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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 May 7;67(Pt 6):o1321–o1322. doi: 10.1107/S1600536811016151

2-(Naphthalen-1-yl)-4-(thio­phen-2-yl­methyl­idene)-1,3-oxazol-5(4H)-one

Cevher Gündoğdu a, Serap Alp a, Yavuz Ergün a, Barış Tercan b, Tuncer Hökelek c,*
PMCID: PMC3120366  PMID: 21754719

Abstract

The asymmetric unit of the title compound, C18H11NO2S, contains two crystallographically independent mol­ecules. In one mol­ecule, the oxazole and thio­phene rings are oriented at dihedral angles of 17.40 (9) and 18.18 (7)° with respect to the naphthalene ring system, while the oxazole and thio­phene rings are oriented to each other at a dihedral angle of 0.86 (9)°. In the other mol­ecule, the corresponding angles are 3.05 (8), 9.62 (6) and 7.02 (8)°, respectively. In each mol­ecule, a weak intra­molecular C—H⋯N hydrogen bond links the oxazole N atom to the naphthalene group. Weak inter­molecular C—H⋯O hydrogen bonding is present in the crystal structure. π–π stacking between the oxazole and thio­phene rings, between the thio­phene and naphthalene rings, and between the oxaozole and naphthalene rings, [centroid–centroid distances = 3.811 (2), 3.889 (2), 3.697 (2) and 3.525 (2) Å] may further stabilize the crystal structure.

Related literature

For potential applications of the title compound, such as organic light-emitting diodes (OLEDs), organic thin-film transistors (OTFTs), and organic photovoltaics (OPVs) of various aromatic ring-based conjugated polymers, see: Liu et al. (2007); Allard et al. (2008); Woudenbergh et al. (2004); Zhang et al. (2007); Güneş et al. (2007); Soci et al. (2007). For the roles of thio­phene-based mol­ecules widely used in the syntheses of the charge-transporting mol­ecules used in organic field effect transistors, organic solar cells and organic light emitting diodes, see: Mas-Torrent & Rovira (2008); Shirota & Kageyama (2007); Varis et al. (2006). For bond-length data, see: Allen et al. (1987).graphic file with name e-67-o1321-scheme1.jpg

Experimental

Crystal data

  • C18H11NO2S

  • M r = 305.35

  • Monoclinic, Inline graphic

  • a = 11.1509 (3) Å

  • b = 7.0871 (2) Å

  • c = 35.2592 (5) Å

  • β = 97.914 (4)°

  • V = 2759.91 (12) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.24 mm−1

  • T = 294 K

  • 0.35 × 0.22 × 0.20 mm

Data collection

  • Bruker Kappa APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2005) T min = 0.921, T max = 0.953

  • 25128 measured reflections

  • 6899 independent reflections

  • 3925 reflections with I > 2σ(I)

  • R int = 0.061

Refinement

  • R[F 2 > 2σ(F 2)] = 0.054

  • wR(F 2) = 0.133

  • S = 1.01

  • 6899 reflections

  • 405 parameters

  • 2 restraints

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.44 e Å−3

  • Δρmin = −0.44 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: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999) and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811016151/xu5202sup1.cif

e-67-o1321-sup1.cif (26.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811016151/xu5202Isup2.hkl

e-67-o1321-Isup2.hkl (330.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811016151/xu5202Isup3.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
C3—H3⋯N1 0.93 2.27 2.924 (3) 127
C3′—H3′⋯N1′ 0.93 2.29 2.946 (3) 127
C6—H6⋯O2i 0.93 2.59 3.483 (3) 160
C9′—H9′⋯O2ii 0.93 2.46 3.310 (3) 152
C16′—H16′⋯O2′iii 0.93 2.50 3.329 (3) 149

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

Acknowledgments

The authors are indebted to Anadolu University and the Medicinal Plants and Medicine Research Centre of Anadolu University, Eskişehir, Turkey, for the use of X-ray diffractometer. This study was supported by TUBITAK (grant No. 107T817).

supplementary crystallographic information

Comment

The design and syntheses of new conjugated polymers are a significant part of the conducting polymers research and have attracted great attention. Various aromatic ring-based conjugated polymers have been developed for use in potential applications, such as organic light-emitting diodes (OLEDs) (Liu et al., 2007; Allard et al., 2008), organic thin-film transistors (OTFTs) (Woudenbergh et al., 2004; Zhang et al., 2007), and organic photovoltaics (OPVs) (Güneş et al., 2007; Soci et al., 2007). Among conducting polymers, polythiophene and its derivatives have become a subject of considerable interest as electrochromic materials, due to their chemical stabilities. Thiophene based molecules are widely used in the sytheses of the charge transporting molecules used in organic field effect transistors, organic solar cells and organic light emitting diodes (Mas-Torrent & Rovira, 2008; Shirota & Kageyama, 2007; Varis et al., 2006). The present study was undertaken to ascertain the crystal structure of the title compound.

The asymmetric unit of the title compound contains two crystallographically independent molecules. Each molecule consists of an oxazol ring, a thiophene ring and a naphthalene group (Fig. 1), where the bond lengths are close to standard values (Allen et al., 1987). In each molecule, the intramolecular C-H···N hydrogen bonds link the oxazol nitrogen atoms to the naphthalene groups (Table 1 and Fig. 1).

An examination of the deviations from the least-squares planes through individual rings shows that rings A (C2—C7), B (C1/C2/C7—C10), C (O1/N1/C11—C13), D (S1/C15—C18) and A' (C2'—C7'), B' (C1'/C2'/C7'—C10'), C' (O1'/N1'/C11'—C13'), D' (S1'/C15'—C18') are planar. The naphthalene groups, containing the rings A, B and A', B' are also nearly planar [with maximum deviations of -0.032 (3) Å for atom C3 and 0.028 (3) Å for atom C4'] with dihedral angles of A/B = 2.28 (8) and A'/B' = 1.65 (8) °. In each molecule, rings C, D and C', D' are oriented with respect to the planar naphthalene groups at dihedral angles of 17.40 (9), 18.18 (7) ° and 3.05 (8), 9.62 (6) °, while the oxazole and thiophene rings are oriented at dihedral angles of 0.86 (9) and 7.02 (8) °,respectively.

In the crystal, intermolecular C'—H'···O' hydrogen bonds link the molecules into centrosymmetric dimers, in which they are also linked through C'-H'···O and C-H···O hydrogen bonds to form a three dimensional network (Table 1 and Fig. 2). The π–π contacts between the oxazol and thiophene rings, between the thiophene and naphthalene rings and between the oxaozole and naphthalene rings Cg3—Cg4i, Cg6—Cg8ii, Cg6—Cg7iii and Cg5—Cg7iii [symmetry codes: (i) -x, 1/2 + y, 1/2 - z, (ii) -x, 2 - y, -z, (iii) -x, 1 - y, -z, where Cg3, Cg4, Cg5, Cg6, Cg7 and Cg8 are centroids of the rings C (O1/N1/C11—C13), D (S1/C15—C18), A' (C2'—C7'), B' (C1'/C2'/C7'—C10'), C' (O1'/N1'/C11'—C13') and D' (S1'/C15'—C18'), respectively] may further stabilize the structure, with centroid-centroid distances of 3.811 (2), 3.889 (2), 3.697 (2) and 3.525 (2) Å, respectively.

Experimental

For the preparation of the title compound, (I), thiophene-2-carbaldehyde (0.46 g, 5 mmol), naphthalen-1-yl glycine (1.14 g, 5 mmol), acetic anhydride (2.49 ml, 12 mmol) and sodium acetate (0.41 g, 5 mmol) were heated until the mixture just liquefied, and then heating was continued for a further 2 h at 353 K. After completion of the reaction, ethanol (25 ml) was added and the mixture was kept at room temperature for 18 h. The solid product obtained was purified by washing with cold ethanol, hot water and a small amount of hexane, respectively. It was crystallized from hot ethanol (yield; 0.23 g, 49%, m.p. 460 K).

Refinement

H14 and H14' atoms are located in a difference Fourier synthesis and refined isotropically. The remaining C-bound H-atoms were positioned geometrically with C—H = 0.93 Å, and constrained to ride on their parent atoms with Uiso(H) = 1.2Ueq(C).

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title molecule with the atom-numbering scheme. Displacement ellipsoids are drawn at the 50% probability level. The intramolecular C-H···N and C'-H'···N' hydrogen bonds are shown as dashed lines.

Fig. 2.

Fig. 2.

A view of the crystal packing of the title compound. The C-H···O, C'-H'···O and C'-H'···O' hydrogen bonds are shown as dashed lines.

Crystal data

C18H11NO2S F(000) = 1264
Mr = 305.35 Dx = 1.470 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 3188 reflections
a = 11.1509 (3) Å θ = 2.3–22.5°
b = 7.0871 (2) Å µ = 0.24 mm1
c = 35.2592 (5) Å T = 294 K
β = 97.914 (4)° Block, orange
V = 2759.91 (12) Å3 0.35 × 0.22 × 0.20 mm
Z = 8

Data collection

Bruker Kappa APEXII CCD area-detector diffractometer 6899 independent reflections
Radiation source: fine-focus sealed tube 3925 reflections with I > 2σ(I)
graphite Rint = 0.061
φ and ω scans θmax = 28.4°, θmin = 1.2°
Absorption correction: multi-scan (SADABS; Bruker, 2005) h = −14→12
Tmin = 0.921, Tmax = 0.953 k = −9→9
25128 measured reflections l = −46→46

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)] = 0.054 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.133 H atoms treated by a mixture of independent and constrained refinement
S = 1.01 w = 1/[σ2(Fo2) + (0.0482P)2 + 0.9624P] where P = (Fo2 + 2Fc2)/3
6899 reflections (Δ/σ)max = 0.001
405 parameters Δρmax = 0.44 e Å3
2 restraints Δρmin = −0.44 e Å3

Special details

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)

x y z Uiso*/Ueq
S1 0.99971 (6) 0.92533 (10) 0.81233 (2) 0.02622 (19)
O1 0.95294 (14) 0.9314 (3) 0.66466 (5) 0.0240 (4)
O2 1.15707 (16) 0.9326 (3) 0.66746 (5) 0.0376 (5)
N1 0.93214 (17) 0.9251 (3) 0.72760 (6) 0.0190 (5)
C1 0.7483 (2) 0.9271 (3) 0.67941 (7) 0.0196 (6)
C2 0.6604 (2) 0.8757 (3) 0.70390 (7) 0.0189 (6)
C3 0.6894 (2) 0.8215 (3) 0.74272 (7) 0.0203 (6)
H3 0.7697 0.8241 0.7541 0.024*
C4 0.6018 (2) 0.7657 (4) 0.76358 (8) 0.0238 (6)
H4 0.6232 0.7300 0.7890 0.029*
C5 0.4792 (2) 0.7611 (4) 0.74733 (8) 0.0250 (6)
H5 0.4203 0.7209 0.7618 0.030*
C6 0.4478 (2) 0.8160 (4) 0.71037 (8) 0.0252 (6)
H6 0.3666 0.8148 0.6998 0.030*
C7 0.5358 (2) 0.8747 (4) 0.68781 (8) 0.0222 (6)
C8 0.5026 (2) 0.9324 (4) 0.64940 (8) 0.0259 (6)
H8 0.4211 0.9341 0.6391 0.031*
C9 0.5870 (2) 0.9852 (4) 0.62716 (8) 0.0260 (7)
H9 0.5632 1.0256 0.6022 0.031*
C10 0.7102 (2) 0.9788 (4) 0.64199 (8) 0.0234 (6)
H10 0.7675 1.0102 0.6262 0.028*
C11 0.8774 (2) 0.9272 (3) 0.69294 (7) 0.0200 (6)
C12 1.0706 (2) 0.9308 (4) 0.68424 (8) 0.0255 (6)
C13 1.0557 (2) 0.9265 (4) 0.72456 (7) 0.0205 (6)
C14 1.1464 (2) 0.9264 (4) 0.75406 (8) 0.0217 (6)
H14 1.2267 (16) 0.931 (4) 0.7486 (7) 0.031 (8)*
C15 1.1363 (2) 0.9271 (4) 0.79395 (7) 0.0202 (6)
C16 1.2332 (2) 0.9287 (4) 0.82323 (7) 0.0249 (6)
H16 1.3139 0.9308 0.8193 0.030*
C17 1.1949 (2) 0.9268 (4) 0.85972 (8) 0.0285 (7)
H17 1.2478 0.9270 0.8825 0.034*
C18 1.0734 (2) 0.9248 (4) 0.85800 (8) 0.0272 (7)
H18 1.0337 0.9233 0.8796 0.033*
S1' 0.77988 (6) 0.09732 (10) 0.902561 (19) 0.02376 (18)
O1' 0.83801 (14) 0.2656 (2) 1.04723 (5) 0.0204 (4)
O2' 0.63925 (15) 0.2045 (3) 1.04855 (5) 0.0264 (5)
N1' 0.85670 (17) 0.2013 (3) 0.98541 (6) 0.0169 (5)
C1' 1.0382 (2) 0.3041 (3) 1.02992 (7) 0.0175 (6)
C2' 1.1273 (2) 0.2914 (3) 1.00435 (7) 0.0155 (5)
C3' 1.1032 (2) 0.2400 (4) 0.96522 (7) 0.0195 (6)
H3' 1.0246 0.2082 0.9547 0.023*
C4' 1.1931 (2) 0.2364 (4) 0.94265 (8) 0.0220 (6)
H4' 1.1744 0.2048 0.9169 0.026*
C5' 1.3133 (2) 0.2796 (4) 0.95750 (8) 0.0224 (6)
H5' 1.3739 0.2740 0.9419 0.027*
C6' 1.3403 (2) 0.3296 (4) 0.99488 (8) 0.0226 (6)
H6' 1.4200 0.3575 1.0047 0.027*
C7' 1.2499 (2) 0.3402 (3) 1.01921 (7) 0.0175 (6)
C8' 1.2781 (2) 0.3959 (3) 1.05784 (7) 0.0216 (6)
H8' 1.3580 0.4243 1.0675 0.026*
C9' 1.1912 (2) 0.4091 (3) 1.08129 (7) 0.0218 (6)
H9' 1.2114 0.4485 1.1065 0.026*
C10' 1.0716 (2) 0.3634 (3) 1.06731 (7) 0.0208 (6)
H10' 1.0128 0.3730 1.0835 0.025*
C11' 0.9113 (2) 0.2551 (3) 1.01834 (7) 0.0177 (6)
C12' 0.7230 (2) 0.2106 (3) 1.03059 (7) 0.0197 (6)
C13' 0.7361 (2) 0.1687 (3) 0.99081 (7) 0.0175 (6)
C14' 0.6466 (2) 0.1050 (3) 0.96414 (8) 0.0182 (6)
H14' 0.5738 (16) 0.084 (3) 0.9725 (6) 0.019 (7)*
C15' 0.6534 (2) 0.0608 (3) 0.92518 (7) 0.0181 (6)
C16' 0.5598 (2) −0.0199 (4) 0.89970 (7) 0.0200 (6)
H16' 0.4840 −0.0495 0.9062 0.024*
C17' 0.5937 (2) −0.0509 (4) 0.86334 (8) 0.0256 (6)
H17' 0.5430 −0.1050 0.8431 0.031*
C18' 0.7089 (2) 0.0068 (4) 0.86086 (8) 0.0256 (6)
H18' 0.7448 −0.0024 0.8386 0.031*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0254 (4) 0.0327 (4) 0.0211 (4) −0.0023 (3) 0.0051 (3) −0.0003 (3)
O1 0.0216 (9) 0.0343 (11) 0.0166 (10) 0.0025 (8) 0.0043 (8) 0.0011 (9)
O2 0.0263 (10) 0.0643 (15) 0.0240 (12) 0.0058 (10) 0.0098 (9) 0.0037 (11)
N1 0.0182 (11) 0.0220 (12) 0.0169 (12) 0.0003 (10) 0.0023 (9) 0.0003 (10)
C1 0.0244 (13) 0.0154 (13) 0.0189 (14) 0.0006 (11) 0.0026 (11) −0.0023 (12)
C2 0.0212 (13) 0.0147 (13) 0.0200 (15) 0.0007 (11) −0.0003 (11) −0.0037 (11)
C3 0.0203 (13) 0.0204 (14) 0.0201 (15) 0.0013 (12) 0.0020 (11) −0.0012 (12)
C4 0.0264 (15) 0.0210 (15) 0.0239 (16) 0.0002 (12) 0.0028 (12) 0.0013 (12)
C5 0.0236 (14) 0.0215 (15) 0.0312 (18) 0.0002 (12) 0.0083 (12) −0.0008 (13)
C6 0.0188 (13) 0.0233 (15) 0.0329 (17) −0.0008 (12) 0.0013 (12) −0.0044 (13)
C7 0.0253 (14) 0.0173 (14) 0.0228 (15) 0.0019 (12) −0.0018 (12) −0.0036 (12)
C8 0.0221 (14) 0.0262 (16) 0.0270 (16) 0.0045 (12) −0.0050 (12) −0.0037 (13)
C9 0.0318 (16) 0.0273 (16) 0.0166 (15) 0.0045 (13) −0.0046 (12) 0.0015 (12)
C10 0.0273 (15) 0.0232 (15) 0.0198 (15) 0.0016 (12) 0.0034 (12) −0.0027 (12)
C11 0.0232 (13) 0.0160 (14) 0.0214 (15) 0.0019 (12) 0.0056 (11) 0.0013 (12)
C12 0.0232 (14) 0.0280 (16) 0.0251 (16) 0.0020 (13) 0.0026 (12) 0.0011 (13)
C13 0.0199 (13) 0.0211 (14) 0.0213 (15) 0.0011 (12) 0.0053 (11) 0.0016 (12)
C14 0.0203 (14) 0.0205 (15) 0.0249 (16) −0.0007 (12) 0.0051 (12) 0.0010 (12)
C15 0.0200 (13) 0.0196 (14) 0.0215 (15) −0.0013 (12) 0.0044 (11) 0.0009 (12)
C16 0.0332 (15) 0.0194 (14) 0.0216 (16) 0.0021 (13) 0.0019 (12) −0.0039 (13)
C17 0.0339 (16) 0.0276 (16) 0.0214 (16) 0.0029 (13) −0.0055 (12) −0.0013 (13)
C18 0.0335 (16) 0.0315 (17) 0.0169 (15) −0.0015 (14) 0.0044 (12) 0.0012 (13)
S1' 0.0223 (3) 0.0278 (4) 0.0218 (4) −0.0035 (3) 0.0053 (3) −0.0007 (3)
O1' 0.0207 (9) 0.0254 (10) 0.0156 (10) −0.0007 (8) 0.0042 (7) −0.0004 (8)
O2' 0.0241 (10) 0.0336 (12) 0.0228 (11) 0.0001 (9) 0.0085 (8) 0.0013 (9)
N1' 0.0168 (10) 0.0155 (11) 0.0184 (12) 0.0010 (9) 0.0028 (9) 0.0007 (9)
C1' 0.0202 (13) 0.0121 (13) 0.0204 (14) 0.0011 (11) 0.0035 (11) 0.0004 (11)
C2' 0.0180 (12) 0.0099 (12) 0.0185 (14) 0.0037 (10) 0.0022 (10) 0.0016 (11)
C3' 0.0206 (13) 0.0193 (14) 0.0184 (15) −0.0004 (11) 0.0018 (11) −0.0013 (11)
C4' 0.0275 (15) 0.0215 (15) 0.0173 (14) 0.0012 (12) 0.0039 (11) −0.0008 (12)
C5' 0.0213 (14) 0.0225 (15) 0.0254 (16) 0.0013 (12) 0.0101 (12) 0.0023 (12)
C6' 0.0193 (13) 0.0189 (14) 0.0300 (17) 0.0012 (12) 0.0052 (12) 0.0029 (13)
C7' 0.0189 (13) 0.0108 (13) 0.0221 (15) 0.0009 (11) 0.0005 (11) 0.0037 (11)
C8' 0.0220 (13) 0.0180 (14) 0.0231 (15) −0.0022 (11) −0.0031 (11) 0.0021 (12)
C9' 0.0288 (14) 0.0189 (14) 0.0162 (14) 0.0007 (12) −0.0018 (11) −0.0020 (12)
C10' 0.0255 (14) 0.0177 (14) 0.0201 (15) 0.0011 (12) 0.0066 (11) 0.0010 (12)
C11' 0.0249 (14) 0.0144 (13) 0.0149 (14) 0.0036 (11) 0.0069 (11) 0.0017 (11)
C12' 0.0186 (13) 0.0172 (14) 0.0232 (15) 0.0024 (12) 0.0030 (11) 0.0037 (12)
C13' 0.0183 (13) 0.0166 (13) 0.0181 (14) 0.0048 (11) 0.0040 (10) 0.0023 (11)
C14' 0.0133 (12) 0.0191 (14) 0.0231 (15) 0.0015 (11) 0.0054 (11) 0.0034 (12)
C15' 0.0174 (12) 0.0173 (13) 0.0200 (15) 0.0018 (11) 0.0036 (11) 0.0053 (12)
C16' 0.0192 (13) 0.0203 (14) 0.0207 (15) 0.0021 (11) 0.0040 (11) 0.0021 (12)
C17' 0.0204 (14) 0.0294 (16) 0.0251 (16) −0.0003 (12) −0.0038 (11) −0.0015 (13)
C18' 0.0292 (15) 0.0331 (16) 0.0149 (15) 0.0064 (13) 0.0048 (12) 0.0021 (12)

Geometric parameters (Å, °)

S1—C15 1.735 (3) S1'—C15' 1.732 (2)
S1—C18 1.704 (3) S1'—C18' 1.697 (3)
O1—C11 1.391 (3) O1'—C11' 1.393 (3)
O1—C12 1.396 (3) O1'—C12' 1.391 (3)
O2—C12 1.199 (3) O2'—C12' 1.199 (3)
N1—C11 1.289 (3) N1'—C11' 1.292 (3)
N1—C13 1.397 (3) N1'—C13' 1.403 (3)
C1—C10 1.379 (3) C1'—C10' 1.385 (3)
C1—C11 1.453 (3) C2'—C1' 1.434 (3)
C2—C1 1.440 (3) C3'—C2' 1.417 (3)
C2—C3 1.415 (3) C3'—C4' 1.363 (3)
C2—C7 1.427 (3) C3'—H3' 0.9300
C3—H3 0.9300 C4'—H4' 0.9300
C4—C3 1.361 (3) C5'—C4' 1.404 (3)
C4—H4 0.9300 C5'—C6' 1.358 (3)
C5—C4 1.407 (3) C5'—H5' 0.9300
C5—C6 1.359 (4) C6'—H6' 0.9300
C5—H5 0.9300 C7'—C2' 1.437 (3)
C6—C7 1.408 (4) C7'—C6' 1.412 (3)
C6—H6 0.9300 C8'—C7' 1.412 (3)
C8—C7 1.414 (4) C8'—C9' 1.361 (3)
C8—C9 1.358 (4) C8'—H8' 0.9300
C8—H8 0.9300 C9'—C10' 1.394 (3)
C9—C10 1.401 (3) C9'—H9' 0.9300
C9—H9 0.9300 C10'—H10' 0.9300
C10—H10 0.9300 C11'—C1' 1.459 (3)
C13—C12 1.454 (4) C13'—C14' 1.351 (3)
C14—C13 1.347 (3) C13'—C12' 1.460 (3)
C14—H14 0.942 (16) C14'—H14' 0.913 (16)
C15—C14 1.426 (4) C15'—C14' 1.421 (3)
C15—C16 1.388 (3) C15'—C16' 1.402 (3)
C16—H16 0.9300 C16'—C17' 1.403 (4)
C17—C16 1.410 (4) C16'—H16' 0.9300
C17—H17 0.9300 C17'—H17' 0.9300
C18—C17 1.348 (3) C18'—C17' 1.362 (3)
C18—H18 0.9300 C18'—H18' 0.9300
C18—S1—C15 91.12 (13) C18'—S1'—C15' 91.74 (13)
C11—O1—C12 105.42 (19) C12'—O1'—C11' 106.03 (19)
C11—N1—C13 105.7 (2) C11'—N1'—C13' 105.6 (2)
C2—C1—C11 122.0 (2) C2'—C1'—C11' 122.6 (2)
C10—C1—C2 119.7 (2) C10'—C1'—C2' 119.9 (2)
C10—C1—C11 118.4 (2) C10'—C1'—C11' 117.5 (2)
C3—C2—C1 124.4 (2) C1'—C2'—C7' 117.6 (2)
C3—C2—C7 117.6 (2) C3'—C2'—C1' 125.0 (2)
C7—C2—C1 118.0 (2) C3'—C2'—C7' 117.4 (2)
C2—C3—H3 119.5 C2'—C3'—H3' 119.4
C4—C3—C2 121.1 (2) C4'—C3'—C2' 121.1 (2)
C4—C3—H3 119.5 C4'—C3'—H3' 119.4
C3—C4—C5 121.1 (3) C3'—C4'—C5' 121.3 (2)
C3—C4—H4 119.5 C3'—C4'—H4' 119.4
C5—C4—H4 119.5 C5'—C4'—H4' 119.4
C4—C5—H5 120.3 C4'—C5'—H5' 120.3
C6—C5—C4 119.5 (3) C6'—C5'—C4' 119.4 (2)
C6—C5—H5 120.3 C6'—C5'—H5' 120.3
C5—C6—C7 121.2 (2) C5'—C6'—C7' 121.5 (2)
C5—C6—H6 119.4 C5'—C6'—H6' 119.3
C7—C6—H6 119.4 C7'—C6'—H6' 119.3
C6—C7—C2 119.5 (2) C6'—C7'—C2' 119.2 (2)
C6—C7—C8 121.0 (2) C8'—C7'—C2' 119.6 (2)
C8—C7—C2 119.4 (2) C8'—C7'—C6' 121.2 (2)
C7—C8—H8 119.3 C7'—C8'—H8' 119.3
C9—C8—C7 121.5 (2) C9'—C8'—C7' 121.5 (2)
C9—C8—H8 119.3 C9'—C8'—H8' 119.3
C8—C9—C10 119.8 (3) C8'—C9'—C10' 119.7 (2)
C8—C9—H9 120.1 C8'—C9'—H9' 120.1
C10—C9—H9 120.1 C10'—C9'—H9' 120.1
C1—C10—C9 121.5 (3) C1'—C10'—C9' 121.7 (2)
C1—C10—H10 119.2 C1'—C10'—H10' 119.1
C9—C10—H10 119.2 C9'—C10'—H10' 119.1
O1—C11—C1 115.8 (2) O1'—C11'—C1' 115.2 (2)
N1—C11—O1 115.2 (2) N1'—C11'—O1' 114.9 (2)
N1—C11—C1 129.0 (2) N1'—C11'—C1' 129.8 (2)
O1—C12—C13 104.9 (2) O1'—C12'—C13' 104.7 (2)
O2—C12—O1 121.4 (2) O2'—C12'—O1' 121.8 (2)
O2—C12—C13 133.7 (2) O2'—C12'—C13' 133.5 (2)
N1—C13—C12 108.8 (2) N1'—C13'—C12' 108.8 (2)
C14—C13—N1 125.8 (2) C14'—C13'—N1' 126.2 (2)
C14—C13—C12 125.5 (2) C14'—C13'—C12' 125.0 (2)
C13—C14—C15 127.5 (2) C13'—C14'—C15' 127.8 (2)
C13—C14—H14 118.3 (16) C13'—C14'—H14' 115.7 (15)
C15—C14—H14 114.2 (16) C15'—C14'—H14' 116.5 (15)
C14—C15—S1 124.13 (19) C14'—C15'—S1' 124.58 (19)
C16—C15—S1 110.8 (2) C16'—C15'—S1' 110.32 (19)
C16—C15—C14 125.0 (2) C16'—C15'—C14' 125.1 (2)
C15—C16—C17 112.1 (2) C15'—C16'—C17' 112.3 (2)
C15—C16—H16 124.0 C15'—C16'—H16' 123.9
C17—C16—H16 124.0 C17'—C16'—H16' 123.9
C16—C17—H17 123.6 C16'—C17'—H17' 123.6
C18—C17—C16 112.8 (2) C18'—C17'—C16' 112.8 (2)
C18—C17—H17 123.6 C18'—C17'—H17' 123.6
S1—C18—H18 123.4 S1'—C18'—H18' 123.5
C17—C18—S1 113.1 (2) C17'—C18'—S1' 112.9 (2)
C17—C18—H18 123.4 C17'—C18'—H18' 123.5
C15—S1—C18—C17 0.3 (2) C18'—S1'—C15'—C14' 179.3 (2)
C18—S1—C15—C14 179.3 (2) C18'—S1'—C15'—C16' −0.2 (2)
C18—S1—C15—C16 −0.5 (2) C15'—S1'—C18'—C17' −0.3 (2)
C12—O1—C11—N1 0.3 (3) C12'—O1'—C11'—N1' 0.4 (3)
C12—O1—C11—C1 180.0 (2) C12'—O1'—C11'—C1' −178.9 (2)
C11—O1—C12—O2 179.5 (3) C11'—O1'—C12'—O2' 179.7 (2)
C11—O1—C12—C13 −0.1 (3) C11'—O1'—C12'—C13' 0.0 (2)
C13—N1—C11—O1 −0.4 (3) C13'—N1'—C11'—O1' −0.6 (3)
C13—N1—C11—C1 −180.0 (2) C13'—N1'—C11'—C1' 178.5 (2)
C11—N1—C13—C12 0.3 (3) C11'—N1'—C13'—C12' 0.6 (3)
C11—N1—C13—C14 179.5 (3) C11'—N1'—C13'—C14' −178.0 (2)
C2—C1—C10—C9 0.8 (4) C2'—C1'—C10'—C9' −1.0 (4)
C11—C1—C10—C9 −178.8 (2) C11'—C1'—C10'—C9' 178.5 (2)
C2—C1—C11—O1 164.0 (2) C3'—C2'—C1'—C10' −177.3 (2)
C2—C1—C11—N1 −16.4 (4) C3'—C2'—C1'—C11' 3.2 (4)
C10—C1—C11—O1 −16.3 (3) C7'—C2'—C1'—C10' 0.6 (3)
C10—C1—C11—N1 163.3 (3) C7'—C2'—C1'—C11' −178.9 (2)
C3—C2—C1—C10 −179.6 (2) C4'—C3'—C2'—C1' 178.2 (2)
C3—C2—C1—C11 0.1 (4) C4'—C3'—C2'—C7' 0.2 (4)
C7—C2—C1—C10 2.0 (4) C2'—C3'—C4'—C5' 1.4 (4)
C7—C2—C1—C11 −178.3 (2) C6'—C5'—C4'—C3' −1.3 (4)
C1—C2—C3—C4 −176.7 (2) C4'—C5'—C6'—C7' −0.3 (4)
C7—C2—C3—C4 1.7 (4) C6'—C7'—C2'—C1' −179.9 (2)
C1—C2—C7—C6 176.8 (2) C6'—C7'—C2'—C3' −1.8 (3)
C1—C2—C7—C8 −3.1 (4) C8'—C7'—C2'—C1' 0.6 (3)
C3—C2—C7—C6 −1.7 (4) C8'—C7'—C2'—C3' 178.8 (2)
C3—C2—C7—C8 178.4 (2) C2'—C7'—C6'—C5' 1.9 (4)
C5—C4—C3—C2 −0.4 (4) C8'—C7'—C6'—C5' −178.7 (2)
C6—C5—C4—C3 −1.0 (4) C9'—C8'—C7'—C2' −1.6 (4)
C4—C5—C6—C7 1.0 (4) C9'—C8'—C7'—C6' 179.0 (2)
C5—C6—C7—C2 0.3 (4) C7'—C8'—C9'—C10' 1.2 (4)
C5—C6—C7—C8 −179.8 (3) C8'—C9'—C10'—C1' 0.1 (4)
C9—C8—C7—C2 1.4 (4) O1'—C11'—C1'—C2' 176.7 (2)
C9—C8—C7—C6 −178.5 (3) O1'—C11'—C1'—C10' −2.8 (3)
C7—C8—C9—C10 1.5 (4) N1'—C11'—C1'—C2' −2.4 (4)
C8—C9—C10—C1 −2.7 (4) N1'—C11'—C1'—C10' 178.0 (2)
N1—C13—C12—O1 −0.1 (3) N1'—C13'—C12'—O1' −0.4 (3)
N1—C13—C12—O2 −179.6 (3) N1'—C13'—C12'—O2' 180.0 (3)
C14—C13—C12—O1 −179.3 (3) C14'—C13'—C12'—O1' 178.3 (2)
C14—C13—C12—O2 1.1 (5) C14'—C13'—C12'—O2' −1.4 (5)
C15—C14—C13—N1 −0.9 (5) N1'—C13'—C14'—C15' −1.2 (4)
C15—C14—C13—C12 178.3 (3) C12'—C13'—C14'—C15' −179.7 (2)
S1—C15—C14—C13 0.9 (4) S1'—C15'—C14'—C13' −5.1 (4)
C16—C15—C14—C13 −179.4 (3) C16'—C15'—C14'—C13' 174.3 (3)
S1—C15—C16—C17 0.5 (3) S1'—C15'—C16'—C17' 0.7 (3)
C14—C15—C16—C17 −179.3 (3) C14'—C15'—C16'—C17' −178.8 (2)
C18—C17—C16—C15 −0.3 (3) C15'—C16'—C17'—C18' −0.9 (3)
S1—C18—C17—C16 −0.1 (3) S1'—C18'—C17'—C16' 0.8 (3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C3—H3···N1 0.93 2.27 2.924 (3) 127
C3'—H3'···N1' 0.93 2.29 2.946 (3) 127
C6—H6···O2i 0.93 2.59 3.483 (3) 160
C9'—H9'···O2ii 0.93 2.46 3.310 (3) 152
C16'—H16'···O2'iii 0.93 2.50 3.329 (3) 149

Symmetry codes: (i) x−1, y, z; (ii) x, −y+3/2, z+1/2; (iii) −x+1, −y, −z+2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5202).

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 datablocks I, global. DOI: 10.1107/S1600536811016151/xu5202sup1.cif

e-67-o1321-sup1.cif (26.6KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811016151/xu5202Isup2.hkl

e-67-o1321-Isup2.hkl (330.8KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811016151/xu5202Isup3.cml

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


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