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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Jan 28;65(Pt 2):o385–o386. doi: 10.1107/S1600536809002591

5,11,17,23-Tetra-tert-butyl-25,26,27,28-tetra­kis[2-(2-chloro­ethoxy)eth­oxy]-2,8,14,20-tetra­sulfonyl­calix[4]arene

Ling Hu a, Yang Liu a, Jiang-Ping Ma a, Dian-Shun Guo a,*
PMCID: PMC2968348  PMID: 21581981

Abstract

Mol­ecules of the title compound, C56H76Cl4O16S4, have crystallographic C 2 symmetry and adopt a 1,3-alternate conformation where the four –OCH2CH2OCH2CH2Cl groups are located alternately above and below the virtual plane (R) defined by the four bridging S atoms. The dihedral angles between the plane (R) and the phenolic rings are 72.85 (7) and 74.57 (7)°. An unusual 24-membered macrocyclic ring is formed in the crystal structure with an array of eight intra­molecular C—H⋯O hydrogen bonds between the ether arm H atoms and the sulfonyl O atoms. In the supra­molecular structure, the mol­ecular components are linked into infinite zigzag one-dimensional chains by a combination of four inter­molecular C—H⋯O hydrogen bonds, forming R 2 2(13), R 2 2(16), R 2 2(21) and R 2 2(26) ring motifs. These chains are augmented into a wave-like two-dimensional network by weak C⋯O inter­actions. One tert-butyl group shows rotational disorder, and one CH2CH2Cl group is disordered over two orientations; the site-occupation factors are 0.756 (6) and 0.244 (6) for the two tert-butyl groups, and 0.808 (3) and 0.192 (3) for the two CH2CH2Cl units.

Related literature

For general background on the chemistry of thia­calix[4]arene derivatives, see: Shokova & Kovalev (2003); Lhoták (2004); Morohashi et al. (2006). For related crystal structures, see: Mislin et al. (1998, 1999); Akdas et al. (1999, 2000); Lhoták et al. (2002); Horiuchi et al. (2007); Xu et al. (2008). For the synthesis of sulfonyl­calix[4]arene derivatives, see: Iki et al. (1998); Guo et al. (2007). For hydrogen-bond motifs, see: Bernstein et al. (1995). For C⋯O short contacts, see: Manoj et al. (2007). For atomic radii, see: Bondi (1964).graphic file with name e-65-0o385-scheme1.jpg

Experimental

Crystal data

  • C56H76Cl4O16S4

  • M r = 1275.21

  • Monoclinic, Inline graphic

  • a = 22.496 (2) Å

  • b = 16.0372 (15) Å

  • c = 19.8646 (19) Å

  • β = 120.355 (1)°

  • V = 6184.1 (10) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.39 mm−1

  • T = 173 (2) K

  • 0.41 × 0.28 × 0.24 mm

Data collection

  • Bruker SMART CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 1999) T min = 0.856, T max = 0.912

  • 15381 measured reflections

  • 5442 independent reflections

  • 4709 reflections with I > 2σ(I)

  • R int = 0.022

Refinement

  • R[F 2 > 2σ(F 2)] = 0.058

  • wR(F 2) = 0.166

  • S = 1.09

  • 5442 reflections

  • 402 parameters

  • 27 restraints

  • H-atom parameters constrained

  • Δρmax = 1.30 e Å−3

  • Δρmin = −0.80 e Å−3

Data collection: SMART (Bruker, 1999); cell refinement: SAINT (Bruker, 1999); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809002591/zl2171sup1.cif

e-65-0o385-sup1.cif (29.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809002591/zl2171Isup2.hkl

e-65-0o385-Isup2.hkl (266.6KB, 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
C11—H11A⋯O1i 0.99 2.48 3.232 (4) 133
C11—H11B⋯O3 0.99 2.51 3.103 (4) 118
C20—H20B⋯O1ii 0.98 2.57 3.377 (5) 139
C21—H21C⋯O8iii 0.98 2.60 3.462 (6) 146
C25—H25A⋯O2 0.99 2.58 3.099 (4) 113
C25—H25B⋯O4 0.99 2.45 3.217 (4) 134

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

Acknowledgments

Financial support from the National Natural Science Foundation of China (grant No. 20572064) and the Natural Science Foundation of Shandong Province (grant No. Y2006B30) is gratefully acknowledged.

supplementary crystallographic information

Comment

Thiacalix[4]arenes have attracted considerable interest in recent years as useful scaffolds for highly organized ionophores (Shokova & Kovalev, 2003; Lhoták, 2004; Morohashi et al., 2006; Guo et al., 2007). Compared with classical calix[4]arenes, the presence of four bridging S atoms results in a differing complexation ability, and a diverse cavity and conformational behavior. Moreover, by virtue of the sulfide function, thiacalix[4]arenes can undergo unique transformations that are not applicable to the classical calix[4]arenes, the most important of which is oxidation to sulfinyl and sulfonyl functions. All four sulfide groups of thiacalix[4]arenes, for instance, can be easily converted to sulfones by a small excess amount of an oxidant such as hydrogen peroxide or sodium perborate in an organic acid solvent (Iki et al., 1998; Mislin et al., 1998). A number of crystal stuctures of sulfonyl derivatives of thiacalix[4]arenes (Mislin et al., 1998; Akdas et al., 2000; Lhoták et al., 2002; Horiuchi et al., 2007) have been described. We now present the crystal structure of a new sulfonyl derivative thiacalix[4]arene, 5,11,17,23-tetra-tert-butyl-25,26,27,28-tetrakis[2-(2-chloroethoxy)ethoxy]-2,8,14,20-tetrasulfonylcalix[4]arene.

The title sulfonylcalix[4]arene derivative is shown in Fig. 1. It was found to adopt a 1,3-alternate conformation with O atoms of the sulfones pointing outward. The main geometric parameters of the title molecule are comparable to those reported for the similar structures (Mislin et al., 1998; Akdas et al., 2000) and most bond lengths and angles are consistent with the values presented for 1,3-alternate-5,11,17,23-tetra-tert-butyl-25,26,27,28-tetrakismethyl-2,8,14,20-tetrasulfonylcalix[4]arene (Mislin et al., 1998). The sulfonylcalix[4]arene shape of the title compound can be characterized by the values of the dihedral angles between the phenolic rings and the plane (R) defined by the four bridging S atoms. The dihedral angles between the plane (R) and the aromatic rings are 74.57 (7) and 72.85 (7)°, respectively. Actually, the title molecule has a pseudo 4-fold rotation-reflection (S4) axis. Consistent with this symmetry, the adjacent phenyl rings lie above and below the plane (R), and interplanar angles of the opposing aromatic rings are 34.31 (8) and 38.86 (14)°. The pseudo S4 symmetry also reasonably depicts the almost parallel orientation of the four ether arms above and below the plane (R). The separations between diametrically located ethereal O5 and O5i, O7 and O7i [Symmetry code: (i) -x + 1, y, -z + 3/2] are 4.660 (4) and 4.347 (4) Å, respectively. In the crystal packing, 1,3-alternate molecules are packed along the b axis, forming a type of a beautiful nanotubular array extending in the b direction (Fig. 3). Such a packing was found in the cases of several 1,3-alternate thiaclix[4]arene derivatives (Akdas et al., 1999, 2000; Guo et al., 2007; Xu et al., 2008).

Although no conventional hydrogen bonds are found, various intra- and intermolecular C—H···O hydrogen bonds exist in the crystal structure (Table 1). Interestingly, an unusual 24-membered macrocyclic ring is formed by an array of eight intramolecular C—H···O hydrogen bonds between the sulfonyl O atoms and the ether arm protons closer the phenolic rings, which stabilize the 1,3-alternate conformation (Fig. 4). In this macrocyclic ring, both O atoms of each sulfonyl group act as a hydrogen-bond acceptor, via H, to two C atoms belonging to both adjacent ether arms, respectively. A similar hydrogen bonding array was observed in the structure of the related compound p-tert-butyltetrasulfinylcalix[4]arene, however, it is formed with only four intramolecular O—H···O hydrogen bonds between the OH and SO groups (Mislin, et al., 1999). On the other hand, in the supramolecular structure, infinite zigzag one-dimensional chains are generated by a combination of four intermolecular C—H···O hydrogen bonds, locally forming different ring motifs: two R22(13), one R22(16), two R22(21), and one R22(26) (Bernstein et al., 1995), and making a distorted capsule at each link in the chain (Fig. 4). These motifs arise from atoms C20 and C21 at (x, y, z) and (-x + 1, -y + 1, -z + 1) in neighboring molecules that act as hydrogen-bond donors, respectively, via H20B, to atoms O1 at (-x + 1, -y + 1, -z + 1) and (x, y, z), via H21C, to atoms O8 at (x, -y + 1, z - 1/2) and (-x + 1, y, -z + 3/2). The zigzag chains are linked into wave-like two-dimensional networks by the C···O weak interactions (Manoj et al., 2007) between C10iv [symmetry code: (iv) – x + 3/2, – y + 3/2, –z + 2] and O3. The C10iv···O3 distance is 3.143 (4) Å, less than the sum of the van der Waals radii for C and O atoms (C = 1.70 Å, O = 1.52 Å; Bondi, 1964).

Experimental

For the synthesis of the title compound, to a solution of 1,3-alternate-5,11,17,23-tetra-tert-butyl-25,26,27,28-tetrakis[2-(2-chloroethoxy)ethoxy]thiacalix[4]arene, prepared according to the published precedure (Guo et al., 2007), (0.200 g, 0.174 mmol) in CHCl3 (10 ml) and CF3CO2H (1.50 ml) was added 30% H2O2 (0.90 ml, 7.840 mmol). The resulting mixture was stirred at 298 K for 50 h, and neutralized with a saturated aqueous solution of NaHCO3. The organic layer was separated and washed with brine, and dried over anhydrous MgSO4. Removal of the solvent under reduced pressure gave the title compound as a white solid (yield 95%) by recrystallization from CH2Cl2/CH3OH. 1H NMR (300 MHz, CDCl3): δ 8.38 (s, 8H), 4.58 (t, 8H, J = 5.67 Hz), 3.84 (t, 16H, J = 5.98 Hz), 3.71 (t, 8H, J = 5.83 Hz), 1.40 (s, 36H). IR (KBr pellets, cm-1): 1304, 1137. Single crystals of the title molecule suitable for X-ray diffraction analysis were obtained by slow evaporation of a solution in CH2Cl2 and CH3OH at 273 K.

Refinement

All non-hydrogen atoms were refined with anisotropic displacement parameters. Hydrogen atoms attached to refined atoms were placed in geometrically idealized positions and refined using a riding model, with C—H = 0.93, 0.98 and 0.97 Å for aromatic, methylene and methyl H, respectively, and Uiso(H) = 1.5Ueq(C) for methyl H, and Uiso(H) = 1.2Ueq(C) for all other H atoms. In the title molecule, one of the symmetry-independent tert-butyl groups (C1—C4) shows rotational disorder, with refined site occupation factors of 0.756 (6):0.244 (6). The C—C bond lengths involving the disordered C atoms were restrained to be the same within a standard deviation of 0.02 Å, C—C distances refined to values between 1.472 and 1.5559 Å. The ADPs of C1', C2' and C3' were restrained to be isotropic within a standard deviation of 0.01 Å2. The atoms C27, C28 and Cl1 are disordered over two orientations, with refined site occupation factors of 0.808 (3):0.192 (3). The C—C, C—O and C—Cl bonds were restrained to be each the same within a standard deviation of 0.02 Å and refined to 1.453–1.461, 1.425–1.436 and 1.790–1.794 Å, respectively. The atoms C27', C28' and Cl1' were constrained to have the same ADPs as the atoms C27, C28 and Cl1.

Figures

Fig. 1.

Fig. 1.

The molecular structure of the title compound with displacement ellipsoids drawn at the 30% probability level for non-H atoms. The disordered atoms are shown, but hydrogen atoms are omitted for clarity. [Symmetry code: (i) -x + 1, y, -z + 3/2].

Fig. 2.

Fig. 2.

The crystal packing of the title compound viewed along the b axis. Hydrogen atoms and the minor disordered units are omitted for clarity.

Fig. 3.

Fig. 3.

The array of intramolecular hydrogen-bonded rings of the title molecule viewed approximatively along the c axis. The minor disordered units and some hydrogen atoms are omitted for clarity. [Symmetry code: (i) -x + 1, y, -z + 3/2].

Fig. 4.

Fig. 4.

The hydrogen-bonded zigzag one-dimensional chains of the title molecule with R22(13), R22(16), R22(21) and R22(26) motifs. The minor disordered moieties and some hydrogen atoms are omitted for clarity. [Symmetry codes: (i) -x + 1, y, -z + 3/2; (ii) -x + 1, -y + 1, -z + 1; (iii) x, -y + 1, z - 1/2].

Crystal data

C56H76Cl4O16S4 F(000) = 2688
Mr = 1275.21 Dx = 1.370 Mg m3
Monoclinic, C2/c Mo Kα radiation, λ = 0.71073 Å
a = 22.496 (2) Å Cell parameters from 7613 reflections
b = 16.0372 (15) Å θ = 2.2–28.1°
c = 19.8646 (19) Å µ = 0.39 mm1
β = 120.355 (1)° T = 173 K
V = 6184.1 (10) Å3 Block, colourless
Z = 4 0.41 × 0.28 × 0.24 mm

Data collection

Bruker SMART CCD area-detector diffractometer 5442 independent reflections
Radiation source: fine-focus sealed tube 4709 reflections with I > 2σ(I)
graphite Rint = 0.022
φ and ω scans θmax = 25.0°, θmin = 1.7°
Absorption correction: multi-scan (SADABS; Bruker, 1999) h = −26→26
Tmin = 0.856, Tmax = 0.912 k = −16→19
15381 measured reflections l = −23→23

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)] = 0.058 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.166 H-atom parameters constrained
S = 1.09 w = 1/[σ2(Fo2) + (0.0863P)2 + 20.079P] where P = (Fo2 + 2Fc2)/3
5442 reflections (Δ/σ)max = 0.001
402 parameters Δρmax = 1.30 e Å3
27 restraints Δρmin = −0.80 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)
C5 0.63360 (14) 0.93392 (17) 0.93979 (16) 0.0206 (6)
C6 0.58157 (15) 0.89626 (18) 0.94656 (16) 0.0216 (6)
H6 0.5574 0.9283 0.9653 0.026*
C7 0.56341 (14) 0.81334 (18) 0.92702 (15) 0.0206 (6)
C8 0.59817 (14) 0.76368 (17) 0.90004 (15) 0.0198 (6)
C9 0.65037 (14) 0.80187 (17) 0.89320 (15) 0.0200 (6)
C10 0.66757 (14) 0.88537 (17) 0.91240 (16) 0.0202 (6)
H10 0.7033 0.9093 0.9066 0.024*
C11 0.60405 (18) 0.61541 (18) 0.92839 (18) 0.0298 (7)
H11A 0.5787 0.6106 0.9570 0.036*
H11B 0.6537 0.6229 0.9665 0.036*
C12 0.5924 (2) 0.5401 (2) 0.8784 (2) 0.0429 (9)
H12A 0.5460 0.5428 0.8313 0.051*
H12B 0.6269 0.5386 0.8615 0.051*
C13 0.5939 (3) 0.3938 (2) 0.8805 (3) 0.0513 (10)
H13A 0.6368 0.3866 0.8787 0.062*
H13B 0.5550 0.3982 0.8262 0.062*
C14 0.5834 (2) 0.3196 (2) 0.9195 (3) 0.0529 (10)
H14A 0.5730 0.2701 0.8855 0.063*
H14B 0.5432 0.3299 0.9260 0.063*
C15 0.64816 (14) 0.70631 (17) 0.77013 (16) 0.0191 (6)
C16 0.65912 (14) 0.62388 (18) 0.75768 (17) 0.0220 (6)
H16 0.6922 0.5919 0.8006 0.026*
C17 0.62342 (15) 0.58698 (18) 0.68504 (17) 0.0242 (6)
C22 0.57340 (15) 0.63497 (18) 0.62448 (17) 0.0245 (6)
H22 0.5466 0.6110 0.5741 0.029*
C23 0.56198 (15) 0.71742 (18) 0.63650 (17) 0.0217 (6)
C24 0.60033 (14) 0.75573 (17) 0.70897 (16) 0.0196 (6)
Cl2 0.65663 (6) 0.29815 (6) 1.01204 (7) 0.0613 (3)
O1 0.46758 (12) 0.71591 (14) 0.49020 (12) 0.0331 (5)
O2 0.53371 (11) 0.84535 (14) 0.54324 (13) 0.0309 (5)
O3 0.72979 (11) 0.67345 (13) 0.91607 (12) 0.0303 (5)
O4 0.75042 (11) 0.80237 (13) 0.86416 (13) 0.0295 (5)
O7 0.57763 (11) 0.68433 (12) 0.87321 (11) 0.0252 (5)
O8 0.59813 (14) 0.46765 (14) 0.92163 (14) 0.0395 (6)
S1 0.50048 (4) 0.77435 (5) 0.55345 (4) 0.0239 (2)
S2 0.70254 (4) 0.74481 (4) 0.86614 (4) 0.0216 (2)
C1 0.7049 (3) 1.0578 (3) 0.9434 (4) 0.0496 (16) 0.756 (6)
H1A 0.7484 1.0276 0.9745 0.074* 0.756 (6)
H1B 0.7124 1.1174 0.9555 0.074* 0.756 (6)
H1C 0.6882 1.0492 0.8878 0.074* 0.756 (6)
C2 0.5861 (2) 1.0799 (3) 0.9178 (3) 0.0416 (13) 0.756 (6)
H2A 0.5975 1.1385 0.9326 0.062* 0.756 (6)
H2B 0.5518 1.0614 0.9311 0.062* 0.756 (6)
H2C 0.5672 1.0739 0.8615 0.062* 0.756 (6)
C3 0.6783 (3) 1.0349 (3) 1.0494 (3) 0.0467 (14) 0.756 (6)
H3A 0.7201 1.0013 1.0792 0.070* 0.756 (6)
H3B 0.6428 1.0156 1.0604 0.070* 0.756 (6)
H3C 0.6888 1.0936 1.0644 0.070* 0.756 (6)
C4 0.65239 (16) 1.02564 (18) 0.96255 (18) 0.0263 (7) 0.756 (6)
C1' 0.6356 (10) 1.0747 (10) 0.8892 (9) 0.056 (5) 0.244 (6)
H1E 0.5872 1.0658 0.8494 0.084* 0.244 (6)
H1F 0.6652 1.0557 0.8692 0.084* 0.244 (6)
H1D 0.6435 1.1343 0.9018 0.084* 0.244 (6)
C2' 0.7322 (6) 1.0296 (9) 1.0160 (9) 0.039 (4) 0.244 (6)
H2D 0.7461 1.0868 1.0346 0.059* 0.244 (6)
H2F 0.7540 1.0122 0.9862 0.059* 0.244 (6)
H2E 0.7467 0.9922 1.0606 0.059* 0.244 (6)
C3' 0.6215 (9) 1.0616 (10) 1.0060 (11) 0.052 (5) 0.244 (6)
H3E 0.5711 1.0590 0.9738 0.078* 0.244 (6)
H3D 0.6360 1.1198 1.0189 0.078* 0.244 (6)
H3F 0.6367 1.0298 1.0541 0.078* 0.244 (6)
C4' 0.65239 (16) 1.02564 (18) 0.96255 (18) 0.0263 (7) 0.244 (6)
C18 0.63795 (17) 0.49736 (19) 0.66984 (19) 0.0303 (7)
C19 0.6904 (2) 0.4528 (2) 0.7460 (2) 0.0483 (10)
H19A 0.6721 0.4501 0.7814 0.072*
H19B 0.7339 0.4839 0.7709 0.072*
H19C 0.6985 0.3962 0.7339 0.072*
C20 0.5723 (3) 0.4473 (3) 0.6328 (3) 0.0730 (10)
H20A 0.5541 0.4447 0.6683 0.110*
H20B 0.5817 0.3907 0.6220 0.110*
H20C 0.5383 0.4739 0.5838 0.110*
C21 0.6712 (3) 0.5009 (3) 0.6204 (3) 0.0730 (10)
H21A 0.6829 0.4443 0.6125 0.110*
H21B 0.7132 0.5347 0.6468 0.110*
H21C 0.6391 0.5259 0.5697 0.110*
O5 0.58700 (10) 0.83690 (12) 0.71892 (11) 0.0222 (4)
C25 0.63180 (16) 0.89918 (18) 0.71453 (19) 0.0285 (7)
H25A 0.6423 0.8847 0.6732 0.034*
H25B 0.6756 0.9033 0.7649 0.034*
C26 0.59268 (19) 0.9801 (2) 0.6958 (2) 0.0406 (8)
H26A 0.5534 0.9793 0.6416 0.049*
H26B 0.5745 0.9888 0.7315 0.049*
O6 0.63887 (13) 1.04475 (14) 0.70517 (16) 0.0440 (6) 0.808 (3)
C27 0.6023 (3) 1.1211 (3) 0.6756 (3) 0.0425 (13) 0.808 (3)
H27A 0.5774 1.1352 0.7033 0.051* 0.808 (3)
H27B 0.5681 1.1150 0.6194 0.051* 0.808 (3)
C28 0.6508 (5) 1.1877 (6) 0.6868 (4) 0.0571 (18) 0.808 (3)
H28A 0.6245 1.2387 0.6606 0.069* 0.808 (3)
H28B 0.6770 1.1713 0.6611 0.069* 0.808 (3)
Cl1 0.71051 (11) 1.21148 (10) 0.78691 (10) 0.0777 (6) 0.808 (3)
O6' 0.63887 (13) 1.04475 (14) 0.70517 (16) 0.0440 (6) 0.192 (3)
C27' 0.6214 (13) 1.1202 (16) 0.6602 (17) 0.0425 (13) 0.192 (3)
H27C 0.5721 1.1329 0.6394 0.051* 0.192 (3)
H27D 0.6285 1.1120 0.6154 0.051* 0.192 (3)
C28' 0.663 (3) 1.190 (3) 0.706 (2) 0.0571 (18) 0.192 (3)
H28C 0.6464 1.2395 0.6712 0.069* 0.192 (3)
H28D 0.7103 1.1793 0.7181 0.069* 0.192 (3)
Cl1' 0.6696 (5) 1.2238 (4) 0.7962 (5) 0.0777 (6) 0.192 (3)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C5 0.0221 (14) 0.0180 (14) 0.0176 (14) −0.0005 (11) 0.0071 (12) −0.0007 (11)
C6 0.0251 (15) 0.0190 (14) 0.0192 (14) −0.0007 (11) 0.0100 (12) −0.0019 (11)
C7 0.0229 (14) 0.0199 (14) 0.0151 (13) −0.0034 (11) 0.0066 (12) 0.0010 (11)
C8 0.0243 (15) 0.0152 (14) 0.0126 (13) −0.0018 (11) 0.0039 (11) 0.0009 (10)
C9 0.0217 (14) 0.0194 (14) 0.0138 (13) 0.0031 (11) 0.0051 (11) −0.0002 (10)
C10 0.0213 (14) 0.0158 (14) 0.0194 (13) −0.0008 (11) 0.0072 (11) −0.0001 (11)
C11 0.0421 (19) 0.0162 (15) 0.0281 (16) −0.0005 (13) 0.0156 (14) 0.0035 (12)
C12 0.077 (3) 0.0179 (17) 0.045 (2) −0.0033 (16) 0.040 (2) 0.0011 (14)
C13 0.085 (3) 0.0215 (18) 0.056 (2) −0.0058 (18) 0.042 (2) −0.0071 (16)
C14 0.058 (3) 0.0266 (19) 0.071 (3) −0.0038 (17) 0.031 (2) −0.0027 (18)
C15 0.0207 (14) 0.0191 (14) 0.0193 (14) −0.0015 (11) 0.0114 (12) −0.0036 (11)
C16 0.0214 (14) 0.0183 (14) 0.0252 (15) 0.0022 (11) 0.0109 (12) −0.0001 (11)
C17 0.0266 (15) 0.0209 (15) 0.0286 (15) 0.0021 (12) 0.0165 (13) −0.0017 (12)
C22 0.0283 (16) 0.0217 (15) 0.0224 (15) 0.0020 (12) 0.0119 (13) −0.0055 (11)
C23 0.0230 (14) 0.0212 (15) 0.0212 (14) 0.0051 (11) 0.0113 (12) 0.0014 (11)
C24 0.0229 (15) 0.0152 (14) 0.0239 (15) 0.0008 (11) 0.0143 (13) −0.0003 (11)
Cl2 0.0629 (7) 0.0338 (5) 0.0756 (8) −0.0030 (5) 0.0264 (6) 0.0063 (5)
O1 0.0391 (13) 0.0349 (13) 0.0200 (11) 0.0114 (10) 0.0110 (10) −0.0027 (9)
O2 0.0374 (12) 0.0321 (12) 0.0307 (12) 0.0093 (10) 0.0227 (10) 0.0087 (9)
O3 0.0319 (12) 0.0228 (11) 0.0237 (11) 0.0081 (9) 0.0049 (9) −0.0014 (8)
O4 0.0228 (11) 0.0255 (11) 0.0382 (12) −0.0023 (9) 0.0141 (10) −0.0090 (9)
O7 0.0332 (11) 0.0144 (10) 0.0211 (10) −0.0039 (8) 0.0088 (9) −0.0010 (8)
O8 0.0649 (17) 0.0150 (11) 0.0445 (14) −0.0022 (10) 0.0321 (13) −0.0002 (10)
S1 0.0294 (4) 0.0249 (4) 0.0178 (4) 0.0076 (3) 0.0122 (3) 0.0014 (3)
S2 0.0203 (4) 0.0175 (4) 0.0215 (4) 0.0023 (3) 0.0065 (3) −0.0035 (3)
C1 0.057 (3) 0.025 (2) 0.089 (5) −0.017 (2) 0.053 (3) −0.020 (3)
C2 0.041 (3) 0.018 (2) 0.059 (3) −0.0003 (19) 0.020 (2) −0.003 (2)
C3 0.061 (4) 0.030 (3) 0.040 (3) −0.013 (2) 0.018 (3) −0.017 (2)
C4 0.0317 (16) 0.0156 (14) 0.0333 (17) −0.0031 (12) 0.0176 (14) −0.0046 (12)
C1' 0.065 (9) 0.034 (7) 0.052 (8) −0.002 (6) 0.017 (6) 0.003 (6)
C2' 0.035 (7) 0.023 (6) 0.050 (7) −0.007 (5) 0.013 (5) −0.009 (5)
C3' 0.056 (8) 0.039 (7) 0.064 (8) −0.007 (6) 0.033 (7) −0.019 (6)
C4' 0.0317 (16) 0.0156 (14) 0.0333 (17) −0.0031 (12) 0.0176 (14) −0.0046 (12)
C18 0.0352 (17) 0.0196 (16) 0.0318 (17) 0.0063 (13) 0.0137 (14) −0.0069 (12)
C19 0.071 (3) 0.0274 (19) 0.044 (2) 0.0165 (18) 0.027 (2) 0.0012 (16)
C20 0.086 (3) 0.0380 (18) 0.091 (3) 0.0217 (17) 0.042 (2) −0.0082 (17)
C21 0.086 (3) 0.0380 (18) 0.091 (3) 0.0217 (17) 0.042 (2) −0.0082 (17)
O5 0.0275 (11) 0.0138 (10) 0.0269 (11) 0.0020 (8) 0.0149 (9) −0.0013 (8)
C25 0.0317 (17) 0.0172 (15) 0.0345 (17) −0.0007 (12) 0.0153 (14) 0.0019 (12)
C26 0.039 (2) 0.0198 (16) 0.055 (2) −0.0003 (14) 0.0174 (17) 0.0041 (15)
O6 0.0430 (14) 0.0185 (12) 0.0572 (16) −0.0014 (10) 0.0157 (13) 0.0086 (11)
C27 0.042 (3) 0.0233 (19) 0.053 (3) −0.002 (2) 0.018 (2) 0.012 (2)
C28 0.055 (5) 0.031 (2) 0.055 (5) −0.011 (3) 0.006 (5) 0.012 (3)
Cl1 0.0839 (13) 0.0500 (8) 0.0731 (10) −0.0158 (8) 0.0204 (9) 0.0028 (7)
O6' 0.0430 (14) 0.0185 (12) 0.0572 (16) −0.0014 (10) 0.0157 (13) 0.0086 (11)
C27' 0.042 (3) 0.0233 (19) 0.053 (3) −0.002 (2) 0.018 (2) 0.012 (2)
C28' 0.055 (5) 0.031 (2) 0.055 (5) −0.011 (3) 0.006 (5) 0.012 (3)
Cl1' 0.0839 (13) 0.0500 (8) 0.0731 (10) −0.0158 (8) 0.0204 (9) 0.0028 (7)

Geometric parameters (Å, °)

C5—C10 1.381 (4) C2—H2A 0.9800
C5—C6 1.383 (4) C2—H2B 0.9800
C5—C4 1.534 (4) C2—H2C 0.9800
C6—C7 1.388 (4) C3—C4 1.523 (5)
C6—H6 0.9500 C3—H3A 0.9800
C7—C8 1.399 (4) C3—H3B 0.9800
C7—S1i 1.781 (3) C3—H3C 0.9800
C8—O7 1.367 (3) C1'—H1E 0.9800
C8—C9 1.391 (4) C1'—H1F 0.9800
C9—C10 1.393 (4) C1'—H1D 0.9800
C9—S2 1.772 (3) C2'—H2D 0.9800
C10—H10 0.9500 C2'—H2F 0.9800
C11—O7 1.455 (4) C2'—H2E 0.9800
C11—C12 1.499 (5) C3'—H3E 0.9800
C11—H11A 0.9900 C3'—H3D 0.9800
C11—H11B 0.9900 C3'—H3F 0.9800
C12—O8 1.411 (4) C18—C20 1.506 (6)
C12—H12A 0.9900 C18—C21 1.507 (6)
C12—H12B 0.9900 C18—C19 1.545 (5)
C13—O8 1.414 (4) C19—H19A 0.9800
C13—C14 1.503 (6) C19—H19B 0.9800
C13—H13A 0.9900 C19—H19C 0.9800
C13—H13B 0.9900 C20—H20A 0.9800
C14—Cl2 1.775 (5) C20—H20B 0.9800
C14—H14A 0.9900 C20—H20C 0.9800
C14—H14B 0.9900 C21—H21A 0.9800
C15—C16 1.390 (4) C21—H21B 0.9800
C15—C24 1.393 (4) C21—H21C 0.9800
C15—S2 1.777 (3) O5—C25 1.453 (4)
C16—C17 1.381 (4) C25—C26 1.505 (4)
C16—H16 0.9500 C25—H25A 0.9900
C17—C22 1.392 (4) C25—H25B 0.9900
C17—C18 1.537 (4) C26—O6 1.412 (4)
C22—C23 1.391 (4) C26—H26A 0.9900
C22—H22 0.9500 C26—H26B 0.9900
C23—C24 1.392 (4) O6—C27 1.425 (6)
C23—S1 1.778 (3) C27—C28 1.461 (7)
C24—O5 1.373 (3) C27—H27A 0.9900
O1—S1 1.437 (2) C27—H27B 0.9900
O2—S1 1.432 (2) C28—Cl1 1.790 (6)
O3—S2 1.433 (2) C28—H28A 0.9900
O4—S2 1.434 (2) C28—H28B 0.9900
S1—C7i 1.781 (3) C27'—C28' 1.453 (18)
C1—C4 1.503 (5) C27'—H27C 0.9900
C1—H1A 0.9800 C27'—H27D 0.9900
C1—H1B 0.9800 C28'—Cl1' 1.79 (2)
C1—H1C 0.9800 C28'—H28C 0.9900
C2—C4 1.560 (5) C28'—H28D 0.9900
C10—C5—C6 117.1 (3) C1—C4—C3 110.6 (4)
C10—C5—C4 122.1 (3) C1—C4—C5 112.9 (3)
C6—C5—C4 120.7 (3) C3—C4—C5 108.5 (3)
C5—C6—C7 122.4 (3) C1—C4—C2 108.2 (4)
C5—C6—H6 118.8 C3—C4—C2 107.5 (3)
C7—C6—H6 118.8 C5—C4—C2 109.0 (3)
C6—C7—C8 120.7 (3) H1E—C1'—H1F 109.5
C6—C7—S1i 115.6 (2) H1E—C1'—H1D 109.5
C8—C7—S1i 123.5 (2) H1F—C1'—H1D 109.5
O7—C8—C9 120.5 (3) H2D—C2'—H2F 109.5
O7—C8—C7 122.4 (3) H2D—C2'—H2E 109.5
C9—C8—C7 116.7 (3) H2F—C2'—H2E 109.5
C8—C9—C10 121.9 (3) H3E—C3'—H3D 109.5
C8—C9—S2 121.6 (2) H3E—C3'—H3F 109.5
C10—C9—S2 116.4 (2) H3D—C3'—H3F 109.5
C5—C10—C9 121.2 (3) C20—C18—C21 112.8 (4)
C5—C10—H10 119.4 C20—C18—C17 110.0 (3)
C9—C10—H10 119.4 C21—C18—C17 108.5 (3)
O7—C11—C12 104.2 (2) C20—C18—C19 107.9 (3)
O7—C11—H11A 110.9 C21—C18—C19 105.7 (3)
C12—C11—H11A 110.9 C17—C18—C19 111.9 (3)
O7—C11—H11B 110.9 C18—C19—H19A 109.5
C12—C11—H11B 110.9 C18—C19—H19B 109.5
H11A—C11—H11B 108.9 H19A—C19—H19B 109.5
O8—C12—C11 109.2 (3) C18—C19—H19C 109.5
O8—C12—H12A 109.8 H19A—C19—H19C 109.5
C11—C12—H12A 109.8 H19B—C19—H19C 109.5
O8—C12—H12B 109.8 C18—C20—H20A 109.5
C11—C12—H12B 109.8 C18—C20—H20B 109.5
H12A—C12—H12B 108.3 H20A—C20—H20B 109.5
O8—C13—C14 110.3 (3) C18—C20—H20C 109.5
O8—C13—H13A 109.6 H20A—C20—H20C 109.5
C14—C13—H13A 109.6 H20B—C20—H20C 109.5
O8—C13—H13B 109.6 C18—C21—H21A 109.5
C14—C13—H13B 109.6 C18—C21—H21B 109.5
H13A—C13—H13B 108.1 H21A—C21—H21B 109.5
C13—C14—Cl2 112.5 (3) C18—C21—H21C 109.5
C13—C14—H14A 109.1 H21A—C21—H21C 109.5
Cl2—C14—H14A 109.1 H21B—C21—H21C 109.5
C13—C14—H14B 109.1 C24—O5—C25 115.8 (2)
Cl2—C14—H14B 109.1 O5—C25—C26 105.7 (2)
H14A—C14—H14B 107.8 O5—C25—H25A 110.6
C16—C15—C24 120.9 (3) C26—C25—H25A 110.6
C16—C15—S2 115.7 (2) O5—C25—H25B 110.6
C24—C15—S2 123.2 (2) C26—C25—H25B 110.6
C17—C16—C15 122.1 (3) H25A—C25—H25B 108.7
C17—C16—H16 118.9 O6—C26—C25 107.5 (3)
C15—C16—H16 118.9 O6—C26—H26A 110.2
C16—C17—C22 117.1 (3) C25—C26—H26A 110.2
C16—C17—C18 122.5 (3) O6—C26—H26B 110.2
C22—C17—C18 120.4 (3) C25—C26—H26B 110.2
C23—C22—C17 121.1 (3) H26A—C26—H26B 108.5
C23—C22—H22 119.5 C26—O6—C27 110.1 (3)
C17—C22—H22 119.5 O6—C27—C28 109.5 (6)
C22—C23—C24 121.7 (3) O6—C27—H27A 109.8
C22—C23—S1 117.0 (2) C28—C27—H27A 109.8
C24—C23—S1 121.2 (2) O6—C27—H27B 109.8
O5—C24—C23 120.1 (2) C28—C27—H27B 109.8
O5—C24—C15 122.9 (2) H27A—C27—H27B 108.2
C23—C24—C15 116.9 (2) C27—C28—Cl1 114.0 (5)
C8—O7—C11 119.0 (2) C27—C28—H28A 108.7
C12—O8—C13 112.3 (3) Cl1—C28—H28A 108.7
O2—S1—O1 118.02 (14) C27—C28—H28B 108.7
O2—S1—C23 108.83 (14) Cl1—C28—H28B 108.7
O1—S1—C23 106.96 (13) H28A—C28—H28B 107.6
O2—S1—C7i 106.76 (13) C28'—C27'—H27C 109.2
O1—S1—C7i 107.68 (13) C28'—C27'—H27D 109.2
C23—S1—C7i 108.26 (13) H27C—C27'—H27D 107.9
O3—S2—O4 117.92 (14) C27'—C28'—Cl1' 124 (3)
O3—S2—C9 108.63 (13) C27'—C28'—H28C 106.2
O4—S2—C9 107.32 (13) Cl1'—C28'—H28C 106.2
O3—S2—C15 106.68 (13) C27'—C28'—H28D 106.2
O4—S2—C15 108.27 (13) Cl1'—C28'—H28D 106.2
C9—S2—C15 107.62 (13) H28C—C28'—H28D 106.4
C10—C5—C6—C7 0.0 (4) C14—C13—O8—C12 −166.6 (4)
C4—C5—C6—C7 −179.6 (3) C22—C23—S1—O2 −120.7 (2)
C5—C6—C7—C8 0.7 (4) C24—C23—S1—O2 54.8 (3)
C5—C6—C7—S1i 175.6 (2) C22—C23—S1—O1 7.8 (3)
C6—C7—C8—O7 −173.6 (2) C24—C23—S1—O1 −176.6 (2)
S1i—C7—C8—O7 11.9 (4) C22—C23—S1—C7i 123.6 (2)
C6—C7—C8—C9 −0.8 (4) C24—C23—S1—C7i −60.9 (3)
S1i—C7—C8—C9 −175.2 (2) C8—C9—S2—O3 −51.8 (3)
O7—C8—C9—C10 173.2 (2) C10—C9—S2—O3 123.9 (2)
C7—C8—C9—C10 0.2 (4) C8—C9—S2—O4 179.7 (2)
O7—C8—C9—S2 −11.4 (4) C10—C9—S2—O4 −4.6 (3)
C7—C8—C9—S2 175.6 (2) C8—C9—S2—C15 63.4 (3)
C6—C5—C10—C9 −0.6 (4) C10—C9—S2—C15 −120.9 (2)
C4—C5—C10—C9 179.0 (3) C16—C15—S2—O3 −19.6 (3)
C8—C9—C10—C5 0.5 (4) C24—C15—S2—O3 164.5 (2)
S2—C9—C10—C5 −175.2 (2) C16—C15—S2—O4 108.3 (2)
O7—C11—C12—O8 −164.0 (3) C24—C15—S2—O4 −67.7 (3)
O8—C13—C14—Cl2 −67.9 (4) C16—C15—S2—C9 −136.0 (2)
C24—C15—C16—C17 −0.3 (4) C24—C15—S2—C9 48.1 (3)
S2—C15—C16—C17 −176.3 (2) C10—C5—C4—C1 6.4 (5)
C15—C16—C17—C22 −2.5 (4) C6—C5—C4—C1 −174.1 (4)
C15—C16—C17—C18 176.6 (3) C10—C5—C4—C3 −116.7 (4)
C16—C17—C22—C23 2.3 (4) C6—C5—C4—C3 62.9 (4)
C18—C17—C22—C23 −176.9 (3) C10—C5—C4—C2 126.6 (3)
C17—C22—C23—C24 0.7 (5) C6—C5—C4—C2 −53.8 (4)
C17—C22—C23—S1 176.2 (2) C16—C17—C18—C20 125.9 (4)
C22—C23—C24—O5 −179.1 (3) C22—C17—C18—C20 −54.9 (4)
S1—C23—C24—O5 5.6 (4) C16—C17—C18—C21 −110.2 (4)
C22—C23—C24—C15 −3.5 (4) C22—C17—C18—C21 68.9 (4)
S1—C23—C24—C15 −178.8 (2) C16—C17—C18—C19 6.0 (4)
C16—C15—C24—O5 178.8 (2) C22—C17—C18—C19 −174.9 (3)
S2—C15—C24—O5 −5.5 (4) C23—C24—O5—C25 −98.1 (3)
C16—C15—C24—C23 3.3 (4) C15—C24—O5—C25 86.5 (3)
S2—C15—C24—C23 179.0 (2) C24—O5—C25—C26 158.7 (3)
C9—C8—O7—C11 99.0 (3) O5—C25—C26—O6 169.4 (3)
C7—C8—O7—C11 −88.4 (3) C25—C26—O6—C27 170.1 (4)
C12—C11—O7—C8 −160.8 (3) C26—O6—C27—C28 179.1 (5)
C11—C12—O8—C13 −174.6 (3) O6—C27—C28—Cl1 −65.1 (9)

Symmetry codes: (i) −x+1, y, −z+3/2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C11—H11A···O1i 0.99 2.48 3.232 (4) 133
C11—H11B···O3 0.99 2.51 3.103 (4) 118
C20—H20B···O1ii 0.98 2.57 3.377 (5) 139
C21—H21C···O8iii 0.98 2.60 3.462 (6) 146
C25—H25A···O2 0.99 2.58 3.099 (4) 113
C25—H25B···O4 0.99 2.45 3.217 (4) 134

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: ZL2171).

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/S1600536809002591/zl2171sup1.cif

e-65-0o385-sup1.cif (29.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809002591/zl2171Isup2.hkl

e-65-0o385-Isup2.hkl (266.6KB, hkl)

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


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