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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2013 Aug 3;69(Pt 9):o1368. doi: 10.1107/S1600536813021053

1-[3-({[Bis(2-methyl­prop­yl)carbamo­thio­yl]amino}­carbon­yl)benzoyl]-3,3-bis­(2-methyl­prop­yl)thio­urea

N Selvakumaran a, R Karvembu a,, Seik Weng Ng b,c, Edward R T Tiekink b,*
PMCID: PMC3884506  PMID: 24427014

Abstract

The title compound, C26H42N4O2S2, adopts a shallow U-shape as both pendant arms of the 1,3-substituted benzene ring are orientated in the same direction. The thione S atoms lie to the same side of the benzene ring and the carbonyl O atoms to the other. The most prominent feature of the crystal packing is the formation of inversion dimers mediated by N—H⋯S hydrogen bonds. One of the 2-methyl­propyl groups is statistically disordered over two positions.

Related literature  

For the use of the title compound in the synthesis of metal macrocycles, see: Nguyen et al. (2011). For the structure of the methanol solvate, see: Rodenstein et al. (2007).graphic file with name e-69-o1368-scheme1.jpg

Experimental  

Crystal data  

  • C26H42N4O2S2

  • M r = 506.76

  • Monoclinic, Inline graphic

  • a = 12.6926 (2) Å

  • b = 11.8015 (2) Å

  • c = 19.9701 (4) Å

  • β = 103.883 (2)°

  • V = 2903.97 (9) Å3

  • Z = 4

  • Cu Kα radiation

  • μ = 1.87 mm−1

  • T = 100 K

  • 0.30 × 0.25 × 0.20 mm

Data collection  

  • Agilent SuperNova Dual diffractometer with an Atlas detector

  • Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2013) T min = 0.217, T max = 1.000

  • 11629 measured reflections

  • 5743 independent reflections

  • 5234 reflections with I > 2σ(I)

  • R int = 0.028

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.050

  • wR(F 2) = 0.142

  • S = 1.01

  • 5743 reflections

  • 316 parameters

  • 30 restraints

  • H-atom parameters constrained

  • Δρmax = 0.89 e Å−3

  • Δρmin = −0.82 e Å−3

Data collection: CrysAlis PRO (Agilent, 2013); 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) general, I. DOI: 10.1107/S1600536813021053/hg5336sup1.cif

e-69-o1368-sup1.cif (28KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813021053/hg5336Isup2.hkl

e-69-o1368-Isup2.hkl (281.2KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536813021053/hg5336Isup3.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
N2—H2⋯S2i 0.88 2.62 3.4745 (17) 163
N3—H3⋯S2i 0.88 2.54 3.3870 (18) 162

Symmetry code: (i) Inline graphic.

Acknowledgments

NS thanks NITT for a Fellowship. The authors also thank the Ministry of Higher Education (Malaysia) for funding structural studies through the High-Impact Research scheme (UM.C/HIR-MOHE/SC/12).

supplementary crystallographic information

1. Comment

The title compound, (I), for which the structure of a methanol solvate is known (Rodenstein et al., 2007), plays a vital role in forming a metallamacrocyclic square-planar d8 metal complexes via self-assembly (Nguyen et al., 2011).

In (I), Fig. 1, there is an almost orthogonal relationship between adjacent thione and carbonyl groups as seen in the C10—N2—C9—S1 and C17—N3—C18—S2 torsion angles of -113.25 (18) and 112.56 (18)°, respectively. Globally, the molecule adopts a flattened U-shape. The thione-S atoms lie to one side of the plane through the central benzene and the carbonyl-O atoms to the other so that the molecule has approximate mirror symmetry. The structure reported here for (I) is quite distinct that that observed in the methanol solvate of (I) (Rodenstein et al., 2007). In the latter, the thione-S atoms lie to either side of the benzene ring and, to a first approximation, the carbonyl-O atoms are co-planar with the ring.

Being direct towards the centre of the U-shaped molecule, the nitrogen-bound hydrogen atoms are well placed to form two N—H···S hydrogen bonds with an inverted U-shaped molecule with the central pair forming an eight-membered {···HNCS}2 synthon, Fig. 2 and Table 1. A detailed analysis of the crystal packing is precluded owing to the presence of disorder in the molecule.

2. Experimental

Isophthaloyl dichloride (2.0302 g, 10 mmol) dissolved in acetone (80 ml) was placed in a dropping funnel and added drop wise with stirring to potassium thiocyanate (1.9436 g, 20 mmol) dissolved in acetone (80 ml), under an N2 atmosphere, in a three-necked round bottom flask. The mixture was heated to reflux for 30 min. and then allowed to cool. A solution of diisobutylamine (2.2850 g, 20 mmol) in acetone (80 ml) was added drop wise from a dropping funnel to the reaction mixture and the resulting mixture was stirred for 2 h. Hydrochloric acid (0.1 N, 300 ml) was added and the resulting white solid was filtered off, washed with water and dried in vacuo. Single crystals were grown at room temperature from its acetonitrile solution. FT—IR (KBr): ν(N—H) 3275, ν(C═O) 1694, ν(C═C) 1604, ν(C═S) 1262 cm-1.

3. Refinement

Carbon-bound H-atoms were placed in calculated positions [N—H = 0.88 Å; C—H = 0.95–0.99 Å, Uiso(H) = 1.2–1.5Ueq(N, C)] and were included in the refinement in the riding model approximation. The C24-containing groups was disordered over two positions of equal weight, from refinement. Pairs of 1,2-related distances were restrained to 1.50±0.01 Å and the 1,3-related ones to 2.35±0.01 Å. The anisotropic displacement parameters (adp) of the primed atoms were set to those of the unprimed ones, and the adp of the three components of the affected atoms were tightly restrained with the ISOR command in SHELXL97.

Figures

Fig. 1.

Fig. 1.

Molecular structure of (I) showing atom-labelling scheme and displacement ellipsoids at the 70% probability level.

Fig. 2.

Fig. 2.

A view of the supramolecular dimer sustained by N—H···S hydrogen bonding, shown as orange dashed lines.

Crystal data

C26H42N4O2S2 F(000) = 1096
Mr = 506.76 Dx = 1.159 Mg m3
Monoclinic, P21/c Cu Kα radiation, λ = 1.54184 Å
Hall symbol: -P 2ybc Cell parameters from 7250 reflections
a = 12.6926 (2) Å θ = 3.6–74.2°
b = 11.8015 (2) Å µ = 1.87 mm1
c = 19.9701 (4) Å T = 100 K
β = 103.883 (2)° Prism, colourless
V = 2903.97 (9) Å3 0.30 × 0.25 × 0.20 mm
Z = 4

Data collection

Agilent SuperNova Dual diffractometer with an Atlas detector 5743 independent reflections
Radiation source: SuperNova (Cu) X-ray Source 5234 reflections with I > 2σ(I)
Mirror monochromator Rint = 0.028
Detector resolution: 10.4041 pixels mm-1 θmax = 74.4°, θmin = 3.6°
ω scan h = −15→13
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2013) k = −12→14
Tmin = 0.217, Tmax = 1.000 l = −24→24
11629 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)] = 0.050 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.142 H-atom parameters constrained
S = 1.01 w = 1/[σ2(Fo2) + (0.0843P)2 + 2.364P] where P = (Fo2 + 2Fc2)/3
5743 reflections (Δ/σ)max = 0.001
316 parameters Δρmax = 0.89 e Å3
30 restraints Δρmin = −0.82 e Å3

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 Occ. (<1)
S1 0.11609 (4) 0.55881 (4) 0.67655 (3) 0.02477 (15)
S2 0.62752 (4) 0.46118 (4) 0.44878 (3) 0.02293 (15)
O1 0.17340 (12) 0.22802 (13) 0.68690 (8) 0.0241 (3)
O2 0.61704 (11) 0.15808 (12) 0.54351 (7) 0.0206 (3)
N1 0.24077 (13) 0.43431 (13) 0.77683 (8) 0.0169 (3)
N2 0.25286 (13) 0.39332 (14) 0.66500 (8) 0.0170 (3)
H2 0.2964 0.4261 0.6426 0.020*
N3 0.56570 (13) 0.34366 (14) 0.54531 (9) 0.0176 (3)
H3 0.5191 0.3901 0.5572 0.021*
N4 0.75240 (13) 0.37320 (13) 0.56575 (9) 0.0178 (3)
C1 0.18861 (16) 0.48806 (17) 0.82699 (10) 0.0203 (4)
H1A 0.1745 0.5688 0.8145 0.024*
H1B 0.2388 0.4851 0.8733 0.024*
C2 0.08139 (17) 0.43044 (18) 0.82988 (11) 0.0219 (4)
H2A 0.0328 0.4316 0.7824 0.026*
C3 0.0975 (2) 0.3077 (2) 0.85294 (13) 0.0306 (5)
H3A 0.1339 0.2665 0.8223 0.046*
H3B 0.0268 0.2729 0.8511 0.046*
H3C 0.1421 0.3046 0.9003 0.046*
C4 0.02682 (19) 0.4997 (2) 0.87688 (13) 0.0323 (5)
H4A −0.0413 0.4630 0.8796 0.048*
H4B 0.0116 0.5763 0.8580 0.048*
H4C 0.0752 0.5042 0.9231 0.048*
C5 0.33477 (16) 0.36086 (17) 0.80564 (10) 0.0196 (4)
H5A 0.3458 0.3086 0.7691 0.023*
H5B 0.3183 0.3143 0.8431 0.023*
C6 0.44031 (17) 0.42639 (19) 0.83420 (11) 0.0239 (4)
H6 0.4305 0.4746 0.8734 0.029*
C7 0.47084 (19) 0.5028 (2) 0.78033 (13) 0.0334 (5)
H7A 0.5390 0.5420 0.8008 0.050*
H7B 0.4132 0.5587 0.7643 0.050*
H7C 0.4800 0.4568 0.7412 0.050*
C8 0.52897 (19) 0.3391 (2) 0.86208 (13) 0.0347 (5)
H8A 0.5980 0.3782 0.8804 0.052*
H8B 0.5363 0.2881 0.8248 0.052*
H8C 0.5094 0.2952 0.8990 0.052*
C9 0.20600 (16) 0.45859 (16) 0.71007 (10) 0.0177 (4)
C10 0.23093 (15) 0.27912 (16) 0.65600 (10) 0.0173 (4)
C11 0.28645 (15) 0.22035 (16) 0.60795 (10) 0.0164 (4)
C12 0.23975 (16) 0.12179 (16) 0.57527 (10) 0.0183 (4)
H12 0.1725 0.0956 0.5824 0.022*
C13 0.29103 (16) 0.06192 (16) 0.53250 (10) 0.0196 (4)
H13 0.2580 −0.0040 0.5093 0.024*
C14 0.39096 (16) 0.09851 (16) 0.52349 (10) 0.0179 (4)
H14 0.4266 0.0568 0.4947 0.021*
C15 0.43890 (15) 0.19632 (16) 0.55670 (10) 0.0162 (4)
C16 0.38622 (15) 0.25765 (16) 0.59863 (9) 0.0158 (4)
H16 0.4182 0.3248 0.6208 0.019*
C17 0.54908 (15) 0.22891 (16) 0.54792 (10) 0.0164 (4)
C18 0.65585 (16) 0.38956 (16) 0.52398 (10) 0.0173 (4)
C19 0.85265 (15) 0.40405 (17) 0.54486 (11) 0.0200 (4)
H19A 0.8997 0.4496 0.5819 0.024*
H19B 0.8337 0.4515 0.5028 0.024*
C20 0.91545 (16) 0.29955 (17) 0.53062 (11) 0.0217 (4)
H20 0.9352 0.2529 0.5736 0.026*
C21 1.02006 (16) 0.33990 (19) 0.51283 (11) 0.0252 (4)
H21A 1.0612 0.3873 0.5504 0.038*
H21B 1.0020 0.3841 0.4700 0.038*
H21C 1.0639 0.2741 0.5067 0.038*
C22 0.84824 (19) 0.22679 (19) 0.47291 (13) 0.0292 (5)
H22A 0.7817 0.2023 0.4854 0.044*
H22B 0.8904 0.1601 0.4660 0.044*
H22C 0.8294 0.2711 0.4302 0.044*
C23 0.76747 (16) 0.33369 (17) 0.63803 (10) 0.0208 (4)
H23A 0.7282 0.2611 0.6375 0.025* 0.50
H23B 0.8456 0.3181 0.6570 0.025* 0.50
H23C 0.8314 0.2830 0.6501 0.025* 0.50
H23D 0.7030 0.2898 0.6423 0.025* 0.50
C24 0.7304 (4) 0.4126 (4) 0.6856 (2) 0.0249 (7) 0.50
H24 0.6498 0.4219 0.6718 0.030* 0.50
C25 0.7662 (18) 0.3648 (9) 0.7587 (4) 0.0535 (12) 0.50
H25A 0.7500 0.2835 0.7580 0.080* 0.50
H25B 0.7272 0.4038 0.7888 0.080* 0.50
H25C 0.8445 0.3764 0.7763 0.080* 0.50
C26 0.7866 (5) 0.5259 (4) 0.6858 (3) 0.0385 (8) 0.50
H26A 0.7744 0.5723 0.7239 0.058* 0.50
H26B 0.7571 0.5649 0.6420 0.058* 0.50
H26C 0.8647 0.5138 0.6916 0.058* 0.50
C24' 0.7841 (4) 0.4354 (4) 0.6890 (2) 0.0249 (7) 0.50
H24' 0.8598 0.4653 0.6964 0.030* 0.50
C25' 0.7669 (18) 0.3828 (10) 0.7565 (4) 0.0535 (12) 0.50
H25D 0.7828 0.4395 0.7934 0.080* 0.50
H25E 0.8156 0.3178 0.7695 0.080* 0.50
H25F 0.6915 0.3576 0.7494 0.080* 0.50
C26' 0.7058 (5) 0.5276 (4) 0.6693 (3) 0.0385 (8) 0.50
H26D 0.7060 0.5536 0.6227 0.058* 0.50
H26E 0.7257 0.5905 0.7019 0.058* 0.50
H26F 0.6331 0.5003 0.6700 0.058* 0.50

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0289 (3) 0.0230 (3) 0.0233 (3) 0.00895 (19) 0.0080 (2) 0.00262 (19)
S2 0.0208 (3) 0.0234 (3) 0.0279 (3) 0.00407 (18) 0.0124 (2) 0.00993 (19)
O1 0.0282 (8) 0.0239 (7) 0.0252 (7) −0.0074 (6) 0.0163 (6) −0.0031 (6)
O2 0.0200 (7) 0.0164 (7) 0.0286 (8) 0.0007 (5) 0.0119 (6) −0.0014 (5)
N1 0.0179 (8) 0.0179 (8) 0.0167 (8) 0.0007 (6) 0.0078 (6) −0.0014 (6)
N2 0.0189 (8) 0.0175 (8) 0.0175 (8) −0.0016 (6) 0.0101 (6) −0.0002 (6)
N3 0.0165 (8) 0.0143 (8) 0.0255 (9) 0.0001 (6) 0.0121 (7) 0.0015 (6)
N4 0.0187 (8) 0.0141 (7) 0.0228 (8) −0.0011 (6) 0.0092 (6) 0.0005 (6)
C1 0.0227 (10) 0.0206 (10) 0.0200 (9) −0.0001 (8) 0.0098 (8) −0.0042 (8)
C2 0.0219 (10) 0.0248 (10) 0.0217 (10) −0.0019 (8) 0.0106 (8) −0.0042 (8)
C3 0.0328 (12) 0.0269 (11) 0.0376 (13) −0.0042 (9) 0.0190 (10) 0.0012 (9)
C4 0.0283 (11) 0.0371 (13) 0.0369 (13) −0.0012 (10) 0.0186 (10) −0.0105 (10)
C5 0.0212 (10) 0.0207 (10) 0.0180 (9) 0.0021 (8) 0.0071 (8) 0.0010 (7)
C6 0.0206 (10) 0.0299 (11) 0.0215 (10) 0.0002 (8) 0.0052 (8) −0.0059 (8)
C7 0.0249 (11) 0.0387 (13) 0.0370 (13) −0.0099 (10) 0.0085 (10) −0.0008 (10)
C8 0.0256 (11) 0.0425 (14) 0.0326 (12) 0.0074 (10) 0.0002 (9) −0.0060 (10)
C9 0.0188 (9) 0.0161 (9) 0.0202 (9) −0.0026 (7) 0.0086 (8) −0.0020 (7)
C10 0.0170 (9) 0.0193 (9) 0.0168 (9) −0.0005 (7) 0.0063 (7) 0.0005 (7)
C11 0.0189 (9) 0.0156 (9) 0.0163 (9) −0.0002 (7) 0.0070 (7) 0.0023 (7)
C12 0.0167 (9) 0.0177 (9) 0.0216 (9) −0.0022 (7) 0.0065 (7) 0.0009 (7)
C13 0.0215 (10) 0.0157 (9) 0.0221 (10) −0.0032 (7) 0.0058 (8) −0.0023 (7)
C14 0.0202 (9) 0.0159 (9) 0.0187 (9) 0.0010 (7) 0.0071 (7) −0.0012 (7)
C15 0.0175 (9) 0.0151 (9) 0.0171 (9) −0.0002 (7) 0.0066 (7) 0.0029 (7)
C16 0.0182 (9) 0.0134 (8) 0.0164 (9) −0.0017 (7) 0.0052 (7) −0.0002 (7)
C17 0.0190 (9) 0.0157 (9) 0.0162 (9) −0.0010 (7) 0.0078 (7) −0.0005 (7)
C18 0.0192 (9) 0.0122 (8) 0.0235 (10) 0.0000 (7) 0.0110 (7) −0.0003 (7)
C19 0.0160 (9) 0.0181 (9) 0.0285 (10) −0.0021 (7) 0.0104 (8) 0.0025 (8)
C20 0.0220 (10) 0.0202 (10) 0.0261 (10) 0.0045 (8) 0.0118 (8) 0.0060 (8)
C21 0.0174 (10) 0.0325 (11) 0.0266 (11) 0.0029 (8) 0.0073 (8) 0.0022 (9)
C22 0.0303 (11) 0.0215 (10) 0.0416 (13) −0.0044 (9) 0.0202 (10) −0.0055 (9)
C23 0.0198 (9) 0.0217 (10) 0.0217 (10) −0.0007 (8) 0.0067 (8) 0.0020 (8)
C24 0.026 (2) 0.0248 (17) 0.0264 (14) −0.0041 (16) 0.0106 (18) −0.0030 (13)
C25 0.072 (2) 0.066 (3) 0.0243 (14) 0.030 (3) 0.0160 (14) 0.0035 (15)
C26 0.050 (2) 0.0312 (17) 0.0356 (19) 0.0013 (19) 0.0119 (18) −0.0110 (15)
C24' 0.026 (2) 0.0248 (17) 0.0264 (14) −0.0041 (16) 0.0106 (18) −0.0030 (13)
C25' 0.072 (2) 0.066 (3) 0.0243 (14) 0.030 (3) 0.0160 (14) 0.0035 (15)
C26' 0.050 (2) 0.0312 (17) 0.0356 (19) 0.0013 (19) 0.0119 (18) −0.0110 (15)

Geometric parameters (Å, º)

S1—C9 1.668 (2) C12—H12 0.9500
S2—C18 1.685 (2) C13—C14 1.392 (3)
O1—C10 1.222 (2) C13—H13 0.9500
O2—C17 1.219 (2) C14—C15 1.396 (3)
N1—C9 1.331 (3) C14—H14 0.9500
N1—C1 1.470 (2) C15—C16 1.393 (3)
N1—C5 1.475 (2) C15—C17 1.501 (3)
N2—C10 1.379 (3) C16—H16 0.9500
N2—C9 1.419 (2) C19—C20 1.532 (3)
N2—H2 0.8800 C19—H19A 0.9900
N3—C17 1.374 (2) C19—H19B 0.9900
N3—C18 1.421 (2) C20—C22 1.524 (3)
N3—H3 0.8800 C20—C21 1.530 (3)
N4—C18 1.321 (3) C20—H20 1.0000
N4—C19 1.477 (2) C21—H21A 0.9800
N4—C23 1.485 (3) C21—H21B 0.9800
C1—C2 1.535 (3) C21—H21C 0.9800
C1—H1A 0.9900 C22—H22A 0.9800
C1—H1B 0.9900 C22—H22B 0.9800
C2—C3 1.519 (3) C22—H22C 0.9800
C3—H3A 0.9800 C23—C24 1.485 (4)
C3—H3B 0.9800 C23—C24' 1.556 (4)
C3—H3C 0.9800 C23—H23A 0.9900
C2—C4 1.530 (3) C23—H23B 0.9900
C2—H2A 1.0000 C23—H23C 0.9900
C4—H4A 0.9800 C23—H23D 0.9900
C4—H4B 0.9800 C24—C26 1.515 (6)
C4—H4C 0.9800 C24—C25 1.529 (8)
C5—C6 1.533 (3) C24—H24 1.0000
C5—H5A 0.9900 C25—H25A 0.9800
C5—H5B 0.9900 C25—H25B 0.9800
C6—C7 1.523 (3) C25—H25C 0.9800
C6—C8 1.528 (3) C26—H26A 0.9800
C6—H6 1.0000 C26—H26B 0.9800
C7—H7A 0.9800 C26—H26C 0.9800
C7—H7B 0.9800 C24'—C26' 1.463 (6)
C7—H7C 0.9800 C24'—C25' 1.547 (8)
C8—H8A 0.9800 C24'—H24' 1.0000
C8—H8B 0.9800 C25'—H25D 0.9800
C8—H8C 0.9800 C25'—H25E 0.9800
C10—C11 1.491 (3) C25'—H25F 0.9800
C11—C16 1.395 (3) C26'—H26D 0.9800
C11—C12 1.395 (3) C26'—H26E 0.9800
C12—C13 1.385 (3) C26'—H26F 0.9800
C9—N1—C1 119.61 (16) N3—C17—C15 114.39 (16)
C9—N1—C5 124.04 (16) N4—C18—N3 116.55 (17)
C1—N1—C5 116.23 (15) N4—C18—S2 127.12 (15)
C10—N2—C9 120.73 (16) N3—C18—S2 116.32 (14)
C10—N2—H2 119.6 N4—C19—C20 112.09 (16)
C9—N2—H2 119.6 N4—C19—H19A 109.2
C17—N3—C18 121.97 (16) C20—C19—H19A 109.2
C17—N3—H3 119.0 N4—C19—H19B 109.2
C18—N3—H3 119.0 C20—C19—H19B 109.2
C18—N4—C19 121.16 (17) H19A—C19—H19B 107.9
C18—N4—C23 122.92 (16) C22—C20—C21 111.05 (17)
C19—N4—C23 115.67 (16) C22—C20—C19 111.87 (17)
N1—C1—C2 112.50 (16) C21—C20—C19 108.17 (17)
N1—C1—H1A 109.1 C22—C20—H20 108.6
C2—C1—H1A 109.1 C21—C20—H20 108.6
N1—C1—H1B 109.1 C19—C20—H20 108.6
C2—C1—H1B 109.1 C20—C21—H21A 109.5
H1A—C1—H1B 107.8 C20—C21—H21B 109.5
C2—C3—H3A 109.5 H21A—C21—H21B 109.5
C2—C3—H3B 109.5 C20—C21—H21C 109.5
H3A—C3—H3B 109.5 H21A—C21—H21C 109.5
C2—C3—H3C 109.5 H21B—C21—H21C 109.5
H3A—C3—H3C 109.5 C20—C22—H22A 109.5
H3B—C3—H3C 109.5 C20—C22—H22B 109.5
C3—C2—C4 111.80 (19) H22A—C22—H22B 109.5
C3—C2—C1 112.21 (18) C20—C22—H22C 109.5
C4—C2—C1 108.81 (17) H22A—C22—H22C 109.5
C3—C2—H2A 108.0 H22B—C22—H22C 109.5
C4—C2—H2A 108.0 C24—C23—N4 116.0 (2)
C1—C2—H2A 108.0 C24—C23—C24' 27.3 (2)
C2—C4—H4A 109.5 N4—C23—C24' 111.1 (2)
C2—C4—H4B 109.5 C24—C23—H23A 108.3
H4A—C4—H4B 109.5 N4—C23—H23A 108.3
C2—C4—H4C 109.5 C24'—C23—H23A 131.6
H4A—C4—H4C 109.5 C24—C23—H23B 108.3
H4B—C4—H4C 109.5 N4—C23—H23B 108.3
N1—C5—C6 113.66 (17) C24'—C23—H23B 85.8
N1—C5—H5A 108.8 H23A—C23—H23B 107.4
C6—C5—H5A 108.8 C24—C23—H23C 126.2
N1—C5—H5B 108.8 N4—C23—H23C 109.4
C6—C5—H5B 108.8 C24'—C23—H23C 109.4
H5A—C5—H5B 107.7 H23A—C23—H23C 82.0
C7—C6—C8 111.48 (19) H23B—C23—H23C 26.8
C7—C6—C5 112.55 (18) C24—C23—H23D 82.9
C8—C6—C5 107.27 (18) N4—C23—H23D 109.4
C7—C6—H6 108.5 C24'—C23—H23D 109.4
C8—C6—H6 108.5 H23A—C23—H23D 28.7
C5—C6—H6 108.5 H23B—C23—H23D 130.0
C6—C7—H7A 109.5 H23C—C23—H23D 108.0
C6—C7—H7B 109.5 C23—C24—C26 109.5 (3)
H7A—C7—H7B 109.5 C23—C24—C25 108.2 (6)
C6—C7—H7C 109.5 C26—C24—C25 106.9 (7)
H7A—C7—H7C 109.5 C23—C24—H24 110.7
H7B—C7—H7C 109.5 C26—C24—H24 110.7
C6—C8—H8A 109.5 C25—C24—H24 110.7
C6—C8—H8B 109.5 C24—C25—H25A 109.5
H8A—C8—H8B 109.5 C24—C25—H25B 109.5
C6—C8—H8C 109.5 H25A—C25—H25B 109.5
H8A—C8—H8C 109.5 C24—C25—H25C 109.5
H8B—C8—H8C 109.5 H25A—C25—H25C 109.5
N1—C9—N2 115.45 (17) H25B—C25—H25C 109.5
N1—C9—S1 125.80 (15) C24—C26—H26A 109.5
N2—C9—S1 118.74 (15) C24—C26—H26B 109.5
O1—C10—N2 122.87 (18) H26A—C26—H26B 109.5
O1—C10—C11 121.82 (18) C24—C26—H26C 109.5
N2—C10—C11 115.26 (16) H26A—C26—H26C 109.5
C16—C11—C12 119.89 (18) H26B—C26—H26C 109.5
C16—C11—C10 121.58 (17) C26'—C24'—C25' 107.7 (7)
C12—C11—C10 118.41 (17) C26'—C24'—C23 114.8 (4)
C13—C12—C11 120.28 (18) C25'—C24'—C23 103.6 (5)
C13—C12—H12 119.9 C26'—C24'—H24' 110.1
C11—C12—H12 119.9 C25'—C24'—H24' 110.1
C12—C13—C14 119.94 (18) C23—C24'—H24' 110.1
C12—C13—H13 120.0 C24'—C25'—H25D 109.5
C14—C13—H13 120.0 C24'—C25'—H25E 109.5
C13—C14—C15 120.12 (18) H25D—C25'—H25E 109.5
C13—C14—H14 119.9 C24'—C25'—H25F 109.5
C15—C14—H14 119.9 H25D—C25'—H25F 109.5
C16—C15—C14 119.86 (17) H25E—C25'—H25F 109.5
C16—C15—C17 122.16 (17) C24'—C26'—H26D 109.5
C14—C15—C17 117.94 (17) C24'—C26'—H26E 109.5
C15—C16—C11 119.89 (17) H26D—C26'—H26E 109.5
C15—C16—H16 120.1 C24'—C26'—H26F 109.5
C11—C16—H16 120.1 H26D—C26'—H26F 109.5
O2—C17—N3 123.74 (17) H26E—C26'—H26F 109.5
O2—C17—C15 121.87 (17)
C9—N1—C1—C2 80.0 (2) C10—C11—C16—C15 175.89 (17)
C5—N1—C1—C2 −103.8 (2) C18—N3—C17—O2 12.4 (3)
N1—C1—C2—C3 62.2 (2) C18—N3—C17—C15 −167.52 (17)
N1—C1—C2—C4 −173.59 (18) C16—C15—C17—O2 142.2 (2)
C9—N1—C5—C6 96.8 (2) C14—C15—C17—O2 −35.2 (3)
C1—N1—C5—C6 −79.3 (2) C16—C15—C17—N3 −37.8 (3)
N1—C5—C6—C7 −57.2 (2) C14—C15—C17—N3 144.76 (18)
N1—C5—C6—C8 179.81 (17) C19—N4—C18—N3 172.06 (16)
C1—N1—C9—N2 −173.21 (16) C23—N4—C18—N3 −13.9 (3)
C5—N1—C9—N2 10.8 (3) C19—N4—C18—S2 −9.2 (3)
C1—N1—C9—S1 8.1 (3) C23—N4—C18—S2 164.81 (15)
C5—N1—C9—S1 −167.84 (15) C17—N3—C18—N4 −68.6 (2)
C10—N2—C9—N1 68.0 (2) C17—N3—C18—S2 112.56 (18)
C10—N2—C9—S1 −113.25 (18) C18—N4—C19—C20 −108.5 (2)
C9—N2—C10—O1 −1.9 (3) C23—N4—C19—C20 77.1 (2)
C9—N2—C10—C11 −179.25 (17) N4—C19—C20—C22 60.0 (2)
O1—C10—C11—C16 −148.7 (2) N4—C19—C20—C21 −177.34 (17)
N2—C10—C11—C16 28.7 (3) C18—N4—C23—C24 −65.4 (3)
O1—C10—C11—C12 27.3 (3) C19—N4—C23—C24 108.9 (3)
N2—C10—C11—C12 −155.33 (18) C18—N4—C23—C24' −94.8 (3)
C16—C11—C12—C13 −1.2 (3) C19—N4—C23—C24' 79.6 (3)
C10—C11—C12—C13 −177.27 (18) N4—C23—C24—C26 −56.3 (4)
C11—C12—C13—C14 1.7 (3) C24'—C23—C24—C26 29.6 (5)
C12—C13—C14—C15 −0.9 (3) N4—C23—C24—C25 −172.5 (8)
C13—C14—C15—C16 −0.3 (3) C24'—C23—C24—C25 −86.6 (10)
C13—C14—C15—C17 177.14 (18) C24—C23—C24'—C26' −58.2 (6)
C14—C15—C16—C11 0.8 (3) N4—C23—C24'—C26' 47.9 (4)
C17—C15—C16—C11 −176.57 (17) C24—C23—C24'—C25' 59.0 (10)
C12—C11—C16—C15 0.0 (3) N4—C23—C24'—C25' 165.1 (8)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N2—H2···S2i 0.88 2.62 3.4745 (17) 163
N3—H3···S2i 0.88 2.54 3.3870 (18) 162

Symmetry code: (i) −x+1, −y+1, −z+1.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG5336).

References

  1. Agilent (2013). CrysAlis PRO Agilent Technologies Inc., Santa Clara, CA, USA.
  2. Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
  3. Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.
  4. Nguyen, H. H., Thang, P. C., Rodenstein, A., Kirmse, R. & Abram, U. (2011). Inorg. Chem. 50, 590–596. [DOI] [PubMed]
  5. Rodenstein, A., Richter, R. & Kirmse, R. (2007). Z. Anorg. Allg. Chem. 633, 1713–1717.
  6. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  7. 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) general, I. DOI: 10.1107/S1600536813021053/hg5336sup1.cif

e-69-o1368-sup1.cif (28KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813021053/hg5336Isup2.hkl

e-69-o1368-Isup2.hkl (281.2KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536813021053/hg5336Isup3.cml

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


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