supplementary materials


sj2460 scheme

Acta Cryst. (2008). E64, o964    [ doi:10.1107/S1600536808006405 ]

(E)-2-[2-(2-Thienyl)vinyl]-1H-1,3-benzimidazole

T. Hang and Q. Ye

Abstract top

In the title compound, C13H10N2S, the dihedral angle between the imidazole and thiophene rings is 16.89 (19)°, and the double bond adopts an E configuration. In the crystal structure, N-H...N hydrogen bonds link the molecules into rows along b. There is also evidence of weak C-H...S interactions.

Comment top

It has been generally accepted that imidazole groups play an important role in coordination chemistry (Huang et al., 2003). A flexible ligand readily induces coordination compounds to crystallize in non-centrosymmetric space groups, which makes it possible to investigate their interesting physical properties such as second harmonic generation, ferroelectric and piezoelectric properties (Wang et al., 2005). As a continuation of our work in this field, (Ye et al., 2006, 2007), we have synthesized the title compound, 1, Fig 1.

The title compound, C12H10N2S, was successfully prepared through the reaction between 2-methyl-1H-benzo[d]imidazole and thiophene-2-carbaldehyde. It adopts a trans configuration about the C9?C11 bond and the dihedral angle between the mean plane of the imidazole ring and thiophenyl ring is 16.89 (19)°. The crystal packing is dominated by N—H···N interactions linking the molecules into rows along b, Fig 2. There is also evidence of weak C—H···S interactions.

Related literature top

For general background, see: Huang et al. (2003); Wang et al. (2005); Ye et al. (2006, 2007). For the crystal structures of related compounds, see: Ozbey et al. (1998); Li & Clarkson (2007).

Experimental top

2-methyl-1H-benzo[d]imidazole (10 mmol, 1.32 g) and thiophene-2-carbaldehyde (45 mmol, 5.04 g) were reacted as a melt at 180°C with stirring for 18 h. Then 20 ml 2-propanol and 1.5 g oxalic acid were added to the reaction mixture, the solution filtered and the precipitate washed with copious quantities of boiling water. The pH was adjusted to 8–9 with ammonia to afford the title compound as a pale-yellow solid powder. Crystals suitable for single-crystal X-ray diffraction studies were obtained by slow evaporation of a solution in ethanol at room temperature over several days.

Refinement top

All carbon-bound H atoms were positioned geometrically, with C—H = 0.93 Å and included in the refinement as riding, withUiso(H) = 1.2Ueq. The H atoms attached to N were found in the difference Fourier map and were subsequently treated as riding atoms, with N—H = 0.86 Å, and Uiso(H) = 1.2Ueq(N).

Computing details top

Data collection: CrystalClear (Rigaku, 2005); cell refinement: CrystalClear (Rigaku, 2005); data reduction: CrystalClear (Rigaku, 2005); 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 molecular structure of the compound with the atomic numbering scheme. Displacement ellipsoids were drawn at the 30% probability level.
[Figure 2] Fig. 2. The crystal packing of 1 with hydrogen bonds drawn as dashed lines.
(E)-2-[2-(2-Thienyl)vinyl]-1H-1,3-benzimidazole top
Crystal data top
C13H10N2SF000 = 944
Mr = 226.06Dx = 1.305 Mg m3
Orthorhombic, PnnaMo Kα radiation
λ = 0.71073 Å
Hall symbol: -P 2a 2bcCell parameters from 14820 reflections
a = 12.239 (2) Åθ = 3.0–29.2º
b = 16.389 (3) ŵ = 0.25 mm1
c = 11.487 (2) ÅT = 293 (2) K
V = 2304.1 (7) Å3Block, colorless
Z = 80.15 × 0.10 × 0.07 mm
Data collection top
Mercury2 (2x2 bin mode)
diffractometer
2637 independent reflections
Radiation source: fine-focus sealed tube1360 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.145
Detector resolution: 13.6612 pixels mm-1θmax = 27.5º
T = 293(2) Kθmin = 3.3º
CCD profile fitting scansh = 15→15
Absorption correction: multi-scan
(CrystalClear; Rigaku, 2005)
k = 21→21
Tmin = 0.796, Tmax = 1.000l = 14→14
21849 measured reflections
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)] = 0.084H-atom parameters constrained
wR(F2) = 0.214  w = 1/[σ2(Fo2) + (0.081P)2 + 0.7151P]
where P = (Fo2 + 2Fc2)/3
S = 1.07(Δ/σ)max < 0.001
2637 reflectionsΔρmax = 0.22 e Å3
145 parametersΔρmin = 0.28 e Å3
1 restraintExtinction correction: none
Primary atom site location: structure-invariant direct methods
Crystal data top
C13H10N2SV = 2304.1 (7) Å3
Mr = 226.06Z = 8
Orthorhombic, PnnaMo Kα
a = 12.239 (2) ŵ = 0.25 mm1
b = 16.389 (3) ÅT = 293 (2) K
c = 11.487 (2) Å0.15 × 0.10 × 0.07 mm
Data collection top
Mercury2 (2x2 bin mode)
diffractometer
2637 independent reflections
Absorption correction: multi-scan
(CrystalClear; Rigaku, 2005)
1360 reflections with I > 2σ(I)
Tmin = 0.796, Tmax = 1.000Rint = 0.145
21849 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0841 restraint
wR(F2) = 0.214H-atom parameters constrained
S = 1.07Δρmax = 0.22 e Å3
2637 reflectionsΔρmin = 0.28 e Å3
145 parameters
Special details top

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) top
xyzUiso*/UeqOcc. (<1)
S10.88515 (10)0.06908 (7)0.51647 (11)0.0801 (5)
N10.6821 (2)0.07121 (18)0.1000 (3)0.0577 (9)
H1B0.72640.03090.09240.069*0.50
N20.5945 (2)0.17665 (16)0.1790 (2)0.0452 (7)
H2B0.57510.21340.22830.054*0.50
C10.5111 (4)0.1178 (3)0.1555 (4)0.0824 (14)
H1A0.49560.10280.23190.099*
C20.8179 (4)0.1317 (3)0.7051 (4)0.0898 (15)
H2A0.81360.14530.78360.108*
C30.8987 (5)0.0855 (3)0.6610 (4)0.0890 (16)
H3A0.95590.06470.70530.107*
C40.7391 (3)0.1583 (3)0.6209 (3)0.0653 (11)
H4A0.67900.19130.63640.078*
C50.5901 (4)0.0750 (3)0.0942 (4)0.0753 (13)
H5A0.62780.03160.12770.090*
C60.4751 (3)0.2076 (2)0.0054 (3)0.0604 (11)
H6A0.43760.25140.03810.073*
C70.4546 (4)0.1825 (3)0.1057 (4)0.0720 (12)
H7A0.40150.20940.14920.086*
C80.7672 (3)0.1264 (2)0.5105 (3)0.0581 (10)
C90.7079 (3)0.1380 (2)0.4039 (3)0.0532 (10)
H9A0.64610.17090.40740.064*
C100.6101 (3)0.0995 (2)0.0186 (3)0.0515 (9)
C110.7328 (3)0.1064 (2)0.3007 (3)0.0526 (10)
H11A0.79500.07400.29610.063*
C120.6700 (3)0.1188 (2)0.1941 (3)0.0479 (9)
C130.5538 (3)0.1655 (2)0.0678 (3)0.0461 (9)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0830 (9)0.0654 (8)0.0918 (10)0.0012 (6)0.0304 (7)0.0032 (6)
N10.0607 (19)0.0583 (19)0.054 (2)0.0158 (16)0.0072 (15)0.0140 (16)
N20.0532 (17)0.0401 (16)0.0422 (17)0.0063 (13)0.0015 (13)0.0027 (13)
C10.097 (3)0.096 (4)0.054 (3)0.004 (3)0.017 (3)0.015 (3)
C20.113 (4)0.106 (4)0.050 (3)0.026 (3)0.023 (2)0.013 (3)
C30.112 (4)0.076 (3)0.079 (4)0.023 (3)0.043 (3)0.023 (3)
C40.070 (3)0.081 (3)0.045 (2)0.018 (2)0.0037 (18)0.001 (2)
C50.083 (3)0.079 (3)0.064 (3)0.018 (2)0.011 (2)0.028 (2)
C60.072 (3)0.054 (2)0.055 (2)0.009 (2)0.009 (2)0.001 (2)
C70.081 (3)0.071 (3)0.064 (3)0.009 (2)0.021 (2)0.007 (2)
C80.063 (2)0.051 (2)0.061 (3)0.0153 (19)0.014 (2)0.0087 (19)
C90.055 (2)0.049 (2)0.056 (3)0.0009 (18)0.0023 (18)0.0054 (18)
C100.053 (2)0.051 (2)0.051 (2)0.0034 (18)0.0051 (18)0.0070 (18)
C110.051 (2)0.048 (2)0.059 (3)0.0005 (17)0.0004 (19)0.0009 (18)
C120.048 (2)0.049 (2)0.047 (2)0.0011 (17)0.0016 (17)0.0022 (17)
C130.052 (2)0.0418 (19)0.044 (2)0.0023 (17)0.0020 (17)0.0001 (16)
Geometric parameters (Å, °) top
S1—C31.690 (5)C4—C81.415 (5)
S1—C81.723 (4)C4—H4A0.9300
N1—C121.341 (4)C5—C101.379 (5)
N1—C101.366 (4)C5—H5A0.9300
N1—H1B0.8600C6—C71.365 (5)
N2—C121.335 (4)C6—C131.385 (5)
N2—C131.383 (4)C6—H6A0.9300
N2—H2B0.8600C7—H7A0.9300
C1—C51.386 (6)C8—C91.436 (5)
C1—C71.390 (6)C9—C111.329 (5)
C1—H1A0.9300C9—H9A0.9300
C2—C31.344 (6)C10—C131.401 (5)
C2—C41.435 (6)C11—C121.461 (4)
C2—H2A0.9300C11—H11A0.9300
C3—H3A0.9300
C3—S1—C892.0 (3)C7—C6—H6A121.3
C12—N1—C10106.4 (3)C13—C6—H6A121.3
C12—N1—H1B126.8C6—C7—C1121.6 (4)
C10—N1—H1B126.8C6—C7—H7A119.2
C12—N2—C13106.0 (3)C1—C7—H7A119.2
C12—N2—H2B127.0C4—C8—C9126.3 (4)
C13—N2—H2B127.0C4—C8—S1111.7 (3)
C5—C1—C7121.6 (4)C9—C8—S1122.0 (3)
C5—C1—H1A119.2C11—C9—C8126.3 (4)
C7—C1—H1A119.2C11—C9—H9A116.8
C3—C2—C4114.3 (4)C8—C9—H9A116.8
C3—C2—H2A122.8N1—C10—C5131.2 (4)
C4—C2—H2A122.8N1—C10—C13107.7 (3)
C2—C3—S1112.8 (4)C5—C10—C13121.1 (4)
C2—C3—H3A123.6C9—C11—C12125.0 (3)
S1—C3—H3A123.6C9—C11—H11A117.5
C8—C4—C2109.2 (4)C12—C11—H11A117.5
C8—C4—H4A125.4N1—C12—N2112.7 (3)
C2—C4—H4A125.4N1—C12—C11122.5 (3)
C1—C5—C10117.0 (4)N2—C12—C11124.9 (3)
C1—C5—H5A121.5N2—C13—C6131.5 (3)
C10—C5—H5A121.5N2—C13—C10107.3 (3)
C7—C6—C13117.5 (4)C6—C13—C10121.2 (3)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C11—H11A···S10.932.763.161 (4)107
N1—H1B···N1i0.862.012.865 (6)170
N2—H2B···N2ii0.862.112.906 (5)154
Symmetry codes: (i) −x+3/2, −y, z; (ii) x, −y+1/2, −z+1/2.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
C11—H11A···S10.932.763.161 (4)107
N1—H1B···N1i0.862.012.865 (6)170
N2—H2B···N2ii0.862.112.906 (5)154
Symmetry codes: (i) −x+3/2, −y, z; (ii) x, −y+1/2, −z+1/2.
Acknowledgements top

This work was supported by a Start-up Grant from Southeast University (to YQ).

references
References top

Huang, X.-C., Zhang, J.-P. & Chen, X.-M. (2003). Chin. Sci. Bull. 48, 1531–1534.

Li, L. & Clarkson, G. J. (2007). Org. Lett. 9, 497–500.

Ozbey, S., Ide, S. & Kendi, E. (1998). J. Mol. Struct. 442, 23–?.

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Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Wang, X.-S., Song, Y.-M., Ye, Q. & Xiong, R.-G. (2005). Chin. Sci. Bull. 50, 2317–2340.

Ye, Q., Song, Y.-M., Fu, D.-W., Wang, G.-X. & Xiong, R.-G. (2007). Cryst. Growth Des. 7, 1568–1570.

Ye, Q., Song, Y.-M., Wang, G.-X. & Xiong, R.-G. (2006). J. Am. Chem. Soc. 128, 6554–6555.