Abstract
In the title compound, C16H22N2OS2, the S atom of the thiadiazole ring and the attached methyl groups are disordered over two orientations with a refined site-occupancy ratio of 0.641 (11):0.359 (11). The thiadiazole ring is in a twist conformation in both disorder components. The mean plane through the thiadiazole ring makes dihedral angles of 77.39 (8) (major component) and 67.45 (11)° (minor component) with the benzene ring. Intramolecular C—H⋯N interactions generate two S(6) ring motifs. In the crystal, molecules are linked by C—H⋯O hydrogen bonds into zigzag chains parallel to the b axis.
Related literature
For background to the pharmacological properties of thiadiazole derivatives, see: Noolvi et al. (2011 ▶); Yusuf et al. (2008 ▶). For a related structure, see: Fun et al. (2011 ▶). For hydrogen-bond motifs, see: Bernstein et al. (1995 ▶). For the stability of the temperature controller used in the data collection, see: Cosier & Glazer (1986 ▶). For ring conformations, see: Cremer & Pople (1975 ▶).
Experimental
Crystal data
C16H22N2OS2
M r = 322.48
Monoclinic,
a = 16.6174 (2) Å
b = 10.5178 (1) Å
c = 9.6758 (1) Å
β = 96.345 (1)°
V = 1680.76 (3) Å3
Z = 4
Mo Kα radiation
μ = 0.32 mm−1
T = 100 K
0.26 × 0.19 × 0.12 mm
Data collection
Bruker SMART APEXII CCD area-detector diffractometer
Absorption correction: multi-scan (SADABS; Bruker, 2009 ▶) T min = 0.922, T max = 0.962
22216 measured reflections
5972 independent reflections
4678 reflections with I > 2σ(I)
R int = 0.033
Refinement
R[F 2 > 2σ(F 2)] = 0.039
wR(F 2) = 0.092
S = 1.02
5972 reflections
225 parameters
H-atom parameters constrained
Δρmax = 0.38 e Å−3
Δρmin = −0.25 e Å−3
Data collection: APEX2 (Bruker, 2009 ▶); cell refinement: SAINT (Bruker, 2009 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009 ▶).
Supplementary Material
Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812012639/rz2718sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812012639/rz2718Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812012639/rz2718Isup3.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 |
|---|---|---|---|---|
| C14—H14B⋯N1 | 0.98 | 2.36 | 2.9893 (15) | 122 |
| C15—H15B⋯N1 | 0.98 | 2.37 | 2.9803 (15) | 120 |
| C11—H11B⋯O1i | 0.98 | 2.56 | 3.490 (4) | 159 |
Symmetry code: (i)
.
Acknowledgments
The authors thank the Malaysian Government, Universiti Malaysia Terengganu and Universiti Sains Malaysia for research facilities and the Fundamental Research Grant Scheme (FRGS) Nos. 203/PFIZIK/6711171 and FRGS 59166 to conduct this work.
supplementary crystallographic information
Comment
Thiadiazole derivatives have been reported to posses anti-cancer (Noolvi et al., 2011) and anti-depressant activity (Yusuf et al., 2008). The title compound is one of these thiadiazole derivatives, and its crystal structure is reported herein.
In the molecule of the title compound (Fig. 1), the S atom of the thiadiazole ring and the attached dimethyl groups (C10/C10X and C11/C11X) are disordered over two orientations with a refined site-occupancy ratio of 0.641 (11):0.359 (11). The disordered thiadiazole (S1/N1/N2/C8/C9 and S1X/N1/N2/C8/C9) rings are both in twist conformation (Cremer & Pople, 1975) in which the ring is twisted about the C9–S1 bond [puckering parameters: Q = 0.1477 (19) Å and φ= 167.7 (5)°] and about the S1X–C8 bond [puckering parameters: Q = 0.131 (2) Å and φ= 298.6 (8)°], respectively. The mean plane through the thiadiazole rings make dihedral angles of 77.39 (8) and 67.45 (11)°, respectively, with the benzene (C1–C6) ring. Intramolecular C14—H14B···N1 and C15—H15B···N1 interactions (Table 1) generate two S(6) ring motifs (Bernstein et al., 1995). The bond lengths and angles are within normal ranges and are comparable to those reported in a related structure (Fun et al., 2011). The crystal packing is shown in Fig. 2. Intermolecular C11—H11B···O1 (Table 1) hydrogen bonds link the molecules into one dimensional zigzag chains parallel to the b axis.
Experimental
A solution of pivaloylisothiocyanate (1.0 g, 8 mmol) in 30 ml acetone was added into a flask containing 30 ml acetone solution of s-benzyldithiocarbazate (1.5 g, 8.00 mmol). The mixture was refluxed for 4 h, then, the solution was filtered-off and left to evaporate at room temperature. Colourless crystals suitable for X-ray analyisis were obtained after one day on slow evaporation of the solvent (yield 60%, M.p. 503.5–504.5 K, IR(KBr)cm-1: 1334.72 (νC—N), 1547.95 (νC═N), 1647.08 (νC═O), 8944.79 (νC—S). 1H NMR (CDCl3)δp.p.m. 1.289 (s, 9H, -(CH3)3), 2.004 (s, 6H, -(CH3)2), 4.330 (s, 2H, –CH2), 7.35–7.45 (m, 2H, ar-H). 13C NMR (CDCl3)δp.p.m. 127.86–135.40 (6 C, ar-C), 144.57 (thiadiazole carbon), 176.72 (C═O), 27.06–37.50(4 C, –C-(CH3)3). Anal. Found (calc.) for C16H22N2OS2 (%): C, 59.59(58.98); H, 6.88(6.86); N, 8.69(8.66); S, 19.89(19.86).
Refinement
The S atom of the thiadiazole ring and the attached dimethyl groups (C10/C10X) and C11/C11X) are disordered over two orientations with a refined site-occupancy ratio of 0.641 (11):0.359 (11). All H atoms were positioned geometrically [C–H = 0.95–0.99 Å] and refined using a riding model with Uiso(H) = 1.2 or 1.5 Ueq(C). A rotating group model was applied to the methyl groups.
Figures
Fig. 1.
The molecular structure of the title compound with 30% probability displacement ellipsoids. Dashed lines indicate intramolecular hydrogen bonds. Bonds involving the minor component of the disorder are shown as empty sticks.
Fig. 2.
The crystal packing of the title compound viewed along the c axis. The H atoms not involved in the intermolecular interactions (dashed lines) are omitted for clarity. Only major disordered components are shown.
Crystal data
| C16H22N2OS2 | F(000) = 688 |
| Mr = 322.48 | Dx = 1.274 Mg m−3 |
| Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -P 2ybc | Cell parameters from 6904 reflections |
| a = 16.6174 (2) Å | θ = 2.9–32.3° |
| b = 10.5178 (1) Å | µ = 0.32 mm−1 |
| c = 9.6758 (1) Å | T = 100 K |
| β = 96.345 (1)° | Block, colourless |
| V = 1680.76 (3) Å3 | 0.26 × 0.19 × 0.12 mm |
| Z = 4 |
Data collection
| Bruker SMART APEXII CCD area-detector diffractometer | 5972 independent reflections |
| Radiation source: fine-focus sealed tube | 4678 reflections with I > 2σ(I) |
| Graphite monochromator | Rint = 0.033 |
| φ and ω scans | θmax = 32.4°, θmin = 2.3° |
| Absorption correction: multi-scan (SADABS; Bruker, 2009) | h = −25→13 |
| Tmin = 0.922, Tmax = 0.962 | k = −15→15 |
| 22216 measured reflections | l = −12→14 |
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)] = 0.039 | Hydrogen site location: inferred from neighbouring sites |
| wR(F2) = 0.092 | H-atom parameters constrained |
| S = 1.02 | w = 1/[σ2(Fo2) + (0.0355P)2 + 0.5012P] where P = (Fo2 + 2Fc2)/3 |
| 5972 reflections | (Δ/σ)max = 0.001 |
| 225 parameters | Δρmax = 0.38 e Å−3 |
| 0 restraints | Δρmin = −0.25 e Å−3 |
Special details
| Experimental. The crystal was placed in the cold stream of an Oxford Cryosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K. |
| 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 | Occ. (<1) | |
| S1 | 0.36774 (15) | 0.26997 (19) | 0.2500 (3) | 0.0233 (4) | 0.641 (11) |
| S1X | 0.3827 (2) | 0.28188 (18) | 0.2089 (6) | 0.0216 (6) | 0.359 (11) |
| S2 | 0.214397 (18) | 0.34659 (3) | 0.07503 (3) | 0.01843 (7) | |
| O1 | 0.41502 (5) | −0.14077 (8) | 0.14798 (9) | 0.02125 (18) | |
| N1 | 0.28175 (6) | 0.11644 (9) | 0.08318 (10) | 0.01500 (18) | |
| N2 | 0.34822 (6) | 0.04481 (9) | 0.13754 (10) | 0.01761 (19) | |
| C1 | 0.09412 (8) | 0.41815 (12) | −0.21819 (12) | 0.0227 (2) | |
| H1A | 0.1467 | 0.4243 | −0.2475 | 0.027* | |
| C2 | 0.03192 (8) | 0.49319 (13) | −0.28083 (14) | 0.0279 (3) | |
| H2A | 0.0420 | 0.5505 | −0.3528 | 0.033* | |
| C3 | −0.04488 (8) | 0.48490 (12) | −0.23872 (14) | 0.0250 (3) | |
| H3A | −0.0875 | 0.5360 | −0.2822 | 0.030* | |
| C4 | −0.05940 (7) | 0.40174 (11) | −0.13292 (13) | 0.0223 (2) | |
| H4A | −0.1120 | 0.3961 | −0.1036 | 0.027* | |
| C5 | 0.00308 (7) | 0.32658 (11) | −0.06983 (12) | 0.0193 (2) | |
| H5A | −0.0070 | 0.2701 | 0.0029 | 0.023* | |
| C6 | 0.08002 (7) | 0.33358 (10) | −0.11244 (11) | 0.0166 (2) | |
| C7 | 0.14763 (7) | 0.25122 (11) | −0.04636 (12) | 0.0183 (2) | |
| H7A | 0.1786 | 0.2155 | −0.1190 | 0.022* | |
| H7B | 0.1250 | 0.1798 | 0.0036 | 0.022* | |
| C8 | 0.28772 (7) | 0.23196 (10) | 0.12453 (11) | 0.0161 (2) | |
| C9 | 0.41461 (7) | 0.11385 (10) | 0.22346 (11) | 0.0159 (2) | |
| C10 | 0.4419 (3) | 0.0577 (4) | 0.3624 (4) | 0.0267 (7) | 0.641 (11) |
| H10A | 0.4695 | −0.0232 | 0.3500 | 0.040* | 0.641 (11) |
| H10B | 0.3949 | 0.0431 | 0.4131 | 0.040* | 0.641 (11) |
| H10C | 0.4794 | 0.1165 | 0.4153 | 0.040* | 0.641 (11) |
| C10X | 0.4118 (6) | 0.0686 (8) | 0.3771 (8) | 0.0296 (14) | 0.359 (11) |
| H10D | 0.4294 | −0.0202 | 0.3860 | 0.044* | 0.359 (11) |
| H10E | 0.3563 | 0.0760 | 0.4016 | 0.044* | 0.359 (11) |
| H10F | 0.4479 | 0.1218 | 0.4397 | 0.044* | 0.359 (11) |
| C11 | 0.4847 (2) | 0.1317 (4) | 0.1339 (4) | 0.0252 (7) | 0.641 (11) |
| H11A | 0.5099 | 0.0491 | 0.1195 | 0.038* | 0.641 (11) |
| H11B | 0.5251 | 0.1892 | 0.1814 | 0.038* | 0.641 (11) |
| H11C | 0.4639 | 0.1680 | 0.0438 | 0.038* | 0.641 (11) |
| C11X | 0.4988 (4) | 0.1030 (7) | 0.1826 (10) | 0.0275 (14) | 0.359 (11) |
| H11D | 0.5184 | 0.0158 | 0.1986 | 0.041* | 0.359 (11) |
| H11E | 0.5346 | 0.1620 | 0.2385 | 0.041* | 0.359 (11) |
| H11F | 0.4983 | 0.1242 | 0.0839 | 0.041* | 0.359 (11) |
| C12 | 0.35519 (7) | −0.08096 (10) | 0.10018 (11) | 0.0146 (2) | |
| C13 | 0.28826 (7) | −0.14282 (10) | −0.00111 (11) | 0.0147 (2) | |
| C14 | 0.28175 (7) | −0.07640 (11) | −0.14377 (11) | 0.0178 (2) | |
| H14A | 0.3346 | −0.0783 | −0.1799 | 0.027* | |
| H14B | 0.2648 | 0.0120 | −0.1336 | 0.027* | |
| H14C | 0.2417 | −0.1207 | −0.2086 | 0.027* | |
| C15 | 0.20567 (7) | −0.14025 (11) | 0.05629 (12) | 0.0202 (2) | |
| H15A | 0.1667 | −0.1908 | −0.0041 | 0.030* | |
| H15B | 0.1865 | −0.0523 | 0.0592 | 0.030* | |
| H15C | 0.2112 | −0.1760 | 0.1504 | 0.030* | |
| C16 | 0.31270 (8) | −0.28173 (10) | −0.02075 (13) | 0.0210 (2) | |
| H16A | 0.3649 | −0.2846 | −0.0588 | 0.031* | |
| H16B | 0.2715 | −0.3239 | −0.0852 | 0.031* | |
| H16C | 0.3173 | −0.3255 | 0.0692 | 0.031* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.0205 (5) | 0.0179 (4) | 0.0287 (7) | 0.0056 (3) | −0.0097 (5) | −0.0087 (4) |
| S1X | 0.0196 (8) | 0.0125 (4) | 0.0302 (13) | −0.0001 (4) | −0.0078 (8) | −0.0024 (6) |
| S2 | 0.01715 (14) | 0.01447 (12) | 0.02242 (14) | 0.00448 (10) | −0.00341 (11) | −0.00322 (10) |
| O1 | 0.0199 (4) | 0.0168 (4) | 0.0253 (4) | 0.0047 (3) | −0.0053 (3) | −0.0004 (3) |
| N1 | 0.0120 (4) | 0.0150 (4) | 0.0175 (4) | 0.0024 (3) | −0.0007 (3) | 0.0005 (3) |
| N2 | 0.0152 (5) | 0.0142 (4) | 0.0215 (5) | 0.0033 (3) | −0.0065 (4) | −0.0029 (3) |
| C1 | 0.0196 (6) | 0.0273 (6) | 0.0219 (6) | 0.0068 (5) | 0.0048 (5) | 0.0048 (5) |
| C2 | 0.0276 (7) | 0.0321 (7) | 0.0243 (6) | 0.0092 (5) | 0.0042 (5) | 0.0108 (5) |
| C3 | 0.0204 (6) | 0.0257 (6) | 0.0277 (6) | 0.0078 (5) | −0.0030 (5) | 0.0033 (5) |
| C4 | 0.0147 (5) | 0.0203 (5) | 0.0314 (6) | 0.0012 (4) | 0.0002 (5) | −0.0008 (5) |
| C5 | 0.0177 (6) | 0.0171 (5) | 0.0227 (5) | −0.0007 (4) | 0.0003 (4) | 0.0007 (4) |
| C6 | 0.0167 (5) | 0.0152 (5) | 0.0168 (5) | 0.0029 (4) | −0.0024 (4) | −0.0018 (4) |
| C7 | 0.0169 (5) | 0.0163 (5) | 0.0204 (5) | 0.0027 (4) | −0.0037 (4) | −0.0021 (4) |
| C8 | 0.0149 (5) | 0.0157 (5) | 0.0171 (5) | 0.0023 (4) | −0.0013 (4) | −0.0013 (4) |
| C9 | 0.0143 (5) | 0.0144 (4) | 0.0180 (5) | 0.0018 (4) | −0.0029 (4) | −0.0025 (4) |
| C10 | 0.037 (2) | 0.0245 (11) | 0.0163 (13) | −0.0004 (14) | −0.0060 (14) | −0.0003 (9) |
| C10X | 0.043 (4) | 0.025 (2) | 0.020 (2) | −0.009 (3) | 0.001 (3) | 0.0002 (17) |
| C11 | 0.0236 (14) | 0.0246 (14) | 0.0280 (16) | −0.0058 (10) | 0.0061 (12) | −0.0046 (11) |
| C11X | 0.020 (2) | 0.024 (2) | 0.040 (4) | −0.0046 (18) | 0.007 (2) | −0.010 (2) |
| C12 | 0.0162 (5) | 0.0134 (4) | 0.0142 (5) | 0.0011 (4) | 0.0018 (4) | 0.0008 (4) |
| C13 | 0.0153 (5) | 0.0136 (4) | 0.0149 (5) | −0.0005 (4) | 0.0007 (4) | −0.0004 (4) |
| C14 | 0.0199 (6) | 0.0182 (5) | 0.0147 (5) | −0.0004 (4) | −0.0004 (4) | −0.0001 (4) |
| C15 | 0.0178 (6) | 0.0202 (5) | 0.0229 (5) | −0.0037 (4) | 0.0043 (5) | −0.0005 (4) |
| C16 | 0.0258 (6) | 0.0142 (5) | 0.0223 (5) | 0.0004 (4) | −0.0004 (5) | −0.0015 (4) |
Geometric parameters (Å, º)
| S1—C8 | 1.7448 (16) | C9—C11 | 1.539 (3) |
| S1—C9 | 1.8473 (15) | C9—C10X | 1.566 (8) |
| S1X—C8 | 1.774 (2) | C10—H10A | 0.9800 |
| S1X—C9 | 1.846 (2) | C10—H10B | 0.9800 |
| S2—C8 | 1.7432 (11) | C10—H10C | 0.9800 |
| S2—C7 | 1.8245 (12) | C10X—H10D | 0.9800 |
| O1—C12 | 1.2233 (13) | C10X—H10E | 0.9800 |
| N1—C8 | 1.2795 (14) | C10X—H10F | 0.9800 |
| N1—N2 | 1.3913 (13) | C11—H11A | 0.9800 |
| N2—C12 | 1.3796 (14) | C11—H11B | 0.9800 |
| N2—C9 | 1.4942 (14) | C11—H11C | 0.9800 |
| C1—C2 | 1.3857 (17) | C11X—H11D | 0.9800 |
| C1—C6 | 1.3950 (16) | C11X—H11E | 0.9800 |
| C1—H1A | 0.9500 | C11X—H11F | 0.9800 |
| C2—C3 | 1.3847 (18) | C12—C13 | 1.5428 (15) |
| C2—H2A | 0.9500 | C13—C16 | 1.5339 (15) |
| C3—C4 | 1.3878 (18) | C13—C15 | 1.5365 (16) |
| C3—H3A | 0.9500 | C13—C14 | 1.5401 (15) |
| C4—C5 | 1.3912 (17) | C14—H14A | 0.9800 |
| C4—H4A | 0.9500 | C14—H14B | 0.9800 |
| C5—C6 | 1.3880 (16) | C14—H14C | 0.9800 |
| C5—H5A | 0.9500 | C15—H15A | 0.9800 |
| C6—C7 | 1.5042 (16) | C15—H15B | 0.9800 |
| C7—H7A | 0.9900 | C15—H15C | 0.9800 |
| C7—H7B | 0.9900 | C16—H16A | 0.9800 |
| C9—C10 | 1.492 (4) | C16—H16B | 0.9800 |
| C9—C11X | 1.499 (6) | C16—H16C | 0.9800 |
| C8—S1—C9 | 90.02 (7) | C11X—C9—S1 | 121.6 (2) |
| C8—S1X—C9 | 89.16 (10) | C11—C9—S1 | 109.09 (13) |
| C8—S2—C7 | 98.83 (5) | C10X—C9—S1 | 94.7 (3) |
| C8—N1—N2 | 111.41 (9) | C9—C10—H10A | 109.5 |
| C12—N2—N1 | 120.42 (9) | C9—C10—H10B | 109.5 |
| C12—N2—C9 | 122.25 (9) | C9—C10—H10C | 109.5 |
| N1—N2—C9 | 116.98 (8) | C9—C10X—H10D | 109.5 |
| C2—C1—C6 | 120.42 (12) | C9—C10X—H10E | 109.5 |
| C2—C1—H1A | 119.8 | H10D—C10X—H10E | 109.5 |
| C6—C1—H1A | 119.8 | C9—C10X—H10F | 109.5 |
| C3—C2—C1 | 120.18 (12) | H10D—C10X—H10F | 109.5 |
| C3—C2—H2A | 119.9 | H10E—C10X—H10F | 109.5 |
| C1—C2—H2A | 119.9 | C9—C11—H11A | 109.5 |
| C2—C3—C4 | 119.85 (11) | C9—C11—H11B | 109.5 |
| C2—C3—H3A | 120.1 | C9—C11—H11C | 109.5 |
| C4—C3—H3A | 120.1 | C9—C11X—H11D | 109.5 |
| C3—C4—C5 | 119.98 (12) | C9—C11X—H11E | 109.5 |
| C3—C4—H4A | 120.0 | H11D—C11X—H11E | 109.5 |
| C5—C4—H4A | 120.0 | C9—C11X—H11F | 109.5 |
| C6—C5—C4 | 120.45 (11) | H11D—C11X—H11F | 109.5 |
| C6—C5—H5A | 119.8 | H11E—C11X—H11F | 109.5 |
| C4—C5—H5A | 119.8 | O1—C12—N2 | 118.84 (10) |
| C5—C6—C1 | 119.12 (11) | O1—C12—C13 | 121.47 (9) |
| C5—C6—C7 | 120.83 (10) | N2—C12—C13 | 119.69 (9) |
| C1—C6—C7 | 120.06 (11) | C16—C13—C15 | 108.72 (9) |
| C6—C7—S2 | 109.24 (8) | C16—C13—C14 | 108.32 (9) |
| C6—C7—H7A | 109.8 | C15—C13—C14 | 109.81 (9) |
| S2—C7—H7A | 109.8 | C16—C13—C12 | 107.35 (9) |
| C6—C7—H7B | 109.8 | C15—C13—C12 | 111.90 (9) |
| S2—C7—H7B | 109.8 | C14—C13—C12 | 110.64 (9) |
| H7A—C7—H7B | 108.3 | C13—C14—H14A | 109.5 |
| N1—C8—S2 | 122.90 (9) | C13—C14—H14B | 109.5 |
| N1—C8—S1 | 117.51 (10) | H14A—C14—H14B | 109.5 |
| S2—C8—S1 | 119.24 (7) | C13—C14—H14C | 109.5 |
| N1—C8—S1X | 117.33 (12) | H14A—C14—H14C | 109.5 |
| S2—C8—S1X | 118.74 (9) | H14B—C14—H14C | 109.5 |
| C10—C9—N2 | 116.2 (2) | C13—C15—H15A | 109.5 |
| C10—C9—C11X | 90.4 (3) | C13—C15—H15B | 109.5 |
| N2—C9—C11X | 118.0 (3) | H15A—C15—H15B | 109.5 |
| C10—C9—C11 | 112.43 (18) | C13—C15—H15C | 109.5 |
| N2—C9—C11 | 107.73 (16) | H15A—C15—H15C | 109.5 |
| N2—C9—C10X | 106.4 (3) | H15B—C15—H15C | 109.5 |
| C11X—C9—C10X | 110.7 (3) | C13—C16—H16A | 109.5 |
| N2—C9—S1X | 103.56 (9) | C13—C16—H16B | 109.5 |
| C11X—C9—S1X | 108.7 (2) | H16A—C16—H16B | 109.5 |
| C10X—C9—S1X | 109.0 (3) | C13—C16—H16C | 109.5 |
| C10—C9—S1 | 108.51 (15) | H16A—C16—H16C | 109.5 |
| N2—C9—S1 | 102.27 (8) | H16B—C16—H16C | 109.5 |
| C8—N1—N2—C12 | −176.95 (10) | N1—N2—C9—C11 | −103.8 (2) |
| C8—N1—N2—C9 | −3.69 (13) | C12—N2—C9—C10X | −77.1 (4) |
| C6—C1—C2—C3 | 0.1 (2) | N1—N2—C9—C10X | 109.8 (4) |
| C1—C2—C3—C4 | 0.4 (2) | C12—N2—C9—S1X | 168.1 (2) |
| C2—C3—C4—C5 | −0.26 (19) | N1—N2—C9—S1X | −5.0 (3) |
| C3—C4—C5—C6 | −0.34 (18) | C12—N2—C9—S1 | −175.75 (17) |
| C4—C5—C6—C1 | 0.79 (17) | N1—N2—C9—S1 | 11.12 (18) |
| C4—C5—C6—C7 | −179.04 (11) | C8—S1X—C9—C10 | −123.1 (4) |
| C2—C1—C6—C5 | −0.66 (18) | C8—S1X—C9—N2 | 8.7 (3) |
| C2—C1—C6—C7 | 179.17 (12) | C8—S1X—C9—C11X | 135.0 (5) |
| C5—C6—C7—S2 | −103.10 (11) | C8—S1X—C9—C11 | 118.0 (4) |
| C1—C6—C7—S2 | 77.07 (12) | C8—S1X—C9—C10X | −104.3 (5) |
| C8—S2—C7—C6 | −176.36 (8) | C8—S1X—C9—S1 | −78.5 (3) |
| N2—N1—C8—S2 | 179.94 (8) | C8—S1—C9—C10 | −134.8 (3) |
| N2—N1—C8—S1 | −7.0 (2) | C8—S1—C9—N2 | −11.51 (19) |
| N2—N1—C8—S1X | 11.7 (3) | C8—S1—C9—C11X | 122.7 (5) |
| C7—S2—C8—N1 | −4.34 (11) | C8—S1—C9—C11 | 102.4 (3) |
| C7—S2—C8—S1 | −177.32 (18) | C8—S1—C9—C10X | −119.5 (4) |
| C7—S2—C8—S1X | 163.8 (3) | C8—S1—C9—S1X | 84.9 (3) |
| C9—S1—C8—N1 | 11.8 (2) | N1—N2—C12—O1 | 178.79 (10) |
| C9—S1—C8—S2 | −174.86 (9) | C9—N2—C12—O1 | 5.89 (16) |
| C9—S1—C8—S1X | −81.9 (3) | N1—N2—C12—C13 | −0.76 (15) |
| C9—S1X—C8—N1 | −12.7 (3) | C9—N2—C12—C13 | −173.67 (9) |
| C9—S1X—C8—S2 | 178.57 (12) | O1—C12—C13—C16 | 1.05 (14) |
| C9—S1X—C8—S1 | 82.3 (3) | N2—C12—C13—C16 | −179.41 (10) |
| C12—N2—C9—C10 | −57.8 (3) | O1—C12—C13—C15 | 120.25 (11) |
| N1—N2—C9—C10 | 129.1 (2) | N2—C12—C13—C15 | −60.21 (13) |
| C12—N2—C9—C11X | 48.0 (5) | O1—C12—C13—C14 | −116.95 (11) |
| N1—N2—C9—C11X | −125.2 (4) | N2—C12—C13—C14 | 62.59 (13) |
| C12—N2—C9—C11 | 69.4 (2) |
Hydrogen-bond geometry (Å, º)
| D—H···A | D—H | H···A | D···A | D—H···A |
| C14—H14B···N1 | 0.98 | 2.36 | 2.9893 (15) | 122 |
| C15—H15B···N1 | 0.98 | 2.37 | 2.9803 (15) | 120 |
| C11—H11B···O1i | 0.98 | 2.56 | 3.490 (4) | 159 |
Symmetry code: (i) −x+1, y+1/2, −z+1/2.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ2718).
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/S1600536812012639/rz2718sup1.cif
Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812012639/rz2718Isup2.hkl
Supplementary material file. DOI: 10.1107/S1600536812012639/rz2718Isup3.cml
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


