organic compounds
2-Methyl-12H-benzimidazo[2,1-b][1,3]benzothiazin-12-one
aSchool of Petrochemical Engineering, Changzhou University, Changzhou, Jiangsu, 213164, People's Republic of China
*Correspondence e-mail: wzmmol@hotmail.com
In the title compound, C15H10N2OS, prepared by the reaction of 2-iodo-5-methylbenzoyl chloride with 2-mercaptobenzimidazole, the four-membered fused-ring system is essentially planar [maximum deviation from the least-squares plane = 0.137 (6) Å]. The crystal packing is stabilized by weak intermolecular π–π interactions [minimum ring centroid separation = 3.536 (4) Å] and weak C—H⋯π interactions.
Related literature
For general background to imidazo[2,1-b][1,3]thiazinones, see: van der Helm et al. (1987); Dolbier et al. (1994); Sekar et al. (2011).
Experimental
Crystal data
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Refinement
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Data collection: CrysAlis PRO (Agilent, 2010); cell CrysAlis PRO; data reduction: CrysAlis PRO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2.
Supporting information
https://doi.org/10.1107/S1600536811050501/zs2165sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536811050501/zs2165Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S1600536811050501/zs2165Isup3.cml
An oven-dried Schlenk tube was charged with a magnetic stirring bar, CuI (0.05 mmol), 1,10-phenanthroline (0.10 mmol), Cs2CO3 (0.50 mmol), and 2-mercaptobenzimidazole. The Schlenk tube was capped, and then evacuated and backfilled with N2 (3 times), then under a positive pressure of N2, a solution of 2-iodo-5-methylbenzoyl chloride (0.75 mmol) in toluene (2 ml, freshly distilled from sodium) was added dropwise via syringe, and the mixture was pre-stirred for 1 h at room temperature. The reaction mixture was then stirred at 100 °C. After the reaction was completed, the mixture was cooled to room temperature, passed through Celite and rinsed with 30 ml of CH2Cl2. The combined filtrate was concentrated and purified by flash
to give a yellow solid (93% yield). Single crystals of the title compound suitable for X-ray diffraction were obtained by evaporation of a petroleum ether–chloroform solution.All the H atoms were placed in geometrically idealized positions and constrained to ride on their parent atoms, with C—H = 0.93 (aromatic C) and 0.96 Å (methyl C), with Uiso(H)= 1.2Ueq(aromatic C) or 1.5Ueq(methyl C).
Owing to the promising biological activities as antimicrobial agents against bacteria, yeast and fungi, imidazo[2,1-b][1,3]thiazinones have been studied (van der Helm et al., 1987). In the past decades, most of these investigations were carried out with imidazole derivatives (Dolbier et al., 1994; Sekar et al., 2011). We herein present the structure of the title compound C15H10N2OS, prepared from the reaction of 2-iodo-5-methylbenzoyl chloride with 2-mercaptobenzimidazole.
In the
the title compound adopts an essentially planar conformation (Fig. 1), with the maximum atom deviation from the least-squares plane to the four-membered fused-ring system = 0.137 (6) Å]. The dihedral angles between the benzimidazole ring (N1–C15) and the thiazine ring (S1–C9) = 3.18 (5) °, the benzene ring (C2–C7) and the thiazine ring (S1–C9) = 0.38 (6)° and the benzimidazole ring (N1–C15) and the benzene ring (C2–C7) = 3.55 (6)°.The crystal packing is stabilized by weak intermolecular π–π interactions involving the six-membered aromatic rings: (a) the thiazine ring S1–C9 (ring 1) and the benzene ring C10–C15i (ring 2) of the benzimazole moiety [ring centroid separation = 3.628 (8) Å: symmetry code (i) -x + 1, -y + 1, -z + 1]; (b) between the benzene ring C2–C7 (ring 3) and ring C2–C7i = 3.817 (6) Å; (c) between ring 3···and ring 2i = 3.536 (4) Å. There are also C—H···π interactions present.
For general background to imidazo[2,1-b][1,3]thiazinones, see: van der Helm et al. (1987); Dolbier et al. (1994); Sekar et al. (2011).
Data collection: CrysAlis PRO (Agilent, 2010); cell
CrysAlis PRO (Agilent, 2010); data reduction: CrysAlis PRO (Agilent, 2010); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).Fig. 1. Molecular conformation and atom numbering scheme for the title compound, with displacement ellipsoids drawn at the 40% probability level. |
C15H10N2OS | F(000) = 1104 |
Mr = 266.31 | Dx = 1.421 Mg m−3 |
Orthorhombic, Pbca | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ac 2ab | Cell parameters from 3080 reflections |
a = 11.7737 (5) Å | θ = 3.0–29.4° |
b = 8.1122 (3) Å | µ = 0.25 mm−1 |
c = 26.0694 (10) Å | T = 293 K |
V = 2489.90 (17) Å3 | Block, yellow |
Z = 8 | 0.38 × 0.35 × 0.32 mm |
Agilent Xcalibur Atlas Gemini Ultra CCD diffractometer | 2277 independent reflections |
Radiation source: fine-focus sealed tube | 1826 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.029 |
Detector resolution: 10.3592 pixels mm-1 | θmax = 25.3°, θmin = 3.1° |
ω scans | h = −11→14 |
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) | k = −9→8 |
Tmin = 0.911, Tmax = 0.924 | l = −23→31 |
9905 measured reflections |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.039 | H-atom parameters constrained |
wR(F2) = 0.097 | w = 1/[σ2(Fo2) + (0.0364P)2 + 1.3827P] where P = (Fo2 + 2Fc2)/3 |
S = 1.03 | (Δ/σ)max = 0.001 |
2277 reflections | Δρmax = 0.20 e Å−3 |
174 parameters | Δρmin = −0.28 e Å−3 |
0 restraints | Extinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0028 (6) |
C15H10N2OS | V = 2489.90 (17) Å3 |
Mr = 266.31 | Z = 8 |
Orthorhombic, Pbca | Mo Kα radiation |
a = 11.7737 (5) Å | µ = 0.25 mm−1 |
b = 8.1122 (3) Å | T = 293 K |
c = 26.0694 (10) Å | 0.38 × 0.35 × 0.32 mm |
Agilent Xcalibur Atlas Gemini Ultra CCD diffractometer | 2277 independent reflections |
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2010) | 1826 reflections with I > 2σ(I) |
Tmin = 0.911, Tmax = 0.924 | Rint = 0.029 |
9905 measured reflections |
R[F2 > 2σ(F2)] = 0.039 | 0 restraints |
wR(F2) = 0.097 | H-atom parameters constrained |
S = 1.03 | Δρmax = 0.20 e Å−3 |
2277 reflections | Δρmin = −0.28 e Å−3 |
174 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
S1 | 0.45576 (4) | 0.18140 (6) | 0.52857 (2) | 0.04458 (19) | |
O1 | 0.75080 (13) | 0.5194 (2) | 0.54191 (6) | 0.0570 (4) | |
N1 | 0.61252 (13) | 0.36927 (19) | 0.58004 (6) | 0.0374 (4) | |
N2 | 0.48456 (15) | 0.2302 (2) | 0.62773 (7) | 0.0481 (4) | |
C1 | 0.7132 (2) | 0.4616 (3) | 0.34806 (9) | 0.0636 (7) | |
H1A | 0.7911 | 0.4271 | 0.3497 | 0.095* | |
H1B | 0.7096 | 0.5798 | 0.3482 | 0.095* | |
H1C | 0.6792 | 0.4202 | 0.3172 | 0.095* | |
C2 | 0.64986 (18) | 0.3952 (3) | 0.39380 (8) | 0.0466 (5) | |
C3 | 0.55839 (19) | 0.2897 (3) | 0.38835 (8) | 0.0503 (6) | |
H3 | 0.5351 | 0.2601 | 0.3555 | 0.060* | |
C4 | 0.50108 (19) | 0.2273 (3) | 0.42974 (8) | 0.0462 (5) | |
H4 | 0.4396 | 0.1571 | 0.4248 | 0.055* | |
C5 | 0.53490 (16) | 0.2692 (2) | 0.47915 (7) | 0.0379 (5) | |
C6 | 0.62652 (15) | 0.3757 (2) | 0.48622 (7) | 0.0364 (4) | |
C7 | 0.68198 (17) | 0.4383 (2) | 0.44302 (8) | 0.0438 (5) | |
H7 | 0.7422 | 0.5109 | 0.4475 | 0.053* | |
C8 | 0.66993 (16) | 0.4285 (2) | 0.53662 (7) | 0.0398 (5) | |
C9 | 0.52023 (16) | 0.2624 (2) | 0.58172 (8) | 0.0386 (5) | |
C10 | 0.55487 (18) | 0.3226 (3) | 0.65964 (8) | 0.0461 (5) | |
C11 | 0.63516 (17) | 0.4092 (2) | 0.63143 (8) | 0.0438 (5) | |
C12 | 0.7143 (2) | 0.5112 (3) | 0.65415 (10) | 0.0635 (7) | |
H12 | 0.7689 | 0.5669 | 0.6351 | 0.076* | |
C13 | 0.7076 (3) | 0.5259 (4) | 0.70691 (10) | 0.0807 (9) | |
H13 | 0.7590 | 0.5940 | 0.7238 | 0.097* | |
C14 | 0.6269 (3) | 0.4423 (4) | 0.73537 (10) | 0.0780 (8) | |
H14 | 0.6248 | 0.4565 | 0.7708 | 0.094* | |
C15 | 0.5500 (2) | 0.3393 (3) | 0.71257 (9) | 0.0635 (7) | |
H15 | 0.4964 | 0.2823 | 0.7319 | 0.076* |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0453 (3) | 0.0446 (3) | 0.0439 (3) | −0.0113 (2) | 0.0033 (2) | −0.0054 (2) |
O1 | 0.0457 (8) | 0.0675 (10) | 0.0579 (9) | −0.0228 (8) | −0.0004 (7) | −0.0013 (8) |
N1 | 0.0372 (9) | 0.0359 (8) | 0.0390 (9) | −0.0022 (7) | −0.0023 (7) | −0.0007 (7) |
N2 | 0.0501 (10) | 0.0510 (10) | 0.0430 (10) | −0.0068 (9) | 0.0010 (8) | 0.0020 (8) |
C1 | 0.0615 (15) | 0.0777 (17) | 0.0516 (14) | 0.0096 (13) | 0.0139 (11) | 0.0128 (12) |
C2 | 0.0450 (12) | 0.0503 (12) | 0.0446 (12) | 0.0131 (11) | 0.0070 (9) | 0.0055 (10) |
C3 | 0.0571 (13) | 0.0532 (13) | 0.0405 (12) | 0.0106 (11) | −0.0017 (10) | −0.0021 (10) |
C4 | 0.0462 (11) | 0.0455 (11) | 0.0469 (12) | 0.0013 (10) | −0.0028 (10) | −0.0043 (10) |
C5 | 0.0373 (10) | 0.0337 (10) | 0.0426 (11) | 0.0062 (9) | 0.0029 (8) | 0.0004 (8) |
C6 | 0.0332 (9) | 0.0359 (10) | 0.0402 (10) | 0.0072 (8) | 0.0000 (8) | 0.0007 (8) |
C7 | 0.0367 (10) | 0.0436 (11) | 0.0511 (13) | 0.0063 (9) | 0.0046 (9) | 0.0070 (9) |
C8 | 0.0348 (10) | 0.0390 (10) | 0.0458 (12) | 0.0023 (9) | 0.0017 (9) | 0.0023 (9) |
C9 | 0.0388 (11) | 0.0334 (10) | 0.0437 (11) | 0.0009 (9) | 0.0002 (9) | 0.0007 (8) |
C10 | 0.0506 (12) | 0.0453 (12) | 0.0425 (12) | 0.0023 (10) | −0.0040 (10) | −0.0003 (9) |
C11 | 0.0474 (11) | 0.0414 (11) | 0.0426 (11) | 0.0025 (10) | −0.0076 (9) | −0.0007 (9) |
C12 | 0.0667 (16) | 0.0666 (15) | 0.0572 (15) | −0.0181 (13) | −0.0133 (12) | −0.0018 (12) |
C13 | 0.097 (2) | 0.089 (2) | 0.0560 (16) | −0.0283 (18) | −0.0232 (15) | −0.0049 (14) |
C14 | 0.099 (2) | 0.091 (2) | 0.0431 (14) | −0.0121 (18) | −0.0148 (14) | −0.0053 (13) |
C15 | 0.0733 (16) | 0.0757 (17) | 0.0416 (13) | −0.0061 (14) | −0.0016 (11) | 0.0042 (11) |
S1—C9 | 1.711 (2) | C4—C5 | 1.390 (3) |
S1—C5 | 1.742 (2) | C4—H4 | 0.9300 |
O1—C8 | 1.212 (2) | C5—C6 | 1.394 (3) |
N1—C9 | 1.391 (2) | C6—C7 | 1.397 (3) |
N1—C8 | 1.403 (2) | C6—C8 | 1.473 (3) |
N1—C11 | 1.404 (2) | C7—H7 | 0.9300 |
N2—C9 | 1.297 (3) | C10—C15 | 1.388 (3) |
N2—C10 | 1.392 (3) | C10—C11 | 1.388 (3) |
C1—C2 | 1.506 (3) | C11—C12 | 1.380 (3) |
C1—H1A | 0.9600 | C12—C13 | 1.383 (3) |
C1—H1B | 0.9600 | C12—H12 | 0.9300 |
C1—H1C | 0.9600 | C13—C14 | 1.383 (4) |
C2—C7 | 1.382 (3) | C13—H13 | 0.9300 |
C2—C3 | 1.383 (3) | C14—C15 | 1.368 (4) |
C3—C4 | 1.370 (3) | C14—H14 | 0.9300 |
C3—H3 | 0.9300 | C15—H15 | 0.9300 |
C9—S1—C5 | 101.80 (10) | C2—C7—H7 | 119.0 |
C9—N1—C8 | 127.96 (16) | C6—C7—H7 | 119.0 |
C9—N1—C11 | 105.20 (16) | O1—C8—N1 | 119.66 (18) |
C8—N1—C11 | 126.82 (16) | O1—C8—C6 | 123.41 (18) |
C9—N2—C10 | 104.57 (17) | N1—C8—C6 | 116.93 (17) |
C2—C1—H1A | 109.5 | N2—C9—N1 | 114.04 (17) |
C2—C1—H1B | 109.5 | N2—C9—S1 | 121.86 (16) |
H1A—C1—H1B | 109.5 | N1—C9—S1 | 124.09 (14) |
C2—C1—H1C | 109.5 | C15—C10—C11 | 120.4 (2) |
H1A—C1—H1C | 109.5 | C15—C10—N2 | 128.4 (2) |
H1B—C1—H1C | 109.5 | C11—C10—N2 | 111.14 (18) |
C7—C2—C3 | 117.69 (19) | C12—C11—C10 | 122.4 (2) |
C7—C2—C1 | 120.6 (2) | C12—C11—N1 | 132.6 (2) |
C3—C2—C1 | 121.7 (2) | C10—C11—N1 | 105.04 (17) |
C4—C3—C2 | 122.1 (2) | C11—C12—C13 | 116.1 (2) |
C4—C3—H3 | 119.0 | C11—C12—H12 | 121.9 |
C2—C3—H3 | 119.0 | C13—C12—H12 | 121.9 |
C3—C4—C5 | 119.9 (2) | C12—C13—C14 | 122.0 (2) |
C3—C4—H4 | 120.0 | C12—C13—H13 | 119.0 |
C5—C4—H4 | 120.0 | C14—C13—H13 | 119.0 |
C4—C5—C6 | 119.70 (18) | C15—C14—C13 | 121.4 (2) |
C4—C5—S1 | 115.59 (15) | C15—C14—H14 | 119.3 |
C6—C5—S1 | 124.71 (15) | C13—C14—H14 | 119.3 |
C5—C6—C7 | 118.68 (18) | C14—C15—C10 | 117.6 (2) |
C5—C6—C8 | 124.49 (17) | C14—C15—H15 | 121.2 |
C7—C6—C8 | 116.83 (18) | C10—C15—H15 | 121.2 |
C2—C7—C6 | 121.9 (2) |
Cg1 is the centroid of the N1/N2/C9–C11 ring. |
D—H···A | D—H | H···A | D···A | D—H···A |
C12—H12···Cg1i | 0.93 | 2.90 | 3.765 (3) | 156 |
Symmetry code: (i) −x+3/2, y+1/2, z. |
Experimental details
Crystal data | |
Chemical formula | C15H10N2OS |
Mr | 266.31 |
Crystal system, space group | Orthorhombic, Pbca |
Temperature (K) | 293 |
a, b, c (Å) | 11.7737 (5), 8.1122 (3), 26.0694 (10) |
V (Å3) | 2489.90 (17) |
Z | 8 |
Radiation type | Mo Kα |
µ (mm−1) | 0.25 |
Crystal size (mm) | 0.38 × 0.35 × 0.32 |
Data collection | |
Diffractometer | Agilent Xcalibur Atlas Gemini Ultra CCD |
Absorption correction | Multi-scan (CrysAlis PRO; Agilent, 2010) |
Tmin, Tmax | 0.911, 0.924 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 9905, 2277, 1826 |
Rint | 0.029 |
(sin θ/λ)max (Å−1) | 0.602 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.039, 0.097, 1.03 |
No. of reflections | 2277 |
No. of parameters | 174 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.20, −0.28 |
Computer programs: CrysAlis PRO (Agilent, 2010), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), OLEX2 (Dolomanov et al., 2009).
Cg1 is the centroid of the N1/N2/C9–C11 ring. |
D—H···A | D—H | H···A | D···A | D—H···A |
C12—H12···Cg1i | 0.93 | 2.90 | 3.765 (3) | 156 |
Symmetry code: (i) −x+3/2, y+1/2, z. |
Acknowledgements
This work was supported financially by the Priority Academic Program Development of Jiangsu Higher Education Institutions.
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
Owing to the promising biological activities as antimicrobial agents against bacteria, yeast and fungi, imidazo[2,1-b][1,3]thiazinones have been studied (van der Helm et al., 1987). In the past decades, most of these investigations were carried out with imidazole derivatives (Dolbier et al., 1994; Sekar et al., 2011). We herein present the structure of the title compound C15H10N2OS, prepared from the reaction of 2-iodo-5-methylbenzoyl chloride with 2-mercaptobenzimidazole.
In the crystal structure, the title compound adopts an essentially planar conformation (Fig. 1), with the maximum atom deviation from the least-squares plane to the four-membered fused-ring system = 0.137 (6) Å]. The dihedral angles between the benzimidazole ring (N1–C15) and the thiazine ring (S1–C9) = 3.18 (5) °, the benzene ring (C2–C7) and the thiazine ring (S1–C9) = 0.38 (6)° and the benzimidazole ring (N1–C15) and the benzene ring (C2–C7) = 3.55 (6)°.
The crystal packing is stabilized by weak intermolecular π–π interactions involving the six-membered aromatic rings: (a) the thiazine ring S1–C9 (ring 1) and the benzene ring C10–C15i (ring 2) of the benzimazole moiety [ring centroid separation = 3.628 (8) Å: symmetry code (i) -x + 1, -y + 1, -z + 1]; (b) between the benzene ring C2–C7 (ring 3) and ring C2–C7i = 3.817 (6) Å; (c) between ring 3···and ring 2i = 3.536 (4) Å. There are also C—H···π interactions present.