organic papers
o1976
Liu, Zhong and Xu C24H19N3O2 doi:10.1107/S1600536805016946 Acta Cryst.(2005). E61, o1976–o1977 Acta Crystallographica Section E
Structure Reports
Online
ISSN 1600-5368
4-[4,5-Bis(4-methoxyphenyl)-1
H
-imidazol-2-yl]-benzonitrile
Xu-Feng Liu, Zeng-Pei Zhong* and Zun-Le Xu
School of Chemistry and Chemical Engineering, Sun Yat-Sen University, Guangzhou 510275, People’s Republic of China
Correspondence e-mail: ceszzp@zsu.edu.cn
Key indicators
Single-crystal X-ray study
T= 273 K
Mean(C–C) = 0.003 A˚ Disorder in main residue
Rfactor = 0.054
wRfactor = 0.130
Data-to-parameter ratio = 16.6
For details of how these key indicators were automatically derived from the article, see http://journals.iucr.org/e.
#2005 International Union of Crystallography Printed in Great Britain – all rights reserved
The title compound, C24H19N3O2, is an analogue of lophine
and exhibits two-photon induced blue fluorescent emission. It adopts a distorted T-shape.
Comment
Heterocyclic imidazoles based on a non-linear optical (NLO) chromophore have received increasing interest due to their excellent thermal stability in guest–host systems (Santoset al., 2001). Previously, we found this type of compound to exhibit two-photon induced blue fluorescent emission (Huang et al., 2002, 2003). In our recent research, the title compound, (I), was found to have the same property.
Compound (I) was obtained in high yield by refluxing a mixture of 4-cyanobenzaldehyde, 4,40-dimethoxybenzil and
ammonium acetate in acetic acid for 3 h (Nakashima et al., 1998). The structure of (I) was also confirmed by 1H NMR, elemental analysis and FAB–MS spectroscopic analysis.
Compound (I) has a distorted T-shaped molecule (Fig. 1). Adjacent molecules are arrangement in a staggered manner (Fig. 2).
[image:1.610.207.460.530.705.2]Received 15 April 2005 Accepted 27 May 2005 Online 10 June 2005
Figure 1
Experimental
Compound (I) was obtained, in 91% yield, by refluxing 4-cyano-benzaldehyde, 4,40-dimethoxybenzil and ammonium acetate in acetic acid for 3 h. A single crystal suitable for X-ray analysis was obtained from ethanol (m.p. 504 K).1H NMR (500 MHz in DMSO/TMS):
3.79 (s, 6H), 6.93–6.96 (m, 2H), 6.99–7.02 (m, 2H), 7.40–7.45 (m, 4H), 7.90 (d, J= 10.0 Hz, 2H), 8.21 (d, J= 10.0 Hz, 2H). Elemental analysis (%) calculated for C24H19N3O2: C 75.57, H 5.02, N 11.02; found C 75.69, H 11.11, N 10.94. FAB–MSm/z(%): 382 (M++ H, 8).
Crystal data
C24H19N3O2 Mr= 381.42 Orthorhombic,Pbca a= 9.801 (3) A˚
b= 15.549 (4) A˚
c= 26.142 (7) A˚
V= 3984.1 (19) A˚3 Z= 8
Dx= 1.272 Mg m3
MoKradiation Cell parameters from 4326
reflections = 2.6–27.0
= 0.08 mm1 T= 273 (2) K Block, colorless 0.480.370.32 mm
Data collection
Bruker SMART CCD 1K area-detector diffractometer ’and!scans
Absorption correction: multi-scan (SADABS; Sheldrick, 1996)
Tmin= 0.961,Tmax= 0.974
17659 measured reflections
4326 independent reflections 2563 reflections withI> 2(I)
Rint= 0.041
max= 27.1 h=12!12
k=19!19
l=33!18
Refinement
Refinement onF2 R[F2> 2(F2)] = 0.054 wR(F2) = 0.130 S= 1.02 4326 reflections 261 parameters Only H-atomU’s refined
w= 1/[2(Fo2) + (0.0634P)2
+ 2.2522P]
whereP= (Fo2+ 2Fc2)/3
(/)max< 0.001
max= 0.38 e A˚
3
min=0.56 e A˚
3
All H atoms were included as riding atoms (C—H = 0.96 A˚ ) and their isotropic displacement parameters were refined. One of the methoxy groups (atoms C24A/C24Band O2A/O2B) exhibits twofold disorder and these atoms were refined isotropically with site-occu-pancy factors 0.453 (10) and 0.547 (10).
Data collection:SMART(Bruker, 1998); cell refinement:SAINT
(Bruker, 1998); data reduction:SAINT; program(s) used to solve structure: SHELXTL (Bruker, 1997); program(s) used to refine structure:SHELXTL; molecular graphics:SHELXTL; software used to prepare material for publication:SHELXTLandPLATON(Spek, 2003).
This project is supported by the Guangdong Provincial Natural Science Foundation of China.
References
Bruker (1997). SHELXTL. Version 5.1. Bruker AXS Inc., Madison, Wisconsin, USA.
Bruker (1998).SMART(Version 5.625) andSAINT(Version 6.02a). Bruker AXS Inc., Madison, Wisconsin, USA.
Huang, Z. L., Lei, H., Li, N., Qiu, Z. R., Wang, H. Z., Guo, J. D., Luo, Y., Zhong, Z. P., Liu, X. F. & Zhou, Z. H. (2003).J. Mater. Chem.13, 1–5. Huang, Z. L., Li, N., Lei, H., Qiu, Z. R., Wang, H. Z., Zhong, Z. P. & Zhou, Z.
H. (2002).Chem Commun.pp. 2400–2401.
Nakashima, K., Fukuzaki, Y., Nomura, R., Shimoda, R., Nakamura, Y., Kuroda, N., Akiyama, S. & Irgum, K. (1998).Dyes Pigments,38, 127–136. Santos, J., Mintz, E. A., Zehnder, O., Bosshard, C., Bu, X. R. & Gunter, P.
(2001).Tetrahedron Lett.42, 805–808.
[image:2.610.316.564.75.228.2]Sheldrick, G. M. (1996).SADABS.University of Go¨ttingen, Germany. Spek, A. L. (2003).J. Appl. Cryst.36, 7–13.
Figure 2
supporting information
sup-1 Acta Cryst. (2005). E61, o1976–o1977
supporting information
Acta Cryst. (2005). E61, o1976–o1977 [https://doi.org/10.1107/S1600536805016946]
4-[4,5-Bis(4-methoxyphenyl)-1
H
-imidazol-2-yl]benzonitrile
Xu-Feng Liu, Zeng-Pei Zhong and Zun-Le Xu
4-[4,5-Bis(4-methoxyphenyl)-1H-imidazol-2-yl]benzonitrile
Crystal data C24H19N3O2
Mr = 381.42
Orthorhombic, Pbca Hall symbol: -P 2ac 2ab a = 9.801 (3) Å
b = 15.549 (4) Å c = 26.142 (7) Å V = 3984.1 (19) Å3
Z = 8
F(000) = 1600 Dx = 1.272 Mg m−3
Mo Kα radiation, λ = 0.71073 Å Cell parameters from 4326 reflections θ = 2.6–27.0°
µ = 0.08 mm−1
T = 273 K Block, colorless 0.48 × 0.37 × 0.32 mm
Data collection
Bruker SMART CCD 1K area-detector diffractometer
φ and ω scans
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) Tmin = 0.961, Tmax = 0.974
17659 measured reflections
4326 independent reflections 2563 reflections with I > 2σ(I) Rint = 0.041
θmax = 27.1°, θmin = 2.6°
h = −12→12 k = −19→19 l = −33→18
Refinement Refinement on F2
Least-squares matrix: full R[F2 > 2σ(F2)] = 0.054
wR(F2) = 0.130
S = 1.02 4326 reflections 261 parameters
4 restraints
Only H-atom displacement parameters refined w = 1/[σ2(F
o2) + (0.0634P)2 + 2.2522P]
where P = (Fo2 + 2Fc2)/3
(Δ/σ)max < 0.001
Δρmax = 0.38 e Å−3
Δρmin = −0.56 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.
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
x y z Uiso*/Ueq Occ. (<1)
O1 −0.1756 (2) 0.30445 (13) 0.00221 (6) 0.0669 (6)
O2B 0.5977 (3) 0.4568 (2) 0.1741 (2) 0.0599 (14)* 0.547 (10) N1 −0.03100 (18) 0.16509 (12) 0.22640 (6) 0.0365 (4)
H1A −0.1083 0.1414 0.2198 0.044* N2 0.15676 (18) 0.19979 (12) 0.26803 (6) 0.0375 (4) N3 −0.2246 (3) −0.02281 (18) 0.48686 (10) 0.0870 (9) C1 0.0502 (2) 0.12506 (16) 0.36298 (8) 0.0426 (6) H1 0.1312 0.1561 0.3647 0.051* C2 −0.0146 (2) 0.11409 (14) 0.31590 (7) 0.0342 (5) C3 0.0395 (2) 0.15785 (14) 0.27065 (8) 0.0344 (5) C4 0.1590 (2) 0.23811 (14) 0.22041 (8) 0.0357 (5) C5 0.0422 (2) 0.21675 (14) 0.19388 (8) 0.0343 (5) C6 −0.1337 (2) 0.06622 (15) 0.31409 (9) 0.0434 (6) H6 −0.1770 0.0572 0.2829 0.052* C7 −0.1890 (3) 0.03175 (16) 0.35818 (9) 0.0477 (6) H7 −0.2695 0.0003 0.3565 0.057* C8 −0.1246 (3) 0.04394 (15) 0.40491 (8) 0.0436 (6) C9 −0.0042 (3) 0.09058 (16) 0.40698 (9) 0.0467 (6) H9 0.0398 0.0986 0.4381 0.056* C10 −0.1822 (3) 0.00799 (18) 0.45080 (10) 0.0578 (7) C11 0.2726 (2) 0.29387 (15) 0.20442 (8) 0.0386 (5) C12 0.3309 (3) 0.35160 (17) 0.23854 (10) 0.0514 (6) H12 0.2973 0.3551 0.2718 0.062* C13 0.4376 (3) 0.40379 (18) 0.22395 (12) 0.0629 (8) H13 0.4748 0.4419 0.2476 0.076* C14 0.4902 (2) 0.40073 (16) 0.17515 (13) 0.0615 (8) C15 0.4324 (3) 0.34407 (18) 0.14061 (11) 0.0585 (8) H15 0.4656 0.3414 0.1073 0.070* C16 0.3252 (2) 0.29106 (16) 0.15525 (10) 0.0456 (6) H16 0.2880 0.2530 0.1316 0.055* C17 −0.0113 (2) 0.23867 (14) 0.14317 (8) 0.0353 (5) C18 −0.0015 (2) 0.32100 (15) 0.12327 (8) 0.0412 (5) H18 0.0428 0.3636 0.1419 0.049* C19 −0.0565 (2) 0.34054 (16) 0.07613 (9) 0.0452 (6) H19 −0.0481 0.3959 0.0631 0.054* C20 −0.1239 (2) 0.27831 (17) 0.04820 (8) 0.0441 (6) C21 −0.1337 (3) 0.19588 (17) 0.06687 (8) 0.0482 (6) H21 −0.1776 0.1534 0.0480 0.058* C22 −0.0774 (2) 0.17702 (16) 0.11402 (8) 0.0435 (6) H22 −0.0840 0.1212 0.1266 0.052* C23 −0.2822 (4) 0.2570 (2) −0.01908 (11) 0.0846 (11) H23A −0.3084 0.2821 −0.0511 0.127* H23B −0.3587 0.2573 0.0038 0.127* H23C −0.2527 0.1988 −0.0246 0.127*
supporting information
sup-3 Acta Cryst. (2005). E61, o1976–o1977
H24D 0.7534 0.4805 0.1305 0.117* 0.547 (10) H24E 0.6227 0.4514 0.1006 0.117* 0.547 (10) H24F 0.7091 0.3836 0.1309 0.117* 0.547 (10)
Atomic displacement parameters (Å2)
U11 U22 U33 U12 U13 U23
O1 0.0731 (13) 0.0811 (14) 0.0465 (10) −0.0207 (11) −0.0216 (9) 0.0206 (10) N1 0.0314 (9) 0.0441 (11) 0.0341 (10) −0.0072 (8) −0.0013 (7) −0.0002 (8) N2 0.0312 (10) 0.0452 (11) 0.0362 (10) −0.0021 (9) −0.0015 (8) 0.0025 (8) N3 0.123 (3) 0.0772 (19) 0.0605 (16) −0.0118 (17) 0.0285 (16) 0.0173 (14) C1 0.0370 (12) 0.0502 (14) 0.0406 (12) −0.0026 (11) −0.0040 (10) 0.0034 (11) C2 0.0306 (11) 0.0363 (12) 0.0357 (11) 0.0029 (10) 0.0005 (9) 0.0023 (9) C3 0.0312 (11) 0.0390 (12) 0.0330 (11) 0.0004 (10) −0.0004 (9) −0.0003 (9) C4 0.0319 (11) 0.0400 (13) 0.0350 (11) −0.0009 (10) 0.0026 (9) −0.0004 (9) C5 0.0313 (11) 0.0388 (12) 0.0330 (11) −0.0023 (10) 0.0031 (9) −0.0008 (9) C6 0.0443 (14) 0.0446 (14) 0.0412 (13) −0.0043 (11) −0.0032 (10) 0.0023 (10) C7 0.0472 (14) 0.0429 (14) 0.0531 (15) −0.0111 (12) 0.0033 (11) 0.0063 (11) C8 0.0549 (15) 0.0368 (13) 0.0393 (12) 0.0024 (12) 0.0084 (11) 0.0053 (10) C9 0.0529 (15) 0.0514 (15) 0.0358 (12) 0.0000 (13) −0.0041 (11) 0.0038 (11) C10 0.0739 (19) 0.0497 (16) 0.0499 (15) −0.0016 (15) 0.0118 (13) 0.0092 (13) C11 0.0295 (11) 0.0409 (13) 0.0455 (13) 0.0006 (10) −0.0027 (9) 0.0063 (10) C12 0.0471 (14) 0.0529 (16) 0.0543 (15) −0.0068 (13) −0.0078 (12) 0.0037 (12) C13 0.0485 (16) 0.0516 (17) 0.089 (2) −0.0145 (14) −0.0167 (15) 0.0069 (15) C14 0.0297 (13) 0.0402 (15) 0.115 (3) −0.0059 (12) 0.0046 (15) 0.0234 (16) C15 0.0431 (14) 0.0549 (17) 0.0774 (19) 0.0078 (14) 0.0225 (13) 0.0215 (14) C16 0.0369 (13) 0.0468 (14) 0.0531 (14) 0.0026 (11) 0.0057 (11) 0.0059 (11) C17 0.0312 (11) 0.0434 (13) 0.0313 (11) −0.0017 (10) 0.0018 (9) −0.0004 (9) C18 0.0389 (12) 0.0427 (13) 0.0419 (12) −0.0048 (11) −0.0024 (10) −0.0030 (10) C19 0.0457 (13) 0.0436 (14) 0.0462 (13) −0.0021 (12) −0.0017 (11) 0.0087 (11) C20 0.0416 (13) 0.0569 (16) 0.0337 (12) −0.0058 (12) −0.0014 (10) 0.0070 (10) C21 0.0547 (15) 0.0542 (16) 0.0357 (12) −0.0168 (13) −0.0063 (11) −0.0017 (11) C22 0.0502 (14) 0.0429 (14) 0.0375 (12) −0.0103 (12) −0.0003 (10) 0.0046 (10) C23 0.091 (2) 0.106 (3) 0.0569 (18) −0.024 (2) −0.0336 (17) 0.0160 (18)
Geometric parameters (Å, º)
N3—C10 1.136 (3) C18—C19 1.379 (3) C1—C9 1.377 (3) C18—H18 0.9300 C1—C2 1.395 (3) C19—C20 1.381 (3) C1—H1 0.9300 C19—H19 0.9300 C2—C6 1.386 (3) C20—C21 1.375 (3) C2—C3 1.464 (3) C21—C22 1.382 (3) C4—C5 1.380 (3) C21—H21 0.9300 C4—C11 1.472 (3) C22—H22 0.9300 C5—C17 1.466 (3) C23—H23A 0.9600 C6—C7 1.381 (3) C23—H23B 0.9600 C6—H6 0.9300 C23—H23C 0.9600 C7—C8 1.388 (3) C24A—H24A 0.9600 C7—H7 0.9300 C24A—H24B 0.9600 C8—C9 1.386 (3) C24A—H24C 0.9600 C8—C10 1.439 (3) C24B—H24D 0.9600 C9—H9 0.9300 C24B—H24E 0.9600 C11—C16 1.386 (3) C24B—H24F 0.9600
supporting information
sup-5 Acta Cryst. (2005). E61, o1976–o1977
C7—C8—C10 120.1 (2) O1—C23—H23C 109.5 C1—C9—C8 120.1 (2) H23A—C23—H23C 109.5 C1—C9—H9 120.0 H23B—C23—H23C 109.5 C8—C9—H9 120.0 O2A—C24A—H24A 109.5 N3—C10—C8 177.5 (3) O2A—C24A—H24B 109.5 C16—C11—C12 117.6 (2) H24A—C24A—H24B 109.5 C16—C11—C4 121.8 (2) O2A—C24A—H24C 109.5 C12—C11—C4 120.6 (2) H24A—C24A—H24C 109.5 C13—C12—C11 121.0 (3) H24B—C24A—H24C 109.5 C13—C12—H12 119.5 O2B—C24B—H24D 109.5 C11—C12—H12 119.5 O2B—C24B—H24E 109.5 C14—C13—C12 121.4 (3) H24D—C24B—H24E 109.5 C14—C13—H13 119.3 O2B—C24B—H24F 109.5 C12—C13—H13 119.3 H24D—C24B—H24F 109.5 O2A—C14—C13 129.4 (4) H24E—C24B—H24F 109.5 O2B—C14—C13 106.5 (3)