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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 May 20;65(Pt 6):o1308. doi: 10.1107/S1600536809017498

2-Phenyl-1H-1,3,7,8-tetra­azacyclo­penta­[l]phenanthrene

Dong-Ming Liu a, Xiu-Ying Li b, Xiang-Cheng Wang b, Chun-Xiang Li b, Chun-Bo Liu b,*
PMCID: PMC2969696  PMID: 21583165

Abstract

There are two mol­ecules in the asymmetric unit of the title compound, C19H12N4, with dihedral angles of 2.41 (10) and 10.53 (12)° between the fused ring system and the pendant phenyl ring. In the crystal, mol­ecules are linked into chains by N—H⋯N hydrogen bonds and aromatic π–π stacking inter­actions [shortest centroid–centroid distance = 3.6176 (16) Å] complete the structure.

Related literature

For the synthesis, see: Steck & Day (1943); For related structures, see: Che et al. (2008); Stephenson & Hardie (2006); Xi (2008).graphic file with name e-65-o1308-scheme1.jpg

Experimental

Crystal data

  • C19H12N4

  • M r = 296.33

  • Triclinic, Inline graphic

  • a = 10.016 (2) Å

  • b = 12.210 (2) Å

  • c = 12.415 (3) Å

  • α = 89.90 (3)°

  • β = 78.44 (3)°

  • γ = 77.96 (3)°

  • V = 1453.7 (5) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 292 K

  • 0.30 × 0.25 × 0.20 mm

Data collection

  • Rigaku R-AXIS RAPID diffractometer

  • Absorption correction: multi-scan (ABSCOR; Higashi, 1995) T min = 0.975, T max = 0.984

  • 14453 measured reflections

  • 6587 independent reflections

  • 3657 reflections with I > 2σ(I)

  • R int = 0.048

Refinement

  • R[F 2 > 2σ(F 2)] = 0.059

  • wR(F 2) = 0.156

  • S = 1.01

  • 6587 reflections

  • 415 parameters

  • H-atom parameters constrained

  • Δρmax = 0.41 e Å−3

  • Δρmin = −0.20 e Å−3

Data collection: PROCESS-AUTO (Rigaku, 1998); cell refinement: PROCESS-AUTO; data reduction: PROCESS-AUTO; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809017498/hb2971sup1.cif

e-65-o1308-sup1.cif (23.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809017498/hb2971Isup2.hkl

e-65-o1308-Isup2.hkl (315.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N3—H3⋯N5i 0.86 2.10 2.932 (3) 164
N7—H7⋯N1 0.86 2.12 2.951 (2) 163

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors thank the Postdoctoral Foundation of Jiangsu Province (No. 0801010B) for support.

supplementary crystallographic information

Comment

1,10-Phenanthroline (phen) or its derivatives, as an important chelating ligands with excellent coordinating abilities and fruitful aromatic systems, have been extensively used to build supramolecular architectures (Che, Liu et al., 2008; Stephenson, Hardie et al., 2006). We report here the synthesis and structure of the title compound, namely, C19H12N4 (I), using the phen derivative 2-Phenyl-1H-1,3,7,8-tetraazacyclopenta- [l]phenanthrene (L).

The asymmetric unit of (I) consists of two independent L molecules (Fig.1). The two phenyl rings are slightly twisted with respect to the fused-ring system [dihedral angles = 1.34 and 1.54 °], which is different from a related compound that has been reported (Xi, 2008). In the crystal structure, N—H···N hydrogen bonds (Table 1) link the molecules into chains along the b axis. The neighbouring chains interact through π-π contact between two L ligands [centroid separation = 3.541 Å], leading to the ultimate supramolecular structure (Fig. 2).

Experimental

The L ligand was synthesized according to the literature method of Steck & Day (1943): a mixture of L, MnCl2 and water in a molar ratio of 2:1:5000 was sealed in a Teflon-lined autoclave and heated to 413 K for 3 d. Upon cooling and opening the bomb, accidentally, pale yellow blocks of (I) were obtained.

Refinement

The H atoms were positioned geometrically (C—H = 0.93 Å, N—H = 0.86Å) and refined as riding, with Uiso(H) = 1.2Ueq(carrier).

Figures

Fig. 1.

Fig. 1.

The structure of (I). Displacement ellipsoids are drawn at the 30% probability level (arbitrary spheres for the H atoms).

Fig. 2.

Fig. 2.

A view of the crystal packing, showing the N—H···N hydrogen bonds and π-π stacking interactions. H atoms have been omitted.

Crystal data

C19H12N4 Z = 4
Mr = 296.33 F(000) = 616
Triclinic, P1 Dx = 1.354 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 10.016 (2) Å Cell parameters from 3449 reflections
b = 12.210 (2) Å θ = 3.0–27.5°
c = 12.415 (3) Å µ = 0.08 mm1
α = 89.90 (3)° T = 292 K
β = 78.44 (3)° Block, pale yellow
γ = 77.96 (3)° 0.30 × 0.25 × 0.20 mm
V = 1453.7 (5) Å3

Data collection

Rigaku R-AXIS RAPID diffractometer 6587 independent reflections
Radiation source: fine-focus sealed tube 3657 reflections with I > 2σ(I)
graphite Rint = 0.048
Detector resolution: 10.0 pixels mm-1 θmax = 27.5°, θmin = 3.0°
ω scans h = −12→12
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) k = −15→15
Tmin = 0.975, Tmax = 0.984 l = −16→16
14453 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)] = 0.059 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.156 H-atom parameters constrained
S = 1.01 w = 1/[σ2(Fo2) + (0.0719P)2 + 0.0624P] where P = (Fo2 + 2Fc2)/3
6587 reflections (Δ/σ)max < 0.001
415 parameters Δρmax = 0.41 e Å3
0 restraints Δρmin = −0.20 e Å3

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
C1 −0.0622 (2) 0.23344 (19) 0.81330 (18) 0.0490 (6)
H1 −0.1221 0.2801 0.8697 0.059*
C2 −0.0895 (2) 0.12895 (19) 0.79496 (18) 0.0484 (6)
H2 −0.1658 0.1068 0.8380 0.058*
C3 −0.0027 (2) 0.05936 (18) 0.71295 (17) 0.0450 (5)
H3A −0.0182 −0.0115 0.7001 0.054*
C4 0.1104 (2) 0.09578 (17) 0.64798 (15) 0.0372 (5)
C5 0.2049 (2) 0.03323 (16) 0.55681 (16) 0.0389 (5)
C6 0.3066 (2) 0.07524 (17) 0.48872 (16) 0.0399 (5)
C7 0.3291 (2) 0.18394 (18) 0.51052 (16) 0.0411 (5)
C8 0.4316 (2) 0.2316 (2) 0.44514 (19) 0.0511 (6)
H8 0.4916 0.1918 0.3843 0.061*
C9 0.4418 (3) 0.3372 (2) 0.4723 (2) 0.0620 (7)
H9 0.5088 0.3707 0.4300 0.074*
C10 0.3510 (3) 0.3944 (2) 0.5639 (2) 0.0602 (7)
H10 0.3590 0.4665 0.5808 0.072*
C11 0.2416 (2) 0.24813 (17) 0.60234 (16) 0.0396 (5)
C12 0.1303 (2) 0.20394 (17) 0.67106 (15) 0.0376 (5)
C13 0.3167 (2) −0.08769 (19) 0.42188 (16) 0.0441 (5)
C14 0.3576 (2) −0.1902 (2) 0.35036 (18) 0.0471 (6)
C15 0.3037 (3) −0.2845 (2) 0.3759 (2) 0.0621 (7)
H15 0.2408 −0.2852 0.4419 0.075*
C16 0.3416 (3) −0.3775 (2) 0.3051 (2) 0.0745 (8)
H16 0.3036 −0.4401 0.3231 0.089*
C17 0.4350 (3) −0.3777 (3) 0.2086 (3) 0.0802 (10)
H17 0.4613 −0.4406 0.1609 0.096*
C18 0.4895 (3) −0.2857 (3) 0.1823 (2) 0.0781 (9)
H18 0.5529 −0.2861 0.1163 0.094*
C19 0.4521 (3) −0.1917 (2) 0.2523 (2) 0.0631 (7)
H19 0.4904 −0.1295 0.2335 0.076*
C20 −0.0061 (2) 0.71983 (19) 0.57979 (18) 0.0495 (6)
H20 −0.0384 0.7605 0.5233 0.059*
C21 −0.0429 (2) 0.61739 (19) 0.60084 (18) 0.0485 (6)
H21 −0.0989 0.5910 0.5600 0.058*
C22 0.0046 (2) 0.55589 (18) 0.68273 (17) 0.0455 (5)
H22 −0.0169 0.4862 0.6976 0.055*
C23 0.0864 (2) 0.59938 (17) 0.74404 (16) 0.0382 (5)
C24 0.1393 (2) 0.54495 (17) 0.83266 (16) 0.0379 (5)
C25 0.2102 (2) 0.59356 (18) 0.89767 (16) 0.0406 (5)
C26 0.2425 (2) 0.70078 (18) 0.87370 (16) 0.0405 (5)
C27 0.3175 (2) 0.7535 (2) 0.93361 (18) 0.0510 (6)
H27 0.3498 0.7192 0.9931 0.061*
C28 0.3424 (3) 0.8564 (2) 0.9033 (2) 0.0599 (7)
H28 0.3910 0.8936 0.9423 0.072*
C29 0.2938 (3) 0.9040 (2) 0.8131 (2) 0.0611 (7)
H29 0.3119 0.9737 0.7931 0.073*
C30 0.1977 (2) 0.75555 (17) 0.78341 (16) 0.0404 (5)
C31 0.1167 (2) 0.70490 (17) 0.71880 (16) 0.0384 (5)
C32 0.1928 (2) 0.43446 (18) 0.96433 (16) 0.0415 (5)
C33 0.2076 (2) 0.33528 (19) 1.03149 (17) 0.0447 (5)
C34 0.1535 (3) 0.2436 (2) 1.0129 (2) 0.0654 (7)
H34 0.1045 0.2443 0.9566 0.078*
C35 0.1709 (3) 0.1517 (3) 1.0762 (2) 0.0797 (9)
H35 0.1332 0.0908 1.0627 0.096*
C36 0.2433 (3) 0.1487 (3) 1.1591 (2) 0.0751 (8)
H36 0.2558 0.0859 1.2015 0.090*
C37 0.2964 (3) 0.2383 (3) 1.1787 (2) 0.0709 (8)
H37 0.3447 0.2371 1.2355 0.085*
C38 0.2797 (3) 0.3312 (2) 1.11548 (19) 0.0603 (7)
H38 0.3174 0.3918 1.1297 0.072*
N1 0.04442 (19) 0.27076 (14) 0.75517 (14) 0.0444 (5)
N2 0.2540 (2) 0.35239 (16) 0.62830 (15) 0.0488 (5)
N3 0.21246 (18) −0.07178 (14) 0.51377 (13) 0.0429 (4)
H3 0.1617 −0.1184 0.5395 0.052*
N4 0.37586 (19) 0.00010 (16) 0.40376 (14) 0.0461 (5)
N5 0.0722 (2) 0.76364 (15) 0.63503 (14) 0.0460 (5)
N6 0.2236 (2) 0.85701 (16) 0.75407 (15) 0.0505 (5)
N7 0.12911 (18) 0.44362 (14) 0.87635 (13) 0.0403 (4)
H7 0.0899 0.3947 0.8529 0.048*
N8 0.24317 (19) 0.52409 (15) 0.98030 (14) 0.0441 (4)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0537 (14) 0.0477 (14) 0.0407 (12) −0.0078 (11) −0.0015 (11) −0.0058 (11)
C2 0.0496 (13) 0.0490 (14) 0.0437 (12) −0.0115 (11) −0.0017 (11) 0.0028 (11)
C3 0.0518 (13) 0.0392 (12) 0.0451 (12) −0.0118 (10) −0.0098 (11) 0.0036 (10)
C4 0.0449 (12) 0.0340 (11) 0.0327 (10) −0.0070 (9) −0.0098 (9) 0.0033 (9)
C5 0.0489 (12) 0.0327 (11) 0.0346 (11) −0.0057 (10) −0.0103 (10) 0.0025 (9)
C6 0.0452 (12) 0.0406 (12) 0.0347 (11) −0.0076 (10) −0.0118 (10) 0.0055 (9)
C7 0.0446 (12) 0.0435 (13) 0.0382 (11) −0.0108 (10) −0.0140 (10) 0.0070 (10)
C8 0.0479 (14) 0.0620 (16) 0.0468 (13) −0.0183 (12) −0.0106 (11) 0.0090 (11)
C9 0.0588 (16) 0.0709 (18) 0.0647 (16) −0.0337 (14) −0.0118 (13) 0.0143 (14)
C10 0.0650 (17) 0.0540 (16) 0.0692 (17) −0.0279 (13) −0.0156 (14) 0.0053 (13)
C11 0.0452 (12) 0.0385 (12) 0.0385 (11) −0.0092 (10) −0.0162 (10) 0.0054 (9)
C12 0.0446 (12) 0.0364 (11) 0.0328 (10) −0.0066 (9) −0.0121 (9) 0.0031 (9)
C13 0.0481 (13) 0.0463 (13) 0.0351 (11) −0.0030 (11) −0.0094 (10) 0.0002 (10)
C14 0.0477 (13) 0.0498 (14) 0.0415 (12) −0.0009 (11) −0.0139 (10) −0.0055 (11)
C15 0.0723 (17) 0.0529 (16) 0.0540 (15) −0.0022 (13) −0.0077 (13) −0.0143 (13)
C16 0.086 (2) 0.0588 (18) 0.0757 (19) −0.0058 (15) −0.0186 (17) −0.0197 (15)
C17 0.0701 (19) 0.081 (2) 0.082 (2) 0.0056 (17) −0.0209 (17) −0.0417 (18)
C18 0.0578 (17) 0.103 (3) 0.0629 (17) −0.0055 (17) 0.0007 (14) −0.0354 (18)
C19 0.0541 (15) 0.0762 (18) 0.0535 (15) −0.0076 (13) −0.0047 (12) −0.0152 (14)
C20 0.0639 (15) 0.0469 (14) 0.0419 (12) −0.0100 (12) −0.0224 (11) 0.0082 (10)
C21 0.0564 (14) 0.0453 (14) 0.0483 (13) −0.0087 (11) −0.0235 (11) 0.0018 (11)
C22 0.0580 (14) 0.0366 (12) 0.0465 (12) −0.0103 (11) −0.0209 (11) 0.0018 (10)
C23 0.0429 (12) 0.0340 (12) 0.0366 (11) −0.0050 (9) −0.0092 (9) −0.0008 (9)
C24 0.0468 (12) 0.0322 (11) 0.0343 (10) −0.0053 (9) −0.0103 (9) 0.0005 (9)
C25 0.0449 (12) 0.0423 (12) 0.0330 (11) −0.0043 (10) −0.0094 (9) 0.0003 (9)
C26 0.0414 (12) 0.0431 (13) 0.0361 (11) −0.0079 (10) −0.0069 (9) −0.0017 (9)
C27 0.0543 (14) 0.0593 (16) 0.0434 (13) −0.0175 (12) −0.0142 (11) −0.0027 (11)
C28 0.0663 (16) 0.0649 (17) 0.0567 (15) −0.0290 (14) −0.0160 (13) −0.0051 (13)
C29 0.0739 (18) 0.0540 (16) 0.0648 (16) −0.0317 (14) −0.0175 (14) 0.0048 (13)
C30 0.0456 (12) 0.0366 (12) 0.0393 (11) −0.0104 (10) −0.0073 (10) −0.0009 (9)
C31 0.0434 (12) 0.0368 (12) 0.0337 (11) −0.0052 (9) −0.0087 (9) −0.0003 (9)
C32 0.0459 (13) 0.0442 (13) 0.0321 (10) −0.0027 (10) −0.0095 (9) 0.0022 (9)
C33 0.0474 (13) 0.0467 (13) 0.0350 (11) −0.0013 (10) −0.0059 (10) 0.0067 (10)
C34 0.085 (2) 0.0583 (17) 0.0612 (16) −0.0206 (15) −0.0298 (14) 0.0237 (13)
C35 0.103 (2) 0.0656 (19) 0.079 (2) −0.0267 (17) −0.0296 (18) 0.0329 (16)
C36 0.080 (2) 0.070 (2) 0.0656 (18) −0.0016 (16) −0.0087 (16) 0.0328 (15)
C37 0.0715 (19) 0.088 (2) 0.0504 (15) −0.0020 (17) −0.0226 (14) 0.0220 (15)
C38 0.0646 (17) 0.0678 (18) 0.0473 (14) −0.0062 (14) −0.0167 (12) 0.0108 (13)
N1 0.0540 (11) 0.0385 (10) 0.0400 (10) −0.0086 (9) −0.0094 (9) −0.0009 (8)
N2 0.0573 (12) 0.0411 (11) 0.0536 (11) −0.0171 (9) −0.0179 (9) 0.0032 (9)
N3 0.0521 (11) 0.0370 (10) 0.0377 (10) −0.0091 (8) −0.0049 (9) −0.0007 (8)
N4 0.0486 (11) 0.0494 (12) 0.0369 (9) −0.0057 (9) −0.0052 (8) −0.0018 (9)
N5 0.0581 (12) 0.0423 (11) 0.0408 (10) −0.0114 (9) −0.0165 (9) 0.0046 (8)
N6 0.0622 (13) 0.0431 (11) 0.0516 (11) −0.0204 (10) −0.0146 (10) 0.0027 (9)
N7 0.0514 (11) 0.0349 (10) 0.0373 (9) −0.0093 (8) −0.0149 (8) 0.0042 (8)
N8 0.0496 (11) 0.0466 (11) 0.0369 (9) −0.0079 (9) −0.0134 (8) 0.0042 (8)

Geometric parameters (Å, °)

C1—N1 1.327 (3) C20—C21 1.386 (3)
C1—C2 1.388 (3) C20—H20 0.9300
C1—H1 0.9300 C21—C22 1.366 (3)
C2—C3 1.362 (3) C21—H21 0.9300
C2—H2 0.9300 C22—C23 1.402 (3)
C3—C4 1.405 (3) C22—H22 0.9300
C3—H3A 0.9300 C23—C31 1.405 (3)
C4—C12 1.414 (3) C23—C24 1.420 (3)
C4—C5 1.426 (3) C24—N7 1.365 (3)
C5—N3 1.371 (2) C24—C25 1.384 (3)
C5—C6 1.374 (3) C25—N8 1.377 (3)
C6—N4 1.371 (3) C25—C26 1.430 (3)
C6—C7 1.427 (3) C26—C27 1.399 (3)
C7—C8 1.402 (3) C26—C30 1.407 (3)
C7—C11 1.414 (3) C27—C28 1.369 (3)
C8—C9 1.363 (3) C27—H27 0.9300
C8—H8 0.9300 C28—C29 1.388 (4)
C9—C10 1.390 (3) C28—H28 0.9300
C9—H9 0.9300 C29—N6 1.319 (3)
C10—N2 1.320 (3) C29—H29 0.9300
C10—H10 0.9300 C30—N6 1.352 (3)
C11—N2 1.350 (3) C30—C31 1.468 (3)
C11—C12 1.459 (3) C31—N5 1.358 (3)
C12—N1 1.359 (3) C32—N8 1.327 (3)
C13—N4 1.327 (3) C32—N7 1.365 (3)
C13—N3 1.367 (3) C32—C33 1.468 (3)
C13—C14 1.472 (3) C33—C38 1.377 (3)
C14—C19 1.381 (3) C33—C34 1.380 (3)
C14—C15 1.381 (3) C34—C35 1.371 (4)
C15—C16 1.377 (3) C34—H34 0.9300
C15—H15 0.9300 C35—C36 1.370 (4)
C16—C17 1.364 (4) C35—H35 0.9300
C16—H16 0.9300 C36—C37 1.354 (4)
C17—C18 1.360 (4) C36—H36 0.9300
C17—H17 0.9300 C37—C38 1.380 (4)
C18—C19 1.381 (3) C37—H37 0.9300
C18—H18 0.9300 C38—H38 0.9300
C19—H19 0.9300 N3—H3 0.8600
C20—N5 1.328 (3) N7—H7 0.8600
N1—C1—C2 123.9 (2) C21—C22—C23 119.0 (2)
N1—C1—H1 118.1 C21—C22—H22 120.5
C2—C1—H1 118.1 C23—C22—H22 120.5
C3—C2—C1 118.9 (2) C22—C23—C31 118.7 (2)
C3—C2—H2 120.5 C22—C23—C24 124.4 (2)
C1—C2—H2 120.5 C31—C23—C24 116.91 (18)
C2—C3—C4 119.3 (2) N7—C24—C25 105.51 (18)
C2—C3—H3A 120.3 N7—C24—C23 131.11 (18)
C4—C3—H3A 120.3 C25—C24—C23 123.3 (2)
C3—C4—C12 118.36 (18) N8—C25—C24 110.69 (19)
C3—C4—C5 124.80 (19) N8—C25—C26 128.53 (19)
C12—C4—C5 116.80 (18) C24—C25—C26 120.8 (2)
N3—C5—C6 105.81 (17) C27—C26—C30 118.2 (2)
N3—C5—C4 130.73 (19) C27—C26—C25 124.0 (2)
C6—C5—C4 123.36 (19) C30—C26—C25 117.79 (19)
N4—C6—C5 110.98 (18) C28—C27—C26 119.0 (2)
N4—C6—C7 128.25 (19) C28—C27—H27 120.5
C5—C6—C7 120.76 (18) C26—C27—H27 120.5
C8—C7—C11 118.0 (2) C27—C28—C29 118.6 (2)
C8—C7—C6 123.79 (19) C27—C28—H28 120.7
C11—C7—C6 118.21 (19) C29—C28—H28 120.7
C9—C8—C7 118.9 (2) N6—C29—C28 124.3 (2)
C9—C8—H8 120.6 N6—C29—H29 117.8
C7—C8—H8 120.6 C28—C29—H29 117.8
C8—C9—C10 119.2 (2) N6—C30—C26 122.15 (19)
C8—C9—H9 120.4 N6—C30—C31 117.3 (2)
C10—C9—H9 120.4 C26—C30—C31 120.52 (19)
N2—C10—C9 124.0 (2) N5—C31—C23 121.66 (18)
N2—C10—H10 118.0 N5—C31—C30 117.79 (19)
C9—C10—H10 118.0 C23—C31—C30 120.55 (19)
N2—C11—C7 122.30 (19) N8—C32—N7 112.31 (19)
N2—C11—C12 117.46 (19) N8—C32—C33 123.9 (2)
C7—C11—C12 120.21 (18) N7—C32—C33 123.74 (19)
N1—C12—C4 121.24 (19) C38—C33—C34 117.9 (2)
N1—C12—C11 118.20 (18) C38—C33—C32 119.7 (2)
C4—C12—C11 120.53 (18) C34—C33—C32 122.4 (2)
N4—C13—N3 112.41 (17) C35—C34—C33 120.9 (3)
N4—C13—C14 123.79 (19) C35—C34—H34 119.5
N3—C13—C14 123.8 (2) C33—C34—H34 119.5
C19—C14—C15 118.4 (2) C36—C35—C34 120.5 (3)
C19—C14—C13 118.8 (2) C36—C35—H35 119.7
C15—C14—C13 122.9 (2) C34—C35—H35 119.7
C16—C15—C14 121.1 (3) C37—C36—C35 119.2 (3)
C16—C15—H15 119.5 C37—C36—H36 120.4
C14—C15—H15 119.5 C35—C36—H36 120.4
C17—C16—C15 119.8 (3) C36—C37—C38 120.8 (3)
C17—C16—H16 120.1 C36—C37—H37 119.6
C15—C16—H16 120.1 C38—C37—H37 119.6
C18—C17—C16 119.9 (2) C33—C38—C37 120.7 (3)
C18—C17—H17 120.1 C33—C38—H38 119.7
C16—C17—H17 120.1 C37—C38—H38 119.7
C17—C18—C19 120.9 (3) C1—N1—C12 118.24 (18)
C17—C18—H18 119.6 C10—N2—C11 117.7 (2)
C19—C18—H18 119.6 C13—N3—C5 106.42 (18)
C14—C19—C18 120.0 (3) C13—N3—H3 126.8
C14—C19—H19 120.0 C5—N3—H3 126.8
C18—C19—H19 120.0 C13—N4—C6 104.37 (17)
N5—C20—C21 124.2 (2) C20—N5—C31 117.64 (19)
N5—C20—H20 117.9 C29—N6—C30 117.6 (2)
C21—C20—H20 117.9 C24—N7—C32 107.11 (17)
C22—C21—C20 118.7 (2) C24—N7—H7 126.4
C22—C21—H21 120.6 C32—N7—H7 126.4
C20—C21—H21 120.6 C32—N8—C25 104.37 (17)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N3—H3···N5i 0.86 2.10 2.932 (3) 164
N7—H7···N1 0.86 2.12 2.951 (2) 163

Symmetry codes: (i) x, y−1, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB2971).

References

  1. Che, G.-B., Liu, C.-B., Liu, B., Wang, Q.-W. & Xu, Z.-L. (2008). CrystEngComm, 10, 184–191.
  2. Higashi, T. (1995). ABSCOR Rigaku Corporation, Tokyo, Japan.
  3. Rigaku (1998). PROCESS-AUTO Rigaku Corporation, Tokyo, Japan.
  4. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  5. Steck, E. A. & Day, A. R. (1943). J. Am. Chem. Soc.65, 452–456.
  6. Stephenson, M. D. & Hardie, M. J. (2006). Cryst. Growth Des 6, 423–432.
  7. Xi, H.-M. (2008). Acta Cryst. E64, o1981. [DOI] [PMC free article] [PubMed]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809017498/hb2971sup1.cif

e-65-o1308-sup1.cif (23.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809017498/hb2971Isup2.hkl

e-65-o1308-Isup2.hkl (315.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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