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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2014 Nov 8;70(Pt 12):o1244–o1245. doi: 10.1107/S1600536814024167

Crystal structure of 2-[12-methyl-14-phenyl-10,13,14,16-tetra­aza­tetra­cyclo[7.7.0.02,7.011,15]hexa­deca-1(16),2,4,6,9,11(15),12-heptaen-8-yl­idene]propandi­nitrile

Joel T Mague a, Shaaban K Mohamed b,c, Mehmet Akkurt d, Hussein M S El-Kashef e, Mustafa R Albayati f,*
PMCID: PMC4257392  PMID: 25553023

Abstract

In the title mol­ecule, C22H12N6, the fused tetracyclic core shows a small lengthwise twist as indicated by the dihedral of 2.7 (2)° between the outer rings. In the crystal, mol­ecules stack along the b-axis direction via offset π-stacking [centroid–centroid distances = 3.5282 (13) and 3.5597 (14) Å] with the stacks weakly associated through C—H⋯N hydrogen bonds. The phenyl ring is rotationally disordered over two orientations with an occupancy ratio of 0.516 (4):0.484 (4).

Keywords: crystal structure, hepta­ene, propandi­nitrile, pyrazine scaffold compound, fused tetracyclic core

Related literature  

For the biological properties of pyrazine scaffold compounds, see: Kaliszan et al. (1985); Makino et al. (1990); Emary & Ibrahim (2006); Silva et al. (2010); Rusinov et al. (2005); Johnston & Kau (1993); Myadaraboina et al. (2010); Metobo et al. (2006). For use of pyrazines in industrial chemistry see: Rangnekar & Dhamnaskar, 1990). For the preparation of the title compound, see: El-Emary & El-Kashef (2013)graphic file with name e-70-o1244-scheme1.jpg

Experimental  

Crystal data  

  • C22H12N6

  • M r = 360.38

  • Monoclinic, Inline graphic

  • a = 35.968 (5) Å

  • b = 4.6483 (6) Å

  • c = 26.596 (3) Å

  • β = 129.6130 (12)°

  • V = 3425.5 (8) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.09 mm−1

  • T = 150 K

  • 0.21 × 0.13 × 0.07 mm

Data collection  

  • Bruker SMART APEX CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2014) T min = 0.77, T max = 0.99

  • 15751 measured reflections

  • 3921 independent reflections

  • 2489 reflections with I > 2σ(I)

  • R int = 0.050

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.053

  • wR(F 2) = 0.136

  • S = 1.03

  • 3921 reflections

  • 249 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.31 e Å−3

  • Δρmin = −0.20 e Å−3

Data collection: APEX2 (Bruker, 2014); cell refinement: SAINT (Bruker, 2014); data reduction: SAINT; program(s) used to solve structure: SHELXT (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg & Putz, 2012); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536814024167/su5012sup1.cif

e-70-o1244-sup1.cif (509.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814024167/su5012Isup2.hkl

e-70-o1244-Isup2.hkl (215.2KB, hkl)

Supporting information file. DOI: 10.1107/S1600536814024167/su5012Isup3.cml

. DOI: 10.1107/S1600536814024167/su5012fig1.tif

The mol­ecular structure of the title mol­ecule, showing the atom labelling. Displacement ellipsoids are drawn at the 50% probability level.

. DOI: 10.1107/S1600536814024167/su5012fig2.tif

Portions of two neighboring stacks showing the offset π-stacking and C—H⋯N inter­actions (Table 1) as green and blue dotted line, respectively.

b . DOI: 10.1107/S1600536814024167/su5012fig3.tif

Crystal packing viewed along the b axis showing stacks of mol­ecules connected by the weak C—H⋯N inter­actions (blue dotted lines; see Table 1 for details).

CCDC reference: 1032263

Additional supporting information: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (, ).

DHA DH HA D A DHA
C10H10AN5i 0.98 2.69 3.362(3) 126

Symmetry code: (i) Inline graphic.

Acknowledgments

JTM thanks Tulane University for support of the Tulane Crystallography Laboratory. SKM and HMSE would like to thank Professor T. El-Emary, Assiut University, for his contribution to this study.

supplementary crystallographic information

S1. Comment

Over recent years there has been an increasing interest in the chemistry of pyrazine scaffold compounds due to their biological significance. Pyrazine ring is found in numerous pharmaceutically active compounds such as analgesic (Kaliszan et al., 1985), antiallergic (Makino et al., 1990), antibacterial (Emary & Ibrahim 2006), anti-inflammatory (Silva et al., 2010), antiviral (Rusinov et al., 2005), diuretic (Johnston & Kau, 1993), anticancer (Myadaraboina et al., 2010), and anti-HIV (Metobo et al., 2006) medications. Other pyrazine derivatives are also used as fluorescent dyes or dispersed dyes for polyester fibers (Rangnekar & Dhamnaskar, 1990). As part of our investigations of pyrazine derivatives to compare their chemical and biological activities, we have undertaken the X-ray crystal structure analysis of the title compound.

In the title compound, Fig. 1, the fused 4-ring core of the title molecule is nearly planar with only a slight lengthwise twist as indicated by the dihedral angle between the N1/N2/C7/C8/C9 and C12–C17 rings of 2.7 (2)°.

In the crystal, molecules pack in columns along [010] which involve offset π-stacking in which atom N2 is 3.36 (4) Å from the centroid of the N3/C11/C19/N4/C8/C7 ring one unit cell translation in b above it while C17 is 3.41 (4) Å from the centroid of the N3/C11/C19/N4/C8/C7 ring one unit cell translation in b below it (Fig. 2). Adjacent stacks are weakly associated via C—H···N hydrogen bonds (Fig. 3 and Table 1) and are inclined at ca 43.5° in opposite directions from (010).

S2. Experimental

The title compound was prepared according to the reported procedure (El-Emary & El-Kashef, 2013). Orange crystals suitable for X-ray diffraction were obtained by recrystallization of the reaction product from dimethylformamide (m.p. 587–589 K).

S3. Refinement

C-bound H atoms were placed in calculated positions and treated as riding atoms, with C—H = 0.95–0.98 Å and with Uiso(H) = 1.5Ueq(C) for methyl H atoms and = 1.2Ueq(C) for other H atoms. The phenyl ring attached to N1 is rotationally disordered over two sites with an occupancy ratio of 0.516 (4):0.484 (4). The components of the disorder were refined as rigid hexagons.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title molecule, showing the atom labelling. Displacement ellipsoids are drawn at the 50% probability level.

Fig. 2.

Fig. 2.

Portions of two neighboring stacks showing the offset π-stacking and C—H···N interactions (Table 1) as green and blue dotted line, respectively.

Fig. 3.

Fig. 3.

Crystal packing viewed along the b axis showing stacks of molecules connected by the weak C—H···N interactions (blue dotted lines; see Table 1 for details).

Crystal data

C22H12N6 F(000) = 1488
Mr = 360.38 Dx = 1.398 Mg m3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
a = 35.968 (5) Å Cell parameters from 4540 reflections
b = 4.6483 (6) Å θ = 2.3–27.4°
c = 26.596 (3) Å µ = 0.09 mm1
β = 129.6130 (12)° T = 150 K
V = 3425.5 (8) Å3 Column, orange
Z = 8 0.21 × 0.13 × 0.07 mm

Data collection

Bruker SMART APEX CCD diffractometer 3921 independent reflections
Radiation source: fine-focus sealed tube 2489 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.050
Detector resolution: 8.3660 pixels mm-1 θmax = 27.5°, θmin = 2.0°
φ and ω scans h = −46→46
Absorption correction: multi-scan (SADABS; Bruker, 2014) k = −6→6
Tmin = 0.77, Tmax = 0.99 l = −34→34
15751 measured reflections

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)] = 0.053 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.136 H-atom parameters constrained
S = 1.03 w = 1/[σ2(Fo2) + (0.0537P)2 + 1.9123P] where P = (Fo2 + 2Fc2)/3
3921 reflections (Δ/σ)max = 0.001
249 parameters Δρmax = 0.31 e Å3
1 restraint Δρmin = −0.20 e Å3

Special details

Experimental. The diffraction data were collected in three sets of 400 frames (0.5° width in ω) at φ = 0, 120 and 240°. A scan time of 90 sec/frame was used.
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. H-atoms attached to carbon were placed in calculated positions (C—H = 0.95 - 0.98 Å). All were included as riding contributions with isotropic displacement parameters 1.2 - 1.5 times those of the attached atoms. The phenyl ring attached to N1 is rotationally disordered over two sites in approximately equal amounts. The components of the disorder were refined as rigid hexagons.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
N1 0.69392 (6) 0.2255 (4) 0.36211 (8) 0.0427 (4)
N2 0.66369 (7) 0.0716 (4) 0.36798 (9) 0.0482 (5)
N3 0.68329 (6) 0.5915 (3) 0.28798 (8) 0.0385 (4)
N4 0.58234 (6) 0.5174 (4) 0.23053 (8) 0.0418 (4)
N5 0.46527 (7) 0.6261 (5) 0.12918 (10) 0.0679 (6)
N6 0.46809 (7) 1.2638 (5) 0.01592 (10) 0.0657 (6)
C1 0.74396 (18) 0.1886 (11) 0.4101 (2) 0.0444 (5) 0.516 (4)
C2 0.7750 (3) 0.2928 (12) 0.4002 (2) 0.0565 (14) 0.516 (4)
H2 0.7624 0.3876 0.3605 0.068* 0.516 (4)
C3 0.8246 (2) 0.2582 (13) 0.4482 (3) 0.0568 (13) 0.516 (4)
H3 0.8458 0.3294 0.4414 0.068* 0.516 (4)
C4 0.84309 (16) 0.1195 (12) 0.5063 (3) 0.0611 (7) 0.516 (4)
H4 0.8770 0.0959 0.5391 0.073* 0.516 (4)
C5 0.81201 (19) 0.0153 (11) 0.5163 (2) 0.0596 (12) 0.516 (4)
H5 0.8246 −0.0795 0.5559 0.072* 0.516 (4)
C6 0.76244 (18) 0.0498 (11) 0.4682 (2) 0.0551 (11) 0.516 (4)
H6 0.7412 −0.0214 0.4750 0.066* 0.516 (4)
C1A 0.74487 (19) 0.1788 (12) 0.4091 (2) 0.0444 (5) 0.484 (4)
C2A 0.7774 (3) 0.3742 (10) 0.4168 (3) 0.0565 (14) 0.484 (4)
H2A 0.7660 0.5350 0.3884 0.068* 0.484 (4)
C3A 0.8267 (3) 0.3344 (11) 0.4661 (4) 0.0568 (13) 0.484 (4)
H3A 0.8490 0.4679 0.4714 0.068* 0.484 (4)
C4A 0.84344 (17) 0.0991 (13) 0.5077 (3) 0.0611 (7) 0.484 (4)
H4A 0.8771 0.0719 0.5414 0.073* 0.484 (4)
C5A 0.8109 (2) −0.0963 (11) 0.5000 (2) 0.0596 (12) 0.484 (4)
H5A 0.8223 −0.2571 0.5284 0.072* 0.484 (4)
C6A 0.76159 (19) −0.0564 (11) 0.4507 (3) 0.0551 (11) 0.484 (4)
H6A 0.7393 −0.1900 0.4454 0.066* 0.484 (4)
C7 0.66759 (7) 0.4096 (4) 0.31061 (9) 0.0385 (5)
C8 0.61906 (7) 0.3724 (4) 0.28314 (10) 0.0395 (5)
C9 0.61930 (8) 0.1579 (4) 0.32169 (11) 0.0458 (5)
C10 0.57752 (8) 0.0445 (5) 0.31473 (12) 0.0575 (6)
H10A 0.5884 −0.1118 0.3461 0.086*
H10B 0.5530 −0.0286 0.2703 0.086*
H10C 0.5636 0.1991 0.3232 0.086*
C11 0.64643 (7) 0.7328 (4) 0.23600 (9) 0.0360 (4)
C12 0.64814 (7) 0.9456 (4) 0.19683 (9) 0.0368 (4)
C13 0.68659 (7) 1.0487 (4) 0.20208 (10) 0.0424 (5)
H13 0.7185 0.9834 0.2359 0.051*
C14 0.67732 (8) 1.2503 (5) 0.15671 (10) 0.0470 (5)
H14 0.7032 1.3228 0.1594 0.056*
C15 0.63093 (8) 1.3466 (5) 0.10772 (10) 0.0480 (5)
H15 0.6255 1.4850 0.0774 0.058*
C16 0.59220 (7) 1.2445 (4) 0.10213 (10) 0.0440 (5)
H16 0.5604 1.3125 0.0684 0.053*
C17 0.60064 (7) 1.0419 (4) 0.14650 (9) 0.0387 (5)
C18 0.56731 (7) 0.8908 (4) 0.15189 (9) 0.0389 (5)
C19 0.59741 (7) 0.6983 (4) 0.20825 (9) 0.0379 (4)
C20 0.51870 (7) 0.9165 (4) 0.11397 (10) 0.0421 (5)
C21 0.49030 (8) 0.7526 (5) 0.12444 (11) 0.0499 (5)
C22 0.49111 (8) 1.1104 (5) 0.05965 (11) 0.0491 (5)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0487 (10) 0.0408 (9) 0.0452 (10) 0.0038 (8) 0.0331 (9) 0.0037 (8)
N2 0.0606 (12) 0.0437 (10) 0.0563 (11) 0.0011 (9) 0.0447 (11) 0.0022 (9)
N3 0.0421 (9) 0.0351 (9) 0.0406 (9) 0.0017 (7) 0.0274 (8) −0.0007 (7)
N4 0.0452 (10) 0.0383 (9) 0.0471 (10) −0.0017 (8) 0.0318 (9) −0.0063 (8)
N5 0.0494 (12) 0.0848 (16) 0.0745 (15) −0.0056 (11) 0.0418 (12) −0.0071 (12)
N6 0.0538 (12) 0.0703 (14) 0.0579 (13) 0.0127 (11) 0.0287 (11) 0.0066 (12)
C1 0.0527 (13) 0.0398 (12) 0.0459 (12) 0.0081 (10) 0.0339 (11) 0.0016 (9)
C2 0.0545 (17) 0.058 (3) 0.060 (3) 0.018 (2) 0.037 (2) 0.020 (3)
C3 0.0543 (17) 0.058 (3) 0.063 (4) 0.015 (2) 0.040 (2) 0.006 (2)
C4 0.0583 (15) 0.0649 (17) 0.0510 (14) 0.0200 (13) 0.0306 (13) 0.0071 (13)
C5 0.073 (2) 0.056 (3) 0.047 (3) 0.017 (3) 0.038 (2) 0.008 (2)
C6 0.0618 (18) 0.054 (3) 0.050 (3) 0.006 (2) 0.036 (2) 0.006 (2)
C1A 0.0527 (13) 0.0398 (12) 0.0459 (12) 0.0081 (10) 0.0339 (11) 0.0016 (9)
C2A 0.0545 (17) 0.058 (3) 0.060 (3) 0.018 (2) 0.037 (2) 0.020 (3)
C3A 0.0543 (17) 0.058 (3) 0.063 (4) 0.015 (2) 0.040 (2) 0.006 (2)
C4A 0.0583 (15) 0.0649 (17) 0.0510 (14) 0.0200 (13) 0.0306 (13) 0.0071 (13)
C5A 0.073 (2) 0.056 (3) 0.047 (3) 0.017 (3) 0.038 (2) 0.008 (2)
C6A 0.0618 (18) 0.054 (3) 0.050 (3) 0.006 (2) 0.036 (2) 0.006 (2)
C7 0.0458 (11) 0.0339 (10) 0.0412 (11) 0.0034 (9) 0.0302 (10) −0.0016 (9)
C8 0.0460 (12) 0.0344 (10) 0.0469 (12) 0.0009 (9) 0.0337 (10) −0.0038 (9)
C9 0.0551 (13) 0.0421 (11) 0.0521 (13) −0.0012 (10) 0.0398 (12) −0.0045 (10)
C10 0.0674 (15) 0.0569 (14) 0.0712 (16) −0.0045 (12) 0.0548 (14) −0.0006 (12)
C11 0.0381 (11) 0.0328 (10) 0.0377 (10) 0.0001 (8) 0.0245 (9) −0.0044 (8)
C12 0.0396 (11) 0.0326 (10) 0.0381 (10) −0.0005 (8) 0.0247 (9) −0.0043 (8)
C13 0.0393 (11) 0.0429 (11) 0.0410 (11) −0.0017 (9) 0.0238 (10) −0.0040 (9)
C14 0.0468 (12) 0.0497 (12) 0.0511 (13) −0.0024 (10) 0.0342 (11) −0.0006 (10)
C15 0.0541 (13) 0.0479 (12) 0.0446 (12) 0.0024 (10) 0.0327 (11) 0.0035 (10)
C16 0.0442 (12) 0.0431 (11) 0.0404 (11) 0.0038 (10) 0.0249 (10) −0.0008 (9)
C17 0.0392 (11) 0.0352 (10) 0.0407 (11) 0.0004 (8) 0.0250 (9) −0.0051 (9)
C18 0.0410 (11) 0.0352 (10) 0.0409 (11) −0.0011 (8) 0.0262 (10) −0.0088 (9)
C19 0.0394 (11) 0.0345 (10) 0.0409 (11) 0.0003 (8) 0.0261 (10) −0.0042 (8)
C20 0.0391 (11) 0.0420 (11) 0.0411 (11) 0.0023 (9) 0.0238 (10) −0.0052 (9)
C21 0.0392 (12) 0.0558 (13) 0.0516 (13) −0.0009 (11) 0.0274 (11) −0.0101 (11)
C22 0.0412 (12) 0.0528 (13) 0.0481 (13) 0.0026 (11) 0.0261 (11) −0.0072 (11)

Geometric parameters (Å, º)

N1—C7 1.361 (2) C4A—C5A 1.3900
N1—N2 1.391 (2) C4A—H4A 0.9500
N1—C1 1.403 (5) C5A—C6A 1.3900
N1—C1A 1.430 (5) C5A—H5A 0.9500
N2—C9 1.311 (3) C6A—H6A 0.9500
N3—C11 1.328 (2) C7—C8 1.409 (3)
N3—C7 1.353 (2) C8—C9 1.426 (3)
N4—C19 1.327 (2) C9—C10 1.489 (3)
N4—C8 1.342 (3) C10—H10A 0.9800
N5—C21 1.147 (3) C10—H10B 0.9800
N6—C22 1.148 (3) C10—H10C 0.9800
C1—C2 1.3900 C11—C19 1.421 (3)
C1—C6 1.3900 C11—C12 1.466 (3)
C2—C3 1.3900 C12—C13 1.384 (3)
C2—H2 0.9500 C12—C17 1.413 (3)
C3—C4 1.3900 C13—C14 1.390 (3)
C3—H3 0.9500 C13—H13 0.9500
C4—C5 1.3900 C14—C15 1.382 (3)
C4—H4 0.9500 C14—H14 0.9500
C5—C6 1.3900 C15—C16 1.387 (3)
C5—H5 0.9500 C15—H15 0.9500
C6—H6 0.9500 C16—C17 1.384 (3)
C1A—C2A 1.3900 C16—H16 0.9500
C1A—C6A 1.3900 C17—C18 1.474 (3)
C2A—C3A 1.3900 C18—C20 1.356 (3)
C2A—H2A 0.9500 C18—C19 1.466 (3)
C3A—C4A 1.3900 C20—C22 1.434 (3)
C3A—H3A 0.9500 C20—C21 1.437 (3)
C7—N1—N2 110.14 (16) N1—C7—C8 106.37 (17)
C7—N1—C1 131.2 (3) N4—C8—C7 123.33 (18)
N2—N1—C1 118.4 (3) N4—C8—C9 130.67 (19)
C7—N1—C1A 131.0 (3) C7—C8—C9 105.99 (18)
N2—N1—C1A 118.8 (3) N2—C9—C8 109.54 (18)
C9—N2—N1 107.95 (16) N2—C9—C10 122.5 (2)
C11—N3—C7 110.46 (16) C8—C9—C10 128.0 (2)
C19—N4—C8 111.93 (16) C9—C10—H10A 109.5
C2—C1—C6 120.0 C9—C10—H10B 109.5
C2—C1—N1 120.3 (4) H10A—C10—H10B 109.5
C6—C1—N1 119.7 (4) C9—C10—H10C 109.5
C3—C2—C1 120.0 H10A—C10—H10C 109.5
C3—C2—H2 120.0 H10B—C10—H10C 109.5
C1—C2—H2 120.0 N3—C11—C19 124.72 (17)
C2—C3—C4 120.0 N3—C11—C12 127.38 (17)
C2—C3—H3 120.0 C19—C11—C12 107.90 (16)
C4—C3—H3 120.0 C13—C12—C17 120.84 (18)
C5—C4—C3 120.0 C13—C12—C11 130.85 (18)
C5—C4—H4 120.0 C17—C12—C11 108.30 (16)
C3—C4—H4 120.0 C12—C13—C14 118.35 (19)
C6—C5—C4 120.0 C12—C13—H13 120.8
C6—C5—H5 120.0 C14—C13—H13 120.8
C4—C5—H5 120.0 C15—C14—C13 120.9 (2)
C5—C6—C1 120.0 C15—C14—H14 119.5
C5—C6—H6 120.0 C13—C14—H14 119.5
C1—C6—H6 120.0 C14—C15—C16 121.1 (2)
C2A—C1A—C6A 120.0 C14—C15—H15 119.4
C2A—C1A—N1 121.3 (4) C16—C15—H15 119.4
C6A—C1A—N1 118.5 (4) C17—C16—C15 118.82 (19)
C1A—C2A—C3A 120.0 C17—C16—H16 120.6
C1A—C2A—H2A 120.0 C15—C16—H16 120.6
C3A—C2A—H2A 120.0 C16—C17—C12 119.95 (18)
C4A—C3A—C2A 120.0 C16—C17—C18 131.13 (18)
C4A—C3A—H3A 120.0 C12—C17—C18 108.91 (17)
C2A—C3A—H3A 120.0 C20—C18—C19 125.14 (18)
C5A—C4A—C3A 120.0 C20—C18—C17 128.95 (19)
C5A—C4A—H4A 120.0 C19—C18—C17 105.91 (16)
C3A—C4A—H4A 120.0 N4—C19—C11 124.33 (18)
C4A—C5A—C6A 120.0 N4—C19—C18 126.69 (17)
C4A—C5A—H5A 120.0 C11—C19—C18 108.98 (17)
C6A—C5A—H5A 120.0 C18—C20—C22 122.7 (2)
C5A—C6A—C1A 120.0 C18—C20—C21 123.22 (19)
C5A—C6A—H6A 120.0 C22—C20—C21 114.06 (18)
C1A—C6A—H6A 120.0 N5—C21—C20 176.0 (2)
N3—C7—N1 128.40 (18) N6—C22—C20 178.4 (2)
N3—C7—C8 125.22 (18)
C7—N1—N2—C9 −0.6 (2) N3—C7—C8—C9 178.93 (17)
C1—N1—N2—C9 174.4 (2) N1—C7—C8—C9 0.0 (2)
C1A—N1—N2—C9 177.4 (3) N1—N2—C9—C8 0.6 (2)
C7—N1—C1—C2 −18.7 (4) N1—N2—C9—C10 −177.98 (18)
N2—N1—C1—C2 167.6 (2) N4—C8—C9—N2 178.80 (19)
C1A—N1—C1—C2 69 (11) C7—C8—C9—N2 −0.3 (2)
C7—N1—C1—C6 160.6 (3) N4—C8—C9—C10 −2.8 (4)
N2—N1—C1—C6 −13.1 (4) C7—C8—C9—C10 178.1 (2)
C1A—N1—C1—C6 −112 (11) C7—N3—C11—C19 0.2 (3)
C6—C1—C2—C3 0.0 C7—N3—C11—C12 −179.09 (17)
N1—C1—C2—C3 179.3 (4) N3—C11—C12—C13 1.4 (3)
C1—C2—C3—C4 0.0 C19—C11—C12—C13 −177.97 (19)
C2—C3—C4—C5 0.0 N3—C11—C12—C17 −179.69 (18)
C3—C4—C5—C6 0.0 C19—C11—C12—C17 0.9 (2)
C4—C5—C6—C1 0.0 C17—C12—C13—C14 0.2 (3)
C2—C1—C6—C5 0.0 C11—C12—C13—C14 178.95 (19)
N1—C1—C6—C5 −179.3 (4) C12—C13—C14—C15 0.3 (3)
C7—N1—C1A—C2A 14.8 (4) C13—C14—C15—C16 −0.3 (3)
N2—N1—C1A—C2A −162.6 (3) C14—C15—C16—C17 −0.3 (3)
C1—N1—C1A—C2A −80 (11) C15—C16—C17—C12 0.8 (3)
C7—N1—C1A—C6A −169.9 (3) C15—C16—C17—C18 −178.22 (19)
N2—N1—C1A—C6A 12.7 (4) C13—C12—C17—C16 −0.8 (3)
C1—N1—C1A—C6A 95 (11) C11—C12—C17—C16 −179.76 (17)
C6A—C1A—C2A—C3A 0.0 C13—C12—C17—C18 178.45 (17)
N1—C1A—C2A—C3A 175.2 (4) C11—C12—C17—C18 −0.6 (2)
C1A—C2A—C3A—C4A 0.0 C16—C17—C18—C20 −0.9 (3)
C2A—C3A—C4A—C5A 0.0 C12—C17—C18—C20 179.99 (19)
C3A—C4A—C5A—C6A 0.0 C16—C17—C18—C19 179.1 (2)
C4A—C5A—C6A—C1A 0.0 C12—C17—C18—C19 0.0 (2)
C2A—C1A—C6A—C5A 0.0 C8—N4—C19—C11 0.8 (3)
N1—C1A—C6A—C5A −175.3 (4) C8—N4—C19—C18 −179.82 (17)
C11—N3—C7—N1 179.02 (18) N3—C11—C19—N4 −0.8 (3)
C11—N3—C7—C8 0.3 (3) C12—C11—C19—N4 178.58 (17)
N2—N1—C7—N3 −178.56 (18) N3—C11—C19—C18 179.68 (17)
C1—N1—C7—N3 7.3 (4) C12—C11—C19—C18 −0.9 (2)
C1A—N1—C7—N3 3.8 (4) C20—C18—C19—N4 1.1 (3)
N2—N1—C7—C8 0.4 (2) C17—C18—C19—N4 −178.91 (18)
C1—N1—C7—C8 −173.8 (3) C20—C18—C19—C11 −179.43 (18)
C1A—N1—C7—C8 −177.2 (3) C17—C18—C19—C11 0.6 (2)
C19—N4—C8—C7 −0.3 (3) C19—C18—C20—C22 179.49 (18)
C19—N4—C8—C9 −179.28 (19) C17—C18—C20—C22 −0.5 (3)
N3—C7—C8—N4 −0.3 (3) C19—C18—C20—C21 −0.6 (3)
N1—C7—C8—N4 −179.24 (17) C17—C18—C20—C21 179.43 (18)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C10—H10A···N5i 0.98 2.69 3.362 (3) 126

Symmetry code: (i) −x+1, y−1, −z+1/2.

Footnotes

Supporting information for this paper is available from the IUCr electronic archives (Reference: SU5012).

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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/S1600536814024167/su5012sup1.cif

e-70-o1244-sup1.cif (509.6KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536814024167/su5012Isup2.hkl

e-70-o1244-Isup2.hkl (215.2KB, hkl)

Supporting information file. DOI: 10.1107/S1600536814024167/su5012Isup3.cml

. DOI: 10.1107/S1600536814024167/su5012fig1.tif

The mol­ecular structure of the title mol­ecule, showing the atom labelling. Displacement ellipsoids are drawn at the 50% probability level.

. DOI: 10.1107/S1600536814024167/su5012fig2.tif

Portions of two neighboring stacks showing the offset π-stacking and C—H⋯N inter­actions (Table 1) as green and blue dotted line, respectively.

b . DOI: 10.1107/S1600536814024167/su5012fig3.tif

Crystal packing viewed along the b axis showing stacks of mol­ecules connected by the weak C—H⋯N inter­actions (blue dotted lines; see Table 1 for details).

CCDC reference: 1032263

Additional supporting information: crystallographic information; 3D view; checkCIF report


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