| Literature DB >> 22798780 |
David K Ford1, Victor G Young, George Barany.
Abstract
The title compound, C(4)H(6)O(2)S(4), was prepared by repeating, with subtle improvements, a multi-step route originally described by Mott & Barany [J. Chem. Soc. Perkin Trans. 1 (1984) ▶, pp. 2615-2621]. The title compound was obtained for the first time as a crystalline material. The two [(methyl-sulfan-yl)carbon-yl]sulfenyl moieties are essentially perpendic-ular to each other, each approximately planar (r.m.s. deviations of 0.02 and 0.01 Å) and with a C-S-S-C torsion angle = 90.99 (6)°, which compares well with the theoretical value of 90°.Entities:
Year: 2012 PMID: 22798780 PMCID: PMC3393915 DOI: 10.1107/S1600536812024750
Source DB: PubMed Journal: Acta Crystallogr Sect E Struct Rep Online ISSN: 1600-5368
| C4H6O2S4 | |
| Triclinic, | |
| Mo | |
| Cell parameters from 2965 reflections | |
| θ = 2.2–27.5° | |
| α = 109.875 (2)° | µ = 1.07 mm−1 |
| β = 92.154 (2)° | |
| γ = 101.481 (2)° | Block, colourless |
| 0.35 × 0.30 × 0.25 mm |
| Bruker SMART CCD area-detector diffractometer | 1894 independent reflections |
| Radiation source: sealed tube | 1774 reflections with |
| Graphite monochromator | |
| φ and ω scans | θmax = 27.5°, θmin = 2.2° |
| Absorption correction: multi-scan ( | |
| 5024 measured reflections |
| Refinement on | Primary atom site location: structure-invariant direct methods |
| Least-squares matrix: full | Secondary atom site location: difference Fourier map |
| Hydrogen site location: inferred from neighbouring sites | |
| H-atom parameters constrained | |
| 1894 reflections | (Δ/σ)max = 0.001 |
| 93 parameters | Δρmax = 0.36 e Å−3 |
| 0 restraints | Δρmin = −0.24 e Å−3 |
| 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 |
| S1 | 0.14601 (6) | 0.32879 (4) | 0.88175 (3) | 0.01738 (9) | |
| S2 | 0.29712 (6) | 0.29567 (4) | 0.58244 (3) | 0.01738 (9) | |
| S3 | 0.59396 (6) | 0.46586 (4) | 0.72293 (4) | 0.01720 (9) | |
| S4 | 0.23910 (6) | 0.67401 (4) | 0.66158 (4) | 0.01664 (9) | |
| O1 | −0.13318 (18) | 0.13895 (12) | 0.63241 (11) | 0.0206 (2) | |
| O2 | 0.68271 (19) | 0.78866 (12) | 0.83115 (12) | 0.0242 (2) | |
| C1 | −0.1386 (3) | 0.22275 (18) | 0.93481 (15) | 0.0203 (3) | |
| H1A | −0.1228 | 0.2564 | 1.0402 | 0.030* | |
| H1B | −0.1567 | 0.1011 | 0.8914 | 0.030* | |
| H1C | −0.2906 | 0.2533 | 0.9016 | 0.030* | |
| C2 | 0.0631 (2) | 0.23846 (16) | 0.69410 (14) | 0.0151 (3) | |
| C3 | 0.5248 (2) | 0.66889 (17) | 0.75182 (14) | 0.0162 (3) | |
| C4 | 0.2779 (3) | 0.89933 (17) | 0.72402 (17) | 0.0224 (3) | |
| H4A | 0.1240 | 0.9264 | 0.6889 | 0.034* | |
| H4B | 0.4291 | 0.9490 | 0.6872 | 0.034* | |
| H4C | 0.3016 | 0.9447 | 0.8298 | 0.034* |
| S1 | 0.01675 (17) | 0.01802 (17) | 0.01540 (17) | 0.00122 (12) | 0.00094 (12) | 0.00507 (13) |
| S2 | 0.01809 (17) | 0.01627 (17) | 0.01596 (17) | 0.00210 (12) | 0.00280 (12) | 0.00433 (13) |
| S3 | 0.01357 (16) | 0.01617 (17) | 0.02213 (18) | 0.00337 (12) | 0.00094 (13) | 0.00725 (13) |
| S4 | 0.01479 (16) | 0.01637 (17) | 0.01887 (17) | 0.00321 (12) | −0.00024 (12) | 0.00678 (13) |
| O1 | 0.0178 (5) | 0.0190 (5) | 0.0212 (5) | 0.0005 (4) | −0.0005 (4) | 0.0048 (4) |
| O2 | 0.0210 (5) | 0.0181 (5) | 0.0297 (6) | 0.0003 (4) | −0.0060 (4) | 0.0070 (4) |
| C1 | 0.0189 (7) | 0.0214 (7) | 0.0213 (7) | 0.0026 (5) | 0.0049 (5) | 0.0094 (6) |
| C2 | 0.0164 (6) | 0.0130 (6) | 0.0169 (6) | 0.0058 (5) | 0.0021 (5) | 0.0050 (5) |
| C3 | 0.0151 (6) | 0.0169 (6) | 0.0184 (6) | 0.0037 (5) | 0.0031 (5) | 0.0083 (5) |
| C4 | 0.0231 (7) | 0.0162 (7) | 0.0288 (8) | 0.0053 (5) | 0.0006 (6) | 0.0090 (6) |
| S1—C2 | 1.7553 (14) | O2—C3 | 1.2067 (17) |
| S1—C1 | 1.8057 (14) | C1—H1A | 0.9800 |
| S2—C2 | 1.8057 (13) | C1—H1B | 0.9800 |
| S2—S3 | 2.0332 (5) | C1—H1C | 0.9800 |
| S3—C3 | 1.8047 (14) | C4—H4A | 0.9800 |
| S4—C3 | 1.7528 (14) | C4—H4B | 0.9800 |
| S4—C4 | 1.8077 (14) | C4—H4C | 0.9800 |
| O1—C2 | 1.2037 (16) | ||
| C2—S1—C1 | 98.04 (6) | O1—C2—S2 | 116.70 (10) |
| C2—S2—S3 | 105.23 (5) | S1—C2—S2 | 117.13 (7) |
| C3—S3—S2 | 105.85 (5) | O2—C3—S4 | 126.34 (11) |
| C3—S4—C4 | 97.96 (7) | O2—C3—S3 | 116.20 (10) |
| S1—C1—H1A | 109.5 | S4—C3—S3 | 117.46 (7) |
| S1—C1—H1B | 109.5 | S4—C4—H4A | 109.5 |
| H1A—C1—H1B | 109.5 | S4—C4—H4B | 109.5 |
| S1—C1—H1C | 109.5 | H4A—C4—H4B | 109.5 |
| H1A—C1—H1C | 109.5 | S4—C4—H4C | 109.5 |
| H1B—C1—H1C | 109.5 | H4A—C4—H4C | 109.5 |
| O1—C2—S1 | 126.15 (10) | H4B—C4—H4C | 109.5 |
| C2—S2—S3—C3 | −90.99 (6) | C4—S4—C3—O2 | 1.13 (14) |
| C1—S1—C2—O1 | 1.09 (13) | C4—S4—C3—S3 | −178.16 (8) |
| C1—S1—C2—S2 | −177.21 (8) | S2—S3—C3—O2 | −178.71 (10) |
| S3—S2—C2—O1 | 179.07 (9) | S2—S3—C3—S4 | 0.65 (8) |
| S3—S2—C2—S1 | −2.46 (8) |