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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Jan 9;66(Pt 2):o305–o306. doi: 10.1107/S1600536809055846

2-[(E)-2-(4-Ethoxy­phen­yl)ethen­yl]-1-methyl­pyridinium 4-bromo­benzene­sulfonate monohydrate1

Hoong-Kun Fun a,*,, Kullapa Chanawanno b, Suchada Chantrapromma b,§
PMCID: PMC2979781  PMID: 21579738

Abstract

In the title compound, C16H18NO+·C6H4BrO3S·H2O, the cation exists in an E configuration with respect to the ethenyl bond and is slightly twisted with a dihedral angle of 8.5 (2)° between pyridinium and benzene rings. In the crystal, the cations are arranged in layers parallel to (100), with π–π inter­actions between pyridinium and benzene rings [centroid–centroid distances = 3.651 (3) and 3.613 (3) Å]. The anions and water mol­ecules are located between the cationic layers. The ions and water mol­ecules are linked into a three-dimensional framework by O—H⋯O and C—H⋯O hydrogen bonds.

Related literature

The title compound was synthesized as part of an investigation of the influence of the counter-ions on non-linear optical (NLO) properties. For background to NLO materials research, see: Coe et al. (2002); Pan et al. (1996). For related structures, see: Chanawanno et al. (2009); Chantrapromma et al. (2006, 2009); Laksana et al. (2008). For bond-length data, see: Allen et al. (1987). For the stability of the temperature controller used in the data collection, see: Cosier & Glazer (1986).graphic file with name e-66-0o305-scheme1.jpg

Experimental

Crystal data

  • C16H18NO+·C6H4BrO3S·H2O

  • M r = 494.39

  • Monoclinic, Inline graphic

  • a = 9.8022 (5) Å

  • b = 6.5162 (3) Å

  • c = 34.9982 (17) Å

  • β = 105.102 (3)°

  • V = 2158.24 (18) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 2.04 mm−1

  • T = 100 K

  • 0.34 × 0.31 × 0.19 mm

Data collection

  • Bruker APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2005) T min = 0.547, T max = 0.703

  • 30564 measured reflections

  • 6286 independent reflections

  • 4937 reflections with I > 2σ(I)

  • R int = 0.076

Refinement

  • R[F 2 > 2σ(F 2)] = 0.071

  • wR(F 2) = 0.224

  • S = 1.15

  • 6286 reflections

  • 275 parameters

  • H-atom parameters constrained

  • Δρmax = 1.26 e Å−3

  • Δρmin = −1.36 e Å−3

Data collection: APEX2 (Bruker, 2005); cell refinement: SAINT (Bruker, 2005); data reduction: SAINT; program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809055846/ci5012sup1.cif

e-66-0o305-sup1.cif (22.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809055846/ci5012Isup2.hkl

e-66-0o305-Isup2.hkl (307.7KB, hkl)

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
O1W—H2W1⋯O4 0.85 2.09 2.929 (6) 171
O1W—H1W1⋯O2i 0.85 1.99 2.827 (6) 168
C1—H1A⋯O1Wii 0.93 2.23 3.154 (7) 176
C2—H2A⋯O1Wiii 0.93 2.43 3.223 (7) 143
C4—H4A⋯O4 0.93 2.50 3.378 (7) 158
C6—H6A⋯O3iv 0.93 2.56 3.442 (7) 159
C13—H13A⋯O3iv 0.93 2.49 3.387 (7) 161
C14—H14A⋯O2v 0.96 2.57 3.384 (7) 143
C14—H14C⋯O3iv 0.96 2.51 3.129 (7) 122

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

Acknowledgments

The authors thank the Prince of Songkla University for a research grant and Universiti Sains Malaysia for the Research University Golden Goose grant No. 1001/PFIZIK/811012. KC thanks the Development and Promotion of Science and Technology Talents Project (DPST) for a study grant.

supplementary crystallographic information

Comment

Ionic organic crystals are of special interest due to their high second order optical nonlinearities (Coe et al., 2002). The orientation of ionic chromophores can be arranged simply by changing the counter-ions (Pan et al., 1996). During the course of our NLO materials research, we have previously synthesized and reported crystal structures of related pyridinium salts containing the 2-[(E)-2-(4-ethoxyphenyl)ethenyl]-1-methylpyridinium cationic part (Chanawanno et al., 2009; Laksana et al., 2008). The title compound was synthesized by retaining the same cationic part but changing the anion counter part to 4-bromobenzenesulfonate in order to investigate the influence of the counter-ions on the NLO properties. However, it was found that the title compound crystallized in a centrosymmetric space group P21/c and hence no second-order nonlinear optical properties are observed.

In the title compound (Fig. 1), the cation exists in an E configuration with respect to the ethenyl bond [C5—C6—C7—C8 = -179.9 (5)°]. The cation is slightly twisted with a dihedral angle between the pyridinium and benzene rings of 8.5 (2)°. The pyridinium and benzene rings of the cation form dihedral angles of 79.2 (2) and 71.0 (2)°, respectively, with the benzene ring of the anion. Bond distances in both cation and anion have normal values (Allen et al., 1987) and are comparable to those observed in related structures (Chanawanno et al., 2009; Chantrapromma et al., 2009; Laksana et al., 2008).

In the crystal, the cations are stacked along the b axis and are arranged in layers parallel to the (100) with π–π interactions involving pyridinium (centroid Cg1) and benzene (centroid Cg2) rings [Cg1···Cg1ii = 3.651 (3) Å and Cg1···Cg2iii = 3.613 (3) Å; symmetry codes as in Table 1]. The anions and water molecules are located between the cationic layers. The cations are linked with the water molecules and anions by C—H···O weak interactions (Table 1), whereas the anions are linked with water molecules by O—H···O hydrogen bonds (Table 1). These interactions connect the ionic units and water molecules into a three-dimensional network (Fig. 2).

Experimental

2-[(E)-2-(4-Ethoxyphenyl)ethenyl]-1-methylpyridinium iodide (0.21 g, 0.58 mmol) which was prepared according to the previous method (Laksana et al., 2008) was mixed with silver 4-bromobenzenesulfonate (Chantrapromma et al., 2006) (0.20 g, 0.58 mmol) in methanol (100 ml) and stirred for 0.5 h. The precipitate of silver iodide which formed was filtered and the filtrate was evaporated to give the title compound as a yellow solid. Yellow block-shaped single crystals of the title compound suitable for X-ray structure determination were recrystallized from methanol by slow evaporation at room temperature over a few weeks (m.p. 463-465 K).

Refinement

H atoms were positioned geometrically and allowed to ride on their parent atoms, with O–H = 0.85 Å and C–H = 0.93-0.97 Å. The Uiso values were constrained to be 1.5Ueq of the carrier atom for methyl H atoms and 1.2Ueq for the remaining H atoms. A rotating group model was used for the methyl groups. The highest residual electron density peak is located at 0.81 Å from Br1 and the deepest hole is located at 1.90 Å from Br1.

Figures

Fig. 1.

Fig. 1.

The asymmetric unit of the title compound, with 50% probability displacement ellipsoids and the atom-numbering scheme.

Fig. 2.

Fig. 2.

The crystal packing of the title compound, viewed down the b axis. Hydrogen bonds are shown as dashed lines.

Crystal data

C16H18NO+·C6H4BrO3S·H2O F(000) = 1016
Mr = 494.39 Dx = 1.522 Mg m3
Monoclinic, P21/c Melting point = 463–465 K
Hall symbol: -P 2ybc Mo Kα radiation, λ = 0.71073 Å
a = 9.8022 (5) Å Cell parameters from 6286 reflections
b = 6.5162 (3) Å θ = 2.4–30.0°
c = 34.9982 (17) Å µ = 2.04 mm1
β = 105.102 (3)° T = 100 K
V = 2158.24 (18) Å3 Block, yellow
Z = 4 0.34 × 0.31 × 0.19 mm

Data collection

Bruker APEXII CCD area-detector diffractometer 6286 independent reflections
Radiation source: sealed tube 4937 reflections with I > 2σ(I)
graphite Rint = 0.076
φ and ω scans θmax = 30.0°, θmin = 2.4°
Absorption correction: multi-scan (SADABS; Bruker, 2005) h = −13→12
Tmin = 0.547, Tmax = 0.703 k = −7→9
30564 measured reflections l = −49→49

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)] = 0.071 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.224 H-atom parameters constrained
S = 1.15 w = 1/[σ2(Fo2) + (0.0686P)2 + 18.6991P] where P = (Fo2 + 2Fc2)/3
6286 reflections (Δ/σ)max = 0.001
275 parameters Δρmax = 1.25 e Å3
0 restraints Δρmin = −1.36 e Å3

Special details

Experimental. The crystal was placed in the cold stream of an Oxford Cryosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K.
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
Br1 0.61259 (6) 1.18042 (10) 0.235458 (16) 0.02660 (17)
S1 0.57829 (13) 0.5608 (2) 0.09005 (4) 0.0181 (3)
O1 0.0959 (4) 1.1839 (6) 0.19616 (10) 0.0174 (7)
O2 0.5793 (5) 0.6847 (7) 0.05563 (12) 0.0308 (9)
O3 0.6973 (4) 0.4215 (7) 0.10216 (13) 0.0288 (9)
O4 0.4420 (4) 0.4596 (6) 0.08582 (11) 0.0212 (7)
N1 −0.0521 (5) 0.0228 (7) 0.05416 (12) 0.0165 (8)
C1 −0.0322 (6) −0.1561 (8) 0.03624 (14) 0.0190 (10)
H1A −0.1099 −0.2379 0.0248 0.023*
C2 0.0992 (6) −0.2181 (8) 0.03460 (14) 0.0200 (10)
H2A 0.1112 −0.3418 0.0226 0.024*
C3 0.2145 (6) −0.0946 (8) 0.05103 (15) 0.0205 (10)
H3A 0.3045 −0.1329 0.0497 0.025*
C4 0.1943 (6) 0.0864 (9) 0.06946 (15) 0.0201 (10)
H4A 0.2718 0.1689 0.0807 0.024*
C5 0.0596 (5) 0.1481 (8) 0.07152 (14) 0.0159 (9)
C6 0.0314 (5) 0.3379 (8) 0.09094 (14) 0.0168 (9)
H6A −0.0618 0.3793 0.0875 0.020*
C7 0.1350 (5) 0.4535 (8) 0.11338 (14) 0.0164 (9)
H7A 0.2272 0.4087 0.1163 0.020*
C8 0.1164 (5) 0.6439 (8) 0.13376 (14) 0.0160 (9)
C9 0.2375 (5) 0.7467 (8) 0.15528 (14) 0.0173 (9)
H9A 0.3262 0.6938 0.1559 0.021*
C10 0.2276 (5) 0.9264 (8) 0.17581 (14) 0.0175 (9)
H10A 0.3092 0.9922 0.1901 0.021*
C11 0.0950 (5) 1.0080 (7) 0.17496 (13) 0.0142 (8)
C12 −0.0272 (5) 0.9066 (8) 0.15352 (14) 0.0151 (9)
H12A −0.1159 0.9596 0.1528 0.018*
C13 −0.0152 (5) 0.7263 (8) 0.13326 (14) 0.0161 (9)
H13A −0.0967 0.6596 0.1191 0.019*
C14 −0.1979 (5) 0.0792 (9) 0.05387 (16) 0.0207 (10)
H14A −0.2612 −0.0282 0.0415 0.031*
H14B −0.2233 0.2044 0.0393 0.031*
H14C −0.2042 0.0981 0.0806 0.031*
C15 −0.0362 (5) 1.2805 (8) 0.19457 (14) 0.0174 (9)
H15A −0.1005 1.1843 0.2019 0.021*
H15B −0.0792 1.3308 0.1681 0.021*
C16 −0.0034 (6) 1.4575 (8) 0.22382 (15) 0.0211 (10)
H16A −0.0891 1.5296 0.2235 0.032*
H16B 0.0619 1.5497 0.2165 0.032*
H16C 0.0377 1.4051 0.2499 0.032*
C17 0.5949 (5) 0.7380 (8) 0.13010 (14) 0.0165 (9)
C18 0.5583 (5) 0.9431 (8) 0.12275 (15) 0.0194 (9)
H18A 0.5304 0.9911 0.0969 0.023*
C19 0.5634 (5) 1.0763 (8) 0.15409 (16) 0.0206 (10)
H19A 0.5389 1.2137 0.1495 0.025*
C20 0.6059 (5) 1.0000 (8) 0.19242 (15) 0.0187 (9)
C21 0.6451 (5) 0.7944 (9) 0.20045 (15) 0.0203 (10)
H21A 0.6745 0.7465 0.2263 0.024*
C22 0.6388 (5) 0.6640 (8) 0.16850 (15) 0.0194 (9)
H22A 0.6641 0.5268 0.1729 0.023*
O1W 0.2862 (4) 0.4509 (7) 0.00213 (12) 0.0272 (9)
H2W1 0.3391 0.4482 0.0256 0.06 (3)*
H1W1 0.3314 0.3960 −0.0129 0.04 (2)*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Br1 0.0304 (3) 0.0266 (3) 0.0250 (3) −0.0038 (2) 0.0113 (2) −0.0113 (2)
S1 0.0172 (5) 0.0182 (6) 0.0201 (5) −0.0051 (4) 0.0070 (4) −0.0055 (4)
O1 0.0171 (16) 0.0143 (16) 0.0206 (16) −0.0004 (13) 0.0045 (13) −0.0053 (13)
O2 0.043 (2) 0.029 (2) 0.0243 (19) −0.011 (2) 0.0162 (18) −0.0062 (17)
O3 0.0190 (18) 0.028 (2) 0.038 (2) 0.0020 (16) 0.0049 (16) −0.0159 (18)
O4 0.0161 (16) 0.0216 (19) 0.0256 (18) −0.0063 (14) 0.0049 (14) −0.0051 (15)
N1 0.020 (2) 0.014 (2) 0.0161 (18) −0.0013 (16) 0.0057 (15) −0.0011 (15)
C1 0.028 (3) 0.015 (2) 0.015 (2) −0.0033 (19) 0.0065 (18) −0.0008 (17)
C2 0.030 (3) 0.014 (2) 0.016 (2) 0.0012 (19) 0.0053 (19) −0.0025 (17)
C3 0.024 (2) 0.019 (2) 0.019 (2) 0.005 (2) 0.0057 (18) −0.0003 (19)
C4 0.021 (2) 0.021 (3) 0.018 (2) −0.0006 (19) 0.0046 (18) −0.0046 (18)
C5 0.020 (2) 0.013 (2) 0.0142 (19) −0.0031 (17) 0.0036 (16) −0.0017 (16)
C6 0.018 (2) 0.015 (2) 0.018 (2) 0.0004 (18) 0.0046 (17) −0.0012 (17)
C7 0.018 (2) 0.016 (2) 0.016 (2) 0.0005 (18) 0.0070 (17) −0.0011 (17)
C8 0.018 (2) 0.016 (2) 0.0148 (19) −0.0022 (17) 0.0051 (16) −0.0016 (17)
C9 0.018 (2) 0.016 (2) 0.018 (2) −0.0004 (17) 0.0060 (17) −0.0034 (17)
C10 0.016 (2) 0.019 (2) 0.017 (2) −0.0034 (18) 0.0034 (16) −0.0048 (18)
C11 0.017 (2) 0.013 (2) 0.0131 (19) −0.0020 (16) 0.0043 (16) −0.0019 (16)
C12 0.014 (2) 0.016 (2) 0.0152 (19) 0.0006 (17) 0.0043 (16) −0.0012 (17)
C13 0.017 (2) 0.016 (2) 0.015 (2) −0.0011 (17) 0.0040 (16) −0.0018 (17)
C14 0.017 (2) 0.018 (2) 0.027 (2) −0.0029 (18) 0.0048 (18) −0.0055 (19)
C15 0.022 (2) 0.012 (2) 0.018 (2) 0.0016 (18) 0.0047 (17) −0.0020 (17)
C16 0.025 (2) 0.017 (2) 0.021 (2) 0.006 (2) 0.0044 (19) −0.0040 (18)
C17 0.014 (2) 0.017 (2) 0.019 (2) −0.0039 (17) 0.0065 (17) −0.0058 (17)
C18 0.018 (2) 0.020 (2) 0.020 (2) −0.0010 (19) 0.0049 (18) −0.0013 (19)
C19 0.018 (2) 0.016 (2) 0.026 (2) −0.0003 (18) 0.0045 (19) −0.0038 (19)
C20 0.017 (2) 0.020 (2) 0.020 (2) −0.0020 (18) 0.0061 (17) −0.0057 (18)
C21 0.020 (2) 0.021 (3) 0.019 (2) −0.001 (2) 0.0047 (18) −0.0016 (19)
C22 0.019 (2) 0.017 (2) 0.023 (2) −0.0015 (18) 0.0068 (18) −0.0037 (19)
O1W 0.0217 (18) 0.036 (2) 0.0234 (19) −0.0020 (17) 0.0056 (15) −0.0065 (17)

Geometric parameters (Å, °)

Br1—C20 1.898 (5) C10—C11 1.397 (7)
S1—O3 1.451 (4) C10—H10A 0.93
S1—O2 1.452 (4) C11—C12 1.402 (6)
S1—O4 1.462 (4) C12—C13 1.393 (7)
S1—C17 1.790 (5) C12—H12A 0.93
O1—C11 1.365 (6) C13—H13A 0.93
O1—C15 1.427 (6) C14—H14A 0.96
N1—C1 1.361 (6) C14—H14B 0.96
N1—C5 1.374 (6) C14—H14C 0.96
N1—C14 1.473 (7) C15—C16 1.520 (7)
C1—C2 1.366 (8) C15—H15A 0.97
C1—H1A 0.93 C15—H15B 0.97
C2—C3 1.385 (8) C16—H16A 0.96
C2—H2A 0.93 C16—H16B 0.96
C3—C4 1.383 (7) C16—H16C 0.96
C3—H3A 0.93 C17—C22 1.387 (7)
C4—C5 1.401 (7) C17—C18 1.390 (8)
C4—H4A 0.93 C18—C19 1.390 (7)
C5—C6 1.471 (7) C18—H18A 0.93
C6—C7 1.341 (7) C19—C20 1.389 (7)
C6—H6A 0.93 C19—H19A 0.93
C7—C8 1.466 (7) C20—C21 1.402 (8)
C7—H7A 0.93 C21—C22 1.393 (7)
C8—C13 1.393 (7) C21—H21A 0.93
C8—C9 1.400 (7) C22—H22A 0.93
C9—C10 1.390 (7) O1W—H2W1 0.85
C9—H9A 0.93 O1W—H1W1 0.85
O3—S1—O2 114.3 (3) C13—C12—C11 119.7 (4)
O3—S1—O4 113.0 (3) C13—C12—H12A 120.1
O2—S1—O4 111.7 (3) C11—C12—H12A 120.1
O3—S1—C17 105.8 (2) C12—C13—C8 121.3 (5)
O2—S1—C17 105.8 (3) C12—C13—H13A 119.4
O4—S1—C17 105.3 (2) C8—C13—H13A 119.4
C11—O1—C15 118.2 (4) N1—C14—H14A 109.5
C1—N1—C5 121.3 (4) N1—C14—H14B 109.5
C1—N1—C14 117.7 (4) H14A—C14—H14B 109.5
C5—N1—C14 121.0 (4) N1—C14—H14C 109.5
N1—C1—C2 121.5 (5) H14A—C14—H14C 109.5
N1—C1—H1A 119.2 H14B—C14—H14C 109.5
C2—C1—H1A 119.2 O1—C15—C16 106.1 (4)
C1—C2—C3 119.2 (5) O1—C15—H15A 110.5
C1—C2—H2A 120.4 C16—C15—H15A 110.5
C3—C2—H2A 120.4 O1—C15—H15B 110.5
C4—C3—C2 119.3 (5) C16—C15—H15B 110.5
C4—C3—H3A 120.4 H15A—C15—H15B 108.7
C2—C3—H3A 120.4 C15—C16—H16A 109.5
C3—C4—C5 121.3 (5) C15—C16—H16B 109.5
C3—C4—H4A 119.3 H16A—C16—H16B 109.5
C5—C4—H4A 119.3 C15—C16—H16C 109.5
N1—C5—C4 117.4 (4) H16A—C16—H16C 109.5
N1—C5—C6 118.7 (4) H16B—C16—H16C 109.5
C4—C5—C6 123.9 (4) C22—C17—C18 120.9 (5)
C7—C6—C5 122.6 (5) C22—C17—S1 118.5 (4)
C7—C6—H6A 118.7 C18—C17—S1 120.6 (4)
C5—C6—H6A 118.7 C19—C18—C17 120.0 (5)
C6—C7—C8 126.1 (5) C19—C18—H18A 120.0
C6—C7—H7A 116.9 C17—C18—H18A 120.0
C8—C7—H7A 116.9 C20—C19—C18 118.6 (5)
C13—C8—C9 118.4 (5) C20—C19—H19A 120.7
C13—C8—C7 123.5 (4) C18—C19—H19A 120.7
C9—C8—C7 118.1 (4) C19—C20—C21 122.2 (5)
C10—C9—C8 121.2 (5) C19—C20—Br1 119.0 (4)
C10—C9—H9A 119.4 C21—C20—Br1 118.8 (4)
C8—C9—H9A 119.4 C22—C21—C20 118.0 (5)
C9—C10—C11 119.9 (4) C22—C21—H21A 121.0
C9—C10—H10A 120.0 C20—C21—H21A 121.0
C11—C10—H10A 120.0 C17—C22—C21 120.2 (5)
O1—C11—C10 115.7 (4) C17—C22—H22A 119.9
O1—C11—C12 124.7 (4) C21—C22—H22A 119.9
C10—C11—C12 119.5 (4) H2W1—O1W—H1W1 107.7
C5—N1—C1—C2 −0.3 (7) O1—C11—C12—C13 −179.3 (4)
C14—N1—C1—C2 178.9 (5) C10—C11—C12—C13 −0.2 (7)
N1—C1—C2—C3 −1.0 (8) C11—C12—C13—C8 −0.1 (7)
C1—C2—C3—C4 1.4 (8) C9—C8—C13—C12 0.1 (7)
C2—C3—C4—C5 −0.6 (8) C7—C8—C13—C12 179.2 (5)
C1—N1—C5—C4 1.1 (7) C11—O1—C15—C16 174.6 (4)
C14—N1—C5—C4 −178.1 (5) O3—S1—C17—C22 −39.4 (5)
C1—N1—C5—C6 −179.1 (4) O2—S1—C17—C22 −161.1 (4)
C14—N1—C5—C6 1.8 (7) O4—S1—C17—C22 80.5 (4)
C3—C4—C5—N1 −0.6 (7) O3—S1—C17—C18 143.5 (4)
C3—C4—C5—C6 179.5 (5) O2—S1—C17—C18 21.8 (5)
N1—C5—C6—C7 170.2 (5) O4—S1—C17—C18 −96.6 (4)
C4—C5—C6—C7 −10.0 (8) C22—C17—C18—C19 −1.0 (7)
C5—C6—C7—C8 −179.9 (5) S1—C17—C18—C19 176.0 (4)
C6—C7—C8—C13 2.2 (8) C17—C18—C19—C20 0.2 (7)
C6—C7—C8—C9 −178.7 (5) C18—C19—C20—C21 0.8 (8)
C13—C8—C9—C10 0.1 (7) C18—C19—C20—Br1 −179.8 (4)
C7—C8—C9—C10 −179.0 (5) C19—C20—C21—C22 −0.9 (8)
C8—C9—C10—C11 −0.4 (8) Br1—C20—C21—C22 179.7 (4)
C15—O1—C11—C10 176.5 (4) C18—C17—C22—C21 0.9 (7)
C15—O1—C11—C12 −4.3 (7) S1—C17—C22—C21 −176.2 (4)
C9—C10—C11—O1 179.6 (4) C20—C21—C22—C17 0.1 (7)
C9—C10—C11—C12 0.4 (7)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
O1W—H2W1···O4 0.85 2.09 2.929 (6) 171
O1W—H1W1···O2i 0.85 1.99 2.827 (6) 168
C1—H1A···O1Wii 0.93 2.23 3.154 (7) 176
C2—H2A···O1Wiii 0.93 2.43 3.223 (7) 143
C4—H4A···O4 0.93 2.50 3.378 (7) 158
C6—H6A···O3iv 0.93 2.56 3.442 (7) 159
C13—H13A···O3iv 0.93 2.49 3.387 (7) 161
C14—H14A···O2v 0.96 2.57 3.384 (7) 143
C14—H14C···O3iv 0.96 2.51 3.129 (7) 122

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

Footnotes

1

This paper is dedicated to His Majesty King Bhumibol Adulyadej of Thailand (King Rama IX) for his sustainable development of the country.

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: CI5012).

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 global, I. DOI: 10.1107/S1600536809055846/ci5012sup1.cif

e-66-0o305-sup1.cif (22.5KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809055846/ci5012Isup2.hkl

e-66-0o305-Isup2.hkl (307.7KB, hkl)

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


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