Abstract
The molecule of the title compound, C25H20N2OS2, has imposed twofold rotation symmetry. The dihedral angle formed by the two crystallographically independent phenyl rings is 79.23 (7)°. In the crystal packing, the molecules are linked by intermolecular N—H⋯O hydrogen bonds, forming chains running parallel to [102].
Related literature
For the properties and applications of the title compound and related derivatives, see: Wang et al. (2006a
▶,b
▶); Jiang et al. (2006 ▶); Aritomi & Terauchi (1985 ▶); Aritomi & Fujiwara (1986 ▶). For the synthesis of the title compound, see: Yang et al. (2007 ▶); Chen et al. (2009 ▶).
Experimental
Crystal data
C25H20N2OS2
M r = 428.55
Monoclinic,
a = 18.945 (3) Å
b = 6.025 (2) Å
c = 20.793 (5) Å
β = 110.64 (4)°
V = 2221.1 (11) Å3
Z = 4
Mo Kα radiation
μ = 0.26 mm−1
T = 292 K
0.52 × 0.48 × 0.42 mm
Data collection
Enraf–Nonius CAD-4 diffractometer
Absorption correction: spherical (WinGX; Farrugia, 1999 ▶) T min = 0.877, T max = 0.899
2261 measured reflections
1990 independent reflections
1441 reflections with I > 2σ(I)
R int = 0.010
3 standard reflections every 150 reflections intensity decay: 2.4%
Refinement
R[F 2 > 2σ(F 2)] = 0.050
wR(F 2) = 0.146
S = 1.05
1990 reflections
145 parameters
H atoms treated by a mixture of independent and constrained refinement
Δρmax = 0.22 e Å−3
Δρmin = −0.30 e Å−3
Data collection: DIFRAC (Gabe et al., 1993 ▶); cell refinement: DIFRAC; data reduction: NRCVAX (Gabe et al., 1989 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997 ▶); software used to prepare material for publication: SHELXL97.
Supplementary Material
Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536809016948/rz2311sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809016948/rz2311Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report
Table 1. Hydrogen-bond geometry (Å, °).
| D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A |
|---|---|---|---|---|
| N1—HN2⋯O1i | 0.77 (3) | 2.52 (3) | 3.231 (4) | 154 (3) |
Symmetry code: (i)
.
Acknowledgments
The authors thank Mr Zhi-Hua Mao of Sichuan University for the X-ray data collection.
supplementary crystallographic information
Comment
The title compound is a major active photo-initiator used in coatings, optics and microelectronic materials (Wang et al., 2006a,b; Jiang et al., 2006) and can be used as monomer in the synthesis of high performance polyamide. Moreover, as photo initiator it has showed superior to the natural compound 4,4'-difluorobenzophenone (Wang et al., 2006a). Besides their properties as photo-initiators, some derivatives of the title compound have also been reported to possess good thermostability and chemical resistance (Aritomi & Terauchi, 1985; Aritomi & Fujiwara, 1986). The synthetic procedure of the title compound have been reported elsewhere (Yang et al., 2007; Chen et al., 2009).
The molecule of the title compound (Fig. 1) has crystallographically imposed twofold rotation symmetry. In the asymmetric unit, the phenyl rings form a dihedral angle of 79.23 (7)°. The C2–C1–C2i–C7i torsion angle is 29.49 (15)° (symmetry code: i = 1-x, y, 1/2-z). In the crystal packing, intermolecular N—H···O hydrogen bonding interactions (Table 1) link the molecules into chains running parallel to the [102] direction.
Experimental
A mixture of 4,4'-difluorobenzophenone (21.8 g, 0.1 mol), 4-aminothiophenol (25 g, 0.2 mol), K2CO3 (14.0 g, 0.101 mol) and dimethyl acetamide (120 ml) were charged into a three-necked round-bottomed flask fitted with a mechanical stirrer, a thermometer and a nitrogen inlet. The mixture was stirred vigorously at 120°C for 3 h, then the mixture was heated to 166°C and kept for 5 h under nitrogen atmosphere. After the reactor was cooled to room temperature, the reaction solution was poured into water. The resulting solid was filtered, washed with hot water and methanol, dried and recrystallized from a mixture of dimethyl formamide and water (3:1 v/v) to get a yellow powder. Light yellow crystals suitable for X-ray analysis were obtained by slow evaporation of a formamide/water (3:1 v/v) solution at 60°C.
Refinement
The H atoms bound to the N atom were found in a difference Fourier map and refined freely. All other H atoms were positioned geometrically and refined using a riding model, with C—H = 0.93 Å and Uiso(H) = 1.2Ueq (C).
Figures
Fig. 1.
The molecular structure of the title compound. Unlabelled atoms are related to the labelled atoms by the symmetry operator (1-x, y, 1/2-z).
Crystal data
| C25H20N2OS2 | F(000) = 896 |
| Mr = 428.55 | Dx = 1.282 Mg m−3 |
| Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
| Hall symbol: -C 2yc | Cell parameters from 31 reflections |
| a = 18.945 (3) Å | θ = 4.3–9.4° |
| b = 6.025 (2) Å | µ = 0.26 mm−1 |
| c = 20.793 (5) Å | T = 292 K |
| β = 110.64 (4)° | Block, yellow |
| V = 2221.1 (11) Å3 | 0.52 × 0.48 × 0.42 mm |
| Z = 4 |
Data collection
| Enraf–Nonius CAD-4 diffractometer | 1441 reflections with I > 2σ(I) |
| Radiation source: fine-focus sealed tube | Rint = 0.010 |
| graphite | θmax = 25.5°, θmin = 2.1° |
| ω–2θ scans | h = −22→21 |
| Absorption correction: for a sphere (WinGX; Farrugia, 1999) | k = 0→7 |
| Tmin = 0.877, Tmax = 0.899 | l = −18→24 |
| 2261 measured reflections | 3 standard reflections every 150 reflections |
| 1990 independent reflections | intensity decay: 2.4% |
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)] = 0.050 | Hydrogen site location: mixed |
| wR(F2) = 0.146 | H atoms treated by a mixture of independent and constrained refinement |
| S = 1.05 | w = 1/[σ2(Fo2) + (0.0979P)2 + 0.2492P] where P = (Fo2 + 2Fc2)/3 |
| 1990 reflections | (Δ/σ)max = 0.001 |
| 145 parameters | Δρmax = 0.22 e Å−3 |
| 0 restraints | Δρmin = −0.30 e Å−3 |
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 > 2σ(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 | 0.59611 (4) | 0.88028 (12) | 0.52196 (3) | 0.0591 (3) | |
| O1 | 0.5000 | 0.1894 (4) | 0.2500 | 0.0638 (7) | |
| N1 | 0.8241 (2) | 0.3345 (7) | 0.73370 (17) | 0.0954 (11) | |
| HN1 | 0.811 (2) | 0.224 (7) | 0.7515 (19) | 0.096 (13)* | |
| HN2 | 0.8651 (18) | 0.371 (5) | 0.7407 (16) | 0.071 (11)* | |
| C1 | 0.5000 | 0.3937 (5) | 0.2500 | 0.0397 (7) | |
| C2 | 0.52388 (11) | 0.5146 (3) | 0.31641 (10) | 0.0364 (5) | |
| C3 | 0.57458 (12) | 0.4134 (4) | 0.37505 (11) | 0.0427 (5) | |
| H3 | 0.5933 | 0.2731 | 0.3714 | 0.051* | |
| C4 | 0.59739 (12) | 0.5168 (4) | 0.43805 (11) | 0.0437 (5) | |
| H4 | 0.6312 | 0.4466 | 0.4764 | 0.052* | |
| C5 | 0.56977 (12) | 0.7271 (4) | 0.44448 (11) | 0.0409 (5) | |
| C6 | 0.51783 (12) | 0.8281 (4) | 0.38664 (10) | 0.0396 (5) | |
| H6 | 0.4979 | 0.9662 | 0.3907 | 0.048* | |
| C7 | 0.49596 (11) | 0.7241 (3) | 0.32367 (10) | 0.0371 (5) | |
| H7 | 0.4621 | 0.7944 | 0.2854 | 0.045* | |
| C8 | 0.66367 (12) | 0.7082 (4) | 0.58244 (11) | 0.0484 (6) | |
| C9 | 0.73981 (14) | 0.7565 (5) | 0.60170 (13) | 0.0606 (7) | |
| H9 | 0.7555 | 0.8750 | 0.5814 | 0.073* | |
| C10 | 0.79254 (14) | 0.6301 (5) | 0.65085 (14) | 0.0650 (8) | |
| H10 | 0.8435 | 0.6644 | 0.6631 | 0.078* | |
| C11 | 0.77125 (14) | 0.4541 (5) | 0.68221 (12) | 0.0580 (7) | |
| C12 | 0.69484 (15) | 0.4026 (5) | 0.66200 (13) | 0.0634 (7) | |
| H12 | 0.6794 | 0.2819 | 0.6816 | 0.076* | |
| C13 | 0.64197 (13) | 0.5290 (5) | 0.61320 (12) | 0.0567 (7) | |
| H13 | 0.5911 | 0.4940 | 0.6007 | 0.068* |
Atomic displacement parameters (Å2)
| U11 | U22 | U33 | U12 | U13 | U23 | |
| S1 | 0.0615 (5) | 0.0678 (5) | 0.0395 (4) | 0.0091 (3) | 0.0073 (3) | −0.0110 (3) |
| O1 | 0.0882 (19) | 0.0344 (13) | 0.0499 (14) | 0.000 | 0.0009 (13) | 0.000 |
| N1 | 0.0612 (19) | 0.134 (3) | 0.084 (2) | 0.0128 (19) | 0.0163 (16) | 0.042 (2) |
| C1 | 0.0395 (16) | 0.0318 (16) | 0.0397 (16) | 0.000 | 0.0038 (13) | 0.000 |
| C2 | 0.0376 (11) | 0.0363 (11) | 0.0336 (10) | −0.0016 (9) | 0.0103 (8) | 0.0045 (8) |
| C3 | 0.0456 (12) | 0.0357 (12) | 0.0413 (12) | 0.0045 (9) | 0.0084 (10) | 0.0046 (9) |
| C4 | 0.0408 (12) | 0.0475 (13) | 0.0364 (11) | 0.0030 (10) | 0.0058 (9) | 0.0049 (10) |
| C5 | 0.0375 (11) | 0.0475 (13) | 0.0379 (11) | −0.0045 (10) | 0.0137 (9) | −0.0013 (9) |
| C6 | 0.0395 (11) | 0.0413 (12) | 0.0401 (11) | 0.0021 (9) | 0.0166 (10) | 0.0012 (9) |
| C7 | 0.0350 (10) | 0.0383 (11) | 0.0366 (11) | 0.0017 (9) | 0.0109 (9) | 0.0039 (9) |
| C8 | 0.0412 (13) | 0.0668 (16) | 0.0348 (11) | −0.0065 (11) | 0.0102 (10) | −0.0071 (11) |
| C9 | 0.0500 (14) | 0.0760 (18) | 0.0540 (15) | −0.0172 (13) | 0.0164 (12) | 0.0067 (13) |
| C10 | 0.0364 (13) | 0.092 (2) | 0.0602 (16) | −0.0089 (13) | 0.0092 (12) | 0.0043 (15) |
| C11 | 0.0501 (15) | 0.0776 (17) | 0.0433 (13) | 0.0015 (13) | 0.0126 (11) | 0.0023 (12) |
| C12 | 0.0585 (16) | 0.079 (2) | 0.0537 (15) | −0.0130 (14) | 0.0206 (13) | 0.0093 (13) |
| C13 | 0.0380 (12) | 0.0843 (19) | 0.0454 (13) | −0.0144 (12) | 0.0115 (10) | −0.0014 (13) |
Geometric parameters (Å, °)
| S1—C5 | 1.769 (2) | C5—C6 | 1.397 (3) |
| S1—C8 | 1.777 (3) | C6—C7 | 1.377 (3) |
| O1—C1 | 1.231 (3) | C6—H6 | 0.9300 |
| N1—C11 | 1.383 (4) | C7—H7 | 0.9300 |
| N1—HN1 | 0.84 (4) | C8—C9 | 1.385 (3) |
| N1—HN2 | 0.77 (3) | C8—C13 | 1.389 (4) |
| C1—C2 | 1.484 (2) | C9—C10 | 1.380 (4) |
| C1—C2i | 1.484 (2) | C9—H9 | 0.9300 |
| C2—C7 | 1.397 (3) | C10—C11 | 1.377 (4) |
| C2—C3 | 1.398 (3) | C10—H10 | 0.9300 |
| C3—C4 | 1.375 (3) | C11—C12 | 1.393 (4) |
| C3—H3 | 0.9300 | C12—C13 | 1.377 (4) |
| C4—C5 | 1.395 (3) | C12—H12 | 0.9300 |
| C4—H4 | 0.9300 | C13—H13 | 0.9300 |
| C5—S1—C8 | 103.99 (12) | C6—C7—C2 | 121.02 (19) |
| C11—N1—HN1 | 121 (2) | C6—C7—H7 | 119.5 |
| C11—N1—HN2 | 114 (2) | C2—C7—H7 | 119.5 |
| HN1—N1—HN2 | 125 (3) | C9—C8—C13 | 118.5 (2) |
| O1—C1—C2 | 119.39 (12) | C9—C8—S1 | 119.9 (2) |
| O1—C1—C2i | 119.39 (12) | C13—C8—S1 | 121.52 (17) |
| C2—C1—C2i | 121.2 (2) | C10—C9—C8 | 120.4 (2) |
| C7—C2—C3 | 118.00 (18) | C10—C9—H9 | 119.8 |
| C7—C2—C1 | 122.75 (18) | C8—C9—H9 | 119.8 |
| C3—C2—C1 | 119.21 (19) | C11—C10—C9 | 121.3 (2) |
| C4—C3—C2 | 121.4 (2) | C11—C10—H10 | 119.4 |
| C4—C3—H3 | 119.3 | C9—C10—H10 | 119.4 |
| C2—C3—H3 | 119.3 | C10—C11—N1 | 120.9 (3) |
| C3—C4—C5 | 120.0 (2) | C10—C11—C12 | 118.4 (2) |
| C3—C4—H4 | 120.0 | N1—C11—C12 | 120.7 (3) |
| C5—C4—H4 | 120.0 | C13—C12—C11 | 120.5 (3) |
| C4—C5—C6 | 119.15 (19) | C13—C12—H12 | 119.7 |
| C4—C5—S1 | 124.48 (16) | C11—C12—H12 | 119.7 |
| C6—C5—S1 | 116.37 (17) | C12—C13—C8 | 120.8 (2) |
| C7—C6—C5 | 120.3 (2) | C12—C13—H13 | 119.6 |
| C7—C6—H6 | 119.8 | C8—C13—H13 | 119.6 |
| C5—C6—H6 | 119.8 | ||
| O1—C1—C2—C7 | −150.51 (15) | C3—C2—C7—C6 | 0.2 (3) |
| C2i—C1—C2—C7 | 29.49 (15) | C1—C2—C7—C6 | 178.04 (18) |
| O1—C1—C2—C3 | 27.3 (2) | C5—S1—C8—C9 | 102.6 (2) |
| C2i—C1—C2—C3 | −152.7 (2) | C5—S1—C8—C13 | −79.8 (2) |
| C7—C2—C3—C4 | −0.8 (3) | C13—C8—C9—C10 | −0.6 (4) |
| C1—C2—C3—C4 | −178.80 (18) | S1—C8—C9—C10 | 177.1 (2) |
| C2—C3—C4—C5 | 0.1 (3) | C8—C9—C10—C11 | −0.3 (4) |
| C3—C4—C5—C6 | 1.3 (3) | C9—C10—C11—N1 | −177.0 (3) |
| C3—C4—C5—S1 | −178.56 (17) | C9—C10—C11—C12 | 1.5 (4) |
| C8—S1—C5—C4 | 1.7 (2) | C10—C11—C12—C13 | −1.8 (4) |
| C8—S1—C5—C6 | −178.18 (16) | N1—C11—C12—C13 | 176.7 (3) |
| C4—C5—C6—C7 | −2.0 (3) | C11—C12—C13—C8 | 0.9 (4) |
| S1—C5—C6—C7 | 177.89 (16) | C9—C8—C13—C12 | 0.3 (4) |
| C5—C6—C7—C2 | 1.3 (3) | S1—C8—C13—C12 | −177.4 (2) |
Symmetry codes: (i) −x+1, y, −z+1/2.
Hydrogen-bond geometry (Å, °)
| D—H···A | D—H | H···A | D···A | D—H···A |
| N1—HN2···O1ii | 0.77 (3) | 2.52 (3) | 3.231 (4) | 154 (3) |
Symmetry codes: (ii) −x+3/2, −y+1/2, −z+1.
Footnotes
Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: RZ2311).
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 datablocks global, I. DOI: 10.1107/S1600536809016948/rz2311sup1.cif
Structure factors: contains datablocks I. DOI: 10.1107/S1600536809016948/rz2311Isup2.hkl
Additional supplementary materials: crystallographic information; 3D view; checkCIF report

