research communications
and Hirshfeld surface analysis of a pyridiniminium bromide salt: 1-[2-([1,1′-biphenyl]-4-yl)-2-oxoethyl]-3-methyl-1,4-dihydropyridin-4-iminium bromide
aDepartment of Chemistry, GSSS Institute of Engineering & Technology for Women, Mysuru 570 016, Karnataka, India, bSchool of Chemical Sciences, Universiti Sains Malaysia, Penang 11800 USM, Malaysia, cDepartment of Engineering Chemistry, Vidya Vikas Institute of Engineering & Technology, Visvesvaraya Technological University, Alanahally, Mysuru 570 028, Karnataka, India, dX-ray Crystallography Unit, School of Physics, Universiti Sains Malaysia, 11800 USM, Penang, Malaysia, eDepartment of Chemistry, Cauvery Institute of Technology, Mandya 571 402, Karnataka, India, fDepartment of Chemistry, Sri Siddhartha Institute of Technology, Tumkur 572 105, Karnataka, India, and gDepartment of Chemistry, Science College, An-Najah National University, PO Box 7, Nablus, West Bank, Palestinian Territories
*Correspondence e-mail: chidankumar@gmail.com, khalil.i@najah.edu
In the cation of the title salt, C20H19N2O+·Br−, the phenyl rings are inclined to one another by 38.38 (8)°, whereas the central phenyl ring and the pyridiniminium ring are almost perpendicular with a dihedral angle of 87.37 (9)°. The N+=C cationic double bond was verified by the shortened bond length of 1.337 (2) Å. In the crystal, the Br− anion is linked to the cation by an N—H⋯Br hydrogen bond. C—H⋯O hydrogen bonds link adjacent pyridiniminium cations into inversion dimers with an R22(18) graph-set motif. These dimers are stacked in a phenyl–phenyl T-shaped geometry through C—H⋯π interactions. A Hirshfeld surface analysis was conducted to verify the contributions of the different intermolecular interactions.
Keywords: crystal structure; ionic liquids; pyridiniminium salt; hydrogen bonding; Hirshfeld surface analysis.
CCDC reference: 1839059
1. Chemical context
Over the past decade, ionic liquids have been the subject of intense research as a customizable replacement for volatile organic solvents because of their negligible vapor pressure, excellent thermal stability, high ). A wide range of applications using ionic liquids has been reported in many areas, such as their use as homogeneous and heterogeneous catalysts (Dong et al., 2016) and biological reaction media (Lopes et al., 2017), and in nuclear waste treatment (Ha et al., 2010) and water purification (Fuerhacker et al., 2012; Wang & Wei, 2017).
and solvation ability (Davis, 2004In the view of the above and of our research interest in the synthesis of ionic liquids, we present in this study the
and Hirshfeld surface analysis of the title pyridiniminium halide salt.2. Structural commentary
Fig. 1 shows the of the title salt, consisting of one 1-(2-([1,1′-biphenyl]-4-yl)-2-oxoethyl)-3-methylpyridin-4(1H)-iminium cation and one bromide anion. The cation is constructed from a pyridiniminium ring (N1/C15–C19) and a biphenyl unit (C1–C6 and C7–C12), interconnected by a (C=O)—C ketone bridge. The biphenyl conformation experiences non-bounded steric repulsion between ortho-hydrogen atoms (Poater et al., 2006), with the phenyl rings inclined to one another by 38.38 (8)°. The second phenyl ring (C7–C12) is nearly parallel to the ketone bridge (O1/C13–C14), as shown by the torsion angles C9—C10—C13—O1 [−179.10 (18)°] and C9—C10—C13—C14 [1.7 (2)°]. Conversely, this phenyl ring is almost perpendicular to the pyridiniminium ring [dihedral angle = 87.37 (9)°]. The bond lengths and angles in the cation are generally within normal ranges. However, the N2—C17 bond [1.337 (2) Å] is shorter than expected for an NH2—Car single bond [1.38 (3) Å] although similar bond lengths have been observed in related compounds with an N+=C double bond (Chidan Kumar et al., 2017; Sharmila et al., 2014; Yue et al., 2013).
3. Supramolecular features
In the crystal, the bromide anion is linked to the cation via an N2—H2N2⋯Br1 hydrogen bond (Table 1). The bromide anion is surrounded by three other cations with short H⋯Br contracts varying from 2.52 to 2.88 Å (Table 1). Pairs of C1—H1A⋯O1 hydrogen bonds link the pyridiniminium cations into inversion dimers with an (18) graph-set motif (Table 1, Fig. 2). The dimers are stacked in a phenyl–phenyl T-shaped geometry through C3—H3A⋯Cg1 interactions (Cg1 is the centroid of the C1–C6 phenyl ring).
4. Hirshfeld surface analysis
The Hirshfeld surface analysis (Spackman & Jayatilaka, 2009) of the title salt was generated by CrystalExplorer3.1 (Wolff et al., 2012), and comprised dnorm surface plots, electrostatic potentials and 2D fingerprint plots (Spackman & McKinnon, 2002). The ball-and-stick model, dnorm surface plots and electrostatic potentials of the title salt are shown in Fig. 3. Those plots were generated to quantify and visualize the intermolecular interactions and to explain the observed crystal packing. The dark-red spots on the dnorm surface arise as a result of short interatomic contacts, while the other weak intermolecular interactions appear as light-red spots. Furthermore, negative electrostatic potential (red regions) in the electrostatic potential map indicates hydrogen-acceptor potential, whereas the hydrogen donors are represented by positive electrostatic potential (blue regions) (Spackman et al., 2008).
The dnorm surface of the title salt shows a dark-red spot on the N–H hydrogen atom and on the bromide atom, which is the result of the strong N2—H1N2⋯Br1 and N2—H2N2⋯Br1 hydrogen bonds present in the structure (Fig. 4a). These observations are further confirmed by the respective electrostatic potential maps, where the atoms involved in strong hydrogen bonds are seen as dark-blue and dark-red regions (Fig. 4b). Beside those two short intermolecular contacts, the C—H⋯O and C—H⋯Br interactions are shown as light-red spots on the dnorm surface (Fig. 5). Finally, the C—H⋯π interaction is shown as a light-red spot on the dnorm surface (Fig. 6).
A quantitative analysis of the intermolecular interactions can be made by studying the fingerprint plots (FP). The FP is shown with characteristic pseudo-symmetry wings in the de and di diagonal axes represent the overall two-dimensional FP and those delineated into H⋯H, H⋯C/C⋯H, H⋯Br/Br⋯H and H⋯O/O⋯H contacts, respectively (Fig. 7). The most significant intermolecular interactions are the H⋯H interaction (41.8%), which appear at the central region of the FP with de = di ≃ 2.2 Å (Fig. 7b). The reciprocal H⋯C/C⋯H interactions appear as two symmetrical broad wings with de + di ≃ 2.7 Å and contribute 29.2% to the Hirshfeld surface (Fig. 7c). The reciprocal H⋯Br/Br⋯H and H⋯O/O⋯H interactions with 16.7% and 7.3% contributions are present as sharp symmetrical spikes at diagonal axes de + di ≃ 2.3 and 2.4 Å, respectively (Fig. 7d–e). The percentage contributions for other intermolecular contacts are less than 5% in the Hirshfeld surface mapping.
5. Synthesis and crystallization
The synthesis of the title compound is illustrated in Fig. 8. A mixture of 1-([1,1′-biphenyl]-4-yl)-2-bromoethan-1-one (2.75 g, 10 mmol) and 3-methylpyridin-4-amine (0.11 g, 1mmol) was dissolved in 10 ml of toluene at room temperature, followed by stirring at 358 K for 18 h. The completion of the reaction was marked by the amount of the separated solid from the initially clear and homogenous mixture of the starting materials. The solid was filtered from the unreacted starting materials and solvent, and subsequently washed with ethyl acetate. The final pyridiniminium salt was obtained after the solid was dried under reduced pressure to remove all volatile organic compounds (Said et al., 2017). Plate-like yellow crystals were obtained by slow evaporation of a solution in acetone.
6. Refinement
Crystal data, data collection and structure . C-bound H atoms were positioned geometrically [C—H = 0.95–0.99 Å] and refined using a riding model with Uiso(H) = 1.2 or 1.5Ueq(C). All N-bound H atoms were located from a difference-Fourier map and freely refined.
details are summarized in Table 2
|
Supporting information
CCDC reference: 1839059
https://doi.org/10.1107/S2056989018006217/xu5923sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989018006217/xu5923Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2056989018006217/xu5923Isup3.cml
Data collection: APEX2 (Bruker, 2012); cell
SAINT (Bruker, 2012); data reduction: SAINT (Bruker, 2012); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2013 (Sheldrick, 2015); molecular graphics: SHELXL2013 (Sheldrick, 2015) and Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXL2013 (Sheldrick, 2015) and PLATON (Spek, 2009).C20H19N2O+·Br− | F(000) = 784 |
Mr = 383.28 | Dx = 1.441 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
a = 15.3991 (10) Å | Cell parameters from 7970 reflections |
b = 7.9078 (5) Å | θ = 2.6–28.7° |
c = 15.7645 (10) Å | µ = 2.34 mm−1 |
β = 113.037 (1)° | T = 100 K |
V = 1766.6 (2) Å3 | Plate, yellow |
Z = 4 | 0.27 × 0.11 × 0.08 mm |
Bruker APEXII DUO CCD area-detector diffractometer | 4731 independent reflections |
Radiation source: fine-focus sealed tube | 3913 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.040 |
φ and ω scans | θmax = 29.2°, θmin = 2.6° |
Absorption correction: multi-scan (SADABS; Bruker, 2012) | h = −20→21 |
Tmin = 0.499, Tmax = 0.574 | k = −10→10 |
28949 measured reflections | l = −21→21 |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.030 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.075 | w = 1/[σ2(Fo2) + (0.0375P)2 + 0.8608P] where P = (Fo2 + 2Fc2)/3 |
S = 1.03 | (Δ/σ)max = 0.001 |
4731 reflections | Δρmax = 0.70 e Å−3 |
226 parameters | Δρmin = −0.23 e Å−3 |
Experimental. The following wavelength and cell were deduced by SADABS from the direction cosines etc. They are given here for emergency use only: CELL 0.71093 15.443 7.924 15.800 89.974 113.042 90.030 |
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. |
x | y | z | Uiso*/Ueq | ||
Br1 | 0.92732 (2) | 1.53732 (2) | 0.32391 (2) | 0.02112 (6) | |
N1 | 0.85797 (10) | 0.77203 (18) | 0.52316 (10) | 0.0165 (3) | |
N2 | 0.92877 (11) | 1.25846 (19) | 0.48455 (12) | 0.0191 (3) | |
H1N2 | 0.9168 (16) | 1.296 (3) | 0.4320 (17) | 0.028 (6)* | |
H2N2 | 0.9689 (16) | 1.310 (3) | 0.5315 (16) | 0.026 (6)* | |
O1 | 0.68941 (9) | 0.74507 (17) | 0.53143 (11) | 0.0288 (3) | |
C1 | 0.48304 (13) | −0.0147 (2) | 0.60543 (12) | 0.0190 (3) | |
H1A | 0.4442 | 0.0614 | 0.5597 | 0.023* | |
C2 | 0.44287 (13) | −0.1546 (2) | 0.62926 (12) | 0.0217 (4) | |
H2A | 0.3769 | −0.1739 | 0.5993 | 0.026* | |
C3 | 0.49803 (13) | −0.2662 (2) | 0.69624 (13) | 0.0232 (4) | |
H3A | 0.4703 | −0.3613 | 0.7127 | 0.028* | |
C4 | 0.59455 (14) | −0.2375 (2) | 0.73918 (13) | 0.0241 (4) | |
H4A | 0.6328 | −0.3130 | 0.7856 | 0.029* | |
C5 | 0.63554 (13) | −0.0997 (2) | 0.71483 (13) | 0.0209 (4) | |
H5A | 0.7018 | −0.0830 | 0.7436 | 0.025* | |
C6 | 0.57967 (12) | 0.0150 (2) | 0.64790 (12) | 0.0166 (3) | |
C7 | 0.62172 (12) | 0.1671 (2) | 0.62368 (11) | 0.0160 (3) | |
C8 | 0.71004 (12) | 0.1613 (2) | 0.61812 (12) | 0.0177 (3) | |
H8A | 0.7449 | 0.0587 | 0.6312 | 0.021* | |
C9 | 0.74715 (12) | 0.3039 (2) | 0.59364 (12) | 0.0176 (3) | |
H9A | 0.8072 | 0.2981 | 0.5900 | 0.021* | |
C10 | 0.69697 (12) | 0.4563 (2) | 0.57416 (12) | 0.0159 (3) | |
C11 | 0.60974 (12) | 0.4633 (2) | 0.58173 (12) | 0.0173 (3) | |
H11A | 0.5756 | 0.5667 | 0.5703 | 0.021* | |
C12 | 0.57262 (12) | 0.3209 (2) | 0.60576 (12) | 0.0181 (3) | |
H12A | 0.5129 | 0.3273 | 0.6102 | 0.022* | |
C13 | 0.73288 (12) | 0.6126 (2) | 0.54717 (12) | 0.0174 (3) | |
C14 | 0.82786 (12) | 0.6034 (2) | 0.53803 (13) | 0.0187 (3) | |
H14A | 0.8757 | 0.5539 | 0.5948 | 0.022* | |
H14B | 0.8224 | 0.5293 | 0.4856 | 0.022* | |
C15 | 0.83058 (12) | 0.8351 (2) | 0.43666 (12) | 0.0178 (3) | |
H15A | 0.7958 | 0.7642 | 0.3861 | 0.021* | |
C16 | 0.85084 (12) | 0.9961 (2) | 0.41921 (12) | 0.0181 (3) | |
C17 | 0.90417 (11) | 1.1006 (2) | 0.49601 (12) | 0.0160 (3) | |
C18 | 0.92986 (12) | 1.0325 (2) | 0.58534 (12) | 0.0168 (3) | |
H18A | 0.9638 | 1.0999 | 0.6378 | 0.020* | |
C19 | 0.90626 (12) | 0.8711 (2) | 0.59677 (12) | 0.0175 (3) | |
H19A | 0.9239 | 0.8270 | 0.6573 | 0.021* | |
C20 | 0.81947 (15) | 1.0614 (3) | 0.32252 (13) | 0.0268 (4) | |
H20A | 0.7890 | 0.9700 | 0.2790 | 0.040* | |
H20B | 0.8743 | 1.1026 | 0.3118 | 0.040* | |
H20C | 0.7745 | 1.1541 | 0.3135 | 0.040* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.02487 (10) | 0.02019 (10) | 0.01683 (9) | −0.00208 (7) | 0.00658 (7) | 0.00115 (7) |
N1 | 0.0153 (7) | 0.0152 (7) | 0.0203 (7) | −0.0005 (5) | 0.0083 (6) | −0.0004 (6) |
N2 | 0.0222 (8) | 0.0166 (7) | 0.0195 (8) | −0.0018 (6) | 0.0091 (6) | 0.0010 (6) |
O1 | 0.0230 (7) | 0.0184 (6) | 0.0487 (9) | 0.0050 (5) | 0.0179 (6) | 0.0081 (6) |
C1 | 0.0190 (8) | 0.0230 (9) | 0.0155 (8) | −0.0001 (7) | 0.0072 (7) | 0.0000 (7) |
C2 | 0.0197 (9) | 0.0271 (9) | 0.0200 (9) | −0.0050 (7) | 0.0097 (7) | −0.0031 (7) |
C3 | 0.0284 (10) | 0.0218 (9) | 0.0233 (9) | −0.0050 (7) | 0.0144 (8) | 0.0009 (7) |
C4 | 0.0272 (10) | 0.0219 (9) | 0.0245 (9) | 0.0033 (7) | 0.0116 (8) | 0.0063 (7) |
C5 | 0.0197 (8) | 0.0205 (8) | 0.0230 (9) | 0.0004 (7) | 0.0090 (7) | 0.0026 (7) |
C6 | 0.0193 (8) | 0.0172 (8) | 0.0155 (8) | −0.0003 (6) | 0.0093 (7) | −0.0008 (6) |
C7 | 0.0165 (8) | 0.0174 (8) | 0.0134 (8) | −0.0011 (6) | 0.0052 (6) | 0.0001 (6) |
C8 | 0.0173 (8) | 0.0158 (8) | 0.0201 (8) | 0.0011 (6) | 0.0073 (7) | 0.0006 (6) |
C9 | 0.0163 (8) | 0.0178 (8) | 0.0204 (9) | 0.0007 (6) | 0.0089 (7) | −0.0007 (7) |
C10 | 0.0160 (8) | 0.0165 (8) | 0.0145 (8) | −0.0005 (6) | 0.0052 (6) | −0.0005 (6) |
C11 | 0.0161 (8) | 0.0164 (8) | 0.0181 (8) | 0.0030 (6) | 0.0053 (6) | 0.0011 (7) |
C12 | 0.0147 (8) | 0.0203 (8) | 0.0198 (8) | 0.0020 (6) | 0.0072 (7) | 0.0008 (7) |
C13 | 0.0151 (8) | 0.0162 (8) | 0.0198 (8) | 0.0005 (6) | 0.0054 (7) | 0.0011 (7) |
C14 | 0.0189 (8) | 0.0136 (7) | 0.0248 (9) | 0.0001 (6) | 0.0096 (7) | 0.0012 (7) |
C15 | 0.0166 (8) | 0.0196 (8) | 0.0164 (8) | −0.0010 (6) | 0.0056 (7) | −0.0014 (6) |
C16 | 0.0145 (8) | 0.0225 (9) | 0.0171 (8) | 0.0010 (6) | 0.0059 (7) | 0.0009 (6) |
C17 | 0.0141 (8) | 0.0163 (8) | 0.0199 (8) | 0.0019 (6) | 0.0092 (7) | −0.0007 (7) |
C18 | 0.0181 (8) | 0.0183 (8) | 0.0152 (8) | −0.0007 (7) | 0.0078 (6) | −0.0023 (7) |
C19 | 0.0179 (8) | 0.0189 (8) | 0.0178 (8) | 0.0024 (6) | 0.0093 (7) | 0.0016 (7) |
C20 | 0.0282 (10) | 0.0311 (10) | 0.0169 (9) | −0.0046 (8) | 0.0044 (7) | 0.0049 (8) |
N1—C15 | 1.355 (2) | C8—H8A | 0.9500 |
N1—C19 | 1.356 (2) | C9—C10 | 1.400 (2) |
N1—C14 | 1.460 (2) | C9—H9A | 0.9500 |
N2—C17 | 1.337 (2) | C10—C11 | 1.395 (2) |
N2—H1N2 | 0.83 (2) | C10—C13 | 1.483 (2) |
N2—H2N2 | 0.86 (2) | C11—C12 | 1.381 (2) |
O1—C13 | 1.215 (2) | C11—H11A | 0.9500 |
C1—C2 | 1.389 (3) | C12—H12A | 0.9500 |
C1—C6 | 1.392 (2) | C13—C14 | 1.526 (2) |
C1—H1A | 0.9500 | C14—H14A | 0.9900 |
C2—C3 | 1.383 (3) | C14—H14B | 0.9900 |
C2—H2A | 0.9500 | C15—C16 | 1.365 (2) |
C3—C4 | 1.390 (3) | C15—H15A | 0.9500 |
C3—H3A | 0.9500 | C16—C17 | 1.430 (2) |
C4—C5 | 1.387 (3) | C16—C20 | 1.499 (3) |
C4—H4A | 0.9500 | C17—C18 | 1.412 (2) |
C5—C6 | 1.402 (2) | C18—C19 | 1.358 (2) |
C5—H5A | 0.9500 | C18—H18A | 0.9500 |
C6—C7 | 1.485 (2) | C19—H19A | 0.9500 |
C7—C8 | 1.397 (2) | C20—H20A | 0.9800 |
C7—C12 | 1.401 (2) | C20—H20B | 0.9800 |
C8—C9 | 1.385 (2) | C20—H20C | 0.9800 |
C15—N1—C19 | 119.94 (15) | C12—C11—C10 | 120.46 (16) |
C15—N1—C14 | 120.28 (15) | C12—C11—H11A | 119.8 |
C19—N1—C14 | 119.51 (15) | C10—C11—H11A | 119.8 |
C17—N2—H1N2 | 120.3 (16) | C11—C12—C7 | 120.95 (16) |
C17—N2—H2N2 | 118.3 (15) | C11—C12—H12A | 119.5 |
H1N2—N2—H2N2 | 120 (2) | C7—C12—H12A | 119.5 |
C2—C1—C6 | 120.64 (17) | O1—C13—C10 | 122.65 (16) |
C2—C1—H1A | 119.7 | O1—C13—C14 | 119.56 (16) |
C6—C1—H1A | 119.7 | C10—C13—C14 | 117.78 (15) |
C3—C2—C1 | 120.60 (17) | N1—C14—C13 | 110.35 (14) |
C3—C2—H2A | 119.7 | N1—C14—H14A | 109.6 |
C1—C2—H2A | 119.7 | C13—C14—H14A | 109.6 |
C2—C3—C4 | 119.21 (17) | N1—C14—H14B | 109.6 |
C2—C3—H3A | 120.4 | C13—C14—H14B | 109.6 |
C4—C3—H3A | 120.4 | H14A—C14—H14B | 108.1 |
C5—C4—C3 | 120.62 (17) | N1—C15—C16 | 122.72 (16) |
C5—C4—H4A | 119.7 | N1—C15—H15A | 118.6 |
C3—C4—H4A | 119.7 | C16—C15—H15A | 118.6 |
C4—C5—C6 | 120.33 (17) | C15—C16—C17 | 118.01 (16) |
C4—C5—H5A | 119.8 | C15—C16—C20 | 121.21 (17) |
C6—C5—H5A | 119.8 | C17—C16—C20 | 120.78 (16) |
C1—C6—C5 | 118.57 (16) | N2—C17—C18 | 120.51 (16) |
C1—C6—C7 | 120.31 (16) | N2—C17—C16 | 121.62 (16) |
C5—C6—C7 | 121.11 (16) | C18—C17—C16 | 117.87 (16) |
C8—C7—C12 | 118.53 (16) | C19—C18—C17 | 120.40 (16) |
C8—C7—C6 | 121.51 (15) | C19—C18—H18A | 119.8 |
C12—C7—C6 | 119.96 (15) | C17—C18—H18A | 119.8 |
C9—C8—C7 | 120.55 (16) | N1—C19—C18 | 121.01 (16) |
C9—C8—H8A | 119.7 | N1—C19—H19A | 119.5 |
C7—C8—H8A | 119.7 | C18—C19—H19A | 119.5 |
C8—C9—C10 | 120.64 (16) | C16—C20—H20A | 109.5 |
C8—C9—H9A | 119.7 | C16—C20—H20B | 109.5 |
C10—C9—H9A | 119.7 | H20A—C20—H20B | 109.5 |
C11—C10—C9 | 118.85 (16) | C16—C20—H20C | 109.5 |
C11—C10—C13 | 118.12 (15) | H20A—C20—H20C | 109.5 |
C9—C10—C13 | 123.02 (16) | H20B—C20—H20C | 109.5 |
C6—C1—C2—C3 | 0.6 (3) | C11—C10—C13—O1 | −0.1 (3) |
C1—C2—C3—C4 | −0.5 (3) | C9—C10—C13—O1 | −179.10 (18) |
C2—C3—C4—C5 | −0.6 (3) | C11—C10—C13—C14 | −179.35 (16) |
C3—C4—C5—C6 | 1.5 (3) | C9—C10—C13—C14 | 1.7 (2) |
C2—C1—C6—C5 | 0.3 (3) | C15—N1—C14—C13 | −87.86 (19) |
C2—C1—C6—C7 | −178.51 (16) | C19—N1—C14—C13 | 86.16 (18) |
C4—C5—C6—C1 | −1.4 (3) | O1—C13—C14—N1 | 8.2 (2) |
C4—C5—C6—C7 | 177.47 (17) | C10—C13—C14—N1 | −172.54 (14) |
C1—C6—C7—C8 | −142.49 (18) | C19—N1—C15—C16 | 1.1 (3) |
C5—C6—C7—C8 | 38.7 (3) | C14—N1—C15—C16 | 175.11 (16) |
C1—C6—C7—C12 | 37.5 (2) | N1—C15—C16—C17 | 0.7 (3) |
C5—C6—C7—C12 | −141.33 (18) | N1—C15—C16—C20 | 179.90 (17) |
C12—C7—C8—C9 | −1.2 (3) | C15—C16—C17—N2 | 178.41 (16) |
C6—C7—C8—C9 | 178.73 (16) | C20—C16—C17—N2 | −0.8 (3) |
C7—C8—C9—C10 | 0.1 (3) | C15—C16—C17—C18 | −2.1 (2) |
C8—C9—C10—C11 | 1.4 (3) | C20—C16—C17—C18 | 178.76 (17) |
C8—C9—C10—C13 | −179.68 (16) | N2—C17—C18—C19 | −178.81 (16) |
C9—C10—C11—C12 | −1.6 (3) | C16—C17—C18—C19 | 1.7 (2) |
C13—C10—C11—C12 | 179.36 (16) | C15—N1—C19—C18 | −1.6 (2) |
C10—C11—C12—C7 | 0.5 (3) | C14—N1—C19—C18 | −175.62 (15) |
C8—C7—C12—C11 | 1.0 (3) | C17—C18—C19—N1 | 0.2 (3) |
C6—C7—C12—C11 | −179.00 (16) |
Cg1 is the centroid of the C1–C6 ring. |
D—H···A | D—H | H···A | D···A | D—H···A |
N2—H1N2···Br1 | 0.83 (2) | 2.61 (2) | 3.3514 (17) | 150 (2) |
N2—H2N2···Br1i | 0.86 (2) | 2.52 (2) | 3.3763 (17) | 174 (2) |
C1—H1A···O1ii | 0.95 | 2.52 | 3.431 (2) | 162 |
C14—H14A···Br1iii | 0.99 | 2.88 | 3.710 (2) | 141 |
C19—H19A···Br1iv | 0.95 | 2.82 | 3.5415 (18) | 134 |
C3—H3A···Cg1v | 0.95 | 2.81 | 3.6963 (19) | 155 |
Symmetry codes: (i) −x+2, −y+3, −z+1; (ii) −x+1, −y+1, −z+1; (iii) −x+2, −y+2, −z+1; (iv) x, −y+5/2, z+1/2; (v) −x+1, y−1/2, −z+3/2. |
Acknowledgements
HCK thanks the Malaysian Government for a MyBrain15 (MyPhD) scholarship.
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