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The regio- and absolute stereochemistry of (7S)-N-[4-(3-thien­yl)tricyclo­[4.2.1.02,5]non-3-en-3-ylcarbon­yl]-2,10-camphorsultam tetra­hydro­furan hemisolvate, C24H29NO3S2·0.5C4H8O, and (7S)-N-[4-(4-tol­yl)tricyclo­[4.2.1.02,5]non-3-en-3-ylcarbon­yl]-2,10-camphorsultam, C27H33NO3S, have been established. One contains a half-occupancy tetra­hydro­furan solvent mol­ecule located on a twofold axis and the other contains two crystallographically unique mol­ecules which are nearly identical. The extended structures of both complexes can be explained via weak C—H...O interactions, which link the molecules together into two-dimensional sheets in the ab plane for the thienyl complex and ultimately into a three-dimensional structure for the tolyl derivative. The stereochemistry of both structures confirms that [2+2] cyclo­additions of bicyclic alkenes and alkynes catalysed by ruthenium are exclusively exo.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270109045284/ga3134sup1.cif
Contains datablocks global, VI, VII

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270109045284/ga3134VIsup2.hkl
Contains datablock VI

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270109045284/ga3134VIIsup3.hkl
Contains datablock VII

CCDC references: 763612; 763613

Comment top

Recently, the metal-catalyzed [2+2] cycloaddition reaction between bicyclic alkenes and alkynes has been utilized by several research groups as a means to generate cyclobutene rings. In terms of an asymmetric version of this process, both a chiral rhodium catalyst (Shibata et al., 2006) and a ruthenium-catalyzed (Villeneuve & Tam, 2004) reaction involving a chiral precursor have produced chiral [2+2] cyclobutene products. The ruthenium-catalyzed [2+2] cycloaddition between norbornene and a phenylactyleneacyl camphorsultam (chiral) yielded two diastereomers in a 131:1 ratio. The absolute stereochemistry of the major diastereomer (V) was established by single-crystal X-ray diffraction (Lough et al.,2004).

As an extension of this study, the Tam group is investigating the selectivity effect of different organic groups attached at the acetylenic position (see scheme). In this paper, we present the results of ruthenium-catalyzed [2+2] cycloadditions of norbornene, (I), with 3-thiophenylacteyleneacylcamphorsultam, (III), and 4-tolylacteyleneacylcamphorsultam, (IV). This yielded the expected complexes C24H29NO3S2.0.5C4H8O, (VI), and C27H33NO3S, (VII). Two diastereomers of (VI) were obtained in a 20:1 ratio, whereas the major stereoisomer of (VII) was obtained in a 104:1 ratio over the minor isomer. The absolute stereochemistry of the major isomers, (VI) and (VII), were established by the single-crystal X-ray diffraction analysis described here.

A view of (VI) is shown in Fig. 1. Elucidation of the X-ray structure establishes the absolute configuration of the following atoms in Fig. 1: C2-S, C5-R, C8-R, C14-S, C15-R, C18-S and C19-R. This is the same configuration as that observed for the phenyl derivative (V). There is a tetrahydrofuran (THF) solvent molecule occluded in the structure. It was modeled at half-occupancy, as it is located on a symmetry element, and was refined giving reasonable displacement parameters; this molecule is involved in the extended structure as discussed below.

There are two chemically identical molecules of (VII) in the asymmetric unit. They are very similar structurally with an r.m.s. fit of 0.207 Å (PLATON; Spek, 2009). As expected, both have the same configuration as that observed for (VI). The absolute configuration, as determined by anomalous dispersion, is as follows: C2-S, C5-R, C8-R, C14-S, C15-R, C18-S and C19-R for one molecule, and C32-S, C35-R, C38-R, C44-S, C45-R, C48-S and C49-R for the second. A structure of one of the molecules of (VII) is shown in Fig. 2. The difference in the two molecules is attributed to their spatially different orientations with respect to one another (see below). The geometric data for both structures (VI) and (VII) are in the normal ranges.

Weak C—H···O interactions in (VI) (see Table 1 for geometric parameters and symmetry codes) tie the molecules together. Perhaps the simplest method to describe the packing is using two `classical model' graph-set descriptors (Bernstein et al., 1995). Firstly, a `chain of rings' is formed between two weak interactions (C8—H8A···O2i and C1—H1B···O3ii) that link molecules together into ribbons along the a axis {motif C22(10)[R22(9)]; Fig. 3}. Secondly, adjacent ribbons are linked together via reciprocating C14—H14A···O1iii interactions, forming a two-dimensional network [motif R22(16)]. There are two further layers in the extension along the c axis, each of which is rotated by 120° with respect to the previous layer. The THF molecule of solvation was refined at half-occupancy, as it is located on a rotational axis; the O atom serves to link the layers together via another weak interaction (C1—H1A···O31).

As with (VI), it is the weak C—H···O interactions that control the geometry observed in the crystal structure of (VII) (Table 2). The nine weak interactions lead to a very extensive set of hydrogen-bonding motifs so only the key graph-set descriptors are noted here. The asymmetric unit contains two molecules, which couple together via two weak interactions (C3—H3B···O31 and C31—H31B···O3) to form an 11-membered ring, and, adjacent to this, a nine-membered ring is formed via C38—H38A···O1i and C1—H1B···O33ii interactions. This quaternary graph set, somewhat similar to (VI), has the motifs C22(10)[R22(11)R22(9)]: a `chain of rings' yielding ribbons along the a axis (Fig. 4). These a-axis ribbons are connected up and down the c axis according to the binary graph-set descriptor C22(12) via C50—H50A···O2iii and C9—H9A···O3iv interactions, thus forming parallel ribbons in the [010] plane. Finally, a full three-dimensional network is established via C27—H27A···O32v and C9—H9A···O3iv interactions, making C22(25) connections along the b axis. For completeness, the last two interactions in Table 2 can be described as motif S(7).

While there are no classical hydrogen-bonding networks in either of these structures, the weak interactions do seem to explain the observed geometry, which is understandable as even a weak hydrogen bond will be stronger than the van der Waals interactions. Unlike the previously published phenyl cycloadduct which shows partial ππ stacking between neighbouring phenyl rings (closest contact 3.64 Å) through secondary orbital overlap interactions (Lough et al., 2004), no such π-stacking interactions between either thiophenyl rings or tolyl rings are observed in these crystal structures.

In the case of the [2+2] cycloaddition, these crystal structures have unambiguously identified which are the major diastereomers formed in the asymmetric cycloaddition. The previous phenyl derivative combined with both the thiophenyl and tolyl derivatives herein reaffirm that [2+2] cycloadditions of bicyclic alkenes and alkynes catalyzed by ruthenium are exclusively exo with respect to their stereochemistry.

Related literature top

For related literature, see: Lough et al. (2004); Shibata et al. (2006); Spek (2009); Villeneuve & Tam (2004).

Experimental top

Preparation of compound (VI) was achieved by addition of norbornene (72.0 mg, 765 mmol), (I), and chiral alkyne (III) (52.2 mg, 0.149 mmol) to Cp*Ru(cod)Cl (please define; 7.6 mg, 0.020 mmol) in THF (0.6 ml). The mixture was stirred for 18 h at 298 K, and subsequent column chromatography of the crude reaction mixture provided a 98% yield of the two diastereomeric cycloadducts in a 20:1 ratio. Evaporative recrystallization of the column-purified product in THF provided the major diastereomer (VI), giving colourless crystals suitable for X-ray analysis.

Similarly, compound (VII) was prepared by addition of norbornene (83.0 mg, 0.881 mmol), (I), and chiral alkyne (IV) (63.2 mg, 0.177 mmol) to Cp*Ru(cod)Cl (7.1 mg, 0.018 mmol) in THF (0.5 ml). The mixture was stirred for 17 h at 298 K, and subsequent column chromatography of the crude reaction mixture provided a 79% yield of the two diastereomeric cycloadducts in a 104:1 ratio. Evaporative recrystallization of the column-purified product in THF provided major diastereomer (VII), giving colourless crystals suitable for X-ray analysis.

Both diastereomeric ratios were back-calculated from the corresponding enantiomeric excesses obtained through cleavage of the chiral auxiliary under reductive conditions (LiAlH4, AlCl3), giving an enantiomeric mixture of cycloadduct alcohols that can be resolved using a Chiralcel OJ-H high-performance liquid chromatography column.

Refinement top

Standard SADI restraints were used for the dimensions of the disordered solvent (THF), which was refined at half-occupancy. H atoms were positioned geometrically and refined using a riding model with C—H distances of 0.98 Å (CH3), 0.99 Å (CH2), 1.00 Å (CH) or 0.95 Å (aromatic CH). Uiso(H) were set at 1.2 times Ueq(C) for all except the methyl H atoms, where Uiso(H) = 1.5Ueq(C).

Computing details top

For both compounds, data collection: COLLECT (Nonius, 1997); cell refinement: DENZO–SMN (Otwinowski & Minor, 1997); data reduction: DENZO–SMN (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL/PC (Sheldrick, 2008); software used to prepare material for publication: SHELXTL/PC (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. A view of the structure of (VI), showing the crystallographic labelling scheme. Displacement ellipsoids are drawn at the 50% probablility level. For the sake of clarity, non-chiral H atoms have been omitted, as has the partial-occupancy THF molecule of solvation.
[Figure 2] Fig. 2. The molecular structure of one of the molecules of (VII), showing the atom-labelling scheme and with displacement ellipsoids drawn at the 50% probablility level. For the sake of clarity, the non-chiral H atoms have been omitted.
[Figure 3] Fig. 3. The packing of (I), showing weak C—H···O interactions as dashed lines. All H atoms, except those attached to atoms involved in weak interactions, have been omitted for clarity. The view is down the c axis, showing the ribbons along the a axis.
[Figure 4] Fig. 4. The packing of (II), showing the weak C—H···O interactions as dashed lines. All H atoms, except those involved in the displayed weak interactions, have been omitted for clarity. The view is down the c axis, showing the formation of a chain along the a axis.
(VI) (7S)-N-[4-(3-thienyl)tricyclo[4.2.1.02,5]non-3-ene-3- carbonyl]-2,10-camphorsultam tetrahydrofuran hemisolvate top
Crystal data top
C24H29NO3S2·0.5C4H8ODx = 1.335 Mg m3
Mr = 479.65Melting point: 199 K
Trigonal, P3221Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 32 2"Cell parameters from 19735 reflections
a = 12.0797 (17) Åθ = 2.0–27.5°
c = 28.326 (6) ŵ = 0.25 mm1
V = 3579.5 (10) Å3T = 150 K
Z = 6Plate, colourless
F(000) = 15360.35 × 0.22 × 0.15 mm
Data collection top
Nonius KappaCCD
diffractometer
4207 independent reflections
Radiation source: fine-focus sealed tube3310 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.041
ϕ scans, and ω scans with κ offsetsθmax = 25.0°, θmin = 2.9°
Absorption correction: multi-scan
(DENZO–SMN; Otwinowski & Minor, 1997)
h = 1414
Tmin = 0.916, Tmax = 0.963k = 1111
8354 measured reflectionsl = 3333
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.038H-atom parameters constrained
wR(F2) = 0.084 w = 1/[σ^2^(Fo^2^) + (0.0432P)^2^]
where P = (Fo^2^ + 2Fc^2^)/3
S = 1.01(Δ/σ)max < 0.001
4207 reflectionsΔρmax = 0.19 e Å3
318 parametersΔρmin = 0.31 e Å3
4 restraintsAbsolute structure: Flack (1983), 1788 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.03 (7)
Crystal data top
C24H29NO3S2·0.5C4H8OZ = 6
Mr = 479.65Mo Kα radiation
Trigonal, P3221µ = 0.25 mm1
a = 12.0797 (17) ÅT = 150 K
c = 28.326 (6) Å0.35 × 0.22 × 0.15 mm
V = 3579.5 (10) Å3
Data collection top
Nonius KappaCCD
diffractometer
4207 independent reflections
Absorption correction: multi-scan
(DENZO–SMN; Otwinowski & Minor, 1997)
3310 reflections with I > 2σ(I)
Tmin = 0.916, Tmax = 0.963Rint = 0.041
8354 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.038H-atom parameters constrained
wR(F2) = 0.084Δρmax = 0.19 e Å3
S = 1.01Δρmin = 0.31 e Å3
4207 reflectionsAbsolute structure: Flack (1983), 1788 Friedel pairs
318 parametersAbsolute structure parameter: 0.03 (7)
4 restraints
Special details top

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 F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > σ(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ 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) top
xyzUiso*/UeqOcc. (<1)
O10.60309 (17)0.69194 (15)0.12342 (5)0.0322 (5)
S10.62469 (6)0.60943 (6)0.15376 (2)0.02461 (16)
N10.52685 (17)0.57178 (19)0.20119 (6)0.0208 (5)
C10.5534 (2)0.4517 (2)0.13028 (8)0.0260 (6)
H1A0.50870.44620.10030.031*
H1B0.61980.42830.12390.031*
O20.75321 (16)0.65168 (16)0.16832 (6)0.0321 (4)
S20.33154 (8)0.91996 (7)0.31771 (2)0.0390 (2)
C20.4595 (2)0.3623 (2)0.16665 (8)0.0221 (6)
O30.39805 (16)0.62130 (17)0.24296 (6)0.0281 (4)
C30.3339 (3)0.2492 (3)0.14789 (9)0.0357 (7)
H3A0.35050.19910.12410.043*
H3B0.27790.27860.13390.043*
C40.2753 (3)0.1710 (3)0.19347 (10)0.0436 (8)
H4A0.19460.16900.20170.052*
H4B0.25780.08220.18970.052*
C50.3773 (3)0.2418 (2)0.23128 (9)0.0345 (7)
H5A0.37150.18780.25900.041*
C60.5030 (3)0.2946 (2)0.20299 (9)0.0282 (6)
C70.3740 (3)0.3634 (2)0.24425 (9)0.0334 (7)
H7A0.43410.41040.27030.040*
H7B0.28690.34360.25340.040*
C80.4166 (2)0.4394 (2)0.19764 (8)0.0236 (6)
H8A0.34240.44070.18260.028*
C90.6237 (3)0.3820 (3)0.23148 (9)0.0376 (8)
H9A0.63100.33410.25810.056*
H9B0.61820.45520.24350.056*
H9C0.69900.41250.21110.056*
C100.5244 (3)0.1911 (3)0.18097 (9)0.0387 (8)
H10A0.59780.23080.15950.058*
H10B0.44800.13080.16330.058*
H10C0.54120.14530.20600.058*
C110.5041 (2)0.6601 (2)0.22510 (8)0.0215 (6)
C120.6077 (2)0.7928 (2)0.23004 (8)0.0234 (6)
C130.6085 (2)0.8955 (2)0.25049 (8)0.0231 (6)
C140.7498 (2)0.9844 (2)0.24120 (8)0.0237 (6)
H14A0.76921.05480.21830.028*
C150.8422 (2)1.0227 (2)0.28271 (8)0.0234 (6)
H15A0.83451.07930.30660.028*
C160.9761 (2)1.0750 (2)0.26124 (9)0.0267 (6)
H16A1.04331.11870.28540.032*
H16B0.99061.13550.23520.032*
C170.9743 (2)0.9525 (3)0.24244 (9)0.0287 (7)
H17A0.99130.95860.20810.034*
H17B1.03840.93830.25900.034*
C180.8373 (2)0.8452 (2)0.25365 (8)0.0240 (6)
H18A0.82500.75700.25370.029*
C190.7505 (2)0.8655 (2)0.21943 (8)0.0221 (6)
H19A0.77430.87270.18530.027*
C200.8139 (3)0.8906 (2)0.30137 (8)0.0259 (6)
H20A0.87490.89710.32610.031*
H20B0.72490.83740.31270.031*
C210.5224 (2)0.9252 (2)0.27616 (8)0.0238 (6)
C220.3957 (3)0.8448 (3)0.28677 (8)0.0304 (7)
H22A0.34930.75730.27790.036*
C230.4727 (3)1.0620 (3)0.31785 (8)0.0291 (6)
H23A0.48501.13830.33230.035*
C240.5655 (3)1.0508 (3)0.29432 (9)0.0309 (7)
H24A0.65031.11970.29040.037*
O310.4857 (5)0.3920 (5)0.01939 (16)0.0602 (14)0.50
C320.3989 (9)0.4359 (10)0.0075 (6)0.096 (6)0.50
H32A0.32770.40220.03050.115*0.50
H32B0.36250.40460.02430.115*0.50
C330.4687 (16)0.5782 (14)0.0082 (8)0.084 (7)0.50
H33A0.45170.61080.03780.101*0.50
H33B0.44430.61270.01900.101*0.50
C340.6067 (13)0.6130 (13)0.0051 (13)0.051 (4)0.50
H34A0.64970.67120.02180.061*0.50
H34B0.65300.65460.03460.061*0.50
C350.6007 (13)0.4869 (16)0.0020 (6)0.054 (4)0.50
H35A0.60060.46910.03620.065*0.50
H35B0.67550.48800.01280.065*0.50
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0450 (12)0.0249 (11)0.0283 (9)0.0187 (10)0.0033 (8)0.0076 (8)
S10.0238 (4)0.0212 (4)0.0264 (3)0.0094 (3)0.0036 (3)0.0015 (3)
N10.0170 (11)0.0187 (12)0.0228 (10)0.0060 (10)0.0044 (8)0.0026 (9)
C10.0289 (16)0.0247 (14)0.0252 (14)0.0141 (13)0.0006 (12)0.0050 (11)
O20.0179 (10)0.0315 (11)0.0447 (10)0.0107 (8)0.0006 (8)0.0082 (9)
S20.0400 (5)0.0405 (5)0.0433 (4)0.0252 (4)0.0084 (4)0.0032 (4)
C20.0196 (14)0.0179 (13)0.0256 (13)0.0070 (12)0.0041 (11)0.0012 (11)
O30.0198 (10)0.0269 (11)0.0351 (11)0.0099 (9)0.0052 (9)0.0035 (9)
C30.0295 (17)0.0261 (17)0.0422 (17)0.0069 (14)0.0008 (14)0.0128 (14)
C40.0345 (19)0.0233 (17)0.0572 (19)0.0027 (15)0.0126 (16)0.0094 (15)
C50.0431 (19)0.0220 (16)0.0334 (15)0.0125 (14)0.0099 (14)0.0021 (13)
C60.0339 (17)0.0228 (15)0.0303 (14)0.0161 (14)0.0042 (13)0.0016 (12)
C70.0351 (18)0.0240 (16)0.0334 (16)0.0090 (14)0.0119 (14)0.0001 (13)
C80.0182 (14)0.0174 (15)0.0279 (14)0.0035 (12)0.0001 (11)0.0046 (11)
C90.0433 (19)0.0416 (19)0.0338 (16)0.0256 (16)0.0045 (15)0.0029 (14)
C100.049 (2)0.0316 (17)0.0431 (17)0.0258 (16)0.0092 (15)0.0035 (14)
C110.0248 (15)0.0228 (15)0.0207 (13)0.0148 (12)0.0042 (11)0.0044 (11)
C120.0259 (16)0.0220 (15)0.0240 (13)0.0134 (13)0.0002 (12)0.0012 (12)
C130.0222 (15)0.0277 (16)0.0209 (13)0.0137 (13)0.0036 (11)0.0017 (12)
C140.0268 (16)0.0201 (15)0.0244 (14)0.0119 (13)0.0004 (12)0.0020 (11)
C150.0250 (15)0.0186 (14)0.0242 (13)0.0092 (12)0.0013 (11)0.0029 (11)
C160.0229 (16)0.0211 (15)0.0317 (14)0.0077 (13)0.0016 (12)0.0009 (12)
C170.0216 (15)0.0295 (17)0.0343 (15)0.0124 (13)0.0008 (13)0.0027 (13)
C180.0230 (15)0.0201 (14)0.0280 (14)0.0101 (12)0.0021 (11)0.0026 (11)
C190.0232 (15)0.0206 (13)0.0212 (13)0.0099 (13)0.0012 (11)0.0028 (11)
C200.0263 (16)0.0254 (15)0.0248 (13)0.0120 (13)0.0034 (12)0.0000 (12)
C210.0239 (16)0.0265 (16)0.0251 (13)0.0157 (13)0.0013 (11)0.0006 (12)
C220.0316 (17)0.0285 (16)0.0348 (15)0.0178 (14)0.0046 (13)0.0058 (13)
C230.0392 (17)0.0277 (16)0.0294 (15)0.0235 (14)0.0038 (13)0.0065 (12)
C240.0328 (16)0.0275 (17)0.0355 (15)0.0173 (14)0.0033 (13)0.0037 (13)
O310.061 (4)0.053 (3)0.048 (3)0.014 (3)0.001 (3)0.007 (3)
C320.051 (6)0.158 (14)0.066 (11)0.043 (7)0.008 (5)0.040 (11)
C330.076 (11)0.163 (17)0.062 (10)0.096 (12)0.012 (8)0.025 (9)
C340.074 (9)0.051 (7)0.028 (12)0.032 (3)0.010 (6)0.006 (5)
C350.045 (6)0.080 (10)0.027 (5)0.022 (6)0.018 (5)0.005 (6)
Geometric parameters (Å, º) top
O1—S11.4354 (17)C13—C211.454 (3)
S1—O21.4313 (18)C13—C141.517 (3)
S1—N11.6944 (18)C14—C151.525 (3)
S1—C11.782 (2)C14—C191.567 (3)
N1—C111.402 (3)C14—H14A1.0000
N1—C81.487 (3)C15—C161.537 (3)
C1—C21.513 (3)C15—C201.548 (3)
C1—H1A0.9900C15—H15A1.0000
C1—H1B0.9900C16—C171.563 (3)
S2—C221.702 (2)C16—H16A0.9900
S2—C231.710 (3)C16—H16B0.9900
C2—C31.542 (3)C17—C181.541 (3)
C2—C81.546 (3)C17—H17A0.9900
C2—C61.560 (3)C17—H17B0.9900
O3—C111.232 (3)C18—C191.535 (3)
C3—C41.546 (4)C18—C201.537 (3)
C3—H3A0.9900C18—H18A1.0000
C3—H3B0.9900C19—H19A1.0000
C4—C51.531 (4)C20—H20A0.9900
C4—H4A0.9900C20—H20B0.9900
C4—H4B0.9900C21—C221.374 (4)
C5—C71.533 (3)C21—C241.431 (3)
C5—C61.545 (4)C22—H22A0.9500
C5—H5A1.0000C23—C241.367 (4)
C6—C101.531 (4)C23—H23A0.9500
C6—C91.534 (3)C24—H24A0.9500
C7—C81.543 (3)O31—C351.422 (12)
C7—H7A0.9900O31—C321.431 (12)
C7—H7B0.9900C32—C331.489 (14)
C8—H8A1.0000C32—H32A0.9900
C9—H9A0.9800C32—H32B0.9900
C9—H9B0.9800C33—C341.504 (11)
C9—H9C0.9800C33—H33A0.9900
C10—H10A0.9800C33—H33B0.9900
C10—H10B0.9800C34—C351.502 (12)
C10—H10C0.9800C34—H34A0.9900
C11—C121.466 (4)C34—H34B0.9900
C12—C131.365 (3)C35—H35A0.9900
C12—C191.524 (3)C35—H35B0.9900
O2—S1—O1117.80 (11)C13—C14—C15118.3 (2)
O2—S1—N1110.72 (10)C13—C14—C1986.51 (19)
O1—S1—N1108.45 (10)C15—C14—C19104.01 (19)
O2—S1—C1110.29 (11)C13—C14—H14A114.7
O1—S1—C1111.15 (11)C15—C14—H14A114.7
N1—S1—C196.30 (11)C19—C14—H14A114.7
C11—N1—C8116.10 (18)C14—C15—C16106.25 (19)
C11—N1—S1123.68 (16)C14—C15—C20101.5 (2)
C8—N1—S1111.38 (14)C16—C15—C20101.7 (2)
C2—C1—S1107.33 (16)C14—C15—H15A115.2
C2—C1—H1A110.2C16—C15—H15A115.2
S1—C1—H1A110.2C20—C15—H15A115.2
C2—C1—H1B110.2C15—C16—C17103.43 (19)
S1—C1—H1B110.2C15—C16—H16A111.1
H1A—C1—H1B108.5C17—C16—H16A111.1
C22—S2—C2392.56 (14)C15—C16—H16B111.1
C1—C2—C3116.88 (19)C17—C16—H16B111.1
C1—C2—C8108.33 (19)H16A—C16—H16B109.0
C3—C2—C8104.6 (2)C18—C17—C16103.1 (2)
C1—C2—C6119.6 (2)C18—C17—H17A111.2
C3—C2—C6101.7 (2)C16—C17—H17A111.2
C8—C2—C6104.09 (19)C18—C17—H17B111.2
C2—C3—C4101.6 (2)C16—C17—H17B111.2
C2—C3—H3A111.5H17A—C17—H17B109.1
C4—C3—H3A111.5C19—C18—C20103.7 (2)
C2—C3—H3B111.5C19—C18—C17105.5 (2)
C4—C3—H3B111.5C20—C18—C17101.2 (2)
H3A—C3—H3B109.3C19—C18—H18A115.0
C5—C4—C3104.4 (2)C20—C18—H18A115.0
C5—C4—H4A110.9C17—C18—H18A115.0
C3—C4—H4A110.9C12—C19—C18116.75 (19)
C5—C4—H4B110.9C12—C19—C1485.83 (18)
C3—C4—H4B110.9C18—C19—C14102.42 (18)
H4A—C4—H4B108.9C12—C19—H19A115.7
C4—C5—C7107.7 (2)C18—C19—H19A115.7
C4—C5—C6102.6 (2)C14—C19—H19A115.7
C7—C5—C6102.7 (2)C18—C20—C1594.70 (18)
C4—C5—H5A114.2C18—C20—H20A112.8
C7—C5—H5A114.2C15—C20—H20A112.8
C6—C5—H5A114.2C18—C20—H20B112.8
C10—C6—C9106.6 (2)C15—C20—H20B112.8
C10—C6—C5114.0 (2)H20A—C20—H20B110.2
C9—C6—C5114.3 (2)C22—C21—C24110.9 (2)
C10—C6—C2113.5 (2)C22—C21—C13128.0 (2)
C9—C6—C2116.1 (2)C24—C21—C13121.1 (2)
C5—C6—C292.3 (2)C21—C22—S2112.2 (2)
C5—C7—C8101.8 (2)C21—C22—H22A123.9
C5—C7—H7A111.4S2—C22—H22A123.9
C8—C7—H7A111.4C24—C23—S2110.8 (2)
C5—C7—H7B111.4C24—C23—H23A124.6
C8—C7—H7B111.4S2—C23—H23A124.6
H7A—C7—H7B109.3C23—C24—C21113.5 (3)
N1—C8—C7115.79 (19)C23—C24—H24A123.3
N1—C8—C2107.22 (18)C21—C24—H24A123.3
C7—C8—C2103.9 (2)C35—O31—C32101.7 (10)
N1—C8—H8A109.9O31—C32—C33109.1 (10)
C7—C8—H8A109.9O31—C32—H32A109.9
C2—C8—H8A109.9C33—C32—H32A109.9
C6—C9—H9A109.5O31—C32—H32B109.9
C6—C9—H9B109.5C33—C32—H32B109.9
H9A—C9—H9B109.5H32A—C32—H32B108.3
C6—C9—H9C109.5C32—C33—C34103.4 (9)
H9A—C9—H9C109.5C32—C33—H33A111.1
H9B—C9—H9C109.5C34—C33—H33A111.1
C6—C10—H10A109.5C32—C33—H33B111.1
C6—C10—H10B109.5C34—C33—H33B111.1
H10A—C10—H10B109.5H33A—C33—H33B109.1
C6—C10—H10C109.5C35—C34—C33103.8 (6)
H10A—C10—H10C109.5C35—C34—H34A111.0
H10B—C10—H10C109.5C33—C34—H34A111.0
O3—C11—N1118.1 (2)C35—C34—H34B111.0
O3—C11—C12122.3 (2)C33—C34—H34B111.0
N1—C11—C12119.5 (2)H34A—C34—H34B109.0
C13—C12—C11130.4 (2)O31—C35—C34107.0 (9)
C13—C12—C1993.9 (2)O31—C35—H35A110.3
C11—C12—C19135.5 (2)C34—C35—H35A110.3
C12—C13—C21139.1 (3)O31—C35—H35B110.3
C12—C13—C1493.7 (2)C34—C35—H35B110.3
C21—C13—C14127.0 (2)H35A—C35—H35B108.6
O2—S1—N1—C1188.8 (2)N1—C11—C12—C13178.4 (2)
O1—S1—N1—C1141.9 (2)O3—C11—C12—C19169.1 (2)
C1—S1—N1—C11156.72 (19)N1—C11—C12—C197.9 (4)
O2—S1—N1—C8125.26 (16)C11—C12—C13—C212.5 (5)
O1—S1—N1—C8104.06 (17)C19—C12—C13—C21173.2 (3)
C1—S1—N1—C810.75 (18)C11—C12—C13—C14177.7 (3)
O2—S1—C1—C2106.05 (18)C19—C12—C13—C142.10 (19)
O1—S1—C1—C2121.40 (18)C12—C13—C14—C15106.1 (2)
N1—S1—C1—C28.80 (19)C21—C13—C14—C1570.0 (3)
S1—C1—C2—C3142.6 (2)C12—C13—C14—C192.04 (19)
S1—C1—C2—C824.9 (2)C21—C13—C14—C19174.1 (2)
S1—C1—C2—C694.0 (2)C13—C14—C15—C16162.6 (2)
C1—C2—C3—C4171.7 (2)C19—C14—C15—C1669.0 (2)
C8—C2—C3—C468.6 (2)C13—C14—C15—C2056.6 (3)
C6—C2—C3—C439.5 (2)C19—C14—C15—C2037.0 (2)
C2—C3—C4—C54.3 (3)C14—C15—C16—C1772.8 (2)
C3—C4—C5—C775.2 (3)C20—C15—C16—C1733.0 (2)
C3—C4—C5—C632.7 (3)C15—C16—C17—C182.2 (2)
C4—C5—C6—C1062.5 (3)C16—C17—C18—C1970.7 (2)
C7—C5—C6—C10174.1 (2)C16—C17—C18—C2037.0 (2)
C4—C5—C6—C9174.6 (2)C13—C12—C19—C1899.8 (2)
C7—C5—C6—C962.9 (3)C11—C12—C19—C1875.4 (3)
C4—C5—C6—C254.5 (2)C13—C12—C19—C142.04 (19)
C7—C5—C6—C257.1 (2)C11—C12—C19—C14177.3 (3)
C1—C2—C6—C1070.6 (3)C20—C18—C19—C1260.2 (3)
C3—C2—C6—C1059.8 (3)C17—C18—C19—C12166.12 (19)
C8—C2—C6—C10168.3 (2)C20—C18—C19—C1431.4 (2)
C1—C2—C6—C953.4 (3)C17—C18—C19—C1474.5 (2)
C3—C2—C6—C9176.2 (2)C13—C14—C19—C121.83 (17)
C8—C2—C6—C967.7 (3)C15—C14—C19—C12120.17 (19)
C1—C2—C6—C5171.9 (2)C13—C14—C19—C18114.66 (19)
C3—C2—C6—C557.6 (2)C15—C14—C19—C183.7 (2)
C8—C2—C6—C550.8 (2)C19—C18—C20—C1553.0 (2)
C4—C5—C7—C865.1 (3)C17—C18—C20—C1556.2 (2)
C6—C5—C7—C842.8 (3)C14—C15—C20—C1854.6 (2)
C11—N1—C8—C769.3 (3)C16—C15—C20—C1854.9 (2)
S1—N1—C8—C7141.92 (19)C12—C13—C21—C222.8 (5)
C11—N1—C8—C2175.32 (19)C14—C13—C21—C22176.9 (2)
S1—N1—C8—C226.6 (2)C12—C13—C21—C24176.8 (3)
C5—C7—C8—N1126.1 (2)C14—C13—C21—C242.8 (4)
C5—C7—C8—C28.8 (3)C24—C21—C22—S20.1 (3)
C1—C2—C8—N132.7 (3)C13—C21—C22—S2179.8 (2)
C3—C2—C8—N1158.00 (19)C23—S2—C22—C210.3 (2)
C6—C2—C8—N195.7 (2)C22—S2—C23—C240.5 (2)
C1—C2—C8—C7155.7 (2)S2—C23—C24—C210.5 (3)
C3—C2—C8—C778.9 (2)C22—C21—C24—C230.3 (3)
C6—C2—C8—C727.4 (3)C13—C21—C24—C23179.4 (2)
C8—N1—C11—O33.1 (3)C35—O31—C32—C3335.6 (13)
S1—N1—C11—O3147.63 (18)O31—C32—C33—C3418 (2)
C8—N1—C11—C12179.8 (2)C32—C33—C34—C356 (3)
S1—N1—C11—C1235.3 (3)C32—O31—C35—C3438.8 (19)
O3—C11—C12—C134.7 (4)C33—C34—C35—O3128 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C8—H8A···O2i1.02.593.516 (3)154
C1—H1B···O3ii0.992.453.422 (3)168
C14—H14A···O1iii1.002.663.500 (3)141
C1—H1A···O310.992.363.235 (14)147
Symmetry codes: (i) xy, y+1, z+1/3; (ii) xy+1, y+1, z+1/3; (iii) xy+1, y+2, z+1/3.
(VII) (7S)-N-[4-(4-tolyl)tricyclo[4.2.1.02,5]non-3-ene-3-carbonyl]- 2,10-camphorsultam top
Crystal data top
C27H33NO3SDx = 1.266 Mg m3
Mr = 451.60Melting point: 186 K
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 43635 reflections
a = 11.687 (2) Åθ = 1.7–27.5°
b = 12.849 (3) ŵ = 0.17 mm1
c = 31.547 (6) ÅT = 150 K
V = 4737.2 (16) Å3Block, colourless
Z = 80.40 × 0.35 × 0.17 mm
F(000) = 1936
Data collection top
Nonius KappaCCD
diffractometer
9673 independent reflections
Radiation source: fine-focus sealed tube7676 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.068
ϕ scans, and ω scans with κ offsetsθmax = 26.4°, θmin = 2.6°
Absorption correction: multi-scan
(DENZO–SMN; Otwinowski & Minor, 1997)
h = 1414
Tmin = 0.937, Tmax = 0.972k = 1616
44242 measured reflectionsl = 3939
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.041H-atom parameters constrained
wR(F2) = 0.096 w = 1/[σ2(Fo2) + (0.052P)2 + 0.1513P]
where P = (Fo2 + 2Fc2)/3
S = 1.03(Δ/σ)max = 0.001
9673 reflectionsΔρmax = 0.19 e Å3
583 parametersΔρmin = 0.31 e Å3
0 restraintsAbsolute structure: Flack (1983), 4291 Friedel pairs
Primary atom site location: structure-invariant direct methodsAbsolute structure parameter: 0.02 (5)
Crystal data top
C27H33NO3SV = 4737.2 (16) Å3
Mr = 451.60Z = 8
Orthorhombic, P212121Mo Kα radiation
a = 11.687 (2) ŵ = 0.17 mm1
b = 12.849 (3) ÅT = 150 K
c = 31.547 (6) Å0.40 × 0.35 × 0.17 mm
Data collection top
Nonius KappaCCD
diffractometer
9673 independent reflections
Absorption correction: multi-scan
(DENZO–SMN; Otwinowski & Minor, 1997)
7676 reflections with I > 2σ(I)
Tmin = 0.937, Tmax = 0.972Rint = 0.068
44242 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.041H-atom parameters constrained
wR(F2) = 0.096Δρmax = 0.19 e Å3
S = 1.03Δρmin = 0.31 e Å3
9673 reflectionsAbsolute structure: Flack (1983), 4291 Friedel pairs
583 parametersAbsolute structure parameter: 0.02 (5)
0 restraints
Special details top

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 F^2^ against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F^2^, conventional R-factors R are based on F, with F set to zero for negative F^2^. The threshold expression of F^2^ > σ(F^2^) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F^2^ are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger.

To verify the positions of the C27 methyl hydrogen atoms, they were refined to reliable, stable positions with Uavg = 0.0478.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
O10.81519 (13)0.82842 (12)0.87280 (5)0.0391 (4)
S10.70189 (5)0.78856 (4)0.868799 (17)0.02823 (13)
C10.70490 (19)0.65036 (16)0.86702 (7)0.0305 (5)
H1A0.65200.62440.84490.037*
H1B0.78310.62560.86040.037*
N10.63077 (14)0.79703 (13)0.91532 (5)0.0228 (4)
O20.63070 (14)0.83102 (13)0.83626 (5)0.0404 (4)
C20.66810 (18)0.61133 (17)0.91030 (7)0.0264 (5)
C30.6002 (2)0.50883 (17)0.91136 (8)0.0341 (6)
H3A0.64130.45260.89620.041*
H3B0.52320.51750.89880.041*
O30.47143 (12)0.86942 (11)0.94353 (5)0.0292 (4)
C40.5927 (2)0.48613 (19)0.95972 (8)0.0401 (6)
H4A0.51240.48840.96970.048*
H4B0.62570.41710.96650.048*
C50.6638 (2)0.57418 (17)0.97980 (8)0.0358 (6)
H5A0.69310.55801.00880.043*
C60.7588 (2)0.59377 (17)0.94655 (7)0.0320 (5)
C70.5918 (2)0.67435 (18)0.97728 (7)0.0329 (5)
H7A0.62950.73260.99240.040*
H7B0.51440.66370.98920.040*
C80.58690 (18)0.69448 (16)0.92906 (6)0.0262 (5)
H8A0.50730.68380.91830.031*
C90.8369 (2)0.68475 (19)0.95728 (8)0.0401 (6)
H9A0.87950.66910.98330.060*
H9B0.79080.74760.96160.060*
H9C0.89080.69620.93390.060*
C100.8372 (2)0.49984 (19)0.93830 (9)0.0431 (6)
H10A0.88340.51280.91290.065*
H10B0.79040.43740.93400.065*
H10C0.88770.48940.96270.065*
C110.56299 (18)0.88439 (16)0.92545 (6)0.0236 (5)
C120.61030 (17)0.98763 (16)0.91705 (6)0.0232 (5)
C130.56549 (18)1.08492 (16)0.92125 (6)0.0243 (5)
C140.68049 (17)1.13723 (16)0.91663 (6)0.0245 (5)
H14A0.68791.18650.89220.029*
C150.73742 (18)1.17224 (17)0.95815 (7)0.0286 (5)
H15A0.69481.22730.97400.034*
C160.86076 (18)1.20032 (19)0.94685 (8)0.0367 (6)
H16A0.90011.23420.97100.044*
H16B0.86381.24700.92190.044*
C170.91466 (18)1.09233 (18)0.93672 (8)0.0353 (6)
H17A0.93861.08820.90670.042*
H17B0.98181.07870.95500.042*
C180.81748 (18)1.01510 (18)0.94609 (7)0.0294 (5)
H18A0.84260.94220.95220.035*
C190.73200 (17)1.02632 (16)0.90952 (7)0.0250 (5)
H19A0.76361.01290.88060.030*
C200.7550 (2)1.07006 (17)0.98262 (7)0.0313 (5)
H20A0.80351.07871.00810.038*
H20B0.68201.03580.99030.038*
C210.45561 (17)1.13654 (16)0.92709 (6)0.0223 (5)
C220.35456 (18)1.08700 (17)0.93909 (7)0.0275 (5)
H22A0.35561.01480.94560.033*
C230.25308 (18)1.14160 (16)0.94155 (7)0.0272 (5)
H23A0.18561.10620.95010.033*
C240.24691 (18)1.24753 (17)0.93178 (6)0.0252 (5)
C250.34828 (17)1.29767 (17)0.92094 (6)0.0267 (5)
H25A0.34721.37010.91490.032*
C260.45045 (18)1.24384 (16)0.91889 (6)0.0269 (5)
H26A0.51861.28020.91180.032*
C270.13450 (17)1.30333 (18)0.93233 (7)0.0304 (5)
H27A0.14691.37730.92640.046*
H27B0.09901.29560.96030.046*
H27C0.08411.27360.91070.046*
O310.34129 (15)0.59886 (15)0.86620 (7)0.0638 (6)
S310.23370 (6)0.62631 (5)0.88508 (2)0.04078 (17)
C310.2371 (2)0.75909 (18)0.90151 (7)0.0337 (5)
H31A0.19790.76750.92910.040*
H31B0.31720.78330.90450.040*
N310.13308 (15)0.64214 (14)0.84736 (5)0.0265 (4)
O320.1911 (2)0.56063 (14)0.91745 (6)0.0692 (7)
C320.17624 (18)0.82052 (16)0.86750 (6)0.0269 (5)
C330.1095 (2)0.91680 (18)0.88247 (8)0.0366 (6)
H33A0.04140.89670.89930.044*
H33B0.15840.96340.89970.044*
O330.04204 (13)0.58735 (12)0.82572 (5)0.0352 (4)
C340.0750 (2)0.9685 (2)0.84054 (9)0.0456 (7)
H34A0.00930.96970.83730.055*
H34B0.10441.04070.83890.055*
C350.1307 (2)0.8996 (2)0.80669 (8)0.0407 (6)
H35A0.14180.93500.77880.049*
C360.2439 (2)0.86511 (18)0.82844 (7)0.0325 (5)
C370.0622 (2)0.79756 (18)0.80405 (7)0.0376 (6)
H37A0.02040.81110.79980.045*
H37B0.09060.75240.78090.045*
C380.08545 (18)0.74915 (17)0.84772 (7)0.0272 (5)
H38A0.01410.75090.86520.033*
C390.3137 (2)0.7869 (2)0.80242 (8)0.0444 (6)
H39A0.33530.81840.77530.067*
H39B0.26760.72450.79720.067*
H39C0.38290.76770.81810.067*
C400.3246 (2)0.9547 (2)0.83956 (9)0.0447 (7)
H40A0.38520.92930.85840.067*
H40B0.28151.00990.85390.067*
H40C0.35890.98240.81350.067*
C410.0557 (2)0.56291 (17)0.83499 (7)0.0266 (5)
C420.10053 (18)0.45719 (17)0.83037 (7)0.0256 (5)
C430.04976 (18)0.36382 (17)0.82181 (6)0.0258 (5)
C440.16350 (17)0.30849 (17)0.81514 (7)0.0272 (5)
H44A0.18090.25180.83590.033*
C450.20066 (18)0.28688 (17)0.76923 (7)0.0306 (5)
H45A0.15250.23520.75360.037*
C460.32879 (18)0.26056 (19)0.77134 (8)0.0381 (6)
H46A0.35610.23120.74420.046*
H46B0.34490.21040.79440.046*
C470.3854 (2)0.3682 (2)0.78050 (9)0.0430 (6)
H47A0.42870.36670.80750.052*
H47B0.43770.38860.75730.052*
C480.28339 (19)0.44268 (18)0.78337 (7)0.0315 (5)
H48A0.30240.51790.77940.038*
C490.22163 (18)0.41645 (17)0.82486 (7)0.0286 (5)
H49A0.27040.41840.85090.034*
C500.2030 (2)0.39671 (18)0.74987 (7)0.0331 (5)
H50A0.23640.39790.72100.040*
H50B0.12680.43030.74980.040*
C510.06397 (19)0.31822 (17)0.81778 (6)0.0263 (5)
C520.16743 (18)0.37249 (18)0.82097 (7)0.0308 (5)
H52A0.16650.44530.82610.037*
C530.27067 (19)0.32178 (18)0.81681 (7)0.0331 (5)
H53A0.33950.36060.81910.040*
C540.27698 (18)0.21476 (18)0.80924 (6)0.0294 (5)
C550.17470 (19)0.16141 (18)0.80577 (7)0.0311 (5)
H55A0.17600.08870.80040.037*
C560.07091 (19)0.21139 (17)0.80990 (7)0.0299 (5)
H56A0.00230.17220.80730.036*
C570.3900 (2)0.1602 (2)0.80431 (8)0.0407 (6)
H57A0.41800.16960.77530.061*
H57B0.44530.18980.82430.061*
H57C0.38030.08590.81010.061*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0289 (8)0.0299 (9)0.0586 (11)0.0047 (7)0.0163 (8)0.0051 (8)
S10.0301 (3)0.0258 (3)0.0287 (3)0.0023 (2)0.0071 (2)0.0004 (2)
C10.0336 (12)0.0285 (12)0.0294 (11)0.0011 (10)0.0041 (10)0.0037 (10)
N10.0233 (9)0.0186 (9)0.0266 (9)0.0012 (8)0.0026 (7)0.0015 (7)
O20.0521 (10)0.0441 (10)0.0251 (8)0.0144 (9)0.0014 (7)0.0071 (7)
C20.0277 (11)0.0225 (11)0.0290 (11)0.0023 (9)0.0008 (9)0.0024 (9)
C30.0341 (13)0.0242 (12)0.0439 (15)0.0002 (11)0.0007 (11)0.0054 (11)
O30.0263 (8)0.0240 (8)0.0373 (9)0.0007 (7)0.0088 (7)0.0008 (7)
C40.0499 (16)0.0267 (13)0.0437 (15)0.0008 (12)0.0022 (12)0.0065 (11)
C50.0468 (15)0.0252 (12)0.0354 (13)0.0033 (11)0.0043 (11)0.0055 (10)
C60.0350 (13)0.0270 (12)0.0341 (12)0.0045 (11)0.0061 (10)0.0020 (10)
C70.0436 (14)0.0252 (12)0.0300 (12)0.0026 (11)0.0071 (10)0.0028 (9)
C80.0267 (12)0.0207 (12)0.0311 (12)0.0002 (9)0.0021 (9)0.0002 (9)
C90.0386 (14)0.0371 (15)0.0444 (14)0.0009 (12)0.0143 (11)0.0032 (11)
C100.0407 (14)0.0337 (14)0.0548 (16)0.0135 (12)0.0066 (13)0.0024 (12)
C110.0226 (11)0.0254 (12)0.0228 (11)0.0011 (10)0.0005 (9)0.0011 (9)
C120.0233 (11)0.0223 (12)0.0239 (11)0.0042 (9)0.0018 (9)0.0003 (9)
C130.0242 (11)0.0255 (11)0.0233 (11)0.0010 (10)0.0001 (9)0.0024 (9)
C140.0265 (11)0.0203 (11)0.0267 (11)0.0007 (9)0.0046 (9)0.0012 (9)
C150.0253 (12)0.0249 (12)0.0358 (12)0.0006 (10)0.0021 (10)0.0063 (9)
C160.0274 (12)0.0300 (14)0.0525 (15)0.0057 (11)0.0007 (11)0.0027 (11)
C170.0228 (12)0.0329 (14)0.0502 (15)0.0023 (11)0.0001 (11)0.0011 (11)
C180.0249 (12)0.0260 (12)0.0374 (13)0.0012 (10)0.0013 (10)0.0002 (10)
C190.0247 (11)0.0214 (11)0.0289 (11)0.0019 (9)0.0043 (9)0.0004 (9)
C200.0314 (12)0.0328 (13)0.0295 (12)0.0020 (11)0.0036 (10)0.0043 (10)
C210.0220 (11)0.0228 (11)0.0222 (11)0.0016 (9)0.0019 (8)0.0004 (9)
C220.0279 (12)0.0201 (11)0.0343 (12)0.0017 (10)0.0042 (10)0.0001 (9)
C230.0243 (11)0.0239 (12)0.0334 (12)0.0040 (10)0.0050 (9)0.0005 (9)
C240.0256 (11)0.0256 (11)0.0246 (11)0.0014 (10)0.0034 (9)0.0006 (9)
C250.0286 (12)0.0194 (11)0.0322 (12)0.0011 (10)0.0028 (9)0.0026 (10)
C260.0275 (12)0.0242 (11)0.0290 (11)0.0036 (10)0.0001 (10)0.0024 (9)
C270.0262 (11)0.0282 (13)0.0367 (12)0.0022 (10)0.0015 (9)0.0006 (10)
O310.0364 (10)0.0484 (12)0.1067 (17)0.0185 (9)0.0333 (11)0.0334 (11)
S310.0509 (4)0.0242 (3)0.0473 (4)0.0014 (3)0.0262 (3)0.0016 (3)
C310.0390 (13)0.0290 (13)0.0331 (12)0.0010 (11)0.0095 (11)0.0028 (10)
N310.0276 (10)0.0218 (10)0.0302 (10)0.0020 (8)0.0061 (8)0.0035 (8)
O320.1203 (18)0.0377 (11)0.0497 (12)0.0267 (12)0.0399 (12)0.0164 (9)
C320.0290 (11)0.0254 (11)0.0263 (11)0.0019 (9)0.0055 (10)0.0027 (9)
C330.0378 (13)0.0279 (13)0.0442 (14)0.0027 (11)0.0023 (11)0.0083 (11)
O330.0241 (9)0.0283 (9)0.0530 (10)0.0034 (7)0.0067 (7)0.0076 (8)
C340.0451 (16)0.0261 (14)0.0655 (19)0.0037 (12)0.0179 (14)0.0020 (12)
C350.0491 (15)0.0366 (15)0.0366 (14)0.0011 (13)0.0129 (12)0.0083 (11)
C360.0367 (13)0.0313 (13)0.0296 (12)0.0031 (11)0.0018 (10)0.0014 (10)
C370.0416 (13)0.0319 (14)0.0391 (13)0.0018 (12)0.0153 (11)0.0014 (11)
C380.0256 (12)0.0241 (12)0.0319 (12)0.0037 (9)0.0007 (10)0.0053 (9)
C390.0442 (15)0.0507 (17)0.0384 (14)0.0015 (14)0.0081 (12)0.0072 (12)
C400.0434 (15)0.0394 (15)0.0513 (16)0.0125 (13)0.0004 (13)0.0061 (12)
C410.0268 (12)0.0261 (12)0.0269 (11)0.0000 (10)0.0011 (10)0.0026 (9)
C420.0268 (12)0.0241 (12)0.0258 (11)0.0030 (10)0.0018 (9)0.0031 (9)
C430.0296 (12)0.0258 (12)0.0219 (11)0.0025 (10)0.0008 (9)0.0003 (9)
C440.0287 (12)0.0243 (12)0.0287 (11)0.0024 (10)0.0043 (9)0.0008 (9)
C450.0319 (12)0.0245 (12)0.0354 (12)0.0052 (11)0.0031 (10)0.0069 (10)
C460.0341 (13)0.0343 (14)0.0458 (14)0.0075 (11)0.0046 (11)0.0072 (11)
C470.0271 (13)0.0420 (16)0.0600 (17)0.0027 (12)0.0037 (12)0.0097 (13)
C480.0269 (12)0.0270 (13)0.0407 (13)0.0009 (10)0.0043 (10)0.0027 (10)
C490.0294 (12)0.0265 (12)0.0298 (12)0.0046 (10)0.0062 (10)0.0030 (9)
C500.0355 (13)0.0353 (14)0.0285 (12)0.0033 (11)0.0038 (10)0.0032 (10)
C510.0302 (12)0.0260 (12)0.0226 (11)0.0015 (10)0.0014 (9)0.0005 (9)
C520.0317 (12)0.0283 (12)0.0325 (12)0.0023 (11)0.0010 (10)0.0042 (10)
C530.0273 (12)0.0354 (14)0.0367 (13)0.0003 (11)0.0016 (10)0.0039 (10)
C540.0309 (12)0.0335 (13)0.0237 (11)0.0047 (11)0.0022 (9)0.0015 (10)
C550.0369 (14)0.0238 (12)0.0326 (12)0.0012 (11)0.0001 (10)0.0008 (9)
C560.0283 (11)0.0277 (12)0.0338 (12)0.0033 (11)0.0000 (10)0.0024 (10)
C570.0354 (13)0.0442 (16)0.0426 (14)0.0056 (12)0.0019 (11)0.0037 (12)
Geometric parameters (Å, º) top
O1—S11.4253 (16)O31—S311.435 (2)
S1—O21.4296 (16)S31—O321.415 (2)
S1—N11.6902 (17)S31—N311.6852 (18)
S1—C11.777 (2)S31—C311.784 (2)
C1—C21.517 (3)C31—C321.510 (3)
C1—H1A0.9900C31—H31A0.9900
C1—H1B0.9900C31—H31B0.9900
N1—C111.410 (3)N31—C411.417 (3)
N1—C81.479 (3)N31—C381.483 (3)
C2—C31.538 (3)C32—C381.535 (3)
C2—C81.547 (3)C32—C331.537 (3)
C2—C61.575 (3)C32—C361.572 (3)
C3—C41.556 (3)C33—C341.534 (4)
C3—H3A0.9900C33—H33A0.9900
C3—H3B0.9900C33—H33B0.9900
O3—C111.228 (2)O33—C411.220 (3)
C4—C51.540 (3)C34—C351.532 (4)
C4—H4A0.9900C34—H34A0.9900
C4—H4B0.9900C34—H34B0.9900
C5—C71.539 (3)C35—C371.539 (3)
C5—C61.548 (3)C35—C361.555 (3)
C5—H5A1.0000C35—H35A1.0000
C6—C91.522 (3)C36—C401.529 (3)
C6—C101.538 (3)C36—C391.533 (3)
C7—C81.544 (3)C37—C381.536 (3)
C7—H7A0.9900C37—H37A0.9900
C7—H7B0.9900C37—H37B0.9900
C8—H8A1.0000C38—H38A1.0000
C9—H9A0.9800C39—H39A0.9800
C9—H9B0.9800C39—H39B0.9800
C9—H9C0.9800C39—H39C0.9800
C10—H10A0.9800C40—H40A0.9800
C10—H10B0.9800C40—H40B0.9800
C10—H10C0.9800C40—H40C0.9800
C11—C121.461 (3)C41—C421.463 (3)
C12—C131.362 (3)C42—C431.365 (3)
C12—C191.525 (3)C42—C491.519 (3)
C13—C211.457 (3)C43—C511.458 (3)
C13—C141.510 (3)C43—C441.522 (3)
C14—C151.536 (3)C44—C451.537 (3)
C14—C191.563 (3)C44—C491.575 (3)
C14—H14A1.0000C44—H44A1.0000
C15—C161.528 (3)C45—C461.537 (3)
C15—C201.537 (3)C45—C501.538 (3)
C15—H15A1.0000C45—H45A1.0000
C16—C171.557 (3)C46—C471.560 (3)
C16—H16A0.9900C46—H46A0.9900
C16—H16B0.9900C46—H46B0.9900
C17—C181.537 (3)C47—C481.532 (3)
C17—H17A0.9900C47—H47A0.9900
C17—H17B0.9900C47—H47B0.9900
C18—C191.533 (3)C48—C491.532 (3)
C18—C201.536 (3)C48—C501.532 (3)
C18—H18A1.0000C48—H48A1.0000
C19—H19A1.0000C49—H49A1.0000
C20—H20A0.9900C50—H50A0.9900
C20—H20B0.9900C50—H50B0.9900
C21—C221.394 (3)C51—C561.397 (3)
C21—C261.404 (3)C51—C521.399 (3)
C22—C231.380 (3)C52—C531.378 (3)
C22—H22A0.9500C52—H52A0.9500
C23—C241.398 (3)C53—C541.398 (3)
C23—H23A0.9500C53—H53A0.9500
C24—C251.391 (3)C54—C551.382 (3)
C24—C271.497 (3)C54—C571.503 (3)
C25—C261.381 (3)C55—C561.379 (3)
C25—H25A0.9500C55—H55A0.9500
C26—H26A0.9500C56—H56A0.9500
C27—H27A0.9800C57—H57A0.9800
C27—H27B0.9800C57—H57B0.9800
C27—H27C0.9800C57—H57C0.9800
O1—S1—O2117.85 (11)O32—S31—O31117.47 (14)
O1—S1—N1110.90 (9)O32—S31—N31109.61 (11)
O2—S1—N1108.23 (9)O31—S31—N31110.36 (11)
O1—S1—C1110.09 (11)O32—S31—C31111.64 (12)
O2—S1—C1111.73 (11)O31—S31—C31109.63 (12)
N1—S1—C195.82 (9)N31—S31—C3196.06 (10)
C2—C1—S1107.24 (14)C32—C31—S31106.43 (15)
C2—C1—H1A110.3C32—C31—H31A110.4
S1—C1—H1A110.3S31—C31—H31A110.4
C2—C1—H1B110.3C32—C31—H31B110.4
S1—C1—H1B110.3S31—C31—H31B110.4
H1A—C1—H1B108.5H31A—C31—H31B108.6
C11—N1—C8116.61 (16)C41—N31—C38115.37 (17)
C11—N1—S1121.60 (14)C41—N31—S31123.60 (15)
C8—N1—S1111.56 (13)C38—N31—S31111.61 (13)
C1—C2—C3116.68 (18)C31—C32—C38107.59 (18)
C1—C2—C8106.85 (17)C31—C32—C33116.21 (18)
C3—C2—C8105.46 (17)C38—C32—C33104.78 (17)
C1—C2—C6120.67 (18)C31—C32—C36120.67 (19)
C3—C2—C6102.05 (17)C38—C32—C36104.29 (17)
C8—C2—C6103.53 (17)C33—C32—C36101.69 (18)
C2—C3—C4102.16 (18)C34—C33—C32102.55 (18)
C2—C3—H3A111.3C34—C33—H33A111.3
C4—C3—H3A111.3C32—C33—H33A111.3
C2—C3—H3B111.3C34—C33—H33B111.3
C4—C3—H3B111.3C32—C33—H33B111.3
H3A—C3—H3B109.2H33A—C33—H33B109.2
C5—C4—C3103.62 (19)C35—C34—C33103.82 (19)
C5—C4—H4A111.0C35—C34—H34A111.0
C3—C4—H4A111.0C33—C34—H34A111.0
C5—C4—H4B111.0C35—C34—H34B111.0
C3—C4—H4B111.0C33—C34—H34B111.0
H4A—C4—H4B109.0H34A—C34—H34B109.0
C7—C5—C4107.39 (19)C34—C35—C37108.0 (2)
C7—C5—C6102.76 (17)C34—C35—C36102.63 (19)
C4—C5—C6103.16 (19)C37—C35—C36102.91 (19)
C7—C5—H5A114.1C34—C35—H35A114.0
C4—C5—H5A114.1C37—C35—H35A114.0
C6—C5—H5A114.1C36—C35—H35A114.0
C9—C6—C10106.44 (19)C40—C36—C39106.8 (2)
C9—C6—C5113.88 (19)C40—C36—C35114.3 (2)
C10—C6—C5114.49 (19)C39—C36—C35113.8 (2)
C9—C6—C2117.08 (18)C40—C36—C32113.88 (18)
C10—C6—C2112.98 (19)C39—C36—C32116.6 (2)
C5—C6—C291.86 (17)C35—C36—C3291.24 (17)
C5—C7—C8102.19 (17)C38—C37—C35101.81 (17)
C5—C7—H7A111.3C38—C37—H37A111.4
C8—C7—H7A111.3C35—C37—H37A111.4
C5—C7—H7B111.3C38—C37—H37B111.4
C8—C7—H7B111.3C35—C37—H37B111.4
H7A—C7—H7B109.2H37A—C37—H37B109.3
N1—C8—C7115.15 (17)N31—C38—C32107.31 (16)
N1—C8—C2106.90 (16)N31—C38—C37115.78 (18)
C7—C8—C2103.78 (17)C32—C38—C37104.18 (18)
N1—C8—H8A110.2N31—C38—H38A109.8
C7—C8—H8A110.2C32—C38—H38A109.8
C2—C8—H8A110.2C37—C38—H38A109.8
C6—C9—H9A109.5C36—C39—H39A109.5
C6—C9—H9B109.5C36—C39—H39B109.5
H9A—C9—H9B109.5H39A—C39—H39B109.5
C6—C9—H9C109.5C36—C39—H39C109.5
H9A—C9—H9C109.5H39A—C39—H39C109.5
H9B—C9—H9C109.5H39B—C39—H39C109.5
C6—C10—H10A109.5C36—C40—H40A109.5
C6—C10—H10B109.5C36—C40—H40B109.5
H10A—C10—H10B109.5H40A—C40—H40B109.5
C6—C10—H10C109.5C36—C40—H40C109.5
H10A—C10—H10C109.5H40A—C40—H40C109.5
H10B—C10—H10C109.5H40B—C40—H40C109.5
O3—C11—N1118.04 (18)O33—C41—N31118.61 (19)
O3—C11—C12123.79 (19)O33—C41—C42123.4 (2)
N1—C11—C12117.96 (18)N31—C41—C42117.74 (19)
C13—C12—C11132.08 (19)C43—C42—C41132.8 (2)
C13—C12—C1994.27 (17)C43—C42—C4994.56 (17)
C11—C12—C19132.60 (18)C41—C42—C49131.7 (2)
C12—C13—C21140.3 (2)C42—C43—C51140.0 (2)
C12—C13—C1493.26 (16)C42—C43—C4493.34 (17)
C21—C13—C14126.45 (18)C51—C43—C44126.60 (19)
C13—C14—C15115.69 (17)C43—C44—C45117.48 (17)
C13—C14—C1987.19 (15)C43—C44—C4986.47 (16)
C15—C14—C19102.86 (16)C45—C44—C49102.75 (18)
C13—C14—H14A115.7C43—C44—H44A115.3
C15—C14—H14A115.7C45—C44—H44A115.3
C19—C14—H14A115.7C49—C44—H44A115.3
C16—C15—C14106.19 (18)C46—C45—C44105.91 (18)
C16—C15—C20101.13 (18)C46—C45—C50101.65 (19)
C14—C15—C20103.63 (17)C44—C45—C50102.32 (17)
C16—C15—H15A114.8C46—C45—H45A115.1
C14—C15—H15A114.8C44—C45—H45A115.1
C20—C15—H15A114.8C50—C45—H45A115.1
C15—C16—C17102.65 (18)C45—C46—C47103.09 (18)
C15—C16—H16A111.2C45—C46—H46A111.1
C17—C16—H16A111.2C47—C46—H46A111.1
C15—C16—H16B111.2C45—C46—H46B111.1
C17—C16—H16B111.2C47—C46—H46B111.1
H16A—C16—H16B109.1H46A—C46—H46B109.1
C18—C17—C16103.71 (18)C48—C47—C46103.56 (17)
C18—C17—H17A111.0C48—C47—H47A111.0
C16—C17—H17A111.0C46—C47—H47A111.0
C18—C17—H17B111.0C48—C47—H47B111.0
C16—C17—H17B111.0C46—C47—H47B111.0
H17A—C17—H17B109.0H47A—C47—H47B109.0
C19—C18—C20102.20 (17)C47—C48—C49106.24 (19)
C19—C18—C17106.04 (18)C47—C48—C50101.29 (18)
C20—C18—C17101.47 (18)C49—C48—C50102.45 (17)
C19—C18—H18A115.1C47—C48—H48A115.1
C20—C18—H18A115.1C49—C48—H48A115.1
C17—C18—H18A115.1C50—C48—H48A115.1
C12—C19—C18117.38 (17)C42—C49—C48117.44 (18)
C12—C19—C1485.16 (15)C42—C49—C4485.63 (16)
C18—C19—C14103.22 (17)C48—C49—C44103.33 (17)
C12—C19—H19A115.5C42—C49—H49A115.3
C18—C19—H19A115.5C48—C49—H49A115.3
C14—C19—H19A115.5C44—C49—H49A115.3
C18—C20—C1594.56 (17)C48—C50—C4595.21 (17)
C18—C20—H20A112.8C48—C50—H50A112.7
C15—C20—H20A112.8C45—C50—H50A112.7
C18—C20—H20B112.8C48—C50—H50B112.7
C15—C20—H20B112.8C45—C50—H50B112.7
H20A—C20—H20B110.3H50A—C50—H50B110.2
C22—C21—C26117.5 (2)C56—C51—C52116.9 (2)
C22—C21—C13124.97 (19)C56—C51—C43117.6 (2)
C26—C21—C13117.49 (19)C52—C51—C43125.5 (2)
C23—C22—C21120.7 (2)C53—C52—C51120.9 (2)
C23—C22—H22A119.6C53—C52—H52A119.5
C21—C22—H22A119.6C51—C52—H52A119.5
C22—C23—C24121.8 (2)C52—C53—C54121.9 (2)
C22—C23—H23A119.1C52—C53—H53A119.1
C24—C23—H23A119.1C54—C53—H53A119.1
C25—C24—C23117.5 (2)C55—C54—C53117.1 (2)
C25—C24—C27121.91 (19)C55—C54—C57121.4 (2)
C23—C24—C27120.6 (2)C53—C54—C57121.5 (2)
C26—C25—C24121.1 (2)C56—C55—C54121.5 (2)
C26—C25—H25A119.5C56—C55—H55A119.3
C24—C25—H25A119.5C54—C55—H55A119.3
C25—C26—C21121.3 (2)C55—C56—C51121.7 (2)
C25—C26—H26A119.3C55—C56—H56A119.2
C21—C26—H26A119.3C51—C56—H56A119.2
C24—C27—H27A109.5C54—C57—H57A109.5
C24—C27—H27B109.5C54—C57—H57B109.5
H27A—C27—H27B109.5H57A—C57—H57B109.5
C24—C27—H27C109.5C54—C57—H57C109.5
H27A—C27—H27C109.5H57A—C57—H57C109.5
H27B—C27—H27C109.5H57B—C57—H57C109.5
O1—S1—C1—C2102.92 (16)O32—S31—C31—C32128.40 (17)
O2—S1—C1—C2124.13 (15)O31—S31—C31—C3299.65 (18)
N1—S1—C1—C211.85 (16)N31—S31—C31—C3214.50 (17)
O1—S1—N1—C1192.08 (17)O32—S31—N31—C4135.3 (2)
O2—S1—N1—C1138.64 (18)O31—S31—N31—C4195.59 (19)
C1—S1—N1—C11153.81 (17)C31—S31—N31—C41150.86 (18)
O1—S1—N1—C8123.95 (14)O32—S31—N31—C38109.44 (17)
O2—S1—N1—C8105.34 (15)O31—S31—N31—C38119.68 (16)
C1—S1—N1—C89.84 (16)C31—S31—N31—C386.12 (17)
S1—C1—C2—C3146.51 (17)S31—C31—C32—C3830.1 (2)
S1—C1—C2—C828.9 (2)S31—C31—C32—C33147.16 (17)
S1—C1—C2—C688.8 (2)S31—C31—C32—C3689.2 (2)
C1—C2—C3—C4172.51 (19)C31—C32—C33—C34171.8 (2)
C8—C2—C3—C469.1 (2)C38—C32—C33—C3469.6 (2)
C6—C2—C3—C438.8 (2)C36—C32—C33—C3438.8 (2)
C2—C3—C4—C53.6 (2)C32—C33—C34—C352.8 (2)
C3—C4—C5—C774.6 (2)C33—C34—C35—C3773.7 (2)
C3—C4—C5—C633.6 (2)C33—C34—C35—C3634.6 (2)
C7—C5—C6—C963.9 (2)C34—C35—C36—C4061.6 (3)
C4—C5—C6—C9175.46 (19)C37—C35—C36—C40173.73 (19)
C7—C5—C6—C10173.30 (19)C34—C35—C36—C39175.4 (2)
C4—C5—C6—C1061.7 (2)C37—C35—C36—C3963.3 (2)
C7—C5—C6—C256.95 (19)C34—C35—C36—C3255.4 (2)
C4—C5—C6—C254.62 (19)C37—C35—C36—C3256.7 (2)
C1—C2—C6—C953.4 (3)C31—C32—C36—C4070.2 (3)
C3—C2—C6—C9175.2 (2)C38—C32—C36—C40168.91 (19)
C8—C2—C6—C965.9 (2)C33—C32—C36—C4060.1 (2)
C1—C2—C6—C1070.8 (3)C31—C32—C36—C3954.9 (3)
C3—C2—C6—C1060.6 (2)C38—C32—C36—C3966.0 (2)
C8—C2—C6—C10169.93 (19)C33—C32—C36—C39174.77 (19)
C1—C2—C6—C5171.57 (19)C31—C32—C36—C35172.46 (19)
C3—C2—C6—C557.10 (19)C38—C32—C36—C3551.55 (19)
C8—C2—C6—C552.27 (18)C33—C32—C36—C3557.21 (19)
C4—C5—C7—C866.9 (2)C34—C35—C37—C3865.9 (2)
C6—C5—C7—C841.5 (2)C36—C35—C37—C3842.1 (2)
C11—N1—C8—C771.3 (2)C41—N31—C38—C32172.48 (17)
S1—N1—C8—C7142.75 (15)S31—N31—C38—C3224.6 (2)
C11—N1—C8—C2173.99 (17)C41—N31—C38—C3771.7 (2)
S1—N1—C8—C228.06 (19)S31—N31—C38—C37140.45 (17)
C5—C7—C8—N1122.93 (19)C31—C32—C38—N3135.0 (2)
C5—C7—C8—C26.5 (2)C33—C32—C38—N31159.22 (17)
C1—C2—C8—N136.0 (2)C36—C32—C38—N3194.31 (19)
C3—C2—C8—N1160.78 (17)C31—C32—C38—C37158.23 (18)
C6—C2—C8—N192.41 (19)C33—C32—C38—C3777.5 (2)
C1—C2—C8—C7158.12 (18)C36—C32—C38—C3729.0 (2)
C3—C2—C8—C777.1 (2)C35—C37—C38—N31125.1 (2)
C6—C2—C8—C729.7 (2)C35—C37—C38—C327.5 (2)
C8—N1—C11—O32.3 (3)C38—N31—C41—O330.0 (3)
S1—N1—C11—O3139.98 (16)S31—N31—C41—O33143.59 (18)
C8—N1—C11—C12172.59 (17)C38—N31—C41—C42174.63 (18)
S1—N1—C11—C1245.1 (2)S31—N31—C41—C4241.8 (3)
O3—C11—C12—C139.0 (4)O33—C41—C42—C4310.5 (4)
N1—C11—C12—C13176.4 (2)N31—C41—C42—C43175.2 (2)
O3—C11—C12—C19156.2 (2)O33—C41—C42—C49155.5 (2)
N1—C11—C12—C1918.4 (3)N31—C41—C42—C4918.8 (3)
C11—C12—C13—C2114.9 (4)C41—C42—C43—C518.6 (4)
C19—C12—C13—C21176.0 (3)C49—C42—C43—C51178.2 (3)
C11—C12—C13—C14166.4 (2)C41—C42—C43—C44169.8 (2)
C19—C12—C13—C142.70 (17)C49—C42—C43—C440.20 (17)
C12—C13—C14—C15100.3 (2)C42—C43—C44—C45102.7 (2)
C21—C13—C14—C1580.7 (3)C51—C43—C44—C4576.0 (3)
C12—C13—C14—C192.63 (17)C42—C43—C44—C490.19 (16)
C21—C13—C14—C19176.4 (2)C51—C43—C44—C49178.5 (2)
C13—C14—C15—C16168.01 (18)C43—C44—C45—C46164.30 (18)
C19—C14—C15—C1674.9 (2)C49—C44—C45—C4671.6 (2)
C13—C14—C15—C2061.9 (2)C43—C44—C45—C5058.2 (2)
C19—C14—C15—C2031.2 (2)C49—C44—C45—C5034.5 (2)
C14—C15—C16—C1769.9 (2)C44—C45—C46—C4772.8 (2)
C20—C15—C16—C1738.0 (2)C50—C45—C46—C4733.8 (2)
C15—C16—C17—C183.3 (2)C45—C46—C47—C481.0 (2)
C16—C17—C18—C1973.9 (2)C46—C47—C48—C4971.1 (2)
C16—C17—C18—C2032.5 (2)C46—C47—C48—C5035.6 (2)
C13—C12—C19—C18105.0 (2)C43—C42—C49—C48102.6 (2)
C11—C12—C19—C1864.0 (3)C41—C42—C49—C4867.2 (3)
C13—C12—C19—C142.61 (17)C43—C42—C49—C440.19 (17)
C11—C12—C19—C14166.4 (2)C41—C42—C49—C44170.0 (2)
C20—C18—C19—C1254.2 (2)C47—C48—C49—C42163.88 (19)
C17—C18—C19—C12160.10 (18)C50—C48—C49—C4258.0 (2)
C20—C18—C19—C1437.2 (2)C47—C48—C49—C4471.9 (2)
C17—C18—C19—C1468.7 (2)C50—C48—C49—C4434.0 (2)
C13—C14—C19—C122.35 (15)C43—C44—C49—C420.17 (15)
C15—C14—C19—C12113.37 (16)C45—C44—C49—C42117.56 (17)
C13—C14—C19—C18119.37 (16)C43—C44—C49—C48117.01 (17)
C15—C14—C19—C183.65 (19)C45—C44—C49—C480.4 (2)
C19—C18—C20—C1554.77 (19)C47—C48—C50—C4555.5 (2)
C17—C18—C20—C1554.63 (19)C49—C48—C50—C4554.19 (19)
C16—C15—C20—C1857.16 (19)C46—C45—C50—C4854.90 (19)
C14—C15—C20—C1852.72 (19)C44—C45—C50—C4854.46 (19)
C12—C13—C21—C2214.2 (4)C42—C43—C51—C56177.2 (2)
C14—C13—C21—C22167.4 (2)C44—C43—C51—C564.8 (3)
C12—C13—C21—C26164.0 (3)C42—C43—C51—C523.1 (4)
C14—C13—C21—C2614.4 (3)C44—C43—C51—C52174.9 (2)
C26—C21—C22—C231.8 (3)C56—C51—C52—C530.5 (3)
C13—C21—C22—C23176.4 (2)C43—C51—C52—C53179.8 (2)
C21—C22—C23—C240.7 (3)C51—C52—C53—C540.0 (3)
C22—C23—C24—C252.4 (3)C52—C53—C54—C550.4 (3)
C22—C23—C24—C27176.5 (2)C52—C53—C54—C57179.4 (2)
C23—C24—C25—C261.7 (3)C53—C54—C55—C560.5 (3)
C27—C24—C25—C26177.25 (19)C57—C54—C55—C56179.4 (2)
C24—C25—C26—C210.8 (3)C54—C55—C56—C510.0 (3)
C22—C21—C26—C252.6 (3)C52—C51—C56—C550.5 (3)
C13—C21—C26—C25175.77 (19)C43—C51—C56—C55179.76 (19)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C3—H3B···O310.992.583.539 (3)163
C31—H31B···O30.992.453.356 (2)152
C38—H38A···O1i1.002.543.412 (2)146
C1—H1B···O33ii0.992.373.332 (3)164
C50—H50A···O2iii0.992.533.446 (2)153
C9—H9A···O3iv0.982.593.570 (3)174
C27—H27A···O32v0.982.433.404 (3)174
C22—H22A···O30.952.313.115 (3)142
C52—H52A···O330.952.333.129 (3)141
Symmetry codes: (i) x1, y, z; (ii) x+1, y, z; (iii) x+1, y1/2, z+3/2; (iv) x+1/2, y+3/2, z+2; (v) x, y+1, z.

Experimental details

(VI)(VII)
Crystal data
Chemical formulaC24H29NO3S2·0.5C4H8OC27H33NO3S
Mr479.65451.60
Crystal system, space groupTrigonal, P3221Orthorhombic, P212121
Temperature (K)150150
a, b, c (Å)12.0797 (17), 12.0797 (17), 28.326 (6)11.687 (2), 12.849 (3), 31.547 (6)
α, β, γ (°)90, 90, 12090, 90, 90
V3)3579.5 (10)4737.2 (16)
Z68
Radiation typeMo KαMo Kα
µ (mm1)0.250.17
Crystal size (mm)0.35 × 0.22 × 0.150.40 × 0.35 × 0.17
Data collection
DiffractometerNonius KappaCCD
diffractometer
Nonius KappaCCD
diffractometer
Absorption correctionMulti-scan
(DENZO–SMN; Otwinowski & Minor, 1997)
Multi-scan
(DENZO–SMN; Otwinowski & Minor, 1997)
Tmin, Tmax0.916, 0.9630.937, 0.972
No. of measured, independent and
observed [I > 2σ(I)] reflections
8354, 4207, 3310 44242, 9673, 7676
Rint0.0410.068
(sin θ/λ)max1)0.5950.625
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.038, 0.084, 1.01 0.041, 0.096, 1.03
No. of reflections42079673
No. of parameters318583
No. of restraints40
H-atom treatmentH-atom parameters constrainedH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.19, 0.310.19, 0.31
Absolute structureFlack (1983), 1788 Friedel pairsFlack (1983), 4291 Friedel pairs
Absolute structure parameter0.03 (7)0.02 (5)

Computer programs: COLLECT (Nonius, 1997), DENZO–SMN (Otwinowski & Minor, 1997), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL/PC (Sheldrick, 2008).

Hydrogen-bond geometry (Å, º) for (VI) top
D—H···AD—HH···AD···AD—H···A
C8—H8A···O2i1.02.593.516 (3)154
C1—H1B···O3ii0.992.453.422 (3)168
C14—H14A···O1iii1.002.663.500 (3)141
C1—H1A···O310.992.363.235 (14)147
Symmetry codes: (i) xy, y+1, z+1/3; (ii) xy+1, y+1, z+1/3; (iii) xy+1, y+2, z+1/3.
Hydrogen-bond geometry (Å, º) for (VII) top
D—H···AD—HH···AD···AD—H···A
C3—H3B···O310.992.583.539 (3)163
C31—H31B···O30.992.453.356 (2)152
C38—H38A···O1i1.002.543.412 (2)146
C1—H1B···O33ii0.992.373.332 (3)164
C50—H50A···O2iii0.992.533.446 (2)153
C9—H9A···O3iv0.982.593.570 (3)174
C27—H27A···O32v0.982.433.404 (3)174
C22—H22A···O30.952.313.115 (3)142
C52—H52A···O330.952.333.129 (3)141
Symmetry codes: (i) x1, y, z; (ii) x+1, y, z; (iii) x+1, y1/2, z+3/2; (iv) x+1/2, y+3/2, z+2; (v) x, y+1, z.
 

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