Abstract
The fused five- and six-membered rings in the title compound, C14H12N2O, are essentially planar, the largest deviation from the mean plane being 0.023 (2) Å. The dihedral angle between the benzimidazole mean plane and the phenyl ring is 68.50 (6)°. In the crystal, each molecule is linked to its symmetry equivalent created by a crystallographic inversion center by pairs of N—H⋯O hydrogen bonds, forming inversion dimers.
Related literature
For the biological activity of benzimidazole derivatives, see: Gravatt et al. (1994 ▶); Horton et al. (2003 ▶); Kim et al. (1996 ▶); Roth et al. (1997 ▶). For related structures, see: Ouzidan et al. (2011a ▶,b ▶).
Experimental
Crystal data
C14H12N2O
M r = 224.26
Monoclinic,
a = 13.8652 (7) Å
b = 5.7975 (3) Å
c = 14.9337 (7) Å
β = 109.5346 (12)°
V = 1131.33 (10) Å3
Z = 4
Mo Kα radiation
μ = 0.09 mm−1
T = 298 K
0.50 × 0.44 × 0.28 mm
Data collection
Bruker CCD three-circle diffractometer
Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.959, T max = 0.977
9007 measured reflections
3392 independent reflections
2514 reflections with I > 2σ(I)
R int = 0.020
Refinement
R[F 2 > 2σ(F 2)] = 0.045
wR(F 2) = 0.126
S = 1.05
3392 reflections
166 parameters
H-atom parameters constrained
Δρmax = 0.21 e Å−3
Δρmin = −0.19 e Å−3
Data collection: SMART (Bruker, 1997 ▶); cell refinement: SAINT (Bruker, 1997 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: XP (Sheldrick, 2008 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶).
Supplementary Material
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S160053681102455X/im2298sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681102455X/im2298Isup2.hkl
Table 1. Hydrogen-bond geometry (Å, °).
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
---|---|---|---|---|
N1—H1⋯O1i | 0.86 | 2.03 | 2.845 (1) | 158 |
Symmetry code: (i) .
supplementary crystallographic information
Comment
Benzimidazoles are very useful intermediates/subunits for the development of molecules of pharmaceutical or biological interest and its derivatives are an important class of bioactive molecules in the field of drugs and pharmaceuticals. Benzimidazole derivatives have found applications in diverse therapeutic areas including anti-ulcers, anti-hypertensives, anti-virals, anti-fungals, anti-cancers, (Gravatt et al. 1994; Horton et al. 2003; Kim et al. 1996; Roth et al. 1997).
As a continuation of our research work devoted to the development of substituted benzimidazol-2-one derivatives (Ouzidan et al., 2011a, 2011b), we report in this paper the synthesis of a new benzimidazol-2-one derivative by action of benzyl chloride with 1H-benzimidazol-2-one in the presence of a catalytic quantity of tetra-n-butylammonium bromide under mild conditions to furnish the title compound (Scheme 1).
The two fused five and six-membered rings are almost planar with the maximum deviation of 0.023 (2) Å from C2. The dihedral angle between the benzimidazole system and the phenyl ring is 68.50 (6)° (Fig.1). In the crystal structure each molecule is linked to its symmetry equivalent created by the crystallographic inversion center by N–H···O hydrogen bonds to form pseudo-dimers as shown in Fg.2.
Experimental
To 1H-benzimidazol-2-one (0.2 g, 1.5 mmol), potassium carbonate (0.41 g, 3 mmol) and tetra-n-butylammonium bromide (0.05 g, 0.15 mmol) in DMF (15 ml) was added benzyl chloride (0.34 ml, 3 mmol). Stirring was continued at room temperature for 6 h. The salt was removed by filtration and the filtrate concentrated under reduced pressure. The residue was separated by chromatography on a column of silica gel with ethyl acetate/hexane (1/2) as eluent. The compound was recrystallized from ethanol to give colorless crystals (yield: 12%).
Refinement
H atoms were located in a difference map and treated as riding with C—H = 0.93 Å, and 0.97 Å for aromatic and methylene H atoms, respectively, and with Uiso(H) = 1.2 Ueq(C).
Figures
Crystal data
C14H12N2O | F(000) = 472 |
Mr = 224.26 | Dx = 1.317 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2yn | Cell parameters from 3392 reflections |
a = 13.8652 (7) Å | θ = 1.7–30.5° |
b = 5.7975 (3) Å | µ = 0.09 mm−1 |
c = 14.9337 (7) Å | T = 298 K |
β = 109.5346 (12)° | Prism, colourless |
V = 1131.33 (10) Å3 | 0.50 × 0.44 × 0.28 mm |
Z = 4 |
Data collection
Bruker CCD three-circle diffractometer | 3392 independent reflections |
Radiation source: fine-focus sealed tube | 2514 reflections with I > 2σ(I) |
graphite | Rint = 0.020 |
ω scans | θmax = 30.5°, θmin = 1.7° |
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) | h = −18→19 |
Tmin = 0.959, Tmax = 0.977 | k = −8→8 |
9007 measured reflections | l = −16→21 |
Refinement
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.045 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.126 | H-atom parameters constrained |
S = 1.05 | w = 1/[σ2(Fo2) + (0.0584P)2 + 0.1866P] where P = (Fo2 + 2Fc2)/3 |
3392 reflections | (Δ/σ)max < 0.001 |
166 parameters | Δρmax = 0.21 e Å−3 |
0 restraints | Δρmin = −0.19 e Å−3 |
Special details
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. |
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
x | y | z | Uiso*/Ueq | ||
O1 | 0.59908 (7) | 0.79068 (16) | 0.53088 (6) | 0.0462 (2) | |
N1 | 0.46509 (7) | 0.82117 (17) | 0.38695 (7) | 0.0391 (2) | |
H1 | 0.4387 | 0.9497 | 0.3958 | 0.066 (5)* | |
C1 | 0.54932 (8) | 0.72077 (19) | 0.45072 (8) | 0.0354 (2) | |
N2 | 0.56888 (7) | 0.52373 (16) | 0.40851 (7) | 0.0350 (2) | |
C2 | 0.49440 (8) | 0.49698 (19) | 0.31953 (8) | 0.0343 (2) | |
C3 | 0.47930 (10) | 0.3259 (2) | 0.25181 (9) | 0.0429 (3) | |
H3 | 0.5232 | 0.2003 | 0.2611 | 0.050 (4)* | |
C4 | 0.39558 (11) | 0.3498 (3) | 0.16918 (9) | 0.0513 (3) | |
H4 | 0.3834 | 0.2382 | 0.1220 | 0.060 (4)* | |
C5 | 0.32981 (10) | 0.5368 (3) | 0.15565 (9) | 0.0510 (3) | |
H5 | 0.2745 | 0.5477 | 0.0995 | 0.058 (4)* | |
C6 | 0.34472 (10) | 0.7081 (2) | 0.22409 (9) | 0.0455 (3) | |
H6 | 0.3002 | 0.8326 | 0.2151 | 0.056 (4)* | |
C7 | 0.42820 (9) | 0.68586 (19) | 0.30576 (8) | 0.0357 (2) | |
C8 | 0.64791 (9) | 0.3581 (2) | 0.45689 (8) | 0.0378 (2) | |
H8A | 0.6173 | 0.2060 | 0.4513 | 0.044 (4)* | |
H8B | 0.6744 | 0.3968 | 0.5239 | 0.041 (3)* | |
C11 | 0.73601 (8) | 0.34906 (19) | 0.41875 (8) | 0.0354 (2) | |
C12 | 0.75053 (11) | 0.1565 (2) | 0.36992 (10) | 0.0491 (3) | |
H12 | 0.7048 | 0.0339 | 0.3591 | 0.061 (5)* | |
C13 | 0.83286 (13) | 0.1452 (3) | 0.33705 (12) | 0.0638 (4) | |
H13 | 0.8416 | 0.0160 | 0.3036 | 0.088 (6)* | |
C14 | 0.90122 (13) | 0.3235 (3) | 0.35368 (12) | 0.0659 (4) | |
H14 | 0.9569 | 0.3145 | 0.3324 | 0.085 (6)* | |
C15 | 0.88757 (11) | 0.5165 (3) | 0.40199 (12) | 0.0597 (4) | |
H15 | 0.9338 | 0.6382 | 0.4129 | 0.068 (5)* | |
C16 | 0.80491 (10) | 0.5294 (2) | 0.43437 (10) | 0.0459 (3) | |
H16 | 0.7958 | 0.6601 | 0.4668 | 0.054 (4)* |
Atomic displacement parameters (Å2)
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0430 (5) | 0.0475 (5) | 0.0452 (5) | −0.0005 (4) | 0.0110 (4) | −0.0138 (4) |
N1 | 0.0386 (5) | 0.0356 (5) | 0.0443 (5) | 0.0044 (4) | 0.0155 (4) | −0.0033 (4) |
C1 | 0.0336 (5) | 0.0348 (5) | 0.0411 (6) | −0.0025 (4) | 0.0171 (5) | −0.0040 (4) |
N2 | 0.0330 (4) | 0.0349 (5) | 0.0367 (5) | 0.0019 (4) | 0.0114 (4) | −0.0035 (4) |
C2 | 0.0326 (5) | 0.0368 (5) | 0.0347 (5) | −0.0011 (4) | 0.0130 (4) | 0.0000 (4) |
C3 | 0.0447 (6) | 0.0405 (6) | 0.0429 (6) | 0.0018 (5) | 0.0137 (5) | −0.0065 (5) |
C4 | 0.0515 (7) | 0.0566 (8) | 0.0422 (7) | −0.0042 (6) | 0.0109 (6) | −0.0116 (6) |
C5 | 0.0412 (6) | 0.0656 (9) | 0.0404 (6) | −0.0013 (6) | 0.0060 (5) | 0.0005 (6) |
C6 | 0.0381 (6) | 0.0500 (7) | 0.0479 (7) | 0.0064 (5) | 0.0134 (5) | 0.0065 (6) |
C7 | 0.0346 (5) | 0.0364 (5) | 0.0395 (6) | −0.0003 (4) | 0.0167 (5) | 0.0006 (4) |
C8 | 0.0389 (6) | 0.0371 (6) | 0.0384 (6) | 0.0039 (4) | 0.0141 (5) | 0.0041 (5) |
C11 | 0.0356 (5) | 0.0365 (5) | 0.0327 (5) | 0.0070 (4) | 0.0094 (4) | 0.0053 (4) |
C12 | 0.0516 (7) | 0.0422 (7) | 0.0547 (8) | 0.0073 (6) | 0.0195 (6) | −0.0022 (6) |
C13 | 0.0697 (10) | 0.0637 (9) | 0.0675 (9) | 0.0226 (8) | 0.0354 (8) | −0.0002 (8) |
C14 | 0.0551 (9) | 0.0814 (11) | 0.0728 (10) | 0.0221 (8) | 0.0367 (8) | 0.0184 (9) |
C15 | 0.0445 (7) | 0.0656 (9) | 0.0710 (10) | −0.0033 (7) | 0.0221 (7) | 0.0141 (8) |
C16 | 0.0446 (7) | 0.0432 (6) | 0.0499 (7) | 0.0009 (5) | 0.0158 (5) | 0.0008 (5) |
Geometric parameters (Å, °)
O1—C1 | 1.2332 (14) | C6—H6 | 0.9300 |
N1—C1 | 1.3660 (15) | C8—C11 | 1.5114 (15) |
N1—C7 | 1.3901 (15) | C8—H8A | 0.9700 |
N1—H1 | 0.8600 | C8—H8B | 0.9700 |
C1—N2 | 1.3749 (14) | C11—C16 | 1.3824 (17) |
N2—C2 | 1.3922 (14) | C11—C12 | 1.3845 (17) |
N2—C8 | 1.4546 (14) | C12—C13 | 1.387 (2) |
C2—C3 | 1.3815 (16) | C12—H12 | 0.9300 |
C2—C7 | 1.3991 (15) | C13—C14 | 1.368 (3) |
C3—C4 | 1.3897 (19) | C13—H13 | 0.9300 |
C3—H3 | 0.9300 | C14—C15 | 1.379 (2) |
C4—C5 | 1.387 (2) | C14—H14 | 0.9300 |
C4—H4 | 0.9300 | C15—C16 | 1.3869 (19) |
C5—C6 | 1.3902 (19) | C15—H15 | 0.9300 |
C5—H5 | 0.9300 | C16—H16 | 0.9300 |
C6—C7 | 1.3783 (17) | ||
C1—N1—C7 | 110.31 (9) | N1—C7—C2 | 106.35 (10) |
C1—N1—H1 | 124.8 | N2—C8—C11 | 113.90 (9) |
C7—N1—H1 | 124.8 | N2—C8—H8A | 108.8 |
O1—C1—N1 | 127.38 (11) | C11—C8—H8A | 108.8 |
O1—C1—N2 | 125.88 (11) | N2—C8—H8B | 108.8 |
N1—C1—N2 | 106.74 (10) | C11—C8—H8B | 108.8 |
C1—N2—C2 | 109.46 (9) | H8A—C8—H8B | 107.7 |
C1—N2—C8 | 123.52 (10) | C16—C11—C12 | 119.00 (11) |
C2—N2—C8 | 126.56 (9) | C16—C11—C8 | 120.68 (11) |
C3—C2—N2 | 131.39 (10) | C12—C11—C8 | 120.30 (11) |
C3—C2—C7 | 121.52 (11) | C11—C12—C13 | 120.43 (14) |
N2—C2—C7 | 107.09 (9) | C11—C12—H12 | 119.8 |
C2—C3—C4 | 117.10 (11) | C13—C12—H12 | 119.8 |
C2—C3—H3 | 121.5 | C14—C13—C12 | 120.16 (14) |
C4—C3—H3 | 121.5 | C14—C13—H13 | 119.9 |
C5—C4—C3 | 121.38 (12) | C12—C13—H13 | 119.9 |
C5—C4—H4 | 119.3 | C13—C14—C15 | 120.03 (14) |
C3—C4—H4 | 119.3 | C13—C14—H14 | 120.0 |
C4—C5—C6 | 121.48 (12) | C15—C14—H14 | 120.0 |
C4—C5—H5 | 119.3 | C14—C15—C16 | 120.02 (14) |
C6—C5—H5 | 119.3 | C14—C15—H15 | 120.0 |
C7—C6—C5 | 117.27 (11) | C16—C15—H15 | 120.0 |
C7—C6—H6 | 121.4 | C11—C16—C15 | 120.36 (13) |
C5—C6—H6 | 121.4 | C11—C16—H16 | 119.8 |
C6—C7—N1 | 132.40 (11) | C15—C16—H16 | 119.8 |
C6—C7—C2 | 121.25 (11) |
Hydrogen-bond geometry (Å, °)
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1···O1i | 0.86 | 2.03 | 2.845 (1) | 158 |
Symmetry codes: (i) −x+1, −y+2, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IM2298).
References
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S160053681102455X/im2298sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S160053681102455X/im2298Isup2.hkl