organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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Crystal structure of (E)-3-[4-(benzyl­­idene­amino)-5-sulfanyl­­idene-3-(p-tol­yl)-4,5-di­hydro-1H-1,2,4-triazol-1-yl]-3-(4-meth­­oxy­phen­yl)-1-phenyl­propan-1-one

aCollege of Chemical Engineering, Huanggang Normal University, Huanggang 438000, People's Republic of China
*Correspondence e-mail: tjuchemistry@gmail.com

Edited by M. Weil, Vienna University of Technology, Austria (Received 2 December 2015; accepted 10 December 2015; online 24 December 2015)

The title compound, C32H28N4O2S, crystallizes as a racemate. In the mol­ecule, the bond-angle sum at the C atom of the sulfanyl­idene entity bound to the triazole ring is 360°, with an annular N—C—N bond angle of 102.6 (2)° and two larger N—C—S angles of 127.3 (2) and 130.1 (2)°. The essentially planar 1,2,4-triazole ring (r.m.s. deviation = 0.013 Å) is nearly perpendicular to the phenylpropanone and methoxyphenyl rings , making dihedral angles of 76.9 (2) and 85.2 (2)°, respectively and subtends dihedral angles of 17.6 (2) and 40.3 (2)° with the tolyl and benzylideneamino rings, respectively. There is no ππ stacking between the mol­ecules. The crystal packing is dominated by weak C—H⋯O and C—H⋯N inter­actions, leading to a three-dimensional network structure. An intra­molecular C—H⋯S inter­action also occurs.

1. Related literature

Mannich base derivatives are used in numerous applications, e.g. in agrochemistry, pharmacy and polymer chemistry. Synthesis and crystal structures of such compounds were reported recently (Wang et al., 2011[Wang, W., Gao, Y., Xiao, Z., Yao, H. & Zhang, J. (2011). Acta Cryst. E67, o269.]; Shams et al., 2011[Shams, H. Z., Mohareb, R. M., Helal, M. H. & Mahmoud, A. (2011). Molecules, 16, 52-73.]). Bond lengths and angles of the title compound are comparable with related 1,2,4-triazole-5(4H)-thione derivatives (Al-Tamimi et al., 2010[Al-Tamimi, A.-M. S., Bari, A., Al-Omar, M. A., Alrashood, K. A. & El-Emam, A. A. (2010). Acta Cryst. E66, o1756.]; Fun et al., 2009[Fun, H.-K., Chantrapromma, S., Sujith, K. V. & Kalluraya, B. (2009). Acta Cryst. E65, o495-o496.]; Tan et al., 2010[Tan, K. W., Maah, M. J. & Ng, S. W. (2010). Acta Cryst. E66, o2224.]). For the crystal structures of other triazole derivatives, see: Zhao et al. (2010[Zhao, B., Liu, Z., Gao, Y., Song, B. & Deng, Q. (2010). Acta Cryst. E66, o2814.]); Gao et al. (2011[Gao, Y., Zhang, L. & Wang, H. (2011). Acta Cryst. E67, o1794.]).

[Scheme 1]

2. Experimental

2.1. Crystal data

  • C32H28N4O2S

  • Mr = 532.64

  • Triclinic, [P \overline 1]

  • a = 6.2343 (6) Å

  • b = 14.6968 (14) Å

  • c = 15.0540 (17) Å

  • α = 90.234 (9)°

  • β = 92.612 (13)°

  • γ = 99.497 (10)°

  • V = 1358.9 (2) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.16 mm−1

  • T = 113 K

  • 0.20 × 0.18 × 0.12 mm

2.2. Data collection

  • Rigaku Saturn CCD area-detector diffractometer

  • Absorption correction: multi-scan (CrystalClear; Rigaku/MSC, 2005[Rigaku/MSC (2005). CrystalClear and CrystalStructure. Molecular Structure Corporation, The Woodlands, Texas, USA, and Rigaku Corporation, Tokyo, Japan.]) Tmin = 0.969, Tmax = 0.982

  • 11718 measured reflections

  • 4778 independent reflections

  • 3450 reflections with I > 2σ(I)

  • Rint = 0.057

2.3. Refinement

  • R[F2 > 2σ(F2)] = 0.065

  • wR(F2) = 0.126

  • S = 1.08

  • 4778 reflections

  • 354 parameters

  • H-atom parameters constrained

  • Δρmax = 0.23 e Å−3

  • Δρmin = −0.25 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
C11—H11⋯N2 0.95 2.60 3.250 (4) 126
C20—H20⋯N4 0.95 2.39 2.990 (4) 121
C24—H24⋯O1i 0.95 2.58 3.464 (4) 156
C26—H26⋯S1 0.95 2.71 3.188 (3) 112
Symmetry code: (i) x+1, y, z.

Data collection: CrystalClear (Rigaku/MSC, 2005[Rigaku/MSC (2005). CrystalClear and CrystalStructure. Molecular Structure Corporation, The Woodlands, Texas, USA, and Rigaku Corporation, Tokyo, Japan.]); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: SHELXTL (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); software used to prepare material for publication: CrystalStructure (Rigaku/MSC, 2005[Rigaku/MSC (2005). CrystalClear and CrystalStructure. Molecular Structure Corporation, The Woodlands, Texas, USA, and Rigaku Corporation, Tokyo, Japan.]).

Supporting information


Related literature top

Mannich base derivatives are used in numerous applications, e.g. in agrochemistry, pharmacy or polymer chemistry. Synthesis and crystal structures of such compounds were reported recently (Wang et al., 2011; Shams et al., 2011). Bond lengths and angles of the title compound are comparable with related 1,2,4-triazole-5(4H)-thione derivatives (Al-Tamimi et al., 2010; Fun et al., 2009; Tan et al., 2010). For the crystal structures of other triazole derivatives, see: Zhao et al. (2010); Gao et al. (2011).

Experimental top

The title compound was synthesized by the reaction of benzaldehyde (2.0 mmol) and 3-(4-amino-5-thioxo-3-(p-tolyl)-4,5-dihydro-1H-1,2,4-triazol-1-yl)-3-(4-methoxyphenyl)-1-phenylpropan-1-one (2.0 mmol) under reflux in ethanol. The reaction progress was monitored via TLC. The resulting precipitate was filtered off, washed with cold ethanol, dried and purified to give the target product as a colorless solid in 75% yield. Crystals of the title compound suitable for single-crystal X-ray analysis were grown by slow evaporation of a chloroform-ethanol (1:1, v/v) mixture.

Refinement top

All H atoms were positioned geometrically and refined as riding (C—H = 0.95-0.99 Å) and allowed to ride on their parent atoms, with Uiso(H) = 1.2Ueq(C)aromatic or 1.5Ueq(C)methyl.

Structure description top

Mannich base derivatives are used in numerous applications, e.g. in agrochemistry, pharmacy or polymer chemistry. Synthesis and crystal structures of such compounds were reported recently (Wang et al., 2011; Shams et al., 2011). Bond lengths and angles of the title compound are comparable with related 1,2,4-triazole-5(4H)-thione derivatives (Al-Tamimi et al., 2010; Fun et al., 2009; Tan et al., 2010). For the crystal structures of other triazole derivatives, see: Zhao et al. (2010); Gao et al. (2011).

Computing details top

Data collection: CrystalClear (Rigaku/MSC, 2005); cell refinement: CrystalClear (Rigaku/MSC, 2005); data reduction: CrystalClear (Rigaku/MSC, 2005); 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: CrystalStructure (Rigaku/MSC, 2005).

Figures top
[Figure 1] Fig. 1. View of the title molecule showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 30% probability level.
(E)-3-[4-(Benzylideneamino)-5-sulfanylidene-3-(p-tolyl)-4,5-dihydro-1H-1,2,4-triazol-1-yl]-3-(4-methoxyphenyl)-1-phenylpropan-1-one top
Crystal data top
C32H28N4O2SZ = 2
Mr = 532.64F(000) = 560
Triclinic, P1Dx = 1.302 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 6.2343 (6) ÅCell parameters from 4230 reflections
b = 14.6968 (14) Åθ = 1.4–27.9°
c = 15.0540 (17) ŵ = 0.16 mm1
α = 90.234 (9)°T = 113 K
β = 92.612 (13)°Prism, colorless
γ = 99.497 (10)°0.20 × 0.18 × 0.12 mm
V = 1358.9 (2) Å3
Data collection top
Rigaku Saturn CCD area-detector
diffractometer
4778 independent reflections
Radiation source: rotating anode3450 reflections with I > 2σ(I)
Multilayer monochromatorRint = 0.057
Detector resolution: 14.22 pixels mm-1θmax = 25.0°, θmin = 1.4°
φ and ω scansh = 77
Absorption correction: multi-scan
(CrystalClear; Rigaku/MSC, 2005)
k = 1717
Tmin = 0.969, Tmax = 0.982l = 1517
11718 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.065Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.126H-atom parameters constrained
S = 1.08 w = 1/[σ2(Fo2) + (0.0362P)2]
where P = (Fo2 + 2Fc2)/3
4778 reflections(Δ/σ)max < 0.001
354 parametersΔρmax = 0.23 e Å3
0 restraintsΔρmin = 0.25 e Å3
Crystal data top
C32H28N4O2Sγ = 99.497 (10)°
Mr = 532.64V = 1358.9 (2) Å3
Triclinic, P1Z = 2
a = 6.2343 (6) ÅMo Kα radiation
b = 14.6968 (14) ŵ = 0.16 mm1
c = 15.0540 (17) ÅT = 113 K
α = 90.234 (9)°0.20 × 0.18 × 0.12 mm
β = 92.612 (13)°
Data collection top
Rigaku Saturn CCD area-detector
diffractometer
4778 independent reflections
Absorption correction: multi-scan
(CrystalClear; Rigaku/MSC, 2005)
3450 reflections with I > 2σ(I)
Tmin = 0.969, Tmax = 0.982Rint = 0.057
11718 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0650 restraints
wR(F2) = 0.126H-atom parameters constrained
S = 1.08Δρmax = 0.23 e Å3
4778 reflectionsΔρmin = 0.25 e Å3
354 parameters
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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 > 2sigma(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) top
xyzUiso*/Ueq
S10.30821 (12)0.76134 (6)0.33347 (5)0.0326 (2)
O10.2917 (3)0.84691 (17)0.03956 (14)0.0466 (6)
O21.1239 (3)1.11680 (15)0.44187 (14)0.0418 (6)
N10.5946 (4)0.78848 (17)0.20148 (16)0.0288 (6)
N20.7452 (4)0.74728 (17)0.15811 (15)0.0289 (6)
N30.5736 (4)0.65289 (16)0.25500 (15)0.0251 (6)
N40.5344 (4)0.57402 (17)0.30854 (15)0.0282 (6)
C10.4101 (5)0.7859 (2)0.1241 (2)0.0378 (8)
H10.26460.76740.10710.045*
C20.4689 (5)0.7603 (2)0.2071 (2)0.0414 (9)
H20.36520.72340.24610.050*
C30.6790 (6)0.7886 (2)0.2330 (2)0.0463 (9)
H30.72100.77130.28970.056*
C40.8290 (6)0.8429 (3)0.1749 (2)0.0573 (11)
H40.97280.86390.19280.069*
C50.7699 (5)0.8662 (3)0.0917 (2)0.0477 (10)
H50.87450.90190.05220.057*
C60.5594 (5)0.8382 (2)0.0651 (2)0.0341 (8)
C70.4844 (5)0.8637 (2)0.0235 (2)0.0345 (8)
C80.6475 (5)0.9123 (2)0.09322 (19)0.0337 (8)
H8A0.79250.89610.08310.040*
H8B0.65810.97980.08630.040*
C90.5869 (5)0.8870 (2)0.1874 (2)0.0318 (8)
H90.43430.89740.19490.038*
C100.7354 (5)0.9461 (2)0.2563 (2)0.0305 (7)
C110.9305 (5)0.9220 (2)0.2886 (2)0.0354 (8)
H110.97160.86650.26800.042*
C121.0670 (5)0.9768 (2)0.3501 (2)0.0336 (8)
H121.19950.95890.37150.040*
C131.0064 (5)1.0585 (2)0.3798 (2)0.0330 (8)
C140.8140 (5)1.0844 (2)0.3471 (2)0.0346 (8)
H140.77501.14090.36640.042*
C150.6780 (5)1.0282 (2)0.2863 (2)0.0333 (8)
H150.54521.04590.26510.040*
C161.3209 (5)1.0916 (2)0.4790 (2)0.0444 (9)
H16A1.28971.02960.50390.067*
H16B1.38211.13570.52620.067*
H16C1.42591.09230.43240.067*
C170.4885 (4)0.7336 (2)0.26328 (18)0.0268 (7)
C180.7328 (4)0.6653 (2)0.19328 (18)0.0265 (7)
C190.8735 (4)0.5993 (2)0.16637 (18)0.0249 (7)
C200.8278 (5)0.5049 (2)0.18174 (19)0.0303 (7)
H200.70200.47970.21230.036*
C210.9675 (5)0.4476 (2)0.15206 (19)0.0322 (8)
H210.93580.38340.16370.039*
C221.1507 (5)0.4811 (2)0.10621 (18)0.0286 (7)
C231.1946 (5)0.5765 (2)0.09149 (18)0.0305 (7)
H231.32000.60150.06060.037*
C241.0587 (4)0.6352 (2)0.12106 (18)0.0277 (7)
H241.09170.69960.11050.033*
C251.2951 (5)0.4167 (2)0.0723 (2)0.0392 (8)
H25A1.28100.41340.00730.059*
H25B1.25100.35500.09660.059*
H25C1.44690.43990.09120.059*
C260.3327 (5)0.5466 (2)0.32321 (19)0.0315 (8)
H260.22440.57760.29660.038*
C270.2695 (5)0.4680 (2)0.38059 (19)0.0321 (8)
C280.0539 (5)0.4429 (3)0.4000 (2)0.0554 (11)
H280.05270.47530.37420.066*
C290.0081 (6)0.3699 (3)0.4574 (3)0.0706 (14)
H290.15730.35280.46990.085*
C300.1416 (6)0.3229 (2)0.4957 (2)0.0433 (9)
H300.09830.27420.53570.052*
C310.3562 (6)0.3468 (2)0.4759 (2)0.0470 (9)
H310.46140.31320.50110.056*
C320.4202 (5)0.4186 (2)0.4199 (2)0.0468 (10)
H320.56980.43500.40790.056*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0324 (5)0.0306 (5)0.0362 (5)0.0091 (4)0.0037 (4)0.0018 (4)
O10.0281 (13)0.0631 (18)0.0462 (15)0.0003 (13)0.0005 (11)0.0048 (12)
O20.0445 (14)0.0375 (15)0.0433 (14)0.0086 (12)0.0049 (11)0.0091 (11)
N10.0253 (14)0.0267 (15)0.0349 (16)0.0053 (12)0.0010 (12)0.0043 (12)
N20.0302 (15)0.0265 (15)0.0305 (15)0.0058 (13)0.0030 (11)0.0035 (11)
N30.0264 (14)0.0225 (14)0.0266 (14)0.0046 (12)0.0004 (11)0.0059 (11)
N40.0312 (15)0.0244 (15)0.0294 (15)0.0048 (12)0.0031 (12)0.0024 (11)
C10.0347 (19)0.031 (2)0.046 (2)0.0024 (16)0.0027 (16)0.0098 (16)
C20.047 (2)0.032 (2)0.042 (2)0.0002 (18)0.0043 (17)0.0038 (16)
C30.059 (3)0.044 (2)0.036 (2)0.010 (2)0.0048 (19)0.0079 (17)
C40.046 (2)0.081 (3)0.042 (2)0.003 (2)0.0046 (19)0.013 (2)
C50.041 (2)0.061 (3)0.037 (2)0.002 (2)0.0027 (17)0.0081 (18)
C60.0324 (19)0.034 (2)0.035 (2)0.0054 (16)0.0014 (15)0.0093 (15)
C70.038 (2)0.0267 (19)0.038 (2)0.0054 (16)0.0018 (16)0.0073 (14)
C80.0357 (19)0.0268 (19)0.038 (2)0.0027 (16)0.0004 (15)0.0086 (14)
C90.0334 (18)0.0216 (18)0.041 (2)0.0068 (15)0.0029 (15)0.0067 (14)
C100.0311 (18)0.0236 (18)0.0374 (19)0.0054 (15)0.0040 (15)0.0044 (14)
C110.0353 (19)0.029 (2)0.044 (2)0.0100 (16)0.0020 (16)0.0002 (15)
C120.0306 (18)0.033 (2)0.0375 (19)0.0063 (16)0.0006 (15)0.0019 (15)
C130.0341 (19)0.034 (2)0.0299 (19)0.0018 (16)0.0037 (15)0.0012 (14)
C140.040 (2)0.0265 (19)0.040 (2)0.0107 (16)0.0069 (16)0.0007 (15)
C150.0337 (19)0.030 (2)0.037 (2)0.0057 (16)0.0040 (15)0.0073 (15)
C160.041 (2)0.045 (2)0.045 (2)0.0032 (18)0.0027 (17)0.0065 (17)
C170.0267 (17)0.0237 (18)0.0295 (18)0.0043 (14)0.0040 (13)0.0009 (13)
C180.0250 (17)0.0257 (18)0.0273 (18)0.0008 (14)0.0021 (14)0.0017 (13)
C190.0232 (16)0.0288 (18)0.0219 (16)0.0029 (14)0.0010 (13)0.0001 (13)
C200.0294 (17)0.0278 (19)0.0330 (18)0.0019 (15)0.0049 (14)0.0013 (14)
C210.0371 (19)0.0246 (18)0.0336 (19)0.0010 (16)0.0028 (15)0.0020 (14)
C220.0309 (18)0.0310 (19)0.0236 (17)0.0052 (15)0.0012 (14)0.0036 (13)
C230.0252 (17)0.040 (2)0.0256 (17)0.0026 (16)0.0028 (13)0.0024 (14)
C240.0287 (17)0.0239 (18)0.0286 (18)0.0001 (15)0.0015 (14)0.0009 (13)
C250.0389 (19)0.044 (2)0.036 (2)0.0107 (18)0.0033 (15)0.0045 (16)
C260.0346 (19)0.030 (2)0.0298 (18)0.0058 (16)0.0009 (15)0.0017 (14)
C270.0367 (19)0.0299 (19)0.0289 (18)0.0024 (16)0.0044 (14)0.0033 (14)
C280.034 (2)0.060 (3)0.075 (3)0.011 (2)0.0095 (19)0.036 (2)
C290.042 (2)0.073 (3)0.099 (4)0.007 (2)0.022 (2)0.047 (3)
C300.050 (2)0.038 (2)0.042 (2)0.0069 (19)0.0027 (17)0.0100 (16)
C310.047 (2)0.040 (2)0.054 (2)0.0081 (19)0.0018 (18)0.0150 (18)
C320.037 (2)0.041 (2)0.062 (3)0.0067 (18)0.0026 (18)0.0205 (19)
Geometric parameters (Å, º) top
S1—C171.674 (3)C13—C141.388 (4)
O1—C71.221 (3)C14—C151.390 (4)
O2—C131.366 (4)C14—H140.9500
O2—C161.431 (3)C15—H150.9500
N1—C171.356 (3)C16—H16A0.9800
N1—N21.384 (3)C16—H16B0.9800
N1—C91.472 (3)C16—H16C0.9800
N2—C181.310 (3)C18—C191.478 (4)
N3—C181.381 (3)C19—C201.392 (4)
N3—C171.385 (3)C19—C241.397 (4)
N3—N41.409 (3)C20—C211.393 (4)
N4—C261.285 (3)C20—H200.9500
C1—C21.387 (4)C21—C221.383 (4)
C1—C61.388 (4)C21—H210.9500
C1—H10.9500C22—C231.404 (4)
C2—C31.381 (4)C22—C251.512 (4)
C2—H20.9500C23—C241.390 (4)
C3—C41.396 (5)C23—H230.9500
C3—H30.9500C24—H240.9500
C4—C51.379 (4)C25—H25A0.9800
C4—H40.9500C25—H25B0.9800
C5—C61.387 (4)C25—H25C0.9800
C5—H50.9500C26—C271.458 (4)
C6—C71.501 (4)C26—H260.9500
C7—C81.517 (4)C27—C281.378 (4)
C8—C91.516 (4)C27—C321.392 (4)
C8—H8A0.9900C28—C291.396 (4)
C8—H8B0.9900C28—H280.9500
C9—C101.525 (4)C29—C301.359 (4)
C9—H91.0000C29—H290.9500
C10—C111.389 (4)C30—C311.373 (4)
C10—C151.394 (4)C30—H300.9500
C11—C121.387 (4)C31—C321.372 (4)
C11—H110.9500C31—H310.9500
C12—C131.395 (4)C32—H320.9500
C12—H120.9500
C13—O2—C16117.5 (2)C10—C15—H15119.8
C17—N1—N2113.2 (2)O2—C16—H16A109.5
C17—N1—C9126.6 (2)O2—C16—H16B109.5
N2—N1—C9119.4 (2)H16A—C16—H16B109.5
C18—N2—N1104.8 (2)O2—C16—H16C109.5
C18—N3—C17109.2 (2)H16A—C16—H16C109.5
C18—N3—N4122.9 (2)H16B—C16—H16C109.5
C17—N3—N4127.3 (2)N1—C17—N3102.6 (2)
C26—N4—N3114.4 (2)N1—C17—S1127.3 (2)
C2—C1—C6121.4 (3)N3—C17—S1130.1 (2)
C2—C1—H1119.3N2—C18—N3110.0 (2)
C6—C1—H1119.3N2—C18—C19122.0 (3)
C3—C2—C1119.7 (3)N3—C18—C19127.9 (3)
C3—C2—H2120.2C20—C19—C24119.4 (3)
C1—C2—H2120.2C20—C19—C18123.7 (3)
C2—C3—C4119.3 (3)C24—C19—C18116.8 (3)
C2—C3—H3120.3C19—C20—C21119.7 (3)
C4—C3—H3120.3C19—C20—H20120.2
C5—C4—C3120.4 (3)C21—C20—H20120.2
C5—C4—H4119.8C22—C21—C20122.2 (3)
C3—C4—H4119.8C22—C21—H21118.9
C4—C5—C6120.7 (3)C20—C21—H21118.9
C4—C5—H5119.6C21—C22—C23117.4 (3)
C6—C5—H5119.6C21—C22—C25120.9 (3)
C5—C6—C1118.4 (3)C23—C22—C25121.7 (3)
C5—C6—C7123.0 (3)C24—C23—C22121.5 (3)
C1—C6—C7118.5 (3)C24—C23—H23119.2
O1—C7—C6120.3 (3)C22—C23—H23119.2
O1—C7—C8119.6 (3)C23—C24—C19119.8 (3)
C6—C7—C8120.0 (3)C23—C24—H24120.1
C9—C8—C7112.9 (3)C19—C24—H24120.1
C9—C8—H8A109.0C22—C25—H25A109.5
C7—C8—H8A109.0C22—C25—H25B109.5
C9—C8—H8B109.0H25A—C25—H25B109.5
C7—C8—H8B109.0C22—C25—H25C109.5
H8A—C8—H8B107.8H25A—C25—H25C109.5
N1—C9—C8109.4 (2)H25B—C25—H25C109.5
N1—C9—C10110.5 (2)N4—C26—C27120.2 (3)
C8—C9—C10111.9 (3)N4—C26—H26119.9
N1—C9—H9108.3C27—C26—H26119.9
C8—C9—H9108.3C28—C27—C32118.0 (3)
C10—C9—H9108.3C28—C27—C26119.5 (3)
C11—C10—C15118.5 (3)C32—C27—C26122.5 (3)
C11—C10—C9122.0 (3)C27—C28—C29120.2 (3)
C15—C10—C9119.4 (3)C27—C28—H28119.9
C12—C11—C10121.9 (3)C29—C28—H28119.9
C12—C11—H11119.1C30—C29—C28121.0 (3)
C10—C11—H11119.1C30—C29—H29119.5
C11—C12—C13118.8 (3)C28—C29—H29119.5
C11—C12—H12120.6C29—C30—C31119.1 (3)
C13—C12—H12120.6C29—C30—H30120.4
O2—C13—C14115.6 (3)C31—C30—H30120.4
O2—C13—C12124.3 (3)C32—C31—C30120.6 (3)
C14—C13—C12120.1 (3)C32—C31—H31119.7
C13—C14—C15120.3 (3)C30—C31—H31119.7
C13—C14—H14119.9C31—C32—C27121.1 (3)
C15—C14—H14119.9C31—C32—H32119.5
C14—C15—C10120.4 (3)C27—C32—H32119.5
C14—C15—H15119.8
C17—N1—N2—C180.1 (3)N2—N1—C17—N32.2 (3)
C9—N1—N2—C18171.3 (2)C9—N1—C17—N3172.6 (3)
C18—N3—N4—C26143.4 (3)N2—N1—C17—S1175.6 (2)
C17—N3—N4—C2646.8 (4)C9—N1—C17—S15.2 (4)
C6—C1—C2—C31.3 (5)C18—N3—C17—N13.4 (3)
C1—C2—C3—C40.1 (5)N4—N3—C17—N1174.3 (2)
C2—C3—C4—C51.6 (5)C18—N3—C17—S1174.3 (2)
C3—C4—C5—C61.6 (6)N4—N3—C17—S13.4 (4)
C4—C5—C6—C10.2 (5)N1—N2—C18—N32.1 (3)
C4—C5—C6—C7178.3 (3)N1—N2—C18—C19178.4 (2)
C2—C1—C6—C51.2 (5)C17—N3—C18—N23.6 (3)
C2—C1—C6—C7179.8 (3)N4—N3—C18—N2175.1 (2)
C5—C6—C7—O1171.1 (3)C17—N3—C18—C19177.0 (3)
C1—C6—C7—O17.4 (5)N4—N3—C18—C195.6 (4)
C5—C6—C7—C87.7 (5)N2—C18—C19—C20161.1 (3)
C1—C6—C7—C8173.8 (3)N3—C18—C19—C2018.2 (4)
O1—C7—C8—C933.4 (4)N2—C18—C19—C2417.2 (4)
C6—C7—C8—C9147.8 (3)N3—C18—C19—C24163.5 (3)
C17—N1—C9—C8157.2 (3)C24—C19—C20—C210.2 (4)
N2—N1—C9—C832.8 (3)C18—C19—C20—C21178.5 (3)
C17—N1—C9—C1079.1 (4)C19—C20—C21—C220.9 (4)
N2—N1—C9—C1090.8 (3)C20—C21—C22—C231.0 (4)
C7—C8—C9—N165.0 (3)C20—C21—C22—C25178.0 (3)
C7—C8—C9—C10172.2 (2)C21—C22—C23—C240.5 (4)
N1—C9—C10—C1134.7 (4)C25—C22—C23—C24178.6 (3)
C8—C9—C10—C1187.6 (3)C22—C23—C24—C190.1 (4)
N1—C9—C10—C15147.2 (3)C20—C19—C24—C230.3 (4)
C8—C9—C10—C1590.6 (3)C18—C19—C24—C23178.1 (2)
C15—C10—C11—C120.7 (5)N3—N4—C26—C27177.5 (3)
C9—C10—C11—C12178.8 (3)N4—C26—C27—C28176.1 (3)
C10—C11—C12—C130.3 (5)N4—C26—C27—C321.3 (5)
C16—O2—C13—C14178.5 (3)C32—C27—C28—C290.1 (6)
C16—O2—C13—C120.5 (5)C26—C27—C28—C29177.7 (4)
C11—C12—C13—O2178.2 (3)C27—C28—C29—C300.6 (7)
C11—C12—C13—C140.9 (5)C28—C29—C30—C311.4 (6)
O2—C13—C14—C15177.5 (3)C29—C30—C31—C321.7 (6)
C12—C13—C14—C151.6 (5)C30—C31—C32—C271.2 (6)
C13—C14—C15—C101.2 (5)C28—C27—C32—C310.4 (5)
C11—C10—C15—C140.0 (5)C26—C27—C32—C31177.9 (3)
C9—C10—C15—C14178.2 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C11—H11···N20.952.603.250 (4)126
C20—H20···N40.952.392.990 (4)121
C24—H24···O1i0.952.583.464 (4)156
C26—H26···S10.952.713.188 (3)112
Symmetry code: (i) x+1, y, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C11—H11···N20.952.603.250 (4)126
C20—H20···N40.952.392.990 (4)121
C24—H24···O1i0.952.583.464 (4)156
C26—H26···S10.952.713.188 (3)112
Symmetry code: (i) x+1, y, z.
 

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