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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2008 Oct 25;64(Pt 11):o2207. doi: 10.1107/S1600536808034302

3,5-Difluoro­phenyl phenyl sulfone

David A Grossie a,*, Eric Fossum a, Andrea Elsen a, Tricia Meyer a
PMCID: PMC2959527  PMID: 21581065

Abstract

In the title compound, C12H8F2O2S, which is a precursor of functionalised poly(aryl­ene ether sulfone) polymers, the dihedral angle between the aromatic ring planes is 84.43 (8)°. In the crystal structure, aromatic π–π stacking [centroid–centroid separations = 3.808 (3) and 3.867 (3) Å] helps to establish the packing. A short C—H⋯F contact also occurs.

Related literature

For general background, see: Attwood et al. (1977); Salamon (1999); Johnson et al. (1967); Kaiti et al. (2006).graphic file with name e-64-o2207-scheme1.jpg

Experimental

Crystal data

  • C12H8F2O2S

  • M r = 254.24

  • Monoclinic, Inline graphic

  • a = 10.328 (6) Å

  • b = 14.256 (9) Å

  • c = 7.641 (4) Å

  • β = 108.17 (4)°

  • V = 1068.9 (11) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.32 mm−1

  • T = 173 (2) K

  • 0.31 × 0.23 × 0.07 mm

Data collection

  • Bruker SMART APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2003) T min = 0.892, T max = 0.977

  • 9888 measured reflections

  • 2841 independent reflections

  • 2312 reflections with I > 2σ(I)

  • R int = 0.035

Refinement

  • R[F 2 > 2σ(F 2)] = 0.049

  • wR(F 2) = 0.138

  • S = 1.07

  • 2841 reflections

  • 154 parameters

  • H-atom parameters constrained

  • Δρmax = 1.03 e Å−3

  • Δρmin = −0.37 e Å−3

Data collection: SMART (Bruker, 2003); cell refinement: SAINT-Plus (Bruker, 2003); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2006) and OSCAIL (McArdle, 1995); software used to prepare material for publication: enCIFer (Allen et al. 2004) and publCIF (Westrip, 2008).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808034302/hb2817sup1.cif

e-64-o2207-sup1.cif (17KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808034302/hb2817Isup2.hkl

e-64-o2207-Isup2.hkl (139.5KB, hkl)

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
C2—H2⋯F5i 0.95 2.44 3.337 (3) 157

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors acknowledge the diffractometer time granted by A. Hunter, Youngstown State University.

supplementary crystallographic information

Comment

Poly(arylene ether sulfone)s, PAESs, are a class of tough, amorphous polymers that possess excellent thermo and oxidative stability as well as low dielectric constants (Salamon, 1999). Several of these systems have found commercial applications that require hydrolytic and thermal stability. Classically, PAESs are synthesized through nucleophilic aromatic substitution (NAS) reactions of 4-chloro (or fluoro-) phenyl sulfone (I) with various bisphenolates, a well known A~2~ + B~2~ polycondensation, to afford linear PAESs (Attwood et al., 1977, Johnson et al., 1967). In order to tailor the chemical and physical properties of PAESs, it is often desirable to introduce functional groups along or pendant to the backbone. To that end, a geometric isomer of (I), the title compound, (II), has been prepared and successfully polymerized, under NAS conditions, to generate PAESs carrying a pendant phenyl sulfonyl group (Kaiti et al., 2006). The pendant phenyl sulfonyl group provides a unique platform from which to access PAESs bearing a wide variety of functional groups. We now describe the crystal structure of (II) (Fig. 1).

The bond lengths within (I) are all within their expeted ranges of values. Bond angles within the molecule were also mostly observed as expected. The O1—S1—O2 angle is 120.39 (10)° and angles near 108° are seen for Ox—S1—Cy (with x = 1 or 2 and y = 1 or 7). The angle between C1—S1—C7 is 102.68 (10)°, which is smaller than would have been expected, based on prediction or comparison with similar structures in CSD.

Four molecules are present within the unit cell, in two columns in which the fluorine substituted rings are stacked in the c direction with a centroid-centroid separation of 3.867 (3)Å. Neighboring columns are interconnected viaπ-π interactions between the unsubstituted phenyl rings that lie parallel to each other, separated by 3.808 (3)Å. A short C—H···F contact (Table 1) interconnects the columns within the crystal.

Experimental

In a 250-ml round bottomed flask equipped with a stir bar, addition funnel, condenser, and gas inlet were placed 2.105 g (86.6 mmol) of Mg turnings and enough THF to cover the metal. A solution of 15.94 g (82.5 mmol) of 1-bromo-3,5-difluorobenzene and 50 ml of THF was added slowly to the stirred Mg at room temperature; upon complete addition, the reaction mixture was stirred and allowed to react for 4 h. The resulting solution of 3,5-difluorophenylmagnesium bromide was transferred to an addition funnel and added dropwise to a mixture of 16.01 g (90.8 mmol) of benzenesulfonyl chloride in 60 ml of THF at 273 K. The reaction mixture was stirred overnight. The reaction mixture was then diluted in 500 ml of ether and washed in a separatory funnel with dilute HCl, distilled water, 5% NaHCO3, and again with distilled H2O. The ether layer was dried over MgSO4, filtered, and then evaporated to dryness to afford a yellow solid which was recrystallized, first from ethanol/water and then from hexanes to yield colourless blocks of (I).

Figures

Fig. 1.

Fig. 1.

The molecular structure of (I) showing 50% displacement ellipsoids for the non-hydrogen atoms.

Crystal data

C12H8F2O2S F(000) = 520
Mr = 254.24 Dx = 1.580 Mg m3
Monoclinic, P21/c Melting point: 373 K
Hall symbol: -P 2ybc Mo Kα radiation, λ = 0.71069 Å
a = 10.328 (6) Å Cell parameters from 2499 reflections
b = 14.256 (9) Å θ = 2.5–29.0°
c = 7.641 (4) Å µ = 0.32 mm1
β = 108.17 (4)° T = 173 K
V = 1068.9 (11) Å3 Block, colourless
Z = 4 0.31 × 0.23 × 0.07 mm

Data collection

Bruker SMART APEXII CCD diffractometer 2841 independent reflections
Radiation source: fine-focus sealed tube 2312 reflections with I > 2σ(I)
graphite Rint = 0.036
ω scans θmax = 29.0°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Bruker, 2003) h = −14→14
Tmin = 0.892, Tmax = 0.977 k = −19→19
9888 measured reflections l = −10→10

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)] = 0.049 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.138 H-atom parameters constrained
S = 1.07 w = 1/[σ2(Fo2) + (0.0653P)2 + 0.8586P] where P = (Fo2 + 2Fc2)/3
2841 reflections (Δ/σ)max = 0.001
154 parameters Δρmax = 1.03 e Å3
0 restraints Δρmin = −0.37 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.Least-squares planes (x,y,z in crystal coordinates) and deviations from them (* indicates atom used to define plane)0.6216 (0.0092) x - 0.3744 (0.0129) y + 7.1009 (0.0056) z = 6.1246 (0.0124)* -0.0042 (0.0015) C1 * 0.0030 (0.0015) C2 * 0.0017 (0.0017) C3 * -0.0051 (0.0016) C4 * 0.0041 (0.0015) C5 * 0.0006 (0.0015) C6 - 0.1026 (0.0029) S1Rms deviation of fitted atoms = 0.00357.3721 (0.0082) x + 9.8314 (0.0114) y - 2.5872 (0.0066) z = 9.1191 (0.0077)Angle to previous plane (with approximate e.s.d.) = 84.43 (0.08)* -0.0002 (0.0014) C7 * -0.0020 (0.0015) C8 * 0.0008 (0.0016) C9 * 0.0026 (0.0016) C10 * -0.0048 (0.0015) C11 * 0.0036 (0.0015) C12 0.1082 (0.0028) S1Rms deviation of fitted atoms = 0.0028
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
S1 0.75260 (5) 0.58823 (4) 0.81320 (7) 0.02008 (16)
F3 1.22708 (15) 0.66341 (11) 0.7875 (2) 0.0422 (4)
F5 0.94947 (16) 0.91584 (10) 0.8343 (2) 0.0382 (4)
O1 0.67321 (17) 0.62902 (12) 0.9183 (2) 0.0278 (4)
O2 0.81161 (17) 0.49637 (11) 0.8585 (2) 0.0283 (4)
C1 0.8867 (2) 0.66759 (14) 0.8195 (3) 0.0186 (4)
C2 1.0092 (2) 0.63183 (15) 0.8079 (3) 0.0231 (4)
H2 1.0244 0.5663 0.8039 0.028*
C3 1.1074 (2) 0.69651 (16) 0.8025 (3) 0.0251 (5)
C4 1.0896 (2) 0.79234 (15) 0.8082 (3) 0.0243 (4)
H4 1.1588 0.8351 0.8029 0.029*
C5 0.9666 (2) 0.82280 (15) 0.8219 (3) 0.0229 (4)
C6 0.8626 (2) 0.76354 (15) 0.8274 (3) 0.0213 (4)
H6 0.7786 0.7869 0.8361 0.026*
C7 0.6541 (2) 0.58940 (14) 0.5789 (3) 0.0180 (4)
C8 0.6894 (2) 0.53032 (15) 0.4556 (3) 0.0231 (4)
H8 0.7620 0.4867 0.4979 0.028*
C9 0.6162 (3) 0.53652 (16) 0.2697 (3) 0.0282 (5)
H9 0.6389 0.4969 0.1836 0.034*
C10 0.5105 (2) 0.60012 (17) 0.2093 (3) 0.0291 (5)
H10 0.4613 0.6041 0.0817 0.035*
C11 0.4758 (2) 0.65775 (17) 0.3324 (3) 0.0269 (5)
H11 0.4022 0.7005 0.2895 0.032*
C12 0.5479 (2) 0.65361 (15) 0.5189 (3) 0.0227 (4)
H12 0.5252 0.6939 0.6041 0.027*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
S1 0.0243 (3) 0.0206 (3) 0.0158 (3) −0.00311 (19) 0.0069 (2) 0.00231 (19)
F3 0.0273 (8) 0.0336 (8) 0.0690 (12) 0.0042 (6) 0.0201 (8) −0.0013 (8)
F5 0.0413 (9) 0.0185 (7) 0.0601 (11) −0.0006 (6) 0.0236 (8) −0.0012 (6)
O1 0.0335 (9) 0.0347 (9) 0.0195 (8) −0.0071 (7) 0.0144 (7) −0.0025 (7)
O2 0.0316 (8) 0.0224 (8) 0.0273 (8) −0.0026 (7) 0.0041 (7) 0.0089 (6)
C1 0.0217 (10) 0.0199 (9) 0.0141 (9) −0.0014 (8) 0.0054 (8) 0.0014 (7)
C2 0.0240 (10) 0.0188 (10) 0.0255 (11) 0.0013 (8) 0.0063 (9) 0.0018 (8)
C3 0.0188 (10) 0.0264 (11) 0.0300 (12) 0.0022 (8) 0.0073 (9) 0.0004 (9)
C4 0.0249 (10) 0.0223 (10) 0.0266 (11) −0.0053 (8) 0.0092 (9) −0.0017 (9)
C5 0.0294 (11) 0.0166 (9) 0.0225 (11) −0.0011 (8) 0.0077 (9) −0.0019 (8)
C6 0.0247 (10) 0.0207 (10) 0.0194 (10) 0.0000 (8) 0.0081 (8) −0.0008 (8)
C7 0.0192 (9) 0.0188 (9) 0.0171 (9) −0.0038 (7) 0.0072 (8) 0.0007 (7)
C8 0.0285 (11) 0.0197 (10) 0.0231 (11) −0.0009 (8) 0.0111 (9) −0.0005 (8)
C9 0.0392 (13) 0.0261 (11) 0.0220 (11) −0.0087 (9) 0.0135 (10) −0.0059 (9)
C10 0.0302 (12) 0.0358 (13) 0.0179 (10) −0.0131 (10) 0.0024 (9) 0.0017 (9)
C11 0.0208 (10) 0.0313 (12) 0.0279 (12) −0.0029 (9) 0.0066 (9) 0.0080 (9)
C12 0.0228 (10) 0.0241 (10) 0.0237 (11) 0.0010 (8) 0.0110 (8) 0.0017 (8)

Geometric parameters (Å, °)

S1—O1 1.4375 (18) C5—C6 1.378 (3)
S1—O2 1.4403 (18) C6—H6 0.9500
S1—C7 1.762 (2) C7—C12 1.392 (3)
S1—C1 1.777 (2) C7—C8 1.394 (3)
F3—C3 1.361 (3) C8—C9 1.388 (3)
F5—C5 1.346 (3) C8—H8 0.9500
C1—C2 1.392 (3) C9—C10 1.383 (4)
C1—C6 1.395 (3) C9—H9 0.9500
C2—C3 1.381 (3) C10—C11 1.378 (4)
C2—H2 0.9500 C10—H10 0.9500
C3—C4 1.381 (3) C11—C12 1.388 (3)
C4—C5 1.377 (3) C11—H11 0.9500
C4—H4 0.9500 C12—H12 0.9500
O1—S1—O2 120.39 (10) C5—C6—C1 116.6 (2)
O1—S1—C7 108.34 (11) C5—C6—H6 121.7
O2—S1—C7 108.65 (10) C1—C6—H6 121.7
O1—S1—C1 107.63 (10) C12—C7—C8 121.3 (2)
O2—S1—C1 107.72 (11) C12—C7—S1 119.13 (16)
C7—S1—C1 102.68 (10) C8—C7—S1 119.42 (17)
C2—C1—C6 122.68 (19) C9—C8—C7 118.7 (2)
C2—C1—S1 118.76 (16) C9—C8—H8 120.7
C6—C1—S1 118.50 (16) C7—C8—H8 120.7
C3—C2—C1 116.6 (2) C10—C9—C8 120.3 (2)
C3—C2—H2 121.7 C10—C9—H9 119.9
C1—C2—H2 121.7 C8—C9—H9 119.9
F3—C3—C4 118.6 (2) C11—C10—C9 120.6 (2)
F3—C3—C2 117.8 (2) C11—C10—H10 119.7
C4—C3—C2 123.6 (2) C9—C10—H10 119.7
C5—C4—C3 116.7 (2) C10—C11—C12 120.4 (2)
C5—C4—H4 121.7 C10—C11—H11 119.8
C3—C4—H4 121.7 C12—C11—H11 119.8
F5—C5—C4 117.46 (19) C11—C12—C7 118.8 (2)
F5—C5—C6 118.8 (2) C11—C12—H12 120.6
C4—C5—C6 123.8 (2) C7—C12—H12 120.6
O1—S1—C1—C2 150.34 (17) C2—C1—C6—C5 0.4 (3)
O2—S1—C1—C2 19.1 (2) S1—C1—C6—C5 −176.56 (16)
C7—S1—C1—C2 −95.46 (18) O1—S1—C7—C12 22.96 (19)
O1—S1—C1—C6 −32.6 (2) O2—S1—C7—C12 155.37 (16)
O2—S1—C1—C6 −163.77 (16) C1—S1—C7—C12 −90.72 (18)
C7—S1—C1—C6 81.64 (18) O1—S1—C7—C8 −161.09 (16)
C6—C1—C2—C3 −0.6 (3) O2—S1—C7—C8 −28.68 (19)
S1—C1—C2—C3 176.34 (17) C1—S1—C7—C8 85.23 (18)
C1—C2—C3—F3 −178.7 (2) C12—C7—C8—C9 0.0 (3)
C1—C2—C3—C4 0.1 (3) S1—C7—C8—C9 −175.82 (16)
F3—C3—C4—C5 179.5 (2) C7—C8—C9—C10 −0.1 (3)
C2—C3—C4—C5 0.7 (4) C8—C9—C10—C11 −0.3 (3)
C3—C4—C5—F5 177.6 (2) C9—C10—C11—C12 0.9 (3)
C3—C4—C5—C6 −0.9 (3) C10—C11—C12—C7 −0.9 (3)
F5—C5—C6—C1 −178.16 (19) C8—C7—C12—C11 0.5 (3)
C4—C5—C6—C1 0.4 (3) S1—C7—C12—C11 176.35 (16)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
C2—H2···F5i 0.95 2.44 3.337 (3) 157

Symmetry codes: (i) −x+2, y−1/2, −z+3/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: HB2817).

References

  1. Allen, F. H., Johnson, O., Shields, G. P., Smith, B. R. & Towler, M. (2004). J. Appl. Cryst.37, 335–338.
  2. Attwood, T. E., Barr, D. A., Feasey, G. G., Leslie, V. J., Newton, A. B. & Rose, J. B. (1977). Polymer18, 354–358.
  3. Bruker (2003). SMART and SAINT-Plus Bruker AXS Inc., Madison, Wisconsin, USA.
  4. Johnson, R. N., Farnham, A. G., Clendinning, R., Hale, W. F. & Merriam, C. N. (1967). J. Polym. Sci. Part. A Polym. Chem.5, 2375–2398.
  5. Kaiti, S., Himmelberg, P., Williams, J., Abdellatif, M. & Fossum, E. (2006). Macromolecules, 39, 7909–7914.
  6. Macrae, C. F., Edgington, P. R., McCabe, P., Pidcock, E., Shields, G. P., Taylor, R., Towler, M. & van de Streek, J. (2006). J. Appl. Cryst.39, 453–457.
  7. McArdle, P. (1995). J. Appl. Cryst.28, 65. [DOI] [PMC free article] [PubMed]
  8. Salamon, J. C. (1999). Editor. Concise Polymeric Materials Encyclopedia Boca Raton: CRC Press LLC.
  9. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  10. Westrip, S. P. (2008). publCIF In preparation.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808034302/hb2817sup1.cif

e-64-o2207-sup1.cif (17KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536808034302/hb2817Isup2.hkl

e-64-o2207-Isup2.hkl (139.5KB, hkl)

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


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