organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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6-Meth­­oxy-2-methyl-1-m-tolyl-1H-benzimidazole hemihydrate

aDepartment of Chemistry and Chemical Engineering, Southeast University, Nanjing, People's Republic of China
*Correspondence e-mail: fanglei24@googlemail.com

(Received 17 May 2011; accepted 2 August 2011; online 6 August 2011)

The title compound, C16H16N2O·0.5H2O, is a substituted 1-phenyl­benzimidazole, which belongs to the class of ATP-site inhibitors of the platelet-derived growth-factor receptor. In the crystal, the components are linked by an O—H⋯N hydrogen bond.

Related literature

For related structures, see: Zhong (2004[Zhong, C.-L. (2004). Bioorg. Med. Chem. 12, 4009-4015.]). For medicinal background, see: Palmer (1998[Palmer, B. D. (1998). J. Med. Chem. 41, 5457-5465.]).

[Scheme 1]

Experimental

Crystal data
  • C16H16N2O·0.5H2O

  • Mr = 261.32

  • Orthorhombic, P b c n

  • a = 16.0752 (16) Å

  • b = 13.9140 (14) Å

  • c = 12.6450 (13) Å

  • V = 2828.3 (5) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 293 K

  • 0.25 × 0.23 × 0.21 mm

Data collection
  • Bruker APEX CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996[Sheldrick, G. M. (1996). SADABS. University of Göttingen, Germany]) Tmin = 0.980, Tmax = 0.983

  • 13133 measured reflections

  • 2720 independent reflections

  • 2018 reflections with I > 2σ(I)

  • Rint = 0.029

Refinement
  • R[F2 > 2σ(F2)] = 0.081

  • wR(F2) = 0.155

  • S = 1.03

  • 2720 reflections

  • 178 parameters

  • H-atom parameters constrained

  • Δρmax = 0.69 e Å−3

  • Δρmin = −0.20 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
O1W—H1W⋯N2 0.85 2.08 2.911 (3) 166

Data collection: SMART (Bruker, 2000[Bruker (2000). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2000[Bruker (2000). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); software used to prepare material for publication: SHELXTL.

Supporting information


Comment top

1-Phenylbenzimidazoles are shown to be a new class of ATP-site inhibitors of the platelet derived growth factor receptor (PDGFR), with clear evidence of the relationship between their molecular features and their inhibitory activity (Palmer, 1998). However, few structure-activity relationship studies involving 1-phenylbenzimidazoles have been published and the QSAR models reported were not completely satisfactory (Zhong, 2004). The synthesis of these compounds is relatively uncomplicated, many methods have been proposed in the past years. We have successfully synthesized the title compound as a key analogue of 1-phenylbenzimidazole.

Related literature top

For related structures, see: Zhong (2004). For medicinal background, see: Palmer (1998).

Experimental top

N-(2-amino-5-methoxyphenyl)-N-m-tolylacetamide (1 g, 3.70 mmol) was dissolved in 40 ml of 18% hydrochloric acid, and the solution was cooled to 0°C. A solution of NaNO2 (0.28 g, 4.07 mmol) in 1 ml of water was added under stirring, and the mixture was stirred for 10 min. Copper powder (1 g) was then added, and the mixture was stirred for 30 min at room temperature. The reaction solution was heated to 70°C and stirred for 3 h. The mixture was extracted with ethyl acetate (2×50 ml), and the extract was washed with a 3% aqueous solution of NaHCO3 and water, respectively. The organic phase was dried over Na2SO4 and evaporated. The residue was purified by column chromatography. Yield 0.46 g (49%).

Refinement top

The H atoms were positioned geometrically and allowed to ride on their parent atoms, with C—H = 0.93–0.96 Å, and Uiso =1.2 or 1.5Ueq(parent atom). The maximum residual electron density, 0.685 e/Å3, is located at 0.7013, 0.6556, 0.0873 (1.319 Å from C2 atom). This can be explained by a little disorder of the C7 methyl group.

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The asymmetric unit of the title compound. Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2] Fig. 2. The dimeric structure of the title compound is built via O—H···N hydrogen bonding between water molecule and N atoms of imidazole rings.
6-Methoxy-2-methyl-1-m-tolyl-1H-benzimidazole hemihydrate top
Crystal data top
C16H16N2O·0.5H2OF(000) = 1112
Mr = 261.32Dx = 1.227 Mg m3
Orthorhombic, PbcnMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2n 2abCell parameters from 2720 reflections
a = 16.0752 (16) Åθ = 2.4–28.0°
b = 13.9140 (14) ŵ = 0.08 mm1
c = 12.6450 (13) ÅT = 293 K
V = 2828.3 (5) Å3Plate-like, colourless
Z = 80.25 × 0.23 × 0.21 mm
Data collection top
Bruker APEX CCD
diffractometer
2720 independent reflections
Radiation source: fine-focus sealed tube2018 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.029
ϕ and ω scansθmax = 26.0°, θmin = 2.5°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 1719
Tmin = 0.980, Tmax = 0.983k = 1717
13133 measured reflectionsl = 1514
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.081H-atom parameters constrained
wR(F2) = 0.155 w = 1/[σ2(Fo2) + (0.0196P)2 + 3.0292P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max < 0.001
2720 reflectionsΔρmax = 0.69 e Å3
178 parametersΔρmin = 0.20 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0037 (5)
Crystal data top
C16H16N2O·0.5H2OV = 2828.3 (5) Å3
Mr = 261.32Z = 8
Orthorhombic, PbcnMo Kα radiation
a = 16.0752 (16) ŵ = 0.08 mm1
b = 13.9140 (14) ÅT = 293 K
c = 12.6450 (13) Å0.25 × 0.23 × 0.21 mm
Data collection top
Bruker APEX CCD
diffractometer
2720 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
2018 reflections with I > 2σ(I)
Tmin = 0.980, Tmax = 0.983Rint = 0.029
13133 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0810 restraints
wR(F2) = 0.155H-atom parameters constrained
S = 1.03Δρmax = 0.69 e Å3
2720 reflectionsΔρmin = 0.20 e Å3
178 parameters
Special details top

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) top
xyzUiso*/Ueq
C10.6204 (2)0.6782 (2)0.2566 (2)0.0725 (8)
H1A0.58510.62530.25390.087*
C20.6771 (2)0.6930 (3)0.1781 (3)0.0851 (10)
H2A0.68090.64970.12230.102*
C30.7285 (2)0.7711 (3)0.1814 (3)0.0863 (11)
H3A0.76710.78000.12740.104*
C40.72472 (19)0.8370 (2)0.2623 (3)0.0789 (10)
C50.66713 (18)0.8218 (2)0.3437 (3)0.0699 (8)
H5A0.66360.86500.39960.084*
C60.61540 (17)0.7422 (2)0.3404 (2)0.0624 (7)
C80.5560 (2)0.6505 (2)0.4939 (2)0.0681 (8)
C90.6135 (2)0.5667 (2)0.4845 (3)0.0848 (10)
H9A0.60200.52150.54010.127*
H9B0.67000.58840.49030.127*
H9C0.60550.53610.41720.127*
C100.4610 (2)0.7482 (2)0.5473 (2)0.0681 (8)
C110.3959 (2)0.7953 (3)0.5984 (3)0.0819 (10)
H11A0.37170.76870.65850.098*
C120.3683 (2)0.8807 (3)0.5596 (3)0.0756 (9)
H12A0.32450.91200.59320.091*
C130.40456 (18)0.9223 (2)0.4699 (2)0.0677 (8)
C140.46999 (17)0.8783 (2)0.4176 (2)0.0611 (7)
H14A0.49460.90560.35830.073*
C150.49675 (18)0.7910 (2)0.4588 (2)0.0592 (7)
C160.4029 (2)1.0538 (3)0.3480 (3)0.0863 (10)
H16A0.37311.11230.33410.129*
H16B0.39791.01160.28830.129*
H16C0.46051.06830.36010.129*
N10.55804 (15)0.72736 (17)0.42521 (18)0.0628 (6)
N20.49971 (19)0.66035 (18)0.5677 (2)0.0764 (7)
O10.36911 (13)1.00859 (17)0.43877 (19)0.0811 (7)
O1W0.50000.5327 (2)0.75000.0961 (11)
H1W0.49120.56680.69530.144*
C70.7786 (3)0.9187 (3)0.2623 (4)0.1196 (16)
H7A0.81380.91660.20110.179*
H7B0.81230.91800.32500.179*
H7C0.74590.97640.26090.179*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.077 (2)0.076 (2)0.0645 (18)0.0169 (17)0.0040 (16)0.0042 (16)
C20.092 (2)0.093 (3)0.070 (2)0.029 (2)0.0057 (19)0.0060 (19)
C30.081 (2)0.104 (3)0.074 (2)0.038 (2)0.0189 (18)0.019 (2)
C40.0568 (18)0.074 (2)0.106 (3)0.0035 (16)0.0035 (18)0.033 (2)
C50.0636 (18)0.0701 (19)0.076 (2)0.0092 (16)0.0030 (15)0.0106 (16)
C60.0602 (17)0.0685 (18)0.0584 (16)0.0054 (15)0.0027 (13)0.0111 (14)
C80.083 (2)0.0562 (17)0.0649 (18)0.0107 (16)0.0003 (16)0.0009 (14)
C90.110 (3)0.066 (2)0.079 (2)0.0055 (19)0.004 (2)0.0036 (17)
C100.077 (2)0.0635 (18)0.0634 (17)0.0187 (16)0.0101 (15)0.0055 (14)
C110.083 (2)0.089 (2)0.074 (2)0.025 (2)0.0264 (18)0.0117 (18)
C120.0671 (19)0.079 (2)0.081 (2)0.0068 (17)0.0137 (17)0.0201 (18)
C130.0566 (17)0.075 (2)0.0714 (19)0.0066 (15)0.0019 (15)0.0158 (16)
C140.0597 (16)0.0658 (17)0.0579 (16)0.0049 (14)0.0025 (13)0.0022 (14)
C150.0563 (15)0.0632 (17)0.0582 (15)0.0087 (14)0.0045 (13)0.0069 (13)
C160.090 (2)0.081 (2)0.088 (2)0.011 (2)0.005 (2)0.0008 (19)
N10.0676 (15)0.0610 (14)0.0599 (13)0.0022 (12)0.0055 (12)0.0042 (11)
N20.0991 (19)0.0625 (15)0.0677 (16)0.0165 (15)0.0114 (15)0.0024 (13)
O10.0725 (13)0.0838 (15)0.0870 (16)0.0143 (12)0.0013 (12)0.0094 (13)
O1W0.144 (3)0.0619 (19)0.082 (2)0.0000.002 (2)0.000
C70.100 (3)0.097 (3)0.163 (4)0.008 (2)0.008 (3)0.013 (3)
Geometric parameters (Å, º) top
C1—C21.363 (5)C10—C111.394 (4)
C1—C61.387 (4)C10—N21.395 (4)
C1—H1A0.9300C11—C121.359 (5)
C2—C31.366 (5)C11—H11A0.9300
C2—H2A0.9300C12—C131.401 (4)
C3—C41.375 (5)C12—H12A0.9300
C3—H3A0.9300C13—C141.385 (4)
C4—C51.400 (4)C13—O11.386 (4)
C4—C71.429 (5)C14—C151.389 (4)
C5—C61.385 (4)C14—H14A0.9300
C5—H5A0.9300C15—N11.391 (4)
C6—N11.429 (3)C16—O11.417 (4)
C8—N21.307 (4)C16—H16A0.9600
C8—N11.378 (4)C16—H16B0.9600
C8—C91.492 (4)C16—H16C0.9600
C9—H9A0.9600O1W—H1W0.8500
C9—H9B0.9600C7—H7A0.9600
C9—H9C0.9600C7—H7B0.9600
C10—C151.392 (4)C7—H7C0.9600
C2—C1—C6119.9 (3)C12—C11—H11A120.4
C2—C1—H1A120.1C10—C11—H11A120.4
C6—C1—H1A120.1C11—C12—C13121.2 (3)
C1—C2—C3120.2 (4)C11—C12—H12A119.4
C1—C2—H2A119.9C13—C12—H12A119.4
C3—C2—H2A119.9C14—C13—O1124.1 (3)
C2—C3—C4121.7 (3)C14—C13—C12121.3 (3)
C2—C3—H3A119.1O1—C13—C12114.7 (3)
C4—C3—H3A119.1C13—C14—C15116.3 (3)
C3—C4—C5118.4 (3)C13—C14—H14A121.9
C3—C4—C7120.2 (4)C15—C14—H14A121.9
C5—C4—C7121.4 (4)C14—C15—N1131.4 (3)
C6—C5—C4119.7 (3)C14—C15—C10123.2 (3)
C6—C5—H5A120.1N1—C15—C10105.4 (3)
C4—C5—H5A120.1O1—C16—H16A109.5
C5—C6—C1120.1 (3)O1—C16—H16B109.5
C5—C6—N1118.8 (3)H16A—C16—H16B109.5
C1—C6—N1121.2 (3)O1—C16—H16C109.5
N2—C8—N1112.6 (3)H16A—C16—H16C109.5
N2—C8—C9124.6 (3)H16B—C16—H16C109.5
N1—C8—C9122.8 (3)C8—N1—C15106.6 (2)
C8—C9—H9A109.5C8—N1—C6126.9 (3)
C8—C9—H9B109.5C15—N1—C6126.4 (2)
H9A—C9—H9B109.5C8—N2—C10105.7 (3)
C8—C9—H9C109.5C13—O1—C16117.2 (2)
H9A—C9—H9C109.5C4—C7—H7A109.5
H9B—C9—H9C109.5C4—C7—H7B109.5
C15—C10—C11118.8 (3)H7A—C7—H7B109.5
C15—C10—N2109.8 (3)C4—C7—H7C109.5
C11—C10—N2131.4 (3)H7A—C7—H7C109.5
C12—C11—C10119.2 (3)H7B—C7—H7C109.5
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1W—H1W···N20.852.082.911 (3)166

Experimental details

Crystal data
Chemical formulaC16H16N2O·0.5H2O
Mr261.32
Crystal system, space groupOrthorhombic, Pbcn
Temperature (K)293
a, b, c (Å)16.0752 (16), 13.9140 (14), 12.6450 (13)
V3)2828.3 (5)
Z8
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.25 × 0.23 × 0.21
Data collection
DiffractometerBruker APEX CCD
diffractometer
Absorption correctionMulti-scan
(SADABS; Sheldrick, 1996)
Tmin, Tmax0.980, 0.983
No. of measured, independent and
observed [I > 2σ(I)] reflections
13133, 2720, 2018
Rint0.029
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.081, 0.155, 1.03
No. of reflections2720
No. of parameters178
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.69, 0.20

Computer programs: SMART (Bruker, 2000), SAINT (Bruker, 2000), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1W—H1W···N20.852.082.911 (3)166.0
 

Acknowledgements

The authors thank the National Natural Science Foundation of China and the Program for Young Excellent Talents in Southeast University for financial support.

References

First citationBruker (2000). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationPalmer, B. D. (1998). J. Med. Chem. 41, 5457–5465.  Web of Science CrossRef CAS Google Scholar
First citationSheldrick, G. M. (1996). SADABS. University of Göttingen, Germany  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationZhong, C.-L. (2004). Bioorg. Med. Chem. 12, 4009–4015.  CrossRef CAS Google Scholar

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