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In the title compound, C17H15FO2S, a crystallographic mirror plane bis­ects the mol­ecule, passing through O=S and C=O of the central ring, with statistical disorder of the F atom. Orientational disorder of the aromatic ring is also observed; the site occupancy factors are ca. 0.75 and 0.25. In the mol­ecule, the thio­pyran unit has a chair conformation; the geometries around the S and carbonyl C atoms are tetra­hedral and planar, respectively.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536807053111/cv2320sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536807053111/cv2320Isup2.hkl
Contains datablock I

CCDC reference: 667480

Key indicators

  • Single-crystal X-ray study
  • T = 200 K
  • Mean [sigma](C-C) = 0.003 Å
  • Disorder in main residue
  • R factor = 0.085
  • wR factor = 0.170
  • Data-to-parameter ratio = 12.0

checkCIF/PLATON results

No syntax errors found



Alert level B PLAT222_ALERT_3_B Large Non-Solvent H Ueq(max)/Ueq(min) ... 4.28 Ratio PLAT301_ALERT_3_B Main Residue Disorder ......................... 36.00 Perc. PLAT432_ALERT_2_B Short Inter X...Y Contact O1 .. C4 .. 2.87 Ang. PLAT432_ALERT_2_B Short Inter X...Y Contact C13B .. C16B .. 3.04 Ang.
Alert level C PLAT062_ALERT_4_C Rescale T(min) & T(max) by ..................... 0.95 PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for C13A PLAT241_ALERT_2_C Check High Ueq as Compared to Neighbors for C13B PLAT245_ALERT_2_C U(iso) H2 Smaller than U(eq) C2 by ... 0.01 AngSq
Alert level G ABSTM02_ALERT_3_G When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 0.950 Tmax scaled 0.950 Tmin scaled 0.869 PLAT793_ALERT_1_G Check the Absolute Configuration of C2 = ... R
0 ALERT level A = In general: serious problem 4 ALERT level B = Potentially serious problem 4 ALERT level C = Check and explain 2 ALERT level G = General alerts; check 1 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 5 ALERT type 2 Indicator that the structure model may be wrong or deficient 3 ALERT type 3 Indicator that the structure quality may be low 1 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check

Comment top

The chemistry of organic cyclic sulfoxides continues to attract considerable attention due to their synthetic potential. The main advantage of sulfoxides over other sulfur function groups such as sulfides and sulfones is in their chirality. Sulfoxides are chiral groups which are easy to introduce and easy to remove and which give high asymmetric induction in many reactions. A large number of sulfoxides find applications in medicine and industry (Pandiarajan et al., 1993; Yavari et al., 2006). Thiruvalluvar et al. (2007) have reported a crystal structure of 2-[2,6-bis(4-methoxyphenyl)tetrahydrothiopyran- 4-ylidene]malononitrile, wherein the thiopyran unit is in chair form.

The molecular structure of the title compound, (I), is shown in Fig. 1. The thiopyran unit is in the chair form. The dihedral angle between the two orientations of disordered benzene ring is 16.5 (3)°. The geometry around S1 atom is tetrahedral and around C4 - planar. A crystallographic mirror plane bisects the molecule, passing through the O=S and opposite the C=O atoms of the central ring. The (p-fluoro)phenyl at the 2 position and the phenyl ring at the 6 position have equatorial orientations.

Related literature top

For a related crystal structure, see Thiruvalluvar et al. (2007). For applications of sulfoxides, see: Pandiarajan et al. (1993) and Yavari et al. (2006).

Experimental top

A mixture of cis-2-(p-fluro)phenyl-6-phenyldithian-4-one (2.82 g, 0.01 mol), diethyl ether (60 ml), bromine (3.0 g) in water (30 ml) was shaken for few minutes. The solid that separated was filtered, washed with ether and recrystallized from chloroform-carbon tetrachloride mixture (1:1 v/v). The yield: 2.1 g, 70%.

Refinement top

The structure was solved in the space group Pnma with a half of molecule in the asymmetric unit. The sum of s.o.f. of F1A and F1B is 0.5. The (p-fluoro)phenyl group is disordered over two positions in a 0.751 (2):0.249 (2) ratio. All H atoms were positioned geometrically (C—H = 0.95–1.00 Å). Atom H2 was refined isotropically, while the rest H atoms were refined as riding, with Uiso(H) = 1.2Ueq(C).

Structure description top

The chemistry of organic cyclic sulfoxides continues to attract considerable attention due to their synthetic potential. The main advantage of sulfoxides over other sulfur function groups such as sulfides and sulfones is in their chirality. Sulfoxides are chiral groups which are easy to introduce and easy to remove and which give high asymmetric induction in many reactions. A large number of sulfoxides find applications in medicine and industry (Pandiarajan et al., 1993; Yavari et al., 2006). Thiruvalluvar et al. (2007) have reported a crystal structure of 2-[2,6-bis(4-methoxyphenyl)tetrahydrothiopyran- 4-ylidene]malononitrile, wherein the thiopyran unit is in chair form.

The molecular structure of the title compound, (I), is shown in Fig. 1. The thiopyran unit is in the chair form. The dihedral angle between the two orientations of disordered benzene ring is 16.5 (3)°. The geometry around S1 atom is tetrahedral and around C4 - planar. A crystallographic mirror plane bisects the molecule, passing through the O=S and opposite the C=O atoms of the central ring. The (p-fluoro)phenyl at the 2 position and the phenyl ring at the 6 position have equatorial orientations.

For a related crystal structure, see Thiruvalluvar et al. (2007). For applications of sulfoxides, see: Pandiarajan et al. (1993) and Yavari et al. (2006).

Computing details top

Data collection: CrysAlis CCD (Oxford Diffraction, 2007); cell refinement: CrysAlis CCD (Oxford Diffraction, 2007); data reduction: CrysAlis RED (Oxford Diffraction, 2007); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 (Farrugia, 1997); software used to prepare material for publication: PLATON (Spek, 2003).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound with the atomic numbering and 50% probability displacement ellipsoids. Only major component of the disordered (p-fluoro)phenyl group is shown (the occupancies of C11A—C16A and F1A atoms are 0.751 (2) and 0.376 (1), respectively). The unlabelled and labelled atoms are related by mirror plane [symmetry code: x, y, 1/2 - z].
2-(4-Fluorophenyl)-6-phenyltetrahydro-2H-thiopyran-4-one 1-oxide top
Crystal data top
C17H14FO2SF(000) = 628
Mr = 301.35Dx = 1.375 Mg m3
Orthorhombic, PnmaMelting point: 429 K
Hall symbol: -P 2ac 2nMo Kα radiation, λ = 0.71073 Å
a = 11.3887 (5) ŵ = 0.23 mm1
b = 24.6558 (14) ÅT = 200 K
c = 5.1828 (2) ÅPrism, colourless
V = 1455.32 (12) Å30.47 × 0.42 × 0.22 mm
Z = 4
Data collection top
CrysAlis CCD
diffractometer
1297 independent reflections
Radiation source: Enhance (Mo) X-ray Source1218 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.064
Detector resolution: 10.5081 pixels mm-1θmax = 25.0°, θmin = 4.6°
φ and ω scansh = 1313
Absorption correction: multi-scan
(CrysAlis RED; Oxford Diffraction, 2007)
k = 2929
Tmin = 0.915, Tmax = 1.000l = 66
12255 measured reflections
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)] = 0.085Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.170H atoms treated by a mixture of independent and constrained refinement
S = 1.23 w = 1/[σ2(Fo2) + 6.1662P]
where P = (Fo2 + 2Fc2)/3
1297 reflections(Δ/σ)max < 0.004
108 parametersΔρmax = 0.41 e Å3
0 restraintsΔρmin = 0.61 e Å3
Crystal data top
C17H14FO2SV = 1455.32 (12) Å3
Mr = 301.35Z = 4
Orthorhombic, PnmaMo Kα radiation
a = 11.3887 (5) ŵ = 0.23 mm1
b = 24.6558 (14) ÅT = 200 K
c = 5.1828 (2) Å0.47 × 0.42 × 0.22 mm
Data collection top
CrysAlis CCD
diffractometer
1297 independent reflections
Absorption correction: multi-scan
(CrysAlis RED; Oxford Diffraction, 2007)
1218 reflections with I > 2σ(I)
Tmin = 0.915, Tmax = 1.000Rint = 0.064
12255 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0850 restraints
wR(F2) = 0.170H atoms treated by a mixture of independent and constrained refinement
S = 1.23Δρmax = 0.41 e Å3
1297 reflectionsΔρmin = 0.61 e Å3
108 parameters
Special details top

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles

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*/UeqOcc. (<1)
S10.22216 (6)0.250000.26615 (12)0.0292 (2)
O10.29629 (18)0.250000.0254 (3)0.0430 (6)
O40.53648 (19)0.250000.7603 (5)0.0628 (8)
C20.27869 (17)0.19474 (9)0.4669 (4)0.0363 (6)
C30.41209 (17)0.19809 (10)0.4870 (4)0.0435 (7)
C40.4589 (2)0.250000.6018 (5)0.0407 (9)
C11A0.23702 (14)0.14190 (6)0.3389 (3)0.0389 (7)0.751 (2)
C12A0.29790 (18)0.11851 (8)0.1348 (4)0.0640 (11)0.751 (2)
C13A0.2563 (3)0.07115 (9)0.0215 (5)0.0893 (16)0.751 (2)
C14A0.1539 (3)0.04718 (8)0.1123 (6)0.0757 (13)0.751 (2)
C15A0.09301 (19)0.07057 (9)0.3164 (6)0.0666 (13)0.751 (2)
C16A0.13457 (15)0.11792 (8)0.4297 (4)0.0510 (10)0.751 (2)
F1A0.1134 (4)0.00221 (17)0.0294 (12)0.102 (2)0.376 (1)
F1B0.0819 (14)0.0004 (5)0.184 (4)0.102 (2)0.124 (1)
C11B0.2246 (4)0.14362 (19)0.3974 (10)0.0389 (7)0.249 (2)
C12B0.2571 (6)0.1214 (3)0.1615 (11)0.0640 (11)0.249 (2)
C13B0.2080 (8)0.0727 (3)0.0801 (15)0.0893 (16)0.249 (2)
C14B0.1264 (8)0.0462 (3)0.235 (2)0.0757 (13)0.249 (2)
C15B0.0938 (6)0.0685 (3)0.4705 (19)0.0666 (13)0.249 (2)
C16B0.1430 (5)0.1171 (3)0.5519 (12)0.0510 (10)0.249 (2)
H3A0.445730.193710.312050.0522*
H3B0.440080.167320.593140.0522*
H12A0.367910.134900.072690.0769*0.751 (2)
H13A0.297940.055170.118000.1071*0.751 (2)
H15A0.023000.054180.378480.0796*0.751 (2)
H16A0.092970.133910.569170.0610*0.751 (2)
H20.2454 (15)0.2004 (7)0.636 (3)0.025 (5)*
H12B0.312950.139510.055900.0769*0.249 (2)
H13B0.230270.057540.081160.1071*0.249 (2)
H15B0.038040.050350.576060.0796*0.249 (2)
H16B0.120720.132320.713130.0610*0.249 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0222 (3)0.0475 (4)0.0180 (3)0.00000.0027 (3)0.0000
O10.0384 (10)0.0743 (14)0.0162 (9)0.00000.0048 (9)0.0000
O40.0290 (10)0.124 (2)0.0355 (11)0.00000.0096 (10)0.0000
C20.0271 (9)0.0576 (12)0.0242 (9)0.0057 (9)0.0001 (9)0.0059 (9)
C30.0257 (9)0.0688 (14)0.0360 (11)0.0067 (10)0.0032 (10)0.0015 (11)
C40.0204 (12)0.077 (2)0.0247 (14)0.00000.0015 (12)0.0000
C11A0.0380 (11)0.0472 (12)0.0316 (12)0.0079 (10)0.0068 (11)0.0057 (10)
C12A0.051 (2)0.0641 (16)0.0770 (19)0.0027 (16)0.0194 (19)0.0227 (16)
C13A0.080 (3)0.079 (2)0.109 (3)0.013 (2)0.007 (3)0.042 (2)
C14A0.0651 (19)0.0520 (16)0.110 (3)0.0069 (16)0.024 (2)0.005 (2)
C15A0.0582 (16)0.0645 (17)0.077 (3)0.0136 (15)0.015 (2)0.018 (2)
C16A0.0455 (13)0.0615 (16)0.046 (2)0.0030 (13)0.0031 (16)0.0034 (18)
F1A0.099 (3)0.0493 (17)0.159 (5)0.007 (2)0.035 (3)0.039 (3)
F1B0.099 (3)0.0493 (17)0.159 (5)0.007 (2)0.035 (3)0.039 (3)
C11B0.0380 (11)0.0472 (12)0.0316 (12)0.0079 (10)0.0068 (11)0.0057 (10)
C12B0.051 (2)0.0641 (16)0.0770 (19)0.0027 (16)0.0194 (19)0.0227 (16)
C13B0.080 (3)0.079 (2)0.109 (3)0.013 (2)0.007 (3)0.042 (2)
C14B0.0651 (19)0.0520 (16)0.110 (3)0.0069 (16)0.024 (2)0.005 (2)
C15B0.0582 (16)0.0645 (17)0.077 (3)0.0136 (15)0.015 (2)0.018 (2)
C16B0.0455 (13)0.0615 (16)0.046 (2)0.0030 (13)0.0031 (16)0.0034 (18)
Geometric parameters (Å, º) top
S1—O11.5065 (18)C13B—C14B1.391 (12)
S1—C21.831 (2)C14A—C15A1.390 (4)
S1—C2i1.831 (2)C14B—C15B1.389 (14)
F1A—C14A1.275 (5)C15A—C16A1.390 (3)
F1B—C14B1.266 (15)C15B—C16B1.389 (10)
O4—C41.206 (3)C2—H20.965 (16)
C2—C11B1.448 (5)C3—H3A0.9900
C2—C31.525 (3)C3—H3B0.9900
C2—C11A1.537 (3)C12A—H12A0.9500
C3—C41.509 (3)C12B—H12B0.9500
C11A—C16A1.390 (2)C13A—H13A0.9500
C11A—C12A1.390 (3)C13B—H13B0.9500
C11B—C16B1.390 (8)C15A—H15A0.9500
C11B—C12B1.390 (8)C15B—H15B0.9500
C12A—C13A1.390 (3)C16A—H16A0.9500
C12B—C13B1.390 (11)C16B—H16B0.9500
C13A—C14A1.390 (4)
O1—S1—C2105.88 (8)C11B—C16B—C15B120.1 (6)
O1—S1—C2i105.88 (8)S1—C2—H2105.7 (10)
C2—S1—C2i96.15 (10)C3—C2—H2108.8 (10)
S1—C2—C3110.41 (15)C11A—C2—H2113.2 (10)
S1—C2—C11A106.07 (13)C11B—C2—H2100.6 (11)
S1—C2—C11B110.9 (2)C2—C3—H3A108.00
C3—C2—C11A112.52 (17)C2—C3—H3B108.00
C3—C2—C11B119.2 (2)C4—C3—H3A108.00
C2—C3—C4115.14 (18)C4—C3—H3B108.00
O4—C4—C3121.82 (11)H3A—C3—H3B107.00
O4—C4—C3i121.82 (11)C11A—C12A—H12A120.00
C3—C4—C3i116.1 (2)C13A—C12A—H12A120.00
C2—C11A—C12A121.74 (15)C13B—C12B—H12B120.00
C2—C11A—C16A118.26 (15)C11B—C12B—H12B120.00
C12A—C11A—C16A119.99 (16)C14A—C13A—H13A120.00
C12B—C11B—C16B120.0 (5)C12A—C13A—H13A120.00
C2—C11B—C12B116.7 (5)C14B—C13B—H13B120.00
C2—C11B—C16B123.4 (5)C12B—C13B—H13B120.00
C11A—C12A—C13A120.0 (2)C16A—C15A—H15A120.00
C11B—C12B—C13B120.0 (6)C14A—C15A—H15A120.00
C12A—C13A—C14A120.0 (2)C16B—C15B—H15B120.00
C12B—C13B—C14B120.0 (7)C14B—C15B—H15B120.00
C13A—C14A—C15A120.0 (2)C15A—C16A—H16A120.00
C13B—C14B—C15B120.0 (7)C11A—C16A—H16A120.00
C14A—C15A—C16A120.0 (2)C11B—C16B—H16B120.00
C14B—C15B—C16B120.1 (7)C15B—C16B—H16B120.00
C11A—C16A—C15A120.00 (19)
O1—S1—C2—C348.52 (17)C2—C3—C4—O4135.9 (2)
O1—S1—C2—C11A73.65 (13)C2—C3—C4—C3i50.3 (3)
C2i—S1—C2—C359.94 (16)C2—C11A—C12A—C13A179.0 (2)
C2i—S1—C2—C11A177.89 (13)C16A—C11A—C12A—C13A0.0 (3)
S1—C2—C3—C459.5 (2)C2—C11A—C16A—C15A179.01 (19)
C11A—C2—C3—C4177.76 (17)C12A—C11A—C16A—C15A0.0 (3)
S1—C2—C11A—C12A83.40 (18)C11A—C12A—C13A—C14A0.0 (4)
S1—C2—C11A—C16A95.60 (17)C12A—C13A—C14A—C15A0.0 (4)
C3—C2—C11A—C12A37.4 (2)C13A—C14A—C15A—C16A0.0 (4)
C3—C2—C11A—C16A143.58 (18)C14A—C15A—C16A—C11A0.0 (4)
Symmetry code: (i) x, y+1/2, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C2—H2···O1ii0.965 (16)2.430 (16)3.206 (3)137.2 (13)
Symmetry code: (ii) x, y, z+1.

Experimental details

Crystal data
Chemical formulaC17H14FO2S
Mr301.35
Crystal system, space groupOrthorhombic, Pnma
Temperature (K)200
a, b, c (Å)11.3887 (5), 24.6558 (14), 5.1828 (2)
V3)1455.32 (12)
Z4
Radiation typeMo Kα
µ (mm1)0.23
Crystal size (mm)0.47 × 0.42 × 0.22
Data collection
DiffractometerCrysAlis CCD
Absorption correctionMulti-scan
(CrysAlis RED; Oxford Diffraction, 2007)
Tmin, Tmax0.915, 1.000
No. of measured, independent and
observed [I > 2σ(I)] reflections
12255, 1297, 1218
Rint0.064
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.085, 0.170, 1.23
No. of reflections1297
No. of parameters108
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.41, 0.61

Computer programs: CrysAlis CCD (Oxford Diffraction, 2007), CrysAlis RED (Oxford Diffraction, 2007), SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEP-3 (Farrugia, 1997), PLATON (Spek, 2003).

 

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