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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Oct 23;66(Pt 11):o2925. doi: 10.1107/S1600536810042066

Ethyl 2-[5-(4-chloro­phen­yl)-1-(4-fluoro­phen­yl)-1H-pyrazol-3-yl]-4-methyl­thia­zole-5-carboxyl­ate

Wan-Sin Loh a,, Hoong-Kun Fun a,*,§, R Venkat Ragavan b, V Vijayakumar b, S Sarveswari b
PMCID: PMC3009042  PMID: 21589099

Abstract

In the title compound, C22H17ClFN3O2S, the pyrazole ring is approximately planar with a maximum deviation of 0.001 (4) Å and makes dihedral angles of 4.95 (19), 35.78 (18) and 54.73 (18)° with the thia­zole, fluoro­benzene and chloro­benzene rings, respectively. In the crystal, inter­molecular C—H⋯O hydrogen bonds link the mol­ecules into chains along the a axis.

Related literature

For background to pyrazole derivatives and their anti­microbial activity, see: Ragavan et al. (2009, 2010). For bond-length data, see: Allen et al. (1987). For a related structure, see: Loh et al. (2010). For the stability of the temperature controller used in the data collection, see: Cosier & Glazer (1986).graphic file with name e-66-o2925-scheme1.jpg

Experimental

Crystal data

  • C22H17ClFN3O2S

  • M r = 441.90

  • Monoclinic, Inline graphic

  • a = 12.0296 (5) Å

  • b = 19.4428 (6) Å

  • c = 9.5847 (3) Å

  • β = 112.922 (1)°

  • V = 2064.74 (12) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.32 mm−1

  • T = 100 K

  • 0.42 × 0.17 × 0.08 mm

Data collection

  • Bruker SMART APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS, Bruker, 2009) T min = 0.878, T max = 0.976

  • 30630 measured reflections

  • 4697 independent reflections

  • 3944 reflections with I > 2σ(I)

  • R int = 0.043

Refinement

  • R[F 2 > 2σ(F 2)] = 0.056

  • wR(F 2) = 0.163

  • S = 1.24

  • 4697 reflections

  • 273 parameters

  • H-atom parameters constrained

  • Δρmax = 0.63 e Å−3

  • Δρmin = −0.53 e Å−3

Data collection: APEX2 (Bruker, 2009); cell refinement: SAINT (Bruker, 2009); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; 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/S1600536810042066/fj2354sup1.cif

e-66-o2925-sup1.cif (22.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810042066/fj2354Isup2.hkl

e-66-o2925-Isup2.hkl (230.1KB, 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
C15—H15A⋯O2i 0.93 2.48 3.251 (5) 141

Symmetry code: (i) Inline graphic.

Acknowledgments

HKF and WSL thank Universiti Sains Malaysia (USM) for the Research University Grant (1001/PFIZIK/811160). WSL thanks Malaysian Government and USM for the award of Research Fellowship. VV is grateful to the DST-India for funding through the Young Scientist Scheme (Fast Track Proposal).

supplementary crystallographic information

Comment

Antibacterial and antifungal activities of azoles are most widely studied and some of them are in clinical practice as anti-microbial agents. However, the azole-resistant strains had led to the development of new antimicrobial compounds. In particular pyrazole derivatives are extensively studied and used as antimicrobial agents. Pyrazole is an important class of heterocyclic compounds and many pyrazole derivatives are reported to have a broad spectrum of biological properties, such as anti-inflammatory, antifungal, herbicidal, anti-tumour, cytotoxic, molecular modelling and antiviral activities. Pyrazole derivatives also act as anti-angiogenic agents, A3 adenosine receptor antagonists, neuropeptide YY5 receptor antagonists, kinase inhibitor for treatment of type 2 diabetes, hyperlipidemia, obesity and thrombopiotinmimetics. Recently urea derivatives of pyrazoles have been reported as potent inhibitors of p38 kinase. Since the high electronegativity of halogens (particularly chlorine and fluorine) in the aromatic part of the drug molecules play an important role in enhancing their biological activity, we are interested to have 4-fluoro or 4-chloro substitution in the aryls of 1,5-diaryl pyrazoles. As part of our on-going research aiming the synthesis of new antimicrobial compounds, we have reported the synthesis of novel pyrazole derivatives and their microbial activities (Ragavan et al., 2009;2010).

The title compound consists of four rings, namely pyrazole (C1–C3/N1/N2), thiazole (C4/N3/C5/C6/S1), fluorophenyl (C11–C16/F1) and chlorophenyl (C17–C22/Cl1) rings (Fig. 1). The pyrazole ring is approximately planar with a maximum deviation of 0.001 (4) Å at atom C1 and makes dihedral angles of 4.95 (19), 35.78 (18) and 54.73 (18)° with the thiazole, fluorophenyl and chlorophenyl rings, respectively. Bond lengths (Allen et al., 1987) and angles are within the normal ranges and are comparable to the related structure (Loh et al., 2010).

In the crystal packing (Fig. 2), intermolecular C15—H15A···O2 hydrogen bonds link the molecules into one-dimensional chains along the a axis.

Experimental

The compound has been synthesized using the method available in the literature (Ragavan et al., 2010) and recrystallized using the ethanol-chloroform 1:1 mixture. Yield: 81%. M.p.: 411.3–413 K.

Refinement

All H atoms were positioned geometrically with the bond length of C–H being 0.93 to 0.97 Å and were refined using a riding model, with Uiso(H) = 1.2 or 1.5 Ueq(C). A rotating group model was applied to the methyl groups.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound, showing 50% probability displacement ellipsoids and the atom-numbering scheme.

Fig. 2.

Fig. 2.

The crystal packing of the title compound, showing one-dimensional chains along the a axis. H atoms not involved in the intermolecular interactions (dashed lines) have been omitted for clarity.

Crystal data

C22H17ClFN3O2S F(000) = 912
Mr = 441.90 Dx = 1.422 Mg m3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 9879 reflections
a = 12.0296 (5) Å θ = 2.8–32.9°
b = 19.4428 (6) Å µ = 0.32 mm1
c = 9.5847 (3) Å T = 100 K
β = 112.922 (1)° Plate, colourless
V = 2064.74 (12) Å3 0.42 × 0.17 × 0.08 mm
Z = 4

Data collection

Bruker SMART APEXII CCD area-detector diffractometer 4697 independent reflections
Radiation source: fine-focus sealed tube 3944 reflections with I > 2σ(I)
graphite Rint = 0.043
φ and ω scans θmax = 27.5°, θmin = 1.8°
Absorption correction: multi-scan (SADABS, Bruker, 2009) h = −15→15
Tmin = 0.878, Tmax = 0.976 k = −25→25
30630 measured reflections l = −12→12

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)] = 0.056 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.163 H-atom parameters constrained
S = 1.24 w = 1/[σ2(Fo2) + (0.P)2 + 9.3055P] where P = (Fo2 + 2Fc2)/3
4697 reflections (Δ/σ)max < 0.001
273 parameters Δρmax = 0.63 e Å3
0 restraints Δρmin = −0.53 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 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
S1 0.28859 (8) 0.28472 (4) −0.01128 (10) 0.0162 (2)
Cl1 −0.24355 (9) −0.04920 (5) 0.40468 (12) 0.0288 (2)
F1 −0.2939 (2) 0.38188 (13) 0.2896 (3) 0.0373 (6)
O1 0.4449 (2) 0.36177 (13) −0.1138 (3) 0.0239 (6)
O2 0.5434 (2) 0.27417 (14) −0.1712 (3) 0.0247 (6)
N1 0.0936 (3) 0.24138 (15) 0.0961 (3) 0.0161 (6)
N2 0.0143 (3) 0.21207 (15) 0.1472 (3) 0.0154 (6)
N3 0.3202 (3) 0.15335 (15) 0.0001 (4) 0.0176 (6)
C1 0.0322 (3) 0.14214 (17) 0.1675 (4) 0.0160 (7)
C2 0.1269 (3) 0.12630 (18) 0.1269 (4) 0.0165 (7)
H2A 0.1608 0.0832 0.1279 0.020*
C3 0.1616 (3) 0.18936 (18) 0.0837 (4) 0.0164 (7)
C4 0.2558 (3) 0.20259 (17) 0.0272 (4) 0.0155 (7)
C5 0.4011 (3) 0.18060 (18) −0.0546 (4) 0.0178 (7)
C6 0.3963 (3) 0.25092 (18) −0.0694 (4) 0.0165 (7)
C7 0.4701 (3) 0.29491 (19) −0.1238 (4) 0.0185 (7)
C8 0.5145 (4) 0.4118 (2) −0.1592 (5) 0.0281 (9)
H8A 0.5329 0.3938 −0.2422 0.034*
H8B 0.5898 0.4220 −0.0750 0.034*
C9 0.4385 (4) 0.4758 (2) −0.2080 (5) 0.0326 (10)
H9A 0.4861 0.5124 −0.2229 0.049*
H9B 0.4099 0.4887 −0.1310 0.049*
H9C 0.3708 0.4669 −0.3010 0.049*
C10 0.4855 (4) 0.1330 (2) −0.0880 (5) 0.0257 (9)
H10A 0.4783 0.1399 −0.1903 0.039*
H10B 0.4654 0.0863 −0.0754 0.039*
H10C 0.5669 0.1424 −0.0196 0.039*
C11 −0.0686 (3) 0.25574 (18) 0.1786 (4) 0.0150 (7)
C12 −0.0298 (3) 0.32104 (18) 0.2356 (4) 0.0179 (7)
H12A 0.0474 0.3358 0.2498 0.021*
C13 −0.1070 (3) 0.36415 (19) 0.2714 (4) 0.0207 (8)
H13A −0.0829 0.4083 0.3082 0.025*
C14 −0.2197 (4) 0.3401 (2) 0.2510 (5) 0.0247 (8)
C15 −0.2614 (3) 0.2759 (2) 0.1924 (5) 0.0242 (8)
H15A −0.3383 0.2613 0.1796 0.029*
C16 −0.1848 (3) 0.2336 (2) 0.1528 (4) 0.0215 (8)
H16A −0.2113 0.1908 0.1093 0.026*
C17 −0.0370 (3) 0.09629 (17) 0.2271 (4) 0.0162 (7)
C18 −0.0471 (3) 0.10914 (19) 0.3647 (4) 0.0207 (8)
H18A −0.0105 0.1478 0.4208 0.025*
C19 −0.1115 (3) 0.06460 (19) 0.4186 (5) 0.0229 (8)
H19A −0.1185 0.0732 0.5103 0.027*
C20 −0.1653 (3) 0.00709 (18) 0.3334 (5) 0.0205 (8)
C21 −0.1571 (3) −0.00729 (18) 0.1970 (5) 0.0217 (8)
H21A −0.1939 −0.0461 0.1416 0.026*
C22 −0.0923 (3) 0.03780 (18) 0.1440 (4) 0.0204 (8)
H22A −0.0858 0.0289 0.0521 0.025*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0197 (4) 0.0132 (4) 0.0191 (5) 0.0005 (3) 0.0115 (3) −0.0001 (3)
Cl1 0.0279 (5) 0.0246 (5) 0.0372 (6) −0.0057 (4) 0.0161 (4) 0.0090 (4)
F1 0.0383 (14) 0.0349 (14) 0.0523 (18) 0.0144 (11) 0.0324 (13) 0.0036 (12)
O1 0.0305 (14) 0.0161 (12) 0.0328 (16) −0.0035 (11) 0.0209 (13) 0.0009 (11)
O2 0.0246 (14) 0.0259 (14) 0.0306 (16) −0.0008 (11) 0.0184 (12) 0.0002 (12)
N1 0.0176 (14) 0.0160 (14) 0.0180 (16) −0.0010 (11) 0.0104 (12) 0.0007 (12)
N2 0.0165 (14) 0.0137 (14) 0.0184 (16) −0.0008 (11) 0.0093 (12) −0.0001 (11)
N3 0.0198 (14) 0.0151 (14) 0.0198 (17) −0.0012 (11) 0.0096 (12) −0.0017 (12)
C1 0.0181 (16) 0.0141 (16) 0.0151 (18) −0.0028 (13) 0.0058 (13) −0.0019 (13)
C2 0.0207 (17) 0.0148 (16) 0.0153 (18) −0.0004 (13) 0.0085 (14) −0.0014 (13)
C3 0.0163 (16) 0.0154 (16) 0.0194 (19) −0.0008 (12) 0.0088 (14) −0.0010 (13)
C4 0.0168 (16) 0.0143 (16) 0.0160 (18) −0.0014 (12) 0.0069 (13) −0.0002 (13)
C5 0.0189 (17) 0.0177 (16) 0.0185 (19) −0.0005 (13) 0.0090 (14) −0.0028 (14)
C6 0.0178 (16) 0.0192 (17) 0.0145 (18) −0.0005 (13) 0.0086 (14) −0.0034 (13)
C7 0.0190 (17) 0.0208 (17) 0.0160 (19) −0.0027 (13) 0.0072 (14) −0.0004 (14)
C8 0.031 (2) 0.0214 (19) 0.038 (3) −0.0080 (16) 0.0197 (19) 0.0015 (17)
C9 0.034 (2) 0.022 (2) 0.040 (3) −0.0068 (17) 0.013 (2) 0.0059 (18)
C10 0.0263 (19) 0.0199 (18) 0.038 (2) 0.0011 (15) 0.0207 (18) −0.0050 (17)
C11 0.0191 (16) 0.0188 (16) 0.0097 (17) 0.0032 (13) 0.0084 (13) 0.0027 (13)
C12 0.0187 (17) 0.0179 (17) 0.0174 (19) 0.0013 (13) 0.0074 (14) 0.0022 (14)
C13 0.0302 (19) 0.0203 (17) 0.0136 (18) 0.0050 (15) 0.0105 (15) 0.0018 (14)
C14 0.0262 (19) 0.028 (2) 0.026 (2) 0.0118 (16) 0.0168 (17) 0.0062 (17)
C15 0.0183 (17) 0.030 (2) 0.027 (2) 0.0033 (15) 0.0113 (16) 0.0083 (17)
C16 0.0192 (17) 0.0217 (18) 0.024 (2) −0.0005 (14) 0.0090 (15) 0.0037 (15)
C17 0.0179 (16) 0.0142 (16) 0.0179 (19) 0.0006 (13) 0.0084 (14) 0.0016 (13)
C18 0.0223 (18) 0.0159 (16) 0.024 (2) −0.0039 (14) 0.0097 (15) −0.0008 (14)
C19 0.0252 (19) 0.0219 (18) 0.026 (2) −0.0018 (15) 0.0141 (16) 0.0015 (15)
C20 0.0195 (17) 0.0170 (17) 0.027 (2) −0.0014 (13) 0.0115 (15) 0.0067 (15)
C21 0.0246 (18) 0.0139 (16) 0.026 (2) −0.0033 (14) 0.0094 (16) −0.0010 (15)
C22 0.0265 (19) 0.0164 (17) 0.021 (2) −0.0020 (14) 0.0121 (16) −0.0028 (14)

Geometric parameters (Å, °)

S1—C4 1.719 (3) C9—H9B 0.9600
S1—C6 1.727 (3) C9—H9C 0.9600
Cl1—C20 1.747 (4) C10—H10A 0.9600
F1—C14 1.360 (4) C10—H10B 0.9600
O1—C7 1.347 (4) C10—H10C 0.9600
O1—C8 1.456 (4) C11—C12 1.389 (5)
O2—C7 1.207 (4) C11—C16 1.389 (5)
N1—C3 1.334 (4) C12—C13 1.389 (5)
N1—N2 1.356 (4) C12—H12A 0.9300
N2—C1 1.378 (4) C13—C14 1.375 (5)
N2—C11 1.429 (4) C13—H13A 0.9300
N3—C4 1.319 (4) C14—C15 1.380 (6)
N3—C5 1.378 (4) C15—C16 1.393 (5)
C1—C2 1.374 (5) C15—H15A 0.9300
C1—C17 1.478 (5) C16—H16A 0.9300
C2—C3 1.408 (5) C17—C18 1.394 (5)
C2—H2A 0.9300 C17—C22 1.399 (5)
C3—C4 1.457 (5) C18—C19 1.389 (5)
C5—C6 1.373 (5) C18—H18A 0.9300
C5—C10 1.498 (5) C19—C20 1.387 (5)
C6—C7 1.467 (5) C19—H19A 0.9300
C8—C9 1.507 (6) C20—C21 1.378 (6)
C8—H8A 0.9700 C21—C22 1.394 (5)
C8—H8B 0.9700 C21—H21A 0.9300
C9—H9A 0.9600 C22—H22A 0.9300
C4—S1—C6 88.81 (17) C5—C10—H10B 109.5
C7—O1—C8 116.8 (3) H10A—C10—H10B 109.5
C3—N1—N2 104.8 (3) C5—C10—H10C 109.5
N1—N2—C1 111.8 (3) H10A—C10—H10C 109.5
N1—N2—C11 118.3 (3) H10B—C10—H10C 109.5
C1—N2—C11 129.8 (3) C12—C11—C16 120.9 (3)
C4—N3—C5 110.6 (3) C12—C11—N2 118.1 (3)
C2—C1—N2 106.4 (3) C16—C11—N2 121.0 (3)
C2—C1—C17 128.9 (3) C13—C12—C11 119.6 (3)
N2—C1—C17 124.7 (3) C13—C12—H12A 120.2
C1—C2—C3 105.1 (3) C11—C12—H12A 120.2
C1—C2—H2A 127.4 C14—C13—C12 118.5 (4)
C3—C2—H2A 127.4 C14—C13—H13A 120.8
N1—C3—C2 111.8 (3) C12—C13—H13A 120.8
N1—C3—C4 119.4 (3) F1—C14—C13 118.2 (4)
C2—C3—C4 128.7 (3) F1—C14—C15 118.6 (4)
N3—C4—C3 123.1 (3) C13—C14—C15 123.2 (3)
N3—C4—S1 115.5 (3) C14—C15—C16 118.1 (3)
C3—C4—S1 121.4 (3) C14—C15—H15A 120.9
C6—C5—N3 114.5 (3) C16—C15—H15A 120.9
C6—C5—C10 126.7 (3) C11—C16—C15 119.6 (4)
N3—C5—C10 118.8 (3) C11—C16—H16A 120.2
C5—C6—C7 127.6 (3) C15—C16—H16A 120.2
C5—C6—S1 110.6 (3) C18—C17—C22 119.1 (3)
C7—C6—S1 121.8 (3) C18—C17—C1 121.8 (3)
O2—C7—O1 124.5 (3) C22—C17—C1 119.0 (3)
O2—C7—C6 124.8 (3) C19—C18—C17 120.5 (3)
O1—C7—C6 110.7 (3) C19—C18—H18A 119.8
O1—C8—C9 107.1 (3) C17—C18—H18A 119.8
O1—C8—H8A 110.3 C20—C19—C18 118.9 (4)
C9—C8—H8A 110.3 C20—C19—H19A 120.6
O1—C8—H8B 110.3 C18—C19—H19A 120.6
C9—C8—H8B 110.3 C21—C20—C19 122.2 (3)
H8A—C8—H8B 108.6 C21—C20—Cl1 119.5 (3)
C8—C9—H9A 109.5 C19—C20—Cl1 118.3 (3)
C8—C9—H9B 109.5 C20—C21—C22 118.4 (3)
H9A—C9—H9B 109.5 C20—C21—H21A 120.8
C8—C9—H9C 109.5 C22—C21—H21A 120.8
H9A—C9—H9C 109.5 C21—C22—C17 120.9 (4)
H9B—C9—H9C 109.5 C21—C22—H22A 119.6
C5—C10—H10A 109.5 C17—C22—H22A 119.6
C3—N1—N2—C1 0.2 (4) C5—C6—C7—O1 −176.2 (4)
C3—N1—N2—C11 177.3 (3) S1—C6—C7—O1 2.9 (4)
N1—N2—C1—C2 −0.2 (4) C7—O1—C8—C9 154.3 (4)
C11—N2—C1—C2 −176.9 (3) N1—N2—C11—C12 −34.4 (5)
N1—N2—C1—C17 177.8 (3) C1—N2—C11—C12 142.0 (4)
C11—N2—C1—C17 1.1 (6) N1—N2—C11—C16 145.5 (3)
N2—C1—C2—C3 0.1 (4) C1—N2—C11—C16 −38.0 (5)
C17—C1—C2—C3 −177.8 (4) C16—C11—C12—C13 1.8 (5)
N2—N1—C3—C2 −0.1 (4) N2—C11—C12—C13 −178.2 (3)
N2—N1—C3—C4 178.5 (3) C11—C12—C13—C14 1.0 (5)
C1—C2—C3—N1 0.0 (4) C12—C13—C14—F1 178.4 (3)
C1—C2—C3—C4 −178.5 (4) C12—C13—C14—C15 −2.1 (6)
C5—N3—C4—C3 179.1 (3) F1—C14—C15—C16 179.8 (3)
C5—N3—C4—S1 0.0 (4) C13—C14—C15—C16 0.3 (6)
N1—C3—C4—N3 −174.4 (3) C12—C11—C16—C15 −3.6 (6)
C2—C3—C4—N3 4.0 (6) N2—C11—C16—C15 176.5 (3)
N1—C3—C4—S1 4.7 (5) C14—C15—C16—C11 2.5 (6)
C2—C3—C4—S1 −176.9 (3) C2—C1—C17—C18 123.4 (4)
C6—S1—C4—N3 0.4 (3) N2—C1—C17—C18 −54.1 (5)
C6—S1—C4—C3 −178.8 (3) C2—C1—C17—C22 −55.6 (5)
C4—N3—C5—C6 −0.4 (5) N2—C1—C17—C22 126.9 (4)
C4—N3—C5—C10 178.2 (3) C22—C17—C18—C19 −0.2 (5)
N3—C5—C6—C7 179.9 (3) C1—C17—C18—C19 −179.2 (3)
C10—C5—C6—C7 1.4 (7) C17—C18—C19—C20 0.2 (6)
N3—C5—C6—S1 0.7 (4) C18—C19—C20—C21 −0.1 (6)
C10—C5—C6—S1 −177.8 (3) C18—C19—C20—Cl1 178.8 (3)
C4—S1—C6—C5 −0.6 (3) C19—C20—C21—C22 0.0 (6)
C4—S1—C6—C7 −179.8 (3) Cl1—C20—C21—C22 −178.9 (3)
C8—O1—C7—O2 −2.1 (6) C20—C21—C22—C17 0.0 (6)
C8—O1—C7—C6 178.0 (3) C18—C17—C22—C21 0.1 (5)
C5—C6—C7—O2 3.9 (6) C1—C17—C22—C21 179.1 (3)
S1—C6—C7—O2 −177.0 (3)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C15—H15A···O2i 0.93 2.48 3.251 (5) 141

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: FJ2354).

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/S1600536810042066/fj2354sup1.cif

e-66-o2925-sup1.cif (22.4KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810042066/fj2354Isup2.hkl

e-66-o2925-Isup2.hkl (230.1KB, hkl)

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


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