organic compounds
(E)-N-(4-Bromophenyl)-1-(quinolin-2-yl)methanimine
aSchool of Agriculture and Science, Discipline of Chemistry, University of KwaZulu-Natal, Private Bag X54001, Durban, 4000, South Africa, and bDepartment of Chemical Sciences, Olabisi Onabanjo University, Ago-Iwoye, PMB 2001, Nigeria
*Correspondence e-mail: [email protected]
The title compound, C16H11BrN2, is a Schiff base formed through the condensation reaction of 2-quinolinecarboxaldehyde with 4-bromoaniline. The C=N bond length of 1.282 (2) Å is consistent with its double-bond character. The imine linkage adopts the E configuration, as indicated by the N—C—C—N torsion angle of 174.27 (14)°. This value also demonstrates that the quinoline ring and imine group are arranged in an almost coplanar manner. In contrast, the 4-bromophenyl ring is significantly twisted relative to the imine-quinoline plane, as indicated by the C—N—C—C torsion angle of approximately 46.8 (2)°. Intermolecular C—H⋯π interactions between quinolinyl and bromophenyl rings form a three-dimensional supramolecular network in the crystal packing.
Keywords: crystal structure; Schiff base; quinoline; imine; 4-bromophenyl.
CCDC reference: 2583971
Structure description
Schiff base compounds derived from aromatic and primary constitute an important class of organic ligands that have been extensively investigated owing to their ease of preparation, structural versatility, and broad biological and pharmacological profiles, including antibacterial, antifungal, and anticancer activities (Boulechfar et al., 2023
; Adeleke et al., 2022
). Among the various aldehyde building blocks employed, quinolinecarboxaldehyde is of particular interest because it incorporates the quinoline pharmacophore, a privileged scaffold in medicinal chemistry known for its activity against a wide range of pathogens and tumour cell lines (Solomon et al., 2011
). The resulting quinoline-derived Schiff bases combine the chelating and biological potential of the quinoline unit with the donor flexibility of the imine nitrogen, rendering them attractive precursors for metal-complex synthesis and functional material applications (Sonawane et al., 2023
).
The asymmetric unit of the title compound consists of a single, neutral molecule of (E)-N-(4-bromophenyl)-1-(quinolin-2-yl)methanimine. The molecule comprises a quinoline ring system connected at its 2-position to a methanimine (–CH=N–) bridge, which in turn links to a 4-bromophenyl ring at the imine nitrogen (Fig. 1
). The quinoline ring system and the imine fragment are coplanar, as the torsion angles within the quinoline ring confirm near-perfect planarity of this moiety, and the imine carbon lies in this plane, as reflected by the torsion of −2.9 (2)°. In contrast, the 4-bromophenyl ring is significantly twisted with respect to the quinoline–imine plane, as shown by the torsion angle C10—N2—C11—C12 of 46.8 (2)°. Other intramolecular bond parameters are comparable to closely related quinoline-based Schiff bases reported in the literature (Oladipo et al., 2025
; Wang et al.. 2017a
,b
; Faizi et al., 2015
). The crystal packing of the title compound features C–H⋯π interactions between the quinolinyl and bromophenyl rings of neighbouring molecules, forming a three-dimensional supramolecular network. (Table 1
, Fig. 2
).
|
| Figure 1 The molecular structure of the title compound shown with displacement ellipsoids at the 50% probability level. |
| Figure 2 Representation of the C—H⋯π hydrogen bonds in the of the title compound (dashed orange lines). |
Synthesis and crystallization
The title compound was synthesized by the condensation reaction of an equimolar amount of 2-quinolinecarboxaldehyde with 4-bromoaniline in methanol, with a catalytic amount of glacial acetic acid. The reaction mixture was refluxed for 6 h at 80°C for 4 h, during which time a yellow precipitate was formed. The solid product was isolated by filtration, washed with cold ethanol, and dried in air (Adeleke et al., 2021
). Single crystals were obtained by slow evaporation of the concentrated solution of the product in ethanol at room temperature.
Refinement
Crystal data, data collection and structure details are summarized in Table 2
.
|
Structural data
CCDC reference: 2583971
contains datablock I. DOI: https://doi.org/10.1107/S2414314626008953/bt4206sup1.cif
Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2414314626008953/bt4206Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2414314626008953/bt4206Isup3.cml
| C16H11BrN2 | F(000) = 624 |
| Mr = 311.18 | Dx = 1.607 Mg m−3 |
| Monoclinic, P21/c | Cu Kα radiation, λ = 1.54178 Å |
| a = 15.3817 (4) Å | Cell parameters from 9977 reflections |
| b = 13.9338 (4) Å | θ = 2.9–68.1° |
| c = 6.0050 (2) Å | µ = 4.23 mm−1 |
| β = 91.654 (1)° | T = 100 K |
| V = 1286.49 (7) Å3 | Plate, colourless |
| Z = 4 | 0.42 × 0.33 × 0.05 mm |
| Bruker APEXII CCD diffractometer | 2346 independent reflections |
| Radiation source: microfocus sealed X-ray tube, Incoatec Iµs | 2224 reflections with I > 2σ(I) |
| Mirror optics monochromator | Rint = 0.040 |
| Detector resolution: 7.9 pixels mm-1 | θmax = 68.1°, θmin = 2.9° |
| φ and ω scans | h = −18→17 |
| Absorption correction: multi-scan (SADABS; Krause et al., 2015) wR2(int) was 0.1018 before and 0.0553 after correction. The ratio of minimum to maximum transmission is 0.7237. The λ/2 correction factor is 0.0015. | k = −16→16 |
| Tmin = 0.545, Tmax = 0.753 | l = −6→7 |
| 19912 measured reflections |
| Refinement on F2 | 0 restraints |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.023 | H-atom parameters constrained |
| wR(F2) = 0.062 | w = 1/[σ2(Fo2) + (0.0377P)2 + 0.4867P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.05 | (Δ/σ)max = 0.001 |
| 2346 reflections | Δρmax = 0.22 e Å−3 |
| 172 parameters | Δρmin = −0.45 e Å−3 |
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. Hydrogen atoms were located in a difference map and refined as riding on their parent atom with U(H) = 1.2Ueq(C) and with C—H = 0.95 Å. |
| x | y | z | Uiso*/Ueq | ||
| Br1 | 0.03190 (2) | 0.63813 (2) | 1.15570 (3) | 0.02712 (9) | |
| N1 | 0.59463 (8) | 0.58283 (8) | 0.7717 (2) | 0.0175 (3) | |
| N2 | 0.37000 (9) | 0.61932 (9) | 0.6575 (2) | 0.0185 (3) | |
| C13 | 0.21335 (10) | 0.66459 (10) | 1.1058 (3) | 0.0187 (3) | |
| H13 | 0.211684 | 0.692263 | 1.250160 | 0.022* | |
| C7 | 0.60856 (10) | 0.65857 (10) | 0.3381 (3) | 0.0194 (3) | |
| H7 | 0.612642 | 0.682644 | 0.190800 | 0.023* | |
| C5 | 0.68526 (11) | 0.64033 (9) | 0.4694 (3) | 0.0176 (3) | |
| C8 | 0.52919 (11) | 0.64130 (9) | 0.4251 (3) | 0.0197 (3) | |
| H8 | 0.477397 | 0.653464 | 0.339721 | 0.024* | |
| C4 | 0.76976 (11) | 0.66208 (11) | 0.3979 (3) | 0.0204 (3) | |
| H4 | 0.777239 | 0.689339 | 0.254716 | 0.024* | |
| C1 | 0.74967 (10) | 0.58019 (10) | 0.8203 (3) | 0.0187 (3) | |
| H1 | 0.743555 | 0.551406 | 0.962403 | 0.022* | |
| C6 | 0.67467 (10) | 0.60071 (10) | 0.6855 (2) | 0.0167 (3) | |
| C14 | 0.13806 (11) | 0.62969 (10) | 1.0021 (3) | 0.0187 (3) | |
| C10 | 0.44132 (10) | 0.59306 (10) | 0.7552 (2) | 0.0187 (3) | |
| H10 | 0.440070 | 0.565713 | 0.900039 | 0.022* | |
| C11 | 0.29350 (10) | 0.61891 (10) | 0.7815 (3) | 0.0173 (3) | |
| C9 | 0.52518 (9) | 0.60476 (11) | 0.6458 (2) | 0.0172 (3) | |
| C12 | 0.29111 (10) | 0.65845 (10) | 0.9953 (3) | 0.0183 (3) | |
| H12 | 0.343228 | 0.681321 | 1.065495 | 0.022* | |
| C16 | 0.21614 (10) | 0.58570 (10) | 0.6789 (2) | 0.0186 (3) | |
| H16 | 0.217073 | 0.560089 | 0.532372 | 0.022* | |
| C15 | 0.13827 (10) | 0.58990 (10) | 0.7894 (3) | 0.0199 (3) | |
| H15 | 0.086093 | 0.566078 | 0.721322 | 0.024* | |
| C3 | 0.84113 (11) | 0.64401 (10) | 0.5343 (3) | 0.0217 (3) | |
| H3 | 0.897616 | 0.659973 | 0.486127 | 0.026* | |
| C2 | 0.83087 (10) | 0.60168 (11) | 0.7465 (3) | 0.0212 (3) | |
| H2 | 0.880681 | 0.588095 | 0.838352 | 0.025* |
| U11 | U22 | U33 | U12 | U13 | U23 | |
| Br1 | 0.01970 (13) | 0.03373 (14) | 0.02817 (13) | −0.00120 (6) | 0.00494 (8) | −0.00493 (6) |
| N1 | 0.0213 (6) | 0.0120 (6) | 0.0193 (6) | 0.0004 (5) | 0.0011 (5) | 0.0001 (5) |
| N2 | 0.0214 (7) | 0.0127 (5) | 0.0214 (6) | −0.0001 (5) | 0.0009 (5) | −0.0005 (5) |
| C13 | 0.0238 (8) | 0.0124 (6) | 0.0196 (7) | 0.0003 (6) | −0.0003 (6) | −0.0003 (6) |
| C7 | 0.0270 (8) | 0.0133 (6) | 0.0180 (7) | 0.0010 (6) | 0.0005 (6) | 0.0003 (6) |
| C5 | 0.0239 (8) | 0.0103 (7) | 0.0187 (8) | −0.0004 (5) | 0.0019 (6) | −0.0023 (5) |
| C8 | 0.0229 (8) | 0.0147 (7) | 0.0212 (8) | 0.0002 (5) | −0.0024 (6) | 0.0000 (5) |
| C4 | 0.0268 (8) | 0.0136 (6) | 0.0211 (8) | −0.0023 (6) | 0.0053 (6) | −0.0021 (6) |
| C1 | 0.0233 (8) | 0.0126 (6) | 0.0203 (7) | 0.0007 (5) | −0.0001 (6) | −0.0008 (5) |
| C6 | 0.0202 (7) | 0.0101 (6) | 0.0198 (7) | −0.0003 (5) | 0.0020 (6) | −0.0017 (5) |
| C14 | 0.0184 (8) | 0.0154 (7) | 0.0224 (8) | 0.0017 (5) | 0.0037 (6) | 0.0013 (6) |
| C10 | 0.0224 (8) | 0.0130 (7) | 0.0207 (7) | 0.0002 (5) | 0.0011 (6) | 0.0004 (6) |
| C11 | 0.0208 (8) | 0.0107 (6) | 0.0204 (7) | 0.0018 (5) | 0.0002 (6) | 0.0028 (6) |
| C9 | 0.0199 (8) | 0.0109 (7) | 0.0208 (8) | −0.0001 (5) | 0.0001 (6) | −0.0012 (5) |
| C12 | 0.0207 (8) | 0.0123 (6) | 0.0218 (8) | −0.0005 (6) | −0.0032 (6) | −0.0003 (6) |
| C16 | 0.0239 (8) | 0.0130 (6) | 0.0188 (7) | 0.0006 (5) | −0.0007 (6) | −0.0008 (5) |
| C15 | 0.0200 (8) | 0.0166 (7) | 0.0231 (8) | −0.0019 (6) | −0.0027 (6) | −0.0002 (6) |
| C3 | 0.0227 (8) | 0.0158 (7) | 0.0268 (8) | −0.0027 (5) | 0.0047 (7) | −0.0042 (6) |
| C2 | 0.0200 (8) | 0.0162 (7) | 0.0271 (8) | 0.0010 (6) | −0.0022 (6) | −0.0041 (6) |
| Br1—C14 | 1.9021 (16) | C4—C3 | 1.374 (2) |
| N1—C6 | 1.372 (2) | C1—H1 | 0.9500 |
| N1—C9 | 1.3264 (19) | C1—C6 | 1.419 (2) |
| N2—C10 | 1.282 (2) | C1—C2 | 1.370 (2) |
| N2—C11 | 1.411 (2) | C14—C15 | 1.392 (2) |
| C13—H13 | 0.9500 | C10—H10 | 0.9500 |
| C13—C14 | 1.387 (2) | C10—C9 | 1.474 (2) |
| C13—C12 | 1.387 (2) | C11—C12 | 1.399 (2) |
| C7—H7 | 0.9500 | C11—C16 | 1.403 (2) |
| C7—C5 | 1.423 (2) | C12—H12 | 0.9500 |
| C7—C8 | 1.363 (2) | C16—H16 | 0.9500 |
| C5—C4 | 1.413 (2) | C16—C15 | 1.387 (2) |
| C5—C6 | 1.423 (2) | C15—H15 | 0.9500 |
| C8—H8 | 0.9500 | C3—H3 | 0.9500 |
| C8—C9 | 1.423 (2) | C3—C2 | 1.417 (2) |
| C4—H4 | 0.9500 | C2—H2 | 0.9500 |
| C9—N1—C6 | 117.37 (13) | C15—C14—Br1 | 119.61 (12) |
| C10—N2—C11 | 118.23 (13) | N2—C10—H10 | 119.6 |
| C14—C13—H13 | 120.5 | N2—C10—C9 | 120.83 (14) |
| C14—C13—C12 | 118.95 (14) | C9—C10—H10 | 119.6 |
| C12—C13—H13 | 120.5 | C12—C11—N2 | 121.82 (14) |
| C5—C7—H7 | 120.2 | C12—C11—C16 | 119.25 (15) |
| C8—C7—H7 | 120.2 | C16—C11—N2 | 118.67 (14) |
| C8—C7—C5 | 119.59 (14) | N1—C9—C8 | 123.88 (14) |
| C7—C5—C6 | 117.34 (15) | N1—C9—C10 | 114.92 (13) |
| C4—C5—C7 | 123.26 (15) | C8—C9—C10 | 121.14 (13) |
| C4—C5—C6 | 119.37 (15) | C13—C12—C11 | 120.61 (14) |
| C7—C8—H8 | 120.5 | C13—C12—H12 | 119.7 |
| C7—C8—C9 | 118.90 (14) | C11—C12—H12 | 119.7 |
| C9—C8—H8 | 120.5 | C11—C16—H16 | 119.7 |
| C5—C4—H4 | 119.8 | C15—C16—C11 | 120.62 (14) |
| C3—C4—C5 | 120.37 (15) | C15—C16—H16 | 119.7 |
| C3—C4—H4 | 119.8 | C14—C15—H15 | 120.6 |
| C6—C1—H1 | 119.8 | C16—C15—C14 | 118.72 (14) |
| C2—C1—H1 | 119.8 | C16—C15—H15 | 120.6 |
| C2—C1—C6 | 120.33 (14) | C4—C3—H3 | 119.8 |
| N1—C6—C5 | 122.81 (14) | C4—C3—C2 | 120.30 (16) |
| N1—C6—C1 | 118.13 (13) | C2—C3—H3 | 119.8 |
| C1—C6—C5 | 119.05 (14) | C1—C2—C3 | 120.52 (15) |
| C13—C14—Br1 | 118.56 (12) | C1—C2—H2 | 119.7 |
| C13—C14—C15 | 121.83 (15) | C3—C2—H2 | 119.7 |
| Br1—C14—C15—C16 | 179.06 (11) | C6—N1—C9—C8 | 2.9 (2) |
| N2—C10—C9—N1 | 174.27 (14) | C6—N1—C9—C10 | −174.18 (12) |
| N2—C10—C9—C8 | −2.9 (2) | C6—C5—C4—C3 | 0.8 (2) |
| N2—C11—C12—C13 | 174.38 (13) | C6—C1—C2—C3 | −0.4 (2) |
| N2—C11—C16—C15 | −175.74 (13) | C14—C13—C12—C11 | 0.9 (2) |
| C13—C14—C15—C16 | −0.3 (2) | C10—N2—C11—C12 | 46.8 (2) |
| C7—C5—C4—C3 | 178.98 (13) | C10—N2—C11—C16 | −139.02 (14) |
| C7—C5—C6—N1 | −2.1 (2) | C11—N2—C10—C9 | −171.29 (13) |
| C7—C5—C6—C1 | 179.09 (13) | C11—C16—C15—C14 | 1.4 (2) |
| C7—C8—C9—N1 | −2.5 (2) | C9—N1—C6—C5 | −0.6 (2) |
| C7—C8—C9—C10 | 174.41 (13) | C9—N1—C6—C1 | 178.28 (13) |
| C5—C7—C8—C9 | −0.3 (2) | C12—C13—C14—Br1 | 179.79 (11) |
| C5—C4—C3—C2 | 1.2 (2) | C12—C13—C14—C15 | −0.8 (2) |
| C8—C7—C5—C4 | −175.72 (14) | C12—C11—C16—C15 | −1.4 (2) |
| C8—C7—C5—C6 | 2.5 (2) | C16—C11—C12—C13 | 0.3 (2) |
| C4—C5—C6—N1 | 176.16 (13) | C2—C1—C6—N1 | −176.41 (13) |
| C4—C5—C6—C1 | −2.7 (2) | C2—C1—C6—C5 | 2.5 (2) |
| C4—C3—C2—C1 | −1.4 (2) |
| Cg1, Cg2 and Cg3 are the centroids of the N1/C5–C9, C1–C6 and C11–C16 rings, respectively. |
| D—H···A | D—H | H···A | D···A | D—H···A |
| C1—H1···Cg3i | 0.95 | 2.67 | 3.3703 (16) | 131 |
| C4—H4···Cg2ii | 0.95 | 2.79 | 3.4808 (17) | 130 |
| C7—H7···Cg1ii | 0.95 | 2.85 | 3.5026 (16) | 127 |
| C13—H13···Cg3iii | 0.95 | 2.69 | 3.4042 (16) | 132 |
| C16—H16···Cg2iv | 0.95 | 2.70 | 3.3932 (15) | 131 |
| Symmetry codes: (i) −x+1, −y+1, −z+2; (ii) x, −y+1/2, z−3/2; (iii) x, −y+1/2, z−1/2; (iv) −x+1, −y+1, −z+1. |
Acknowledgements
The authors are grateful to the University of KwaZulu-Natal for providing access to X-ray diffraction facilities.
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