Abstract
There are two molecules in the asymmetric unit of the title compound, C4H13NO2SSi. In the crystal, molecules are linked via intermolecular N—H⋯O hydrogen bonds, forming chains along [001]. The crystal studied was an inversion twin, the refined ratio of twin domains being 0.61 (9):0.39 (9).
Related literature
For the original synthesis of the title compound, see: Roy (1993 ▶). For the synthetic application of the title compound, see: Roy et al. (1993 ▶). For related structures, see: Ni et al. (1995 ▶); Chunechom et al. (1998 ▶).
Experimental
Crystal data
C4H13NO2SSi
M r = 167.30
Monoclinic,
a = 8.2827 (4) Å
b = 10.9513 (5) Å
c = 9.6201 (3) Å
β = 92.536 (2)°
V = 871.75 (6) Å3
Z = 4
Mo Kα radiation
μ = 0.45 mm−1
T = 150 K
0.32 × 0.25 × 0.24 mm
Data collection
Nonius KappaCCD diffractometer
Absorption correction: multi-scan (SORTAV; Blessing 1995 ▶) T min = 0.830, T max = 0.931
6920 measured reflections
4894 independent reflections
4195 reflections with I > 2σ(I)
R int = 0.030
Refinement
R[F 2 > 2σ(F 2)] = 0.039
wR(F 2) = 0.094
S = 1.05
4894 reflections
170 parameters
2 restraints
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.41 e Å−3
Δρmin = −0.49 e Å−3
Absolute structure: Flack (1983 ▶), 1787 Friedel pairs
Flack parameter: 0.39 (9)
Data collection: COLLECT (Nonius, 2002 ▶); cell refinement: DENZO-SMN (Otwinowski & Minor, 1997 ▶); data reduction: DENZO-SMN; program(s) used to solve structure: SIR92 (Altomare et al., 1994 ▶); program(s) used to refine structure: SHELXTL (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXTL.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536810050336/si2314sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810050336/si2314Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1B—H1NB⋯O2A | 0.81 (2) | 2.11 (2) | 2.917 (3) | 173 (3) |
| N1A—H1NA⋯O2Bi | 0.81 (2) | 2.12 (2) | 2.925 (3) | 177 (3) |
Symmetry code: (i)
.
Acknowledgments
AM would like to thank Ryerson University’s Faculty of Engineering, Architecture and Science for funding.
supplementary crystallographic information
Comment
N-trimethylsilylmethylsulfonamide, a key intermediate in the synthesis of polyoxothiazenes (Roy et al., 1993) and polythionylphosphazenes (Chunechom et al., 1998), was prepared via the reaction of methanesulfonyl chloride and hexamethyldisilazane (Roy, 1993). The asymmetric unit of the title compound, which contains two independent molecules, is shown in Fig. 1. The S—N bond distances in each molecule are intermediate between a typical S—N single bond (1.74 Å) and a typical S=N double bond (1.54 Å), (Ni et al., 1995) suggesting the presence of some π-bonding between the sulfur and nitrogen atoms. The S—N—Si bond angles of 127.83 (14)° and 128.59 (14)Å are larger than might be expected, in terms of hybridization priciples, for either a tetrahedral or trigonal planar geometry about the nitrogen atom. In the crystal structure, molecules are linked via intermolecular N—H···O hydrogen bonds to form one-dimensional chains along [001] (Fig. 2).
Experimental
The title compound was prepared via addition of methanesulfonyl chloride (7 ml, 102.5 mmol) to a three-necked round-bottom flask equipped with a magnetic stirring bar, gas inlet, reflux condenser and a rubber septa under an inert N2 atmosphere. Hexamethyldisilazane (20 ml, 103.1 mmol) was added drop wise over 10 minutes with stirring at ambient temperatures. The flask was then placed into an oil bath and the reaction mixture heated to 363–373 K to initiate the reaction. The temperature of the oil bath was increased to between 388–393 K and the reaction mixture refluxed at this temperature for 2 h. The reaction mixture was allowed to cool to room temperature and the reaction by-product (Me3SiCl) was removed in vacuo. The resulting crude white powder was recrystallized from a CH2Cl2/Hexane mixture producing colourless crystals. (Yield = 15.6 g, 91%).
Refinement
Hydrogen atoms were placed in calculated positions with C—H distances ranging from 0.98 Å and included in the refinement in a riding-model approximation with Uiso(H) = 1.5Ueq(C). The positional parameters of the H atoms bonded to N atoms were refined independently and with Uiso(H) = 1.5Ueq(N). The N—H distances were constrained to be the same in each molecule [0.81 (2) Å] using the SADI command in SHELXL (Sheldrick, 2008).
Figures
Fig. 1.
The asymmetric unit of title compound showing 30% probability ellipsoids. The dashed line indicates a hydrogen bond.
Fig. 2.
Part of the crystal structure showing hydrogen bonds as dashed lines.
Crystal data
| C4H13NO2SSi | F(000) = 360 |
| Mr = 167.30 | Dx = 1.275 Mg m−3 |
| Monoclinic, P21 | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: P 2yb | Cell parameters from 6920 reflections |
| a = 8.2827 (4) Å | θ = 2.8–32.0° |
| b = 10.9513 (5) Å | µ = 0.45 mm−1 |
| c = 9.6201 (3) Å | T = 150 K |
| β = 92.536 (2)° | Block, colourless |
| V = 871.75 (6) Å3 | 0.32 × 0.25 × 0.24 mm |
| Z = 4 |
Data collection
| Nonius KappaCCD diffractometer | 4894 independent reflections |
| Radiation source: fine-focus sealed tube | 4195 reflections with I > 2σ(I) |
| graphite | Rint = 0.030 |
| Detector resolution: 9 pixels mm-1 | θmax = 32.0°, θmin = 2.8° |
| φ scans and ω scans with κ offsets | h = −12→12 |
| Absorption correction: multi-scan (SORTAV; Blessing 1995) | k = −14→16 |
| Tmin = 0.830, Tmax = 0.931 | l = −12→14 |
| 6920 measured reflections |
Refinement
| Refinement on F2 | Secondary atom site location: difference Fourier map |
| Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
| R[F2 > 2σ(F2)] = 0.039 | H atoms treated by a mixture of independent and constrained refinement |
| wR(F2) = 0.094 | w = 1/[σ2(Fo2) + (0.0218P)2 + 0.660P] where P = (Fo2 + 2Fc2)/3 |
| S = 1.05 | (Δ/σ)max < 0.001 |
| 4894 reflections | Δρmax = 0.41 e Å−3 |
| 170 parameters | Δρmin = −0.49 e Å−3 |
| 2 restraints | Absolute structure: Flack (1983), 1787 Friedel pairs |
| Primary atom site location: structure-invariant direct methods | Flack parameter: 0.39 (9) |
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 | ||
| S1A | 0.84555 (7) | 0.27915 (6) | 0.95708 (6) | 0.02134 (13) | |
| Si1A | 0.55749 (8) | 0.11459 (7) | 0.99573 (7) | 0.02169 (14) | |
| O1A | 0.8724 (3) | 0.40683 (18) | 0.9815 (2) | 0.0303 (4) | |
| O2A | 0.8188 (2) | 0.2381 (2) | 0.81562 (18) | 0.0308 (4) | |
| N1A | 0.6945 (3) | 0.2334 (2) | 1.0411 (2) | 0.0228 (4) | |
| H1NA | 0.693 (4) | 0.265 (3) | 1.117 (2) | 0.027* | |
| C1A | 1.0156 (4) | 0.2012 (3) | 1.0271 (3) | 0.0329 (6) | |
| H1AA | 1.1115 | 0.2264 | 0.9783 | 0.049* | |
| H1AB | 0.9994 | 0.1131 | 1.0158 | 0.049* | |
| H1AC | 1.0307 | 0.2207 | 1.1262 | 0.049* | |
| C2A | 0.6695 (4) | −0.0301 (3) | 0.9698 (3) | 0.0326 (6) | |
| H2AA | 0.7328 | −0.0505 | 1.0552 | 0.049* | |
| H2AB | 0.7423 | −0.0201 | 0.8930 | 0.049* | |
| H2AC | 0.5926 | −0.0960 | 0.9476 | 0.049* | |
| C3A | 0.4308 (3) | 0.1074 (3) | 1.1496 (3) | 0.0296 (6) | |
| H3AA | 0.3737 | 0.1851 | 1.1595 | 0.044* | |
| H3AB | 0.4997 | 0.0922 | 1.2332 | 0.044* | |
| H3AC | 0.3520 | 0.0411 | 1.1374 | 0.044* | |
| C4A | 0.4362 (4) | 0.1526 (3) | 0.8351 (3) | 0.0322 (6) | |
| H4AA | 0.3771 | 0.2288 | 0.8490 | 0.048* | |
| H4AB | 0.3593 | 0.0866 | 0.8136 | 0.048* | |
| H4AC | 0.5082 | 0.1626 | 0.7577 | 0.048* | |
| S1B | 0.65985 (7) | 0.31234 (6) | 0.45178 (6) | 0.02162 (13) | |
| Si1B | 0.94662 (8) | 0.47963 (7) | 0.51424 (7) | 0.02164 (14) | |
| O1B | 0.6327 (3) | 0.18445 (19) | 0.4738 (2) | 0.0310 (5) | |
| O2B | 0.6801 (2) | 0.3547 (2) | 0.31117 (19) | 0.0307 (4) | |
| N1B | 0.8160 (3) | 0.3552 (2) | 0.5432 (2) | 0.0223 (4) | |
| H1NB | 0.820 (3) | 0.317 (3) | 0.615 (2) | 0.027* | |
| C1B | 0.4928 (4) | 0.3904 (3) | 0.5154 (3) | 0.0340 (7) | |
| H1BA | 0.3947 | 0.3668 | 0.4613 | 0.051* | |
| H1BB | 0.5096 | 0.4787 | 0.5068 | 0.051* | |
| H1BC | 0.4811 | 0.3694 | 0.6134 | 0.051* | |
| C2B | 0.8316 (4) | 0.6243 (3) | 0.5137 (3) | 0.0329 (6) | |
| H2BA | 0.7775 | 0.6327 | 0.6018 | 0.049* | |
| H2BB | 0.7506 | 0.6239 | 0.4363 | 0.049* | |
| H2BC | 0.9057 | 0.6930 | 0.5027 | 0.049* | |
| C3B | 1.0911 (3) | 0.4706 (3) | 0.6667 (3) | 0.0309 (6) | |
| H3BA | 1.0326 | 0.4805 | 0.7523 | 0.046* | |
| H3BB | 1.1719 | 0.5355 | 0.6607 | 0.046* | |
| H3BC | 1.1451 | 0.3910 | 0.6677 | 0.046* | |
| C4B | 1.0488 (3) | 0.4616 (3) | 0.3477 (3) | 0.0304 (6) | |
| H4BA | 0.9686 | 0.4671 | 0.2699 | 0.046* | |
| H4BB | 1.1023 | 0.3818 | 0.3460 | 0.046* | |
| H4BC | 1.1294 | 0.5264 | 0.3392 | 0.046* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1A | 0.0233 (3) | 0.0193 (3) | 0.0216 (3) | −0.0012 (2) | 0.0028 (2) | 0.0028 (2) |
| Si1A | 0.0216 (3) | 0.0221 (4) | 0.0213 (3) | −0.0027 (3) | 0.0008 (2) | −0.0005 (3) |
| O1A | 0.0340 (11) | 0.0163 (10) | 0.0406 (11) | −0.0031 (8) | 0.0019 (9) | 0.0038 (9) |
| O2A | 0.0417 (11) | 0.0324 (11) | 0.0187 (8) | −0.0058 (9) | 0.0065 (7) | 0.0011 (8) |
| N1A | 0.0264 (10) | 0.0239 (12) | 0.0184 (10) | −0.0044 (9) | 0.0032 (8) | −0.0033 (9) |
| C1A | 0.0266 (13) | 0.0273 (16) | 0.0448 (17) | 0.0039 (11) | 0.0010 (12) | 0.0066 (13) |
| C2A | 0.0354 (15) | 0.0216 (15) | 0.0409 (15) | −0.0002 (11) | 0.0039 (12) | −0.0032 (13) |
| C3A | 0.0254 (12) | 0.0378 (16) | 0.0258 (12) | −0.0083 (11) | 0.0038 (9) | −0.0004 (12) |
| C4A | 0.0308 (14) | 0.0392 (18) | 0.0258 (13) | −0.0014 (11) | −0.0066 (10) | −0.0018 (12) |
| S1B | 0.0240 (3) | 0.0198 (3) | 0.0211 (3) | −0.0010 (2) | 0.0015 (2) | −0.0029 (2) |
| Si1B | 0.0230 (3) | 0.0216 (4) | 0.0205 (3) | −0.0035 (3) | 0.0030 (2) | 0.0007 (3) |
| O1B | 0.0349 (11) | 0.0190 (11) | 0.0387 (11) | −0.0052 (8) | −0.0021 (8) | −0.0036 (9) |
| O2B | 0.0388 (11) | 0.0333 (11) | 0.0200 (8) | −0.0036 (8) | 0.0005 (7) | −0.0021 (8) |
| N1B | 0.0258 (10) | 0.0209 (11) | 0.0201 (10) | −0.0035 (8) | 0.0007 (8) | 0.0041 (9) |
| C1B | 0.0244 (13) | 0.0339 (18) | 0.0443 (17) | 0.0034 (11) | 0.0060 (11) | −0.0082 (14) |
| C2B | 0.0368 (15) | 0.0209 (14) | 0.0415 (16) | −0.0004 (12) | 0.0057 (12) | 0.0003 (13) |
| C3B | 0.0277 (13) | 0.0395 (17) | 0.0253 (12) | −0.0071 (12) | −0.0015 (10) | 0.0003 (13) |
| C4B | 0.0321 (14) | 0.0340 (17) | 0.0260 (13) | −0.0037 (11) | 0.0106 (10) | 0.0026 (12) |
Geometric parameters (Å, °)
| S1A—O1A | 1.434 (2) | S1B—O1B | 1.436 (2) |
| S1A—O2A | 1.4410 (19) | S1B—O2B | 1.4469 (19) |
| S1A—N1A | 1.600 (2) | S1B—N1B | 1.602 (2) |
| S1A—C1A | 1.755 (3) | S1B—C1B | 1.759 (3) |
| Si1A—N1A | 1.768 (2) | Si1B—N1B | 1.769 (2) |
| Si1A—C4A | 1.853 (3) | Si1B—C2B | 1.849 (3) |
| Si1A—C3A | 1.853 (3) | Si1B—C3B | 1.854 (3) |
| Si1A—C2A | 1.859 (3) | Si1B—C4B | 1.855 (3) |
| N1A—H1NA | 0.81 (2) | N1B—H1NB | 0.81 (2) |
| C1A—H1AA | 0.9800 | C1B—H1BA | 0.9800 |
| C1A—H1AB | 0.9800 | C1B—H1BB | 0.9800 |
| C1A—H1AC | 0.9800 | C1B—H1BC | 0.9800 |
| C2A—H2AA | 0.9800 | C2B—H2BA | 0.9800 |
| C2A—H2AB | 0.9800 | C2B—H2BB | 0.9800 |
| C2A—H2AC | 0.9800 | C2B—H2BC | 0.9800 |
| C3A—H3AA | 0.9800 | C3B—H3BA | 0.9800 |
| C3A—H3AB | 0.9800 | C3B—H3BB | 0.9800 |
| C3A—H3AC | 0.9800 | C3B—H3BC | 0.9800 |
| C4A—H4AA | 0.9800 | C4B—H4BA | 0.9800 |
| C4A—H4AB | 0.9800 | C4B—H4BB | 0.9800 |
| C4A—H4AC | 0.9800 | C4B—H4BC | 0.9800 |
| O1A—S1A—O2A | 118.36 (12) | O1B—S1B—O2B | 118.44 (12) |
| O1A—S1A—N1A | 110.00 (13) | O1B—S1B—N1B | 109.44 (12) |
| O2A—S1A—N1A | 106.77 (12) | O2B—S1B—N1B | 107.15 (12) |
| O1A—S1A—C1A | 107.19 (15) | O1B—S1B—C1B | 106.99 (15) |
| O2A—S1A—C1A | 107.34 (15) | O2B—S1B—C1B | 107.15 (15) |
| N1A—S1A—C1A | 106.61 (14) | N1B—S1B—C1B | 107.15 (14) |
| N1A—Si1A—C4A | 111.04 (13) | N1B—Si1B—C2B | 110.00 (13) |
| N1A—Si1A—C3A | 102.36 (12) | N1B—Si1B—C3B | 102.23 (12) |
| C4A—Si1A—C3A | 111.74 (14) | C2B—Si1B—C3B | 111.25 (15) |
| N1A—Si1A—C2A | 109.97 (13) | N1B—Si1B—C4B | 111.06 (13) |
| C4A—Si1A—C2A | 109.58 (15) | C2B—Si1B—C4B | 110.09 (15) |
| C3A—Si1A—C2A | 111.98 (15) | C3B—Si1B—C4B | 112.00 (13) |
| S1A—N1A—Si1A | 127.83 (14) | S1B—N1B—Si1B | 128.59 (14) |
| S1A—N1A—H1NA | 112 (2) | S1B—N1B—H1NB | 109 (2) |
| Si1A—N1A—H1NA | 120 (2) | Si1B—N1B—H1NB | 122 (2) |
| S1A—C1A—H1AA | 109.5 | S1B—C1B—H1BA | 109.5 |
| S1A—C1A—H1AB | 109.5 | S1B—C1B—H1BB | 109.5 |
| H1AA—C1A—H1AB | 109.5 | H1BA—C1B—H1BB | 109.5 |
| S1A—C1A—H1AC | 109.5 | S1B—C1B—H1BC | 109.5 |
| H1AA—C1A—H1AC | 109.5 | H1BA—C1B—H1BC | 109.5 |
| H1AB—C1A—H1AC | 109.5 | H1BB—C1B—H1BC | 109.5 |
| Si1A—C2A—H2AA | 109.5 | Si1B—C2B—H2BA | 109.5 |
| Si1A—C2A—H2AB | 109.5 | Si1B—C2B—H2BB | 109.5 |
| H2AA—C2A—H2AB | 109.5 | H2BA—C2B—H2BB | 109.5 |
| Si1A—C2A—H2AC | 109.5 | Si1B—C2B—H2BC | 109.5 |
| H2AA—C2A—H2AC | 109.5 | H2BA—C2B—H2BC | 109.5 |
| H2AB—C2A—H2AC | 109.5 | H2BB—C2B—H2BC | 109.5 |
| Si1A—C3A—H3AA | 109.5 | Si1B—C3B—H3BA | 109.5 |
| Si1A—C3A—H3AB | 109.5 | Si1B—C3B—H3BB | 109.5 |
| H3AA—C3A—H3AB | 109.5 | H3BA—C3B—H3BB | 109.5 |
| Si1A—C3A—H3AC | 109.5 | Si1B—C3B—H3BC | 109.5 |
| H3AA—C3A—H3AC | 109.5 | H3BA—C3B—H3BC | 109.5 |
| H3AB—C3A—H3AC | 109.5 | H3BB—C3B—H3BC | 109.5 |
| Si1A—C4A—H4AA | 109.5 | Si1B—C4B—H4BA | 109.5 |
| Si1A—C4A—H4AB | 109.5 | Si1B—C4B—H4BB | 109.5 |
| H4AA—C4A—H4AB | 109.5 | H4BA—C4B—H4BB | 109.5 |
| Si1A—C4A—H4AC | 109.5 | Si1B—C4B—H4BC | 109.5 |
| H4AA—C4A—H4AC | 109.5 | H4BA—C4B—H4BC | 109.5 |
| H4AB—C4A—H4AC | 109.5 | H4BB—C4B—H4BC | 109.5 |
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1B—H1NB···O2A | 0.81 (2) | 2.11 (2) | 2.917 (3) | 173 (3) |
| N1A—H1NA···O2Bi | 0.81 (2) | 2.12 (2) | 2.925 (3) | 177 (3) |
Symmetry codes: (i) x, y, z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: SI2314).
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 global, I. DOI: 10.1107/S1600536810050336/si2314sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536810050336/si2314Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report


