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In the mol­ecule of the title compound, m-(O2N)C6H4NHSO2C6H4-p-Me or C13H12N2O4S, the planes of two benzene rings are orthogonal to each other [dihedral angle 92.4 (1)°].

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805039395/ya6269sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805039395/ya6269Isup2.hkl
Contains datablock I

CCDC reference: 296712

Key indicators

  • Single-crystal X-ray study
  • T = 293 K
  • Mean [sigma](C-C) = 0.003 Å
  • R factor = 0.043
  • wR factor = 0.147
  • Data-to-parameter ratio = 16.6

checkCIF/PLATON results

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Alert level C PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ? PLAT199_ALERT_1_C Check the Reported _cell_measurement_temperature 293 K PLAT200_ALERT_1_C Check the Reported _diffrn_ambient_temperature . 293 K
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 3 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Experimental top

The title compound was prepared according to the method of Sprague & Miller (1952). To a solution of 3-nitroaniline (27.6 g) in pyridine (100 ml) was added 4-tosyl chloride (41.8 g); the mixture was heated for 0.5 h at 373 K, then cooled to room temperature and poured into 500 ml of dilute HCl, thus yielding 4-methyl-N-(3-nitrophenyl)-benzenesulfonamide in quantitative yield. The X-ray quality crystals of the title compound (m.p. 405–407 K) were obtained by slow evaporation of its ethanol solution.

Refinement top

All H atoms were positioned geometrically and refined using a riding model, with C—H 0.93 and 0.96 Å, and Uiso(H) = 1.2Ueq(Caromatic,N) and 1.5Ueq(CMe).

Computing details top

Data collection: RAPID-AUTO (Rigaku, 1997); cell refinement: RAPID-AUTO; data reduction: RAPID-AUTO; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: please supply; software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. Molecular structure of the title compound. Displacement ellipsoids are drawn at the 30% probability level; H atoms are shown as small spheres of arbitrary radii.
[Figure 2] Fig. 2. The packing of the crystal of the title compound, projected on to the ac plane; the N—H···O bonds are shown as dashed lines. H atoms attached to C atoms have been omitted.
4-Methyl-N-(3-nitrophenyl)benzenesulfonamide top
Crystal data top
C13H12N2O4SF(000) = 608
Mr = 292.31Dx = 1.482 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -p 2ynCell parameters from 10604 reflections
a = 12.766 (3) Åθ = 3.0–27.5°
b = 7.7327 (15) ŵ = 0.26 mm1
c = 13.550 (3) ÅT = 293 K
β = 101.66 (3)°Block, light yellow
V = 1310.0 (5) Å30.29 × 0.15 × 0.07 mm
Z = 4
Data collection top
Rigaku R-AXIS RAPID
diffractometer
2997 independent reflections
Radiation source: rotating anode2519 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.029
oscillation scansθmax = 27.5°, θmin = 3.0°
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
h = 1616
Tmin = 0.928, Tmax = 0.981k = 109
12545 measured reflectionsl = 1716
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.043Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.147H-atom parameters constrained
S = 1.01 w = 1/[σ2(Fo2) + (0.1119P)2 + 0.1885P]
where P = (Fo2 + 2Fc2)/3
2997 reflections(Δ/σ)max = 0.005
181 parametersΔρmax = 0.39 e Å3
0 restraintsΔρmin = 0.44 e Å3
Crystal data top
C13H12N2O4SV = 1310.0 (5) Å3
Mr = 292.31Z = 4
Monoclinic, P21/nMo Kα radiation
a = 12.766 (3) ŵ = 0.26 mm1
b = 7.7327 (15) ÅT = 293 K
c = 13.550 (3) Å0.29 × 0.15 × 0.07 mm
β = 101.66 (3)°
Data collection top
Rigaku R-AXIS RAPID
diffractometer
2997 independent reflections
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
2519 reflections with I > 2σ(I)
Tmin = 0.928, Tmax = 0.981Rint = 0.029
12545 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0430 restraints
wR(F2) = 0.147H-atom parameters constrained
S = 1.01Δρmax = 0.39 e Å3
2997 reflectionsΔρmin = 0.44 e Å3
181 parameters
Special details top

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) top
xyzUiso*/Ueq
S10.46196 (3)0.09564 (5)0.71566 (3)0.03250 (17)
N10.62332 (12)0.2537 (2)1.10913 (11)0.0371 (4)
N20.37809 (11)0.1468 (2)0.78721 (11)0.0362 (3)
H2A0.31140.12980.76220.043*
O10.69094 (11)0.1694 (2)1.07943 (12)0.0545 (4)
O20.64034 (13)0.3258 (2)1.19147 (11)0.0551 (4)
O30.39586 (12)0.02293 (18)0.62717 (10)0.0447 (4)
O40.54622 (11)0.00586 (18)0.77295 (11)0.0426 (3)
C10.32062 (14)0.2970 (2)0.92168 (15)0.0376 (4)
H1A0.25350.30700.87990.045*
C20.33747 (16)0.3626 (3)1.01826 (16)0.0436 (4)
H2B0.28150.41641.04070.052*
C30.43667 (15)0.3495 (3)1.08235 (14)0.0383 (4)
H3A0.44870.39231.14780.046*
C40.51683 (13)0.2697 (2)1.04410 (13)0.0309 (4)
C50.50296 (13)0.2018 (2)0.94798 (13)0.0312 (4)
H5A0.55920.14830.92560.037*
C60.40289 (13)0.2159 (2)0.88594 (12)0.0302 (3)
C70.51791 (13)0.2911 (2)0.68361 (12)0.0303 (3)
C80.62626 (15)0.2973 (3)0.68341 (17)0.0440 (5)
H8A0.66940.20130.70260.053*
C90.66956 (16)0.4490 (3)0.65409 (18)0.0476 (5)
H9A0.74220.45370.65350.057*
C100.60665 (17)0.5932 (2)0.62576 (14)0.0378 (4)
C110.49822 (16)0.5831 (2)0.62596 (15)0.0393 (4)
H11A0.45490.67880.60660.047*
C120.45353 (15)0.4328 (2)0.65451 (14)0.0362 (4)
H12A0.38070.42750.65410.043*
C130.6542 (2)0.7581 (3)0.59509 (17)0.0517 (5)
H13A0.59890.84330.57720.077*
H13B0.68650.73600.53820.077*
H13C0.70750.80020.65030.077*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0320 (3)0.0331 (3)0.0306 (3)0.00429 (14)0.00219 (18)0.00011 (14)
N10.0305 (8)0.0457 (9)0.0323 (8)0.0044 (6)0.0005 (6)0.0065 (6)
N20.0232 (7)0.0518 (9)0.0315 (7)0.0046 (6)0.0002 (5)0.0014 (6)
O10.0289 (7)0.0811 (11)0.0494 (9)0.0104 (7)0.0017 (6)0.0003 (8)
O20.0443 (8)0.0788 (11)0.0359 (8)0.0020 (8)0.0071 (6)0.0086 (7)
O30.0502 (8)0.0446 (7)0.0360 (7)0.0143 (6)0.0009 (6)0.0056 (6)
O40.0407 (7)0.0405 (7)0.0451 (8)0.0066 (5)0.0054 (6)0.0052 (5)
C10.0248 (8)0.0424 (9)0.0434 (10)0.0036 (6)0.0014 (7)0.0056 (7)
C20.0338 (9)0.0500 (11)0.0476 (11)0.0091 (8)0.0097 (8)0.0004 (8)
C30.0380 (9)0.0419 (9)0.0345 (9)0.0009 (7)0.0064 (7)0.0010 (7)
C40.0257 (8)0.0336 (8)0.0312 (8)0.0029 (6)0.0005 (6)0.0068 (6)
C50.0242 (8)0.0363 (8)0.0323 (8)0.0000 (6)0.0040 (6)0.0035 (6)
C60.0269 (8)0.0321 (8)0.0301 (8)0.0023 (6)0.0026 (6)0.0063 (6)
C70.0283 (8)0.0336 (8)0.0279 (7)0.0049 (6)0.0031 (6)0.0025 (6)
C80.0288 (9)0.0430 (10)0.0591 (12)0.0017 (7)0.0066 (8)0.0057 (8)
C90.0315 (10)0.0522 (11)0.0602 (13)0.0073 (8)0.0118 (9)0.0009 (10)
C100.0438 (10)0.0411 (10)0.0292 (8)0.0106 (7)0.0090 (7)0.0033 (6)
C110.0396 (10)0.0358 (9)0.0414 (10)0.0009 (7)0.0052 (8)0.0004 (7)
C120.0285 (8)0.0379 (9)0.0421 (10)0.0008 (6)0.0067 (7)0.0018 (7)
C130.0626 (14)0.0488 (12)0.0465 (11)0.0170 (10)0.0181 (10)0.0004 (9)
Geometric parameters (Å, º) top
S1—O41.4277 (14)C5—C61.384 (2)
S1—O31.4341 (14)C5—H5A0.9300
S1—N21.6316 (16)C7—C121.379 (2)
S1—C71.7628 (17)C7—C81.385 (2)
N1—O11.213 (2)C8—C91.389 (3)
N1—O21.227 (2)C8—H8A0.9300
N1—C41.468 (2)C9—C101.382 (3)
N2—C61.416 (2)C9—H9A0.9300
N2—H2A0.8600C10—C111.387 (3)
C1—C21.379 (3)C10—C131.506 (3)
C1—C61.392 (2)C11—C121.383 (3)
C1—H1A0.9300C11—H11A0.9300
C2—C31.387 (3)C12—H12A0.9300
C2—H2B0.9300C13—H13A0.9600
C3—C41.382 (3)C13—H13B0.9600
C3—H3A0.9300C13—H13C0.9600
C4—C51.382 (2)
O4—S1—O3119.37 (9)C5—C6—C1119.52 (16)
O4—S1—N2108.83 (8)C5—C6—N2123.16 (16)
O3—S1—N2104.23 (9)C1—C6—N2117.29 (16)
O4—S1—C7107.87 (9)C12—C7—C8120.64 (16)
O3—S1—C7109.24 (8)C12—C7—S1120.27 (13)
N2—S1—C7106.61 (8)C8—C7—S1119.01 (14)
O1—N1—O2122.59 (16)C7—C8—C9119.05 (18)
O1—N1—C4118.73 (15)C7—C8—H8A120.5
O2—N1—C4118.68 (16)C9—C8—H8A120.5
C6—N2—S1127.20 (12)C10—C9—C8121.22 (18)
C6—N2—H2A116.4C10—C9—H9A119.4
S1—N2—H2A116.4C8—C9—H9A119.4
C2—C1—C6120.80 (17)C9—C10—C11118.55 (17)
C2—C1—H1A119.6C9—C10—C13121.04 (19)
C6—C1—H1A119.6C11—C10—C13120.41 (19)
C1—C2—C3120.98 (17)C12—C11—C10121.07 (17)
C1—C2—H2B119.5C12—C11—H11A119.5
C3—C2—H2B119.5C10—C11—H11A119.5
C4—C3—C2116.70 (17)C7—C12—C11119.46 (17)
C4—C3—H3A121.6C7—C12—H12A120.3
C2—C3—H3A121.6C11—C12—H12A120.3
C3—C4—C5124.01 (16)C10—C13—H13A109.5
C3—C4—N1118.58 (16)C10—C13—H13B109.5
C5—C4—N1117.41 (15)H13A—C13—H13B109.5
C4—C5—C6117.99 (16)C10—C13—H13C109.5
C4—C5—H5A121.0H13A—C13—H13C109.5
C6—C5—H5A121.0H13B—C13—H13C109.5
O4—S1—N2—C648.29 (18)S1—N2—C6—C1161.38 (14)
O3—S1—N2—C6176.69 (15)O4—S1—C7—C12161.13 (14)
C7—S1—N2—C667.82 (17)O3—S1—C7—C1267.70 (17)
C6—C1—C2—C30.0 (3)N2—S1—C7—C1244.38 (16)
C1—C2—C3—C40.7 (3)O4—S1—C7—C821.97 (17)
C2—C3—C4—C50.9 (3)O3—S1—C7—C8109.20 (16)
C2—C3—C4—N1179.71 (17)N2—S1—C7—C8138.72 (15)
O1—N1—C4—C3172.99 (17)C12—C7—C8—C90.4 (3)
O2—N1—C4—C36.8 (2)S1—C7—C8—C9177.31 (17)
O1—N1—C4—C56.4 (2)C7—C8—C9—C100.3 (3)
O2—N1—C4—C5173.78 (16)C8—C9—C10—C110.8 (3)
C3—C4—C5—C60.6 (3)C8—C9—C10—C13179.3 (2)
N1—C4—C5—C6179.92 (14)C9—C10—C11—C120.5 (3)
C4—C5—C6—C10.1 (2)C13—C10—C11—C12179.61 (18)
C4—C5—C6—N2178.00 (15)C8—C7—C12—C110.7 (3)
C2—C1—C6—C50.4 (3)S1—C7—C12—C11177.56 (14)
C2—C1—C6—N2177.87 (17)C10—C11—C12—C70.2 (3)
S1—N2—C6—C520.5 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···O2i0.862.233.058 (2)162
Symmetry code: (i) x1/2, y+1/2, z1/2.

Experimental details

Crystal data
Chemical formulaC13H12N2O4S
Mr292.31
Crystal system, space groupMonoclinic, P21/n
Temperature (K)293
a, b, c (Å)12.766 (3), 7.7327 (15), 13.550 (3)
β (°) 101.66 (3)
V3)1310.0 (5)
Z4
Radiation typeMo Kα
µ (mm1)0.26
Crystal size (mm)0.29 × 0.15 × 0.07
Data collection
DiffractometerRigaku R-AXIS RAPID
diffractometer
Absorption correctionMulti-scan
(ABSCOR; Higashi, 1995)
Tmin, Tmax0.928, 0.981
No. of measured, independent and
observed [I > 2σ(I)] reflections
12545, 2997, 2519
Rint0.029
(sin θ/λ)max1)0.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.147, 1.01
No. of reflections2997
No. of parameters181
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.39, 0.44

Computer programs: RAPID-AUTO (Rigaku, 1997), RAPID-AUTO, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), please supply, SHELXL97.

Selected geometric parameters (Å, º) top
S1—O41.4277 (14)N1—O11.213 (2)
S1—O31.4341 (14)N1—O21.227 (2)
S1—N21.6316 (16)N1—C41.468 (2)
S1—C71.7628 (17)N2—C61.416 (2)
O4—S1—O3119.37 (9)O3—S1—C7109.24 (8)
O4—S1—N2108.83 (8)N2—S1—C7106.61 (8)
O3—S1—N2104.23 (9)O1—N1—O2122.59 (16)
O4—S1—C7107.87 (9)
C7—S1—N2—C667.82 (17)O3—S1—C7—C1267.70 (17)
S1—N2—C6—C1161.38 (14)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···O2i0.862.233.058 (2)162
Symmetry code: (i) x1/2, y+1/2, z1/2.
 

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