Abstract
In the crystal structure of the title compound, C14H15NO2S, the amino H atom is trans to one of the O atoms of the SO2 group. Furthermore, the N—H bond is anti to the ortho- and meta-methyl groups of the aromatic ring. The two aromatic rings are tilted relative to each other by 64.8 (1)°. The molecules form zigzag chains along the a axis via intermolecular N—H⋯O hydrogen bonds.
Related literature
For related literature, see: Gelbrich et al. (2007 ▶); Gowda et al. (2005 ▶); Gowda et al. (2008a
▶,b
▶,c
▶); Perlovich et al. (2006 ▶).
Experimental
Crystal data
C14H15NO2S
M r = 261.33
Orthorhombic,
a = 6.3969 (5) Å
b = 8.8767 (6) Å
c = 23.082 (2) Å
V = 1310.67 (18) Å3
Z = 4
Mo Kα radiation
μ = 0.24 mm−1
T = 299 (2) K
0.50 × 0.30 × 0.18 mm
Data collection
Oxford Diffraction Xcalibur diffractometer with Sapphire CCD detector
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2007 ▶) T min = 0.889, T max = 0.958
5869 measured reflections
2611 independent reflections
2200 reflections with I > 2σ(I)
R int = 0.014
Refinement
R[F 2 > 2σ(F 2)] = 0.034
wR(F 2) = 0.094
S = 1.07
2611 reflections
168 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.20 e Å−3
Δρmin = −0.19 e Å−3
Absolute structure: Flack (1983 ▶), 1060 Friedel pairs
Flack parameter: −0.04 (9)
Data collection: CrysAlis CCD (Oxford Diffraction, 2004 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2007 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2003 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809002098/bt2853sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809002098/bt2853Isup2.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 |
---|---|---|---|---|
N1—H1N⋯O2i | 0.84 (3) | 2.10 (3) | 2.936 (2) | 176 (2) |
Symmetry code: (i) .
Acknowledgments
BTG thanks the Alexander von Humboldt Foundation, Bonn, Germany, for extensions of his research fellowship.
supplementary crystallographic information
Comment
In the present work, as part of a study of the substituent effects on the crystal structures of N-(aryl)-arylsulfonamides (Gowda et al., 2008a, 2008b, 2008c), the structure of N-(2,3-dimethylphenyl)-benzenesulfonamide has been determined. The amino H atom is trans to one of the O atoms of the SO2 group (Fig. 1), similar to that observed in N-(2,6-dimethylphenyl)- benzenesulfonamide (Gowda et al., 2008a), N-(2-methylphenyl)-benzenesulfonamide (Gowda et al., 2008b) and other aryl sulfonamides (Perlovich et al., 2006; Gelbrich et al., 2007; Gowda et al., 2008c). The two benzene rings are tilted relative to each other by 64.8 (1)°, compared with the values of 44.9 (1)° in N-(2,6-dimethylphenyl)- benzenesulfonamide and 61.5 (1)° in N-(2-methylphenyl)-benzenesulfonamide. The other bond parameters of the title compound are similar to those observed in other N-(aryl)-sulfonamides. The crystal packing is stabilized by intermolecular N—H···O hydrogen bonds forming zigzag chains along the a axis (Table 1, Fig. 2).
Experimental
The solution of benzene (10 cc) in chloroform (40 cc) was treated dropwise with chlorosulfonic acid (25 cc) at 0 ° C. After the initial evolution of hydrogen chloride subsided, the reaction mixture was brought to room temperature and poured into crushed ice in a beaker. The chloroform layer was separated, washed with cold water and allowed to evaporate slowly. The residual benzenesulfonylchloride was treated with 2,3-dimethylaniline in the stoichiometric ratio and boiled for ten minutes. The reaction mixture was then cooled to room temperature and added to ice cold water (100 cc). The resultant solid N-(2,3-dimethylphenyl)-benzenesulfonamide was filtered under suction and washed thoroughly with cold water. It was then recrystallized to constant melting point from dilute ethanol. The purity of the compound was checked and characterized by recording its infrared and NMR spectra (Gowda et al., 2005). The single crystals used in X-ray diffraction studies were grown in ethanolic solution by slow evaporation at room temperature.
Refinement
The C-bound H atoms were positioned with idealized geometry using a riding model with C—H = 0.93 or 0.96 Å. The H atom of the NH group was located in difference map, and its positional parameters were refined freely. All H atoms were refined with isotropic displacement parameters set to 1.2 times of the Ueq of the parent atom.
To improve considerably values of R1, wR2, and GOOF three reflections (0 1 1, 0 1 2, 0 1 3) were omitted from the refinement.
Figures
Fig. 1.
Molecular structure of the title compound, showing the atom labeling scheme. The displacement ellipsoids are drawn at the 50% probability level. The H atoms are represented as small spheres of arbitrary radii.
Fig. 2.
Molecular packing of the title compound with hydrogen bonding shown as dashed lines.
Crystal data
C14H15NO2S | F(000) = 552 |
Mr = 261.33 | Dx = 1.324 Mg m−3 |
Orthorhombic, P212121 | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: P 2ac 2ab | Cell parameters from 2432 reflections |
a = 6.3969 (5) Å | θ = 2.3–27.7° |
b = 8.8767 (6) Å | µ = 0.24 mm−1 |
c = 23.082 (2) Å | T = 299 K |
V = 1310.67 (18) Å3 | Rod, colourless |
Z = 4 | 0.50 × 0.30 × 0.18 mm |
Data collection
Oxford Diffraction Xcalibur diffractometer with Sapphire CCD detector | 2611 independent reflections |
Radiation source: fine-focus sealed tube | 2200 reflections with I > 2σ(I) |
graphite | Rint = 0.014 |
Rotation method data acquisition using ω and φ scans | θmax = 26.4°, θmin = 3.3° |
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2007) | h = −7→7 |
Tmin = 0.889, Tmax = 0.958 | k = −5→11 |
5869 measured reflections | l = −13→28 |
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)] = 0.034 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.094 | w = 1/[σ2(Fo2) + (0.0525P)2 + 0.1566P] where P = (Fo2 + 2Fc2)/3 |
S = 1.07 | (Δ/σ)max = 0.025 |
2611 reflections | Δρmax = 0.20 e Å−3 |
168 parameters | Δρmin = −0.19 e Å−3 |
0 restraints | Absolute structure: Flack (1983), 1060 Friedel pairs |
Primary atom site location: structure-invariant direct methods | Flack parameter: −0.04 (9) |
Special details
Experimental. CrysAlis RED (Oxford Diffraction, 2007) Empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm. |
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 | ||
C1 | 0.2823 (3) | −0.0378 (2) | 0.43543 (9) | 0.0389 (5) | |
C2 | 0.4720 (4) | −0.0422 (3) | 0.46456 (11) | 0.0507 (6) | |
H2 | 0.5124 | 0.0374 | 0.4882 | 0.061* | |
C3 | 0.5998 (4) | −0.1662 (3) | 0.45797 (13) | 0.0651 (7) | |
H3 | 0.7262 | −0.1708 | 0.4778 | 0.078* | |
C4 | 0.5424 (5) | −0.2816 (3) | 0.42263 (14) | 0.0701 (9) | |
H4 | 0.6285 | −0.3655 | 0.4189 | 0.084* | |
C5 | 0.3566 (6) | −0.2746 (3) | 0.39226 (13) | 0.0740 (9) | |
H5 | 0.3206 | −0.3519 | 0.3670 | 0.089* | |
C6 | 0.2245 (5) | −0.1532 (3) | 0.39934 (11) | 0.0564 (6) | |
H6 | 0.0974 | −0.1496 | 0.3798 | 0.068* | |
C7 | 0.2683 (4) | 0.2922 (2) | 0.36164 (9) | 0.0419 (5) | |
C8 | 0.1257 (4) | 0.3805 (2) | 0.33190 (9) | 0.0441 (5) | |
C9 | 0.1664 (4) | 0.4088 (3) | 0.27267 (10) | 0.0536 (6) | |
C10 | 0.3383 (5) | 0.3483 (3) | 0.24667 (12) | 0.0701 (8) | |
H10 | 0.3632 | 0.3679 | 0.2077 | 0.084* | |
C11 | 0.4762 (5) | 0.2585 (3) | 0.27715 (13) | 0.0757 (9) | |
H11 | 0.5909 | 0.2167 | 0.2583 | 0.091* | |
C12 | 0.4452 (4) | 0.2308 (3) | 0.33475 (11) | 0.0566 (7) | |
H12 | 0.5395 | 0.1724 | 0.3557 | 0.068* | |
C13 | −0.0598 (4) | 0.4452 (3) | 0.36156 (12) | 0.0601 (7) | |
H13A | −0.0457 | 0.5528 | 0.3637 | 0.072* | |
H13B | −0.0697 | 0.4045 | 0.4000 | 0.072* | |
H13C | −0.1837 | 0.4203 | 0.3402 | 0.072* | |
C14 | 0.0210 (6) | 0.5071 (4) | 0.23845 (14) | 0.0840 (10) | |
H14A | 0.0214 | 0.6070 | 0.2544 | 0.101* | |
H14B | −0.1179 | 0.4664 | 0.2402 | 0.101* | |
H14C | 0.0665 | 0.5108 | 0.1988 | 0.101* | |
N1 | 0.2351 (3) | 0.2670 (2) | 0.42314 (7) | 0.0413 (5) | |
H1N | 0.337 (4) | 0.290 (3) | 0.4439 (10) | 0.050* | |
O1 | −0.0648 (3) | 0.09633 (19) | 0.41129 (7) | 0.0567 (5) | |
O2 | 0.0967 (3) | 0.13781 (18) | 0.50761 (6) | 0.0577 (5) | |
S1 | 0.11619 (8) | 0.11797 (6) | 0.44610 (2) | 0.04071 (16) |
Atomic displacement parameters (Å2)
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0474 (12) | 0.0325 (11) | 0.0367 (11) | −0.0028 (9) | 0.0072 (10) | 0.0039 (9) |
C2 | 0.0512 (14) | 0.0446 (13) | 0.0562 (15) | 0.0015 (11) | −0.0003 (11) | 0.0037 (11) |
C3 | 0.0525 (15) | 0.0602 (15) | 0.0826 (19) | 0.0094 (13) | 0.0059 (15) | 0.0201 (14) |
C4 | 0.074 (2) | 0.0485 (16) | 0.088 (2) | 0.0167 (14) | 0.0292 (17) | 0.0089 (14) |
C5 | 0.103 (3) | 0.0439 (14) | 0.0747 (19) | −0.0003 (17) | 0.0165 (19) | −0.0139 (13) |
C6 | 0.0650 (16) | 0.0453 (14) | 0.0588 (15) | −0.0036 (13) | 0.0013 (12) | −0.0065 (11) |
C7 | 0.0453 (13) | 0.0366 (12) | 0.0437 (12) | −0.0046 (10) | −0.0013 (10) | 0.0016 (9) |
C8 | 0.0463 (11) | 0.0389 (11) | 0.0471 (11) | −0.0040 (12) | −0.0060 (10) | −0.0038 (10) |
C9 | 0.0728 (18) | 0.0463 (13) | 0.0418 (12) | −0.0153 (12) | −0.0039 (12) | 0.0044 (10) |
C10 | 0.095 (2) | 0.0610 (17) | 0.0545 (15) | −0.0060 (16) | 0.0127 (16) | 0.0077 (13) |
C11 | 0.0747 (19) | 0.0694 (19) | 0.083 (2) | 0.0123 (16) | 0.0330 (17) | 0.0058 (16) |
C12 | 0.0488 (15) | 0.0536 (15) | 0.0674 (17) | 0.0070 (12) | 0.0105 (12) | 0.0128 (12) |
C13 | 0.0515 (16) | 0.0658 (16) | 0.0631 (16) | 0.0125 (13) | 0.0018 (12) | 0.0035 (13) |
C14 | 0.089 (2) | 0.094 (2) | 0.069 (2) | −0.002 (2) | −0.0176 (18) | 0.0251 (17) |
N1 | 0.0473 (11) | 0.0380 (10) | 0.0384 (10) | −0.0017 (9) | −0.0094 (9) | −0.0001 (8) |
O1 | 0.0425 (10) | 0.0555 (11) | 0.0721 (11) | −0.0045 (8) | −0.0070 (7) | 0.0018 (8) |
O2 | 0.0708 (11) | 0.0589 (10) | 0.0432 (8) | 0.0133 (10) | 0.0158 (8) | 0.0008 (7) |
S1 | 0.0425 (3) | 0.0397 (3) | 0.0399 (3) | 0.0026 (3) | 0.0038 (2) | 0.0009 (2) |
Geometric parameters (Å, °)
C1—C6 | 1.371 (3) | C9—C10 | 1.363 (4) |
C1—C2 | 1.388 (3) | C9—C14 | 1.500 (4) |
C1—S1 | 1.762 (2) | C10—C11 | 1.381 (4) |
C2—C3 | 1.379 (4) | C10—H10 | 0.9300 |
C2—H2 | 0.9300 | C11—C12 | 1.367 (4) |
C3—C4 | 1.360 (4) | C11—H11 | 0.9300 |
C3—H3 | 0.9300 | C12—H12 | 0.9300 |
C4—C5 | 1.381 (5) | C13—H13A | 0.9600 |
C4—H4 | 0.9300 | C13—H13B | 0.9600 |
C5—C6 | 1.380 (4) | C13—H13C | 0.9600 |
C5—H5 | 0.9300 | C14—H14A | 0.9600 |
C6—H6 | 0.9300 | C14—H14B | 0.9600 |
C7—C8 | 1.385 (3) | C14—H14C | 0.9600 |
C7—C12 | 1.401 (3) | N1—S1 | 1.615 (2) |
C7—N1 | 1.453 (3) | N1—H1N | 0.84 (3) |
C8—C9 | 1.414 (3) | O1—S1 | 1.4221 (17) |
C8—C13 | 1.485 (3) | O2—S1 | 1.4362 (15) |
C6—C1—C2 | 120.6 (2) | C11—C10—H10 | 119.4 |
C6—C1—S1 | 120.57 (19) | C12—C11—C10 | 120.4 (3) |
C2—C1—S1 | 118.80 (16) | C12—C11—H11 | 119.8 |
C3—C2—C1 | 119.2 (2) | C10—C11—H11 | 119.8 |
C3—C2—H2 | 120.4 | C11—C12—C7 | 118.6 (3) |
C1—C2—H2 | 120.4 | C11—C12—H12 | 120.7 |
C4—C3—C2 | 120.4 (3) | C7—C12—H12 | 120.7 |
C4—C3—H3 | 119.8 | C8—C13—H13A | 109.5 |
C2—C3—H3 | 119.8 | C8—C13—H13B | 109.5 |
C3—C4—C5 | 120.2 (3) | H13A—C13—H13B | 109.5 |
C3—C4—H4 | 119.9 | C8—C13—H13C | 109.5 |
C5—C4—H4 | 119.9 | H13A—C13—H13C | 109.5 |
C6—C5—C4 | 120.1 (3) | H13B—C13—H13C | 109.5 |
C6—C5—H5 | 119.9 | C9—C14—H14A | 109.5 |
C4—C5—H5 | 119.9 | C9—C14—H14B | 109.5 |
C1—C6—C5 | 119.4 (3) | H14A—C14—H14B | 109.5 |
C1—C6—H6 | 120.3 | C9—C14—H14C | 109.5 |
C5—C6—H6 | 120.3 | H14A—C14—H14C | 109.5 |
C8—C7—C12 | 122.2 (2) | H14B—C14—H14C | 109.5 |
C8—C7—N1 | 118.4 (2) | C7—N1—S1 | 121.07 (14) |
C12—C7—N1 | 119.4 (2) | C7—N1—H1N | 114.0 (17) |
C7—C8—C9 | 117.3 (2) | S1—N1—H1N | 112.4 (17) |
C7—C8—C13 | 121.1 (2) | O1—S1—O2 | 120.28 (11) |
C9—C8—C13 | 121.6 (2) | O1—S1—N1 | 107.97 (10) |
C10—C9—C8 | 120.3 (2) | O2—S1—N1 | 105.37 (10) |
C10—C9—C14 | 119.8 (2) | O1—S1—C1 | 107.82 (10) |
C8—C9—C14 | 119.9 (2) | O2—S1—C1 | 106.68 (10) |
C9—C10—C11 | 121.2 (3) | N1—S1—C1 | 108.24 (9) |
C9—C10—H10 | 119.4 | ||
C6—C1—C2—C3 | −1.7 (3) | C14—C9—C10—C11 | 179.4 (3) |
S1—C1—C2—C3 | 177.83 (19) | C9—C10—C11—C12 | −1.4 (5) |
C1—C2—C3—C4 | 1.1 (4) | C10—C11—C12—C7 | 1.6 (4) |
C2—C3—C4—C5 | 1.0 (4) | C8—C7—C12—C11 | −0.5 (4) |
C3—C4—C5—C6 | −2.5 (4) | N1—C7—C12—C11 | −178.6 (2) |
C2—C1—C6—C5 | 0.2 (4) | C8—C7—N1—S1 | 95.3 (2) |
S1—C1—C6—C5 | −179.3 (2) | C12—C7—N1—S1 | −86.4 (2) |
C4—C5—C6—C1 | 1.9 (4) | C7—N1—S1—O1 | −45.5 (2) |
C12—C7—C8—C9 | −0.8 (3) | C7—N1—S1—O2 | −175.20 (17) |
N1—C7—C8—C9 | 177.31 (19) | C7—N1—S1—C1 | 70.97 (19) |
C12—C7—C8—C13 | −179.5 (2) | C6—C1—S1—O1 | −1.1 (2) |
N1—C7—C8—C13 | −1.4 (3) | C2—C1—S1—O1 | 179.35 (17) |
C7—C8—C9—C10 | 1.1 (3) | C6—C1—S1—O2 | 129.3 (2) |
C13—C8—C9—C10 | 179.7 (2) | C2—C1—S1—O2 | −50.2 (2) |
C7—C8—C9—C14 | −178.3 (2) | C6—C1—S1—N1 | −117.7 (2) |
C13—C8—C9—C14 | 0.3 (3) | C2—C1—S1—N1 | 62.79 (19) |
C8—C9—C10—C11 | 0.0 (4) |
Hydrogen-bond geometry (Å, °)
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N···O2i | 0.84 (3) | 2.10 (3) | 2.936 (2) | 176 (2) |
Symmetry codes: (i) x+1/2, −y+1/2, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: BT2853).
References
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- Oxford Diffraction (2004). CrysAlis CCD Oxford Diffraction Ltd, Köln, Germany.
- Oxford Diffraction (2007). CrysAlis RED Oxford Diffraction Ltd, Köln, Germany.
- Perlovich, G. L., Tkachev, V. V., Schaper, K.-J. & Raevsky, O. A. (2006). Acta Cryst. E62, o780–o782.
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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 I, global. DOI: 10.1107/S1600536809002098/bt2853sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809002098/bt2853Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report