research communications
N,N-dimethyl-2-[(4-methylbenzyl)sulfonyl]ethanamine
ofaWestchem, Department of Pure & Applied Chemistry, University of Strathclyde, 295 Cathedral Street, Glasgow G1 1XL, Scotland
*Correspondence e-mail: fraser.j.scott@strath.ac.uk
In the crystal, the title compound, C12H19NO2S, has a disordered structure with two equally populated conformations of the amine fragment. A pair of weak C—H⋯O intermolecular interactions between the CH2 and SO2 groups gives a one-dimensional supramolecular structure that propagates through translation along the a-axis direction.
CCDC reference: 1403422
1. Chemical context
Parasitic helminths possess a number of evolutionary strategies that facilitate their co-existence with their host and, as such, up to one third of the global population may suffer from helminthetic infections (de Silva et al., 2003). These parasites can secrete immunomodulatory molecules that prevent the parasites' clearance from the host without leaving the host vulnerable to opportunistic infections (Hewitson et al., 2009). ES-62 is one such immunomodulatory molecule, a protein, which was discovered in the secretions of the rodent filarial nematode Acanthocheilonema and demonstrated to induce an anti-inflammatory immunological phenotype (Harnett et al., 1989). ES-62 has been studied for its potential to treat human diseases relating to inflammation, for example collagen-induced arthritis or rheumatoid arthritis, and many positive outcomes have been demonstrated.
A number of the significant anti-inflammatory activities of ES-62 are associated with post-translational glycosylation and subsequent esterification by phosphorylcholine. However, ES-62 is an immunogenic protein and is thus unsuitable as a drug itself (Harnett & Harnett, 2009). We have sought to capitalize on the immunomodulatory effects of ES-62 whilst avoiding its inherent undrugability through synthesizing a library of drug-like small molecules based upon phosphorylcholine, the active moiety of ES-62. A series of sulfone analogues (Fig. 1) have proven to be of great significance in our investigations into collagen-induced arthritis. Despite the apparent simplicity of these molecules, we are aware of no relevant crystallographic study. As such, and as the title compound is of particular interest to our ongoing work (Al-Riyami et al., 2013), we report herein on the solid-state structure of the title compound.
2. Structural commentary
The molecular structure of the title compound is shown in Fig. 2. The amine group is disordered over two equally occupied sites such that the lone pair of the pyramidal N atom is anti to O1 with respect to the plane defined by C1—S1—C9 for the conformer containing N1 but syn for the N1A conformer.
3. Supramolecular features
Neighbouring molecules related by translation along the a-axis direction are connected by two weak C—H⋯O hydrogen bonds involving O1 and C1 and C9/C9A (Table 1 and Fig. 3). This gives one-dimensional supramolecular chains of molecules that propagate parallel to the crystallographic a-axis direction.
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Other close interactions involve the disordered fragment. Thus the methyl group of C11A approaches the aromatic ring, giving a C—ċπ interaction [closest contact C6⋯C11A = 3.345 (5) Å] whilst C11 forms unfeasibly short intermolecular interactions with its centrosymmetrically related self – an interaction that is relieved by the observed disorder.
4. Synthesis and crystallization
A mixture of 2-[(4-methylbenzyl)sulfonyl]ethyl methanesulfonate and 1-methyl-4-[(vinylsulfonyl)methyl]benzene (4.880 g) was dissolved in dichloromethane (50 ml, dry) to which dimethylamine (4 ml, 2M in THF) was added at room temperature with stirring. The stirring was continued at room temperature overnight. The reaction mixture was extracted with a of sodium carbonate. The organic layer was collected, dried over MgSO4, filtered and the solvents were removed under reduced pressure and the crude product was applied to a silica gel using first ethyl acetate/n-hexane (1/1, RF = 0.1) and then ethyl acetate/methanol (9/1). The product was obtained as a white solid which was recrystallized from ethyl acetate/n-hexane (2.200 g) (m.p. 341–343 K). HRESIMS: calculated for C12H19NO2S, 241.1136; found: 241.1139.
5. Refinement
Crystal data, data collection and structure . Models where the site occupancy factors of the disordered groups were allowed to refine gave occupancies equal to 50%. So in the final model, occupancies of all the disordered atoms were set to this value. The C9—C10 and C9A—C10A distances were restrained to be 1.53 (1) Å. All H atoms were placed in idealized positions and were refined in riding modes with C—H equal to 0.95, 0.98 and 0.99 Å for CH, CH2 and CH3 groups, respectively, and Uiso(H) = 1.5Ueq(C) for methyl groups and 1.2Ueq(C) for all other groups.
details are summarized in Table 2Supporting information
CCDC reference: 1403422
10.1107/S2056989015010233/is5399sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S2056989015010233/is5399Isup2.hkl
Supporting information file. DOI: 10.1107/S2056989015010233/is5399Isup3.cml
Parasitic helminths possess a number of evolutionary strategies that facilitate their co-existence with their host and, as such, up to one third of the global population may suffer from helminthetic infections (de Silva et al., 2003). These parasites can secrete immunomodulatory molecules that prevent the parasites' clearance from the host without leaving the host vulnerable to opportunistic infections (Hewitson et al., 2009). ES-62 is one such immunomodulatory molecule, a protein, which was discovered in the secretions of the rodent filarial nematode Acanthocheilonema and demonstrated to induce an anti-inflammatory immunological phenotype (Harnett et al., 1989). ES-62 has been studied for its potential to treat human diseases relating to inflammation, for example collagen-induced arthritis or rheumatoid arthritis, and many positive outcomes have been demonstrated. A number of the significant anti-inflammatory activities of ES-62 are associated with post-translational glycosylation and subsequent esterification by phosphorylcholine. However, ES-62 is an immunogenic protein and is thus unsuitable as a drug itself (Harnett & Harnett, 2009). We have sought to capitalize on the immunomodulatory effects of ES-62 whilst avoiding its inherent undrugability through synthesizing a library of drug-like small molecules based upon phosphorylcholine, the active moiety of ES-62. A series of sulfone analogues (Fig. 1) have proven to be of great significance in our investigations into collagen-induced arthritis. Despite the apparent simplicity of these molecules, we are aware of no relevant crystallographic study. As such, and as the title compound is of particular interest to our ongoing work (Al-Riyami et al., 2013), we report herein on the solid-state structure of the title compound.
The molecular structure of the title compound is shown in Fig. 2. The amine group is disordered over two equally occupied sites such that the lone pair of the pyramidal N atom is anti to O1 with respect to the plane defined by C1—S1—C9 for the conformer containing N1 but syn for the N1A conformer.
Neighbouring molecules related by translation along the a-axis direction are connected by two weak C—H···O hydrogen bonds involving O1 and C1 and C9/C9A (Table 1 and Fig. 3). This gives one-dimensional supramolecular chains of molecules that propagate parallel to the crystallographic a-axis direction.
Other close interactions involve the disordered fragment. Thus the methyl group of C11A approaches the aromatic ring in a π geometry [closest contact C6···C11A = 3.345 (5) Å] whilst C11 forms unfeasibly short intermolecular interactions with its centrosymmetrically related self – an interaction that is relieved by the observed disorder.
A mixture of 2-[(4-methylbenzyl)sulfonyl]ethyl methanesulfonate and 1-methyl-4-[(vinylsulfonyl)methyl]benzene (4.880 g) was dissolved in dichloromethane (50 ml, dry) to which dimethylamine (4 ml, 2M in THF) was added at room temperature with stirring. The stirring was continued at room temperature overnight. The reaction mixture was extracted with a
of sodium carbonate. The organic layer was collected, dried over MgSO4, filtered and the solvents were removed under reduced pressure and the crude product was applied to a silica gel using first ethyl acetate/n-hexane (1/1, RF = 0.1) and then ethyl acetate/methanol (9/1). The product was obtained as a white solid which was recrystallized from ethyl acetate/n-hexane (2.200 g) (m.p. 341–343 K). HRESIMS: calculated for C12H19NO2S, 241.1136; found: 241.1139.Crystal data, data collection and structure
details are summarized in Table 2. Models where the site occupancy factors of the disordered groups were allowed to refine gave occupancies equal to 50%. So in the final model, occupancies of all the disordered atoms were set to this value. The C9—C10 and C9A—C10A distances were restrained to be 1.53 (1) Å. All H atoms were placed in idealized positions and were refined in riding modes with C—H equal to 0.95, 0.98 and 0.99 Å for CH, CH2 and CH3 groups, respectively, and Uiso(H) = 1.5Ueq(C) for methyl groups and 1.2Ueq(C) for other groups.Data collection: CrysAlis PRO (Oxford Diffraction, 2009); cell
CrysAlis PRO (Oxford Diffraction, 2009); data reduction: CrysAlis PRO (Oxford Diffraction, 2009); program(s) used to solve structure: SIR92 (Altomare et al., 1994); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012) and Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).Fig. 1. General structure of sulfone analogues. R represents alkyl chains and X represents halogen substituents. | |
Fig. 2. The molecular structure of the title compound with non-H atoms shown as 50% probability ellipsoids. For the disordered fragment, the atoms labelled with the suffix `a' have been shown with hollow bonds whilst all other bonds are shown as solid lines. | |
Fig. 3. Part of the molecular chain formed by translation along a highlighting the C—H···O contacts. Only one of the two disordered conformations is shown. |
C12H19NO2S | Z = 2 |
Mr = 241.34 | F(000) = 260 |
Triclinic, P1 | Dx = 1.252 Mg m−3 |
Hall symbol: -P 1 | Cu Kα radiation, λ = 1.54180 Å |
a = 5.3642 (3) Å | Cell parameters from 3570 reflections |
b = 10.3773 (6) Å | θ = 5.2–72.9° |
c = 12.1784 (7) Å | µ = 2.14 mm−1 |
α = 99.572 (5)° | T = 123 K |
β = 95.498 (5)° | Plate, colourless |
γ = 104.645 (5)° | 0.30 × 0.10 × 0.03 mm |
V = 639.98 (6) Å3 |
Oxford Diffraction Gemini S diffractometer | 2491 independent reflections |
Radiation source: fine-focus sealed tube | 2360 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.023 |
ω scans | θmax = 72.9°, θmin = 3.7° |
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) | h = −4→6 |
Tmin = 0.459, Tmax = 0.938 | k = −12→11 |
5846 measured reflections | l = −15→14 |
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)] = 0.043 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.121 | H-atom parameters constrained |
S = 1.08 | w = 1/[σ2(Fo2) + (0.0758P)2 + 0.2621P] where P = (Fo2 + 2Fc2)/3 |
2491 reflections | (Δ/σ)max < 0.001 |
186 parameters | Δρmax = 0.48 e Å−3 |
2 restraints | Δρmin = −0.35 e Å−3 |
C12H19NO2S | γ = 104.645 (5)° |
Mr = 241.34 | V = 639.98 (6) Å3 |
Triclinic, P1 | Z = 2 |
a = 5.3642 (3) Å | Cu Kα radiation |
b = 10.3773 (6) Å | µ = 2.14 mm−1 |
c = 12.1784 (7) Å | T = 123 K |
α = 99.572 (5)° | 0.30 × 0.10 × 0.03 mm |
β = 95.498 (5)° |
Oxford Diffraction Gemini S diffractometer | 2491 independent reflections |
Absorption correction: multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) | 2360 reflections with I > 2σ(I) |
Tmin = 0.459, Tmax = 0.938 | Rint = 0.023 |
5846 measured reflections |
R[F2 > 2σ(F2)] = 0.043 | 2 restraints |
wR(F2) = 0.121 | H-atom parameters constrained |
S = 1.08 | Δρmax = 0.48 e Å−3 |
2491 reflections | Δρmin = −0.35 e Å−3 |
186 parameters |
Experimental. 1H NMR (DMSO-d6): δ 7.28 (2H, d, J = 8.0 Hz), 7.21 (2H, d, J = 8.0 Hz), 4.44 (2H, s), 3.17 (2H, t, J = 14.3 Hz), 2.65 (2H, t, J = 14.3 Hz), 2.31 (3H, s), 2.16 (6H, s). 13C NMR (DMSO-d6): δ 137.7, 130.8, 129.0, 125.4, 58.4, 51.6, 49.0, 44.9, 20.7. IR (KBr): 1511, 1463, 1399, 1380, 1314, 1258, 1156, 1119, 1050, 892, 853, 822, 749 cm-1. |
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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. |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
S1 | 0.89090 (7) | 0.52015 (4) | 0.66118 (3) | 0.02154 (16) | |
O1 | 1.1289 (2) | 0.48170 (12) | 0.68167 (11) | 0.0307 (3) | |
O2 | 0.9042 (2) | 0.63679 (12) | 0.60940 (10) | 0.0295 (3) | |
C1 | 0.6462 (3) | 0.38079 (16) | 0.57471 (13) | 0.0223 (3) | |
H1A | 0.4763 | 0.4021 | 0.5740 | 0.027* | |
H1B | 0.6866 | 0.3706 | 0.4966 | 0.027* | |
C2 | 0.6217 (3) | 0.24813 (16) | 0.61229 (13) | 0.0211 (3) | |
C3 | 0.7832 (3) | 0.16706 (17) | 0.57982 (14) | 0.0252 (4) | |
H3 | 0.9114 | 0.1961 | 0.5338 | 0.030* | |
C4 | 0.7579 (3) | 0.04422 (17) | 0.61421 (14) | 0.0259 (4) | |
H4 | 0.8692 | −0.0101 | 0.5912 | 0.031* | |
C5 | 0.5729 (3) | −0.00109 (17) | 0.68174 (14) | 0.0262 (4) | |
C6 | 0.4119 (4) | 0.08042 (18) | 0.71320 (16) | 0.0300 (4) | |
H6 | 0.2838 | 0.0513 | 0.7592 | 0.036* | |
C7 | 0.4342 (3) | 0.20319 (17) | 0.67902 (14) | 0.0253 (4) | |
H7 | 0.3211 | 0.2568 | 0.7012 | 0.030* | |
C8 | 0.5437 (4) | −0.13542 (19) | 0.71811 (18) | 0.0377 (5) | |
H8A | 0.5787 | −0.1201 | 0.8004 | 0.057* | |
H8B | 0.6676 | −0.1802 | 0.6856 | 0.057* | |
H8C | 0.3659 | −0.1933 | 0.6920 | 0.057* | |
C9 | 0.7696 (3) | 0.55043 (17) | 0.79112 (14) | 0.0248 (4) | 0.50 |
H9A | 0.5883 | 0.5562 | 0.7768 | 0.030* | 0.50 |
H9B | 0.7692 | 0.4741 | 0.8304 | 0.030* | 0.50 |
N1 | 0.8311 (7) | 0.7301 (3) | 0.9652 (3) | 0.0333 (7) | 0.50 |
C10 | 0.9410 (19) | 0.6837 (8) | 0.8655 (9) | 0.0264 (18) | 0.50 |
H10A | 1.1132 | 0.6711 | 0.8900 | 0.032* | 0.50 |
H10B | 0.9689 | 0.7554 | 0.8200 | 0.032* | 0.50 |
C11 | 0.9697 (14) | 0.8715 (5) | 1.0135 (4) | 0.0648 (15) | 0.50 |
H11A | 0.8822 | 0.9060 | 1.0743 | 0.097* | 0.50 |
H11B | 0.9707 | 0.9261 | 0.9551 | 0.097* | 0.50 |
H11C | 1.1492 | 0.8774 | 1.0435 | 0.097* | 0.50 |
C12 | 0.8399 (16) | 0.6456 (6) | 1.0475 (5) | 0.0683 (18) | 0.50 |
H12A | 0.7464 | 0.5512 | 1.0134 | 0.102* | 0.50 |
H12B | 0.7577 | 0.6770 | 1.1114 | 0.102* | 0.50 |
H12C | 1.0216 | 0.6513 | 1.0737 | 0.102* | 0.50 |
N1A | 0.9175 (6) | 0.6553 (3) | 0.9889 (3) | 0.0297 (7) | 0.50 |
C9A | 0.7696 (3) | 0.55043 (17) | 0.79112 (14) | 0.0248 (4) | 0.50 |
H9C | 0.6106 | 0.5813 | 0.7797 | 0.030* | 0.50 |
H9D | 0.7240 | 0.4654 | 0.8207 | 0.030* | 0.50 |
C10A | 0.9780 (18) | 0.6589 (8) | 0.8749 (8) | 0.0231 (17) | 0.50 |
H10C | 1.1504 | 0.6423 | 0.8688 | 0.028* | 0.50 |
H10D | 0.9848 | 0.7496 | 0.8578 | 0.028* | 0.50 |
C11A | 1.1294 (9) | 0.7511 (4) | 1.0688 (3) | 0.0394 (9) | 0.50 |
H11D | 1.2931 | 0.7284 | 1.0582 | 0.059* | 0.50 |
H11E | 1.0940 | 0.7461 | 1.1457 | 0.059* | 0.50 |
H11F | 1.1434 | 0.8434 | 1.0563 | 0.059* | 0.50 |
C12A | 0.6727 (9) | 0.6851 (5) | 1.0055 (4) | 0.0424 (10) | 0.50 |
H12D | 0.6451 | 0.6851 | 1.0839 | 0.064* | 0.50 |
H12E | 0.5301 | 0.6158 | 0.9554 | 0.064* | 0.50 |
H12F | 0.6772 | 0.7746 | 0.9884 | 0.064* | 0.50 |
U11 | U22 | U33 | U12 | U13 | U23 | |
S1 | 0.0207 (2) | 0.0219 (2) | 0.0214 (2) | 0.00508 (16) | 0.00401 (15) | 0.00319 (16) |
O1 | 0.0228 (6) | 0.0307 (7) | 0.0357 (7) | 0.0074 (5) | 0.0033 (5) | −0.0006 (5) |
O2 | 0.0357 (7) | 0.0258 (6) | 0.0264 (6) | 0.0050 (5) | 0.0073 (5) | 0.0071 (5) |
C1 | 0.0221 (8) | 0.0237 (8) | 0.0190 (7) | 0.0053 (6) | 0.0001 (6) | 0.0018 (6) |
C2 | 0.0199 (7) | 0.0219 (8) | 0.0182 (7) | 0.0031 (6) | −0.0027 (6) | 0.0016 (6) |
C3 | 0.0220 (8) | 0.0285 (9) | 0.0240 (8) | 0.0066 (7) | 0.0043 (6) | 0.0018 (7) |
C4 | 0.0231 (8) | 0.0255 (8) | 0.0267 (8) | 0.0084 (6) | −0.0005 (6) | −0.0011 (7) |
C5 | 0.0261 (8) | 0.0231 (8) | 0.0258 (8) | 0.0039 (6) | −0.0023 (6) | 0.0031 (6) |
C6 | 0.0275 (9) | 0.0309 (9) | 0.0327 (9) | 0.0060 (7) | 0.0102 (7) | 0.0094 (7) |
C7 | 0.0218 (8) | 0.0274 (8) | 0.0265 (8) | 0.0079 (7) | 0.0041 (6) | 0.0029 (7) |
C8 | 0.0437 (11) | 0.0273 (9) | 0.0433 (11) | 0.0098 (8) | 0.0056 (9) | 0.0110 (8) |
C9 | 0.0252 (8) | 0.0284 (8) | 0.0200 (8) | 0.0062 (7) | 0.0042 (6) | 0.0043 (6) |
N1 | 0.045 (2) | 0.0337 (17) | 0.0244 (16) | 0.0202 (16) | 0.0042 (15) | 0.0002 (13) |
C10 | 0.024 (3) | 0.034 (3) | 0.022 (3) | 0.013 (2) | −0.0005 (19) | 0.001 (2) |
C11 | 0.106 (5) | 0.042 (3) | 0.037 (2) | 0.017 (3) | 0.006 (3) | −0.011 (2) |
C12 | 0.121 (6) | 0.066 (4) | 0.033 (3) | 0.045 (4) | 0.025 (3) | 0.016 (3) |
N1A | 0.0366 (17) | 0.0302 (17) | 0.0197 (17) | 0.0083 (14) | −0.0003 (13) | 0.0013 (13) |
C9A | 0.0252 (8) | 0.0284 (8) | 0.0200 (8) | 0.0062 (7) | 0.0042 (6) | 0.0043 (6) |
C10A | 0.023 (3) | 0.027 (3) | 0.019 (2) | 0.009 (2) | −0.0031 (18) | 0.003 (2) |
C11A | 0.046 (2) | 0.040 (2) | 0.0253 (18) | 0.0098 (18) | −0.0103 (16) | −0.0028 (16) |
C12A | 0.046 (2) | 0.053 (3) | 0.028 (2) | 0.020 (2) | 0.0083 (19) | −0.0024 (18) |
S1—O1 | 1.4426 (13) | C9—H9B | 0.9900 |
S1—O2 | 1.4446 (12) | N1—C12 | 1.442 (6) |
S1—C9 | 1.7780 (16) | N1—C11 | 1.460 (6) |
S1—C1 | 1.7867 (16) | N1—C10 | 1.462 (12) |
C1—C2 | 1.501 (2) | C10—H10A | 0.9900 |
C1—H1A | 0.9900 | C10—H10B | 0.9900 |
C1—H1B | 0.9900 | C11—H11A | 0.9800 |
C2—C7 | 1.391 (2) | C11—H11B | 0.9800 |
C2—C3 | 1.392 (2) | C11—H11C | 0.9800 |
C3—C4 | 1.386 (2) | C12—H12A | 0.9800 |
C3—H3 | 0.9500 | C12—H12B | 0.9800 |
C4—C5 | 1.390 (3) | C12—H12C | 0.9800 |
C4—H4 | 0.9500 | N1A—C12A | 1.448 (6) |
C5—C6 | 1.390 (2) | N1A—C11A | 1.457 (5) |
C5—C8 | 1.507 (2) | N1A—C10A | 1.460 (12) |
C6—C7 | 1.385 (2) | C10A—H10C | 0.9900 |
C6—H6 | 0.9500 | C10A—H10D | 0.9900 |
C7—H7 | 0.9500 | C11A—H11D | 0.9800 |
C8—H8A | 0.9800 | C11A—H11E | 0.9800 |
C8—H8B | 0.9800 | C11A—H11F | 0.9800 |
C8—H8C | 0.9800 | C12A—H12D | 0.9800 |
C9—C10 | 1.536 (7) | C12A—H12E | 0.9800 |
C9—H9A | 0.9900 | C12A—H12F | 0.9800 |
O1—S1—O2 | 117.10 (8) | H8B—C8—H8C | 109.5 |
O1—S1—C9 | 108.51 (8) | C10—C9—S1 | 109.9 (5) |
O2—S1—C9 | 108.29 (8) | C10—C9—H9A | 109.7 |
O1—S1—C1 | 109.89 (7) | S1—C9—H9A | 109.7 |
O2—S1—C1 | 107.22 (7) | C10—C9—H9B | 109.7 |
C9—S1—C1 | 105.17 (8) | S1—C9—H9B | 109.7 |
C2—C1—S1 | 113.98 (11) | H9A—C9—H9B | 108.2 |
C2—C1—H1A | 108.8 | C12—N1—C11 | 110.8 (4) |
S1—C1—H1A | 108.8 | C12—N1—C10 | 111.7 (5) |
C2—C1—H1B | 108.8 | C11—N1—C10 | 109.5 (5) |
S1—C1—H1B | 108.8 | N1—C10—C9 | 113.9 (8) |
H1A—C1—H1B | 107.7 | N1—C10—H10A | 108.8 |
C7—C2—C3 | 118.87 (15) | C9—C10—H10A | 108.8 |
C7—C2—C1 | 120.38 (14) | N1—C10—H10B | 108.8 |
C3—C2—C1 | 120.74 (14) | C9—C10—H10B | 108.8 |
C4—C3—C2 | 120.35 (15) | H10A—C10—H10B | 107.7 |
C4—C3—H3 | 119.8 | C12A—N1A—C11A | 110.2 (3) |
C2—C3—H3 | 119.8 | C12A—N1A—C10A | 112.8 (4) |
C3—C4—C5 | 121.28 (15) | C11A—N1A—C10A | 109.0 (4) |
C3—C4—H4 | 119.4 | N1A—C10A—H10C | 109.8 |
C5—C4—H4 | 119.4 | N1A—C10A—H10D | 109.8 |
C4—C5—C6 | 117.86 (16) | H10C—C10A—H10D | 108.2 |
C4—C5—C8 | 121.24 (16) | N1A—C11A—H11D | 109.5 |
C6—C5—C8 | 120.90 (16) | N1A—C11A—H11E | 109.5 |
C7—C6—C5 | 121.50 (16) | H11D—C11A—H11E | 109.5 |
C7—C6—H6 | 119.3 | N1A—C11A—H11F | 109.5 |
C5—C6—H6 | 119.3 | H11D—C11A—H11F | 109.5 |
C6—C7—C2 | 120.15 (15) | H11E—C11A—H11F | 109.5 |
C6—C7—H7 | 119.9 | N1A—C12A—H12D | 109.5 |
C2—C7—H7 | 119.9 | N1A—C12A—H12E | 109.5 |
C5—C8—H8A | 109.5 | H12D—C12A—H12E | 109.5 |
C5—C8—H8B | 109.5 | N1A—C12A—H12F | 109.5 |
H8A—C8—H8B | 109.5 | H12D—C12A—H12F | 109.5 |
C5—C8—H8C | 109.5 | H12E—C12A—H12F | 109.5 |
H8A—C8—H8C | 109.5 | ||
O1—S1—C1—C2 | 47.30 (14) | C8—C5—C6—C7 | −179.06 (16) |
O2—S1—C1—C2 | 175.57 (11) | C5—C6—C7—C2 | −0.4 (3) |
C9—S1—C1—C2 | −69.31 (13) | C3—C2—C7—C6 | 0.7 (2) |
S1—C1—C2—C7 | 96.45 (16) | C1—C2—C7—C6 | 179.81 (14) |
S1—C1—C2—C3 | −84.47 (17) | O1—S1—C9—C10 | 72.2 (3) |
C7—C2—C3—C4 | −0.4 (2) | O2—S1—C9—C10 | −55.9 (3) |
C1—C2—C3—C4 | −179.51 (14) | C1—S1—C9—C10 | −170.2 (3) |
C2—C3—C4—C5 | −0.2 (3) | C12—N1—C10—C9 | 71.5 (7) |
C3—C4—C5—C6 | 0.5 (3) | C11—N1—C10—C9 | −165.3 (5) |
C3—C4—C5—C8 | 179.36 (16) | S1—C9—C10—N1 | 169.5 (4) |
C4—C5—C6—C7 | −0.2 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1A···O1i | 0.99 | 2.60 | 3.493 (2) | 150 |
C9—H9A···O1i | 0.99 | 2.49 | 3.415 (2) | 155 |
C9A—H9C···O1i | 0.99 | 2.61 | 3.415 (2) | 138 |
Symmetry code: (i) x−1, y, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1A···O1i | 0.99 | 2.60 | 3.493 (2) | 150 |
C9—H9A···O1i | 0.99 | 2.49 | 3.415 (2) | 155 |
C9A—H9C···O1i | 0.99 | 2.61 | 3.415 (2) | 138 |
Symmetry code: (i) x−1, y, z. |
Experimental details
Crystal data | |
Chemical formula | C12H19NO2S |
Mr | 241.34 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 123 |
a, b, c (Å) | 5.3642 (3), 10.3773 (6), 12.1784 (7) |
α, β, γ (°) | 99.572 (5), 95.498 (5), 104.645 (5) |
V (Å3) | 639.98 (6) |
Z | 2 |
Radiation type | Cu Kα |
µ (mm−1) | 2.14 |
Crystal size (mm) | 0.30 × 0.10 × 0.03 |
Data collection | |
Diffractometer | Oxford Diffraction Gemini S diffractometer |
Absorption correction | Multi-scan (CrysAlis PRO; Oxford Diffraction, 2009) |
Tmin, Tmax | 0.459, 0.938 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 5846, 2491, 2360 |
Rint | 0.023 |
(sin θ/λ)max (Å−1) | 0.620 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.043, 0.121, 1.08 |
No. of reflections | 2491 |
No. of parameters | 186 |
No. of restraints | 2 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.48, −0.35 |
Computer programs: CrysAlis PRO (Oxford Diffraction, 2009), SIR92 (Altomare et al., 1994), SHELXL97 (Sheldrick, 2008), ORTEP-3 for Windows (Farrugia, 2012) and Mercury (Macrae et al., 2008).
References
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