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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Nov 3;68(Pt 12):o3278. doi: 10.1107/S1600536812044194

2-(5,6-Diphenyl-1,2,4-triazin-3-yl)aniline

Mariusz Mojzych a, Zbigniew Karczmarzyk a,*, Andrzej Fruziński b
PMCID: PMC3588826  PMID: 23468791

Abstract

The title compound, C21H16N4, obtained under standard Suzuki cross-coupling conditions, is a model compound in the synthesis and biological activity evaluation of new aza-analogues of sildenafil containing a pyrazolo­[4,3-e][1,2,4]triazine system. An N—H⋯N intra­molecular hydrogen bond involving the amino­benzene system and the 1,2,4-triazine moiety helps to establish a near coplanar orientation of the rings with a dihedral angle of 12.04 (4)°, which is believed to be necessary for the biological activity of sildenafil analogues. The 1,2,4-triazine ring is slightly distorted from planarity [r.m.s deviation = 0.0299 (11) Å] and forms dihedral angles of 58.60 (4) and 36.35 (3)° with the pendant phenyl rings. The crystal packing features bifurcated N—H⋯(N,N) hydrogen bonds linking screw-axis-related mol­ecules into chains parallel to the [010] direction and π–π inter­actions, with a centroid–centroid separation of 3.8722 (7) Å and a slippage of 1.412 (3) Å. The crystal studied was a nonmerohedral twin with a ratio of 0.707 (2):0293 (2).

Related literature  

For background information on the activity of sildenafil citrate, see: Terrett et al. (1996); Card et al. (2004). For the synthesis of the title compound, see: Agarwal et al. (2010). For a description of the Cambridge Structural Database, see: Allen (2002); Bruno et al. (2002).graphic file with name e-68-o3278-scheme1.jpg

Experimental  

Crystal data  

  • C21H16N4

  • M r = 324.38

  • Monoclinic, Inline graphic

  • a = 11.8797 (3) Å

  • b = 6.0788 (1) Å

  • c = 23.8710 (5) Å

  • β = 101.489 (1)°

  • V = 1689.29 (6) Å3

  • Z = 4

  • Cu Kα radiation

  • μ = 0.61 mm−1

  • T = 293 K

  • 0.21 × 0.14 × 0.01 mm

Data collection  

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2005) T min = 0.906, T max = 1.000

  • 4591 measured reflections

  • 3173 independent reflections

  • 2837 reflections with I > 2σ(I)

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.035

  • wR(F 2) = 0.103

  • S = 1.05

  • 4591 reflections

  • 275 parameters

  • All H-atom parameters refined

  • Δρmax = 0.10 e Å−3

  • Δρmin = −0.13 e Å−3

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2005); data reduction: SAINT; 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, 2012); software used to prepare material for publication: SHELXL97 and WinGX (Farrugia, 2012).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812044194/lr2082sup1.cif

e-68-o3278-sup1.cif (25.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812044194/lr2082Isup2.hkl

e-68-o3278-Isup2.hkl (220.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812044194/lr2082Isup3.cml

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
N7—H72⋯N2 0.94 (2) 2.00 (2) 2.7037 (19) 130 (2)
N7—H71⋯N1i 0.93 (3) 2.26 (3) 3.1779 (19) 169 (2)
N7—H71⋯N2i 0.93 (3) 2.49 (2) 3.2677 (18) 141.3 (19)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

This research was supported by grant No. NN405 092340 from the National Science Centre, Poland.

supplementary crystallographic information

Comment

Nowadays, sildenafil citrate (Viagra) is the first orally effective phosphodiesterase type 5 (PDE5) inhibitor available for the treatment of common and important medical problem e.g. male erectile dysfunction (MED) (Terrett et al., 1996). The earlier work on crystal structures of the catalytic domains of PDEs with different inhibitors have revealed two common features of inhibitor binding to PDEs: a planar ring structure of the inhibitor and hydrogen bond iteractions with an invariant glutamine residue (Card et al., 2004). With this in mind we have planned a new series of sildenafil analogues with pyrazolo[4,3-e][1,2,4]triazine system in which triazine ring nitrogen N1 plays a role of C=O group present in pyrimidinone moiety of sildenafil and ethylamino group in the position 2' of phenyl ring allowed to form intramolecular hydrogen bond between aminophenyl ring and pyrazolotriazine ring system. To clearly define the possibility and the place of intramolecular hydrogen bond formation in the new sildenafil analogues the synthesis and the crystal structure determination of an appropriate model 2-(5,6-diphenyl-1,2,4-triazin-3-yl)aniline, (I), were undertaken.

A search of the Cambridge Structural Database (CSD version 5.33, November 2011; Allen, 2002; Bruno et al., 2002) did not reveal any crystal structures containing the 3-(2-aminophenyl)-1,2,4-triazine structural unit. The structure of the molecule (I) is shown in Fig. 1. One can see that the 3-aminophenyl-1,2,4-triazine system exists in the crystal in the conformation with the torsion angle N2–C3–C31–C32 of -6.86 (17)°. This conformation is forced by the strong N7–H72···N2 intramolecular hydrogen bond (Table 1). The conformation of the 5- and 6-phenyl substituents of the 1,2,4-triazine system in relation to the triazine ring described by the torsion angles N4–C5–C51–C52 of -120.48 (13)° and N1–C6–C61–C62 of 35.44 (15)°, respectively, is forced by the steric effect of these bulky groups in adjacent positions of the heterocyclic system. This strong steric interaction causing the appearance of the strains in the triazine ring results in the distortion of its planarity with the displacements of the triazine atoms from the best plane within 0.0299 (11) Å.

In the crystal structure, the screw-related molecules are linked into chains along the [010] direction by bifurcated N7–H71···N1 and N7–H71···N2 intermolecular hydrogen bonds (Fig. 2) and the methine groups C53—H53 of the inversion-related molecules interact with π-electron system of the aminophenyl ring via C—H···π interaction (Table 1). Moreover, nearly coplanar mutual position of the triazine and aminophenyl rings is stabilized by the π–π interaction of these rings in the crystal structure. The π-electron systems of the pairs of triazine and aminophenyl rings belonging to the translation-related molecules overlap each other, with centroid-to-centroid separation of 3.8722 (7) Å between the triazine ring at (x, y, z) and aminophenyl ring at (x, -1 + y, z) and aminophenyl ring at (x, y, z) and triazine ring at (x, 1 + y, z). The π–π distances are 3.2886 (4) and 3.6055 (6) Å, respectively, the angle between overlapping planes is 12.13 (6)° and the slippage is 1.412 (3) Å.

In conclusion, the X-ray investigations of molecule (I) confirmed the assumed possibility of forming the N7–H···N2 intramolecular hydrogen bond stabilizing its cis conformation in the crystalline state, analogous to active conformation of sildenafil molecule.

Experimental

The title compound, (I), was obtained using standard Suzuki cross-coupling conditions (Agarwal et al., 2010), in the reaction of 3-bromo- and 3-chloro-5,6-diphenyl-1,2,4-triazine with 2-aminophenylboronic acid. To a solution of 3-halogeno-5,6-diphenyl-1,2,4-triazine (0.2 mmol) and 2-aminophenylboronic acid (0.22 mmol) in dioxane/water mixture (4:1) (2.5 ml) solution of K2CO3 (0.6 mmol) in 1 ml of water and Pd(PPh3)4 were added. The reaction mixture was stirred at 70°C for 12 h. After that time the solution was diluted with H2O (1.5 ml), and then the product was extracted three times with CH2Cl2 (3x2mL). The combined organic layer was dried over Na2SO4 and the solvent was removed in vacuo. The crude product was then subjected to column chromatography using CH2Cl2:hexane (4:1) as eluent. mp 161°C. Crystals suitable for X-ray diffraction analysis were grown by slow evaporation of an ethanol solution.

Refinement

The structure of (I) was refined as a nonmerohedral twin using 4591 reflections in the HKLF 5 file format and a BASF parameter of 0.70752 in SHELXL97 (Sheldrick, 2008). All H atoms were located from difference electron-density maps and their coordinates were refined with isotropic displacement parameters taken as 1.5 times those of the respective parent atoms.

Figures

Fig. 1.

Fig. 1.

A view of (I) with displacement ellipsoids drawn at the 50% probability level. H atoms are represented as small spheres of arbitrary radii.

Fig. 2.

Fig. 2.

A view of the molecular packing in (I). Dashed lines indicate N—H···N intermolecular hydrogen bond [symmetry code: (i) –x, y + 1/2, –z+1/2].

Crystal data

C21H16N4 F(000) = 680
Mr = 324.38 Dx = 1.275 Mg m3
Monoclinic, P21/c Melting point: 434 K
Hall symbol: -P 2ybc Cu Kα radiation, λ = 1.54178 Å
a = 11.8797 (3) Å Cell parameters from 241 reflections
b = 6.0788 (1) Å θ = 8.2–35.4°
c = 23.8710 (5) Å µ = 0.61 mm1
β = 101.489 (1)° T = 293 K
V = 1689.29 (6) Å3 Prism, yellow
Z = 4 0.21 × 0.14 × 0.01 mm

Data collection

Bruker APEXII CCD diffractometer 3173 independent reflections
Radiation source: fine-focus sealed tube 2837 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.000
ω scans θmax = 69.9°, θmin = 3.8°
Absorption correction: multi-scan (SADABS; Bruker, 2005) h = −14→14
Tmin = 0.906, Tmax = 1.000 k = 0→7
4591 measured reflections l = 0→29

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)] = 0.035 Hydrogen site location: difference Fourier map
wR(F2) = 0.103 All H-atom parameters refined
S = 1.05 w = 1/[σ2(Fo2) + (0.0591P)2 + 0.0858P] where P = (Fo2 + 2Fc2)/3
4591 reflections (Δ/σ)max < 0.001
275 parameters Δρmax = 0.10 e Å3
0 restraints Δρmin = −0.13 e Å3

Special details

Experimental. 1H-NMR (400 mHz, DMSO) δ: 6.85 (d, J = 7.2 Hz, 1H), 7.31 (t, J = 8.0 Hz, 1H), 7.35–7.45 (m, 6H), 7.60 (d, J = 8.0 Hz, 2H), 7.65 (d, J = 8.0 Hz, 2H), 8.61 (d, J = 8.0 Hz, 1H). 13C-NMR (100 MHz, DMSO) δ:167.68, 164.37, 162.95, 155.22, 153.98, 147.70, 135.91, 135.47, 132.71, 130.89, 130.77, 130.71, 129.82, 129.51, 129.36, 128.81, 128.61, 128.55, 117.98.
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
N1 0.18725 (9) −0.11023 (15) 0.18454 (4) 0.0576 (2)
N2 0.10666 (8) 0.04609 (16) 0.17863 (4) 0.0597 (2)
N4 0.14421 (8) 0.14537 (15) 0.08844 (4) 0.0526 (2)
N7 −0.07122 (15) 0.2512 (2) 0.21174 (7) 0.0864 (5)
H71 −0.114 (2) 0.294 (3) 0.2383 (11) 0.130*
H72 −0.025 (2) 0.125 (4) 0.2158 (10) 0.130*
C3 0.08941 (9) 0.1743 (2) 0.13234 (4) 0.0514 (2)
C5 0.21940 (9) −0.01610 (17) 0.09270 (4) 0.0492 (2)
C6 0.24565 (9) −0.14379 (17) 0.14325 (4) 0.0500 (2)
C31 0.00852 (9) 0.35952 (19) 0.12884 (5) 0.0547 (3)
C32 −0.06168 (10) 0.3956 (2) 0.16965 (5) 0.0637 (3)
C33 −0.12606 (12) 0.5930 (3) 0.16472 (6) 0.0777 (4)
H33 −0.1748 (17) 0.619 (3) 0.1937 (8) 0.117*
C34 −0.12449 (16) 0.7395 (2) 0.12196 (9) 0.0822 (5)
H34 −0.1621 (18) 0.878 (4) 0.1199 (9) 0.123*
C35 −0.06099 (14) 0.6990 (3) 0.07991 (8) 0.0766 (4)
H35 −0.0576 (19) 0.808 (3) 0.0485 (10) 0.115*
C36 0.00405 (11) 0.5109 (2) 0.08408 (6) 0.0641 (3)
H36 0.0494 (15) 0.481 (3) 0.0544 (7) 0.096*
C51 0.27044 (9) −0.05244 (18) 0.04130 (4) 0.0511 (2)
C52 0.25810 (15) −0.25262 (19) 0.01303 (7) 0.0654 (4)
H52 0.2176 (15) −0.371 (3) 0.0296 (8) 0.098*
C53 0.30015 (16) −0.2788 (3) −0.03670 (7) 0.0752 (4)
H53 0.2884 (17) −0.418 (3) −0.0560 (8) 0.113*
C54 0.35701 (13) −0.1102 (3) −0.05686 (5) 0.0746 (4)
H54 0.3858 (16) −0.127 (3) −0.0913 (8) 0.112*
C55 0.37091 (12) 0.0887 (3) −0.02854 (6) 0.0714 (4)
H55 0.412 (2) 0.210 (3) −0.0428 (10) 0.107*
C56 0.32644 (11) 0.1187 (2) 0.02024 (5) 0.0606 (3)
H56 0.3355 (18) 0.266 (2) 0.0396 (9) 0.091*
C61 0.33740 (11) −0.3132 (2) 0.15615 (5) 0.0551 (3)
C62 0.32080 (13) −0.4980 (2) 0.18810 (5) 0.0687 (3)
H62 0.2476 (16) −0.510 (3) 0.2016 (8) 0.103*
C63 0.40801 (19) −0.6518 (2) 0.20237 (6) 0.0890 (5)
H63 0.393 (2) −0.782 (3) 0.2224 (12) 0.133*
C64 0.51152 (18) −0.6245 (3) 0.18542 (7) 0.0932 (5)
H64 0.575 (3) −0.733 (3) 0.1959 (13) 0.140*
C65 0.52850 (15) −0.4423 (3) 0.15449 (6) 0.0865 (5)
H65 0.6019 (19) −0.420 (3) 0.1395 (9) 0.130*
C66 0.44224 (14) −0.2872 (3) 0.13971 (6) 0.0682 (3)
H66 0.4576 (16) −0.156 (3) 0.1189 (8) 0.102*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0658 (6) 0.0613 (5) 0.0496 (5) 0.0045 (4) 0.0205 (4) 0.0065 (4)
N2 0.0642 (6) 0.0681 (6) 0.0514 (5) 0.0073 (5) 0.0225 (4) 0.0050 (4)
N4 0.0578 (5) 0.0561 (5) 0.0460 (5) 0.0022 (4) 0.0153 (4) 0.0013 (4)
N7 0.0968 (11) 0.1108 (12) 0.0611 (8) 0.0297 (7) 0.0386 (7) 0.0003 (6)
C3 0.0519 (6) 0.0588 (6) 0.0452 (5) −0.0024 (5) 0.0135 (4) −0.0032 (5)
C5 0.0530 (5) 0.0511 (5) 0.0451 (5) −0.0014 (4) 0.0136 (4) −0.0003 (4)
C6 0.0563 (6) 0.0514 (6) 0.0440 (5) −0.0031 (4) 0.0144 (4) 0.0006 (4)
C31 0.0508 (6) 0.0607 (6) 0.0507 (6) 0.0018 (5) 0.0058 (4) −0.0076 (5)
C32 0.0571 (6) 0.0798 (8) 0.0524 (6) 0.0077 (6) 0.0062 (5) −0.0177 (5)
C33 0.0649 (8) 0.0954 (10) 0.0671 (8) 0.0208 (7) −0.0006 (6) −0.0267 (7)
C34 0.0694 (10) 0.0752 (10) 0.0900 (13) 0.0193 (6) −0.0132 (9) −0.0201 (7)
C35 0.0697 (9) 0.0695 (7) 0.0828 (10) 0.0051 (7) −0.0039 (7) 0.0023 (8)
C36 0.0578 (7) 0.0660 (7) 0.0659 (7) 0.0021 (6) 0.0057 (5) 0.0011 (6)
C51 0.0525 (6) 0.0593 (6) 0.0426 (5) 0.0065 (5) 0.0121 (4) 0.0044 (4)
C52 0.0730 (10) 0.0680 (8) 0.0584 (8) −0.0055 (5) 0.0212 (7) −0.0080 (5)
C53 0.0830 (10) 0.0850 (9) 0.0607 (9) 0.0037 (7) 0.0216 (7) −0.0181 (6)
C54 0.0779 (9) 0.1029 (11) 0.0487 (6) 0.0177 (8) 0.0259 (6) 0.0037 (6)
C55 0.0747 (8) 0.0833 (8) 0.0635 (7) 0.0113 (7) 0.0315 (6) 0.0178 (6)
C56 0.0680 (7) 0.0609 (6) 0.0571 (6) 0.0083 (5) 0.0225 (5) 0.0090 (5)
C61 0.0674 (7) 0.0539 (5) 0.0433 (5) 0.0046 (6) 0.0093 (5) −0.0016 (5)
C62 0.0915 (9) 0.0567 (7) 0.0547 (6) −0.0009 (6) 0.0064 (6) 0.0018 (5)
C63 0.1393 (15) 0.0572 (8) 0.0612 (8) 0.0166 (8) −0.0020 (8) 0.0044 (6)
C64 0.1146 (13) 0.0931 (11) 0.0642 (8) 0.0476 (10) −0.0003 (8) −0.0045 (8)
C65 0.0844 (10) 0.1098 (11) 0.0645 (8) 0.0360 (9) 0.0129 (7) 0.0006 (8)
C66 0.0714 (9) 0.0806 (8) 0.0543 (7) 0.0163 (7) 0.0165 (6) 0.0052 (6)

Geometric parameters (Å, º)

N1—C6 1.3293 (13) C51—C56 1.3824 (16)
N1—N2 1.3363 (13) C51—C52 1.3850 (16)
N2—C3 1.3344 (14) C52—C53 1.386 (2)
N4—C5 1.3174 (13) C52—H52 0.990 (17)
N4—C3 1.3509 (13) C53—C54 1.367 (2)
N7—C32 1.3559 (19) C53—H53 0.96 (2)
N7—H71 0.92 (3) C54—C55 1.379 (2)
N7—H72 0.94 (2) C54—H54 0.957 (19)
C3—C31 1.4717 (16) C55—C56 1.3831 (17)
C5—C6 1.4164 (14) C55—H55 0.98 (2)
C5—C51 1.4893 (14) C56—H56 1.003 (15)
C6—C61 1.4865 (16) C61—C66 1.3874 (19)
C31—C36 1.4029 (17) C61—C62 1.3936 (17)
C31—C32 1.4200 (16) C62—C63 1.387 (2)
C32—C33 1.4152 (19) C62—H62 0.989 (18)
C33—C34 1.358 (2) C63—C64 1.379 (3)
C33—H33 1.000 (19) C63—H63 0.96 (2)
C34—C35 1.393 (3) C64—C65 1.368 (3)
C34—H34 0.95 (2) C64—H64 0.99 (3)
C35—C36 1.372 (2) C65—C66 1.385 (2)
C35—H35 1.01 (2) C65—H65 1.02 (2)
C36—H36 0.988 (17) C66—H66 0.973 (19)
C6—N1—N2 119.97 (9) C52—C51—C5 120.71 (10)
C3—N2—N1 119.44 (9) C51—C52—C53 119.81 (12)
C5—N4—C3 117.47 (9) C51—C52—H52 117.1 (10)
C32—N7—H71 117.6 (14) C53—C52—H52 123.1 (10)
C32—N7—H72 118.4 (13) C54—C53—C52 120.20 (14)
H71—N7—H72 123 (2) C54—C53—H53 121.8 (11)
N2—C3—N4 123.24 (10) C52—C53—H53 118.0 (11)
N2—C3—C31 118.99 (9) C53—C54—C55 120.29 (12)
N4—C3—C31 117.75 (10) C53—C54—H54 120.6 (12)
N4—C5—C6 120.33 (9) C55—C54—H54 119.1 (12)
N4—C5—C51 115.34 (9) C54—C55—C56 119.98 (13)
C6—C5—C51 124.33 (9) C54—C55—H55 120.5 (12)
N1—C6—C5 119.27 (10) C56—C55—H55 119.6 (12)
N1—C6—C61 114.97 (9) C55—C56—C51 119.95 (12)
C5—C6—C61 125.74 (9) C55—C56—H56 118.8 (11)
C36—C31—C32 118.88 (11) C51—C56—H56 121.2 (11)
C36—C31—C3 118.05 (10) C66—C61—C62 118.64 (13)
C32—C31—C3 123.04 (10) C66—C61—C6 121.68 (11)
N7—C32—C33 119.15 (12) C62—C61—C6 119.60 (11)
N7—C32—C31 123.76 (11) C63—C62—C61 119.86 (15)
C33—C32—C31 117.09 (13) C63—C62—H62 122.1 (10)
C34—C33—C32 122.06 (14) C61—C62—H62 118.0 (10)
C34—C33—H33 120.7 (12) C64—C63—C62 120.86 (15)
C32—C33—H33 117.2 (12) C64—C63—H63 120.9 (15)
C33—C34—C35 121.08 (13) C62—C63—H63 118.1 (15)
C33—C34—H34 122.9 (12) C65—C64—C63 119.45 (15)
C35—C34—H34 116.0 (12) C65—C64—H64 119.1 (15)
C36—C35—C34 118.24 (15) C63—C64—H64 121.5 (15)
C36—C35—H35 119.8 (12) C64—C65—C66 120.48 (17)
C34—C35—H35 121.8 (12) C64—C65—H65 121.9 (12)
C35—C36—C31 122.48 (13) C66—C65—H65 117.5 (12)
C35—C36—H36 118.7 (10) C65—C66—C61 120.72 (14)
C31—C36—H36 118.8 (10) C65—C66—H66 118.8 (11)
C56—C51—C52 119.73 (11) C61—C66—H66 120.4 (11)
C56—C51—C5 119.50 (10)
C6—N1—N2—C3 −3.18 (16) C32—C31—C36—C35 3.59 (18)
N1—N2—C3—N4 4.71 (17) C3—C31—C36—C35 −174.22 (12)
N1—N2—C3—C31 −174.12 (10) N4—C5—C51—C56 56.74 (14)
C5—N4—C3—N2 −1.09 (16) C6—C5—C51—C56 −124.24 (12)
C5—N4—C3—C31 177.74 (10) N4—C5—C51—C52 −120.48 (13)
C3—N4—C5—C6 −3.78 (15) C6—C5—C51—C52 58.55 (16)
C3—N4—C5—C51 175.29 (10) C56—C51—C52—C53 −1.1 (2)
N2—N1—C6—C5 −1.55 (16) C5—C51—C52—C53 176.07 (14)
N2—N1—C6—C61 176.68 (10) C51—C52—C53—C54 2.2 (3)
N4—C5—C6—N1 5.17 (16) C52—C53—C54—C55 −1.3 (2)
C51—C5—C6—N1 −173.81 (10) C53—C54—C55—C56 −0.5 (2)
N4—C5—C6—C61 −172.85 (10) C54—C55—C56—C51 1.5 (2)
C51—C5—C6—C61 8.17 (17) C52—C51—C56—C55 −0.68 (19)
N2—C3—C31—C36 170.85 (10) C5—C51—C56—C55 −177.92 (11)
N4—C3—C31—C36 −8.04 (16) N1—C6—C61—C66 −141.19 (12)
N2—C3—C31—C32 −6.86 (17) C5—C6—C61—C66 36.90 (18)
N4—C3—C31—C32 174.25 (10) N1—C6—C61—C62 35.44 (15)
C36—C31—C32—N7 174.38 (14) C5—C6—C61—C62 −146.47 (11)
C3—C31—C32—N7 −7.92 (19) C66—C61—C62—C63 −0.48 (19)
C36—C31—C32—C33 −4.54 (17) C6—C61—C62—C63 −177.22 (11)
C3—C31—C32—C33 173.16 (11) C61—C62—C63—C64 0.1 (2)
N7—C32—C33—C34 −176.88 (15) C62—C63—C64—C65 0.5 (2)
C31—C32—C33—C34 2.1 (2) C63—C64—C65—C66 −0.7 (2)
C32—C33—C34—C35 1.6 (2) C64—C65—C66—C61 0.3 (2)
C33—C34—C35—C36 −2.7 (2) C62—C61—C66—C65 0.3 (2)
C34—C35—C36—C31 0.1 (2) C6—C61—C66—C65 176.97 (13)

Hydrogen-bond geometry (Å, º)

Cg - the centroid of the C31-C36 phenyl ring.

D—H···A D—H H···A D···A D—H···A
N7—H72···N2 0.94 (2) 2.00 (2) 2.7037 (19) 130 (2)
N7—H71···N1i 0.93 (3) 2.26 (3) 3.1779 (19) 169 (2)
N7—H71···N2i 0.93 (3) 2.49 (2) 3.2677 (18) 141.3 (19)
C53—H53···Cgii 0.96 (2) 2.99 (2) 3.5888 (19) 122.0 (14)

Symmetry codes: (i) −x, y+1/2, −z+1/2; (ii) −x, −y, −z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LR2082).

References

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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/S1600536812044194/lr2082sup1.cif

e-68-o3278-sup1.cif (25.3KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812044194/lr2082Isup2.hkl

e-68-o3278-Isup2.hkl (220.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812044194/lr2082Isup3.cml

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


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