Abstract
The complete molecule of the title compound, C22H16N2O4, is generated by a crystallographic centre of inversion. The plane of the central aromatic ring is tilted by 11.85 (4)° with respect to the outer aromatic ring. The crystal packing is determined by van der Waals interactions, with stair-like stacking between adjacent aromatic rings. The stacks are staggered and each layer is approximately 3.8 Å from the next. The closest intermolecular contact (approximately 2.42 Å) is between an O atom and a vinyl H atom.
Related literature
For background information on photonic materials, see: He et al. (2008 ▶). For stilbenes, see: Moreno-Fuquen et al. (2008 ▶, 2009 ▶). For the synthesis, see: Borsche (1912 ▶); Nakatsuji et al. (1991 ▶). For a related structure, see: Bazan et al. (2000 ▶).
Experimental
Crystal data
C22H16N2O4
M r = 372.37
Monoclinic,
a = 7.4689 (12) Å
b = 16.615 (3) Å
c = 7.3917 (12) Å
β = 108.824 (3)°
V = 868.2 (2) Å3
Z = 2
Mo Kα radiation
μ = 0.10 mm−1
T = 173 K
0.40 × 0.18 × 0.12 mm
Data collection
Bruker SMART Platform CCD diffractometer
Absorption correction: none
10088 measured reflections
2001 independent reflections
1486 reflections with I > 2σ(I)
R int = 0.041
Refinement
R[F 2 > 2σ(F 2)] = 0.038
wR(F 2) = 0.116
S = 1.02
2001 reflections
159 parameters
All H-atom parameters refined
Δρmax = 0.30 e Å−3
Δρmin = −0.18 e Å−3
Data collection: SMART (Bruker, 2001 ▶); cell refinement: SAINT (Bruker, 2001 ▶); data reduction: SAINT; 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: publCIF (Westrip, 2009 ▶).
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809024751/ng2592sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809024751/ng2592Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Acknowledgments
This work was supported in part by Research Development Grants from the Pennsylvania State University. The author also acknowledges Benjamin E. Kucera, Victor G. Young Jr, and the X-Ray Crystallographic Laboratory at the University of Minnesota.
supplementary crystallographic information
Comment
Distyrylbenzene derivatives have been studied as laser dyes, components of organic light-emitting diodes, and as model compounds for the study of conductivity and molecular properties in substituted p-phenylenevinylene (PPV) polymers. For background information on photonic materials, see: He et al. (2008). For related systems of stilbene, see: Moreno-Fuquen et al. (2008, 2009). For literature related to the synthesis, see: Borsche (1912).
Experimental
Synthesis was carried out following literature procedures (Nakatsuj) by standard Wittig synthesis. To a mixture of p-phenylenedimethylene- bis(tripheny1phosphonium chloride) (1.00 g, 1.43 mmol) and p-nitrobenzaldehyde (0.432 g 2.86 mmol) in EtOH (10 ml) was added 0.2 mol/L EtOLi(20 ml, 4.0 mmol) and the mixture was stirred overnight. The resulting reaction mixture was poured into water to give a yellow precipitate (0.4 g, 75%) which was filtered off, washed with EtOH, dried under reduced pressure, m.p. 289–290. Crystallization attempts from various solvents yielded only powders. Yellowish orange crystals however were grown by sublimation.
Refinement
All hydrogen atoms were placed in ideal positions and refined as riding atoms with relative isotropic displacement parameters.
Figures
Fig. 1.
The molecular structure of 1,4-di(4-nitrostyryl)benzene with atom lables.
Fig. 2.
Crystal packing viewed along the a axis.
Crystal data
| C22H16N2O4 | F(000) = 388 |
| Mr = 372.37 | Dx = 1.424 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 851 reflections |
| a = 7.4689 (12) Å | θ = 2.5–27.5° |
| b = 16.615 (3) Å | µ = 0.10 mm−1 |
| c = 7.3917 (12) Å | T = 173 K |
| β = 108.824 (3)° | Needle, yellow |
| V = 868.2 (2) Å3 | 0.40 × 0.18 × 0.12 mm |
| Z = 2 |
Data collection
| Bruker SMART Platform CCD diffractometer | 1486 reflections with I > 2σ(I) |
| Radiation source: normal-focus sealed tube | Rint = 0.041 |
| graphite | θmax = 27.5°, θmin = 2.5° |
| ω scans | h = −9→9 |
| 10088 measured reflections | k = −21→21 |
| 2001 independent reflections | l = −9→9 |
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)] = 0.038 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.116 | All H-atom parameters refined |
| S = 1.01 | w = 1/[σ2(Fo2) + (0.0595P)2 + 0.1981P] where P = (Fo2 + 2Fc2)/3 |
| 2001 reflections | (Δ/σ)max < 0.001 |
| 159 parameters | Δρmax = 0.30 e Å−3 |
| 0 restraints | Δρmin = −0.18 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. |
| 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 | −0.18351 (16) | 0.18081 (7) | −0.31257 (17) | 0.0314 (3) | |
| O1 | −0.31485 (14) | 0.14204 (7) | −0.29133 (16) | 0.0424 (3) | |
| O2 | −0.20374 (14) | 0.23244 (7) | −0.43745 (15) | 0.0415 (3) | |
| C1 | 0.00888 (18) | 0.16483 (8) | −0.18509 (19) | 0.0268 (3) | |
| C2 | 0.03516 (19) | 0.10424 (8) | −0.0511 (2) | 0.0293 (3) | |
| H2 | −0.068 (2) | 0.0758 (9) | −0.037 (2) | 0.034 (4)* | |
| C3 | 0.2169 (2) | 0.08605 (8) | 0.0623 (2) | 0.0299 (3) | |
| H3 | 0.234 (2) | 0.0439 (10) | 0.154 (2) | 0.036 (4)* | |
| C4 | 0.37281 (19) | 0.12795 (8) | 0.04412 (18) | 0.0274 (3) | |
| C5 | 0.3394 (2) | 0.19080 (9) | −0.0888 (2) | 0.0309 (3) | |
| H5 | 0.440 (2) | 0.2209 (9) | −0.102 (2) | 0.032 (4)* | |
| C6 | 0.1573 (2) | 0.20926 (9) | −0.2043 (2) | 0.0302 (3) | |
| H6 | 0.137 (2) | 0.2519 (10) | −0.294 (2) | 0.037 (4)* | |
| C7 | 0.56766 (19) | 0.10807 (9) | 0.1593 (2) | 0.0304 (3) | |
| H7 | 0.659 (2) | 0.1468 (9) | 0.145 (2) | 0.036 (4)* | |
| C8 | 0.62118 (19) | 0.04369 (9) | 0.27155 (19) | 0.0296 (3) | |
| H8 | 0.530 (2) | 0.0058 (9) | 0.282 (2) | 0.027 (4)* | |
| C9 | 0.81506 (18) | 0.02312 (8) | 0.38677 (18) | 0.0270 (3) | |
| C10 | 0.9717 (2) | 0.07130 (9) | 0.39725 (19) | 0.0291 (3) | |
| H10 | 0.959 (2) | 0.1202 (10) | 0.333 (2) | 0.040 (4)* | |
| C11 | 0.8479 (2) | −0.04871 (9) | 0.49188 (19) | 0.0295 (3) | |
| H11 | 0.740 (2) | −0.0827 (10) | 0.482 (2) | 0.039 (4)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| N1 | 0.0255 (6) | 0.0340 (7) | 0.0330 (6) | 0.0040 (5) | 0.0072 (5) | −0.0046 (5) |
| O1 | 0.0245 (5) | 0.0545 (7) | 0.0467 (7) | −0.0036 (5) | 0.0091 (5) | −0.0009 (5) |
| O2 | 0.0348 (6) | 0.0417 (6) | 0.0426 (6) | 0.0100 (5) | 0.0050 (5) | 0.0105 (5) |
| C1 | 0.0224 (6) | 0.0296 (7) | 0.0267 (7) | 0.0041 (5) | 0.0054 (5) | −0.0038 (5) |
| C2 | 0.0261 (7) | 0.0292 (7) | 0.0330 (7) | −0.0030 (5) | 0.0103 (6) | −0.0011 (6) |
| C3 | 0.0309 (7) | 0.0280 (7) | 0.0299 (7) | −0.0001 (5) | 0.0087 (6) | 0.0026 (6) |
| C4 | 0.0267 (7) | 0.0279 (7) | 0.0260 (7) | 0.0015 (5) | 0.0064 (5) | −0.0017 (5) |
| C5 | 0.0246 (7) | 0.0322 (7) | 0.0355 (8) | −0.0021 (5) | 0.0093 (6) | 0.0031 (6) |
| C6 | 0.0295 (7) | 0.0293 (7) | 0.0312 (7) | 0.0027 (5) | 0.0089 (6) | 0.0056 (6) |
| C7 | 0.0244 (7) | 0.0331 (8) | 0.0314 (7) | −0.0010 (6) | 0.0059 (6) | −0.0005 (6) |
| C8 | 0.0260 (7) | 0.0312 (7) | 0.0300 (7) | 0.0002 (6) | 0.0071 (5) | −0.0017 (6) |
| C9 | 0.0278 (7) | 0.0301 (7) | 0.0221 (6) | 0.0037 (5) | 0.0066 (5) | −0.0032 (5) |
| C10 | 0.0313 (7) | 0.0283 (7) | 0.0268 (7) | 0.0034 (5) | 0.0082 (5) | 0.0026 (5) |
| C11 | 0.0270 (7) | 0.0313 (7) | 0.0294 (7) | −0.0008 (5) | 0.0082 (5) | −0.0011 (6) |
Geometric parameters (Å, °)
| N1—O1 | 1.2253 (16) | C5—H5 | 0.932 (16) |
| N1—O2 | 1.2332 (15) | C6—H6 | 0.950 (16) |
| N1—C1 | 1.4661 (17) | C7—C8 | 1.334 (2) |
| C1—C6 | 1.3765 (19) | C7—H7 | 0.969 (16) |
| C1—C2 | 1.381 (2) | C8—C9 | 1.4640 (19) |
| C2—C3 | 1.379 (2) | C8—H8 | 0.951 (15) |
| C2—H2 | 0.940 (16) | C9—C10 | 1.399 (2) |
| C3—C4 | 1.4001 (19) | C9—C11 | 1.4020 (19) |
| C3—H3 | 0.953 (16) | C10—C11i | 1.384 (2) |
| C4—C5 | 1.3999 (19) | C10—H10 | 0.930 (17) |
| C4—C7 | 1.4670 (19) | C11—C10i | 1.384 (2) |
| C5—C6 | 1.3868 (19) | C11—H11 | 0.968 (17) |
| O1—N1—O2 | 123.49 (12) | C1—C6—C5 | 118.71 (13) |
| O1—N1—C1 | 118.79 (12) | C1—C6—H6 | 121.2 (10) |
| O2—N1—C1 | 117.71 (11) | C5—C6—H6 | 120.1 (10) |
| C6—C1—C2 | 122.13 (12) | C8—C7—C4 | 125.71 (13) |
| C6—C1—N1 | 119.44 (12) | C8—C7—H7 | 121.2 (9) |
| C2—C1—N1 | 118.42 (12) | C4—C7—H7 | 113.1 (9) |
| C3—C2—C1 | 118.68 (13) | C7—C8—C9 | 126.21 (14) |
| C3—C2—H2 | 120.4 (9) | C7—C8—H8 | 120.2 (9) |
| C1—C2—H2 | 120.9 (9) | C9—C8—H8 | 113.6 (9) |
| C2—C3—C4 | 121.26 (13) | C10—C9—C11 | 117.57 (12) |
| C2—C3—H3 | 118.2 (9) | C10—C9—C8 | 123.46 (13) |
| C4—C3—H3 | 120.6 (9) | C11—C9—C8 | 118.97 (13) |
| C5—C4—C3 | 118.20 (12) | C11i—C10—C9 | 120.98 (13) |
| C5—C4—C7 | 119.61 (13) | C11i—C10—H10 | 117.5 (10) |
| C3—C4—C7 | 122.18 (13) | C9—C10—H10 | 121.5 (10) |
| C6—C5—C4 | 120.96 (13) | C10i—C11—C9 | 121.45 (13) |
| C6—C5—H5 | 118.6 (9) | C10i—C11—H11 | 121.0 (9) |
| C4—C5—H5 | 120.5 (9) | C9—C11—H11 | 117.6 (9) |
| O1—N1—C1—C6 | −178.44 (12) | N1—C1—C6—C5 | −176.92 (12) |
| O2—N1—C1—C6 | 2.28 (19) | C4—C5—C6—C1 | 0.4 (2) |
| O1—N1—C1—C2 | 2.67 (19) | C5—C4—C7—C8 | −170.57 (14) |
| O2—N1—C1—C2 | −176.61 (12) | C3—C4—C7—C8 | 9.5 (2) |
| C6—C1—C2—C3 | −2.3 (2) | C4—C7—C8—C9 | 179.87 (13) |
| N1—C1—C2—C3 | 176.57 (12) | C7—C8—C9—C10 | 1.9 (2) |
| C1—C2—C3—C4 | 0.3 (2) | C7—C8—C9—C11 | −177.62 (13) |
| C2—C3—C4—C5 | 1.9 (2) | C11—C9—C10—C11i | −0.2 (2) |
| C2—C3—C4—C7 | −178.18 (13) | C8—C9—C10—C11i | −179.77 (13) |
| C3—C4—C5—C6 | −2.3 (2) | C10—C9—C11—C10i | 0.2 (2) |
| C7—C4—C5—C6 | 177.80 (13) | C8—C9—C11—C10i | 179.80 (13) |
| C2—C1—C6—C5 | 1.9 (2) |
Symmetry codes: (i) −x+2, −y, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG2592).
References
- Bazan, G., Bartholomew, G., Bu, X. & Lachicotte, R. (2000). Chem. Mater.12, 1422–1430.
- Borsche, W. (1912). Justus Liebigs Ann. Chem.386, 351-73.
- Bruker (2001). SMART and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
- He, T., Wang, C., Pan, X., Yang, H. & Lu, G. (2008). Dyes Pigm.82, 47–52.
- Moreno-Fuquen, R., Aguirre, L. & Kennedy, A. R. (2008). Acta Cryst. E64, o2259. [DOI] [PMC free article] [PubMed]
- Moreno-Fuquen, R., Dvries, R., Theodoro, J. & Ellena, J. (2009). Acta Cryst. E65, o1371. [DOI] [PMC free article] [PubMed]
- Nakatsuji, S., Akiyama, S., Katzerb, G. & Fabian, W. (1991). J. Chem. Soc. Perkin Trans. 2, pp. 861–867.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Westrip, S. P. (2009). publCIF In preparation.
Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809024751/ng2592sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809024751/ng2592Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


