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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Sep 22;68(Pt 10):o2973. doi: 10.1107/S1600536812039402

N-(2,3-Dimethyl­phen­yl)-4-fluoro-N-[(4-fluoro­phen­yl)sulfon­yl]benzene­sulfonamide

Shumaila Younas Mughal a, Islam Ullah Khan a,*, William T A Harrison b, Muneeb Hayat Khan c, Muhammad Nawaz Tahir d
PMCID: PMC3470340  PMID: 23125753

Abstract

In the title compound, C20H17F2NO4S2, the dihedral angles between the o-xylene ring and the fluoro­benzene rings are 31.7 (1) and 32.8 (1)°, and the dihedral angle between the fluoro­benzene rings is 50.9 (1)°. The C—N—S—C torsion angles are 76.7 (2) and 101.8 (2)°. In the crystal, mol­ecules are connected by C—H⋯O inter­actions into sheets in the ab plane.

Related literature  

For related crystal structures, see: Hanson & Hitchcock (2004); Low et al. (2006); Mughal et al. (2012).graphic file with name e-68-o2973-scheme1.jpg

Experimental  

Crystal data  

  • C20H17F2NO4S2

  • M r = 437.47

  • Orthorhombic, Inline graphic

  • a = 9.9493 (5) Å

  • b = 14.7107 (8) Å

  • c = 26.6871 (17) Å

  • V = 3906.0 (4) Å3

  • Z = 8

  • Mo Kα radiation

  • μ = 0.32 mm−1

  • T = 296 K

  • 0.28 × 0.25 × 0.23 mm

Data collection  

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 2008) T min = 0.916, T max = 0.930

  • 31734 measured reflections

  • 4352 independent reflections

  • 2943 reflections with I > 2σ(I)

  • R int = 0.046

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.048

  • wR(F 2) = 0.133

  • S = 1.02

  • 4352 reflections

  • 264 parameters

  • H-atom parameters constrained

  • Δρmax = 0.47 e Å−3

  • Δρmin = −0.29 e Å−3

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97.

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812039402/ld2072sup1.cif

e-68-o2973-sup1.cif (21.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812039402/ld2072Isup2.hkl

e-68-o2973-Isup2.hkl (213.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812039402/ld2072Isup3.cml

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

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C8—H8A⋯O2i 0.96 2.57 3.517 (5) 170
C19—H19⋯O1ii 0.93 2.39 3.260 (4) 157

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

The authors are grateful to the Higher Education Commission of Pakistan for providing a grant under a project strengthening the Materials Chemistry Laboratory at GC University, Lahore.

supplementary crystallographic information

Comment

Rather than the intended 4-fluoro-N-(2,3-dimethylphenyl)benzenesulfonamide, the title `double' sulfonamide (I), (Fig. 1) was unexpectedly obtained in our ongoing studies (Mughal et al., 2012). The related structures of 4-chloroaniline-N,N-ditoluene-p-sulfonamide, (II) (Hanson & Hitchcock, 2004) and 4-iodo-N,N-bis-(2-nitrophenylsulfonyl)aniline, (III) (Low et al., 2006) have been described previously.

The molecule of (I) cannot possess any local symmetry due to the two methyl groups of the xylene ring. Without them, the rest of the moleucle possesses approximate local twofold symmetry about the C1—N1 axis.

The sulfonamide C—N—S—C torsion angles in (I) [76.7 (2) and 101.8 (2)°] compare well to the corresponding value of 80.2° reported in (II), where the molecule posesses a crystallographic twofold symmetry. The respective values in (III) are 98.9 (2) and 94.3 (2)°. The bond-angle sum for the N atom in (I) of 359.7° implies sp2 hybridization for the N atom.

In the crystal of (I), there are weak C—H···O hydrogen bonds between the molecules (Table 1). The C8 bond results in translational chains along [100] and the C19 bond results in helices along [010]. Together these generate (001) sheets.

Experimental

0.10 g of 2,3-dimethyl aniline was dissolved in 15 ml dichloromethane, and 0.16 g of 4-fluoro benzene sulfonyl chloride was added. The mixture was stirred at room temperature overnight and its pH was maintained at 8–9 with triethylamine. On completion of the reaction (after TLC), 1M HCl solution was added, the organic fraction was separated, and the solvent was evaporated at room temperature to generate dark brown crystals in 94% yield. Yellow blocks were recrystallized from ethanol solution.

Refinement

The H atoms were placed in calculated positions (C—H = 0.93–0.96 Å) and refined as riding with Uiso(H) = 1.2Ueq(C) or 1.5Ueq(methyl C). The methyl groups were allowed to rotate to fit the electron density.

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I), showing displacement ellipsoids at the 50% probability level.

Crystal data

C20H17F2NO4S2 Dx = 1.488 Mg m3
Mr = 437.47 Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Pbca Cell parameters from 202 reflections
a = 9.9493 (5) Å θ = 3.2–20.5°
b = 14.7107 (8) Å µ = 0.32 mm1
c = 26.6871 (17) Å T = 296 K
V = 3906.0 (4) Å3 Block, yellow
Z = 8 0.28 × 0.25 × 0.23 mm
F(000) = 1808

Data collection

Bruker APEXII CCD diffractometer 4352 independent reflections
Radiation source: fine-focus sealed tube 2943 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.046
ω scans θmax = 27.3°, θmin = 1.5°
Absorption correction: multi-scan (SADABS; Sheldrick, 2008) h = −12→12
Tmin = 0.916, Tmax = 0.930 k = −18→14
31734 measured reflections l = −34→34

Refinement

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)] = 0.048 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.133 H-atom parameters constrained
S = 1.02 w = 1/[σ2(Fo2) + (0.0524P)2 + 2.7378P] where P = (Fo2 + 2Fc2)/3
4352 reflections (Δ/σ)max < 0.001
264 parameters Δρmax = 0.47 e Å3
0 restraints Δρmin = −0.29 e Å3

Special details

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 0.6678 (3) 0.45285 (18) 0.13773 (11) 0.0504 (7)
C2 0.7555 (3) 0.48512 (18) 0.10252 (10) 0.0540 (7)
C3 0.8910 (3) 0.4952 (2) 0.11660 (13) 0.0616 (8)
C4 0.9311 (4) 0.4696 (2) 0.16383 (14) 0.0717 (9)
H4 1.0208 0.4763 0.1729 0.086*
C5 0.8414 (4) 0.4343 (2) 0.19804 (14) 0.0765 (10)
H5 0.8715 0.4167 0.2296 0.092*
C6 0.7092 (3) 0.4250 (2) 0.18605 (11) 0.0595 (8)
H6 0.6480 0.4011 0.2089 0.071*
C7 0.7112 (3) 0.5083 (2) 0.05128 (11) 0.0666 (9)
H7A 0.7561 0.4696 0.0276 0.100*
H7B 0.7328 0.5706 0.0443 0.100*
H7C 0.6158 0.4996 0.0486 0.100*
C8 0.9920 (4) 0.5330 (3) 0.08077 (16) 0.0961 (13)
H8A 1.0796 0.5312 0.0958 0.144*
H8B 0.9691 0.5947 0.0729 0.144*
H8C 0.9922 0.4973 0.0506 0.144*
C9 0.4640 (3) 0.62628 (17) 0.11107 (10) 0.0451 (6)
C10 0.5733 (3) 0.68129 (19) 0.12047 (12) 0.0571 (7)
H10 0.6275 0.6707 0.1483 0.069*
C11 0.6018 (4) 0.7518 (2) 0.08853 (14) 0.0733 (9)
H11 0.6744 0.7902 0.0943 0.088*
C12 0.5205 (4) 0.7638 (2) 0.04815 (14) 0.0768 (10)
C13 0.4101 (4) 0.7119 (2) 0.03854 (12) 0.0749 (10)
H13 0.3554 0.7241 0.0111 0.090*
C14 0.3816 (3) 0.6414 (2) 0.07036 (10) 0.0583 (7)
H14 0.3077 0.6041 0.0646 0.070*
C15 0.3779 (3) 0.29685 (18) 0.14708 (9) 0.0449 (6)
C16 0.2445 (3) 0.31051 (19) 0.15903 (10) 0.0517 (7)
H16 0.1919 0.3501 0.1402 0.062*
C17 0.1902 (3) 0.2645 (2) 0.19928 (11) 0.0557 (7)
H17 0.1007 0.2728 0.2083 0.067*
C18 0.2703 (3) 0.2067 (2) 0.22544 (10) 0.0542 (7)
C19 0.4012 (3) 0.1897 (2) 0.21330 (11) 0.0569 (7)
H19 0.4518 0.1480 0.2314 0.068*
C20 0.4558 (3) 0.23611 (19) 0.17354 (10) 0.0518 (7)
H20 0.5450 0.2265 0.1645 0.062*
S1 0.43137 (7) 0.53555 (5) 0.15106 (3) 0.0483 (2)
S2 0.45376 (7) 0.35921 (5) 0.09885 (2) 0.0494 (2)
F1 0.5499 (3) 0.83173 (15) 0.01607 (9) 0.1272 (10)
F2 0.21844 (19) 0.16374 (13) 0.26576 (7) 0.0773 (6)
O1 0.4877 (2) 0.55627 (14) 0.19840 (7) 0.0654 (6)
O2 0.29538 (19) 0.50962 (14) 0.14719 (9) 0.0677 (6)
O3 0.3540 (2) 0.39068 (16) 0.06534 (7) 0.0704 (6)
O4 0.5668 (2) 0.30948 (14) 0.08134 (7) 0.0622 (5)
N1 0.5226 (2) 0.44974 (14) 0.12742 (8) 0.0444 (5)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0518 (16) 0.0389 (14) 0.0604 (17) −0.0005 (12) 0.0075 (13) −0.0049 (12)
C2 0.0611 (17) 0.0435 (16) 0.0574 (17) 0.0019 (13) 0.0051 (14) −0.0018 (13)
C3 0.0486 (16) 0.0509 (17) 0.085 (2) 0.0025 (14) −0.0022 (16) −0.0086 (16)
C4 0.064 (2) 0.063 (2) 0.088 (2) −0.0010 (17) 0.0044 (19) −0.0038 (18)
C5 0.081 (2) 0.080 (2) 0.068 (2) 0.006 (2) −0.0230 (19) 0.0015 (18)
C6 0.0580 (18) 0.0585 (18) 0.0619 (18) −0.0002 (15) −0.0060 (14) 0.0022 (14)
C7 0.083 (2) 0.0597 (19) 0.0573 (18) 0.0066 (17) 0.0038 (16) 0.0049 (15)
C8 0.071 (2) 0.105 (3) 0.112 (3) −0.021 (2) 0.015 (2) 0.003 (3)
C9 0.0491 (15) 0.0359 (13) 0.0502 (14) −0.0006 (12) 0.0011 (12) −0.0053 (11)
C10 0.0583 (18) 0.0478 (16) 0.0653 (18) −0.0045 (14) −0.0030 (15) −0.0058 (14)
C11 0.082 (2) 0.0494 (18) 0.089 (3) −0.0206 (17) 0.008 (2) −0.0050 (17)
C12 0.115 (3) 0.0473 (18) 0.068 (2) −0.007 (2) 0.017 (2) 0.0057 (16)
C13 0.109 (3) 0.068 (2) 0.0487 (17) 0.008 (2) −0.0091 (18) 0.0019 (16)
C14 0.0642 (18) 0.0571 (18) 0.0534 (17) −0.0027 (15) −0.0054 (14) −0.0081 (14)
C15 0.0503 (15) 0.0404 (14) 0.0440 (14) −0.0087 (12) −0.0049 (12) −0.0045 (11)
C16 0.0473 (15) 0.0484 (16) 0.0594 (17) −0.0078 (13) −0.0102 (13) 0.0035 (13)
C17 0.0451 (15) 0.0568 (17) 0.0651 (18) −0.0104 (14) 0.0022 (14) −0.0016 (14)
C18 0.0577 (18) 0.0554 (17) 0.0496 (15) −0.0180 (14) −0.0034 (13) 0.0017 (13)
C19 0.0578 (18) 0.0541 (17) 0.0588 (17) −0.0048 (14) −0.0106 (14) 0.0102 (14)
C20 0.0458 (15) 0.0510 (16) 0.0585 (17) −0.0007 (13) −0.0005 (13) 0.0005 (13)
S1 0.0486 (4) 0.0448 (4) 0.0516 (4) 0.0001 (3) 0.0086 (3) −0.0025 (3)
S2 0.0592 (4) 0.0494 (4) 0.0397 (3) −0.0057 (3) −0.0004 (3) −0.0028 (3)
F1 0.209 (3) 0.0732 (14) 0.0998 (17) −0.0283 (17) 0.0147 (18) 0.0319 (13)
F2 0.0742 (12) 0.0903 (14) 0.0672 (11) −0.0198 (10) 0.0045 (10) 0.0228 (10)
O1 0.0839 (15) 0.0678 (13) 0.0445 (11) 0.0104 (12) 0.0046 (10) −0.0086 (9)
O2 0.0462 (11) 0.0566 (13) 0.1003 (17) −0.0017 (10) 0.0155 (11) 0.0027 (11)
O3 0.0764 (15) 0.0838 (15) 0.0510 (11) −0.0119 (12) −0.0174 (11) 0.0096 (11)
O4 0.0746 (14) 0.0565 (12) 0.0556 (12) −0.0007 (11) 0.0155 (10) −0.0153 (10)
N1 0.0429 (11) 0.0399 (12) 0.0503 (12) −0.0012 (9) 0.0031 (10) −0.0043 (10)

Geometric parameters (Å, º)

C1—C2 1.367 (4) C11—H11 0.9300
C1—C6 1.414 (4) C12—F1 1.348 (4)
C1—N1 1.471 (4) C12—C13 1.362 (5)
C2—C3 1.407 (4) C13—C14 1.371 (4)
C2—C7 1.476 (4) C13—H13 0.9300
C3—C4 1.375 (5) C14—H14 0.9300
C3—C8 1.495 (5) C15—C20 1.377 (4)
C4—C5 1.378 (5) C15—C16 1.380 (4)
C4—H4 0.9300 C15—S2 1.751 (3)
C5—C6 1.361 (4) C16—C17 1.380 (4)
C5—H5 0.9300 C16—H16 0.9300
C6—H6 0.9300 C17—C18 1.358 (4)
C7—H7A 0.9600 C17—H17 0.9300
C7—H7B 0.9600 C18—F2 1.350 (3)
C7—H7C 0.9600 C18—C19 1.365 (4)
C8—H8A 0.9600 C19—C20 1.374 (4)
C8—H8B 0.9600 C19—H19 0.9300
C8—H8C 0.9600 C20—H20 0.9300
C9—C10 1.378 (4) S1—O2 1.410 (2)
C9—C14 1.379 (4) S1—O1 1.415 (2)
C9—S1 1.739 (3) S1—N1 1.678 (2)
C10—C11 1.373 (4) S2—O3 1.414 (2)
C10—H10 0.9300 S2—O4 1.421 (2)
C11—C12 1.359 (5) S2—N1 1.681 (2)
C2—C1—C6 122.8 (3) C11—C12—C13 123.8 (3)
C2—C1—N1 120.6 (3) C12—C13—C14 118.3 (3)
C6—C1—N1 116.6 (2) C12—C13—H13 120.8
C1—C2—C3 117.6 (3) C14—C13—H13 120.8
C1—C2—C7 121.8 (3) C13—C14—C9 119.1 (3)
C3—C2—C7 120.6 (3) C13—C14—H14 120.4
C4—C3—C2 119.6 (3) C9—C14—H14 120.4
C4—C3—C8 119.5 (3) C20—C15—C16 121.1 (3)
C2—C3—C8 120.8 (3) C20—C15—S2 118.3 (2)
C3—C4—C5 121.5 (3) C16—C15—S2 120.5 (2)
C3—C4—H4 119.3 C17—C16—C15 119.0 (3)
C5—C4—H4 119.3 C17—C16—H16 120.5
C6—C5—C4 120.6 (3) C15—C16—H16 120.5
C6—C5—H5 119.7 C18—C17—C16 118.5 (3)
C4—C5—H5 119.7 C18—C17—H17 120.7
C5—C6—C1 117.8 (3) C16—C17—H17 120.7
C5—C6—H6 121.1 F2—C18—C17 118.6 (3)
C1—C6—H6 121.1 F2—C18—C19 117.9 (3)
C2—C7—H7A 109.5 C17—C18—C19 123.5 (3)
C2—C7—H7B 109.5 C18—C19—C20 118.0 (3)
H7A—C7—H7B 109.5 C18—C19—H19 121.0
C2—C7—H7C 109.5 C20—C19—H19 121.0
H7A—C7—H7C 109.5 C19—C20—C15 119.7 (3)
H7B—C7—H7C 109.5 C19—C20—H20 120.1
C3—C8—H8A 109.5 C15—C20—H20 120.1
C3—C8—H8B 109.5 O2—S1—O1 120.26 (14)
H8A—C8—H8B 109.5 O2—S1—N1 106.76 (12)
C3—C8—H8C 109.5 O1—S1—N1 106.45 (12)
H8A—C8—H8C 109.5 O2—S1—C9 110.01 (13)
H8B—C8—H8C 109.5 O1—S1—C9 107.96 (13)
C10—C9—C14 121.2 (3) N1—S1—C9 104.21 (11)
C10—C9—S1 119.1 (2) O3—S2—O4 121.08 (13)
C14—C9—S1 119.7 (2) O3—S2—N1 108.28 (13)
C11—C10—C9 119.6 (3) O4—S2—N1 103.57 (11)
C11—C10—H10 120.2 O3—S2—C15 109.50 (13)
C9—C10—H10 120.2 O4—S2—C15 108.24 (13)
C12—C11—C10 117.9 (3) N1—S2—C15 104.92 (11)
C12—C11—H11 121.0 C1—N1—S1 115.94 (17)
C10—C11—H11 121.0 C1—N1—S2 120.65 (17)
F1—C12—C11 118.1 (4) S1—N1—S2 123.10 (13)
F1—C12—C13 118.1 (4)
C6—C1—C2—C3 −3.5 (4) C18—C19—C20—C15 −0.7 (4)
N1—C1—C2—C3 173.5 (2) C16—C15—C20—C19 −1.6 (4)
C6—C1—C2—C7 176.0 (3) S2—C15—C20—C19 176.6 (2)
N1—C1—C2—C7 −6.9 (4) C10—C9—S1—O2 158.3 (2)
C1—C2—C3—C4 2.3 (4) C14—C9—S1—O2 −22.4 (3)
C7—C2—C3—C4 −177.3 (3) C10—C9—S1—O1 25.3 (3)
C1—C2—C3—C8 −177.9 (3) C14—C9—S1—O1 −155.4 (2)
C7—C2—C3—C8 2.5 (5) C10—C9—S1—N1 −87.6 (2)
C2—C3—C4—C5 −0.2 (5) C14—C9—S1—N1 91.7 (2)
C8—C3—C4—C5 −179.9 (3) C20—C15—S2—O3 158.7 (2)
C3—C4—C5—C6 −0.9 (5) C16—C15—S2—O3 −23.2 (3)
C4—C5—C6—C1 −0.2 (5) C20—C15—S2—O4 24.8 (2)
C2—C1—C6—C5 2.5 (5) C16—C15—S2—O4 −157.1 (2)
N1—C1—C6—C5 −174.6 (3) C20—C15—S2—N1 −85.3 (2)
C14—C9—C10—C11 −0.7 (4) C16—C15—S2—N1 92.8 (2)
S1—C9—C10—C11 178.6 (2) C2—C1—N1—S1 −98.9 (3)
C9—C10—C11—C12 −0.8 (5) C6—C1—N1—S1 78.3 (3)
C10—C11—C12—F1 −178.5 (3) C2—C1—N1—S2 87.2 (3)
C10—C11—C12—C13 2.4 (6) C6—C1—N1—S2 −95.6 (3)
F1—C12—C13—C14 178.4 (3) O2—S1—N1—C1 −166.84 (19)
C11—C12—C13—C14 −2.5 (6) O1—S1—N1—C1 −37.2 (2)
C12—C13—C14—C9 0.9 (5) C9—S1—N1—C1 76.7 (2)
C10—C9—C14—C13 0.6 (4) O2—S1—N1—S2 6.85 (19)
S1—C9—C14—C13 −178.6 (2) O1—S1—N1—S2 136.46 (16)
C20—C15—C16—C17 2.2 (4) C9—S1—N1—S2 −109.56 (16)
S2—C15—C16—C17 −175.9 (2) O3—S2—N1—C1 −141.3 (2)
C15—C16—C17—C18 −0.5 (4) O4—S2—N1—C1 −11.6 (2)
C16—C17—C18—F2 178.0 (2) C15—S2—N1—C1 101.8 (2)
C16—C17—C18—C19 −1.8 (4) O3—S2—N1—S1 45.28 (19)
F2—C18—C19—C20 −177.4 (2) O4—S2—N1—S1 175.00 (15)
C17—C18—C19—C20 2.4 (4) C15—S2—N1—S1 −71.57 (18)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C8—H8A···O2i 0.96 2.57 3.517 (5) 170
C19—H19···O1ii 0.93 2.39 3.260 (4) 157

Symmetry codes: (i) x+1, y, z; (ii) −x+1, y−1/2, −z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LD2072).

References

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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 datablock(s) global, I. DOI: 10.1107/S1600536812039402/ld2072sup1.cif

e-68-o2973-sup1.cif (21.2KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812039402/ld2072Isup2.hkl

e-68-o2973-Isup2.hkl (213.4KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812039402/ld2072Isup3.cml

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


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