Abstract
In the title compound, C18H15N5O2S, a weak intramolecular C—H⋯S hydrogen bond results in a small dihedral angle of 3.71 (9)° between the methylphenyl and triazole rings, which, in turn, form dihedral angles of 80.09 (8) and 77.32 (8)°, respectively, with the benzoxazolone mean plane. In the crystal, N—H⋯O hydrogen bonds link molecules into chains along [001], and weak C—H⋯N hydrogen bonds and π–π interactions between the five- and six-membered rings [centroid–centroid distances = 3.5074 (11) and 3.616 (1) Å] consolidate the crystal packing.
Related literature
For details of the synthesis, see: Urlu-Cicekli et al. (2012 ▶). For related structures, see: Aydın et al. (2005 ▶, 2012 ▶). For a MOPAC AM1 theoretical full-geometry optimization, see: Dewar et al. (1985 ▶); Stewart (1993 ▶).
Experimental
Crystal data
C18H15N5O2S
M r = 365.42
Monoclinic,
a = 18.0823 (13) Å
b = 6.4623 (4) Å
c = 15.1892 (11) Å
β = 100.821 (6)°
V = 1743.4 (2) Å3
Z = 4
Mo Kα radiation
μ = 0.21 mm−1
T = 296 K
0.62 × 0.48 × 0.22 mm
Data collection
Stoe IPDS 2 diffractometer
Absorption correction: integration (X-RED32; Stoe & Cie, 2002 ▶) T min = 0.881, T max = 0.955
10084 measured reflections
3958 independent reflections
3034 reflections with I > 2σ(I)
R int = 0.029
Refinement
R[F 2 > 2σ(F 2)] = 0.042
wR(F 2) = 0.110
S = 1.03
3958 reflections
237 parameters
H-atom parameters constrained
Δρmax = 0.21 e Å−3
Δρmin = −0.27 e Å−3
Data collection: X-AREA (Stoe & Cie, 2002 ▶); cell refinement: X-AREA; data reduction: X-RED32 (Stoe & Cie, 2002 ▶); program(s) used to solve structure: SIR97 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶) and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812051458/cv5375sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812051458/cv5375Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812051458/cv5375Isup3.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 |
|---|---|---|---|---|
| N3—H3A⋯O2i | 0.86 | 2.03 | 2.856 (2) | 162 |
| C4—H4⋯N4ii | 0.93 | 2.52 | 3.387 (3) | 155 |
| C11—H11⋯S1 | 0.93 | 2.48 | 3.2159 (18) | 136 |
Symmetry codes: (i)
; (ii)
.
Acknowledgments
The authors acknowledge the Faculty of Arts and Sciences, Ondokuz Mayıs University, Turkey, for the use of the Stoe IPDS 2 diffractometer (purchased under grant No. F.279 of the University Research Fund).
supplementary crystallographic information
Comment
In continuation of our studies of hybrid molecules containing 2(3H)- benzoxazolone fragment (Aydın et al., 2005), herewith we present the title compound, (I). In (I) (Fig. 1), the 2,3-dihydro-1,3-benzoxazole ring (N1/O1/C1—C7) is essentially planar with the maximum deviation of the C7 atom from the mean plane of -0.034 (2) Å. This ring system makes dihedral angles of 77.32 (8) and 80.09 (8)°, with the 4,5-dihydro-1H-1,2,4-triazole ring (N2–N4/C9/C10) and the benzene ring (C12–C17), respectively. The dihedral angle between the 4,5-dihydro-1H-1,2,4-triazole ring and the benzene ring is 3.71 (9)°. All bond lengths and angles are comparable with those observed in similar compounds (Aydın et al., 2005; 2012).
In the crystal, neighbouring molecules are linked by N—H···O and C—H···N hydrogen bonding interactions, forming a two dimensional network parallel to the (101) plane (Table 1, Fig. 2). In addition, the crystal packing is stabilized by a weak C—H···π interaction and two π-π stacking interactions [Cg1···Cg3(1 - x, -y, -z) = 3.5074 (11) Å and Cg2···Cg4(x, -1 + y,z) = 3.6160 (10) Å; where Cg1, Cg2, Cg3 and Cg4 are the centroids of the O1/C1/C6/N1/C7, N2/C9/N4/N3/C10, C1–C6 and C12–C17 rings, respectively].
Molecular orbital calculations using semi-empirical (AM1) have been carried out for the title compound with MOPAC (Dewar et al., 1985; Stewart, 1993). The values of the structural parameters of the title compound obtained by the results of the theoretical calculations (based on isolated molecules) and X-ray structural determinations in the solid state are almost identical within experimental error. The calculated dipole moment of (I) is 3.243 D. The HOMO and LUMO energy levels are -8.65563 and -.31527 eV, respectively.
Experimental
To a suspension of o-methylbenzaldehyde (0.0022 mol) in glacial acetic acid (3 ml), 0.002 mol [(4-amino-5-sulfanylidene-1,2,4-triazol-3-yl) methyl]-2(3H)-benzoxazolone was added. The reaction mixture was placed in microwave oven and irradiated for minutes changing between 15–30 min at 398 K (300 W). After completion of the reaction by monitoring with TLC, the reaction mixture was kept overnight at room temperature. The precipitate was collected by filtration, washed with water, dried, and crystallized from EtOH-acetone.
Yield, 58%, m.p.: 494–495 K. IR vmax cm-1, 3186, 1772, 1484, 1268. 1H-NMR (DMSO-d6) δ 14.16 (1H, s, NH), 10.28 (1H, s, =CH), 7.84 (1H, d, Ar—H), 7.39 (1H, t, Ar—H), 7.29–7.18 (4H, m, Ar—H, H7, H4), 7.12 (1H, t, H6), 7.06 (1H, t, H5), 5.21 (2H, s, CH2), 2.40 (3H, s, CH3). Elemental analysis: C18H15N5O2S, Calc.(%) / Found (%): C:59.16/59.38, H: 4.14/3.95, N: 19.17/19.15. (Urlu-Cicekli et al., 2012).
Refinement
H atoms were positioned geometrically, with N—H = 0.86 Å, C—H = 0.93(aromatic), 0.97(methylene) and 0.96 Å (methyl), and refined as riding with Uiso(H) = 1.5Ueq(C) for methyl H and 1.2Ueq(C,N) for the others.
Figures
Fig. 1.

The molecule shown with the atom numbering scheme. Displacement ellipsoids for non-H atoms are drawn at the 30% probability level.
Fig. 2.
The packing and hydrogen bonding of the title compound viewed down the b axis. H atoms not involved in hydrogen bondings are omitted for the sake of clarity.
Crystal data
| C18H15N5O2S | F(000) = 760 |
| Mr = 365.42 | Dx = 1.392 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 14230 reflections |
| a = 18.0823 (13) Å | θ = 1.6–28.1° |
| b = 6.4623 (4) Å | µ = 0.21 mm−1 |
| c = 15.1892 (11) Å | T = 296 K |
| β = 100.821 (6)° | Prism, colourless |
| V = 1743.4 (2) Å3 | 0.62 × 0.48 × 0.22 mm |
| Z = 4 |
Data collection
| Stoe IPDS 2 diffractometer | 3958 independent reflections |
| Radiation source: sealed X-ray tube, 12 x 0.4 mm long-fine focus | 3034 reflections with I > 2σ(I) |
| Plane graphite monochromator | Rint = 0.029 |
| Detector resolution: 6.67 pixels mm-1 | θmax = 27.6°, θmin = 2.3° |
| ω scans | h = −23→23 |
| Absorption correction: integration (X-RED32; Stoe & Cie, 2002) | k = −8→8 |
| Tmin = 0.881, Tmax = 0.955 | l = −19→11 |
| 10084 measured reflections |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.042 | H-atom parameters constrained |
| wR(F2) = 0.110 | w = 1/[σ2(Fo2) + (0.0522P)2 + 0.2998P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.03 | (Δ/σ)max < 0.001 |
| 3958 reflections | Δρmax = 0.21 e Å−3 |
| 237 parameters | Δρmin = −0.27 e Å−3 |
| 0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), FC*=KFC[1+0.001XFC2Λ3/SIN(2Θ)]-1/4 |
| Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0052 (11) |
Special details
| Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles |
| Refinement. Refinement on F2 for ALL reflections except those flagged by the user for potential systematic errors. Weighted R-factors wR and all goodnesses of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The observed criterion of F2 > σ(F2) is used only for calculating -R-factor-obs 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 | 0.82101 (3) | 0.21261 (9) | 0.49178 (3) | 0.0661 (2) | |
| O1 | 0.57137 (8) | −0.3003 (2) | 0.04586 (9) | 0.0678 (5) | |
| O2 | 0.69462 (8) | −0.2533 (3) | 0.04013 (11) | 0.0879 (6) | |
| N1 | 0.63001 (7) | −0.0347 (2) | 0.11876 (9) | 0.0488 (4) | |
| N2 | 0.76393 (7) | 0.19558 (19) | 0.30855 (8) | 0.0395 (4) | |
| N3 | 0.73011 (8) | −0.0492 (2) | 0.38509 (9) | 0.0502 (4) | |
| N4 | 0.69353 (8) | −0.0842 (2) | 0.29879 (9) | 0.0506 (4) | |
| N5 | 0.78893 (7) | 0.3744 (2) | 0.27189 (9) | 0.0461 (4) | |
| C1 | 0.51976 (10) | −0.1911 (3) | 0.08396 (12) | 0.0528 (5) | |
| C2 | 0.44430 (11) | −0.2291 (3) | 0.07683 (16) | 0.0697 (7) | |
| C3 | 0.40518 (11) | −0.0913 (4) | 0.11896 (16) | 0.0753 (8) | |
| C4 | 0.43962 (11) | 0.0728 (4) | 0.16624 (15) | 0.0715 (7) | |
| C5 | 0.51655 (10) | 0.1116 (3) | 0.17325 (13) | 0.0599 (6) | |
| C6 | 0.55532 (9) | −0.0251 (3) | 0.13032 (10) | 0.0456 (5) | |
| C7 | 0.63901 (11) | −0.1995 (3) | 0.06662 (12) | 0.0596 (6) | |
| C8 | 0.69017 (9) | 0.1059 (3) | 0.15606 (11) | 0.0529 (5) | |
| C9 | 0.71518 (8) | 0.0672 (2) | 0.25402 (10) | 0.0420 (4) | |
| C10 | 0.77295 (8) | 0.1213 (2) | 0.39537 (10) | 0.0434 (4) | |
| C11 | 0.84178 (9) | 0.4744 (3) | 0.31801 (11) | 0.0505 (5) | |
| C12 | 0.87066 (8) | 0.6636 (2) | 0.28379 (11) | 0.0449 (5) | |
| C13 | 0.85106 (10) | 0.7124 (3) | 0.19330 (12) | 0.0565 (6) | |
| C14 | 0.87728 (12) | 0.8909 (3) | 0.16082 (15) | 0.0698 (8) | |
| C15 | 0.92305 (12) | 1.0222 (3) | 0.21815 (18) | 0.0753 (9) | |
| C16 | 0.94356 (11) | 0.9736 (3) | 0.30694 (17) | 0.0674 (8) | |
| C17 | 0.91832 (9) | 0.7942 (3) | 0.34227 (13) | 0.0529 (6) | |
| C18 | 0.94257 (14) | 0.7470 (4) | 0.44018 (16) | 0.0802 (8) | |
| H2 | 0.42100 | −0.34200 | 0.04520 | 0.0840* | |
| H3 | 0.35370 | −0.11010 | 0.11530 | 0.0900* | |
| H3A | 0.72590 | −0.12990 | 0.42890 | 0.0600* | |
| H4 | 0.41110 | 0.16160 | 0.19460 | 0.0860* | |
| H5 | 0.54000 | 0.22390 | 0.20530 | 0.0720* | |
| H8A | 0.67270 | 0.24760 | 0.14660 | 0.0630* | |
| H8B | 0.73230 | 0.08710 | 0.12570 | 0.0630* | |
| H11 | 0.86300 | 0.42740 | 0.37500 | 0.0610* | |
| H13 | 0.82000 | 0.62380 | 0.15460 | 0.0680* | |
| H14 | 0.86410 | 0.92290 | 0.10020 | 0.0840* | |
| H15 | 0.94010 | 1.14430 | 0.19640 | 0.0900* | |
| H16 | 0.97520 | 1.06280 | 0.34470 | 0.0810* | |
| H18A | 0.98610 | 0.82820 | 0.46430 | 0.1200* | |
| H18B | 0.95470 | 0.60270 | 0.44770 | 0.1200* | |
| H18C | 0.90240 | 0.77980 | 0.47110 | 0.1200* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.0839 (4) | 0.0758 (3) | 0.0346 (2) | −0.0221 (3) | 0.0009 (2) | −0.0032 (2) |
| O1 | 0.0728 (8) | 0.0642 (8) | 0.0609 (8) | 0.0012 (7) | −0.0013 (6) | −0.0295 (7) |
| O2 | 0.0712 (9) | 0.1311 (14) | 0.0591 (9) | 0.0311 (9) | 0.0062 (7) | −0.0369 (9) |
| N1 | 0.0457 (7) | 0.0603 (8) | 0.0389 (7) | −0.0010 (6) | 0.0039 (5) | −0.0145 (6) |
| N2 | 0.0417 (6) | 0.0436 (7) | 0.0328 (6) | −0.0067 (5) | 0.0059 (5) | −0.0014 (5) |
| N3 | 0.0569 (8) | 0.0546 (8) | 0.0386 (7) | −0.0128 (6) | 0.0074 (6) | 0.0046 (6) |
| N4 | 0.0523 (7) | 0.0565 (8) | 0.0421 (7) | −0.0142 (6) | 0.0068 (6) | −0.0025 (6) |
| N5 | 0.0530 (7) | 0.0443 (7) | 0.0399 (7) | −0.0085 (6) | 0.0057 (5) | 0.0031 (6) |
| C1 | 0.0567 (10) | 0.0530 (9) | 0.0448 (9) | −0.0032 (8) | −0.0005 (7) | −0.0062 (7) |
| C2 | 0.0622 (11) | 0.0728 (13) | 0.0676 (13) | −0.0179 (10) | −0.0044 (9) | 0.0032 (10) |
| C3 | 0.0509 (10) | 0.1009 (17) | 0.0711 (14) | −0.0056 (11) | 0.0034 (9) | 0.0198 (12) |
| C4 | 0.0624 (11) | 0.0892 (15) | 0.0650 (12) | 0.0249 (11) | 0.0177 (9) | 0.0078 (11) |
| C5 | 0.0604 (10) | 0.0635 (11) | 0.0539 (10) | 0.0106 (9) | 0.0057 (8) | −0.0113 (9) |
| C6 | 0.0461 (8) | 0.0506 (9) | 0.0375 (8) | 0.0030 (7) | 0.0011 (6) | −0.0051 (6) |
| C7 | 0.0599 (10) | 0.0753 (12) | 0.0400 (9) | 0.0120 (9) | −0.0002 (7) | −0.0175 (8) |
| C8 | 0.0508 (9) | 0.0694 (11) | 0.0367 (8) | −0.0118 (8) | 0.0036 (6) | −0.0021 (7) |
| C9 | 0.0391 (7) | 0.0498 (8) | 0.0368 (7) | −0.0060 (6) | 0.0067 (6) | −0.0036 (6) |
| C10 | 0.0455 (8) | 0.0486 (8) | 0.0363 (7) | −0.0028 (7) | 0.0081 (6) | 0.0003 (6) |
| C11 | 0.0533 (9) | 0.0509 (9) | 0.0434 (8) | −0.0082 (7) | −0.0010 (7) | 0.0060 (7) |
| C12 | 0.0433 (8) | 0.0419 (8) | 0.0495 (9) | −0.0003 (6) | 0.0086 (6) | 0.0042 (6) |
| C13 | 0.0614 (10) | 0.0560 (10) | 0.0519 (10) | −0.0004 (8) | 0.0105 (8) | 0.0082 (8) |
| C14 | 0.0835 (14) | 0.0639 (12) | 0.0674 (13) | 0.0069 (11) | 0.0281 (10) | 0.0218 (10) |
| C15 | 0.0765 (13) | 0.0500 (11) | 0.1094 (19) | −0.0025 (10) | 0.0431 (13) | 0.0200 (12) |
| C16 | 0.0590 (11) | 0.0476 (10) | 0.0968 (17) | −0.0087 (8) | 0.0175 (10) | −0.0044 (10) |
| C17 | 0.0477 (9) | 0.0457 (9) | 0.0638 (11) | −0.0027 (7) | 0.0066 (7) | −0.0027 (8) |
| C18 | 0.0886 (15) | 0.0728 (14) | 0.0678 (14) | −0.0154 (12) | −0.0146 (11) | −0.0060 (11) |
Geometric parameters (Å, º)
| S1—C10 | 1.6643 (15) | C11—C12 | 1.463 (2) |
| O1—C1 | 1.381 (2) | C12—C17 | 1.399 (2) |
| O1—C7 | 1.369 (2) | C12—C13 | 1.390 (2) |
| O2—C7 | 1.202 (3) | C13—C14 | 1.374 (3) |
| N1—C6 | 1.396 (2) | C14—C15 | 1.376 (3) |
| N1—C7 | 1.355 (2) | C15—C16 | 1.367 (4) |
| N1—C8 | 1.449 (2) | C16—C17 | 1.390 (3) |
| N2—N5 | 1.3944 (18) | C17—C18 | 1.501 (3) |
| N2—C9 | 1.3701 (19) | C2—H2 | 0.9300 |
| N2—C10 | 1.3839 (19) | C3—H3 | 0.9300 |
| N3—N4 | 1.3716 (19) | C4—H4 | 0.9300 |
| N3—C10 | 1.3391 (19) | C5—H5 | 0.9300 |
| N4—C9 | 1.2934 (19) | C8—H8A | 0.9700 |
| N5—C11 | 1.253 (2) | C8—H8B | 0.9700 |
| N3—H3A | 0.8600 | C11—H11 | 0.9300 |
| C1—C6 | 1.375 (3) | C13—H13 | 0.9300 |
| C1—C2 | 1.371 (3) | C14—H14 | 0.9300 |
| C2—C3 | 1.369 (3) | C15—H15 | 0.9300 |
| C3—C4 | 1.364 (3) | C16—H16 | 0.9300 |
| C4—C5 | 1.398 (3) | C18—H18A | 0.9600 |
| C5—C6 | 1.367 (3) | C18—H18B | 0.9600 |
| C8—C9 | 1.493 (2) | C18—H18C | 0.9600 |
| C1—O1—C7 | 107.77 (14) | C12—C13—C14 | 120.31 (17) |
| C6—N1—C7 | 109.49 (14) | C13—C14—C15 | 119.9 (2) |
| C6—N1—C8 | 126.61 (14) | C14—C15—C16 | 120.17 (19) |
| C7—N1—C8 | 123.90 (14) | C15—C16—C17 | 121.7 (2) |
| N5—N2—C9 | 118.71 (12) | C16—C17—C18 | 119.74 (19) |
| N5—N2—C10 | 132.76 (12) | C12—C17—C16 | 117.77 (18) |
| C9—N2—C10 | 108.26 (12) | C12—C17—C18 | 122.50 (18) |
| N4—N3—C10 | 114.32 (13) | C1—C2—H2 | 122.00 |
| N3—N4—C9 | 103.80 (13) | C3—C2—H2 | 122.00 |
| N2—N5—C11 | 118.33 (14) | C2—C3—H3 | 119.00 |
| N4—N3—H3A | 123.00 | C4—C3—H3 | 119.00 |
| C10—N3—H3A | 123.00 | C3—C4—H4 | 119.00 |
| C2—C1—C6 | 122.91 (18) | C5—C4—H4 | 119.00 |
| O1—C1—C6 | 109.00 (15) | C4—C5—H5 | 122.00 |
| O1—C1—C2 | 128.06 (18) | C6—C5—H5 | 122.00 |
| C1—C2—C3 | 116.16 (19) | N1—C8—H8A | 110.00 |
| C2—C3—C4 | 121.81 (19) | N1—C8—H8B | 110.00 |
| C3—C4—C5 | 121.9 (2) | C9—C8—H8A | 110.00 |
| C4—C5—C6 | 116.10 (18) | C9—C8—H8B | 110.00 |
| N1—C6—C5 | 133.14 (17) | H8A—C8—H8B | 108.00 |
| N1—C6—C1 | 105.75 (15) | N5—C11—H11 | 119.00 |
| C1—C6—C5 | 121.07 (16) | C12—C11—H11 | 119.00 |
| O1—C7—N1 | 107.96 (16) | C12—C13—H13 | 120.00 |
| O2—C7—N1 | 128.50 (19) | C14—C13—H13 | 120.00 |
| O1—C7—O2 | 123.53 (18) | C13—C14—H14 | 120.00 |
| N1—C8—C9 | 110.46 (14) | C15—C14—H14 | 120.00 |
| N2—C9—C8 | 122.77 (13) | C14—C15—H15 | 120.00 |
| N2—C9—N4 | 111.35 (13) | C16—C15—H15 | 120.00 |
| N4—C9—C8 | 125.86 (14) | C15—C16—H16 | 119.00 |
| N2—C10—N3 | 102.25 (12) | C17—C16—H16 | 119.00 |
| S1—C10—N3 | 126.12 (12) | C17—C18—H18A | 109.00 |
| S1—C10—N2 | 131.61 (11) | C17—C18—H18B | 109.00 |
| N5—C11—C12 | 121.20 (15) | C17—C18—H18C | 109.00 |
| C13—C12—C17 | 120.23 (15) | H18A—C18—H18B | 109.00 |
| C11—C12—C13 | 119.96 (14) | H18A—C18—H18C | 110.00 |
| C11—C12—C17 | 119.81 (15) | H18B—C18—H18C | 109.00 |
| C7—O1—C1—C2 | 176.4 (2) | N3—N4—C9—N2 | 0.12 (17) |
| C7—O1—C1—C6 | −1.5 (2) | N2—N5—C11—C12 | −179.86 (14) |
| C1—O1—C7—O2 | −177.25 (19) | C2—C1—C6—C5 | 0.7 (3) |
| C1—O1—C7—N1 | 1.76 (19) | C2—C1—C6—N1 | −177.42 (18) |
| C7—N1—C6—C1 | 0.53 (19) | O1—C1—C2—C3 | −177.6 (2) |
| C8—N1—C6—C1 | −179.11 (15) | C6—C1—C2—C3 | −0.1 (3) |
| C6—N1—C7—O1 | −1.43 (19) | O1—C1—C6—N1 | 0.57 (19) |
| C8—N1—C7—O2 | −2.8 (3) | O1—C1—C6—C5 | 178.73 (16) |
| C8—N1—C7—O1 | 178.22 (14) | C1—C2—C3—C4 | −0.8 (3) |
| C6—N1—C7—O2 | 177.5 (2) | C2—C3—C4—C5 | 1.0 (4) |
| C8—N1—C6—C5 | 3.1 (3) | C3—C4—C5—C6 | −0.3 (3) |
| C6—N1—C8—C9 | 74.0 (2) | C4—C5—C6—C1 | −0.5 (3) |
| C7—N1—C8—C9 | −105.58 (18) | C4—C5—C6—N1 | 177.04 (19) |
| C7—N1—C6—C5 | −177.31 (19) | N1—C8—C9—N4 | 7.5 (2) |
| C9—N2—N5—C11 | −169.40 (15) | N1—C8—C9—N2 | −170.82 (13) |
| C9—N2—C10—S1 | −176.79 (12) | N5—C11—C12—C13 | −13.5 (2) |
| N5—N2—C10—S1 | −3.0 (3) | N5—C11—C12—C17 | 166.92 (16) |
| C10—N2—C9—C8 | 177.50 (14) | C11—C12—C13—C14 | 179.29 (17) |
| N5—N2—C9—N4 | −175.91 (13) | C17—C12—C13—C14 | −1.1 (3) |
| C10—N2—N5—C11 | 17.3 (2) | C11—C12—C17—C16 | −179.17 (16) |
| C9—N2—C10—N3 | 1.52 (15) | C11—C12—C17—C18 | 0.9 (3) |
| C10—N2—C9—N4 | −1.08 (17) | C13—C12—C17—C16 | 1.2 (2) |
| N5—N2—C10—N3 | 175.34 (15) | C13—C12—C17—C18 | −178.74 (18) |
| N5—N2—C9—C8 | 2.7 (2) | C12—C13—C14—C15 | −0.1 (3) |
| C10—N3—N4—C9 | 0.95 (18) | C13—C14—C15—C16 | 1.2 (3) |
| N4—N3—C10—N2 | −1.55 (17) | C14—C15—C16—C17 | −1.1 (3) |
| N4—N3—C10—S1 | 176.89 (11) | C15—C16—C17—C12 | −0.2 (3) |
| N3—N4—C9—C8 | −178.40 (15) | C15—C16—C17—C18 | 179.8 (2) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N3—H3A···O2i | 0.86 | 2.03 | 2.856 (2) | 162 |
| C4—H4···N4ii | 0.93 | 2.52 | 3.387 (3) | 155 |
| C8—H8B···O2 | 0.97 | 2.58 | 2.924 (3) | 101 |
| C11—H11···S1 | 0.93 | 2.48 | 3.2159 (18) | 136 |
| C3—H3···Cg2iii | 0.93 | 2.94 | 3.635 (2) | 132 |
Symmetry codes: (i) x, −y−1/2, z+1/2; (ii) −x+1, y+1/2, −z+1/2; (iii) −x+1, y−1/2, −z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CV5375).
References
- Altomare, A., Burla, M. C., Camalli, M., Cascarano, G. L., Giacovazzo, C., Guagliardi, A., Moliterni, A. G. G., Polidori, G. & Spagna, R. (1999). J. Appl. Cryst. 32, 115–119.
- Aydın, A., Önkol, T., Akkurt, M. & Büyükgüngör, O. (2005). Anal. Sci. 21, x119–x120.
- Aydın, A., Soyer, Z., Akkurt, M. & Büyükgüngör, O. (2012). Acta Cryst. E68, o1544–o1545. [DOI] [PMC free article] [PubMed]
- Dewar, M. J. S., Zoebish, E. G., Healy, E. F. & Stewart, J. J. P. (1985). J. Am. Chem. Soc. 107, 3902–3909.
- Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
- Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837–838.
- Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
- Spek, A. L. (2009). Acta Cryst. D65, 148–155. [DOI] [PMC free article] [PubMed]
- Stewart, J. J. P. (1993). MOPAC7.0 QCPE Program No. 455. Quantum Chemistry Program Exchange, Department of Chemistry, Indiana University, Bloomington, IN, USA.
- Stoe & Cie (2002). X-AREA and X-RED32 Stoe & Cie, Darmstadt, Germany.
- Urlu-Cicekli, S., Onkol, T., Ozgen, S. & Sahin, M. F. (2012). Rev. Roum. Chim. 57, 187–195.
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/S1600536812051458/cv5375sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812051458/cv5375Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812051458/cv5375Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

