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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Sep 30;67(Pt 10):o2793. doi: 10.1107/S1600536811039134

(S)-N-{1-[5-(4-Chloro­benzyl­sulfanyl)-1,3,4-oxadiazol-2-yl]eth­yl}-4-methyl­benzene­sulfonamide

Tayyaba Syed a, Shahid Hameed a,*, Peter G Jones b
PMCID: PMC3201458  PMID: 22064948

Abstract

The title compound, C18H18ClN3O3S2, adopts by folding the form of a distorted disc. Inter­planar angles are 29.51 (7) and 63.43 (7)° from the five-membered ring to the aromatic systems and 34.80 (6)° between these two latter rings. The absolute configuration was confirmed by determination of the Flack parameter. In the crystal, the mol­ecules are linked by four hydrogen bonds, one classical (N—H⋯N) and three ‘weak’ (C—H⋯O), forming layers parallel to the ac plane; these are in turn linked in the third dimension by Cl⋯N [3.1689 (16) Å] and Cl⋯O [3.3148 (13) Å] contacts to the heterocyclic ring.

Related literature

For the chemotherapeutic effects of substituted-1,3,4-oxadiazole derivatives, see: Aboraia et al. (2006); Akhtar et al. (2008, 2010); Khan et al. (2005); Mishra et al. (2005); Zahid et al. (2009). Based on the known structures of 2,5-disubstituted-1,3,4-oxadiazo­les with diverse biological activity, we have designed and synthesized several new derivatives of 1,3,4-oxadiazo­les and evaluated their anti-HIV activity, see: Syed et al. (2011).graphic file with name e-67-o2793-scheme1.jpg

Experimental

Crystal data

  • C18H18ClN3O3S2

  • M r = 423.92

  • Orthorhombic, Inline graphic

  • a = 5.5928 (3) Å

  • b = 17.5004 (7) Å

  • c = 20.1431 (7) Å

  • V = 1971.53 (15) Å3

  • Z = 4

  • Cu Kα radiation

  • μ = 3.90 mm−1

  • T = 100 K

  • 0.15 × 0.10 × 0.06 mm

Data collection

  • Oxford Diffraction Xcalibur Nova A diffractometer

  • Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) T min = 0.785, T max = 1.000

  • 31188 measured reflections

  • 3762 independent reflections

  • 3625 reflections with I > 2σ(I)

  • R int = 0.046

Refinement

  • R[F 2 > 2σ(F 2)] = 0.026

  • wR(F 2) = 0.069

  • S = 1.04

  • 3762 reflections

  • 250 parameters

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

  • Δρmax = 0.31 e Å−3

  • Δρmin = −0.28 e Å−3

  • Absolute structure: Flack (1983), 1563 Friedel pairs

  • Flack parameter: −0.001 (11)

Data collection: CrysAlis PRO Oxford Diffraction (2010); 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: XP (Siemens, 1994) and RPLUTO (CCDC, 2007); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811039134/bt5653sup1.cif

e-67-o2793-sup1.cif (28.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811039134/bt5653Isup2.hkl

e-67-o2793-Isup2.hkl (184.5KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811039134/bt5653Isup3.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
N5—H05⋯N4i 0.90 (3) 2.19 (3) 3.068 (2) 166 (2)
C15—H15B⋯O2ii 0.99 2.41 3.301 (2) 149
C9—H9⋯O2iii 0.95 2.43 3.178 (2) 136
C15—H15B⋯O3iv 0.99 2.47 3.007 (2) 113

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

supplementary crystallographic information

Comment

Substituted-1,3,4-oxadiazole derivatives are of significant interest because of their chemotherapeutic effects such as anti-proliferative (Zahid et al., 2009), anti-tumour and anti-viral (Akhtar et al., 2008), anti-microbial (Mishra et al., 2005), urease inhibition (Akhtar et al., 2010), tyrosinase inhibition (Khan et al., 2005), and anti-mitotic (Aboraia et al., 2006) activities. Based on the known structures of 2,5-disubstituted-1,3,4-oxadiazoles with diverse biological activities, we have designed and synthesized several new derivatives of 1,3,4-oxadiazoles and evaluated their anti-HIV activity (Syed et al., 2011). In this paper, we report the crystal structure of one of these compounds.

The molecule of the enantiomerically pure title compound is shown in Fig. 1. Bond lengths and angles may be regarded as normal. The molecule has considerable potential for flexibility; the shape actually adopted is that of a short cylinder or disc, albeit distorted, in which the rings form part of the circumference. The smallest dimension of the molecular "box" is calculated by the program RPLUTO (CCDC, 2007) as 6.8 Å, which is close to the calculated distance between the para H atoms of a phenyl group (including van der Waals' radii). All three rings are planar within r.m.s. deviations of < 0.01 Å; interplanar angles are 29.51 (7)° and 63.43 (7)° from the five-membered ring to the aromatic systems C8–13 and C16–21 respectively, and 34.80 (6)° between these two latter rings. To close the circumference of the cylinder, the methyl hydrogen H14C approaches the centroid of the ring C16–21 at a distance of 3.08 Å.

The molecular packing is determined by four hydrogen bonds, one classical and three "weak" (including a three-centre system based on H15B), which link the molecules to form layers parallel to the ac plane (Fig. 2). It can be seen that the Cl atoms project out of this plane (the angle between the bond C19—Cl and the plane is 72°) and the Cl atoms thereby form short contacts Cl···N3 3.1689 (16) Å, operator -x, y - 1/2, -z + 1/2, and Cl···O1 3.3148 (13) Å, operator -x + 1, y - 1/2, -z + 1/2, to the oxadiazole ring, thus linking the layers (Fig. 3). The approximately linear angle C19—Cl···N3 166.31 (8)° is consistent with the description of Cl···N3 as a halogen bond.

Experimental

The title compound was prepared according to a reported procedure (Syed et al., 2011) and recrystallized from acetone/water.

Refinement

The hydrogen at N5 was refined freely. Methyl H atoms were identified in difference syntheses, idealized and refined using rigid groups allowed to rotate but not tip, with C—H 0.98 Å, H—C—H 109.5°. Other H atoms were introduced at the calculated positions and refined using a riding model, with aromatic C—H 0.95, methylene C—H 0.99, methine C—H 1.00 Å. The Uiso(H) values were set equal to mUeq(C) of the parent carbons, with m = 1.5 for methyls and 1.2 for all other H.

The absolute configuration (S at C6) was established by the Flack parameter of -0.001 (11).

Figures

Fig. 1.

Fig. 1.

The molecule of the title compound. Ellipsoids represent 50% probability levels.

Fig. 2.

Fig. 2.

Molecular packing of the title compound viewed parallel to the b axis in the region y≈ 1/2.. Thick dashed lines represent classical and thin dashed lines "weak" hydrogen bonds. The numbering corresponds to the order in the H bond Table. H atoms not involved in H bonds are omitted.

Fig. 3.

Fig. 3.

Molecular packing of the title compound viewed parallel to the c axis in the region z≈ 1/8. A l l H atoms are omitted. The thick dashed lines represent Cl···O and Cl···N contacts.

Crystal data

C18H18ClN3O3S2 Dx = 1.428 Mg m3
Mr = 423.92 Cu Kα radiation, λ = 1.54184 Å
Orthorhombic, P212121 Cell parameters from 23563 reflections
a = 5.5928 (3) Å θ = 3.3–75.8°
b = 17.5004 (7) Å µ = 3.90 mm1
c = 20.1431 (7) Å T = 100 K
V = 1971.53 (15) Å3 Tablet, colourless
Z = 4 0.15 × 0.10 × 0.06 mm
F(000) = 880

Data collection

Oxford Diffraction Xcalibur Nova A diffractometer 3762 independent reflections
Radiation source: Nova (Cu) X-ray Source 3625 reflections with I > 2σ(I)
mirror Rint = 0.046
Detector resolution: 10.3543 pixels mm-1 θmax = 70.2°, θmin = 3.4°
ω–scan h = −6→6
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2010) k = −21→20
Tmin = 0.785, Tmax = 1.000 l = −24→24
31188 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)] = 0.026 H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.069 w = 1/[σ2(Fo2) + (0.0449P)2 + 0.4932P] where P = (Fo2 + 2Fc2)/3
S = 1.04 (Δ/σ)max = 0.001
3762 reflections Δρmax = 0.31 e Å3
250 parameters Δρmin = −0.28 e Å3
0 restraints Absolute structure: Flack (1983), 1563 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: −0.001 (11)

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.Non-bonded contacts:3.1689 (0.0016) Cl - N3_$5 3.3148 (0.0013) Cl - O1_$6 3.7719 (0.0007) Cl - S1_$6166.31 (0.08) C19 - Cl - N3_$5 102.19 (0.11) Cl - N3_$5 - C2_$5 126.37 (0.07) C19 - Cl - O1_$6 109.03 (0.09) Cl - O1_$6 - C2_$6 114.16 (0.06) C19 - Cl - S1_$6 83.66 (0.06) Cl - S1_$6 - C2_$6Operators for generating equivalent atoms: $5 - x, y - 1/2, -z + 1/2 $6 - x + 1, y - 1/2, -z + 1/2===============================================================Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane)2.6855 (0.0038) x - 4.6429 (0.0122) y + 16.8416 (0.0087) z = 2.0416 (0.0053)* -0.0119 (0.0012) C16 * 0.0104 (0.0013) C17 * 0.0005 (0.0013) C18 * -0.0099 (0.0013) C19 * 0.0082 (0.0013) C20 * 0.0027 (0.0013) C21Rms deviation of fitted atoms = 0.0084- 1.1391 (0.0042) x + 17.0266 (0.0034) y - 2.2001 (0.0174) z = 7.9763 (0.0084)Angle to previous plane (with approximate e.s.d.) = 63.43 (0.07)* -0.0027 (0.0009) O1 * 0.0047 (0.0010) C2 * -0.0046 (0.0010) N3 * 0.0027 (0.0010) N4 * -0.0002 (0.0010) C5Rms deviation of fitted atoms = 0.00342.6434 (0.0040) x - 12.9885 (0.0091) y + 9.5712 (0.0144) z = 1.4590 (0.0089)Angle to previous plane (with approximate e.s.d.) = 29.51 (0.07)* 0.0016 (0.0013) C8 * -0.0004 (0.0013) C9 * 0.0015 (0.0014) C10 * -0.0039 (0.0014) C11 * 0.0051 (0.0015) C12 * -0.0040 (0.0014) C13Rms deviation of fitted atoms = 0.00322.6855 (0.0038) x - 4.6429 (0.0122) y + 16.8416 (0.0087) z = 2.0416 (0.0053)Angle to previous plane (with approximate e.s.d.) = 34.80 (0.08)* -0.0119 (0.0012) C16 * 0.0104 (0.0013) C17 * 0.0005 (0.0013) C18 * -0.0099 (0.0013) C19 * 0.0082 (0.0013) C20 * 0.0027 (0.0013) C21Rms deviation of fitted atoms = 0.0084
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
Cl 0.05592 (10) 0.18862 (3) 0.15994 (2) 0.03349 (12)
S1 0.52403 (8) 0.54474 (3) 0.263650 (19) 0.02387 (11)
S2 0.77730 (8) 0.45463 (3) 0.555955 (19) 0.02286 (11)
O1 0.5636 (2) 0.55679 (7) 0.39301 (5) 0.0211 (3)
O2 1.0271 (3) 0.44179 (8) 0.56672 (6) 0.0292 (3)
O3 0.6148 (3) 0.45159 (8) 0.61070 (6) 0.0303 (3)
C2 0.4061 (3) 0.54027 (10) 0.34332 (8) 0.0193 (3)
N3 0.1914 (3) 0.52799 (9) 0.36370 (7) 0.0235 (3)
N4 0.2027 (3) 0.53824 (9) 0.43387 (7) 0.0229 (3)
C5 0.4199 (3) 0.55439 (9) 0.44771 (8) 0.0202 (3)
N5 0.7624 (3) 0.54058 (9) 0.52475 (7) 0.0221 (3)
H05 0.879 (5) 0.5469 (14) 0.4944 (12) 0.034 (6)*
C6 0.5302 (3) 0.57714 (10) 0.51284 (8) 0.0225 (4)
H6 0.4186 0.5626 0.5495 0.027*
C7 0.5667 (4) 0.66361 (11) 0.51427 (9) 0.0311 (4)
H7A 0.6287 0.6788 0.5578 0.047*
H7B 0.4137 0.6892 0.5062 0.047*
H7C 0.6813 0.6783 0.4797 0.047*
C8 0.6782 (3) 0.38998 (10) 0.49450 (9) 0.0236 (4)
C9 0.4622 (4) 0.35176 (11) 0.50209 (10) 0.0289 (4)
H9 0.3651 0.3602 0.5401 0.035*
C10 0.3915 (4) 0.30098 (11) 0.45291 (11) 0.0332 (5)
H10 0.2447 0.2743 0.4577 0.040*
C11 0.5301 (4) 0.28842 (11) 0.39702 (10) 0.0317 (4)
C12 0.7460 (4) 0.32732 (12) 0.39112 (9) 0.0334 (5)
H12 0.8441 0.3185 0.3534 0.040*
C13 0.8207 (4) 0.37862 (11) 0.43917 (9) 0.0278 (4)
H13 0.9671 0.4056 0.4343 0.033*
C14 0.4505 (5) 0.23359 (13) 0.34315 (11) 0.0460 (6)
H14A 0.3121 0.2043 0.3588 0.069*
H14B 0.5816 0.1985 0.3325 0.069*
H14C 0.4062 0.2625 0.3033 0.069*
C15 0.2572 (4) 0.52048 (10) 0.21572 (8) 0.0243 (4)
H15A 0.1158 0.5422 0.2384 0.029*
H15B 0.2691 0.5450 0.1716 0.029*
C16 0.2174 (3) 0.43593 (10) 0.20602 (8) 0.0217 (4)
C17 0.0137 (3) 0.40140 (11) 0.23032 (9) 0.0267 (4)
H17 −0.0945 0.4301 0.2568 0.032*
C18 −0.0354 (4) 0.32510 (11) 0.21652 (9) 0.0273 (4)
H18 −0.1774 0.3020 0.2328 0.033*
C19 0.1239 (4) 0.28349 (11) 0.17903 (9) 0.0249 (4)
C20 0.3328 (4) 0.31573 (11) 0.15569 (9) 0.0284 (4)
H20 0.4433 0.2861 0.1308 0.034*
C21 0.3790 (3) 0.39220 (11) 0.16906 (9) 0.0264 (4)
H21 0.5218 0.4150 0.1529 0.032*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Cl 0.0429 (3) 0.0264 (2) 0.0311 (2) −0.00061 (19) −0.0014 (2) −0.00327 (18)
S1 0.0258 (2) 0.0332 (2) 0.01268 (18) −0.00294 (18) 0.00137 (15) −0.00194 (16)
S2 0.0256 (2) 0.0304 (2) 0.01258 (18) 0.00513 (18) 0.00069 (15) 0.00086 (15)
O1 0.0218 (6) 0.0281 (6) 0.0133 (5) −0.0008 (5) 0.0012 (5) −0.0009 (5)
O2 0.0297 (7) 0.0400 (7) 0.0179 (6) 0.0082 (6) −0.0051 (5) −0.0023 (5)
O3 0.0356 (8) 0.0373 (7) 0.0180 (6) 0.0076 (6) 0.0067 (5) 0.0046 (5)
C2 0.0219 (9) 0.0211 (8) 0.0150 (7) 0.0014 (6) −0.0008 (6) 0.0002 (6)
N3 0.0288 (9) 0.0297 (8) 0.0121 (7) −0.0004 (6) 0.0004 (6) 0.0000 (5)
N4 0.0251 (8) 0.0292 (8) 0.0144 (6) −0.0015 (7) 0.0012 (6) 0.0013 (6)
C5 0.0242 (9) 0.0207 (8) 0.0155 (8) 0.0024 (7) 0.0033 (7) 0.0013 (6)
N5 0.0215 (8) 0.0292 (8) 0.0154 (7) −0.0007 (6) 0.0006 (6) −0.0004 (6)
C6 0.0243 (10) 0.0268 (9) 0.0162 (8) 0.0011 (7) 0.0025 (7) 0.0002 (6)
C7 0.0442 (12) 0.0287 (10) 0.0205 (9) 0.0013 (9) −0.0028 (8) −0.0057 (7)
C8 0.0266 (10) 0.0238 (9) 0.0202 (8) 0.0032 (7) −0.0008 (7) 0.0038 (7)
C9 0.0259 (10) 0.0289 (9) 0.0320 (10) 0.0040 (8) 0.0047 (8) 0.0044 (7)
C10 0.0264 (11) 0.0277 (9) 0.0454 (12) −0.0036 (8) −0.0050 (8) 0.0063 (8)
C11 0.0428 (12) 0.0263 (9) 0.0259 (9) −0.0046 (9) −0.0113 (9) 0.0055 (7)
C12 0.0459 (13) 0.0366 (11) 0.0175 (8) −0.0087 (9) 0.0011 (8) −0.0015 (7)
C13 0.0319 (11) 0.0328 (10) 0.0187 (8) −0.0066 (8) 0.0035 (7) 0.0016 (7)
C14 0.0648 (16) 0.0385 (11) 0.0349 (11) −0.0163 (11) −0.0161 (12) 0.0023 (9)
C15 0.0284 (10) 0.0299 (9) 0.0146 (8) 0.0006 (7) −0.0036 (7) 0.0011 (7)
C16 0.0238 (9) 0.0300 (9) 0.0112 (7) 0.0026 (7) −0.0036 (6) 0.0007 (6)
C17 0.0270 (10) 0.0331 (9) 0.0199 (8) 0.0032 (8) 0.0011 (7) −0.0022 (7)
C18 0.0261 (10) 0.0347 (10) 0.0211 (8) 0.0001 (8) 0.0011 (7) 0.0012 (7)
C19 0.0314 (10) 0.0258 (9) 0.0173 (8) 0.0007 (7) −0.0056 (7) −0.0004 (7)
C20 0.0314 (10) 0.0335 (10) 0.0202 (8) 0.0041 (8) 0.0018 (7) −0.0041 (7)
C21 0.0252 (10) 0.0346 (10) 0.0194 (8) −0.0008 (7) 0.0028 (7) −0.0003 (7)

Geometric parameters (Å, °)

Cl—C19 1.7462 (19) C16—C21 1.399 (3)
S1—C2 1.7369 (17) C17—C18 1.391 (3)
S1—C15 1.8272 (19) C18—C19 1.376 (3)
S2—O3 1.4300 (13) C19—C20 1.380 (3)
S2—O2 1.4314 (15) C20—C21 1.389 (3)
S2—N5 1.6323 (15) C6—H6 1.0000
S2—C8 1.7662 (19) C7—H7A 0.9800
O1—C2 1.364 (2) C7—H7B 0.9800
O1—C5 1.365 (2) C7—H7C 0.9800
C2—N3 1.287 (2) C9—H9 0.9500
N3—N4 1.4262 (19) C10—H10 0.9500
N4—C5 1.278 (2) C12—H12 0.9500
C5—C6 1.504 (2) C13—H13 0.9500
N5—C6 1.468 (2) C14—H14A 0.9800
C6—C7 1.527 (3) C14—H14B 0.9800
C8—C13 1.384 (3) C14—H14C 0.9800
C8—C9 1.389 (3) C15—H15A 0.9900
C9—C10 1.388 (3) C15—H15B 0.9900
C10—C11 1.384 (3) C17—H17 0.9500
C11—C12 1.391 (3) C18—H18 0.9500
C11—C14 1.515 (3) C20—H20 0.9500
C12—C13 1.385 (3) C21—H21 0.9500
C15—C16 1.509 (2) N5—H05 0.90 (3)
C16—C17 1.380 (3)
C2—S1—C15 99.64 (8) C20—C21—C16 120.64 (18)
O3—S2—O2 119.84 (8) C6—N5—H05 118.5 (16)
O3—S2—N5 107.38 (8) S2—N5—H05 109.7 (16)
O2—S2—N5 104.64 (8) N5—C6—H6 108.7
O3—S2—C8 108.50 (9) C5—C6—H6 108.7
O2—S2—C8 108.17 (8) C7—C6—H6 108.7
N5—S2—C8 107.72 (8) C6—C7—H7A 109.5
C2—O1—C5 101.85 (13) C6—C7—H7B 109.5
N3—C2—O1 113.82 (14) H7A—C7—H7B 109.5
N3—C2—S1 131.04 (13) C6—C7—H7C 109.5
O1—C2—S1 115.02 (12) H7A—C7—H7C 109.5
C2—N3—N4 104.70 (14) H7B—C7—H7C 109.5
C5—N4—N3 106.62 (14) C10—C9—H9 120.7
N4—C5—O1 113.00 (15) C8—C9—H9 120.7
N4—C5—C6 129.72 (15) C11—C10—H10 119.3
O1—C5—C6 117.03 (16) C9—C10—H10 119.3
C6—N5—S2 120.65 (12) C13—C12—H12 119.4
N5—C6—C5 112.98 (14) C11—C12—H12 119.4
N5—C6—C7 108.09 (16) C8—C13—H13 120.6
C5—C6—C7 109.49 (15) C12—C13—H13 120.6
C13—C8—C9 121.33 (18) C11—C14—H14A 109.5
C13—C8—S2 118.41 (15) C11—C14—H14B 109.5
C9—C8—S2 120.27 (14) H14A—C14—H14B 109.5
C10—C9—C8 118.51 (18) C11—C14—H14C 109.5
C11—C10—C9 121.49 (19) H14A—C14—H14C 109.5
C10—C11—C12 118.54 (18) H14B—C14—H14C 109.5
C10—C11—C14 121.2 (2) C16—C15—H15A 108.6
C12—C11—C14 120.2 (2) S1—C15—H15A 108.6
C13—C12—C11 121.28 (19) C16—C15—H15B 108.6
C8—C13—C12 118.84 (19) S1—C15—H15B 108.6
C16—C15—S1 114.63 (13) H15A—C15—H15B 107.6
C17—C16—C21 118.88 (17) C16—C17—H17 119.6
C17—C16—C15 120.35 (17) C18—C17—H17 119.6
C21—C16—C15 120.66 (17) C19—C18—H18 120.3
C16—C17—C18 120.82 (17) C17—C18—H18 120.3
C19—C18—C17 119.33 (18) C19—C20—H20 120.5
C18—C19—C20 121.24 (18) C21—C20—H20 120.5
C18—C19—Cl 118.89 (15) C20—C21—H21 119.7
C20—C19—Cl 119.87 (15) C16—C21—H21 119.7
C19—C20—C21 119.05 (17)
C5—O1—C2—N3 −0.76 (19) N5—S2—C8—C9 −110.51 (15)
C5—O1—C2—S1 175.70 (11) C13—C8—C9—C10 0.5 (3)
C15—S1—C2—N3 −3.60 (19) S2—C8—C9—C10 −179.52 (15)
C15—S1—C2—O1 −179.31 (13) C8—C9—C10—C11 −0.5 (3)
O1—C2—N3—N4 0.94 (19) C9—C10—C11—C12 0.8 (3)
S1—C2—N3—N4 −174.82 (14) C9—C10—C11—C14 −179.29 (19)
C2—N3—N4—C5 −0.73 (19) C10—C11—C12—C13 −1.1 (3)
N3—N4—C5—O1 0.3 (2) C14—C11—C12—C13 178.9 (2)
N3—N4—C5—C6 174.36 (16) C9—C8—C13—C12 −0.8 (3)
C2—O1—C5—N4 0.24 (18) S2—C8—C13—C12 179.18 (16)
C2—O1—C5—C6 −174.64 (14) C11—C12—C13—C8 1.1 (3)
O3—S2—N5—C6 −45.79 (14) C2—S1—C15—C16 −86.77 (14)
O2—S2—N5—C6 −174.15 (12) S1—C15—C16—C17 118.83 (16)
C8—S2—N5—C6 70.90 (14) S1—C15—C16—C21 −64.89 (19)
S2—N5—C6—C5 −83.75 (17) C21—C16—C17—C18 −2.2 (3)
S2—N5—C6—C7 154.93 (12) C15—C16—C17—C18 174.13 (16)
N4—C5—C6—N5 138.58 (19) C16—C17—C18—C19 1.1 (3)
O1—C5—C6—N5 −47.6 (2) C17—C18—C19—C20 0.9 (3)
N4—C5—C6—C7 −100.9 (2) C17—C18—C19—Cl −178.08 (14)
O1—C5—C6—C7 73.0 (2) C18—C19—C20—C21 −1.6 (3)
O3—S2—C8—C13 −174.53 (14) Cl—C19—C20—C21 177.35 (14)
O2—S2—C8—C13 −43.07 (17) C19—C20—C21—C16 0.4 (3)
N5—S2—C8—C13 69.52 (17) C17—C16—C21—C20 1.5 (3)
O3—S2—C8—C9 5.45 (17) C15—C16—C21—C20 −174.86 (17)
O2—S2—C8—C9 136.91 (15)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N5—H05···N4i 0.90 (3) 2.19 (3) 3.068 (2) 166 (2)
C15—H15B···O2ii 0.99 2.41 3.301 (2) 149.
C9—H9···O2iii 0.95 2.43 3.178 (2) 136.
C15—H15B···O3iv 0.99 2.47 3.007 (2) 113.

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT5653).

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 datablock(s) I, global. DOI: 10.1107/S1600536811039134/bt5653sup1.cif

e-67-o2793-sup1.cif (28.1KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811039134/bt5653Isup2.hkl

e-67-o2793-Isup2.hkl (184.5KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811039134/bt5653Isup3.cml

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


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