Abstract
In the title compound, C26H23FN6S, the pyrazole ring has an envelope conformation, with the methine C atom being the flap atom. The thiourea group is close to being coplanar with the pyrazole N atoms [N—N—C—S torsion angle = 176.78 (15)°], which allows for an intramolecular N—H⋯N hydrogen bond; the connected triazole ring is nearly coplanar with this ring [N—C—C—N = −172.65 (19)°]. There is a significant twist between the pyrazole ring and attached fluorobenzene ring [N—C—C—C = −18.8 (3)°] and a greater twist between triazole and attached tolyl ring [dihedral angle = 58.25 (14)°]. In the crystal, supramolecular chains aligned along [40,10] are consolidated by π–π interactions between the triazole and phenyl rings [centroid–centroid distance = 3.7053 (13) Å].
Related literature
For the biological activity and synthesis of related compounds, see: Abdel-Wahab, Abdel-Latif et al. (2012 ▶). For a related structure, see: Abdel-Wahab, Mohamed et al. (2012 ▶).
Experimental
Crystal data
C26H23FN6S
M r = 470.56
Monoclinic,
a = 6.5449 (5) Å
b = 26.1030 (17) Å
c = 14.3818 (8) Å
β = 100.604 (7)°
V = 2415.0 (3) Å3
Z = 4
Mo Kα radiation
μ = 0.17 mm−1
T = 295 K
0.40 × 0.30 × 0.20 mm
Data collection
Agilent SuperNova Dual diffractometer with an Atlas detector
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011 ▶) T min = 0.802, T max = 1.000
15173 measured reflections
5578 independent reflections
3313 reflections with I > 2σ(I)
R int = 0.040
Refinement
R[F 2 > 2σ(F 2)] = 0.056
wR(F 2) = 0.162
S = 1.03
5578 reflections
313 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.17 e Å−3
Δρmin = −0.21 e Å−3
Data collection: CrysAlis PRO (Agilent, 2011 ▶); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; 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 ▶) and DIAMOND (Brandenburg, 2006 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536813008155/hg5303sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813008155/hg5303Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536813008155/hg5303Isup3.cml
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 |
|---|---|---|---|---|
| N1—H3⋯N3 | 0.83 (3) | 2.05 (3) | 2.568 (3) | 120 (2) |
Acknowledgments
We thank the Ministry of Higher Education (Malaysia) for funding structural studies through the High-Impact Research scheme (UM.C/HIR-MOHE/SC/03).
supplementary crystallographic information
Comment
In connection with studies into the biological studies on related pyrazolines (Abdel-Wahab, Abdel-Latif et al., 2012), the title compound, (I), was investigated.
In (I), Fig. 1, the pyrazole ring has an envelope conformation with the methine-C8 atom being the flap atom. The thiourea group is close to co-planar with the N atoms of this ring [the N3—N2—C7—S1 torsion angle = 176.78 (15)°], which allows for an intramolecular N1—H···N3 hydrogen bond, Table 1, and the connected triazole ring is slightly twisted out of the plane through this ring [N3—C10—C17—N4 is -172.65 (19)°]. There is a significant twist between the pyrazole ring and attached fluorobenzene ring as seen in the N2—C8—C11—C12 torsion angle of -18.8 (3)°, and an even greater twist between triazole and attached tolyl ring with the dihedral angle being 58.25 (14)°. The relative dispositions of the terminal substituent in (I) resembles those found in a recently determined structure with pyrazole-p-tolyl and triazole-4-(piperidin-1-yl)phenyl substituents (Abdel-Wahab, Mohamed et al., 2012).
The most prominent feature of the crystal packing is the formation of π—π interactions between the triazole and phenyl rings [inter-centroid distance = 3.7053 (13) Å, angle of inclination = 10.17 (12)° for symmetry operation i: 1 + x, 3/2 - y, 1/2 + z]. These lead to a supramolecular chains, aligned approximately along [1 0 2], and which aggregate in the ac plane with no specific interactions between them, Fig. 2. Layers thus formed stack along the b axis, Fig. 3.
Experimental
The title compound was prepared according to the reported method (Abdel-Wahab, Abdel-Latif et al., 2012). Colourless crystals were obtained from its DMF solution by slow evaporation at room temperature.
Refinement
Carbon-bound H-atoms were placed in calculated positions (C—H = 0.93 to 0.98 Å) and were included in the refinement in the riding model approximation, with Uiso(H) = 1.2–1.5Uequiv(C). The nitrogen-bound H-atom was refined freely.
Figures
Fig. 1.
The molecular structure of (I) showing the atom-labelling scheme and displacement ellipsoids at the 35% probability level.
Fig. 2.
A view of the crystal packing in (I) highlighting the supramolecular chains sustained by π—π interactions (purple dashed lines).
Fig. 3.
A view of the crystal packing in projection down the a axis. The π—π interactions are shown as purple dashed lines.
Crystal data
| C26H23FN6S | F(000) = 984 |
| Mr = 470.56 | Dx = 1.294 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 2937 reflections |
| a = 6.5449 (5) Å | θ = 2.9–27.5° |
| b = 26.1030 (17) Å | µ = 0.17 mm−1 |
| c = 14.3818 (8) Å | T = 295 K |
| β = 100.604 (7)° | Prism, colourless |
| V = 2415.0 (3) Å3 | 0.40 × 0.30 × 0.20 mm |
| Z = 4 |
Data collection
| Agilent SuperNova Dual diffractometer with an Atlas detector | 5578 independent reflections |
| Radiation source: SuperNova (Mo) X-ray Source | 3313 reflections with I > 2σ(I) |
| Mirror monochromator | Rint = 0.040 |
| Detector resolution: 10.4041 pixels mm-1 | θmax = 27.6°, θmin = 2.9° |
| ω scan | h = −8→8 |
| Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2011) | k = −33→33 |
| Tmin = 0.802, Tmax = 1.000 | l = −18→18 |
| 15173 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)] = 0.056 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.162 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.03 | w = 1/[σ2(Fo2) + (0.0643P)2 + 0.3514P] where P = (Fo2 + 2Fc2)/3 |
| 5578 reflections | (Δ/σ)max = 0.001 |
| 313 parameters | Δρmax = 0.17 e Å−3 |
| 0 restraints | Δρmin = −0.21 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 | ||
| S1 | 0.28247 (11) | 0.59566 (2) | 0.26576 (4) | 0.0660 (2) | |
| F1 | 0.4921 (5) | 0.53780 (11) | 0.71572 (17) | 0.1882 (13) | |
| N1 | 0.2779 (3) | 0.69941 (8) | 0.25175 (14) | 0.0581 (5) | |
| N2 | 0.5580 (3) | 0.66351 (7) | 0.34286 (12) | 0.0538 (5) | |
| N3 | 0.6368 (3) | 0.71314 (7) | 0.35592 (12) | 0.0519 (5) | |
| N4 | 1.1621 (3) | 0.75227 (8) | 0.45157 (14) | 0.0624 (5) | |
| N5 | 1.2414 (3) | 0.79826 (8) | 0.45671 (15) | 0.0662 (6) | |
| N6 | 1.0814 (3) | 0.83112 (8) | 0.42485 (12) | 0.0584 (5) | |
| C1 | 0.0777 (3) | 0.71154 (8) | 0.20191 (14) | 0.0503 (5) | |
| C2 | 0.0342 (4) | 0.76336 (9) | 0.18895 (15) | 0.0580 (6) | |
| H2 | 0.1373 | 0.7873 | 0.2105 | 0.070* | |
| C3 | −0.1592 (4) | 0.77990 (10) | 0.14473 (15) | 0.0635 (7) | |
| H3A | −0.1860 | 0.8148 | 0.1371 | 0.076* | |
| C4 | −0.3132 (4) | 0.74477 (11) | 0.11172 (15) | 0.0655 (7) | |
| H4 | −0.4442 | 0.7557 | 0.0819 | 0.079* | |
| C5 | −0.2697 (4) | 0.69365 (11) | 0.12361 (16) | 0.0659 (7) | |
| H5 | −0.3729 | 0.6699 | 0.1012 | 0.079* | |
| C6 | −0.0762 (4) | 0.67637 (9) | 0.16809 (15) | 0.0608 (6) | |
| H6 | −0.0500 | 0.6414 | 0.1751 | 0.073* | |
| C7 | 0.3712 (4) | 0.65505 (8) | 0.28600 (14) | 0.0504 (5) | |
| C8 | 0.7040 (3) | 0.62449 (9) | 0.39009 (14) | 0.0532 (6) | |
| H8 | 0.7241 | 0.5976 | 0.3451 | 0.064* | |
| C9 | 0.9037 (3) | 0.65642 (9) | 0.41746 (16) | 0.0572 (6) | |
| H9A | 0.9644 | 0.6520 | 0.4837 | 0.069* | |
| H9B | 1.0056 | 0.6472 | 0.3792 | 0.069* | |
| C10 | 0.8281 (3) | 0.70984 (9) | 0.39768 (14) | 0.0503 (5) | |
| C11 | 0.6339 (4) | 0.60126 (9) | 0.47522 (15) | 0.0547 (6) | |
| C12 | 0.4899 (4) | 0.62432 (10) | 0.51996 (17) | 0.0666 (7) | |
| H12 | 0.4242 | 0.6543 | 0.4956 | 0.080* | |
| C13 | 0.4429 (5) | 0.60252 (14) | 0.6021 (2) | 0.0936 (10) | |
| H13 | 0.3470 | 0.6179 | 0.6336 | 0.112* | |
| C14 | 0.5405 (7) | 0.55819 (17) | 0.6353 (2) | 0.1117 (13) | |
| C15 | 0.6779 (7) | 0.53446 (15) | 0.5924 (3) | 0.1172 (13) | |
| H15 | 0.7404 | 0.5041 | 0.6164 | 0.141* | |
| C16 | 0.7249 (5) | 0.55604 (11) | 0.5117 (2) | 0.0877 (9) | |
| H16 | 0.8202 | 0.5398 | 0.4810 | 0.105* | |
| C17 | 0.9534 (3) | 0.75537 (9) | 0.41700 (14) | 0.0520 (5) | |
| C18 | 0.8996 (3) | 0.80599 (9) | 0.39990 (14) | 0.0530 (5) | |
| C19 | 0.6961 (4) | 0.83117 (10) | 0.36692 (18) | 0.0669 (7) | |
| H19A | 0.7083 | 0.8672 | 0.3802 | 0.100* | |
| H19B | 0.5940 | 0.8165 | 0.3991 | 0.100* | |
| H19C | 0.6543 | 0.8261 | 0.3000 | 0.100* | |
| C20 | 1.1213 (4) | 0.88469 (10) | 0.41824 (18) | 0.0636 (6) | |
| C21 | 1.2087 (4) | 0.91154 (11) | 0.4967 (2) | 0.0790 (8) | |
| H21 | 1.2441 | 0.8953 | 0.5550 | 0.095* | |
| C22 | 1.2439 (5) | 0.96392 (12) | 0.4878 (3) | 0.0979 (10) | |
| H22 | 1.3019 | 0.9826 | 0.5413 | 0.117* | |
| C23 | 1.1953 (5) | 0.98862 (13) | 0.4024 (3) | 0.1023 (11) | |
| C24 | 1.1078 (6) | 0.95997 (14) | 0.3244 (3) | 0.1113 (12) | |
| H24 | 1.0730 | 0.9758 | 0.2657 | 0.134* | |
| C25 | 1.0717 (5) | 0.90862 (12) | 0.3320 (2) | 0.0926 (10) | |
| H25 | 1.0134 | 0.8899 | 0.2786 | 0.111* | |
| C26 | 1.2352 (5) | 1.04560 (13) | 0.3937 (4) | 0.151 (2) | |
| H26A | 1.2715 | 1.0604 | 0.4556 | 0.227* | |
| H26B | 1.1121 | 1.0619 | 0.3599 | 0.227* | |
| H26C | 1.3473 | 1.0506 | 0.3599 | 0.227* | |
| H3 | 0.355 (5) | 0.7242 (10) | 0.2690 (19) | 0.080 (9)* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.0670 (5) | 0.0540 (4) | 0.0691 (4) | 0.0000 (3) | −0.0082 (3) | −0.0048 (3) |
| F1 | 0.231 (3) | 0.219 (3) | 0.1311 (18) | −0.018 (2) | 0.0773 (19) | 0.0845 (19) |
| N1 | 0.0465 (12) | 0.0515 (12) | 0.0686 (12) | −0.0016 (9) | −0.0094 (10) | 0.0012 (10) |
| N2 | 0.0447 (11) | 0.0541 (11) | 0.0577 (10) | −0.0005 (9) | −0.0038 (9) | 0.0055 (9) |
| N3 | 0.0419 (11) | 0.0577 (11) | 0.0533 (10) | −0.0040 (9) | 0.0018 (9) | 0.0021 (8) |
| N4 | 0.0391 (11) | 0.0766 (14) | 0.0691 (12) | −0.0062 (10) | 0.0038 (9) | 0.0110 (10) |
| N5 | 0.0392 (11) | 0.0766 (14) | 0.0799 (13) | −0.0071 (10) | 0.0033 (10) | 0.0126 (11) |
| N6 | 0.0420 (11) | 0.0739 (13) | 0.0585 (10) | −0.0079 (10) | 0.0069 (9) | 0.0072 (10) |
| C1 | 0.0435 (13) | 0.0598 (14) | 0.0438 (10) | 0.0014 (10) | −0.0018 (9) | 0.0020 (10) |
| C2 | 0.0570 (15) | 0.0587 (14) | 0.0543 (12) | 0.0013 (11) | −0.0001 (11) | 0.0060 (10) |
| C3 | 0.0608 (16) | 0.0713 (16) | 0.0552 (13) | 0.0141 (13) | 0.0023 (12) | 0.0123 (12) |
| C4 | 0.0492 (15) | 0.0914 (19) | 0.0517 (12) | 0.0119 (14) | −0.0018 (11) | 0.0060 (13) |
| C5 | 0.0490 (15) | 0.0826 (18) | 0.0605 (13) | −0.0044 (13) | −0.0046 (12) | −0.0059 (13) |
| C6 | 0.0532 (15) | 0.0620 (14) | 0.0617 (13) | 0.0002 (12) | −0.0042 (11) | −0.0070 (11) |
| C7 | 0.0473 (13) | 0.0569 (13) | 0.0445 (10) | 0.0017 (10) | 0.0020 (10) | 0.0008 (10) |
| C8 | 0.0475 (13) | 0.0581 (14) | 0.0511 (11) | 0.0086 (10) | 0.0013 (10) | 0.0023 (10) |
| C9 | 0.0400 (13) | 0.0709 (15) | 0.0592 (12) | 0.0056 (11) | 0.0049 (10) | 0.0081 (11) |
| C10 | 0.0392 (12) | 0.0660 (14) | 0.0450 (10) | 0.0006 (10) | 0.0059 (9) | 0.0041 (10) |
| C11 | 0.0489 (14) | 0.0561 (13) | 0.0555 (12) | −0.0058 (11) | −0.0001 (11) | 0.0023 (10) |
| C12 | 0.0601 (16) | 0.0752 (17) | 0.0637 (14) | −0.0069 (13) | 0.0092 (13) | −0.0015 (13) |
| C13 | 0.085 (2) | 0.122 (3) | 0.0793 (19) | −0.018 (2) | 0.0293 (17) | −0.0031 (19) |
| C14 | 0.124 (3) | 0.132 (3) | 0.081 (2) | −0.026 (3) | 0.023 (2) | 0.041 (2) |
| C15 | 0.131 (3) | 0.108 (3) | 0.111 (3) | 0.013 (2) | 0.020 (3) | 0.055 (2) |
| C16 | 0.092 (2) | 0.082 (2) | 0.0896 (19) | 0.0178 (17) | 0.0177 (17) | 0.0252 (17) |
| C17 | 0.0385 (12) | 0.0715 (15) | 0.0453 (10) | −0.0048 (11) | 0.0058 (9) | 0.0062 (10) |
| C18 | 0.0407 (13) | 0.0708 (15) | 0.0479 (11) | −0.0051 (11) | 0.0088 (10) | 0.0043 (11) |
| C19 | 0.0452 (14) | 0.0740 (17) | 0.0788 (16) | 0.0009 (12) | 0.0045 (12) | 0.0087 (13) |
| C20 | 0.0442 (14) | 0.0697 (16) | 0.0753 (16) | −0.0098 (12) | 0.0070 (12) | 0.0136 (13) |
| C21 | 0.0627 (18) | 0.0807 (19) | 0.0870 (18) | −0.0114 (14) | −0.0036 (15) | 0.0070 (15) |
| C22 | 0.062 (2) | 0.079 (2) | 0.142 (3) | −0.0133 (16) | −0.009 (2) | −0.003 (2) |
| C23 | 0.0480 (17) | 0.078 (2) | 0.175 (3) | −0.0001 (15) | 0.004 (2) | 0.039 (2) |
| C24 | 0.088 (3) | 0.112 (3) | 0.129 (3) | −0.015 (2) | 0.007 (2) | 0.055 (2) |
| C25 | 0.096 (2) | 0.097 (2) | 0.0811 (18) | −0.0215 (18) | 0.0057 (17) | 0.0258 (17) |
| C26 | 0.076 (2) | 0.074 (2) | 0.291 (6) | −0.0018 (18) | −0.002 (3) | 0.058 (3) |
Geometric parameters (Å, º)
| S1—C7 | 1.662 (2) | C10—C17 | 1.442 (3) |
| F1—C14 | 1.363 (4) | C11—C12 | 1.374 (3) |
| N1—C7 | 1.358 (3) | C11—C16 | 1.381 (3) |
| N1—C1 | 1.409 (3) | C12—C13 | 1.395 (4) |
| N1—H3 | 0.83 (3) | C12—H12 | 0.9300 |
| N2—C7 | 1.358 (3) | C13—C14 | 1.365 (5) |
| N2—N3 | 1.394 (2) | C13—H13 | 0.9300 |
| N2—C8 | 1.474 (3) | C14—C15 | 1.333 (5) |
| N3—C10 | 1.288 (3) | C15—C16 | 1.375 (4) |
| N4—N5 | 1.305 (3) | C15—H15 | 0.9300 |
| N4—C17 | 1.367 (3) | C16—H16 | 0.9300 |
| N5—N6 | 1.366 (3) | C17—C18 | 1.378 (3) |
| N6—C18 | 1.348 (3) | C18—C19 | 1.482 (3) |
| N6—C20 | 1.429 (3) | C19—H19A | 0.9600 |
| C1—C6 | 1.383 (3) | C19—H19B | 0.9600 |
| C1—C2 | 1.388 (3) | C19—H19C | 0.9600 |
| C2—C3 | 1.377 (3) | C20—C21 | 1.361 (4) |
| C2—H2 | 0.9300 | C20—C25 | 1.373 (4) |
| C3—C4 | 1.381 (4) | C21—C22 | 1.396 (4) |
| C3—H3A | 0.9300 | C21—H21 | 0.9300 |
| C4—C5 | 1.368 (4) | C22—C23 | 1.372 (5) |
| C4—H4 | 0.9300 | C22—H22 | 0.9300 |
| C5—C6 | 1.385 (3) | C23—C24 | 1.382 (5) |
| C5—H5 | 0.9300 | C23—C26 | 1.519 (4) |
| C6—H6 | 0.9300 | C24—C25 | 1.369 (4) |
| C8—C11 | 1.511 (3) | C24—H24 | 0.9300 |
| C8—C9 | 1.539 (3) | C25—H25 | 0.9300 |
| C8—H8 | 0.9800 | C26—H26A | 0.9600 |
| C9—C10 | 1.489 (3) | C26—H26B | 0.9600 |
| C9—H9A | 0.9700 | C26—H26C | 0.9600 |
| C9—H9B | 0.9700 | ||
| C7—N1—C1 | 133.6 (2) | C11—C12—C13 | 119.7 (3) |
| C7—N1—H3 | 110 (2) | C11—C12—H12 | 120.2 |
| C1—N1—H3 | 116 (2) | C13—C12—H12 | 120.2 |
| C7—N2—N3 | 120.12 (17) | C14—C13—C12 | 118.7 (3) |
| C7—N2—C8 | 126.89 (18) | C14—C13—H13 | 120.7 |
| N3—N2—C8 | 112.83 (17) | C12—C13—H13 | 120.7 |
| C10—N3—N2 | 107.71 (17) | C15—C14—F1 | 119.6 (4) |
| N5—N4—C17 | 109.1 (2) | C15—C14—C13 | 123.0 (3) |
| N4—N5—N6 | 106.63 (18) | F1—C14—C13 | 117.5 (4) |
| C18—N6—N5 | 111.6 (2) | C14—C15—C16 | 118.4 (3) |
| C18—N6—C20 | 128.4 (2) | C14—C15—H15 | 120.8 |
| N5—N6—C20 | 119.91 (19) | C16—C15—H15 | 120.8 |
| C6—C1—C2 | 118.8 (2) | C15—C16—C11 | 121.5 (3) |
| C6—C1—N1 | 125.3 (2) | C15—C16—H16 | 119.2 |
| C2—C1—N1 | 115.9 (2) | C11—C16—H16 | 119.2 |
| C3—C2—C1 | 121.1 (2) | N4—C17—C18 | 109.1 (2) |
| C3—C2—H2 | 119.5 | N4—C17—C10 | 121.1 (2) |
| C1—C2—H2 | 119.5 | C18—C17—C10 | 129.7 (2) |
| C2—C3—C4 | 120.1 (2) | N6—C18—C17 | 103.6 (2) |
| C2—C3—H3A | 120.0 | N6—C18—C19 | 124.5 (2) |
| C4—C3—H3A | 120.0 | C17—C18—C19 | 131.9 (2) |
| C5—C4—C3 | 118.9 (2) | C18—C19—H19A | 109.5 |
| C5—C4—H4 | 120.6 | C18—C19—H19B | 109.5 |
| C3—C4—H4 | 120.6 | H19A—C19—H19B | 109.5 |
| C4—C5—C6 | 121.8 (2) | C18—C19—H19C | 109.5 |
| C4—C5—H5 | 119.1 | H19A—C19—H19C | 109.5 |
| C6—C5—H5 | 119.1 | H19B—C19—H19C | 109.5 |
| C1—C6—C5 | 119.4 (2) | C21—C20—C25 | 120.5 (3) |
| C1—C6—H6 | 120.3 | C21—C20—N6 | 120.2 (2) |
| C5—C6—H6 | 120.3 | C25—C20—N6 | 119.3 (2) |
| N1—C7—N2 | 111.98 (19) | C20—C21—C22 | 118.6 (3) |
| N1—C7—S1 | 127.76 (17) | C20—C21—H21 | 120.7 |
| N2—C7—S1 | 120.26 (16) | C22—C21—H21 | 120.7 |
| N2—C8—C11 | 112.53 (19) | C23—C22—C21 | 121.8 (3) |
| N2—C8—C9 | 101.03 (17) | C23—C22—H22 | 119.1 |
| C11—C8—C9 | 112.35 (18) | C21—C22—H22 | 119.1 |
| N2—C8—H8 | 110.2 | C22—C23—C24 | 117.8 (3) |
| C11—C8—H8 | 110.2 | C22—C23—C26 | 121.3 (4) |
| C9—C8—H8 | 110.2 | C24—C23—C26 | 121.0 (4) |
| C10—C9—C8 | 102.80 (18) | C25—C24—C23 | 121.1 (3) |
| C10—C9—H9A | 111.2 | C25—C24—H24 | 119.4 |
| C8—C9—H9A | 111.2 | C23—C24—H24 | 119.4 |
| C10—C9—H9B | 111.2 | C24—C25—C20 | 120.1 (3) |
| C8—C9—H9B | 111.2 | C24—C25—H25 | 119.9 |
| H9A—C9—H9B | 109.1 | C20—C25—H25 | 119.9 |
| N3—C10—C17 | 120.3 (2) | C23—C26—H26A | 109.5 |
| N3—C10—C9 | 114.3 (2) | C23—C26—H26B | 109.5 |
| C17—C10—C9 | 125.3 (2) | H26A—C26—H26B | 109.5 |
| C12—C11—C16 | 118.8 (2) | C23—C26—H26C | 109.5 |
| C12—C11—C8 | 122.7 (2) | H26A—C26—H26C | 109.5 |
| C16—C11—C8 | 118.5 (2) | H26B—C26—H26C | 109.5 |
| C7—N2—N3—C10 | −168.49 (19) | C11—C12—C13—C14 | −0.8 (4) |
| C8—N2—N3—C10 | 7.2 (2) | C12—C13—C14—C15 | −0.5 (6) |
| C17—N4—N5—N6 | −0.1 (2) | C12—C13—C14—F1 | 179.8 (3) |
| N4—N5—N6—C18 | 0.4 (3) | F1—C14—C15—C16 | −179.6 (3) |
| N4—N5—N6—C20 | −177.4 (2) | C13—C14—C15—C16 | 0.8 (7) |
| C7—N1—C1—C6 | −5.6 (4) | C14—C15—C16—C11 | 0.2 (6) |
| C7—N1—C1—C2 | 172.6 (2) | C12—C11—C16—C15 | −1.4 (4) |
| C6—C1—C2—C3 | 1.1 (3) | C8—C11—C16—C15 | 175.9 (3) |
| N1—C1—C2—C3 | −177.3 (2) | N5—N4—C17—C18 | −0.2 (3) |
| C1—C2—C3—C4 | −0.5 (3) | N5—N4—C17—C10 | 175.68 (19) |
| C2—C3—C4—C5 | −0.1 (4) | N3—C10—C17—N4 | −172.65 (19) |
| C3—C4—C5—C6 | 0.3 (4) | C9—C10—C17—N4 | 3.8 (3) |
| C2—C1—C6—C5 | −0.9 (3) | N3—C10—C17—C18 | 2.3 (3) |
| N1—C1—C6—C5 | 177.3 (2) | C9—C10—C17—C18 | 178.7 (2) |
| C4—C5—C6—C1 | 0.3 (4) | N5—N6—C18—C17 | −0.5 (2) |
| C1—N1—C7—N2 | −170.1 (2) | C20—N6—C18—C17 | 177.1 (2) |
| C1—N1—C7—S1 | 9.8 (4) | N5—N6—C18—C19 | 177.0 (2) |
| N3—N2—C7—N1 | −3.3 (3) | C20—N6—C18—C19 | −5.5 (4) |
| C8—N2—C7—N1 | −178.33 (19) | N4—C17—C18—N6 | 0.4 (2) |
| N3—N2—C7—S1 | 176.78 (15) | C10—C17—C18—N6 | −175.0 (2) |
| C8—N2—C7—S1 | 1.7 (3) | N4—C17—C18—C19 | −176.8 (2) |
| C7—N2—C8—C11 | −75.8 (3) | C10—C17—C18—C19 | 7.8 (4) |
| N3—N2—C8—C11 | 108.8 (2) | C18—N6—C20—C21 | 123.5 (3) |
| C7—N2—C8—C9 | 164.2 (2) | N5—N6—C20—C21 | −59.1 (3) |
| N3—N2—C8—C9 | −11.2 (2) | C18—N6—C20—C25 | −56.8 (4) |
| N2—C8—C9—C10 | 10.3 (2) | N5—N6—C20—C25 | 120.5 (3) |
| C11—C8—C9—C10 | −109.9 (2) | C25—C20—C21—C22 | 0.9 (4) |
| N2—N3—C10—C17 | 177.36 (18) | N6—C20—C21—C22 | −179.5 (3) |
| N2—N3—C10—C9 | 0.6 (2) | C20—C21—C22—C23 | −0.8 (5) |
| C8—C9—C10—N3 | −7.4 (2) | C21—C22—C23—C24 | 0.5 (5) |
| C8—C9—C10—C17 | 175.99 (19) | C21—C22—C23—C26 | −179.8 (3) |
| N2—C8—C11—C12 | −18.8 (3) | C22—C23—C24—C25 | −0.3 (5) |
| C9—C8—C11—C12 | 94.5 (3) | C26—C23—C24—C25 | 180.0 (3) |
| N2—C8—C11—C16 | 164.0 (2) | C23—C24—C25—C20 | 0.4 (6) |
| C9—C8—C11—C16 | −82.8 (3) | C21—C20—C25—C24 | −0.7 (5) |
| C16—C11—C12—C13 | 1.7 (4) | N6—C20—C25—C24 | 179.7 (3) |
| C8—C11—C12—C13 | −175.6 (2) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—H3···N3 | 0.83 (3) | 2.05 (3) | 2.568 (3) | 120 (2) |
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG5303).
References
- Abdel-Wahab, B. F., Abdel-Latif, E., Mohamed, H. A. & Awad, G. E. A. (2012). Eur. J. Med. Chem. 52, 263–268. [DOI] [PubMed]
- Abdel-Wahab, B. F., Mohamed, H. A., Ng, S. W. & Tiekink, E. R. T. (2012). Acta Cryst. E68, o1985. [DOI] [PMC free article] [PubMed]
- Agilent (2011). CrysAlis PRO Agilent Technologies, Yarnton, England.
- Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
- Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.
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/S1600536813008155/hg5303sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813008155/hg5303Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536813008155/hg5303Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report



