Download citation
Download citation
link to html
In the title compound, C24H16F2O5S2, the benzene rings of the central oxydibenzene unit are inclined at an angle of 83.49 (8)° to one another. Each of these benzene rings carries a p-substituted 4-fluoro­sulfonyl­benzene group with dihedral angles of 77.27 (8) and 62.06 (11)° between the respective 4-fluoro­sulfonyl­benzene and oxydibenzene rings. In the crystal structure, a complex network of C—H...F and C—H...O hydrogen bonds and a C—H...π inter­action link the mol­ecules into columns along the bc diagonal.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807047204/gw2026sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807047204/gw2026Isup2.hkl
Contains datablock I

CCDC reference: 667293

Key indicators

  • Single-crystal X-ray study
  • T = 180 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.039
  • wR factor = 0.096
  • Data-to-parameter ratio = 9.2

checkCIF/PLATON results

No syntax errors found




Alert level A THETM01_ALERT_3_A The value of sine(theta_max)/wavelength is less than 0.550 Calculated sin(theta_max)/wavelength = 0.5366 PLAT023_ALERT_3_A Resolution (too) Low [sin(th)/Lambda < 0.6]..... 22.42 Deg. PLAT027_ALERT_3_A _diffrn_reflns_theta_full (too) Low ............ 22.42 Deg.
Alert level C REFNR01_ALERT_3_C Ratio of reflections to parameters is < 10 for a centrosymmetric structure sine(theta)/lambda 0.5366 Proportion of unique data used 1.0000 Ratio reflections to parameters 9.1812 PLAT062_ALERT_4_C Rescale T(min) & T(max) by ..................... 0.99 PLAT088_ALERT_3_C Poor Data / Parameter Ratio .................... 9.18 PLAT480_ALERT_4_C Long H...A H-Bond Reported H11A .. F1 .. 2.67 Ang. PLAT480_ALERT_4_C Long H...A H-Bond Reported H23A .. F1 .. 2.65 Ang.
3 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 5 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 0 ALERT type 2 Indicator that the structure model may be wrong or deficient 5 ALERT type 3 Indicator that the structure quality may be low 3 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

Polysulphones are an important class of high temperature thermoplastics. The properties of these polymers are dependent on the flexibility of the chain (for the glass transition temperature) and any crystallinity (for the melting point transition) (Carlier et al., 1992). An important method of obtaining and refining the X-ray structure for any polymer is by using the X-ray structure of related oligomers (Colquhoun et al., 2003), thus any information on the packing motifs of extended oligomers is very useful. During the preparation of a polysulfone dendrimer, the title compound was obtained as a minor impurity. It probably arose from the nucleophilic attack of trace amounts of water on 4-fluorophenylsulfone under the reaction conditions (160 °C in DMSO).

The benzene rings of the central oxydibenzene unit are inclined at an angle of 83.49 (8)° to one another. Each of these benzene rings carries a p-substituted 4-fluorosulfonylbenzene system with dihedral angles of 77.27 (8)° and 62.06 (11)° between the C1···C6 & C7···C9 and between the C13···C18 & C19···C24 rings respectively.

In the crystal structure, a complex network of C—H···F, C—H···O hydrogen bonds and a C11—H11A···Cg1vii π-interaction link the molecules into columns along the bc diagonal (Cg1 is the centroid of the C1···C6 ring; iv = x, -y + 1/2, z + 1/2), Table 1.

Related literature top

For details of structure–property relationships of crystalline polysulfones, see Carlier et al. (1992), and for information on structure determinations of polymers from powder data, see Colquhoun et al. (2003). For related structures, see for example Colquhoun et al. (2005, 2002) and Holman et al. (2001).

Experimental top

To a solution of a generation 1 polysulfone dendrimer (0.50 g, 0.6 mmol) and 4-fluorophenyl sulphone (3.08 g, 12.1 mmol) in anhydrous DMSO (40 ml) was added Na2CO3 (0.26 g, 2.4 mmol). The mixture was heated under nitrogen at 160 °C for 5 h, water (60 ml) was added and the mixture extracted with ethyl acetate (3 x 40 ml). The combined extracts were then dried over magnesium sulfate, filtered and concentrated in vacuo. Column chromatography using 80:20 hexane:ethyl acetate yielded 0.02 g (1%) of a white solid, the title compound (I). Rf (hexane:ethyl acetate 1:1) 0.80; m.p 140–142 °C; IR (KBr) 2900, 1750, 1590, 1505, 1490, 1410, 1300, 1250, 1150, 1010 cm-1; 1H NMR (400 MHz) δ (CDCl3) 7.96–7.88 (m, 4H, H-3, H-6), 7.18 (t, 2H, H-2, 3JHH = 8.5 Hz), 7.08 (d, 2H, H-7, 3JHH = 9.0 Hz). Colourles needles were obtained by layering a solution in ethyl acetate with hexane.

Refinement top

The crystals were small and very weakly diffracting so that high angle reflections were not obtained beyond θ(max) = 22.5°. All H-atoms were positioned geometrically and refined using a riding model with d(C—H) = 0.95 Å, Uiso = 1.2Ueq (C).

Structure description top

Polysulphones are an important class of high temperature thermoplastics. The properties of these polymers are dependent on the flexibility of the chain (for the glass transition temperature) and any crystallinity (for the melting point transition) (Carlier et al., 1992). An important method of obtaining and refining the X-ray structure for any polymer is by using the X-ray structure of related oligomers (Colquhoun et al., 2003), thus any information on the packing motifs of extended oligomers is very useful. During the preparation of a polysulfone dendrimer, the title compound was obtained as a minor impurity. It probably arose from the nucleophilic attack of trace amounts of water on 4-fluorophenylsulfone under the reaction conditions (160 °C in DMSO).

The benzene rings of the central oxydibenzene unit are inclined at an angle of 83.49 (8)° to one another. Each of these benzene rings carries a p-substituted 4-fluorosulfonylbenzene system with dihedral angles of 77.27 (8)° and 62.06 (11)° between the C1···C6 & C7···C9 and between the C13···C18 & C19···C24 rings respectively.

In the crystal structure, a complex network of C—H···F, C—H···O hydrogen bonds and a C11—H11A···Cg1vii π-interaction link the molecules into columns along the bc diagonal (Cg1 is the centroid of the C1···C6 ring; iv = x, -y + 1/2, z + 1/2), Table 1.

For details of structure–property relationships of crystalline polysulfones, see Carlier et al. (1992), and for information on structure determinations of polymers from powder data, see Colquhoun et al. (2003). For related structures, see for example Colquhoun et al. (2005, 2002) and Holman et al. (2001).

Computing details top

Data collection: COLLECT (Nonius, 1998); cell refinement: SCALEPACK (Otwinowski & Minor, 1997); data reduction: SCALEPACK and DENZO (Otwinowski & Minor, 1997); program(s) used to solve structure: SIR92 (Altomare et al., 1993); program(s) used to refine structure: SHELXL97 (Sheldrick 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: SHELXL97 (Sheldrick 1997), enCIFer (Allen et al., 2004) and PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. The structure of (I) showing the atom numbering with ellipsoids drawn at the 50% probability level.
[Figure 2] Fig. 2. Crystal packing for (I) with hydrogen bonds drawn as dashed lines.
4,4'-Bis(4-fluorophenylsulfonyl)oxydibenzene top
Crystal data top
C24H16F2O5S2F(000) = 1000
Mr = 486.49Dx = 1.517 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 6093 reflections
a = 14.0437 (6) Åθ = 1.0–22.5°
b = 16.0590 (6) ŵ = 0.30 mm1
c = 9.6644 (3) ÅT = 180 K
β = 102.223 (1)°Needle, colourless
V = 2130.18 (14) Å30.23 × 0.07 × 0.05 mm
Z = 4
Data collection top
Nonius KappaCCD
diffractometer
2736 independent reflections
Radiation source: fine-focus sealed tube2084 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.055
Thin–slice ω and φ scansθmax = 22.4°, θmin = 3.5°
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
h = 1515
Tmin = 0.954, Tmax = 0.996k = 1716
10006 measured reflectionsl = 1010
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.039Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.096H-atom parameters constrained
S = 1.06 w = 1/[σ2(Fo2) + (0.0393P)2 + 0.9105P]
where P = (Fo2 + 2Fc2)/3
2736 reflections(Δ/σ)max < 0.001
298 parametersΔρmax = 0.28 e Å3
0 restraintsΔρmin = 0.34 e Å3
Crystal data top
C24H16F2O5S2V = 2130.18 (14) Å3
Mr = 486.49Z = 4
Monoclinic, P21/cMo Kα radiation
a = 14.0437 (6) ŵ = 0.30 mm1
b = 16.0590 (6) ÅT = 180 K
c = 9.6644 (3) Å0.23 × 0.07 × 0.05 mm
β = 102.223 (1)°
Data collection top
Nonius KappaCCD
diffractometer
2736 independent reflections
Absorption correction: multi-scan
(SORTAV; Blessing, 1995)
2084 reflections with I > 2σ(I)
Tmin = 0.954, Tmax = 0.996Rint = 0.055
10006 measured reflectionsθmax = 22.4°
Refinement top
R[F2 > 2σ(F2)] = 0.0390 restraints
wR(F2) = 0.096H-atom parameters constrained
S = 1.06Δρmax = 0.28 e Å3
2736 reflectionsΔρmin = 0.34 e Å3
298 parameters
Special details top

Experimental. Poorly diffracting crystals (ThetaMax=22.5 degrees).

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) top
xyzUiso*/Ueq
S10.13021 (6)0.01325 (5)0.26488 (8)0.0311 (3)
S20.48394 (6)0.32919 (6)0.15358 (8)0.0318 (3)
O10.21631 (15)0.01428 (14)0.2205 (2)0.0387 (6)
O20.06039 (15)0.04715 (13)0.2910 (2)0.0364 (6)
O30.06855 (15)0.26534 (14)0.1351 (2)0.0386 (6)
O40.48671 (16)0.35984 (15)0.0145 (2)0.0428 (6)
O50.53284 (15)0.25302 (14)0.2019 (2)0.0439 (6)
F10.25344 (14)0.20090 (14)0.79030 (19)0.0568 (6)
F20.65833 (17)0.59150 (16)0.5413 (2)0.0847 (8)
C10.2260 (2)0.1570 (2)0.6682 (3)0.0370 (9)
C20.1336 (2)0.1256 (2)0.6377 (3)0.0406 (9)
H2A0.09070.13340.70050.049*
C30.1043 (2)0.0820 (2)0.5124 (3)0.0341 (8)
H3A0.04040.05960.48790.041*
C40.1681 (2)0.0710 (2)0.4232 (3)0.0285 (8)
C50.2618 (2)0.1028 (2)0.4580 (3)0.0347 (9)
H5A0.30560.09440.39670.042*
C60.2913 (2)0.1470 (2)0.5834 (3)0.0394 (9)
H6A0.35510.16960.60920.047*
C70.0686 (2)0.08542 (19)0.1416 (3)0.0266 (8)
C80.0317 (2)0.0945 (2)0.1237 (3)0.0309 (8)
H8A0.06700.05990.17470.037*
C90.0800 (2)0.1539 (2)0.0319 (3)0.0316 (8)
H9A0.14840.16070.01970.038*
C100.0276 (2)0.2034 (2)0.0422 (3)0.0275 (8)
C110.0724 (2)0.1941 (2)0.0261 (3)0.0306 (8)
H11A0.10750.22840.07800.037*
C120.1202 (2)0.1350 (2)0.0651 (3)0.0314 (8)
H12A0.18860.12790.07610.038*
C130.1672 (2)0.2833 (2)0.1457 (3)0.0308 (8)
C140.1924 (2)0.3476 (2)0.0666 (3)0.0367 (9)
H14A0.14350.38030.00810.044*
C150.2898 (2)0.3641 (2)0.0732 (3)0.0372 (9)
H15A0.30830.40790.01820.045*
C160.3603 (2)0.31666 (19)0.1601 (3)0.0266 (8)
C170.3337 (2)0.2549 (2)0.2444 (3)0.0336 (8)
H17A0.38230.22460.30790.040*
C180.2363 (2)0.2377 (2)0.2360 (3)0.0337 (8)
H18A0.21730.19470.29210.040*
C190.5321 (2)0.4080 (2)0.2748 (3)0.0285 (8)
C200.5202 (2)0.4902 (2)0.2328 (3)0.0392 (9)
H20A0.48360.50370.14120.047*
C210.5614 (3)0.5524 (2)0.3236 (4)0.0483 (10)
H21A0.55270.60930.29690.058*
C220.6147 (3)0.5304 (3)0.4519 (4)0.0495 (11)
C230.6269 (2)0.4498 (3)0.4990 (4)0.0481 (10)
H23A0.66350.43720.59100.058*
C240.5846 (2)0.3878 (2)0.4090 (3)0.0387 (9)
H24A0.59120.33130.43840.046*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0289 (5)0.0299 (5)0.0332 (5)0.0017 (4)0.0037 (4)0.0001 (4)
S20.0277 (5)0.0332 (6)0.0339 (5)0.0006 (4)0.0049 (4)0.0033 (4)
O10.0299 (13)0.0412 (15)0.0465 (13)0.0085 (11)0.0112 (11)0.0047 (11)
O20.0341 (13)0.0312 (14)0.0415 (13)0.0064 (11)0.0029 (10)0.0002 (11)
O30.0299 (14)0.0460 (16)0.0406 (13)0.0055 (12)0.0090 (10)0.0136 (11)
O40.0412 (14)0.0584 (17)0.0304 (12)0.0075 (13)0.0112 (10)0.0024 (11)
O50.0329 (13)0.0313 (15)0.0652 (15)0.0065 (12)0.0048 (11)0.0052 (12)
F10.0491 (13)0.0766 (17)0.0446 (12)0.0151 (12)0.0096 (10)0.0244 (11)
F20.0787 (17)0.090 (2)0.0900 (17)0.0365 (15)0.0284 (14)0.0590 (16)
C10.038 (2)0.041 (2)0.0298 (19)0.0054 (18)0.0020 (17)0.0033 (16)
C20.038 (2)0.048 (2)0.039 (2)0.0067 (19)0.0164 (16)0.0064 (18)
C30.0279 (19)0.034 (2)0.0409 (19)0.0040 (16)0.0087 (16)0.0009 (16)
C40.0277 (19)0.028 (2)0.0284 (17)0.0005 (16)0.0024 (15)0.0021 (14)
C50.0267 (19)0.042 (2)0.0367 (19)0.0009 (17)0.0092 (15)0.0020 (17)
C60.0261 (19)0.050 (2)0.040 (2)0.0070 (18)0.0027 (16)0.0015 (18)
C70.0252 (19)0.027 (2)0.0269 (16)0.0006 (15)0.0033 (14)0.0038 (14)
C80.0274 (19)0.038 (2)0.0286 (17)0.0045 (16)0.0086 (14)0.0002 (16)
C90.0193 (17)0.045 (2)0.0304 (17)0.0031 (17)0.0051 (14)0.0017 (17)
C100.028 (2)0.030 (2)0.0238 (16)0.0020 (16)0.0036 (14)0.0003 (15)
C110.0254 (19)0.038 (2)0.0302 (17)0.0028 (16)0.0088 (14)0.0003 (16)
C120.0228 (18)0.037 (2)0.0338 (18)0.0001 (17)0.0040 (15)0.0034 (16)
C130.0248 (19)0.041 (2)0.0265 (17)0.0019 (17)0.0059 (15)0.0082 (16)
C140.030 (2)0.042 (2)0.0357 (18)0.0065 (17)0.0017 (15)0.0091 (17)
C150.033 (2)0.038 (2)0.041 (2)0.0004 (18)0.0082 (16)0.0093 (17)
C160.0307 (19)0.023 (2)0.0245 (16)0.0006 (15)0.0014 (14)0.0026 (15)
C170.038 (2)0.030 (2)0.0303 (17)0.0003 (17)0.0019 (15)0.0025 (16)
C180.037 (2)0.031 (2)0.0350 (19)0.0043 (17)0.0109 (16)0.0034 (16)
C190.0231 (17)0.030 (2)0.0334 (18)0.0038 (16)0.0092 (14)0.0007 (16)
C200.043 (2)0.037 (2)0.0411 (19)0.0020 (19)0.0153 (17)0.0013 (18)
C210.053 (2)0.034 (2)0.064 (3)0.010 (2)0.026 (2)0.005 (2)
C220.038 (2)0.056 (3)0.059 (3)0.016 (2)0.020 (2)0.033 (2)
C230.036 (2)0.071 (3)0.035 (2)0.000 (2)0.0025 (16)0.011 (2)
C240.035 (2)0.046 (2)0.0335 (19)0.0066 (18)0.0026 (16)0.0006 (17)
Geometric parameters (Å, º) top
S1—O11.436 (2)C9—C101.382 (4)
S1—O21.439 (2)C9—H9A0.9500
S1—C71.754 (3)C10—C111.387 (4)
S1—C41.772 (3)C11—C121.370 (4)
S2—O51.432 (2)C11—H11A0.9500
S2—O41.440 (2)C12—H12A0.9500
S2—C191.759 (3)C13—C181.372 (4)
S2—C161.762 (3)C13—C141.376 (5)
O3—C101.381 (4)C14—C151.381 (4)
O3—C131.397 (4)C14—H14A0.9500
F1—C11.359 (4)C15—C161.384 (4)
F2—C221.363 (4)C15—H15A0.9500
C1—C61.362 (4)C16—C171.384 (4)
C1—C21.365 (4)C17—C181.382 (4)
C2—C31.383 (4)C17—H17A0.9500
C2—H2A0.9500C18—H18A0.9500
C3—C41.380 (4)C19—C201.381 (5)
C3—H3A0.9500C19—C241.387 (4)
C4—C51.384 (4)C20—C211.374 (5)
C5—C61.390 (4)C20—H20A0.9500
C5—H5A0.9500C21—C221.353 (5)
C6—H6A0.9500C21—H21A0.9500
C7—C81.390 (4)C22—C231.372 (5)
C7—C121.391 (4)C23—C241.371 (5)
C8—C91.379 (4)C23—H23A0.9500
C8—H8A0.9500C24—H24A0.9500
O1—S1—O2119.54 (14)C12—C11—C10119.6 (3)
O1—S1—C7109.04 (14)C12—C11—H11A120.2
O2—S1—C7107.93 (13)C10—C11—H11A120.2
O1—S1—C4107.54 (14)C11—C12—C7119.9 (3)
O2—S1—C4107.03 (14)C11—C12—H12A120.1
C7—S1—C4104.80 (14)C7—C12—H12A120.1
O5—S2—O4119.39 (15)C18—C13—C14121.6 (3)
O5—S2—C19107.87 (14)C18—C13—O3119.6 (3)
O4—S2—C19107.08 (15)C14—C13—O3118.8 (3)
O5—S2—C16107.39 (14)C13—C14—C15119.2 (3)
O4—S2—C16107.11 (13)C13—C14—H14A120.4
C19—S2—C16107.50 (14)C15—C14—H14A120.4
C10—O3—C13117.9 (2)C14—C15—C16119.7 (3)
F1—C1—C6118.7 (3)C14—C15—H15A120.1
F1—C1—C2117.5 (3)C16—C15—H15A120.1
C6—C1—C2123.8 (3)C17—C16—C15120.3 (3)
C1—C2—C3118.0 (3)C17—C16—S2119.6 (2)
C1—C2—H2A121.0C15—C16—S2119.9 (2)
C3—C2—H2A121.0C18—C17—C16119.8 (3)
C4—C3—C2120.0 (3)C18—C17—H17A120.1
C4—C3—H3A120.0C16—C17—H17A120.1
C2—C3—H3A120.0C13—C18—C17119.3 (3)
C3—C4—C5120.7 (3)C13—C18—H18A120.4
C3—C4—S1119.4 (2)C17—C18—H18A120.4
C5—C4—S1119.9 (2)C20—C19—C24120.3 (3)
C4—C5—C6119.5 (3)C20—C19—S2119.1 (2)
C4—C5—H5A120.2C24—C19—S2120.5 (3)
C6—C5—H5A120.2C21—C20—C19120.0 (3)
C1—C6—C5118.1 (3)C21—C20—H20A120.0
C1—C6—H6A121.0C19—C20—H20A120.0
C5—C6—H6A121.0C22—C21—C20118.1 (4)
C8—C7—C12120.2 (3)C22—C21—H21A120.9
C8—C7—S1119.7 (2)C20—C21—H21A120.9
C12—C7—S1120.1 (2)C21—C22—F2118.7 (4)
C9—C8—C7120.0 (3)C21—C22—C23123.8 (3)
C9—C8—H8A120.0F2—C22—C23117.5 (4)
C7—C8—H8A120.0C24—C23—C22117.9 (3)
C8—C9—C10119.2 (3)C24—C23—H23A121.0
C8—C9—H9A120.4C22—C23—H23A121.0
C10—C9—H9A120.4C23—C24—C19119.8 (3)
O3—C10—C9123.8 (3)C23—C24—H24A120.1
O3—C10—C11115.0 (3)C19—C24—H24A120.1
C9—C10—C11121.2 (3)
F1—C1—C2—C3178.9 (3)C10—O3—C13—C1885.5 (3)
C6—C1—C2—C30.9 (5)C10—O3—C13—C1495.6 (4)
C1—C2—C3—C40.3 (5)C18—C13—C14—C153.1 (5)
C2—C3—C4—C50.5 (5)O3—C13—C14—C15178.0 (3)
C2—C3—C4—S1178.7 (3)C13—C14—C15—C160.8 (5)
O1—S1—C4—C3159.3 (3)C14—C15—C16—C172.5 (5)
O2—S1—C4—C329.7 (3)C14—C15—C16—S2172.6 (2)
C7—S1—C4—C384.8 (3)O5—S2—C16—C1719.8 (3)
O1—S1—C4—C518.9 (3)O4—S2—C16—C17149.1 (2)
O2—S1—C4—C5148.6 (3)C19—S2—C16—C1796.1 (3)
C7—S1—C4—C597.0 (3)O5—S2—C16—C15155.3 (2)
C3—C4—C5—C60.8 (5)O4—S2—C16—C1526.0 (3)
S1—C4—C5—C6179.1 (2)C19—S2—C16—C1588.8 (3)
F1—C1—C6—C5179.2 (3)C15—C16—C17—C183.5 (5)
C2—C1—C6—C50.5 (5)S2—C16—C17—C18171.6 (2)
C4—C5—C6—C10.4 (5)C14—C13—C18—C172.1 (5)
O1—S1—C7—C8152.6 (2)O3—C13—C18—C17179.0 (3)
O2—S1—C7—C821.3 (3)C16—C17—C18—C131.3 (5)
C4—S1—C7—C892.5 (3)O5—S2—C19—C20160.3 (2)
O1—S1—C7—C1229.3 (3)O4—S2—C19—C2030.7 (3)
O2—S1—C7—C12160.6 (2)C16—S2—C19—C2084.1 (3)
C4—S1—C7—C1285.6 (3)O5—S2—C19—C2417.1 (3)
C12—C7—C8—C91.2 (4)O4—S2—C19—C24146.8 (2)
S1—C7—C8—C9176.9 (2)C16—S2—C19—C2498.4 (3)
C7—C8—C9—C100.5 (5)C24—C19—C20—C210.7 (5)
C13—O3—C10—C95.3 (4)S2—C19—C20—C21176.8 (3)
C13—O3—C10—C11174.0 (3)C19—C20—C21—C221.3 (5)
C8—C9—C10—O3179.0 (3)C20—C21—C22—F2178.1 (3)
C8—C9—C10—C110.2 (5)C20—C21—C22—C232.6 (6)
O3—C10—C11—C12179.1 (3)C21—C22—C23—C241.7 (6)
C9—C10—C11—C120.2 (5)F2—C22—C23—C24179.0 (3)
C10—C11—C12—C70.6 (5)C22—C23—C24—C190.4 (5)
C8—C7—C12—C111.3 (4)C20—C19—C24—C231.6 (5)
S1—C7—C12—C11176.9 (2)S2—C19—C24—C23175.8 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H2A···O2i0.952.553.206 (4)126
C6—H6A···O5ii0.952.533.337 (4)143
C14—H14A···O2iii0.952.473.361 (4)157
C17—H17A···O4iv0.952.603.529 (4)168
C11—H11A···F1v0.952.673.396 (4)134
C23—H23A···F1vi0.952.653.373 (5)133
C11—H11A···Cg1iv0.952.973.541 (3)120
Symmetry codes: (i) x, y, z1; (ii) x1, y, z1; (iii) x, y+1/2, z1/2; (iv) x, y+1/2, z+1/2; (v) x, y, z+1; (vi) x+1, y+1/2, z+3/2.

Experimental details

Crystal data
Chemical formulaC24H16F2O5S2
Mr486.49
Crystal system, space groupMonoclinic, P21/c
Temperature (K)180
a, b, c (Å)14.0437 (6), 16.0590 (6), 9.6644 (3)
β (°) 102.223 (1)
V3)2130.18 (14)
Z4
Radiation typeMo Kα
µ (mm1)0.30
Crystal size (mm)0.23 × 0.07 × 0.05
Data collection
DiffractometerNonius KappaCCD
Absorption correctionMulti-scan
(SORTAV; Blessing, 1995)
Tmin, Tmax0.954, 0.996
No. of measured, independent and
observed [I > 2σ(I)] reflections
10006, 2736, 2084
Rint0.055
θmax (°)22.4
(sin θ/λ)max1)0.537
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.039, 0.096, 1.06
No. of reflections2736
No. of parameters298
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.28, 0.34

Computer programs: COLLECT (Nonius, 1998), SCALEPACK (Otwinowski & Minor, 1997), SCALEPACK and DENZO (Otwinowski & Minor, 1997), SIR92 (Altomare et al., 1993), ORTEP-3 (Farrugia, 1997), SHELXL97 (Sheldrick 1997), enCIFer (Allen et al., 2004) and PLATON (Spek, 2003).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H2A···O2i0.952.553.206 (4)126.4
C6—H6A···O5ii0.952.533.337 (4)143.2
C14—H14A···O2iii0.952.473.361 (4)156.8
C17—H17A···O4iv0.952.603.529 (4)167.6
C11—H11A···F1v0.952.673.396 (4)133.8
C23—H23A···F1vi0.952.653.373 (5)133.2
C11—H11A···Cg1iv0.952.973.541 (3)120
Symmetry codes: (i) x, y, z1; (ii) x1, y, z1; (iii) x, y+1/2, z1/2; (iv) x, y+1/2, z+1/2; (v) x, y, z+1; (vi) x+1, y+1/2, z+3/2.
 

Follow Acta Cryst. E
Sign up for e-alerts
Follow Acta Cryst. on Twitter
Follow us on facebook
Sign up for RSS feeds