenzenamine with isothiocyanate.

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