Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536809048399/ng2687sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536809048399/ng2687Isup2.hkl |
CCDC reference: 758349
Key indicators
- Single-crystal X-ray study
- T = 296 K
- Mean (C-C) = 0.004 Å
- R factor = 0.051
- wR factor = 0.152
- Data-to-parameter ratio = 12.9
checkCIF/PLATON results
No syntax errors found
Alert level G PLAT072_ALERT_2_G SHELXL First Parameter in WGHT Unusually Large.. 0.10
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 0 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 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 0 ALERT type 5 Informative message, check
The title compound was prepared by refluxing a mixture of 4-chlorobenzoic acid, benzene sulfonamide and phosphorous oxy chloride for 5 h on a water bath. The resultant mixture was cooled and poured into ice cold water. The Solid obtained was filtered, washed thoroughly with water and then dissolved in sodium bicarbonate solution. The compound was later reprecipitated by acidifying the filtered solution with dilute HCl. The filtered and dried solid was recrystallized to the constant melting point.
Rod like colourless single crystals of the title compound were obtained from a slow evaporation of its toluene solution at room temperature and the X-ray diffraction studies were also carried out at room temperature.
The H atoms were positioned with idealized geometry using a riding model [N—H = 0.86 Å, C—H = 0.93 Å] and were refined with isotropic displacement parameters (set to 1.2 times of the Ueq of the parent atom).
Data collection: CAD-4-PC (Enraf–Nonius, 1996); cell refinement: CAD-4-PC (Enraf–Nonius, 1996); data reduction: REDU4 (Stoe & Cie, 1987); 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 (Sheldrick, 2008).
C13H10ClNO3S | Z = 2 |
Mr = 295.73 | F(000) = 304 |
Triclinic, P1 | Dx = 1.567 Mg m−3 |
Hall symbol: -P 1 | Cu Kα radiation, λ = 1.54180 Å |
a = 5.4176 (4) Å | Cell parameters from 25 reflections |
b = 10.717 (1) Å | θ = 5.9–21.0° |
c = 10.980 (1) Å | µ = 4.30 mm−1 |
α = 86.666 (9)° | T = 296 K |
β = 83.903 (9)° | Rod, colourless |
γ = 81.823 (8)° | 0.48 × 0.42 × 0.23 mm |
V = 626.85 (9) Å3 |
Enraf–Nonius CAD-4 diffractometer | 2058 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.014 |
Graphite monochromator | θmax = 66.9°, θmin = 4.1° |
ω/2θ scans | h = 0→6 |
Absorption correction: ψ scan (North et al., 1968) | k = −12→12 |
Tmin = 0.232, Tmax = 0.438 | l = −13→13 |
2490 measured reflections | 3 standard reflections every 120 min |
2233 independent reflections | intensity decay: 1.5% |
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)] = 0.051 | H-atom parameters constrained |
wR(F2) = 0.152 | w = 1/[σ2(Fo2) + (0.1034P)2 + 0.2756P] where P = (Fo2 + 2Fc2)/3 |
S = 1.07 | (Δ/σ)max = 0.001 |
2233 reflections | Δρmax = 0.57 e Å−3 |
173 parameters | Δρmin = −0.52 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.063 (5) |
C13H10ClNO3S | γ = 81.823 (8)° |
Mr = 295.73 | V = 626.85 (9) Å3 |
Triclinic, P1 | Z = 2 |
a = 5.4176 (4) Å | Cu Kα radiation |
b = 10.717 (1) Å | µ = 4.30 mm−1 |
c = 10.980 (1) Å | T = 296 K |
α = 86.666 (9)° | 0.48 × 0.42 × 0.23 mm |
β = 83.903 (9)° |
Enraf–Nonius CAD-4 diffractometer | 2058 reflections with I > 2σ(I) |
Absorption correction: ψ scan (North et al., 1968) | Rint = 0.014 |
Tmin = 0.232, Tmax = 0.438 | 3 standard reflections every 120 min |
2490 measured reflections | intensity decay: 1.5% |
2233 independent reflections |
R[F2 > 2σ(F2)] = 0.051 | 0 restraints |
wR(F2) = 0.152 | H-atom parameters constrained |
S = 1.07 | Δρmax = 0.57 e Å−3 |
2233 reflections | Δρmin = −0.52 e Å−3 |
173 parameters |
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 | 0.5435 (4) | 0.1733 (2) | 0.8771 (2) | 0.0411 (6) | |
C2 | 0.7400 (5) | 0.0803 (3) | 0.8980 (3) | 0.0532 (7) | |
H2 | 0.8601 | 0.0939 | 0.9485 | 0.064* | |
C3 | 0.7552 (6) | −0.0338 (3) | 0.8426 (3) | 0.0630 (8) | |
H3 | 0.8860 | −0.0976 | 0.8562 | 0.076* | |
C4 | 0.5779 (6) | −0.0531 (3) | 0.7674 (3) | 0.0583 (7) | |
H4 | 0.5904 | −0.1295 | 0.7296 | 0.070* | |
C5 | 0.3821 (6) | 0.0403 (3) | 0.7480 (3) | 0.0555 (7) | |
H5 | 0.2622 | 0.0263 | 0.6976 | 0.067* | |
C6 | 0.3620 (5) | 0.1542 (3) | 0.8027 (2) | 0.0469 (6) | |
H6 | 0.2292 | 0.2171 | 0.7900 | 0.056* | |
C7 | 0.6462 (5) | 0.4535 (2) | 0.7460 (2) | 0.0408 (6) | |
C8 | 0.7940 (4) | 0.5520 (2) | 0.6881 (2) | 0.0387 (5) | |
C9 | 0.7425 (5) | 0.5974 (3) | 0.5720 (2) | 0.0519 (7) | |
H9 | 0.6201 | 0.5657 | 0.5343 | 0.062* | |
C10 | 0.8682 (6) | 0.6884 (3) | 0.5111 (2) | 0.0534 (7) | |
H10 | 0.8306 | 0.7190 | 0.4332 | 0.064* | |
C11 | 1.0517 (5) | 0.7341 (2) | 0.5673 (2) | 0.0441 (6) | |
C12 | 1.1054 (5) | 0.6914 (3) | 0.6829 (3) | 0.0472 (6) | |
H12 | 1.2279 | 0.7236 | 0.7201 | 0.057* | |
C13 | 0.9770 (5) | 0.6006 (2) | 0.7438 (2) | 0.0426 (6) | |
H13 | 1.0125 | 0.5716 | 0.8224 | 0.051* | |
N1 | 0.7013 (4) | 0.4043 (2) | 0.8612 (2) | 0.0465 (5) | |
H1N | 0.8365 | 0.4200 | 0.8882 | 0.056* | |
O1 | 0.2646 (4) | 0.37670 (19) | 0.95259 (19) | 0.0590 (6) | |
O2 | 0.6378 (5) | 0.2966 (2) | 1.05960 (18) | 0.0655 (6) | |
O3 | 0.4823 (4) | 0.41570 (18) | 0.69711 (17) | 0.0524 (5) | |
Cl1 | 1.21303 (15) | 0.84797 (7) | 0.48922 (7) | 0.0649 (3) | |
S1 | 0.51961 (12) | 0.31704 (6) | 0.94915 (5) | 0.0456 (3) |
U11 | U22 | U33 | U12 | U13 | U23 | |
C1 | 0.0404 (12) | 0.0423 (12) | 0.0425 (13) | −0.0149 (10) | −0.0024 (10) | 0.0009 (10) |
C2 | 0.0439 (13) | 0.0557 (15) | 0.0621 (16) | −0.0112 (11) | −0.0109 (12) | −0.0003 (12) |
C3 | 0.0506 (16) | 0.0514 (16) | 0.084 (2) | −0.0013 (13) | −0.0019 (15) | −0.0026 (15) |
C4 | 0.0625 (17) | 0.0472 (14) | 0.0670 (19) | −0.0216 (13) | 0.0094 (14) | −0.0117 (13) |
C5 | 0.0557 (16) | 0.0611 (17) | 0.0556 (16) | −0.0258 (13) | −0.0056 (12) | −0.0081 (13) |
C6 | 0.0426 (13) | 0.0506 (14) | 0.0499 (14) | −0.0117 (11) | −0.0082 (11) | −0.0012 (11) |
C7 | 0.0434 (12) | 0.0408 (12) | 0.0395 (12) | −0.0072 (10) | −0.0069 (10) | −0.0038 (10) |
C8 | 0.0381 (12) | 0.0398 (12) | 0.0383 (12) | −0.0042 (9) | −0.0063 (9) | −0.0011 (9) |
C9 | 0.0573 (15) | 0.0600 (16) | 0.0433 (14) | −0.0180 (13) | −0.0168 (12) | 0.0031 (12) |
C10 | 0.0609 (16) | 0.0624 (16) | 0.0395 (13) | −0.0154 (13) | −0.0141 (11) | 0.0104 (12) |
C11 | 0.0405 (12) | 0.0437 (13) | 0.0462 (13) | −0.0046 (10) | 0.0013 (10) | 0.0000 (10) |
C12 | 0.0408 (13) | 0.0540 (14) | 0.0487 (14) | −0.0125 (11) | −0.0068 (10) | −0.0003 (11) |
C13 | 0.0410 (12) | 0.0507 (14) | 0.0373 (12) | −0.0086 (10) | −0.0094 (10) | 0.0024 (10) |
N1 | 0.0553 (12) | 0.0473 (11) | 0.0426 (12) | −0.0213 (10) | −0.0150 (9) | 0.0043 (9) |
O1 | 0.0572 (12) | 0.0569 (11) | 0.0598 (12) | −0.0047 (9) | 0.0063 (9) | −0.0078 (9) |
O2 | 0.0992 (17) | 0.0649 (13) | 0.0407 (11) | −0.0339 (12) | −0.0190 (10) | 0.0066 (9) |
O3 | 0.0527 (11) | 0.0588 (11) | 0.0511 (10) | −0.0204 (9) | −0.0174 (8) | 0.0049 (8) |
Cl1 | 0.0664 (5) | 0.0603 (5) | 0.0678 (5) | −0.0208 (3) | 0.0014 (4) | 0.0134 (4) |
S1 | 0.0579 (5) | 0.0457 (4) | 0.0362 (4) | −0.0166 (3) | −0.0057 (3) | −0.0003 (3) |
C1—C2 | 1.379 (4) | C8—C9 | 1.381 (3) |
C1—C6 | 1.387 (4) | C8—C13 | 1.393 (4) |
C1—S1 | 1.755 (2) | C9—C10 | 1.371 (4) |
C2—C3 | 1.385 (4) | C9—H9 | 0.9300 |
C2—H2 | 0.9300 | C10—C11 | 1.383 (4) |
C3—C4 | 1.376 (5) | C10—H10 | 0.9300 |
C3—H3 | 0.9300 | C11—C12 | 1.371 (4) |
C4—C5 | 1.376 (5) | C11—Cl1 | 1.735 (3) |
C4—H4 | 0.9300 | C12—C13 | 1.377 (4) |
C5—C6 | 1.377 (4) | C12—H12 | 0.9300 |
C5—H5 | 0.9300 | C13—H13 | 0.9300 |
C6—H6 | 0.9300 | N1—S1 | 1.653 (2) |
C7—O3 | 1.212 (3) | N1—H1N | 0.8600 |
C7—N1 | 1.387 (3) | O1—S1 | 1.435 (2) |
C7—C8 | 1.488 (3) | O2—S1 | 1.422 (2) |
C2—C1—C6 | 121.3 (2) | C10—C9—C8 | 121.3 (2) |
C2—C1—S1 | 119.1 (2) | C10—C9—H9 | 119.4 |
C6—C1—S1 | 119.5 (2) | C8—C9—H9 | 119.4 |
C1—C2—C3 | 118.8 (3) | C9—C10—C11 | 118.9 (2) |
C1—C2—H2 | 120.6 | C9—C10—H10 | 120.5 |
C3—C2—H2 | 120.6 | C11—C10—H10 | 120.5 |
C4—C3—C2 | 120.3 (3) | C12—C11—C10 | 121.0 (2) |
C4—C3—H3 | 119.8 | C12—C11—Cl1 | 120.2 (2) |
C2—C3—H3 | 119.8 | C10—C11—Cl1 | 118.8 (2) |
C3—C4—C5 | 120.1 (3) | C11—C12—C13 | 119.7 (2) |
C3—C4—H4 | 119.9 | C11—C12—H12 | 120.2 |
C5—C4—H4 | 119.9 | C13—C12—H12 | 120.2 |
C4—C5—C6 | 120.6 (3) | C12—C13—C8 | 120.2 (2) |
C4—C5—H5 | 119.7 | C12—C13—H13 | 119.9 |
C6—C5—H5 | 119.7 | C8—C13—H13 | 119.9 |
C5—C6—C1 | 118.8 (3) | C7—N1—S1 | 123.18 (18) |
C5—C6—H6 | 120.6 | C7—N1—H1N | 118.4 |
C1—C6—H6 | 120.6 | S1—N1—H1N | 118.4 |
O3—C7—N1 | 119.6 (2) | O2—S1—O1 | 119.60 (14) |
O3—C7—C8 | 122.9 (2) | O2—S1—N1 | 103.57 (12) |
N1—C7—C8 | 117.5 (2) | O1—S1—N1 | 109.22 (12) |
C9—C8—C13 | 118.9 (2) | O2—S1—C1 | 109.18 (12) |
C9—C8—C7 | 116.9 (2) | O1—S1—C1 | 108.42 (12) |
C13—C8—C7 | 124.2 (2) | N1—S1—C1 | 106.02 (11) |
C6—C1—C2—C3 | 0.4 (4) | C10—C11—C12—C13 | 0.7 (4) |
S1—C1—C2—C3 | 178.9 (2) | Cl1—C11—C12—C13 | −179.7 (2) |
C1—C2—C3—C4 | 0.4 (5) | C11—C12—C13—C8 | 0.2 (4) |
C2—C3—C4—C5 | −0.8 (5) | C9—C8—C13—C12 | −0.8 (4) |
C3—C4—C5—C6 | 0.5 (5) | C7—C8—C13—C12 | 179.8 (2) |
C4—C5—C6—C1 | 0.3 (4) | O3—C7—N1—S1 | −12.7 (3) |
C2—C1—C6—C5 | −0.8 (4) | C8—C7—N1—S1 | 167.24 (17) |
S1—C1—C6—C5 | −179.2 (2) | C7—N1—S1—O2 | −175.7 (2) |
O3—C7—C8—C9 | −1.9 (4) | C7—N1—S1—O1 | −47.2 (2) |
N1—C7—C8—C9 | 178.1 (2) | C7—N1—S1—C1 | 69.4 (2) |
O3—C7—C8—C13 | 177.6 (3) | C2—C1—S1—O2 | −26.5 (3) |
N1—C7—C8—C13 | −2.4 (4) | C6—C1—S1—O2 | 151.9 (2) |
C13—C8—C9—C10 | 0.3 (4) | C2—C1—S1—O1 | −158.4 (2) |
C7—C8—C9—C10 | 179.8 (3) | C6—C1—S1—O1 | 20.1 (2) |
C8—C9—C10—C11 | 0.7 (4) | C2—C1—S1—N1 | 84.5 (2) |
C9—C10—C11—C12 | −1.2 (4) | C6—C1—S1—N1 | −97.1 (2) |
C9—C10—C11—Cl1 | 179.3 (2) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N···O1i | 0.86 | 2.47 | 3.281 (3) | 158 |
Symmetry code: (i) x+1, y, z. |
Experimental details
Crystal data | |
Chemical formula | C13H10ClNO3S |
Mr | 295.73 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 296 |
a, b, c (Å) | 5.4176 (4), 10.717 (1), 10.980 (1) |
α, β, γ (°) | 86.666 (9), 83.903 (9), 81.823 (8) |
V (Å3) | 626.85 (9) |
Z | 2 |
Radiation type | Cu Kα |
µ (mm−1) | 4.30 |
Crystal size (mm) | 0.48 × 0.42 × 0.23 |
Data collection | |
Diffractometer | Enraf–Nonius CAD-4 diffractometer |
Absorption correction | ψ scan (North et al., 1968) |
Tmin, Tmax | 0.232, 0.438 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 2490, 2233, 2058 |
Rint | 0.014 |
(sin θ/λ)max (Å−1) | 0.597 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.051, 0.152, 1.07 |
No. of reflections | 2233 |
No. of parameters | 173 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.57, −0.52 |
Computer programs: CAD-4-PC (Enraf–Nonius, 1996), REDU4 (Stoe & Cie, 1987), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), PLATON (Spek, 2009).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N···O1i | 0.86 | 2.47 | 3.281 (3) | 157.7 |
Symmetry code: (i) x+1, y, z. |
Diaryl acylsulfonamides are known as potent antitumor agents against a broad spectrum of human tumor xenografts (colon, lung, breast, ovary and prostate) in nude mice. As part of a study of the effect of ring and the side chain substituents on the crystal structures of N-aromatic sulfonamides (Gowda et al., 2008, 2009a,b), in the present work, the structure of N-(4-chlorobenzoyl)benzenesulfonamide (I) has been determined (Fig.1). The conformation of the N—H bond in the C—SO2—NH—C(O) segment of the structure is anti to the C=O bond, similar to that observed in N-(benzoyl)benzenesulfonamide (II) (Gowda et al., 2009a) and N-(3-chlorobenzoyl)- benzenesulfonamide (III)(Gowda et al., 2009b). The molecule is twisted at the S atom with a dihedral angle of 75.7 (1)° between the sulfonyl benzene ring and the C—SO2—NH—C—O segment, compared to the values of 86.5(0.1) in (II) and 89.9 (1)° in (III). Furthermore, the dihedral angle between the two benzene rings is 68.6 (1)° in (I) and 80.3(0.1) in (II) and 87.5 (1)° in (III). The packing of molecules linked by of N—H···O(S) hydrogen bonds (Table 1) is shown in Fig. 2.