organic papers
Acta Cryst.(2004). E60, o1563±o1565 DOI: 10.1107/S1600536804019622 Yi-Ping Tong and Wei Li C17H18N2O
o1563
Acta Crystallographica Section EStructure Reports Online
ISSN 1600-5368
2-(2-Ethoxyphenyl)-1-ethyl-1
H
-benzimidazole
Yi-Ping Tong* and Wei Li
Department of Chemistry, Hanshan Normal College, Chaozhou 521041, Guangdong, People's Republic of China
Correspondence e-mail: typ2469@163.com
Key indicators Single-crystal X-ray study
T= 293 K
Mean(C±C) = 0.004 AÊ
Rfactor = 0.050
wRfactor = 0.110
Data-to-parameter ratio = 10.5
For details of how these key indicators were automatically derived from the article, see http://journals.iucr.org/e.
#2004 International Union of Crystallography Printed in Great Britain ± all rights reserved
The title compound, C17H18N2O, was obtained by reaction of
2-(2-hydroxyphenyl)benzimidazole with bromoethane. The
crystal structure is stabilized by intermolecular CÐH
interactions between the benzimidazole/benzimidazole and between the benzimidazole/phenolate moieties of adjacent
molecules. No other hydrogen-bond interactions or ±
stacking interactions occur in the crystal packing, which is somewhat unusual for an aromatic heterocyclic compound.
Comment
Benzimidazole and its derivatives, such as
2-(2-hydroxy-phenyl)benzimidazole and 2-(2-ethoxyphenyl)-1-ethyl-1H
-benzimidazole, are excellent photoluminescent materials (Svejda et al., 1978; Wu et al., 2003). In recent years, more attention has been paid to their complexes and those of other similarN,O-donor ligands with metal ions and non-metal ions, such as ZnII, BeII, AlIII, EuIII and BIII, because of their
potential role as electroluminescent materials in organic
light-emitting diodes (Wang, 2001; Huang et al., 2002). These
complexes are considered to be better electroluminescent materials than free ligands, owing to their increased thermal stability on coordination to metal or non-metal ions.
In an attempt to synthesize complexes of the ligand
2-(1-ethyl-1H-benzimidazol-2-yl)phenol with the metal ions
mentioned above in order to obtain a blue-light emitter for further fabrication of electroluminescent diodes, we obtained another highly photoluminescent compound, (I), which emits strong blue light at room temperature. The crystal structure of (I) is reported here.
In the crystal structure of (I) (Fig. 1), the CÐO and CÐN bond lengths are similar to those found in related compounds,
e.g. 2-(1H-benzimidazol-2-yl)-6-methoxyphenol (Elerman & Kabak, 1997), and the complexes of 2-(1H -benzimidazol-2-yl)-6-methylphenol with CoII and CoIII (Crane et al., 1999).
However, in (I), the benzimidazole and phenolate moieties are almost perpendicular, owing to the steric hindrance arising from ethylation at the O and N positions with, for example, the
C5ÐC6ÐC7ÐN2 torsion angle being ÿ77.6 (3), which is
quite different from the coplanarity observed for 2-(1H
benzimidazol-2-yl)-6-methoxyphenol (Elerman & Kabak, 1997). Furthermore, this non-coplanarity, as well as the steric hindrance from the ethyl groups on the O and N positions, should block formation of intermolecular±stacking actions. This is consistent with the observation of no
inter-molecular ± stacking interactions in (I). However, CÐ
H interactions (Srinivaset al., 2004; Rodriguezet al., 2004) occur between the benzimidazole/benzimidazole and between the benzimidazole/phenolate moieties of adjacent molecules (Fig. 2). These edge-to-face CÐH interactions are
some-what different, with H distances of ca 2.82, 2.81 and
2.70 AÊ, and corresponding CÐH angles ofca151, 140 and 144.
Experimental
The title compound, (I), was synthesized by a two-step reaction based on the method of Anthony & Philip (1981). Salicylic acid (0.138 g,
1 mmol) ando-phenylenediamine (0.108 g, 1 mmol) were mixed and stirred in syrupy phosphoric acid (3 ml) at a temperature ofca520 K for 5 h to give white analytically pure 2-(2-hydroxyphenyl)benz-imidazole after recrystallization of the crude product. The yield was
ca10%. 2-(2-Ethoxyphenyl)-1-ethyl-1H-benzimidazole was prepared by the reaction of 2-(2-hydroxyphenyl)benzimidazole and bromo-ethane under re¯ux conditions with a yield ofca70%. The X-ray quality single crystal used in the structure determination was grown by slow evaporation of an ethanol solution for about one week. Analysis found: C 76.73, H 6.59, N 10.66%; calculated for C17H18N2O:
C 76.66, H 6.81, N 10.52%.
Crystal data C17H18N2O
Mr= 266.33
Orthorhombic,P212121
a= 9.3305 (8) AÊ
b= 12.4070 (10) AÊ
c= 12.7422 (10) AÊ
V= 1475.1 (2) AÊ3
Z= 4
Dx= 1.199 Mg mÿ3
MoKradiation Cell parameters from 1432
re¯ections
= 2.3±20.8
= 0.08 mmÿ1
T= 293 (2) K Block, colorless 0.330.260.22 mm
Data collection
Bruker SMART APEX area-detector diffractometer
'and!scans
Absorption correction: multi-scan (SADABS; Sheldrick, 1996)
Tmin= 0.976,Tmax= 0.984
9232 measured re¯ections
1922 independent re¯ections 1582 re¯ections withI> 2(I)
Rint= 0.036
max= 27.5
h=ÿ11!11
k=ÿ15!16
l=ÿ16!12 Re®nement
Re®nement onF2
R[F2> 2(F2)] = 0.050
wR(F2) = 0.110
S= 1.08 1922 re¯ections 183 parameters
H-atom parameters constrained
w= 1/[2(F
o2) + (0.0455P)2
+ 0.2012P]
whereP= (Fo2+ 2Fc2)/3
(/)max< 0.001
max= 0.15 e AÊÿ3
min=ÿ0.16 e AÊÿ3
Table 1
Selected geometric parameters (AÊ,).
N1ÐC7 1.365 (3)
N1ÐC13 1.382 (3)
N1ÐC14 1.464 (3)
N2ÐC7 1.312 (3)
N2ÐC8 1.387 (3)
O1ÐC1 1.355 (3)
O1ÐC16 1.431 (4)
C14ÐC15 1.498 (4)
C16ÐC17 1.485 (5)
C7ÐN1ÐC13 106.6 (2)
C7ÐN1ÐC14 127.5 (2)
C13ÐN1ÐC14 125.1 (2)
C7ÐN2ÐC8 104.5 (2)
C1ÐO1ÐC16 118.5 (2)
O1ÐC1ÐC2 124.9 (2)
O1ÐC1ÐC6 115.3 (2)
N1ÐC14ÐC15 111.8 (2) O1ÐC16ÐC17 107.8 (3)
H atoms were placed at calculated positions (CÐH = 0.93 AÊ for all aromatic ring H atoms, 0.96 AÊ for all methyl H atoms and 0.97 AÊ for all methylene H atoms) and re®ned using the riding-model approx-imation, withUiso(H) = 1.2Ueq(C) for aromatic ring and methylene H
atoms, andUiso(H) = 1.5Ueq(C) for all methyl H atoms. In the absence
of signi®cant anomalous dispersion effects, Friedel pair re¯ections were merged before the ®nal re®nement.
Data collection:SMART(Bruker, 2001); cell re®nement:SAINT
(Bruker, 2001); data reduction:SAINT; program(s) used to solve structure:SHELXS97 (Sheldrick, 1997); program(s) used to re®ne structure: SHELXL97 (Sheldrick, 1997); molecular graphics:
SHELXTL(Sheldrick, 2000); software used to prepare material for publication:SHELXL97.
organic papers
o1564
Yi-Ping Tong and Wei Li C17H18N2O Acta Cryst.(2004). E60, o1563±o1565Figure 2
The CÐH interactions (dashed lines) in the crystal packing of (I). Figure 1
The authors thank Professor Xiao-Ming Chen, School of Chemistry and Chemical Engineering, Sun Yat-Sen Univer-sity, China, for his generous help and support of this work, and also thank Hanshan Normal College, China, for support of this work.
References
Anthony, W. A. & Philip, J. B. (1981).J. Heterocycl. Chem.18, 803±805. Bruker (2001).SAINTandSMART. Bruker AXS Inc., Madison, Wisconsin,
USA.
Crane, D. J., Sinn, E. & Tann, B. (1999).Polyhedron,18, 1527±1532. Elerman, Y. & Kabak, M. (1997).Acta Cryst.C53, 372±374.
Huang, L., Wang, K. Z., Huang, C. H., Gao, D. C. & Jin, L. P. (2002).Synth. Met.128, 241±245.
Rodriguez, A., Arturo, G. V. J. & Sousa-Pedradres, A. (2004).J. Organomet. Chem.689, 557±563.
Sheldrick, G. M. (1996).SADABS.University of GoÈttingen, Germany. Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of
GoÈttingen, Germany.
Sheldrick, G. M. (2000).SHELXTL.Version 6.10. Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA.
Srinivas, O., Muktha, B., Radhika, S., Guru Row, T. N. & Jayaraman, N. (2004).
Carbohydr. Res.339, 1087±1092.
Svejda, P., Anderson, R. R. & Maki, A. H. (1978).J. Am. Chem. Soc.100, 7131±7138.
Wang, S. (2001).Coord. Chem. Rev.215, 79±98.
Wu, T., Li, D., Feng, X. L. & Cai, J. W. (2003).Inorg. Chem. Commun.6, 886± 890.
organic papers
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Acta Cryst. (2004). E60, o1563–o1565
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Acta Cryst. (2004). E60, o1563–o1565 [https://doi.org/10.1107/S1600536804019622]
2-(2-Ethoxyphenyl)-1-ethyl-1
H
-benzimidazole
Yi-Ping Tong and Wei Li
2-(2-Ethoxyphenyl)-1-ethyl-1H-benzimidazole
Crystal data
C17H18N2O Mr = 266.33
Orthorhombic, P212121
Hall symbol: P 2ac 2ab
a = 9.3305 (8) Å
b = 12.407 (1) Å
c = 12.7422 (10) Å
V = 1475.1 (2) Å3 Z = 4
F(000) = 568
Dx = 1.199 Mg m−3
Mo Kα radiation, λ = 0.71073 Å Cell parameters from 1432 reflections
θ = 2.3–20.8°
µ = 0.08 mm−1 T = 293 K Block, colorless 0.33 × 0.26 × 0.22 mm
Data collection
Bruker APEX area-detector diffractometer
Radiation source: fine-focus sealed tube Graphite monochromator
φ and ω scans
Absorption correction: multi-scan (SADABS; Sheldrick, 1996)
Tmin = 0.976, Tmax = 0.984
9232 measured reflections 1922 independent reflections 1582 reflections with I > 2σ(I)
Rint = 0.036
θmax = 27.5°, θmin = 2.3° h = −11→11
k = −15→16
l = −16→12
Refinement
Refinement on F2
Least-squares matrix: full
R[F2 > 2σ(F2)] = 0.050 wR(F2) = 0.110 S = 1.08 1922 reflections 183 parameters 0 restraints
Primary atom site location: structure-invariant direct methods
Secondary atom site location: difference Fourier map
Hydrogen site location: inferred from neighbouring sites
H-atom parameters constrained
w = 1/[σ2(F
o2) + (0.0455P)2 + 0.2012P]
where P = (Fo2 + 2Fc2)/3
(Δ/σ)max < 0.001
Δρmax = 0.15 e Å−3
Δρmin = −0.16 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
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Acta Cryst. (2004). E60, o1563–o1565
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 0.0603 (2) 0.23129 (16) 0.73990 (17) 0.0405 (5) N2 0.0707 (2) 0.38970 (16) 0.65627 (17) 0.0416 (5) O1 0.1413 (2) 0.38910 (18) 0.92994 (16) 0.0588 (6) C1 0.2718 (3) 0.3787 (2) 0.8844 (2) 0.0438 (6) C2 0.4010 (3) 0.3977 (2) 0.9339 (2) 0.0553 (8)
H2 0.4026 0.4211 1.0033 0.066*
C3 0.5273 (3) 0.3819 (3) 0.8804 (3) 0.0601 (8)
H3 0.6138 0.3934 0.9148 0.072*
C4 0.5283 (3) 0.3494 (3) 0.7773 (3) 0.0591 (8)
H4 0.6144 0.3387 0.7421 0.071*
C5 0.3992 (3) 0.3330 (2) 0.7272 (2) 0.0516 (7)
H5 0.3989 0.3122 0.6571 0.062*
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Acta Cryst. (2004). E60, o1563–o1565
Atomic displacement parameters (Å2)
U11 U22 U33 U12 U13 U23
N1 0.0422 (12) 0.0382 (10) 0.0412 (12) −0.0025 (10) −0.0033 (10) 0.0026 (10) N2 0.0468 (13) 0.0352 (10) 0.0427 (12) 0.0014 (10) 0.0000 (10) 0.0009 (10) O1 0.0508 (12) 0.0767 (14) 0.0490 (12) −0.0036 (11) 0.0069 (10) −0.0170 (11) C1 0.0463 (15) 0.0409 (13) 0.0441 (15) 0.0007 (13) 0.0001 (13) −0.0035 (12) C2 0.0549 (18) 0.0635 (18) 0.0477 (17) −0.0070 (15) −0.0083 (15) −0.0098 (15) C3 0.0483 (18) 0.0622 (18) 0.070 (2) −0.0094 (16) −0.0091 (15) −0.0074 (18) C4 0.0403 (16) 0.066 (2) 0.071 (2) −0.0074 (15) 0.0078 (15) −0.0131 (18) C5 0.0506 (17) 0.0550 (16) 0.0492 (16) −0.0070 (14) 0.0033 (14) −0.0077 (14) C6 0.0427 (14) 0.0346 (12) 0.0448 (15) −0.0035 (11) −0.0010 (12) 0.0014 (12) C7 0.0435 (15) 0.0339 (12) 0.0377 (14) 0.0001 (11) 0.0045 (12) −0.0055 (11) C8 0.0429 (15) 0.0366 (12) 0.0367 (13) 0.0039 (12) 0.0013 (11) −0.0055 (11) C9 0.0561 (17) 0.0463 (15) 0.0445 (17) 0.0068 (14) −0.0057 (13) 0.0000 (13) C10 0.0515 (17) 0.0631 (18) 0.0474 (17) 0.0079 (16) −0.0120 (15) −0.0090 (15) C11 0.0479 (17) 0.0567 (17) 0.0591 (19) −0.0087 (14) −0.0086 (15) −0.0116 (15) C12 0.0521 (16) 0.0409 (14) 0.0558 (18) −0.0044 (13) −0.0037 (14) 0.0017 (14) C13 0.0385 (14) 0.0408 (13) 0.0372 (14) 0.0029 (12) 0.0021 (12) −0.0037 (11) C14 0.0531 (16) 0.0453 (14) 0.0440 (15) −0.0072 (13) −0.0025 (13) 0.0117 (13) C15 0.067 (2) 0.0511 (17) 0.070 (2) 0.0127 (15) 0.0059 (17) 0.0127 (17) C16 0.079 (2) 0.072 (2) 0.053 (2) −0.0078 (18) 0.0163 (18) −0.0139 (17) C17 0.094 (3) 0.095 (3) 0.085 (3) 0.001 (2) 0.041 (2) −0.015 (2)
Geometric parameters (Å, º)
N1—C7 1.365 (3) C9—C10 1.369 (4)
N1—C13 1.382 (3) C9—H9 0.9300
N1—C14 1.464 (3) C10—C11 1.387 (4)
N2—C7 1.312 (3) C10—H10 0.9300
N2—C8 1.387 (3) C11—C12 1.378 (4)
O1—C1 1.355 (3) C11—H11 0.9300
O1—C16 1.431 (4) C12—C13 1.386 (4)
C1—C2 1.381 (4) C12—H12 0.9300
C1—C6 1.401 (4) C14—C15 1.498 (4)
C2—C3 1.375 (4) C14—H14A 0.9700
C2—H2 0.9300 C14—H14B 0.9700
C3—C4 1.374 (4) C15—H15A 0.9600
C3—H3 0.9300 C15—H15B 0.9600
C4—C5 1.379 (4) C15—H15C 0.9600
C4—H4 0.9300 C16—C17 1.485 (5)
C5—C6 1.384 (4) C16—H16A 0.9700
C5—H5 0.9300 C16—H16B 0.9700
C6—C7 1.483 (4) C17—H17A 0.9600
C8—C13 1.394 (3) C17—H17B 0.9600
C8—C9 1.398 (4) C17—H17C 0.9600
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C7—N1—C14 127.5 (2) C12—C11—C10 121.3 (3) C13—N1—C14 125.1 (2) C12—C11—H11 119.4 C7—N2—C8 104.5 (2) C10—C11—H11 119.4 C1—O1—C16 118.5 (2) C11—C12—C13 116.6 (3) O1—C1—C2 124.9 (2) C11—C12—H12 121.7 O1—C1—C6 115.3 (2) C13—C12—H12 121.7 C2—C1—C6 119.7 (3) N1—C13—C12 131.9 (2) C3—C2—C1 119.8 (3) N1—C13—C8 105.1 (2) C3—C2—H2 120.1 C12—C13—C8 123.1 (3) C1—C2—H2 120.1 N1—C14—C15 111.8 (2) C4—C3—C2 121.5 (3) N1—C14—H14A 109.3
C4—C3—H3 119.3 C15—C14—H14A 109.3
C2—C3—H3 119.3 N1—C14—H14B 109.3
C3—C4—C5 118.7 (3) C15—C14—H14B 109.3 C3—C4—H4 120.6 H14A—C14—H14B 107.9
C5—C4—H4 120.6 C14—C15—H15A 109.5
C4—C5—C6 121.4 (3) C14—C15—H15B 109.5 C4—C5—H5 119.3 H15A—C15—H15B 109.5
C6—C5—H5 119.3 C14—C15—H15C 109.5
C5—C6—C1 118.9 (3) H15A—C15—H15C 109.5 C5—C6—C7 120.5 (2) H15B—C15—H15C 109.5 C1—C6—C7 120.6 (2) O1—C16—C17 107.8 (3) N2—C7—N1 113.4 (2) O1—C16—H16A 110.1 N2—C7—C6 125.6 (2) C17—C16—H16A 110.1 N1—C7—C6 121.0 (2) O1—C16—H16B 110.1 N2—C8—C13 110.4 (2) C17—C16—H16B 110.1 N2—C8—C9 130.6 (2) H16A—C16—H16B 108.5 C13—C8—C9 119.0 (2) C16—C17—H17A 109.5 C10—C9—C8 118.2 (3) C16—C17—H17B 109.5 C10—C9—H9 120.9 H17A—C17—H17B 109.5
C8—C9—H9 120.9 C16—C17—H17C 109.5
C9—C10—C11 122.0 (3) H17A—C17—H17C 109.5 C9—C10—H10 119.0 H17B—C17—H17C 109.5
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Acta Cryst. (2004). E60, o1563–o1565