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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2013 Jun 29;69(Pt 7):o1183. doi: 10.1107/S1600536813017455

3-({[Bis(2-methyl­prop­yl)carbamo­thio­yl]amino}­carbon­yl)benzamide

N Selvakumaran a, R Karvembu a,, Seik Weng Ng b,c, Edward R T Tiekink b,*
PMCID: PMC3770438  PMID: 24046723

Abstract

In the title compound, C17H25N3O2S, the terminal and central amide groups are, respectively, twisted and coplanar with the attached benzene ring [O—C—C—C torsion angles = 22.7 (3) and 5.4 (3)°]. In the central part of the mol­ecule, the amide and thio­amide residues are approximately perpendicular [C—N—C—S torsion angle = −104.98 (18)°]. Supra­molecular layers with a zigzag topology are formed in the crystal packing by N—H⋯O, N—H⋯S and C—H⋯O inter­actions; these stack along c, being separated by hydro­phobic inter­actions.

Related literature  

For the preparation of bipodal acyl­thio­urea derivatives, see: Bourne et al. (2005). For a related structure, see: Selvakumaran et al. (2013).graphic file with name e-69-o1183-scheme1.jpg

Experimental  

Crystal data  

  • C17H25N3O2S

  • M r = 335.46

  • Orthorhombic, Inline graphic

  • a = 13.9870 (4) Å

  • b = 15.7103 (4) Å

  • c = 8.5532 (3) Å

  • V = 1879.48 (10) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.18 mm−1

  • T = 100 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, 2013) T min = 0.930, T max = 0.964

  • 6635 measured reflections

  • 4007 independent reflections

  • 3694 reflections with I > 2σ(I)

  • R int = 0.020

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.039

  • wR(F 2) = 0.097

  • S = 1.00

  • 4007 reflections

  • 218 parameters

  • 30 restraints

  • H-atom parameters constrained

  • Δρmax = 0.27 e Å−3

  • Δρmin = −0.24 e Å−3

  • Absolute structure: Flack (1983), 1590 Friedel pairs

  • Flack parameter: −0.03 (8)

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) global, I. DOI: 10.1107/S1600536813017455/hg5326sup1.cif

e-69-o1183-sup1.cif (22KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813017455/hg5326Isup2.hkl

e-69-o1183-Isup2.hkl (196.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536813017455/hg5326Isup3.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
N1—H12⋯O2i 0.88 2.09 2.887 (2) 150
N2—H2⋯O1ii 0.88 1.97 2.797 (2) 155
N1—H11⋯S1ii 0.88 2.54 3.3908 (18) 163
C7—H7⋯O1ii 0.95 2.32 3.210 (2) 155

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

NS thanks the 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/03).

supplementary crystallographic information

Comment

The title compound, (I), was obtained as a by-product in an attempt to prepare a bipodal acylthiourea derivative (Bourne et al., 2005) from diisobutylamine, isophthaloyl dichloride and potassium thiocyanate in acetone. Crystals were grown from a solution of the compound in acetonitrile/dimethyl formamide mixture (1:1). In (I), Fig. 1, the terminal [O1—C1—C2—C7 torsion angle = 22.7 (3)°] and central [C5—C6—C8—O2 = 5.4 (3)°] amide substituents are twisted and co-planar with the attached benzene ring, respectively. A twist is also noted between the amide and adjacent thioamide residues as seen in the C8—N2—C9—S1 torsion angle of -104.98 (18)°. The methylpropyl substituents lie to either side and are approximately perpendicular to the C3N plane with the C9—N3—C10—C11/C11' (50:50 disorder in the isopropyl group) torsion angles being 126.0 (3) and 87.5 (3)°, respectively, and 100.4 (2)° for C9—N3—C14—C1. The aforementioned conformation matches that found in the accompanying paper (Selvakumaran et al., 2013). In the crystal packing, supramolecular layers with a zigzag topology are formed by N—H···O, N—H···S and C—H···O interactions, Fig. 2 and Table 1. Layers stack along the c axis being separated by hydrophobic intertactions.

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 N2 atmosphere, in a three-necked round bottom flask. The mixture was heated to reflux for 30 minutes 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 at room temperature. Then, 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 acetonitrile/dimethyl formamide mixture (1:1) F T—IR (KBr): ν(NH2) 3217 & 3192, ν(N—H) 3405, ν(C═O) 1671 (with adjacent NH2), ν(C═O) 1652 (with adjacent NH), ν(C═C) 1593, ν(C═S) 1257 cm-1. UV-Visible (DMF): νmax; 264, 283, 363 nm.

Refinement

Carbon-bound H-atoms were placed in calculated positions [C—H = 0.95 to 1.00 Å, Uiso(H)= 1.2 to 1.5Ueq(C)] and were included in the refinement in the riding model approximation. The amino H-atoms were similarly constrained [N—H = 0.88 Å, and with Uiso(H)= 1.2Ueq(N)]. One isopropyl arm is disordered; the disorder refined to exactly 0.5. The 1,2-related distances were restrained to 1.54±0.01 Å and the 1,3-related ones to 2.51±0.01 Å. The anisotropic displacement parameters of the primed atoms were set to those of the unprimed ones, and the anisotropic displacement parameters were restrained to be nearly isotropic.

Figures

Fig. 1.

Fig. 1.

Molecular structure of (I) showing atom-labelling scheme and displacement ellipsoids at the 50% probability level.

Fig. 2.

Fig. 2.

A plan view of the zigzag supramolecular layer in (I). The N—H···O, N—H···S and C—H···O interactions are shown as blue, orange and purple dashed lines, respectively.

Fig. 3.

Fig. 3.

A view of the unit-cell contents in projection down the b axis in (I). The N—H···O, N—H···S and C—H···O interactions are shown as blue, orange and purple dashed lines, respectively.

Crystal data

C17H25N3O2S F(000) = 720
Mr = 335.46 Dx = 1.186 Mg m3
Orthorhombic, P21212 Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2 2ab Cell parameters from 3818 reflections
a = 13.9870 (4) Å θ = 2.4–29.3°
b = 15.7103 (4) Å µ = 0.18 mm1
c = 8.5532 (3) Å T = 100 K
V = 1879.48 (10) Å3 Block, colourless
Z = 4 0.40 × 0.30 × 0.20 mm

Data collection

Agilent SuperNova Dual diffractometer with an Atlas detector 4007 independent reflections
Radiation source: SuperNova (Mo) X-ray Source 3694 reflections with I > 2σ(I)
Mirror monochromator Rint = 0.020
Detector resolution: 10.4041 pixels mm-1 θmax = 27.5°, θmin = 2.4°
ω scan h = −17→18
Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2013) k = −17→20
Tmin = 0.930, Tmax = 0.964 l = −7→10
6635 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)] = 0.039 H-atom parameters constrained
wR(F2) = 0.097 w = 1/[σ2(Fo2) + (0.0461P)2 + 0.7082P] where P = (Fo2 + 2Fc2)/3
S = 1.00 (Δ/σ)max = 0.001
4007 reflections Δρmax = 0.27 e Å3
218 parameters Δρmin = −0.24 e Å3
30 restraints Absolute structure: Flack (1983), 1590 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: −0.03 (8)

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
S1 0.01768 (4) 0.15262 (3) 0.66311 (7) 0.03126 (14)
O1 0.05091 (10) 0.60837 (8) 0.73835 (19) 0.0262 (3)
O2 0.26459 (10) 0.25192 (9) 0.70500 (17) 0.0268 (3)
N1 0.12011 (13) 0.68211 (11) 0.5438 (2) 0.0311 (4)
H11 0.0791 0.7243 0.5533 0.037*
H12 0.1655 0.6846 0.4727 0.037*
N2 0.11244 (11) 0.28966 (10) 0.7599 (2) 0.0199 (3)
H2 0.0705 0.3307 0.7742 0.024*
N3 0.12403 (12) 0.17031 (10) 0.9200 (2) 0.0253 (4)
C1 0.11351 (14) 0.61468 (12) 0.6368 (2) 0.0222 (4)
C2 0.18533 (14) 0.54440 (12) 0.6160 (2) 0.0207 (4)
C3 0.27479 (14) 0.55770 (13) 0.5504 (3) 0.0247 (4)
H3 0.2921 0.6127 0.5136 0.030*
C4 0.33900 (16) 0.49082 (14) 0.5385 (3) 0.0299 (5)
H4 0.4006 0.5001 0.4948 0.036*
C5 0.31354 (15) 0.41050 (13) 0.5902 (3) 0.0260 (4)
H5 0.3578 0.3649 0.5817 0.031*
C6 0.22343 (13) 0.39591 (12) 0.6546 (2) 0.0204 (4)
C7 0.15980 (13) 0.46342 (12) 0.6693 (2) 0.0196 (4)
H7 0.0989 0.4545 0.7157 0.024*
C8 0.20241 (14) 0.30731 (12) 0.7075 (2) 0.0202 (4)
C9 0.08818 (13) 0.20345 (12) 0.7909 (2) 0.0221 (4)
C10 0.11303 (17) 0.07868 (12) 0.9522 (3) 0.0371 (6)
H10A 0.0508 0.0592 0.9102 0.045* 0.500 (4)
H10B 0.1122 0.0697 1.0668 0.045* 0.500 (4)
H10C 0.0696 0.0722 1.0429 0.045* 0.500 (4)
H10D 0.0812 0.0522 0.8611 0.045* 0.500 (4)
C11 0.1901 (3) 0.0265 (3) 0.8831 (6) 0.0295 (8) 0.500 (4)
H11A 0.1766 0.0275 0.7683 0.035* 0.500 (4)
C12 0.1752 (7) −0.0672 (4) 0.9301 (7) 0.0374 (13) 0.500 (4)
H12A 0.1078 −0.0765 0.9566 0.056* 0.500 (4)
H12B 0.2152 −0.0805 1.0209 0.056* 0.500 (4)
H12C 0.1930 −0.1042 0.8426 0.056* 0.500 (4)
C13 0.2851 (7) 0.0534 (13) 0.895 (3) 0.0506 (12) 0.500 (4)
H13A 0.2886 0.1149 0.8759 0.076* 0.500 (4)
H13B 0.3241 0.0234 0.8175 0.076* 0.500 (4)
H13C 0.3092 0.0409 1.0002 0.076* 0.500 (4)
C11' 0.2013 (3) 0.0304 (3) 0.9852 (6) 0.0295 (8) 0.50
H11' 0.2189 0.0473 1.0942 0.035* 0.500 (4)
C12' 0.1753 (7) −0.0640 (4) 0.9979 (7) 0.0374 (13) 0.50
H12D 0.1074 −0.0696 1.0237 0.056* 0.500 (4)
H12E 0.2139 −0.0906 1.0801 0.056* 0.500 (4)
H12F 0.1881 −0.0922 0.8978 0.056* 0.500 (4)
C13' 0.2927 (7) 0.0473 (13) 0.889 (3) 0.0506 (12) 0.50
H13D 0.2991 0.1085 0.8696 0.076* 0.500 (4)
H13E 0.2883 0.0172 0.7886 0.076* 0.500 (4)
H13F 0.3485 0.0268 0.9467 0.076* 0.500 (4)
C14 0.16514 (15) 0.22155 (13) 1.0474 (3) 0.0274 (5)
H14A 0.1832 0.2782 1.0063 0.033*
H14B 0.2240 0.1935 1.0861 0.033*
C15 0.09549 (17) 0.23284 (18) 1.1831 (3) 0.0410 (6)
H15 0.0827 0.1756 1.2298 0.049*
C16 0.00072 (19) 0.2703 (2) 1.1290 (3) 0.0612 (9)
H16A −0.0273 0.2335 1.0486 0.092*
H16B 0.0116 0.3272 1.0854 0.092*
H16C −0.0431 0.2744 1.2181 0.092*
C17 0.1423 (2) 0.28857 (19) 1.3076 (3) 0.0475 (7)
H17A 0.2021 0.2622 1.3421 0.071*
H17B 0.0989 0.2944 1.3971 0.071*
H17C 0.1557 0.3449 1.2638 0.071*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0270 (3) 0.0254 (2) 0.0414 (3) −0.0024 (2) −0.0020 (2) −0.0130 (2)
O1 0.0196 (6) 0.0223 (7) 0.0367 (9) 0.0022 (6) 0.0062 (6) 0.0054 (6)
O2 0.0231 (7) 0.0245 (7) 0.0329 (9) 0.0073 (6) 0.0058 (6) 0.0032 (6)
N1 0.0249 (9) 0.0254 (8) 0.0431 (12) 0.0041 (7) 0.0082 (8) 0.0128 (8)
N2 0.0163 (7) 0.0166 (7) 0.0268 (9) 0.0017 (6) 0.0003 (7) −0.0011 (7)
N3 0.0212 (8) 0.0179 (8) 0.0370 (10) −0.0007 (6) −0.0017 (7) 0.0028 (7)
C1 0.0179 (9) 0.0216 (9) 0.0272 (11) −0.0012 (8) −0.0013 (8) 0.0026 (8)
C2 0.0189 (9) 0.0230 (9) 0.0202 (10) 0.0002 (8) −0.0005 (7) 0.0013 (8)
C3 0.0226 (9) 0.0235 (9) 0.0280 (11) −0.0006 (8) 0.0041 (8) 0.0051 (9)
C4 0.0213 (10) 0.0330 (11) 0.0354 (12) −0.0006 (9) 0.0101 (10) 0.0022 (10)
C5 0.0233 (10) 0.0241 (10) 0.0307 (12) 0.0052 (8) 0.0055 (9) 0.0014 (9)
C6 0.0200 (9) 0.0227 (9) 0.0186 (9) 0.0006 (7) −0.0002 (8) 0.0008 (8)
C7 0.0176 (8) 0.0218 (9) 0.0196 (9) −0.0002 (7) −0.0002 (8) 0.0001 (8)
C8 0.0213 (9) 0.0221 (9) 0.0173 (10) 0.0021 (8) −0.0012 (7) −0.0019 (7)
C9 0.0174 (8) 0.0176 (9) 0.0312 (12) 0.0027 (7) 0.0045 (8) −0.0034 (8)
C10 0.0390 (13) 0.0167 (10) 0.0556 (16) 0.0022 (9) 0.0046 (12) 0.0065 (10)
C11 0.0374 (17) 0.0237 (13) 0.0274 (17) 0.0075 (12) −0.0093 (16) 0.0005 (16)
C12 0.0503 (17) 0.0218 (13) 0.040 (4) 0.0101 (12) −0.019 (4) −0.004 (3)
C13 0.0451 (18) 0.042 (2) 0.065 (2) 0.0223 (19) 0.0127 (18) 0.0127 (18)
C11' 0.0374 (17) 0.0237 (13) 0.0274 (17) 0.0075 (12) −0.0093 (16) 0.0005 (16)
C12' 0.0503 (17) 0.0218 (13) 0.040 (4) 0.0101 (12) −0.019 (4) −0.004 (3)
C13' 0.0451 (18) 0.042 (2) 0.065 (2) 0.0223 (19) 0.0127 (18) 0.0127 (18)
C14 0.0238 (10) 0.0267 (10) 0.0318 (12) −0.0025 (8) −0.0064 (9) 0.0066 (9)
C15 0.0399 (13) 0.0582 (16) 0.0249 (12) −0.0110 (12) −0.0014 (11) 0.0082 (11)
C16 0.0314 (13) 0.117 (3) 0.0349 (15) 0.0081 (16) 0.0033 (11) −0.0206 (16)
C17 0.0487 (15) 0.0643 (17) 0.0297 (14) −0.0072 (13) −0.0058 (12) 0.0027 (12)

Geometric parameters (Å, º)

S1—C9 1.675 (2) C11—C13 1.398 (13)
O1—C1 1.237 (2) C11—C12 1.540 (7)
O2—C8 1.230 (2) C11—H11A 1.0000
N1—C1 1.328 (3) C12—H12A 0.9800
N1—H11 0.8800 C12—H12B 0.9800
N1—H12 0.8800 C12—H12C 0.9800
N2—C8 1.364 (2) C13—H13A 0.9800
N2—C9 1.421 (2) C13—H13B 0.9800
N2—H2 0.8800 C13—H13C 0.9800
N3—C9 1.320 (3) C11'—C13' 1.545 (9)
N3—C14 1.472 (3) C11'—C12' 1.531 (6)
N3—C10 1.474 (2) C11'—H11' 1.0000
C1—C2 1.503 (3) C12'—H12D 0.9800
C2—C3 1.387 (3) C12'—H12E 0.9800
C2—C7 1.398 (3) C12'—H12F 0.9800
C3—C4 1.386 (3) C13'—H13D 0.9800
C3—H3 0.9500 C13'—H13E 0.9800
C4—C5 1.384 (3) C13'—H13F 0.9800
C4—H4 0.9500 C14—C15 1.525 (3)
C5—C6 1.394 (3) C14—H14A 0.9900
C5—H5 0.9500 C14—H14B 0.9900
C6—C7 1.390 (3) C15—C17 1.526 (4)
C6—C8 1.493 (3) C15—C16 1.523 (4)
C7—H7 0.9500 C15—H15 1.0000
C10—C11' 1.475 (4) C16—H16A 0.9800
C10—C11 1.478 (5) C16—H16B 0.9800
C10—H10A 0.9900 C16—H16C 0.9800
C10—H10B 0.9900 C17—H17A 0.9800
C10—H10C 0.9900 C17—H17B 0.9800
C10—H10D 0.9900 C17—H17C 0.9800
C1—N1—H11 120.0 C11—C12—H12A 109.5
C1—N1—H12 120.0 C11—C12—H12B 109.5
H11—N1—H12 120.0 H12A—C12—H12B 109.5
C8—N2—C9 118.37 (16) C11—C12—H12C 109.5
C8—N2—H2 120.8 H12A—C12—H12C 109.5
C9—N2—H2 120.8 H12B—C12—H12C 109.5
C9—N3—C14 123.52 (16) C11—C13—H13A 109.5
C9—N3—C10 120.15 (19) C11—C13—H13B 109.5
C14—N3—C10 115.87 (19) H13A—C13—H13B 109.5
O1—C1—N1 122.25 (18) C11—C13—H13C 109.5
O1—C1—C2 119.81 (17) H13A—C13—H13C 109.5
N1—C1—C2 117.94 (18) H13B—C13—H13C 109.5
C3—C2—C7 119.97 (18) C10—C11'—C13' 120.2 (8)
C3—C2—C1 122.69 (17) C10—C11'—C12' 108.2 (4)
C7—C2—C1 117.33 (17) C13'—C11'—C12' 113.6 (8)
C2—C3—C4 120.00 (19) C10—C11'—H11' 104.4
C2—C3—H3 120.0 C13'—C11'—H11' 104.4
C4—C3—H3 120.0 C12'—C11'—H11' 104.4
C5—C4—C3 120.08 (19) C11'—C12'—H12D 109.5
C5—C4—H4 120.0 C11'—C12'—H12E 109.5
C3—C4—H4 120.0 H12D—C12'—H12E 109.5
C4—C5—C6 120.58 (19) C11'—C12'—H12F 109.5
C4—C5—H5 119.7 H12D—C12'—H12F 109.5
C6—C5—H5 119.7 H12E—C12'—H12F 109.5
C7—C6—C5 119.28 (18) C11'—C13'—H13D 109.5
C7—C6—C8 123.91 (17) C11'—C13'—H13E 109.5
C5—C6—C8 116.80 (17) H13D—C13'—H13E 109.5
C6—C7—C2 120.08 (18) C11'—C13'—H13F 109.5
C6—C7—H7 120.0 H13D—C13'—H13F 109.5
C2—C7—H7 120.0 H13E—C13'—H13F 109.5
O2—C8—N2 120.92 (18) N3—C14—C15 112.17 (18)
O2—C8—C6 120.99 (17) N3—C14—H14A 109.2
N2—C8—C6 118.08 (16) C15—C14—H14A 109.2
N3—C9—N2 116.19 (17) N3—C14—H14B 109.2
N3—C9—S1 125.57 (15) C15—C14—H14B 109.2
N2—C9—S1 118.24 (16) H14A—C14—H14B 107.9
C11'—C10—N3 116.8 (2) C14—C15—C17 108.9 (2)
N3—C10—C11 113.0 (2) C14—C15—C16 111.7 (2)
N3—C10—H10A 109.0 C17—C15—C16 111.3 (2)
C11—C10—H10A 109.0 C14—C15—H15 108.3
N3—C10—H10B 109.0 C17—C15—H15 108.3
C11—C10—H10B 109.0 C16—C15—H15 108.3
H10A—C10—H10B 107.8 C15—C16—H16A 109.5
C11'—C10—H10C 108.1 C15—C16—H16B 109.5
N3—C10—H10C 108.1 H16A—C16—H16B 109.5
C11'—C10—H10D 108.1 C15—C16—H16C 109.5
N3—C10—H10D 108.1 H16A—C16—H16C 109.5
H10C—C10—H10D 107.3 H16B—C16—H16C 109.5
C13—C11—C10 119.7 (9) C15—C17—H17A 109.5
C13—C11—C12 113.5 (9) C15—C17—H17B 109.5
C10—C11—C12 109.1 (4) H17A—C17—H17B 109.5
C13—C11—H11A 104.2 C15—C17—H17C 109.5
C10—C11—H11A 104.2 H17A—C17—H17C 109.5
C12—C11—H11A 104.2 H17B—C17—H17C 109.5
O1—C1—C2—C3 −155.8 (2) C10—N3—C9—N2 −172.35 (18)
N1—C1—C2—C3 24.2 (3) C14—N3—C9—S1 −164.30 (16)
O1—C1—C2—C7 22.7 (3) C10—N3—C9—S1 7.6 (3)
N1—C1—C2—C7 −157.3 (2) C8—N2—C9—N3 75.0 (2)
C7—C2—C3—C4 −0.3 (3) C8—N2—C9—S1 −104.98 (18)
C1—C2—C3—C4 178.1 (2) C9—N3—C10—C11' 126.0 (3)
C2—C3—C4—C5 0.8 (4) C14—N3—C10—C11' −61.5 (3)
C3—C4—C5—C6 0.0 (4) C9—N3—C10—C11 87.5 (3)
C4—C5—C6—C7 −1.2 (3) C14—N3—C10—C11 −100.0 (3)
C4—C5—C6—C8 −179.8 (2) C11'—C10—C11—C13 −60.3 (12)
C5—C6—C7—C2 1.7 (3) N3—C10—C11—C13 44.0 (12)
C8—C6—C7—C2 −179.77 (19) C11'—C10—C11—C12 72.9 (5)
C3—C2—C7—C6 −1.0 (3) N3—C10—C11—C12 177.1 (4)
C1—C2—C7—C6 −179.47 (18) N3—C10—C11'—C13' −41.3 (10)
C9—N2—C8—O2 −8.7 (3) C11—C10—C11'—C13' 51.2 (9)
C9—N2—C8—C6 171.83 (18) N3—C10—C11'—C12' −174.1 (4)
C7—C6—C8—O2 −173.1 (2) C11—C10—C11'—C12' −81.5 (5)
C5—C6—C8—O2 5.4 (3) C9—N3—C14—C15 100.4 (2)
C7—C6—C8—N2 6.4 (3) C10—N3—C14—C15 −71.8 (2)
C5—C6—C8—N2 −175.10 (19) N3—C14—C15—C17 −178.37 (19)
C14—N3—C9—N2 15.8 (3) N3—C14—C15—C16 −55.0 (3)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N1—H12···O2i 0.88 2.09 2.887 (2) 150
N2—H2···O1ii 0.88 1.97 2.797 (2) 155
N1—H11···S1ii 0.88 2.54 3.3908 (18) 163
C7—H7···O1ii 0.95 2.32 3.210 (2) 155

Symmetry codes: (i) −x+1/2, y+1/2, −z+1; (ii) −x, −y+1, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HG5326).

References

  1. Agilent (2013). CrysAlis PRO Agilent Technologies Inc., Santa Clara, CA, USA.
  2. Bourne, S. A., Hallale, O. & Koch, K. R. (2005). Cryst. Growth Des. 5, 307–312.
  3. Brandenburg, K. (2006). DIAMOND Crystal Impact GbR, Bonn, Germany.
  4. Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.
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  6. Selvakumaran, N., Karvembu, R., Ng, S. W. & Tiekink, E. R. T. (2013). Acta Cryst. E69, o1184–o1185. [DOI] [PMC free article] [PubMed]
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  8. 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/S1600536813017455/hg5326sup1.cif

e-69-o1183-sup1.cif (22KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813017455/hg5326Isup2.hkl

e-69-o1183-Isup2.hkl (196.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536813017455/hg5326Isup3.cml

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


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