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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 7;67(Pt 5):o1043. doi: 10.1107/S1600536811011822

1-Tosyl-2-[(1-tosyl-1H-benzimidazol-2-yl)methyl­sulfanyl]-1H-benzimidazole

Nassir N Al-Mohammed a,, Yatimah Alias a, Zanariah Abdullah a, Hamid Khaledi a,*
PMCID: PMC3089064  PMID: 21754370

Abstract

In the title compound, C29H24N4O4S3, the two N-tosyl­benzimidazolyl unit are connected through a —S—CH2— fragment, the dihedral angle between the benzimidazole rings being 76.09 (5)°. The methyl­thio group is disordered with respect to exchange of the S and C atoms in a 0.547 (4):0.453 (4) ratio. In the crystal, C—H⋯O and C—H⋯π inter­actions connect adjacent mol­ecules into infinite layers parallel to the ab plane. The crystal packing is further stabilized by a π–π inter­action [centroid–centroid separation = 3.5187 (4) Å].

Related literature

For the structures of similar compounds, see: Hayashi et al. (2008); Rashid et al. (2006, 2007).graphic file with name e-67-o1043-scheme1.jpg

Experimental

Crystal data

  • C29H24N4O4S3

  • M r = 588.70

  • Triclinic, Inline graphic

  • a = 8.2524 (6) Å

  • b = 13.5905 (10) Å

  • c = 13.8117 (10) Å

  • α = 62.5191 (8)°

  • β = 75.4090 (9)°

  • γ = 85.9930 (9)°

  • V = 1327.99 (17) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.32 mm−1

  • T = 100 K

  • 0.38 × 0.35 × 0.21 mm

Data collection

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.887, T max = 0.935

  • 8528 measured reflections

  • 4762 independent reflections

  • 4405 reflections with I > 2σ(I)

  • R int = 0.017

Refinement

  • R[F 2 > 2σ(F 2)] = 0.039

  • wR(F 2) = 0.117

  • S = 1.05

  • 4762 reflections

  • 382 parameters

  • 4 restraints

  • H-atom parameters constrained

  • Δρmax = 0.29 e Å−3

  • Δρmin = −0.41 e Å−3

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: X-SEED (Barbour, 2001); software used to prepare material for publication: SHELXL97 and publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811011822/pv2404sup1.cif

e-67-o1043-sup1.cif (23.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811011822/pv2404Isup2.hkl

e-67-o1043-Isup2.hkl (233.2KB, hkl)

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

Table 1. Hydrogen-bond geometry (Å, °).

Cg1 and Cg2 are the centroids of the C8–C13 and C23–C28 rings, respectively.

D—H⋯A D—H H⋯A DA D—H⋯A
C6—H6⋯O4i 0.95 2.48 3.314 (3) 147
C20—H20⋯O3ii 0.95 2.46 3.386 (3) 164
C25—H25⋯Cg1iii 0.95 2.99 3.744 (3) 138
C15—H15ACg2iv 0.99 2.98 3.62 (2) 124

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

Acknowledgments

The authors thank the University of Malaya for funding this study (FRGS grant No. FP001/2010 A).

supplementary crystallographic information

Comment

The title compound (Fig. 1) is the N-tosylation product of 2-(thiomethyl-2'-benzimidazolyl)-benzimidazole. The two benzimidazolyl rings are connected through the methythio fragment, making a dihedral angle of 76.09 (5)°. The two N-bound tosyl groups and the benzimidazolyl rings subtend angles of 103.77 (10)° at S1 and 104.48 (10)° at S3 atoms. These values are comparable to those reported for similar structures (Hayashi et al., 2008; Rashid et al., 2006; Rashid et al., 2007). In the crystal, intermolecular C—H···O and C—H···π interactions link the adjacent molecules into polymeric layers parallel to the ab plane. The crystal packing is further stabilized by a π—π interaction formed by the six-membered rings (C8—C13) of anti-parallelly arranged benzimidazole rings related by symmetry of -x, -y, -z + 1 [centroids separation = 3.5187 (4) Å]. Moreover, intramolecular C—H···O and C—H···N hydrogen bonding occurs (Table 1).

Experimental

Sodium (0.17 g) was added to a solution of 2-mercaptobenzimidazole (1 g, 6.7 mmol) in anhydrous methanol (20 ml) and the mixture was stirred at room temperature for 20 minutes. To the mixture, 2-chloromethylbenzimidazole (1.11 g, 6.67 mmol) was added dropwise under vigorous stirring, and then left to stir overnight. The solvent was removed under reduced pressure and the remaining liquid was washed with water and crystallized from tetrahydrofuran (THF) to give the white solid of 2-(thiomethyl-2'-benzimidazolyl)-benzimidazole. A solution of p-toluene sulfonyl chloride (0.75 g, 3.91 mmol) in pyridine (5 ml) was added dropwise to a solution of 2-(thiomethyl-2'-benzimidazolyl)-benzimidazole (0.5 g, 1.78 mmol) in pyridine (5 ml) at 273 K, within 2 hr. The mixture was stirred at room temperature overnight and then poured into a beaker containg 100 ml ice water. It was then stirred for another 15 minutes, extracted with dichloromethane and washed with distilled water (3 x 10 ml). The organic layer was dried with magnesium sulfate and evaporated. The obtained solid was recrystallized from toluene to give the colorless crystals of the title compound.

Refinement

Hydrogen atoms were placed at calculated positions at distances C—H = 0.95, 0.98 and 0.99 Å for aryl, methyl and methylene type H-atoms, respectively, and were treated as riding on their parent atoms, with Uiso(H) = 1.2–1.5 times Ueq(C). S2—C15 fragment was found to be disordered over two positions. From anisotropic refinement, the major component of the disorder had a site occupancy factor of 0.547 (4). The corrsponding bond distances involving the disordred groups were restrained to be equal by the SADI command in SHELXL97 (Sheldrick, 2008).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound showing displacement ellipsoids at the 50% probability level. Hydrogen atoms are drawn as spheres of arbitrary radius. Only the major component of the disordered methylthio group is depicted.

Crystal data

C29H24N4O4S3 Z = 2
Mr = 588.70 F(000) = 612
Triclinic, P1 Dx = 1.472 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.2524 (6) Å Cell parameters from 6545 reflections
b = 13.5905 (10) Å θ = 2.6–29.6°
c = 13.8117 (10) Å µ = 0.32 mm1
α = 62.5191 (8)° T = 100 K
β = 75.4090 (9)° Block, colorless
γ = 85.9930 (9)° 0.38 × 0.35 × 0.21 mm
V = 1327.99 (17) Å3

Data collection

Bruker APEXII CCD diffractometer 4762 independent reflections
Radiation source: fine-focus sealed tube 4405 reflections with I > 2σ(I)
graphite Rint = 0.017
φ and ω scans θmax = 25.3°, θmin = 2.6°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −9→8
Tmin = 0.887, Tmax = 0.935 k = −15→16
8528 measured reflections l = −16→16

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) = 0.117 H-atom parameters constrained
S = 1.05 w = 1/[σ2(Fo2) + (0.0548P)2 + 1.7481P] where P = (Fo2 + 2Fc2)/3
4762 reflections (Δ/σ)max < 0.001
382 parameters Δρmax = 0.29 e Å3
4 restraints Δρmin = −0.41 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 0.38609 (8) 0.01814 (5) 0.23234 (5) 0.02441 (16)
S2 0.4294 (5) 0.3694 (3) 0.2743 (3) 0.0161 (5) 0.547 (4)
C15 0.445 (2) 0.2467 (15) 0.257 (2) 0.020 (4) 0.547 (4)
H15A 0.4941 0.2670 0.1768 0.024* 0.547 (4)
H15B 0.5227 0.1974 0.3007 0.024* 0.547 (4)
S2' 0.4759 (8) 0.2429 (4) 0.2489 (6) 0.0158 (7) 0.453 (4)
C15' 0.419 (3) 0.3702 (15) 0.2508 (16) 0.032 (4) 0.453 (4)
H15C 0.3390 0.3536 0.3238 0.039* 0.453 (4)
H15D 0.5210 0.4076 0.2474 0.039* 0.453 (4)
S3 0.22947 (7) 0.59437 (4) 0.24425 (5) 0.01762 (15)
O1 0.3429 (3) −0.09759 (15) 0.30145 (16) 0.0368 (5)
O2 0.5483 (2) 0.06264 (16) 0.21509 (16) 0.0325 (4)
O3 0.3524 (2) 0.55663 (14) 0.30806 (14) 0.0240 (4)
O4 0.2006 (2) 0.70985 (13) 0.18860 (15) 0.0247 (4)
N1 0.2505 (2) 0.08379 (15) 0.29227 (16) 0.0194 (4)
N2 0.1401 (2) 0.21679 (15) 0.33908 (15) 0.0176 (4)
N3 0.2886 (2) 0.55596 (15) 0.14188 (15) 0.0171 (4)
N4 0.3248 (2) 0.42440 (15) 0.08180 (16) 0.0184 (4)
C1 0.3376 (3) 0.05944 (19) 0.10314 (19) 0.0196 (5)
C2 0.3707 (3) 0.1693 (2) 0.0204 (2) 0.0245 (5)
H2 0.4191 0.2222 0.0334 0.029*
C3 0.3317 (3) 0.2000 (2) −0.0811 (2) 0.0258 (5)
H3 0.3539 0.2748 −0.1382 0.031*
C4 0.2606 (3) 0.1234 (2) −0.1015 (2) 0.0217 (5)
C5 0.2307 (3) 0.0143 (2) −0.0176 (2) 0.0248 (5)
H5 0.1836 −0.0389 −0.0307 0.030*
C6 0.2683 (3) −0.01874 (19) 0.0852 (2) 0.0238 (5)
H6 0.2470 −0.0937 0.1421 0.029*
C7 0.2154 (3) 0.1571 (2) −0.2115 (2) 0.0275 (5)
H7A 0.2293 0.0947 −0.2295 0.041*
H7B 0.2890 0.2206 −0.2717 0.041*
H7C 0.0985 0.1779 −0.2049 0.041*
C8 0.0772 (3) 0.05618 (19) 0.33644 (18) 0.0209 (5)
C9 −0.0229 (3) −0.0310 (2) 0.3535 (2) 0.0291 (6)
H9 0.0219 −0.0873 0.3336 0.035*
C10 −0.1929 (4) −0.0311 (2) 0.4016 (2) 0.0347 (7)
H10 −0.2666 −0.0886 0.4139 0.042*
C11 −0.2576 (3) 0.0506 (2) 0.4321 (2) 0.0301 (6)
H11 −0.3740 0.0469 0.4659 0.036*
C12 −0.1562 (3) 0.1371 (2) 0.41446 (19) 0.0245 (5)
H12 −0.2009 0.1931 0.4350 0.029*
C13 0.0131 (3) 0.13913 (18) 0.36571 (18) 0.0186 (5)
C14 0.2774 (3) 0.18328 (18) 0.29586 (18) 0.0173 (4)
C16 0.0379 (3) 0.51977 (18) 0.32649 (18) 0.0158 (4)
C17 0.0298 (3) 0.42479 (19) 0.42717 (19) 0.0205 (5)
H17 0.1282 0.3987 0.4532 0.025*
C18 −0.1247 (3) 0.36822 (19) 0.48967 (19) 0.0215 (5)
H18 −0.1316 0.3031 0.5591 0.026*
C19 −0.2696 (3) 0.40555 (18) 0.45200 (19) 0.0191 (5)
C20 −0.2574 (3) 0.50082 (19) 0.34960 (19) 0.0198 (5)
H20 −0.3552 0.5264 0.3227 0.024*
C21 −0.1050 (3) 0.55858 (18) 0.28654 (19) 0.0185 (5)
H21 −0.0977 0.6237 0.2171 0.022*
C22 −0.4367 (3) 0.3441 (2) 0.5213 (2) 0.0242 (5)
H22A −0.5272 0.3933 0.4979 0.036*
H22B −0.4454 0.3201 0.6012 0.036*
H22C −0.4463 0.2789 0.5099 0.036*
C23 0.2228 (3) 0.59687 (18) 0.04581 (18) 0.0180 (5)
C24 0.1482 (3) 0.69526 (19) −0.0111 (2) 0.0235 (5)
H24 0.1322 0.7512 0.0130 0.028*
C25 0.0988 (3) 0.7073 (2) −0.1043 (2) 0.0270 (5)
H25 0.0469 0.7731 −0.1450 0.032*
C26 0.1228 (3) 0.6259 (2) −0.1402 (2) 0.0260 (5)
H26 0.0863 0.6368 −0.2043 0.031*
C27 0.1992 (3) 0.5289 (2) −0.08383 (19) 0.0227 (5)
H27 0.2167 0.4736 −0.1088 0.027*
C28 0.2491 (3) 0.51520 (18) 0.01016 (18) 0.0178 (5)
C29 0.3434 (3) 0.44894 (18) 0.15870 (18) 0.0169 (4)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0326 (3) 0.0210 (3) 0.0251 (3) 0.0125 (2) −0.0141 (3) −0.0131 (3)
S2 0.0151 (7) 0.0142 (7) 0.0176 (12) 0.0017 (5) −0.0032 (8) −0.0068 (6)
C15 0.015 (7) 0.018 (4) 0.016 (5) 0.010 (3) −0.002 (4) −0.002 (3)
S2' 0.0114 (15) 0.0158 (12) 0.0196 (14) 0.0021 (10) −0.0037 (12) −0.0078 (9)
C15' 0.036 (8) 0.032 (5) 0.026 (8) −0.008 (4) 0.007 (4) −0.017 (5)
S3 0.0140 (3) 0.0182 (3) 0.0225 (3) 0.0000 (2) −0.0041 (2) −0.0110 (2)
O1 0.0639 (14) 0.0200 (9) 0.0298 (10) 0.0163 (9) −0.0213 (9) −0.0112 (8)
O2 0.0270 (9) 0.0440 (11) 0.0452 (11) 0.0198 (8) −0.0213 (8) −0.0320 (10)
O3 0.0165 (8) 0.0313 (9) 0.0294 (9) 0.0016 (7) −0.0076 (7) −0.0174 (8)
O4 0.0230 (9) 0.0179 (8) 0.0325 (9) −0.0025 (7) −0.0036 (7) −0.0122 (7)
N1 0.0219 (10) 0.0167 (9) 0.0209 (10) 0.0049 (7) −0.0082 (8) −0.0088 (8)
N2 0.0157 (9) 0.0158 (9) 0.0177 (9) 0.0000 (7) −0.0035 (7) −0.0050 (8)
N3 0.0153 (9) 0.0166 (9) 0.0171 (9) 0.0006 (7) −0.0021 (7) −0.0067 (8)
N4 0.0142 (9) 0.0180 (9) 0.0198 (9) −0.0022 (7) −0.0011 (7) −0.0071 (8)
C1 0.0218 (12) 0.0194 (11) 0.0198 (11) 0.0059 (9) −0.0062 (9) −0.0110 (9)
C2 0.0289 (13) 0.0197 (12) 0.0288 (13) −0.0003 (10) −0.0117 (10) −0.0120 (10)
C3 0.0284 (13) 0.0200 (12) 0.0263 (12) 0.0011 (10) −0.0088 (10) −0.0075 (10)
C4 0.0181 (11) 0.0273 (12) 0.0221 (12) 0.0065 (9) −0.0041 (9) −0.0146 (10)
C5 0.0266 (12) 0.0239 (12) 0.0290 (13) 0.0002 (10) −0.0054 (10) −0.0171 (11)
C6 0.0288 (13) 0.0168 (11) 0.0244 (12) 0.0006 (9) −0.0027 (10) −0.0102 (10)
C7 0.0286 (13) 0.0326 (14) 0.0274 (13) 0.0086 (11) −0.0106 (11) −0.0178 (11)
C8 0.0248 (12) 0.0201 (11) 0.0142 (10) −0.0011 (9) −0.0076 (9) −0.0033 (9)
C9 0.0387 (15) 0.0221 (12) 0.0271 (13) −0.0040 (11) −0.0153 (11) −0.0076 (10)
C10 0.0416 (16) 0.0285 (14) 0.0280 (13) −0.0144 (12) −0.0202 (12) −0.0001 (11)
C11 0.0243 (13) 0.0377 (15) 0.0181 (12) −0.0101 (11) −0.0070 (10) −0.0020 (11)
C12 0.0208 (12) 0.0291 (13) 0.0166 (11) −0.0051 (10) −0.0034 (9) −0.0045 (10)
C13 0.0195 (11) 0.0170 (11) 0.0145 (10) −0.0019 (9) −0.0067 (9) −0.0018 (9)
C14 0.0193 (11) 0.0161 (11) 0.0140 (10) 0.0029 (8) −0.0052 (8) −0.0045 (9)
C16 0.0141 (10) 0.0180 (11) 0.0194 (11) 0.0018 (8) −0.0038 (8) −0.0123 (9)
C17 0.0164 (11) 0.0234 (12) 0.0215 (11) 0.0046 (9) −0.0048 (9) −0.0105 (10)
C18 0.0224 (12) 0.0190 (11) 0.0191 (11) 0.0028 (9) −0.0054 (9) −0.0056 (9)
C19 0.0185 (11) 0.0176 (11) 0.0223 (11) −0.0008 (9) −0.0016 (9) −0.0118 (9)
C20 0.0171 (11) 0.0233 (12) 0.0225 (11) 0.0039 (9) −0.0071 (9) −0.0127 (10)
C21 0.0176 (11) 0.0165 (11) 0.0203 (11) 0.0015 (9) −0.0036 (9) −0.0081 (9)
C22 0.0188 (12) 0.0233 (12) 0.0271 (12) 0.0012 (9) −0.0030 (10) −0.0102 (10)
C23 0.0138 (10) 0.0181 (11) 0.0148 (10) −0.0026 (8) −0.0014 (8) −0.0023 (9)
C24 0.0208 (12) 0.0194 (12) 0.0234 (12) 0.0031 (9) −0.0035 (9) −0.0055 (10)
C25 0.0226 (12) 0.0248 (13) 0.0199 (12) 0.0019 (10) −0.0055 (10) 0.0010 (10)
C26 0.0171 (11) 0.0336 (14) 0.0176 (11) −0.0034 (10) −0.0034 (9) −0.0034 (10)
C27 0.0157 (11) 0.0273 (13) 0.0207 (11) −0.0042 (9) −0.0001 (9) −0.0088 (10)
C28 0.0122 (10) 0.0180 (11) 0.0171 (10) −0.0035 (8) 0.0004 (8) −0.0044 (9)
C29 0.0115 (10) 0.0157 (11) 0.0163 (10) −0.0014 (8) 0.0015 (8) −0.0037 (9)

Geometric parameters (Å, °)

S1—O1 1.4260 (19) C7—H7A 0.9800
S1—O2 1.426 (2) C7—H7B 0.9800
S1—N1 1.6761 (19) C7—H7C 0.9800
S1—C1 1.750 (2) C8—C9 1.386 (3)
S2—C29 1.758 (3) C8—C13 1.394 (3)
S2—C15 1.781 (14) C9—C10 1.393 (4)
C15—C14 1.521 (15) C9—H9 0.9500
C15—H15A 0.9900 C10—C11 1.390 (4)
C15—H15B 0.9900 C10—H10 0.9500
S2'—C14 1.710 (6) C11—C12 1.383 (4)
S2'—C15' 1.770 (14) C11—H11 0.9500
C15'—C29 1.487 (14) C12—C13 1.386 (3)
C15'—H15C 0.9900 C12—H12 0.9500
C15'—H15D 0.9900 C16—C17 1.383 (3)
S3—O3 1.4246 (17) C16—C21 1.395 (3)
S3—O4 1.4274 (17) C17—C18 1.390 (3)
S3—N3 1.6756 (19) C17—H17 0.9500
S3—C16 1.753 (2) C18—C19 1.394 (3)
N1—C8 1.408 (3) C18—H18 0.9500
N1—C14 1.410 (3) C19—C20 1.394 (3)
N2—C14 1.298 (3) C19—C22 1.508 (3)
N2—C13 1.396 (3) C20—C21 1.383 (3)
N3—C23 1.416 (3) C20—H20 0.9500
N3—C29 1.422 (3) C21—H21 0.9500
N4—C29 1.296 (3) C22—H22A 0.9800
N4—C28 1.403 (3) C22—H22B 0.9800
C1—C6 1.385 (3) C22—H22C 0.9800
C1—C2 1.391 (3) C23—C28 1.392 (3)
C2—C3 1.383 (3) C23—C24 1.394 (3)
C2—H2 0.9500 C24—C25 1.383 (4)
C3—C4 1.395 (3) C24—H24 0.9500
C3—H3 0.9500 C25—C26 1.392 (4)
C4—C5 1.387 (3) C25—H25 0.9500
C4—C7 1.510 (3) C26—C27 1.387 (3)
C5—C6 1.387 (3) C26—H26 0.9500
C5—H5 0.9500 C27—C28 1.388 (3)
C6—H6 0.9500 C27—H27 0.9500
O1—S1—O2 120.60 (12) C11—C10—H10 119.1
O1—S1—N1 106.15 (11) C9—C10—H10 119.1
O2—S1—N1 105.55 (10) C12—C11—C10 121.4 (2)
O1—S1—C1 108.87 (11) C12—C11—H11 119.3
O2—S1—C1 110.46 (11) C10—C11—H11 119.3
N1—S1—C1 103.77 (10) C11—C12—C13 117.5 (2)
C29—S2—C15 96.0 (8) C11—C12—H12 121.2
C14—C15—S2 113.2 (10) C13—C12—H12 121.2
C14—C15—H15A 108.9 C12—C13—C8 120.6 (2)
S2—C15—H15A 108.9 C12—C13—N2 128.5 (2)
C14—C15—H15B 108.9 C8—C13—N2 110.8 (2)
S2—C15—H15B 108.9 N2—C14—N1 112.32 (19)
H15A—C15—H15B 107.8 N2—C14—C15 121.5 (6)
C14—S2'—C15' 97.1 (9) N1—C14—C15 126.1 (6)
C29—C15'—S2' 115.7 (9) N2—C14—S2' 128.0 (2)
C29—C15'—H15C 108.3 N1—C14—S2' 119.7 (2)
S2'—C15'—H15C 108.3 C15—C14—S2' 6.5 (7)
C29—C15'—H15D 108.3 C17—C16—C21 121.3 (2)
S2'—C15'—H15D 108.3 C17—C16—S3 120.80 (17)
H15C—C15'—H15D 107.4 C21—C16—S3 117.91 (17)
O3—S3—O4 120.56 (10) C16—C17—C18 118.9 (2)
O3—S3—N3 106.26 (10) C16—C17—H17 120.6
O4—S3—N3 105.40 (10) C18—C17—H17 120.6
O3—S3—C16 109.64 (10) C17—C18—C19 121.0 (2)
O4—S3—C16 109.22 (10) C17—C18—H18 119.5
N3—S3—C16 104.48 (10) C19—C18—H18 119.5
C8—N1—C14 106.02 (18) C20—C19—C18 118.9 (2)
C8—N1—S1 124.86 (16) C20—C19—C22 120.7 (2)
C14—N1—S1 128.62 (16) C18—C19—C22 120.5 (2)
C14—N2—C13 106.02 (19) C21—C20—C19 121.0 (2)
C23—N3—C29 105.04 (18) C21—C20—H20 119.5
C23—N3—S3 124.58 (15) C19—C20—H20 119.5
C29—N3—S3 124.38 (15) C20—C21—C16 119.0 (2)
C29—N4—C28 105.61 (19) C20—C21—H21 120.5
C6—C1—C2 121.3 (2) C16—C21—H21 120.5
C6—C1—S1 119.01 (18) C19—C22—H22A 109.5
C2—C1—S1 119.63 (18) C19—C22—H22B 109.5
C3—C2—C1 118.6 (2) H22A—C22—H22B 109.5
C3—C2—H2 120.7 C19—C22—H22C 109.5
C1—C2—H2 120.7 H22A—C22—H22C 109.5
C2—C3—C4 121.4 (2) H22B—C22—H22C 109.5
C2—C3—H3 119.3 C28—C23—C24 122.1 (2)
C4—C3—H3 119.3 C28—C23—N3 105.19 (19)
C5—C4—C3 118.5 (2) C24—C23—N3 132.7 (2)
C5—C4—C7 120.1 (2) C25—C24—C23 116.6 (2)
C3—C4—C7 121.5 (2) C25—C24—H24 121.7
C4—C5—C6 121.4 (2) C23—C24—H24 121.7
C4—C5—H5 119.3 C24—C25—C26 121.9 (2)
C6—C5—H5 119.3 C24—C25—H25 119.0
C1—C6—C5 118.8 (2) C26—C25—H25 119.0
C1—C6—H6 120.6 C27—C26—C25 121.0 (2)
C5—C6—H6 120.6 C27—C26—H26 119.5
C4—C7—H7A 109.5 C25—C26—H26 119.5
C4—C7—H7B 109.5 C26—C27—C28 117.9 (2)
H7A—C7—H7B 109.5 C26—C27—H27 121.0
C4—C7—H7C 109.5 C28—C27—H27 121.0
H7A—C7—H7C 109.5 C27—C28—C23 120.5 (2)
H7B—C7—H7C 109.5 C27—C28—N4 128.5 (2)
C9—C8—C13 122.5 (2) C23—C28—N4 111.05 (19)
C9—C8—N1 132.7 (2) N4—C29—N3 113.03 (19)
C13—C8—N1 104.79 (19) N4—C29—C15' 120.7 (6)
C8—C9—C10 116.1 (3) N3—C29—C15' 126.3 (6)
C8—C9—H9 121.9 N4—C29—S2 128.5 (2)
C10—C9—H9 121.9 N3—C29—S2 118.49 (19)
C11—C10—C9 121.8 (2) C15'—C29—S2 7.8 (7)

Hydrogen-bond geometry (Å, °)

Cg1 and Cg2 are the centroids of the C8–C13 and C23–C28 rings, respectively.
D—H···A D—H H···A D···A D—H···A
C6—H6···O1 0.95 2.50 2.886 (3) 105
C9—H9···O1 0.95 2.58 3.094 (4) 114
C15—H15A···N4 0.99 2.48 2.86 (2) 102
C15'—H15C···N2 0.99 2.47 2.84 (3) 102
C24—H24···O4 0.95 2.43 2.991 (3) 118
C6—H6···O4i 0.95 2.48 3.314 (3) 147
C20—H20···O3ii 0.95 2.46 3.386 (3) 164
C25—H25···Cg1iii 0.95 2.99 3.744 (3) 138
C15—H15A···Cg2iv 0.99 2.98 3.62 (2) 124

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PV2404).

References

  1. Barbour, L. J. (2001). J. Supramol. Chem, 1, 189–191.
  2. Bruker (2007). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Hayashi, K., Ogawa, S., Sano, S., Shiro, M., Yamaguchi, K., Sei, Y. & Nagao, Y. (2008). Chem. Pharm. Bull. 56, 802–806. [DOI] [PubMed]
  4. Rashid, N., Hasan, M., Tahir, M. K., Yusof, N. M. & Yamin, B. M. (2007). Acta Cryst. E63, o323–o324.
  5. Rashid, N., Hasan, M., Yusof, N. M. & Yamin, B. M. (2006). Acta Cryst. E62, o5455–o5456.
  6. Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
  7. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  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 datablocks I, global. DOI: 10.1107/S1600536811011822/pv2404sup1.cif

e-67-o1043-sup1.cif (23.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811011822/pv2404Isup2.hkl

e-67-o1043-Isup2.hkl (233.2KB, hkl)

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


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