organic compounds
2,3-Diethylbenzo[g]quinoxaline
aCentral Connecticut State University, Department of Chemistry & Biochemistry, 1619 Stanley Street, New Britain, CT 06050, USA, and bDepartment of Chemistry & Biochemistry, Central Connecticut State University, 1619 Stanley Street, New Britain, CT 06053, USA
*Correspondence e-mail: crundwellg@ccsu.edu
The title compound, C16H16N2, was synthesized by dispersing 3,4-hexanedione in a methanol–water solution containing the acid catalyst NH4HF2, then adding 1,2-diaminonaphthalene. The fused-ring system of the title compound is close to planar (r.m.s. deviation = 0.028 Å); one of the pendant methyl C atoms lies close to the ring plane [deviation = 0.071 (2) Å; N—C—C—C = −0.27 (18)°] whereas the other is significantly displaced [–1.7136 (18) Å; 91.64 (16)°]. The molecules pack in I in a distinctive criss-cross motif supported by numerous aromatic π–π stacking interactions [shortest centroid–centroid separation = 3.5805 (6) Å].
Keywords: crystal structure; benzoquinoxaline.
CCDC reference: 1994287
Structure description
The bond lengths and angles in the title compound fall within their expected values and the C3–C14/N1/N2 fused-ring system is close to planar (r.m.s. deviation = 0.028 Å). The C1 methyl atom lies close to the ring plane [deviation = 0.071 (2) Å; N1—C3—C2—C1 = −0.027 (16)°] whereas C16 is significantly displaced [deviation = −1.7136 (18) Å; N2—C14—C15—C16 = 91.64 (16)°] (Fig. 1).
In the crystal, the molecles pack in a distinctive criss-cross motif (Fig. 2) in I with stacks of molecules propagating in the [001] direction. Numerous aromatic π–π stacking interactions help to consolidate the packing [shortest centroid–centroid separation = 3.5805 (6) Å].
Synthesis and crystallization
2,3-Diethylbenzo[g]quinoxaline, C16H16N2, was prepared using the method used by Lassagne et al. (2015) to create 2,3-diarylpyridopyrazines. In a 50-ml Erlenmeyer flask equipped with a stir bar, 10.0 mmol of hexanedione (1.14 g) was dispersed in 20 ml of a 2.5 × 10−3 M NH4HF2 solution in MeOH and 2 ml of distilled water. To that stirred solution, 10.0 mmol of 1,2-naphthalenediamine (1.58 g) was added. The solution was allowed to stir overnight despite evidence of product after the first hour: 1.44 grams of a pale whitish powder was filtered and washed with two 2 ml aliquots of ice-cold methanol (60.9% yield). The crude product was mostly pure by NMR but was further purified by recrystallization from a 50:50 methanol/toluene solution (1.11 g recovered, 47.0% yield overall). (m.p. 411 K) ATR–IR (cm−1) 2981, 2934, 1703, 1575, 1455, 1351, 1325, 910, 889, 754; 1H NMR (300 MHz, CDCl3): δ 8.58 (s, 1H), 8.07 (m, 1H), 7.55 (m, 1H) 3.09 (q, 2H), 1.49 (t, 3H); 13C (300 MHz, CDCl3): δ 158.14, 138.06, 133.24, 128.35, 126.57, 126.15, 28.63, 12.07. Crystals for the diffraction experiment were grown from slow evaporation of a methylene chloride solution. FTIR, 1H NMR, and 13C NMR spectra are given as supporting information.
Refinement
Crystal data, data collection and structure . The of the crystal chosen for data collection was indeterminate in the reported here.
details are summarized in Table 1Structural data
CCDC reference: 1994287
https://doi.org/10.1107/S241431462000454X/hb4346sup1.cif
contains datablock I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S241431462000454X/hb4346Isup2.hkl
Supplementary Material (FTIR, 1H NMR, 13C NMR). DOI: https://doi.org/10.1107/S241431462000454X/hb4346sup3.pdf
Supporting information file. DOI: https://doi.org/10.1107/S241431462000454X/hb4346Isup4.cml
Data collection: CrysAlis PRO (Rigaku, 2018); cell
CrysAlis PRO (Rigaku, 2018); data reduction: CrysAlis PRO (Rigaku, 2018); program(s) used to solve structure: SHELXM (Sheldrick, 2008); program(s) used to refine structure: SHELXL (Sheldrick, 2008); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).C16H16N2 | Melting point: 411 K |
Mr = 236.31 | Mo Kα radiation, λ = 0.71073 Å |
Tetragonal, I4 | Cell parameters from 7488 reflections |
a = 13.93535 (18) Å | θ = 4.6–31.8° |
c = 13.1629 (3) Å | µ = 0.07 mm−1 |
V = 2556.16 (7) Å3 | T = 293 K |
Z = 8 | Block, white |
F(000) = 1008 | 0.39 × 0.33 × 0.27 mm |
Dx = 1.228 Mg m−3 |
Rigaku Xcalibur, Sapphire3 diffractometer | 4779 independent reflections |
Radiation source: fine-focus sealed X-ray tube, Enhance (Mo) X-ray Source | 3869 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.031 |
Detector resolution: 16.1790 pixels mm-1 | θmax = 33.6°, θmin = 4.3° |
ω scans | h = −21→21 |
Absorption correction: multi-scan (CrysAlisPro; Rigaku, 2018) | k = −21→21 |
Tmin = 0.922, Tmax = 1.000 | l = −20→19 |
31103 measured reflections |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.048 | H-atom parameters constrained |
wR(F2) = 0.136 | w = 1/[σ2(Fo2) + (0.0756P)2 + 0.2732P] where P = (Fo2 + 2Fc2)/3 |
S = 1.04 | (Δ/σ)max < 0.001 |
4779 reflections | Δρmax = 0.28 e Å−3 |
165 parameters | Δρmin = −0.14 e Å−3 |
0 restraints | Absolute structure: Flack H D (1983), Acta Cryst. A39, 876-881 |
Primary atom site location: dual | Absolute structure parameter: 0 (2) |
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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. H atoms were included in calculated positions with C—H = 0.93–0.97 Å and refined as riding atoms with Uiso = 1.2Ueq(C) or 1.5Ueq(methyl C). Reflections affected by the beam stop were omitted from the refinement. |
x | y | z | Uiso*/Ueq | ||
C1 | −0.29561 (13) | −1.16936 (12) | −0.44274 (13) | 0.0600 (4) | |
H1A | −0.3206 | −1.1110 | −0.4711 | 0.090* | |
H1B | −0.3333 | −1.2227 | −0.4659 | 0.090* | |
H1C | −0.2302 | −1.1776 | −0.4640 | 0.090* | |
C2 | −0.29974 (10) | −1.16422 (10) | −0.32887 (12) | 0.0493 (3) | |
H2A | −0.2793 | −1.2256 | −0.3016 | 0.059* | |
H2B | −0.3660 | −1.1546 | −0.3087 | 0.059* | |
C3 | −0.23964 (8) | −1.08656 (8) | −0.28133 (10) | 0.0379 (2) | |
C4 | −0.13277 (8) | −0.96118 (8) | −0.29463 (9) | 0.0328 (2) | |
C5 | −0.07941 (9) | −0.89899 (9) | −0.35476 (9) | 0.0378 (2) | |
H5 | −0.0815 | −0.9047 | −0.4251 | 0.045* | |
C6 | −0.02254 (8) | −0.82781 (8) | −0.31001 (9) | 0.0360 (2) | |
C7 | 0.03189 (10) | −0.76181 (10) | −0.36928 (12) | 0.0475 (3) | |
H7 | 0.0310 | −0.7661 | −0.4398 | 0.057* | |
C8 | 0.08527 (12) | −0.69247 (11) | −0.32317 (15) | 0.0567 (4) | |
H8 | 0.1199 | −0.6493 | −0.3627 | 0.068* | |
C9 | 0.08872 (12) | −0.68520 (11) | −0.21668 (15) | 0.0608 (4) | |
H9 | 0.1253 | −0.6372 | −0.1867 | 0.073* | |
C10 | 0.03930 (10) | −0.74736 (11) | −0.15731 (12) | 0.0515 (3) | |
H10 | 0.0430 | −0.7421 | −0.0870 | 0.062* | |
C11 | −0.01854 (8) | −0.82097 (9) | −0.20173 (10) | 0.0369 (2) | |
C12 | −0.07119 (8) | −0.88458 (9) | −0.14191 (9) | 0.0380 (2) | |
H12 | −0.0676 | −0.8806 | −0.0715 | 0.046* | |
C13 | −0.12889 (8) | −0.95376 (8) | −0.18678 (8) | 0.0333 (2) | |
C14 | −0.23818 (8) | −1.07610 (9) | −0.17124 (10) | 0.0381 (2) | |
C15 | −0.30438 (11) | −1.13340 (11) | −0.10459 (12) | 0.0522 (3) | |
H15A | −0.2763 | −1.1398 | −0.0375 | 0.063* | |
H15B | −0.3123 | −1.1972 | −0.1328 | 0.063* | |
C16 | −0.40207 (12) | −1.08493 (14) | −0.09594 (16) | 0.0684 (5) | |
H16A | −0.4299 | −1.0786 | −0.1623 | 0.103* | |
H16B | −0.3945 | −1.0225 | −0.0661 | 0.103* | |
H16C | −0.4434 | −1.1231 | −0.0539 | 0.103* | |
N1 | −0.18907 (7) | −1.03067 (7) | −0.34033 (9) | 0.0388 (2) | |
N2 | −0.18387 (7) | −1.01278 (8) | −0.12633 (8) | 0.0388 (2) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0616 (8) | 0.0543 (8) | 0.0641 (10) | −0.0115 (7) | −0.0117 (8) | −0.0176 (7) |
C2 | 0.0434 (6) | 0.0432 (7) | 0.0613 (9) | −0.0115 (5) | −0.0068 (6) | −0.0058 (6) |
C3 | 0.0336 (5) | 0.0337 (5) | 0.0463 (6) | −0.0024 (4) | −0.0068 (5) | −0.0029 (4) |
C4 | 0.0293 (5) | 0.0313 (5) | 0.0377 (5) | −0.0020 (4) | −0.0033 (4) | −0.0039 (4) |
C5 | 0.0381 (5) | 0.0396 (6) | 0.0358 (5) | −0.0027 (4) | −0.0006 (4) | −0.0041 (4) |
C6 | 0.0306 (5) | 0.0336 (5) | 0.0439 (6) | −0.0011 (4) | 0.0009 (4) | −0.0024 (4) |
C7 | 0.0441 (6) | 0.0445 (6) | 0.0539 (8) | −0.0059 (5) | 0.0057 (6) | 0.0018 (6) |
C8 | 0.0494 (8) | 0.0470 (7) | 0.0738 (11) | −0.0151 (6) | 0.0073 (7) | 0.0010 (7) |
C9 | 0.0510 (8) | 0.0494 (8) | 0.0820 (12) | −0.0184 (6) | −0.0056 (8) | −0.0122 (8) |
C10 | 0.0467 (7) | 0.0515 (7) | 0.0563 (8) | −0.0122 (6) | −0.0081 (6) | −0.0113 (6) |
C11 | 0.0302 (5) | 0.0360 (5) | 0.0446 (6) | 0.0000 (4) | −0.0049 (4) | −0.0058 (4) |
C12 | 0.0365 (6) | 0.0423 (6) | 0.0353 (5) | −0.0022 (4) | −0.0059 (4) | −0.0042 (4) |
C13 | 0.0292 (5) | 0.0340 (5) | 0.0368 (5) | 0.0016 (4) | −0.0041 (4) | 0.0006 (4) |
C14 | 0.0341 (5) | 0.0356 (5) | 0.0445 (6) | 0.0005 (4) | −0.0041 (5) | 0.0067 (5) |
C15 | 0.0550 (8) | 0.0455 (7) | 0.0561 (8) | −0.0093 (6) | −0.0022 (6) | 0.0152 (6) |
C16 | 0.0504 (8) | 0.0754 (11) | 0.0794 (11) | −0.0118 (8) | 0.0130 (8) | 0.0169 (9) |
N1 | 0.0364 (5) | 0.0390 (5) | 0.0409 (5) | −0.0054 (4) | −0.0047 (4) | −0.0056 (4) |
N2 | 0.0384 (5) | 0.0402 (5) | 0.0378 (5) | −0.0016 (4) | −0.0044 (4) | 0.0044 (4) |
C1—H1A | 0.9600 | C8—H8 | 0.9300 |
C1—H1B | 0.9600 | C8—C9 | 1.406 (3) |
C1—H1C | 0.9600 | C9—H9 | 0.9300 |
C1—C2 | 1.502 (2) | C9—C10 | 1.355 (2) |
C2—H2A | 0.9700 | C10—H10 | 0.9300 |
C2—H2B | 0.9700 | C10—C11 | 1.4296 (16) |
C2—C3 | 1.5047 (17) | C11—C12 | 1.3943 (17) |
C3—C14 | 1.4566 (18) | C12—H12 | 0.9300 |
C3—N1 | 1.3062 (16) | C12—C13 | 1.3873 (15) |
C4—C5 | 1.3894 (15) | C13—N2 | 1.3772 (15) |
C4—C13 | 1.4245 (15) | C14—C15 | 1.5027 (18) |
C4—N1 | 1.3839 (13) | C14—N2 | 1.3042 (16) |
C5—H5 | 0.9300 | C15—H15A | 0.9700 |
C5—C6 | 1.3997 (16) | C15—H15B | 0.9700 |
C6—C7 | 1.4247 (17) | C15—C16 | 1.524 (2) |
C6—C11 | 1.4296 (17) | C16—H16A | 0.9600 |
C7—H7 | 0.9300 | C16—H16B | 0.9600 |
C7—C8 | 1.362 (2) | C16—H16C | 0.9600 |
H1A—C1—H1B | 109.5 | C10—C9—C8 | 120.77 (14) |
H1A—C1—H1C | 109.5 | C10—C9—H9 | 119.6 |
H1B—C1—H1C | 109.5 | C9—C10—H10 | 119.7 |
C2—C1—H1A | 109.5 | C9—C10—C11 | 120.63 (14) |
C2—C1—H1B | 109.5 | C11—C10—H10 | 119.7 |
C2—C1—H1C | 109.5 | C6—C11—C10 | 118.53 (12) |
C1—C2—H2A | 108.4 | C12—C11—C6 | 120.01 (10) |
C1—C2—H2B | 108.4 | C12—C11—C10 | 121.46 (12) |
C1—C2—C3 | 115.34 (12) | C11—C12—H12 | 119.8 |
H2A—C2—H2B | 107.5 | C13—C12—C11 | 120.42 (10) |
C3—C2—H2A | 108.4 | C13—C12—H12 | 119.8 |
C3—C2—H2B | 108.4 | C12—C13—C4 | 119.79 (10) |
C14—C3—C2 | 119.57 (11) | N2—C13—C4 | 120.75 (10) |
N1—C3—C2 | 118.81 (11) | N2—C13—C12 | 119.44 (10) |
N1—C3—C14 | 121.62 (10) | C3—C14—C15 | 121.27 (11) |
C5—C4—C13 | 120.14 (10) | N2—C14—C3 | 121.79 (11) |
N1—C4—C5 | 119.49 (10) | N2—C14—C15 | 116.81 (12) |
N1—C4—C13 | 120.37 (10) | C14—C15—H15A | 109.5 |
C4—C5—H5 | 119.8 | C14—C15—H15B | 109.5 |
C4—C5—C6 | 120.35 (10) | C14—C15—C16 | 110.89 (12) |
C6—C5—H5 | 119.8 | H15A—C15—H15B | 108.1 |
C5—C6—C7 | 121.91 (11) | C16—C15—H15A | 109.5 |
C5—C6—C11 | 119.27 (11) | C16—C15—H15B | 109.5 |
C7—C6—C11 | 118.82 (11) | C15—C16—H16A | 109.5 |
C6—C7—H7 | 119.8 | C15—C16—H16B | 109.5 |
C8—C7—C6 | 120.31 (13) | C15—C16—H16C | 109.5 |
C8—C7—H7 | 119.8 | H16A—C16—H16B | 109.5 |
C7—C8—H8 | 119.5 | H16A—C16—H16C | 109.5 |
C7—C8—C9 | 120.93 (14) | H16B—C16—H16C | 109.5 |
C9—C8—H8 | 119.5 | C3—N1—C4 | 117.69 (10) |
C8—C9—H9 | 119.6 | C14—N2—C13 | 117.71 (10) |
Acknowledgements
This research was funded by a CCSU–AAUP research grant.
References
Dolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339–341. Web of Science CrossRef CAS IUCr Journals Google Scholar
Lassagne, F., Chevallier, F., Roisnel, T., Dorcet, V., Mongin, F. & Domingo, L. R. (2015). Synthesis, 47, 2680–2689. Web of Science CrossRef CAS Google Scholar
Rigaku (2018). CrysAlis PRO. Rigaku Inc., Tokyo, Japan. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.