N-Benzoyl-3-nitro-benzene-sulfonamide.

In the title compound, C(13)H(10)N(2)O(5)S, the dihedral angle between the phenyl and benzene rings is 86.7 (1)°. In the crystal, mol-ecules are linked into zigzag C(4) chains running along the b axis via N-H⋯O hydrogen bonds.

Related literature

For our studies on the effects of substituents on the structures and other aspects of N-(ar­yl)-amides, see: Bowes et al. (2003 ▶); Gowda et al. (2004 ▶), on N-(ar­yl)-methane­sulfonamides, see: Jayalakshmi & Gowda (2004 ▶), on N-(ar­yl)-aryl­sulfonamides, see: Gowda et al. (2003 ▶), on N-(substitutedbenzo­yl)-aryl­sulfonamides, see: Suchetan et al. (2010 ▶) and on N-chloro­aryl­amides, see: Gowda et al. (1996 ▶).

Experimental

Crystal data

C13H10N2O5S

M = 306.29

Monoclinic,

a = 11.546 (1) Å

b = 5.0302 (5) Å

c = 23.387 (2) Å

β = 93.69 (1)°

V = 1355.5 (2) Å3

Z = 4

Mo Kα radiation

μ = 0.26 mm−1

T = 293 K

0.48 × 0.20 × 0.16 mm

Data collection

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector

Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009 ▶) T min = 0.884, T max = 0.959

4929 measured reflections

2768 independent reflections

2225 reflections with I > 2σ(I)

R int = 0.013

Refinement

R[F 2 > 2σ(F 2)] = 0.040

wR(F 2) = 0.093

S = 1.05

2768 reflections

193 parameters

1 restraint

H atoms treated by a mixture of independent and constrained refinement

Δρmax = 0.27 e Å−3

Δρmin = −0.33 e Å−3

Data collection: CrysAlis CCD (Oxford Diffraction, 2009 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2009 ▶); 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, 2009 ▶); software used to prepare material for publication: SHELXL97.

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811051142/bt5732sup1.cif

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811051142/bt5732Isup2.hkl

Supplementary material file. DOI: 10.1107/S1600536811051142/bt5732Isup3.cml

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

C13H10N2O5S	F(000) = 632
Mr = 306.29	Dx = 1.501 Mg m−3
Monoclinic, P21/c	Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc	Cell parameters from 1881 reflections
a = 11.546 (1) Å	θ = 2.6–27.8°
b = 5.0302 (5) Å	µ = 0.26 mm−1
c = 23.387 (2) Å	T = 293 K
β = 93.69 (1)°	Rod, colourless
V = 1355.5 (2) Å3	0.48 × 0.20 × 0.16 mm
Z = 4

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector	2768 independent reflections
Radiation source: fine-focus sealed tube	2225 reflections with I > 2σ(I)
graphite	Rint = 0.013
Rotation method data acquisition using ω and phi scans	θmax = 26.4°, θmin = 2.6°
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009)	h = −9→14
Tmin = 0.884, Tmax = 0.959	k = −6→3
4929 measured reflections	l = −24→29

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)] = 0.040	Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.093	H atoms treated by a mixture of independent and constrained refinement
S = 1.05	w = 1/[σ2(Fo2) + (0.0313P)2 + 0.8565P] where P = (Fo2 + 2Fc2)/3
2768 reflections	(Δ/σ)max = 0.002
193 parameters	Δρmax = 0.27 e Å−3
1 restraint	Δρmin = −0.33 e Å−3

Experimental. 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	0.23224 (16)	0.3781 (4)	0.79448 (8)	0.0329 (4)
C2	0.27622 (17)	0.5700 (4)	0.83229 (8)	0.0363 (4)
H2	0.3546	0.6143	0.8346	0.044*
C3	0.19897 (18)	0.6929 (4)	0.86639 (8)	0.0405 (5)
C4	0.08278 (19)	0.6308 (5)	0.86402 (9)	0.0496 (6)
H4	0.0329	0.7184	0.8874	0.059*
C5	0.04152 (19)	0.4376 (5)	0.82661 (10)	0.0514 (6)
H5	−0.0367	0.3923	0.8249	0.062*
C6	0.11592 (18)	0.3100 (4)	0.79148 (9)	0.0431 (5)
H6	0.0879	0.1795	0.7661	0.052*
C7	0.25229 (17)	0.4841 (4)	0.65601 (8)	0.0357 (4)
C8	0.27975 (17)	0.6755 (4)	0.61050 (8)	0.0374 (4)
C9	0.3905 (2)	0.7661 (6)	0.60253 (10)	0.0608 (7)
H9	0.4533	0.6984	0.6248	0.073*
C10	0.4082 (3)	0.9574 (7)	0.56151 (11)	0.0812 (10)
H10	0.4828	1.0197	0.5567	0.097*
C11	0.3168 (3)	1.0554 (6)	0.52804 (11)	0.0782 (9)
H11	0.3290	1.1853	0.5008	0.094*
C12	0.2079 (3)	0.9630 (6)	0.53456 (11)	0.0722 (8)
H12	0.1460	1.0284	0.5113	0.087*
C13	0.1884 (2)	0.7726 (5)	0.57538 (9)	0.0557 (6)
H13	0.1137	0.7094	0.5793	0.067*
N1	0.34339 (14)	0.4120 (3)	0.69483 (7)	0.0339 (4)
H1N	0.4037 (15)	0.495 (4)	0.6984 (9)	0.041*
N2	0.2428 (2)	0.9045 (4)	0.90566 (8)	0.0564 (5)
O1	0.43954 (12)	0.2116 (3)	0.77920 (6)	0.0501 (4)
O2	0.27356 (14)	−0.0250 (3)	0.73033 (6)	0.0518 (4)
O3	0.15637 (12)	0.3948 (3)	0.66098 (7)	0.0551 (4)
O4	0.34651 (19)	0.9464 (4)	0.90974 (9)	0.0856 (7)
O5	0.17200 (19)	1.0273 (4)	0.93168 (8)	0.0857 (7)
S1	0.32724 (4)	0.21577 (10)	0.74967 (2)	0.03588 (14)

	U11	U22	U33	U12	U13	U23
C1	0.0396 (10)	0.0295 (9)	0.0295 (9)	0.0041 (8)	0.0026 (8)	0.0043 (8)
C2	0.0412 (11)	0.0323 (10)	0.0353 (10)	0.0011 (8)	0.0017 (8)	0.0028 (8)
C3	0.0548 (12)	0.0338 (11)	0.0325 (10)	0.0074 (9)	0.0005 (9)	0.0014 (9)
C4	0.0496 (13)	0.0580 (14)	0.0417 (12)	0.0193 (11)	0.0074 (10)	0.0023 (11)
C5	0.0377 (11)	0.0672 (16)	0.0496 (13)	0.0024 (11)	0.0051 (10)	0.0056 (12)
C6	0.0444 (11)	0.0441 (12)	0.0404 (11)	−0.0023 (10)	0.0006 (9)	0.0018 (10)
C7	0.0380 (10)	0.0349 (10)	0.0337 (10)	−0.0010 (9)	−0.0007 (8)	−0.0030 (8)
C8	0.0452 (11)	0.0374 (11)	0.0295 (9)	0.0010 (9)	0.0019 (8)	−0.0013 (8)
C9	0.0549 (14)	0.0849 (19)	0.0418 (12)	−0.0150 (13)	−0.0014 (10)	0.0196 (13)
C10	0.088 (2)	0.103 (2)	0.0523 (15)	−0.0375 (19)	0.0038 (14)	0.0266 (17)
C11	0.122 (3)	0.0672 (19)	0.0459 (14)	−0.0052 (18)	0.0111 (16)	0.0204 (14)
C12	0.091 (2)	0.079 (2)	0.0462 (14)	0.0293 (17)	0.0040 (14)	0.0187 (14)
C13	0.0570 (14)	0.0676 (16)	0.0423 (12)	0.0123 (12)	0.0013 (10)	0.0089 (12)
N1	0.0338 (8)	0.0331 (9)	0.0349 (8)	−0.0041 (7)	0.0012 (7)	0.0023 (7)
N2	0.0812 (15)	0.0457 (11)	0.0419 (11)	0.0100 (11)	0.0005 (10)	−0.0078 (9)
O1	0.0453 (8)	0.0582 (10)	0.0465 (8)	0.0199 (7)	−0.0001 (7)	0.0066 (8)
O2	0.0786 (11)	0.0269 (8)	0.0513 (9)	−0.0036 (7)	0.0143 (8)	−0.0034 (7)
O3	0.0397 (8)	0.0684 (11)	0.0561 (9)	−0.0162 (8)	−0.0053 (7)	0.0129 (9)
O4	0.0849 (15)	0.0825 (15)	0.0889 (15)	−0.0178 (12)	0.0012 (12)	−0.0401 (12)
O5	0.1106 (16)	0.0775 (14)	0.0689 (12)	0.0278 (12)	0.0056 (11)	−0.0327 (11)
S1	0.0445 (3)	0.0285 (2)	0.0350 (3)	0.0064 (2)	0.0045 (2)	0.0023 (2)

C1—C2	1.383 (3)	C8—C13	1.383 (3)
C1—C6	1.383 (3)	C9—C10	1.383 (3)
C1—S1	1.7654 (19)	C9—H9	0.9300
C2—C3	1.380 (3)	C10—C11	1.365 (4)
C2—H2	0.9300	C10—H10	0.9300
C3—C4	1.375 (3)	C11—C12	1.357 (4)
C3—N2	1.474 (3)	C11—H11	0.9300
C4—C5	1.372 (3)	C12—C13	1.381 (4)
C4—H4	0.9300	C12—H12	0.9300
C5—C6	1.384 (3)	C13—H13	0.9300
C5—H5	0.9300	N1—S1	1.6387 (17)
C6—H6	0.9300	N1—H1N	0.810 (15)
C7—O3	1.208 (2)	N2—O4	1.213 (3)
C7—N1	1.392 (2)	N2—O5	1.219 (3)
C7—C8	1.485 (3)	O1—S1	1.4294 (15)
C8—C9	1.382 (3)	O2—S1	1.4209 (15)
C2—C1—C6	121.36 (18)	C10—C9—H9	119.9
C2—C1—S1	119.06 (15)	C11—C10—C9	120.4 (3)
C6—C1—S1	119.58 (15)	C11—C10—H10	119.8
C3—C2—C1	117.24 (19)	C9—C10—H10	119.8
C3—C2—H2	121.4	C12—C11—C10	120.0 (3)
C1—C2—H2	121.4	C12—C11—H11	120.0
C4—C3—C2	122.7 (2)	C10—C11—H11	120.0
C4—C3—N2	119.0 (2)	C11—C12—C13	120.6 (3)
C2—C3—N2	118.3 (2)	C11—C12—H12	119.7
C5—C4—C3	119.0 (2)	C13—C12—H12	119.7
C5—C4—H4	120.5	C12—C13—C8	120.2 (2)
C3—C4—H4	120.5	C12—C13—H13	119.9
C4—C5—C6	120.2 (2)	C8—C13—H13	119.9
C4—C5—H5	119.9	C7—N1—S1	123.21 (13)
C6—C5—H5	119.9	C7—N1—H1N	122.8 (16)
C1—C6—C5	119.5 (2)	S1—N1—H1N	111.6 (15)
C1—C6—H6	120.2	O4—N2—O5	124.3 (2)
C5—C6—H6	120.2	O4—N2—C3	118.2 (2)
O3—C7—N1	119.97 (18)	O5—N2—C3	117.5 (2)
O3—C7—C8	123.34 (18)	O2—S1—O1	120.32 (10)
N1—C7—C8	116.68 (17)	O2—S1—N1	109.49 (9)
C9—C8—C13	118.7 (2)	O1—S1—N1	103.98 (9)
C9—C8—C7	123.57 (19)	O2—S1—C1	107.95 (10)
C13—C8—C7	117.71 (19)	O1—S1—C1	107.39 (9)
C8—C9—C10	120.1 (2)	N1—S1—C1	107.00 (9)
C8—C9—H9	119.9
C6—C1—C2—C3	−0.8 (3)	C11—C12—C13—C8	0.6 (4)
S1—C1—C2—C3	179.74 (14)	C9—C8—C13—C12	−2.2 (4)
C1—C2—C3—C4	0.3 (3)	C7—C8—C13—C12	176.1 (2)
C1—C2—C3—N2	−177.96 (17)	O3—C7—N1—S1	−2.2 (3)
C2—C3—C4—C5	0.5 (3)	C8—C7—N1—S1	176.65 (14)
N2—C3—C4—C5	178.7 (2)	C4—C3—N2—O4	175.8 (2)
C3—C4—C5—C6	−0.7 (3)	C2—C3—N2—O4	−5.9 (3)
C2—C1—C6—C5	0.6 (3)	C4—C3—N2—O5	−4.7 (3)
S1—C1—C6—C5	−179.95 (16)	C2—C3—N2—O5	173.6 (2)
C4—C5—C6—C1	0.2 (3)	C7—N1—S1—O2	53.95 (18)
O3—C7—C8—C9	−176.0 (2)	C7—N1—S1—O1	−176.27 (16)
N1—C7—C8—C9	5.2 (3)	C7—N1—S1—C1	−62.80 (17)
O3—C7—C8—C13	5.8 (3)	C2—C1—S1—O2	160.32 (15)
N1—C7—C8—C13	−173.01 (19)	C6—C1—S1—O2	−19.17 (18)
C13—C8—C9—C10	2.3 (4)	C2—C1—S1—O1	29.21 (18)
C7—C8—C9—C10	−175.9 (2)	C6—C1—S1—O1	−150.28 (16)
C8—C9—C10—C11	−1.0 (5)	C2—C1—S1—N1	−81.92 (16)
C9—C10—C11—C12	−0.7 (5)	C6—C1—S1—N1	98.59 (17)
C10—C11—C12—C13	0.8 (5)

D—H···A	D—H	H···A	D···A	D—H···A
N1—H1N···O1i	0.81 (2)	2.15 (2)	2.954 (2)	172 (2)

Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯A	D—H	H⋯A	D⋯A	D—H⋯A
N1—H1N⋯O1i	0.81 (2)	2.15 (2)	2.954 (2)	172 (2)

Symmetry code: (i) .