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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Oct 12;67(Pt 11):o2937. doi: 10.1107/S1600536811041389

1-Decyl-6-nitro-1H-benzimidazol-2(3H)-one

Younes Ouzidan a,*, Youssef Kandri Rodi a, El Mokhtar Essassi b, Santiago V Luis c, Michael Bolte d, Lahcen El Ammari e
PMCID: PMC3247349  PMID: 22219967

Abstract

The title mol­ecule, C17H25N3O3, is built up from fused six- and five-membered rings linked to a –C10H21 chain. The fused-ring system is essentially planar, the largest deviation from the mean plane being 0.009 (2) Å. The chain is roughly perpendic­ular to this plane, making a dihedral angle of 79.5 (2)°. In the crystal, N—H⋯O hydrogen bonds build infinite chains along [010]. There are channels in the structure containing disordered hexane. The contribution of this solvent to the scattering power was suppressed using the SQUEEZE option in PLATON [Spek (2009). Acta Cryst. D65, 148–155].

Related literature

For the pharmacological and biochemical properties of related compounds, 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). graphic file with name e-67-o2937-scheme1.jpg

Experimental

Crystal data

  • C17H25N3O3

  • M r = 319.40

  • Monoclinic, Inline graphic

  • a = 32.9827 (6) Å

  • b = 4.55881 (9) Å

  • c = 29.3435 (5) Å

  • β = 109.481 (2)°

  • V = 4159.56 (13) Å3

  • Z = 8

  • Cu Kα radiation

  • μ = 0.57 mm−1

  • T = 206 K

  • 0.15 × 0.11 × 0.05 mm

Data collection

  • Agilent SuperNova Dual (Cu at zero) Atlas diffractometer

  • Absorption correction: analytical [CrysAlis PRO (Agilent, 2011) based on expressions derived by Clark & Reid (1995)] T min = 0.952, T max = 0.985

  • 20838 measured reflections

  • 4129 independent reflections

  • 3475 reflections with I > 2σ(I)

  • R int = 0.029

Refinement

  • R[F 2 > 2σ(F 2)] = 0.041

  • wR(F 2) = 0.126

  • S = 1.09

  • 4129 reflections

  • 208 parameters

  • H-atom parameters constrained

  • Δρmax = 0.16 e Å−3

  • Δρmin = −0.17 e Å−3

Data collection: CrysAlis PRO (Agilent, 2011); cell refinement: 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: XP (Sheldrick, 2008); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811041389/im2324sup1.cif

e-67-o2937-sup1.cif (25.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811041389/im2324Isup2.hkl

e-67-o2937-Isup2.hkl (198.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811041389/im2324Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1⋯O1i 0.86 1.88 2.743 (1) 178

Symmetry code: (i) Inline graphic.

supplementary crystallographic information

Comment

Benzimidazoles are very useful intermediates/subunits for the development of molecules of pharmaceutical or biological interest. Benzimidazole derivatives have found applications in diverse therapeutic areas including anti-ulcers, anti-hypertensives, anti-virals, anti-fungals and 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 1-bromodecane with 5-nitro-1,3-dihydro-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 molecular structure of 1-decyl-6-nitro-1,3-dihydro-benzimidazol-2-one is built up from two fused six-and five-membered rings linked to a C10H21 chain as schown in Fg.1. The fused rings are essentially planar, with maximum deviations of 0.008 (2) Å and -0.004 (2) Å for C2 and N1, respectively. The dihedral angle between them does not exceed 0.68 (7)°. The torsional angles C7–N2–C11–C12 and C17–C18–C19–C20 are -98.4 (2) ° and 176.7 (2)°, respectively. N1—H···O1 hydrogen bonds build up infinite one-dimensional chains along the [0 1 0] direction as shown in Fig.2 and Table 1.

Experimental

To 5-nitro-1,3-dihydro-benzimidazol-2-one (0.2 g, 1.1 mmol), potassium carbonate (0.30 g, 2.2 mmol) and tetra-n-butylammonium bromide (0.07 g, 0.2 mmol) in DMF (15 ml) was added 1-bromodecane (0.34 ml, 1.65 mmol). Stirring was continued at room temperature for 6 h. The precipitated salt was removed by filtration and the filtrate was concentrated under reduced pressure. The residue was separated by chromatography on a column of silica gel with ethyl acetate/hexane (1/2) as eluent. Colorless crystals were isolated when the solvent was allowed to evaporate (yield: 27%).

Refinement

There are channels in the structure containing disordered hexane. The contribution of this solvent to the scattering power was suppressed using the SQUEEZE option in PLATON (Spek, 2009) and the reflections were merged.

H atoms were located in a difference map and treated as riding with C—H = 0.93 Å for all H atoms with Uiso(H) = 1.2 Ueq(aromatic, methine)and Uiso(H) = 1.5 Ueq(methyl).

Figures

Fig. 1.

Fig. 1.

Molecular structure of the title compound with displacement ellipsoids are drawn at the 50% probability level. H atoms are represented as small circles.

Fig. 2.

Fig. 2.

Packing diagram.

Crystal data

C17H25N3O3 F(000) = 1376
Mr = 319.40 Dx = 1.020 Mg m3
Monoclinic, C2/c Cu Kα radiation, λ = 1.54184 Å
Hall symbol: -C 2yc Cell parameters from 8979 reflections
a = 32.9827 (6) Å θ = 2.8–73.1°
b = 4.55881 (9) Å µ = 0.57 mm1
c = 29.3435 (5) Å T = 206 K
β = 109.481 (2)° Block, colourless
V = 4159.56 (13) Å3 0.15 × 0.11 × 0.05 mm
Z = 8

Data collection

Agilent SuperNova Dual (Cu at zero) Atlas diffractometer 4129 independent reflections
Radiation source: fine-focus sealed tube 3475 reflections with I > 2σ(I)
mirror Rint = 0.029
Detector resolution: 0.4051 pixels mm-1 θmax = 73.3°, θmin = 2.8°
ω scans h = −40→40
Absorption correction: analytical [CrysAlis PRO (Agilent, 2011) based on expressions derived by Clark & Reid (1995)] k = −4→5
Tmin = 0.952, Tmax = 0.985 l = −36→36
20838 measured reflections

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)] = 0.041 Hydrogen site location: difference Fourier map
wR(F2) = 0.126 H-atom parameters constrained
S = 1.09 w = 1/[σ2(Fo2) + (0.0706P)2 + 0.8537P] where P = (Fo2 + 2Fc2)/3
4129 reflections (Δ/σ)max = 0.001
208 parameters Δρmax = 0.16 e Å3
0 restraints Δρmin = −0.17 e Å3

Special details

Experimental. CrysAlisPro, Agilent Technologies, Version 1.171.35.11 (release 16-05-2011 CrysAlis171 .NET) Analytical numeric absorption correction using a multifaceted crystal model based on expressions derived by R.C. Clark & J.S. Reid. Clark & Reid (1995).
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 > 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
N1 0.76316 (3) 0.5176 (2) 0.70158 (3) 0.0389 (3)
H1 0.7727 0.4612 0.7312 0.047*
N2 0.72508 (3) 0.7438 (2) 0.63471 (3) 0.0319 (2)
N3 0.80707 (4) 0.2956 (3) 0.53894 (4) 0.0493 (3)
O1 0.70806 (3) 0.8310 (2) 0.70415 (3) 0.0459 (3)
O2 0.83330 (4) 0.1068 (3) 0.53903 (4) 0.0817 (4)
O3 0.78870 (3) 0.4442 (2) 0.50339 (3) 0.0571 (3)
C1 0.77940 (3) 0.4278 (3) 0.66624 (4) 0.0337 (3)
C2 0.75516 (3) 0.5736 (3) 0.62357 (4) 0.0304 (3)
C3 0.76366 (3) 0.5367 (3) 0.58100 (4) 0.0341 (3)
H3 0.7482 0.6341 0.5527 0.041*
C4 0.79688 (4) 0.3445 (3) 0.58314 (4) 0.0384 (3)
C5 0.82078 (4) 0.1954 (3) 0.62471 (5) 0.0451 (3)
H5 0.8425 0.0676 0.6240 0.054*
C6 0.81208 (4) 0.2379 (3) 0.66730 (4) 0.0433 (3)
H6 0.8278 0.1413 0.6956 0.052*
C7 0.72984 (3) 0.7087 (3) 0.68291 (4) 0.0350 (3)
C11 0.69093 (3) 0.9198 (3) 0.60136 (4) 0.0325 (3)
H11A 0.7026 1.0276 0.5800 0.039*
H11B 0.6806 1.0613 0.6197 0.039*
C12 0.65344 (3) 0.7327 (3) 0.57121 (4) 0.0342 (3)
H12A 0.6418 0.6247 0.5925 0.041*
H12B 0.6637 0.5915 0.5529 0.041*
C13 0.61786 (4) 0.9169 (3) 0.53654 (4) 0.0355 (3)
H13A 0.6063 1.0490 0.5551 0.043*
H13B 0.6300 1.0352 0.5168 0.043*
C14 0.58145 (4) 0.7315 (3) 0.50369 (4) 0.0380 (3)
H14A 0.5691 0.6155 0.5235 0.046*
H14B 0.5931 0.5970 0.4856 0.046*
C15 0.54594 (4) 0.9122 (3) 0.46821 (4) 0.0403 (3)
H15A 0.5584 1.0310 0.4488 0.048*
H15B 0.5339 1.0442 0.4863 0.048*
C16 0.50987 (4) 0.7262 (3) 0.43470 (5) 0.0409 (3)
H16A 0.5220 0.5927 0.4170 0.049*
H16B 0.4973 0.6089 0.4541 0.049*
C17 0.47449 (4) 0.9044 (3) 0.39880 (5) 0.0417 (3)
H17A 0.4611 1.0287 0.4165 0.050*
H17B 0.4873 1.0311 0.3808 0.050*
C18 0.43994 (4) 0.7188 (3) 0.36328 (5) 0.0444 (3)
H18A 0.4535 0.5884 0.3466 0.053*
H18B 0.4263 0.5982 0.3812 0.053*
C19 0.40558 (4) 0.8947 (3) 0.32606 (5) 0.0530 (4)
H19A 0.3908 1.0171 0.3426 0.064*
H19B 0.4193 1.0233 0.3092 0.064*
C20 0.37271 (5) 0.7073 (4) 0.28924 (6) 0.0673 (5)
H20A 0.3528 0.8315 0.2659 0.101*
H20B 0.3575 0.5894 0.3053 0.101*
H20C 0.3871 0.5820 0.2732 0.101*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0368 (5) 0.0594 (7) 0.0176 (4) −0.0018 (5) 0.0051 (3) 0.0043 (4)
N2 0.0304 (4) 0.0432 (6) 0.0192 (4) −0.0013 (4) 0.0046 (3) −0.0007 (4)
N3 0.0505 (6) 0.0633 (8) 0.0392 (6) 0.0032 (6) 0.0218 (5) −0.0011 (5)
O1 0.0411 (4) 0.0714 (7) 0.0241 (4) −0.0004 (4) 0.0095 (3) −0.0087 (4)
O2 0.0945 (9) 0.1005 (10) 0.0648 (7) 0.0446 (8) 0.0461 (7) 0.0090 (7)
O3 0.0644 (6) 0.0789 (8) 0.0333 (5) 0.0066 (5) 0.0236 (4) 0.0067 (5)
C1 0.0310 (5) 0.0458 (7) 0.0217 (5) −0.0058 (5) 0.0051 (4) 0.0020 (4)
C2 0.0287 (5) 0.0372 (6) 0.0228 (5) −0.0059 (4) 0.0054 (4) −0.0003 (4)
C3 0.0357 (5) 0.0422 (7) 0.0227 (5) −0.0028 (5) 0.0075 (4) 0.0027 (4)
C4 0.0390 (6) 0.0479 (7) 0.0299 (6) −0.0012 (5) 0.0137 (5) −0.0006 (5)
C5 0.0398 (6) 0.0542 (8) 0.0399 (6) 0.0078 (6) 0.0115 (5) 0.0037 (6)
C6 0.0393 (6) 0.0544 (8) 0.0312 (6) 0.0046 (6) 0.0050 (5) 0.0098 (5)
C7 0.0316 (5) 0.0510 (7) 0.0199 (5) −0.0082 (5) 0.0052 (4) −0.0048 (5)
C11 0.0329 (5) 0.0361 (6) 0.0251 (5) −0.0005 (5) 0.0050 (4) −0.0008 (4)
C12 0.0330 (6) 0.0345 (6) 0.0299 (5) −0.0011 (5) 0.0037 (4) −0.0006 (5)
C13 0.0330 (5) 0.0337 (7) 0.0341 (6) 0.0002 (5) 0.0037 (4) −0.0001 (5)
C14 0.0349 (6) 0.0345 (7) 0.0366 (6) 0.0005 (5) 0.0013 (5) −0.0007 (5)
C15 0.0350 (6) 0.0365 (7) 0.0403 (6) 0.0008 (5) 0.0003 (5) −0.0010 (5)
C16 0.0367 (6) 0.0362 (7) 0.0403 (6) 0.0005 (5) 0.0000 (5) −0.0011 (5)
C17 0.0366 (6) 0.0381 (7) 0.0413 (6) 0.0013 (5) 0.0006 (5) −0.0014 (5)
C18 0.0372 (6) 0.0414 (7) 0.0436 (7) 0.0011 (5) −0.0011 (5) −0.0024 (5)
C19 0.0447 (7) 0.0489 (9) 0.0499 (7) 0.0060 (6) −0.0050 (6) −0.0026 (6)
C20 0.0483 (8) 0.0687 (11) 0.0608 (9) 0.0079 (7) −0.0140 (7) −0.0078 (8)

Geometric parameters (Å, °)

N1—C7 1.3659 (16) C13—C14 1.5208 (15)
N1—C1 1.3785 (15) C13—H13A 0.9700
N1—H1 0.8600 C13—H13B 0.9700
N2—C7 1.3793 (13) C14—C15 1.5235 (15)
N2—C2 1.3819 (15) C14—H14A 0.9700
N2—C11 1.4612 (14) C14—H14B 0.9700
N3—O2 1.2198 (16) C15—C16 1.5235 (16)
N3—O3 1.2218 (15) C15—H15A 0.9700
N3—C4 1.4612 (15) C15—H15B 0.9700
O1—C7 1.2304 (14) C16—C17 1.5201 (16)
C1—C6 1.3745 (18) C16—H16A 0.9700
C1—C2 1.4077 (15) C16—H16B 0.9700
C2—C3 1.3789 (14) C17—C18 1.5194 (16)
C3—C4 1.3879 (17) C17—H17A 0.9700
C3—H3 0.9300 C17—H17B 0.9700
C4—C5 1.3890 (17) C18—C19 1.5148 (17)
C5—C6 1.3862 (18) C18—H18A 0.9700
C5—H5 0.9300 C18—H18B 0.9700
C6—H6 0.9300 C19—C20 1.5138 (19)
C11—C12 1.5197 (15) C19—H19A 0.9700
C11—H11A 0.9700 C19—H19B 0.9700
C11—H11B 0.9700 C20—H20A 0.9600
C12—C13 1.5234 (15) C20—H20B 0.9600
C12—H12A 0.9700 C20—H20C 0.9600
C12—H12B 0.9700
C7—N1—C1 110.52 (9) C14—C13—H13B 109.0
C7—N1—H1 124.7 C12—C13—H13B 109.0
C1—N1—H1 124.7 H13A—C13—H13B 107.8
C7—N2—C2 109.41 (9) C13—C14—C15 113.41 (10)
C7—N2—C11 123.32 (9) C13—C14—H14A 108.9
C2—N2—C11 127.13 (8) C15—C14—H14A 108.9
O2—N3—O3 122.85 (11) C13—C14—H14B 108.9
O2—N3—C4 118.60 (11) C15—C14—H14B 108.9
O3—N3—C4 118.55 (11) H14A—C14—H14B 107.7
C6—C1—N1 131.94 (10) C14—C15—C16 113.39 (10)
C6—C1—C2 121.76 (10) C14—C15—H15A 108.9
N1—C1—C2 106.31 (10) C16—C15—H15A 108.9
C3—C2—N2 131.46 (10) C14—C15—H15B 108.9
C3—C2—C1 121.41 (10) C16—C15—H15B 108.9
N2—C2—C1 107.12 (9) H15A—C15—H15B 107.7
C2—C3—C4 115.61 (10) C17—C16—C15 113.80 (10)
C2—C3—H3 122.2 C17—C16—H16A 108.8
C4—C3—H3 122.2 C15—C16—H16A 108.8
C3—C4—C5 123.84 (11) C17—C16—H16B 108.8
C3—C4—N3 117.89 (10) C15—C16—H16B 108.8
C5—C4—N3 118.28 (12) H16A—C16—H16B 107.7
C6—C5—C4 119.74 (12) C18—C17—C16 113.88 (10)
C6—C5—H5 120.1 C18—C17—H17A 108.8
C4—C5—H5 120.1 C16—C17—H17A 108.8
C1—C6—C5 117.64 (11) C18—C17—H17B 108.8
C1—C6—H6 121.2 C16—C17—H17B 108.8
C5—C6—H6 121.2 H17A—C17—H17B 107.7
O1—C7—N1 127.86 (10) C19—C18—C17 114.19 (11)
O1—C7—N2 125.50 (11) C19—C18—H18A 108.7
N1—C7—N2 106.64 (9) C17—C18—H18A 108.7
N2—C11—C12 112.17 (10) C19—C18—H18B 108.7
N2—C11—H11A 109.2 C17—C18—H18B 108.7
C12—C11—H11A 109.2 H18A—C18—H18B 107.6
N2—C11—H11B 109.2 C20—C19—C18 113.67 (12)
C12—C11—H11B 109.2 C20—C19—H19A 108.8
H11A—C11—H11B 107.9 C18—C19—H19A 108.8
C11—C12—C13 112.06 (10) C20—C19—H19B 108.8
C11—C12—H12A 109.2 C18—C19—H19B 108.8
C13—C12—H12A 109.2 H19A—C19—H19B 107.7
C11—C12—H12B 109.2 C19—C20—H20A 109.5
C13—C12—H12B 109.2 C19—C20—H20B 109.5
H12A—C12—H12B 107.9 H20A—C20—H20B 109.5
C14—C13—C12 112.76 (10) C19—C20—H20C 109.5
C14—C13—H13A 109.0 H20A—C20—H20C 109.5
C12—C13—H13A 109.0 H20B—C20—H20C 109.5

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1···O1i 0.86 1.88 2.743 (1) 178.

Symmetry codes: (i) −x+3/2, y−1/2, −z+3/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: IM2324).

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/S1600536811041389/im2324sup1.cif

e-67-o2937-sup1.cif (25.9KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811041389/im2324Isup2.hkl

e-67-o2937-Isup2.hkl (198.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811041389/im2324Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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