| Literature DB >> 29416894 |
Wafia Boukhedena1, Abdelali Fiala1, Hayet Brahim Ladouani1, Salah Eddine Lemallem1, Noudjoud Hamdouni2, Ali Boudjada2.
Abstract
The title compound, C9H11NO2S2, contains a 1,3-di-thiane ring which has a twist-boat conformation. The dihedral angle between the mean planes of the ethyl acetate group and the di-thiane ring is 17.56 (13)°. In the crystal, mol-ecules stack in layers up the a-axis direction, however, there are no significant inter-molecular inter-actions present.Entities:
Keywords: 1,3-dithian-2-ylidene; crystal structure; twist-boat conformation
Year: 2018 PMID: 29416894 PMCID: PMC5778488 DOI: 10.1107/S2056989017017893
Source DB: PubMed Journal: Acta Crystallogr E Crystallogr Commun
Figure 1The molecular structure of the title compound (I), with the atom labelling. Displacement ellipsoids are drawn at the 50% probability level.
Figure 2A view along the b axis of the crystal packing of the title compound (I).
Figure 3Structural overlap of compounds (I) and (II); the latter is shown in red.
Experimental details
| Crystal data | |
| Chemical formula | C9H11NO2S2 |
|
| 229.31 |
| Crystal system, space group | Monoclinic, |
| Temperature (K) | 293 |
|
| 15.826 (3), 8.0772 (6), 18.431 (2) |
| β (°) | 111.830 (16) |
|
| 2187.1 (5) |
|
| 8 |
| Radiation type | Mo |
| μ (mm−1) | 0.46 |
| Crystal size (mm) | 0.48 × 0.27 × 0.13 |
| Data collection | |
| Diffractometer | Agilent Xcalibur Eos |
| Absorption correction | Multi-scan ( |
|
| 0.334, 1.000 |
| No. of measured, independent and observed [ | 4539, 2132, 1667 |
|
| 0.035 |
| (sin θ/λ)max (Å−1) | 0.617 |
| Refinement | |
|
| 0.049, 0.138, 1.08 |
| No. of reflections | 2132 |
| No. of parameters | 127 |
| H-atom treatment | H-atom parameters constrained |
| Δρmax, Δρmin (e Å−3) | 0.46, −0.34 |
Computer programs: CrysAlis PRO (Agilent, 2013 ▸), SIR92 (Altomare et al., 1994 ▸), ORTEP-3 for Windows (Farrugia, 2012 ▸) and Mercury (Macrae et al., 2008 ▸), SHELXL2016 (Sheldrick, 2015 ▸), PLATON (Spek, 2009 ▸) and publCIF (Westrip, 2010 ▸).
| C9H11NO2S2 | |
| Monoclinic, | Mo |
| Cell parameters from 1541 reflections | |
| θ = 3.7–28.9° | |
| µ = 0.46 mm−1 | |
| β = 111.830 (16)° | |
| Needle, pale yellow | |
| 0.48 × 0.27 × 0.13 mm |
| Agilent Xcalibur Eos diffractometer | 2132 independent reflections |
| Graphite monochromator | 1667 reflections with |
| Detector resolution: 8.02 pixels mm-1 | |
| ω scans | θmax = 26.0°, θmin = 3.4° |
| Absorption correction: multi-scan (CrysAlis PRO; Agilent, 2013) | |
| 4539 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 | |
| 2132 reflections | (Δ/σ)max < 0.001 |
| 127 parameters | Δρmax = 0.46 e Å−3 |
| 0 restraints | Δρmin = −0.34 e Å−3 |
| Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes. |
| S2 | 0.12671 (5) | 0.08363 (8) | 0.29431 (4) | 0.0555 (3) | |
| S1 | 0.11241 (5) | 0.40461 (8) | 0.37170 (4) | 0.0589 (3) | |
| O1 | 0.14349 (14) | −0.1692 (2) | 0.40827 (11) | 0.0641 (5) | |
| O2 | 0.12483 (13) | −0.1107 (2) | 0.52062 (11) | 0.0592 (5) | |
| N1 | 0.1307 (2) | 0.2907 (3) | 0.55919 (14) | 0.0741 (7) | |
| C1 | 0.13376 (16) | −0.0706 (3) | 0.45311 (14) | 0.0477 (6) | |
| C2 | 0.13016 (16) | 0.1100 (3) | 0.44342 (13) | 0.0447 (6) | |
| C3 | 0.13080 (18) | 0.2096 (3) | 0.50818 (15) | 0.0512 (6) | |
| C4 | 0.12494 (15) | 0.1895 (3) | 0.37572 (14) | 0.0449 (6) | |
| C5 | 0.1624 (2) | 0.4577 (4) | 0.30133 (16) | 0.0620 (7) | |
| H5A | 0.166410 | 0.577323 | 0.299200 | 0.074* | |
| H5B | 0.224000 | 0.414405 | 0.319553 | 0.074* | |
| C6 | 0.1113 (2) | 0.3938 (3) | 0.21943 (16) | 0.0639 (7) | |
| H6A | 0.153558 | 0.381976 | 0.192819 | 0.077* | |
| H6B | 0.065809 | 0.474754 | 0.190915 | 0.077* | |
| C7 | 0.06477 (19) | 0.2289 (3) | 0.21774 (15) | 0.0615 (7) | |
| H7A | 0.053615 | 0.176859 | 0.167585 | 0.074* | |
| H7B | 0.006049 | 0.249883 | 0.221227 | 0.074* | |
| C8 | 0.1298 (2) | −0.2859 (3) | 0.54028 (17) | 0.0617 (7) | |
| H8A | 0.185483 | −0.334042 | 0.539292 | 0.074* | |
| H8B | 0.078396 | −0.344992 | 0.503306 | 0.074* | |
| C9 | 0.1279 (2) | −0.2958 (4) | 0.62053 (19) | 0.0731 (9) | |
| H9A | 0.131070 | −0.409675 | 0.636284 | 0.110* | |
| H9B | 0.179046 | −0.236653 | 0.656364 | 0.110* | |
| H9C | 0.072531 | −0.247544 | 0.620570 | 0.110* |
| S2 | 0.0705 (5) | 0.0497 (4) | 0.0437 (4) | 0.0033 (3) | 0.0182 (3) | −0.0037 (3) |
| S1 | 0.0862 (5) | 0.0418 (4) | 0.0494 (4) | 0.0049 (3) | 0.0259 (4) | 0.0024 (3) |
| O1 | 0.0886 (14) | 0.0476 (10) | 0.0518 (11) | 0.0075 (9) | 0.0211 (10) | −0.0022 (9) |
| O2 | 0.0821 (13) | 0.0399 (9) | 0.0561 (11) | 0.0057 (8) | 0.0262 (10) | 0.0067 (8) |
| N1 | 0.115 (2) | 0.0547 (14) | 0.0513 (14) | 0.0002 (13) | 0.0293 (15) | −0.0027 (12) |
| C1 | 0.0463 (13) | 0.0469 (13) | 0.0407 (13) | 0.0027 (10) | 0.0057 (10) | 0.0025 (11) |
| C2 | 0.0471 (12) | 0.0443 (13) | 0.0349 (11) | 0.0026 (10) | 0.0064 (10) | −0.0013 (10) |
| C3 | 0.0616 (15) | 0.0447 (13) | 0.0413 (13) | 0.0019 (11) | 0.0122 (12) | 0.0057 (11) |
| C4 | 0.0417 (12) | 0.0435 (13) | 0.0422 (13) | 0.0018 (9) | 0.0073 (10) | 0.0005 (10) |
| C5 | 0.0682 (17) | 0.0556 (15) | 0.0593 (17) | −0.0084 (13) | 0.0203 (14) | 0.0065 (13) |
| C6 | 0.080 (2) | 0.0629 (17) | 0.0485 (15) | −0.0046 (14) | 0.0235 (14) | 0.0030 (14) |
| C7 | 0.0710 (17) | 0.0669 (17) | 0.0389 (13) | −0.0043 (14) | 0.0116 (13) | 0.0008 (13) |
| C8 | 0.0763 (19) | 0.0408 (13) | 0.0678 (19) | 0.0036 (12) | 0.0266 (15) | 0.0098 (12) |
| C9 | 0.098 (2) | 0.0544 (17) | 0.078 (2) | 0.0146 (15) | 0.0454 (19) | 0.0181 (15) |
| S2—C4 | 1.736 (2) | C5—H5B | 0.9700 |
| S2—C7 | 1.817 (3) | C6—C7 | 1.517 (4) |
| S1—C4 | 1.747 (2) | C6—H6A | 0.9700 |
| S1—C5 | 1.805 (3) | C6—H6B | 0.9700 |
| O1—C1 | 1.198 (3) | C7—H7A | 0.9700 |
| O2—C1 | 1.343 (3) | C7—H7B | 0.9700 |
| O2—C8 | 1.456 (3) | C8—C9 | 1.492 (4) |
| N1—C3 | 1.146 (3) | C8—H8A | 0.9700 |
| C1—C2 | 1.469 (3) | C8—H8B | 0.9700 |
| C2—C4 | 1.378 (3) | C9—H9A | 0.9600 |
| C2—C3 | 1.436 (3) | C9—H9B | 0.9600 |
| C5—C6 | 1.514 (4) | C9—H9C | 0.9600 |
| C5—H5A | 0.9700 | ||
| C4—S2—C7 | 100.12 (13) | C5—C6—H6B | 108.9 |
| C4—S1—C5 | 101.16 (13) | C7—C6—H6B | 108.9 |
| C1—O2—C8 | 116.8 (2) | H6A—C6—H6B | 107.7 |
| O1—C1—O2 | 124.3 (2) | C6—C7—S2 | 115.69 (19) |
| O1—C1—C2 | 125.9 (2) | C6—C7—H7A | 108.4 |
| O2—C1—C2 | 109.8 (2) | S2—C7—H7A | 108.4 |
| C4—C2—C3 | 118.1 (2) | C6—C7—H7B | 108.4 |
| C4—C2—C1 | 124.0 (2) | S2—C7—H7B | 108.4 |
| C3—C2—C1 | 117.9 (2) | H7A—C7—H7B | 107.4 |
| N1—C3—C2 | 179.1 (3) | O2—C8—C9 | 106.2 (2) |
| C2—C4—S2 | 122.55 (18) | O2—C8—H8A | 110.5 |
| C2—C4—S1 | 117.99 (18) | C9—C8—H8A | 110.5 |
| S2—C4—S1 | 119.43 (14) | O2—C8—H8B | 110.5 |
| C6—C5—S1 | 114.9 (2) | C9—C8—H8B | 110.5 |
| C6—C5—H5A | 108.5 | H8A—C8—H8B | 108.7 |
| S1—C5—H5A | 108.5 | C8—C9—H9A | 109.5 |
| C6—C5—H5B | 108.5 | C8—C9—H9B | 109.5 |
| S1—C5—H5B | 108.5 | H9A—C9—H9B | 109.5 |
| H5A—C5—H5B | 107.5 | C8—C9—H9C | 109.5 |
| C5—C6—C7 | 113.3 (2) | H9A—C9—H9C | 109.5 |
| C5—C6—H6A | 108.9 | H9B—C9—H9C | 109.5 |
| C7—C6—H6A | 108.9 | ||
| C8—O2—C1—O1 | 1.6 (4) | C7—S2—C4—C2 | 153.6 (2) |
| C8—O2—C1—C2 | −178.2 (2) | C7—S2—C4—S1 | −24.31 (17) |
| O1—C1—C2—C4 | 9.4 (4) | C5—S1—C4—C2 | 153.59 (19) |
| O2—C1—C2—C4 | −170.8 (2) | C5—S1—C4—S2 | −28.43 (18) |
| O1—C1—C2—C3 | −171.5 (2) | C4—S1—C5—C6 | 65.6 (2) |
| O2—C1—C2—C3 | 8.2 (3) | S1—C5—C6—C7 | −32.9 (3) |
| C3—C2—C4—S2 | 178.22 (18) | C5—C6—C7—S2 | −37.1 (3) |
| C1—C2—C4—S2 | −2.7 (3) | C4—S2—C7—C6 | 65.9 (2) |
| C3—C2—C4—S1 | −3.9 (3) | C1—O2—C8—C9 | 174.2 (2) |
| C1—C2—C4—S1 | 175.18 (18) |