N-(4-Chloro-phen-yl)-2-nitro-benzene-sulfonamide.

In the title compound, C(12)H(9)ClN(2)O(4)S, the dihedral angle between the aromatic rings is 70.27 (8)°. In the crystal, mol-ecules are linked by pairs of N-H⋯O(S) hydrogen bonds, forming inversion dimers.

Related literature

For studies on the effects of substituents on the structures and other aspects of N-(ar­yl)-amides, see: Alkan et al. (2011 ▶); Bowes et al. (2003 ▶); Gowda et al. (2000 ▶); Saeed et al. (2010 ▶); Shahwar et al. (2012 ▶), of N-aroylsulfonamides, see: Chaithanya et al. (2012 ▶), of N-aryl­sulfonamides, see: Gowda et al. (2002 ▶) and of N-chloro­aryl­sulfonamides, see: Gowda & Shetty (2004 ▶); Shetty & Gowda (2004 ▶).

Experimental

Crystal data

C12H9ClN2O4S

M = 312.72

Monoclinic,

a = 8.3295 (4) Å

b = 11.0866 (7) Å

c = 14.5576 (8) Å

β = 92.481 (5)°

V = 1343.07 (13) Å3

Z = 4

Mo Kα radiation

μ = 0.45 mm−1

T = 293 K

0.44 × 0.40 × 0.20 mm

Data collection

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector

Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009 ▶) T min = 0.825, T max = 0.915

5440 measured reflections

2731 independent reflections

2314 reflections with I > 2σ(I)

R int = 0.014

Refinement

R[F 2 > 2σ(F 2)] = 0.035

wR(F 2) = 0.096

S = 1.04

2731 reflections

185 parameters

1 restraint

H atoms treated by a mixture of independent and constrained refinement

Δρmax = 0.30 e Å−3

Δρmin = −0.33 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2009 ▶); cell refinement: CrysAlis CCD; data reduction: CrysAlis RED (Oxford Diffraction, 2009 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXL97.

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536812033429/bt5983sup1.cif

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812033429/bt5983Isup2.hkl

Supplementary material file. DOI: 10.1107/S1600536812033429/bt5983Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

C12H9ClN2O4S	F(000) = 640
Mr = 312.72	Dx = 1.547 Mg m−3
Monoclinic, P21/c	Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc	Cell parameters from 2996 reflections
a = 8.3295 (4) Å	θ = 2.9–27.8°
b = 11.0866 (7) Å	µ = 0.45 mm−1
c = 14.5576 (8) Å	T = 293 K
β = 92.481 (5)°	Prism, yellow
V = 1343.07 (13) Å3	0.44 × 0.40 × 0.20 mm
Z = 4

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector	2731 independent reflections
Radiation source: fine-focus sealed tube	2314 reflections with I > 2σ(I)
Graphite monochromator	Rint = 0.014
Rotation method data acquisition using ω scans	θmax = 26.4°, θmin = 3.3°
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009)	h = −7→10
Tmin = 0.825, Tmax = 0.915	k = −5→13
5440 measured reflections	l = −18→13

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)] = 0.035	H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.096	w = 1/[σ2(Fo2) + (0.048P)2 + 0.5971P] where P = (Fo2 + 2Fc2)/3
S = 1.04	(Δ/σ)max = 0.001
2731 reflections	Δρmax = 0.30 e Å−3
185 parameters	Δρmin = −0.33 e Å−3
1 restraint	Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methods	Extinction coefficient: 0.073 (3)

Experimental. Absorption correction: CrysAlis RED (Oxford Diffraction, 2009) 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.

	x	y	z	Uiso*/Ueq
C1	−0.1798 (2)	0.15532 (16)	0.68296 (11)	0.0370 (4)
C2	−0.3256 (2)	0.10822 (17)	0.64898 (12)	0.0402 (4)
C3	−0.4701 (2)	0.1467 (2)	0.68128 (16)	0.0573 (5)
H3	−0.5663	0.1128	0.6590	0.069*
C4	−0.4699 (3)	0.2359 (3)	0.74690 (18)	0.0693 (7)
H4	−0.5668	0.2630	0.7688	0.083*
C5	−0.3281 (3)	0.2855 (2)	0.78045 (16)	0.0637 (6)
H5	−0.3295	0.3468	0.8241	0.076*
C6	−0.1826 (2)	0.24446 (19)	0.74942 (13)	0.0487 (5)
H6	−0.0868	0.2770	0.7734	0.058*
C7	0.1198 (2)	0.28269 (16)	0.54582 (12)	0.0376 (4)
C8	0.1634 (3)	0.3588 (2)	0.61813 (15)	0.0620 (6)
H8	0.1483	0.3348	0.6784	0.074*
C9	0.2294 (3)	0.4702 (2)	0.60068 (16)	0.0642 (6)
H9	0.2577	0.5216	0.6492	0.077*
C10	0.2532 (3)	0.50542 (18)	0.51187 (15)	0.0511 (5)
C11	0.2103 (3)	0.4313 (2)	0.44058 (15)	0.0668 (7)
H11	0.2248	0.4560	0.3804	0.080*
C12	0.1453 (3)	0.3197 (2)	0.45749 (14)	0.0570 (5)
H12	0.1182	0.2686	0.4085	0.068*
N1	0.0544 (2)	0.16573 (15)	0.55669 (10)	0.0424 (4)
H1N	0.019 (3)	0.1292 (18)	0.5090 (10)	0.051*
N2	−0.33334 (18)	0.01897 (15)	0.57452 (12)	0.0462 (4)
O1	0.12301 (16)	0.13015 (13)	0.72132 (9)	0.0496 (4)
O2	−0.01505 (15)	−0.02583 (11)	0.62602 (9)	0.0449 (3)
O3	−0.27587 (19)	0.04674 (15)	0.50164 (10)	0.0596 (4)
O4	−0.4002 (2)	−0.07600 (16)	0.58813 (15)	0.0779 (5)
Cl1	0.33847 (10)	0.64535 (6)	0.49159 (5)	0.0812 (3)
S1	0.00868 (5)	0.09845 (4)	0.64966 (3)	0.03638 (16)

	U11	U22	U33	U12	U13	U23
C1	0.0395 (9)	0.0376 (9)	0.0342 (8)	0.0032 (7)	0.0038 (7)	0.0049 (7)
C2	0.0402 (9)	0.0407 (9)	0.0400 (9)	0.0001 (7)	0.0041 (7)	0.0040 (8)
C3	0.0405 (10)	0.0664 (14)	0.0658 (13)	0.0030 (10)	0.0088 (9)	−0.0012 (11)
C4	0.0541 (13)	0.0838 (18)	0.0713 (15)	0.0174 (12)	0.0189 (11)	−0.0103 (13)
C5	0.0712 (14)	0.0654 (15)	0.0555 (13)	0.0134 (12)	0.0126 (11)	−0.0142 (11)
C6	0.0534 (11)	0.0507 (12)	0.0418 (10)	0.0028 (9)	0.0011 (8)	−0.0050 (9)
C7	0.0377 (8)	0.0363 (9)	0.0391 (9)	0.0011 (7)	0.0032 (7)	0.0007 (7)
C8	0.0986 (17)	0.0488 (12)	0.0398 (10)	−0.0157 (12)	0.0155 (11)	−0.0041 (9)
C9	0.0994 (18)	0.0435 (12)	0.0503 (12)	−0.0164 (12)	0.0088 (12)	−0.0097 (10)
C10	0.0600 (12)	0.0373 (10)	0.0556 (12)	−0.0039 (9)	−0.0025 (9)	0.0079 (9)
C11	0.0955 (18)	0.0649 (15)	0.0395 (11)	−0.0244 (13)	−0.0053 (11)	0.0119 (10)
C12	0.0789 (14)	0.0545 (12)	0.0369 (10)	−0.0184 (11)	−0.0052 (9)	0.0008 (9)
N1	0.0528 (9)	0.0405 (9)	0.0342 (8)	−0.0085 (7)	0.0060 (7)	−0.0035 (7)
N2	0.0363 (8)	0.0445 (9)	0.0574 (10)	−0.0011 (7)	−0.0027 (7)	−0.0034 (8)
O1	0.0440 (7)	0.0604 (9)	0.0438 (7)	−0.0017 (6)	−0.0070 (6)	0.0037 (6)
O2	0.0472 (7)	0.0353 (7)	0.0524 (8)	0.0035 (5)	0.0041 (6)	0.0027 (6)
O3	0.0684 (9)	0.0651 (10)	0.0452 (8)	0.0018 (8)	0.0016 (7)	−0.0075 (7)
O4	0.0727 (11)	0.0533 (10)	0.1085 (15)	−0.0248 (9)	0.0137 (10)	−0.0102 (10)
Cl1	0.1132 (6)	0.0494 (4)	0.0801 (4)	−0.0267 (3)	−0.0066 (4)	0.0173 (3)
S1	0.0362 (2)	0.0365 (3)	0.0364 (2)	0.00091 (17)	0.00049 (16)	0.00247 (17)

C1—C6	1.384 (3)	C8—C9	1.380 (3)
C1—C2	1.393 (3)	C8—H8	0.9300
C1—S1	1.7782 (17)	C9—C10	1.373 (3)
C2—C3	1.379 (3)	C9—H9	0.9300
C2—N2	1.467 (2)	C10—C11	1.359 (3)
C3—C4	1.375 (3)	C10—Cl1	1.737 (2)
C3—H3	0.9300	C11—C12	1.378 (3)
C4—C5	1.374 (4)	C11—H11	0.9300
C4—H4	0.9300	C12—H12	0.9300
C5—C6	1.388 (3)	N1—S1	1.6056 (15)
C5—H5	0.9300	N1—H1N	0.845 (10)
C6—H6	0.9300	N2—O4	1.212 (2)
C7—C12	1.375 (3)	N2—O3	1.222 (2)
C7—C8	1.385 (3)	O1—S1	1.4258 (14)
C7—N1	1.418 (2)	O2—S1	1.4318 (14)
C6—C1—C2	118.34 (17)	C10—C9—C8	120.2 (2)
C6—C1—S1	119.07 (14)	C10—C9—H9	119.9
C2—C1—S1	122.46 (14)	C8—C9—H9	119.9
C3—C2—C1	121.58 (19)	C11—C10—C9	120.2 (2)
C3—C2—N2	116.70 (17)	C11—C10—Cl1	120.40 (17)
C1—C2—N2	121.67 (16)	C9—C10—Cl1	119.40 (17)
C4—C3—C2	119.0 (2)	C10—C11—C12	119.9 (2)
C4—C3—H3	120.5	C10—C11—H11	120.0
C2—C3—H3	120.5	C12—C11—H11	120.0
C5—C4—C3	120.7 (2)	C7—C12—C11	120.8 (2)
C5—C4—H4	119.7	C7—C12—H12	119.6
C3—C4—H4	119.7	C11—C12—H12	119.6
C4—C5—C6	120.2 (2)	C7—N1—S1	128.70 (13)
C4—C5—H5	119.9	C7—N1—H1N	117.9 (16)
C6—C5—H5	119.9	S1—N1—H1N	112.6 (16)
C1—C6—C5	120.2 (2)	O4—N2—O3	124.13 (19)
C1—C6—H6	119.9	O4—N2—C2	118.12 (18)
C5—C6—H6	119.9	O3—N2—C2	117.71 (16)
C12—C7—C8	118.91 (18)	O1—S1—O2	119.60 (8)
C12—C7—N1	116.91 (17)	O1—S1—N1	109.08 (8)
C8—C7—N1	124.15 (17)	O2—S1—N1	106.25 (8)
C9—C8—C7	119.90 (19)	O1—S1—C1	106.42 (8)
C9—C8—H8	120.0	O2—S1—C1	107.00 (8)
C7—C8—H8	120.0	N1—S1—C1	108.04 (8)
C6—C1—C2—C3	−1.3 (3)	C8—C7—C12—C11	−1.2 (4)
S1—C1—C2—C3	174.54 (16)	N1—C7—C12—C11	−179.2 (2)
C6—C1—C2—N2	176.19 (17)	C10—C11—C12—C7	1.3 (4)
S1—C1—C2—N2	−8.0 (2)	C12—C7—N1—S1	−178.85 (16)
C1—C2—C3—C4	1.7 (3)	C8—C7—N1—S1	3.3 (3)
N2—C2—C3—C4	−175.9 (2)	C3—C2—N2—O4	−58.4 (3)
C2—C3—C4—C5	−0.5 (4)	C1—C2—N2—O4	124.1 (2)
C3—C4—C5—C6	−1.1 (4)	C3—C2—N2—O3	119.5 (2)
C2—C1—C6—C5	−0.3 (3)	C1—C2—N2—O3	−58.1 (2)
S1—C1—C6—C5	−176.30 (17)	C7—N1—S1—O1	−36.12 (19)
C4—C5—C6—C1	1.5 (4)	C7—N1—S1—O2	−166.30 (16)
C12—C7—C8—C9	0.8 (4)	C7—N1—S1—C1	79.17 (18)
N1—C7—C8—C9	178.6 (2)	C6—C1—S1—O1	18.79 (17)
C7—C8—C9—C10	−0.6 (4)	C2—C1—S1—O1	−157.00 (15)
C8—C9—C10—C11	0.7 (4)	C6—C1—S1—O2	147.73 (15)
C8—C9—C10—Cl1	−179.3 (2)	C2—C1—S1—O2	−28.05 (17)
C9—C10—C11—C12	−1.1 (4)	C6—C1—S1—N1	−98.23 (16)
Cl1—C10—C11—C12	178.9 (2)	C2—C1—S1—N1	85.98 (16)

D—H···A	D—H	H···A	D···A	D—H···A
N1—H1N···O2i	0.85 (1)	2.27 (1)	3.084 (2)	161 (2)

Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
N1—H1N⋯O2i	0.85 (1)	2.27 (1)	3.084 (2)	161 (2)

Symmetry code: (i) .