Abstract
The asymmetric unit of the title compound, 2C16H14N4·C8H6N2, consits of one molecule of N,N′-bis(pyridin-2-yl)benzene-1,4-diamine (PDAB) and one half-molecule of quinoxaline (QX) that is located around an inversion centre and disordered over two overlapping positions. The PDAB molecule adopts a non-planar conformation with an E configuration at the two partially double exo C N bonds of the 2-pyridylamine units. In the crystal, these self-complementary units are N—H⋯N hydrogen bonded via a cyclic R 2 2(8) motif, creating tapes of PDAB molecules extending along [010]. Inversion-related tapes are arranged into pairs through π–π stacking interactions between the benzene rings [centroid–centroid distance = 3.818 (1) Å] and the two symmetry-independent pyridine groups [centroid–centroid distance = 3.760 (1) Å]. The QX molecules are enclosed in a cavity formed between six PDAB tapes.
Related literature
For the structures of polymorphic forms of N,N′-di(pyridin-2-yl)benzene-1,4-diamine and its co-crystal with phenazine, see: Bensemann et al. (2002 ▶); Wicher & Gdaniec (2011 ▶); Gdaniec et al. (2005 ▶).
Experimental
Crystal data
2C16H14N4·C8H6N2
M r = 654.77
Monoclinic,
a = 11.8285 (9) Å
b = 9.1223 (7) Å
c = 14.7952 (9) Å
β = 93.698 (5)°
V = 1593.1 (2) Å3
Z = 2
Mo Kα radiation
μ = 0.09 mm−1
T = 130 K
0.50 × 0.30 × 0.25 mm
Data collection
Kuma KM-4-CCD κ-geometry diffractometer
8116 measured reflections
2897 independent reflections
2082 reflections with I > 2σ(I)
R int = 0.033
Refinement
R[F 2 > 2σ(F 2)] = 0.045
wR(F 2) = 0.121
S = 0.97
2897 reflections
226 parameters
H-atom parameters constrained
Δρmax = 0.22 e Å−3
Δρmin = −0.28 e Å−3
Data collection: CrysAlis CCD (Oxford Diffraction, 2002 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2002 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶) and Mercury (Macrae et al., 2006 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811046356/rz2662sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811046356/rz2662Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N14—H14N⋯N2i | 0.90 | 2.12 | 2.9998 (17) | 166 |
| N7—H7N⋯N16ii | 0.90 | 2.13 | 3.0173 (18) | 167 |
Symmetry codes: (i)
; (ii)
.
supplementary crystallographic information
Comment
N,N'-Di(pyridin-2-yl)benzene-1,4-diamine (PDAB) is a very versatile supramolecular reagent. It has been shown that it can cocrystallize with the aromatic base, phenazine, forming cocrystals with the 1:4 molar ratio (Gdaniec et al., 2005). In this cocrystal the PDAB molecule is centrosymmetric and adopts a nearly planar conformation and a Z,Z form, i.e. the configuration at the partially double exo C≐ N bonds of its two 2-pyridylamine units is Z. The PDAB molecules are hydrogen bonded to phenazine molecules but, most importantly, their π-faces are directed to the edges of the phenazine molecules arranged viaπ-π stacking interactions into quartets. To check whether a similar packing motif will be observed for a compound containing the pyrazine fragment but a reduced π-system compared to phenazine, an attempt was made to cocrystallize PDAB with quinoxaline (QX). Cocrystallization was successful when PDAB was dissolved in molten QX (m.p. 301 K) and the solution was slowly evaporated at 331 K yielding the title molecular complex with 2:1 PDAB/QX ratio (Fig. 1). In contrast with the PDAB/phenazine cocrystal, in the title complex the PDAB molecule is nonplanar and adopts an E,E form that promotes formation of a cyclic R22(8) motif via N—H···N hydrogen bond between the self-complementary 2-pyridylamine units (Table 1). These cyclic motifs assemble PDAB molecules into tapes extending along [010]. The tapes related by inversion center are arranged into pairs through π-π stacking interactions between the benzene rings [centroid-centroid distance 3.818 (1) Å] and the two symmetry independent pyridine groups [centroid-centroid distance 3.760 (1) Å] (Fig. 2). Similar tape motifs have been observed in two of the three PDAB polymorphs (Bensemann et al., 2002; Wicher & Gdaniec, 2011), however these polymorphic structures were not stabilized by π-π stacking interactions between the tapes.
The QX molecule, that is not hydrogen bonded to PDAB, is enclosed in a centrosymmetric cavity formed between six PDAB tapes (Fig. 3). This leads to a disorder of the non-centrosymmetric QX molecule which in the cavity is located, with equal occupancies, in two alternative overlapping positions. Thus QX molecule in this crystal structure simulates the shape of a naphthalene molecule.
As there are no specific interactions between QX and PDAB molecules the driving force for the complex formation with PDAB is different in the two cocrystals with the aromatic heterobases containing the pyrazine ring.
Experimental
N,N'-Di(pyridin-2-yl)benzene-1,4-diamine (0.07 g, 0.27 mmol) was dissolved in an excess of the melted quinoxaline. The solution was heated at 331 K and after a few days colourless crystal suitable for X-ray analysis were obtained.
Refinement
All H atoms were located in difference electron-density maps, however for further refinement their positions were determined geometrically with N—H and C—H bond lengths of 0.90 Å and 0.95 Å, respectively. All H atoms were refined in the riding-model approximation, with Uiso(H)=1.2Ueq(N,C).
Figures
Fig. 1.
: Asymmetric unit of the title compound with displacement ellipsoids shown at the 50% probability level. The elipsoids representing positions occupied equally by C and N atoms are coloured in grey and blue. The unlabelled atoms of quinoxaline are related to the labelled one by the symmetry operation: 1 - x,1 - y,1 - z.
Fig. 2.
: π-π stacking interactions connecting hydrogen-bonded PDAB tapes into pairs. N—H···N hydrogen bonds are shown as dashed lines.
Fig. 3.
: Crystal packing diagram viewed along b illustrating arrangement of the hydrogen-bonded tapes of PDAB in the crystal and quinoxaline molecules enclosed in the cavity formed between the tapes.
Crystal data
| 2C16H14N4·C8H6N2 | F(000) = 688 |
| Mr = 654.77 | Dx = 1.365 Mg m−3 |
| Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2yn | Cell parameters from 2533 reflections |
| a = 11.8285 (9) Å | θ = 4.1–25.0° |
| b = 9.1223 (7) Å | µ = 0.09 mm−1 |
| c = 14.7952 (9) Å | T = 130 K |
| β = 93.698 (5)° | Prism, colourless |
| V = 1593.1 (2) Å3 | 0.50 × 0.30 × 0.25 mm |
| Z = 2 |
Data collection
| Kuma KM-4-CCD κ-geometry diffractometer | 2082 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.033 |
| graphite | θmax = 25.4°, θmin = 4.1° |
| ω scans | h = −13→14 |
| 8116 measured reflections | k = −10→9 |
| 2897 independent reflections | l = −17→17 |
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)] = 0.045 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.121 | H-atom parameters constrained |
| S = 0.97 | w = 1/[σ2(Fo2) + (0.0796P)2] where P = (Fo2 + 2Fc2)/3 |
| 2897 reflections | (Δ/σ)max < 0.001 |
| 226 parameters | Δρmax = 0.22 e Å−3 |
| 0 restraints | Δρmin = −0.28 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 | Occ. (<1) | |
| N2 | 0.34420 (10) | 0.46004 (13) | 0.12792 (9) | 0.0251 (3) | |
| N7 | 0.44563 (11) | 0.24793 (13) | 0.12278 (9) | 0.0291 (3) | |
| H7N | 0.5037 | 0.3082 | 0.1126 | 0.035* | |
| N14 | 0.55190 (10) | −0.35168 (13) | 0.12548 (9) | 0.0295 (3) | |
| H14N | 0.4941 | −0.4122 | 0.1359 | 0.035* | |
| N16 | 0.65420 (10) | −0.56243 (13) | 0.11839 (9) | 0.0260 (3) | |
| C1 | 0.34338 (12) | 0.31287 (16) | 0.13482 (10) | 0.0232 (4) | |
| C3 | 0.24879 (13) | 0.53106 (17) | 0.14294 (10) | 0.0282 (4) | |
| H3 | 0.2492 | 0.6349 | 0.1382 | 0.034* | |
| C4 | 0.15003 (13) | 0.46477 (18) | 0.16475 (11) | 0.0301 (4) | |
| H4 | 0.0841 | 0.5205 | 0.1745 | 0.036* | |
| C5 | 0.15028 (13) | 0.31317 (18) | 0.17200 (11) | 0.0292 (4) | |
| H5 | 0.0839 | 0.2630 | 0.1876 | 0.035* | |
| C6 | 0.24654 (13) | 0.23600 (17) | 0.15651 (10) | 0.0266 (4) | |
| H6 | 0.2474 | 0.1321 | 0.1604 | 0.032* | |
| C8 | 0.46942 (13) | 0.09666 (16) | 0.12475 (10) | 0.0243 (4) | |
| C9 | 0.40085 (12) | −0.00484 (17) | 0.07789 (10) | 0.0264 (4) | |
| H9 | 0.3335 | 0.0269 | 0.0452 | 0.032* | |
| C10 | 0.42953 (13) | −0.15119 (16) | 0.07830 (10) | 0.0256 (4) | |
| H10 | 0.3813 | −0.2195 | 0.0463 | 0.031* | |
| C11 | 0.52812 (13) | −0.20032 (16) | 0.12488 (10) | 0.0253 (4) | |
| C12 | 0.59638 (13) | −0.09904 (17) | 0.17195 (11) | 0.0272 (4) | |
| H12 | 0.6637 | −0.1307 | 0.2047 | 0.033* | |
| C13 | 0.56739 (13) | 0.04714 (17) | 0.17172 (10) | 0.0270 (4) | |
| H13 | 0.6152 | 0.1152 | 0.2042 | 0.032* | |
| C15 | 0.65386 (13) | −0.41581 (16) | 0.11138 (10) | 0.0239 (4) | |
| C17 | 0.75049 (13) | −0.63284 (18) | 0.10303 (11) | 0.0302 (4) | |
| H17 | 0.7507 | −0.7367 | 0.1074 | 0.036* | |
| C18 | 0.84841 (14) | −0.56538 (18) | 0.08156 (11) | 0.0310 (4) | |
| H18 | 0.9149 | −0.6201 | 0.0719 | 0.037* | |
| C19 | 0.84671 (13) | −0.41393 (18) | 0.07442 (11) | 0.0303 (4) | |
| H19 | 0.9129 | −0.3628 | 0.0594 | 0.036* | |
| C20 | 0.75006 (13) | −0.33812 (17) | 0.08900 (10) | 0.0276 (4) | |
| H20 | 0.7482 | −0.2343 | 0.0840 | 0.033* | |
| C21 | 0.42626 (15) | 0.38226 (19) | 0.36086 (12) | 0.0393 (5) | |
| H21 | 0.3839 | 0.3310 | 0.3142 | 0.047* | |
| C22 | 0.53039 (16) | 0.44592 (18) | 0.34188 (13) | 0.0410 (5) | |
| H22 | 0.5570 | 0.4363 | 0.2829 | 0.049* | |
| N23 | 0.59282 (13) | 0.51949 (17) | 0.40527 (11) | 0.0368 (4) | 0.50 |
| C23 | 0.59282 (13) | 0.51949 (17) | 0.40527 (11) | 0.0368 (4) | 0.50 |
| H23 | 0.6629 | 0.5629 | 0.3922 | 0.044* | 0.50 |
| C24 | 0.55231 (12) | 0.53158 (16) | 0.49075 (11) | 0.0275 (4) | |
| C25 | 0.61465 (13) | 0.60804 (16) | 0.55764 (11) | 0.0357 (4) | 0.50 |
| H25 | 0.6846 | 0.6529 | 0.5457 | 0.043* | 0.50 |
| N25 | 0.61465 (13) | 0.60804 (16) | 0.55764 (11) | 0.0357 (4) | 0.50 |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| N2 | 0.0240 (7) | 0.0225 (7) | 0.0290 (7) | 0.0005 (5) | 0.0025 (6) | −0.0026 (5) |
| N7 | 0.0227 (7) | 0.0202 (7) | 0.0449 (9) | −0.0022 (5) | 0.0067 (6) | −0.0004 (6) |
| N14 | 0.0224 (7) | 0.0208 (7) | 0.0457 (9) | −0.0006 (5) | 0.0056 (6) | 0.0047 (6) |
| N16 | 0.0248 (7) | 0.0229 (7) | 0.0301 (8) | 0.0004 (5) | 0.0011 (6) | −0.0004 (6) |
| C1 | 0.0249 (8) | 0.0223 (8) | 0.0223 (8) | −0.0012 (6) | 0.0010 (6) | −0.0020 (6) |
| C3 | 0.0301 (9) | 0.0246 (8) | 0.0298 (9) | 0.0026 (7) | 0.0012 (7) | −0.0040 (7) |
| C4 | 0.0243 (8) | 0.0339 (9) | 0.0323 (9) | 0.0032 (7) | 0.0030 (7) | −0.0048 (7) |
| C5 | 0.0247 (8) | 0.0361 (9) | 0.0270 (9) | −0.0044 (7) | 0.0026 (7) | −0.0009 (7) |
| C6 | 0.0283 (9) | 0.0239 (8) | 0.0277 (9) | −0.0022 (7) | 0.0019 (7) | 0.0000 (6) |
| C8 | 0.0238 (8) | 0.0212 (8) | 0.0284 (9) | −0.0007 (6) | 0.0059 (7) | 0.0001 (6) |
| C9 | 0.0241 (8) | 0.0258 (8) | 0.0292 (9) | 0.0000 (7) | 0.0004 (7) | 0.0024 (7) |
| C10 | 0.0244 (8) | 0.0253 (8) | 0.0271 (9) | −0.0034 (6) | 0.0010 (6) | −0.0015 (6) |
| C11 | 0.0257 (8) | 0.0219 (8) | 0.0289 (9) | 0.0009 (6) | 0.0056 (7) | 0.0024 (6) |
| C12 | 0.0231 (8) | 0.0299 (9) | 0.0283 (9) | 0.0019 (7) | 0.0003 (7) | 0.0026 (7) |
| C13 | 0.0248 (8) | 0.0277 (9) | 0.0288 (9) | −0.0034 (7) | 0.0034 (7) | −0.0035 (7) |
| C15 | 0.0242 (8) | 0.0246 (8) | 0.0225 (8) | 0.0002 (6) | −0.0007 (6) | 0.0002 (6) |
| C17 | 0.0298 (9) | 0.0267 (8) | 0.0336 (9) | 0.0037 (7) | −0.0010 (7) | −0.0037 (7) |
| C18 | 0.0259 (9) | 0.0337 (9) | 0.0334 (9) | 0.0028 (7) | 0.0011 (7) | −0.0068 (7) |
| C19 | 0.0231 (9) | 0.0374 (10) | 0.0302 (9) | −0.0054 (7) | 0.0012 (7) | −0.0031 (7) |
| C20 | 0.0273 (9) | 0.0259 (8) | 0.0292 (9) | −0.0028 (7) | −0.0004 (7) | 0.0008 (7) |
| C21 | 0.0462 (11) | 0.0331 (10) | 0.0372 (11) | −0.0056 (8) | −0.0086 (9) | 0.0026 (8) |
| C22 | 0.0550 (12) | 0.0324 (10) | 0.0362 (10) | 0.0004 (9) | 0.0081 (9) | 0.0027 (8) |
| N23 | 0.0364 (9) | 0.0337 (9) | 0.0411 (10) | −0.0045 (7) | 0.0092 (7) | 0.0025 (7) |
| C23 | 0.0364 (9) | 0.0337 (9) | 0.0411 (10) | −0.0045 (7) | 0.0092 (7) | 0.0025 (7) |
| C24 | 0.0263 (8) | 0.0214 (8) | 0.0344 (9) | 0.0003 (6) | −0.0005 (7) | 0.0021 (7) |
| C25 | 0.0314 (8) | 0.0331 (9) | 0.0417 (10) | −0.0057 (7) | −0.0055 (7) | 0.0031 (7) |
| N25 | 0.0314 (8) | 0.0331 (9) | 0.0417 (10) | −0.0057 (7) | −0.0055 (7) | 0.0031 (7) |
Geometric parameters (Å, °)
| N2—C3 | 1.3324 (18) | C11—C12 | 1.385 (2) |
| N2—C1 | 1.3465 (19) | C12—C13 | 1.377 (2) |
| N7—C1 | 1.3686 (19) | C12—H12 | 0.9500 |
| N7—C8 | 1.4083 (19) | C13—H13 | 0.9500 |
| N7—H7N | 0.9001 | C15—C20 | 1.398 (2) |
| N14—C15 | 1.3685 (19) | C17—C18 | 1.367 (2) |
| N14—C11 | 1.4090 (19) | C17—H17 | 0.9500 |
| N14—H14N | 0.9000 | C18—C19 | 1.386 (2) |
| N16—C17 | 1.3397 (19) | C18—H18 | 0.9500 |
| N16—C15 | 1.3415 (19) | C19—C20 | 1.365 (2) |
| C1—C6 | 1.398 (2) | C19—H19 | 0.9500 |
| C3—C4 | 1.372 (2) | C20—H20 | 0.9500 |
| C3—H3 | 0.9500 | C21—N25i | 1.331 (2) |
| C4—C5 | 1.387 (2) | C21—C25i | 1.331 (2) |
| C4—H4 | 0.9500 | C21—C22 | 1.406 (3) |
| C5—C6 | 1.370 (2) | C21—H21 | 0.9499 |
| C5—H5 | 0.9500 | C22—N23 | 1.336 (2) |
| C6—H6 | 0.9500 | C22—H22 | 0.9500 |
| C8—C9 | 1.387 (2) | N23—C24 | 1.385 (2) |
| C8—C13 | 1.388 (2) | N23—H23 | 0.9500 |
| C9—C10 | 1.377 (2) | C24—C25 | 1.384 (2) |
| C9—H9 | 0.9500 | C24—C24i | 1.408 (3) |
| C10—C11 | 1.390 (2) | C25—C21i | 1.331 (2) |
| C10—H10 | 0.9500 | C25—H25 | 0.9499 |
| C3—N2—C1 | 117.51 (13) | C11—C12—H12 | 119.7 |
| C1—N7—C8 | 126.76 (13) | C12—C13—C8 | 121.08 (14) |
| C1—N7—H7N | 116.6 | C12—C13—H13 | 119.5 |
| C8—N7—H7N | 116.6 | C8—C13—H13 | 119.5 |
| C15—N14—C11 | 126.54 (13) | N16—C15—N14 | 114.37 (13) |
| C15—N14—H14N | 116.8 | N16—C15—C20 | 121.68 (14) |
| C11—N14—H14N | 116.7 | N14—C15—C20 | 123.92 (14) |
| C17—N16—C15 | 117.59 (14) | N16—C17—C18 | 124.47 (15) |
| N2—C1—N7 | 114.27 (13) | N16—C17—H17 | 117.8 |
| N2—C1—C6 | 121.83 (14) | C18—C17—H17 | 117.8 |
| N7—C1—C6 | 123.84 (14) | C17—C18—C19 | 117.27 (15) |
| N2—C3—C4 | 124.61 (15) | C17—C18—H18 | 121.4 |
| N2—C3—H3 | 117.7 | C19—C18—H18 | 121.4 |
| C4—C3—H3 | 117.7 | C20—C19—C18 | 120.08 (15) |
| C3—C4—C5 | 117.38 (15) | C20—C19—H19 | 120.0 |
| C3—C4—H4 | 121.3 | C18—C19—H19 | 120.0 |
| C5—C4—H4 | 121.3 | C19—C20—C15 | 118.89 (15) |
| C6—C5—C4 | 119.79 (15) | C19—C20—H20 | 120.6 |
| C6—C5—H5 | 120.1 | C15—C20—H20 | 120.6 |
| C4—C5—H5 | 120.1 | N25i—C21—C22 | 121.85 (16) |
| C5—C6—C1 | 118.86 (15) | C25i—C21—C22 | 121.85 (16) |
| C5—C6—H6 | 120.6 | N25i—C21—H21 | 119.1 |
| C1—C6—H6 | 120.6 | C25i—C21—H21 | 119.1 |
| C9—C8—C13 | 118.40 (14) | C22—C21—H21 | 119.1 |
| C9—C8—N7 | 122.29 (14) | N23—C22—C21 | 121.25 (17) |
| C13—C8—N7 | 119.25 (13) | N23—C22—H22 | 119.3 |
| C10—C9—C8 | 120.60 (14) | C21—C22—H22 | 119.4 |
| C10—C9—H9 | 119.7 | C22—N23—C24 | 118.20 (15) |
| C8—C9—H9 | 119.7 | C22—N23—H23 | 121.1 |
| C9—C10—C11 | 120.88 (14) | C24—N23—H23 | 120.7 |
| C9—C10—H10 | 119.6 | C25—C24—N23 | 119.55 (14) |
| C11—C10—H10 | 119.6 | C25—C24—C24i | 120.10 (19) |
| C12—C11—C10 | 118.52 (14) | N23—C24—C24i | 120.34 (18) |
| C12—C11—N14 | 122.74 (14) | C21i—C25—C24 | 118.25 (15) |
| C10—C11—N14 | 118.68 (13) | C21i—C25—H25 | 120.8 |
| C13—C12—C11 | 120.52 (14) | C24—C25—H25 | 120.9 |
| C13—C12—H12 | 119.7 | ||
| C3—N2—C1—N7 | −177.03 (13) | C11—C12—C13—C8 | 0.1 (2) |
| C3—N2—C1—C6 | 0.3 (2) | C9—C8—C13—C12 | 0.1 (2) |
| C8—N7—C1—N2 | −178.90 (14) | N7—C8—C13—C12 | −177.06 (14) |
| C8—N7—C1—C6 | 3.9 (2) | C17—N16—C15—N14 | 178.27 (13) |
| C1—N2—C3—C4 | −0.1 (2) | C17—N16—C15—C20 | −0.1 (2) |
| N2—C3—C4—C5 | 0.3 (2) | C11—N14—C15—N16 | 178.07 (14) |
| C3—C4—C5—C6 | −0.7 (2) | C11—N14—C15—C20 | −3.6 (2) |
| C4—C5—C6—C1 | 0.9 (2) | C15—N16—C17—C18 | 0.6 (2) |
| N2—C1—C6—C5 | −0.7 (2) | N16—C17—C18—C19 | −0.7 (2) |
| N7—C1—C6—C5 | 176.37 (14) | C17—C18—C19—C20 | 0.3 (2) |
| C1—N7—C8—C9 | 47.3 (2) | C18—C19—C20—C15 | 0.2 (2) |
| C1—N7—C8—C13 | −135.63 (16) | N16—C15—C20—C19 | −0.3 (2) |
| C13—C8—C9—C10 | 0.1 (2) | N14—C15—C20—C19 | −178.51 (14) |
| N7—C8—C9—C10 | 177.18 (14) | N25i—C21—C22—N23 | −0.1 (3) |
| C8—C9—C10—C11 | −0.6 (2) | C25i—C21—C22—N23 | −0.1 (3) |
| C9—C10—C11—C12 | 0.8 (2) | C21—C22—N23—C24 | 0.0 (3) |
| C9—C10—C11—N14 | 178.09 (14) | C22—N23—C24—C25 | −179.52 (15) |
| C15—N14—C11—C12 | −48.1 (2) | C22—N23—C24—C24i | −0.4 (3) |
| C15—N14—C11—C10 | 134.72 (16) | N23—C24—C25—C21i | −179.92 (15) |
| C10—C11—C12—C13 | −0.6 (2) | C24i—C24—C25—C21i | 1.0 (3) |
| N14—C11—C12—C13 | −177.76 (14) |
Symmetry codes: (i) −x+1, −y+1, −z+1.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N14—H14N···N2ii | 0.90 | 2.12 | 2.9998 (17) | 166 |
| N7—H7N···N16iii | 0.90 | 2.13 | 3.0173 (18) | 167 |
Symmetry codes: (ii) x, y−1, z; (iii) x, y+1, z.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ2662).
References
- Bensemann, I., Gdaniec, M. & Połoński, T. (2002). New J. Chem. 26, 448–456.
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- Gdaniec, M., Bensemann, I. & Połoński, T. (2005). CrystEngComm, 7, 433–438.
- Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst. 39, 453–457.
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Supplementary Materials
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536811046356/rz2662sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811046356/rz2662Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



