supplementary materials


zl2115 scheme

Acta Cryst. (2008). E64, o1088    [ doi:10.1107/S1600536808014104 ]

2-(4-Iodophenyl)-5,7-dimethyl-3-methylsulfinyl-1-benzofuran

H. D. Choi, P. J. Seo, B. W. Son and U. Lee

Abstract top

The title compound, C17H15IO2S, was prepared by the oxidation of 2-(4-iodophenyl)-5,7-dimethyl-3-methylsulfanyl-1-benzofuran using 3-chloroperoxybenzoic acid. The 4-iodophenyl ring makes a dihedral angle of 26.0 (1)° with the plane of the benzofuran fragment, and the O atom and the methyl group of the methylsulfinyl substituent lie on opposite sides of this plane. The crystal structure is stabilized by inter- and intramolecular C-H...O hydrogen bonds, and by an I...O halogen bond with an I...O distance of 3.145 (2) Å and a nearly linear C-I...O angle of 164.01 (9)°.

Comment top

As a part of our ongoing studies on the synthesis and structure of 2-aryl-3-methylsulfinyl-1-benzofuran analogues, the crystal structure of 2-(4-bromophenyl)-5-methyl-3-methylsulfinyl-1-benzofuran (Choi et al., 2007a) and 2-(4-bromophenyl)-5,7-dimethyl-3-methylsulfinyl-1-benzofuran (Choi et al., 2007b) have been described in the literature. Here we report the crystal structure of the title compound, 2-(4-iodophenyl)-5,7-dimethyl-3-methylsulfinyl-1-benzofuran (Fig. 1).

The benzofuran unit is essentially planar, with a mean deviation of 0.01 Å from the least-squares plane defined by the nine constituent atoms. The molecular packing (Fig. 2) is stabilized by three different C—H···O hydrogen bonds; one between a methyl H atom and the furan O atom, i.e. C16—H16B···O1, and a second between a methyl H atom and the oxygen of a neighbouring SO unit, i.e. C16—H16A···O2i, and a third between a methyl H atom of the methylsulfinyl substituent and the furan O atom of neighbouring molecules, i.e. C17—H17B···O1ii, (Fig. 2 and Table 1; symmetry code as in Fig. 2). Further stabilization of the structure comes from a weak I···O halogen bond (Fig. 2) (Politzer et al., 2007) between the iodine atom and the oxygen of a neighbouring SO unit, with an I···O2iii distance of 3.145 (2) Å (Symmetry code as in Fig. 2).

Related literature top

For the crystal structures of similar 2-aryl-3-methylsulfinyl-1-benzofuran compounds, see: Choi et al. (2007a,b). For a review of halogen bonding, see: Politzer et al. (2007).

Experimental top

77% 3-chloroperoxybenzoic acid (359 mg, 1.60 mmol) was added in small portions to a stirred solution of 2-(4-iodophenyl)-5,7-dimethyl-3-methylsulfanyl-1-benzofuran (591 mg, 1.50 mmol) in dichloromethane (30 ml) at 273 K. After being stirred at room temperature for 2 h, the mixture was washed with saturated sodium bicarbonate solution and the organic layer was separated, dried over magnesium sulfate, filtered and concentrated in vacuum. The residue was purified by column chromatography (ethyl acetate) to afford the title compound as a colorless solid [yield 80%, m.p. 450–451 K; Rf = 0.57 (ethyl acetate)]. Single crystals suitable for X-ray diffraction were prepared by slow evaporation of a solution of the title compound in tetrahydrofuran at room temperature. Spectroscopic analysis: 1H NMR (CDCl3, 400 MHz) δ 2.44 (s, 3H), 2.53 (s, 3H), 3.10 (s, 3H), 7.03 (s, 1H), 7.59 (d, J = 8.44 Hz, 2H), 7.80 (s, 1H), 7.84 (d, J = 8.44 Hz, 2H); EI—MS 410 [M+].

Refinement top

All H atoms were geometrically located in ideal positions and refined using a riding model, with C—H = 0.95 Å for aromatic H atoms and 0.98 Å for methyl H atoms, and with Uiso(H) = 1.2Ueq(C) for aromatic H atoms, and 1.5Ueq(C) for methyl H atoms.

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SAINT (Bruker, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 1998); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound, showing displacement ellipsoids drawn at the 50% probability level.
[Figure 2] Fig. 2. C—H···O hydrogen bond and I···O halogen bond (dotted lines) in the title compound. [Symmetry codes: (i) x, y + 1, z; (ii) -x, -y + 1, -z + 1; (iii) x, y, z - 1; (iv) x, y, z + 1; (v) x, y - 1, z.]
2-(4-Iodophenyl)-5,7-dimethyl-3-methylsulfinyl-1-benzofuran top
Crystal data top
C17H15IO2SZ = 2
Mr = 410.25F000 = 404
Triclinic, P1Dx = 1.718 Mg m3
Hall symbol: -p_1Melting point = 450–451 K
a = 8.6320 (9) ÅMo Kα radiation
λ = 0.71069 Å
b = 8.917 (1) ÅCell parameters from 5631 reflections
c = 11.638 (1) Åθ = 2.5–28.3º
α = 94.580 (2)ºµ = 2.15 mm1
β = 100.949 (2)ºT = 293 (2) K
γ = 113.725 (2)ºBlock, colorless
V = 792.90 (14) Å30.40 × 0.20 × 0.20 mm
Data collection top
Bruker SMART CCD
diffractometer
3408 independent reflections
Radiation source: fine-focus sealed tube3214 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.029
Detector resolution: 10.0 pixels mm-1θmax = 27.0º
T = 293(2) Kθmin = 1.8º
φ and ω scansh = 11→10
Absorption correction: multi-scan
(SADABS; Sheldrick, 2000)
k = 11→11
Tmin = 0.594, Tmax = 0.647l = 14→14
6882 measured reflections
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.025H-atom parameters constrained
wR(F2) = 0.080  w = 1/[σ2(Fo2) + (0.0374P)2 + 0.4132P]
where P = (Fo2 + 2Fc2)/3
S = 1.22(Δ/σ)max = 0.001
3408 reflectionsΔρmax = 0.50 e Å3
192 parametersΔρmin = 0.66 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
C17H15IO2Sγ = 113.725 (2)º
Mr = 410.25V = 792.90 (14) Å3
Triclinic, P1Z = 2
a = 8.6320 (9) ÅMo Kα
b = 8.917 (1) ŵ = 2.15 mm1
c = 11.638 (1) ÅT = 293 (2) K
α = 94.580 (2)º0.40 × 0.20 × 0.20 mm
β = 100.949 (2)º
Data collection top
Bruker SMART CCD
diffractometer
3408 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2000)
3214 reflections with I > 2σ(I)
Tmin = 0.594, Tmax = 0.647Rint = 0.029
6882 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.025192 parameters
wR(F2) = 0.080H-atom parameters constrained
S = 1.22Δρmax = 0.50 e Å3
3408 reflectionsΔρmin = 0.66 e Å3
Special details top

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
I0.26443 (2)0.23987 (2)0.006964 (16)0.03233 (9)
S0.10120 (10)0.19886 (8)0.60394 (7)0.02931 (16)
O10.3173 (3)0.6586 (2)0.54519 (18)0.0262 (4)
O20.2055 (3)0.1813 (3)0.7150 (2)0.0374 (5)
C10.1717 (4)0.4134 (3)0.6002 (3)0.0262 (6)
C20.2089 (4)0.5443 (3)0.6979 (3)0.0259 (5)
C30.1802 (4)0.5533 (4)0.8114 (3)0.0294 (6)
H30.11970.45690.83930.035*
C40.2430 (4)0.7078 (4)0.8822 (3)0.0309 (6)
C50.3335 (4)0.8521 (4)0.8378 (3)0.0307 (6)
H50.37380.95480.88620.037*
C60.3655 (4)0.8489 (4)0.7256 (3)0.0282 (6)
C70.2995 (4)0.6914 (3)0.6586 (3)0.0256 (6)
C80.2386 (4)0.4876 (3)0.5117 (3)0.0256 (5)
C90.2460 (4)0.4269 (3)0.3936 (2)0.0247 (5)
C100.1189 (4)0.2744 (4)0.3281 (3)0.0286 (6)
H100.02800.20980.35990.034*
C110.1279 (4)0.2191 (4)0.2158 (3)0.0292 (6)
H110.04380.11690.17280.035*
C120.2623 (4)0.3162 (4)0.1674 (3)0.0268 (6)
C130.3902 (4)0.4699 (4)0.2319 (3)0.0289 (6)
H130.48030.53480.19970.035*
C140.3811 (4)0.5239 (3)0.3437 (3)0.0274 (6)
H140.46560.62590.38660.033*
C150.2162 (5)0.7226 (5)1.0062 (3)0.0416 (8)
H15A0.09370.67061.00290.062*
H15B0.26330.83801.04090.062*
H15C0.27450.66871.05380.062*
C160.4651 (4)1.0036 (4)0.6797 (3)0.0387 (7)
H16A0.39791.06710.66820.058*
H16B0.48670.97300.60540.058*
H16C0.57421.06930.73620.058*
C170.1093 (4)0.1531 (4)0.6283 (4)0.0471 (9)
H17A0.16750.03680.63140.071*
H17B0.17640.18010.56460.071*
H17C0.09760.21760.70220.071*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
I0.03823 (13)0.03425 (13)0.02494 (12)0.01616 (9)0.00863 (8)0.00135 (8)
S0.0364 (4)0.0219 (3)0.0299 (4)0.0120 (3)0.0091 (3)0.0058 (3)
O10.0313 (10)0.0209 (9)0.0256 (10)0.0103 (8)0.0077 (8)0.0028 (8)
O20.0405 (12)0.0360 (12)0.0384 (13)0.0193 (10)0.0058 (10)0.0135 (10)
C10.0298 (13)0.0227 (13)0.0263 (14)0.0123 (11)0.0052 (11)0.0037 (11)
C20.0287 (13)0.0234 (13)0.0264 (14)0.0126 (11)0.0052 (11)0.0045 (11)
C30.0312 (14)0.0304 (14)0.0289 (15)0.0145 (12)0.0085 (12)0.0075 (12)
C40.0295 (14)0.0385 (16)0.0265 (15)0.0166 (13)0.0069 (11)0.0027 (12)
C50.0298 (14)0.0269 (14)0.0318 (15)0.0109 (12)0.0050 (12)0.0023 (12)
C60.0240 (13)0.0253 (13)0.0339 (15)0.0100 (11)0.0068 (11)0.0011 (11)
C70.0254 (13)0.0250 (13)0.0264 (14)0.0117 (11)0.0049 (11)0.0031 (11)
C80.0260 (13)0.0219 (13)0.0269 (14)0.0097 (10)0.0032 (11)0.0036 (11)
C90.0271 (13)0.0237 (13)0.0224 (13)0.0114 (11)0.0031 (10)0.0042 (10)
C100.0275 (13)0.0271 (14)0.0272 (14)0.0077 (11)0.0060 (11)0.0051 (11)
C110.0294 (14)0.0248 (13)0.0257 (14)0.0067 (11)0.0017 (11)0.0000 (11)
C120.0299 (14)0.0283 (14)0.0233 (13)0.0150 (11)0.0038 (11)0.0031 (11)
C130.0293 (14)0.0277 (14)0.0296 (15)0.0109 (11)0.0091 (12)0.0069 (11)
C140.0276 (13)0.0227 (13)0.0271 (14)0.0078 (11)0.0037 (11)0.0017 (11)
C150.0498 (19)0.0454 (18)0.0279 (17)0.0184 (15)0.0118 (15)0.0014 (14)
C160.0398 (17)0.0259 (15)0.0469 (19)0.0079 (13)0.0182 (15)0.0024 (14)
C170.0318 (16)0.0336 (17)0.076 (3)0.0111 (14)0.0151 (17)0.0201 (18)
Geometric parameters (Å, °) top
I—C122.094 (3)C9—C101.396 (4)
I—O2i3.145 (2)C9—C141.404 (4)
S—O21.486 (2)C10—C111.387 (4)
S—C11.766 (3)C10—H100.9300
S—C171.780 (4)C11—C121.390 (4)
O1—C71.379 (3)C11—H110.9300
O1—C81.382 (3)C12—C131.401 (4)
C1—C81.364 (4)C13—C141.378 (4)
C1—C21.452 (4)C13—H130.9300
C2—C31.391 (4)C14—H140.9300
C2—C71.396 (4)C15—H15A0.9600
C3—C41.385 (4)C15—H15B0.9600
C3—H30.9300C15—H15C0.9600
C4—C51.409 (4)C16—H16A0.9600
C4—C151.508 (4)C16—H16B0.9600
C5—C61.385 (4)C16—H16C0.9600
C5—H50.9300C17—H17A0.9600
C6—C71.385 (4)C17—H17B0.9600
C6—C161.505 (4)C17—H17C0.9600
C8—C91.459 (4)
C12—I—O2i164.01 (9)C11—C10—H10119.9
O2—S—C1107.81 (13)C9—C10—H10119.9
O2—S—C17105.98 (17)C10—C11—C12120.1 (3)
C1—S—C1799.04 (15)C10—C11—H11119.9
C7—O1—C8106.5 (2)C12—C11—H11119.9
C8—C1—C2107.5 (2)C11—C12—C13120.3 (3)
C8—C1—S123.8 (2)C11—C12—I119.8 (2)
C2—C1—S127.1 (2)C13—C12—I119.8 (2)
C3—C2—C7119.0 (3)C14—C13—C12119.4 (3)
C3—C2—C1136.5 (3)C14—C13—H13120.3
C7—C2—C1104.5 (2)C12—C13—H13120.3
C4—C3—C2119.1 (3)C13—C14—C9120.9 (3)
C4—C3—H3120.5C13—C14—H14119.5
C2—C3—H3120.5C9—C14—H14119.5
C3—C4—C5119.4 (3)C4—C15—H15A109.5
C3—C4—C15120.7 (3)C4—C15—H15B109.5
C5—C4—C15119.9 (3)H15A—C15—H15B109.5
C6—C5—C4123.4 (3)C4—C15—H15C109.5
C6—C5—H5118.3H15A—C15—H15C109.5
C4—C5—H5118.3H15B—C15—H15C109.5
C7—C6—C5114.7 (3)C6—C16—H16A109.5
C7—C6—C16122.2 (3)C6—C16—H16B109.5
C5—C6—C16123.0 (3)H16A—C16—H16B109.5
O1—C7—C6124.7 (3)C6—C16—H16C109.5
O1—C7—C2110.9 (2)H16A—C16—H16C109.5
C6—C7—C2124.4 (3)H16B—C16—H16C109.5
C1—C8—O1110.5 (2)S—C17—H17A109.5
C1—C8—C9134.5 (3)S—C17—H17B109.5
O1—C8—C9115.0 (2)H17A—C17—H17B109.5
C10—C9—C14119.2 (3)S—C17—H17C109.5
C10—C9—C8121.0 (3)H17A—C17—H17C109.5
C14—C9—C8119.8 (2)H17B—C17—H17C109.5
C11—C10—C9120.1 (3)
O2—S—C1—C8120.8 (3)C1—C2—C7—O10.7 (3)
C17—S—C1—C8129.1 (3)C3—C2—C7—C60.5 (4)
O2—S—C1—C243.3 (3)C1—C2—C7—C6178.1 (3)
C17—S—C1—C266.8 (3)C2—C1—C8—O10.1 (3)
C8—C1—C2—C3178.7 (3)S—C1—C8—O1166.67 (19)
S—C1—C2—C312.5 (5)C2—C1—C8—C9179.4 (3)
C8—C1—C2—C70.5 (3)S—C1—C8—C912.6 (5)
S—C1—C2—C7165.7 (2)C7—O1—C8—C10.4 (3)
C7—C2—C3—C40.3 (4)C7—O1—C8—C9179.1 (2)
C1—C2—C3—C4177.8 (3)C1—C8—C9—C1027.6 (5)
C2—C3—C4—C50.3 (4)O1—C8—C9—C10153.1 (3)
C2—C3—C4—C15179.4 (3)C1—C8—C9—C14153.4 (3)
C3—C4—C5—C60.6 (5)O1—C8—C9—C1425.9 (4)
C15—C4—C5—C6179.1 (3)C14—C9—C10—C110.8 (4)
C4—C5—C6—C70.7 (4)C8—C9—C10—C11179.8 (3)
C4—C5—C6—C16178.9 (3)C9—C10—C11—C120.8 (4)
C8—O1—C7—C6178.1 (3)C10—C11—C12—C130.4 (4)
C8—O1—C7—C20.7 (3)C10—C11—C12—I175.5 (2)
C5—C6—C7—O1179.4 (3)C11—C12—C13—C140.1 (4)
C16—C6—C7—O10.2 (5)I—C12—C13—C14175.8 (2)
C5—C6—C7—C20.7 (4)C12—C13—C14—C90.2 (4)
C16—C6—C7—C2178.9 (3)C10—C9—C14—C130.5 (4)
C3—C2—C7—O1179.3 (2)C8—C9—C14—C13179.5 (3)
Symmetry codes: (i) x, y, z−1.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C16—H16B···O10.962.552.975 (4)107
C16—H16A···O2ii0.962.393.288 (4)156
C17—H17B···O1iii0.962.513.422 (4)159
Symmetry codes: (ii) x, y+1, z; (iii) −x, −y+1, −z+1.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
C16—H16B···O10.962.552.975 (4)107
C16—H16A···O2i0.962.393.288 (4)156
C17—H17B···O1ii0.962.513.422 (4)159
Symmetry codes: (i) x, y+1, z; (ii) −x, −y+1, −z+1.
Acknowledgements top

This work was supported by a grant from Dongeui University (2008 A A098).

references
References top

Brandenburg, K. (1998). DIAMOND. Crystal Impact GbR, Bonn, Germany.

Bruker (2001). SAINT and SMART. Bruker AXS Inc., Madison, Wisconsin, USA.

Choi, H. D., Seo, P. J., Son, B. W. & Lee, U. (2007a). Acta Cryst. E63, o3295.

Choi, H. D., Seo, P. J., Son, B. W. & Lee, U. (2007b). Acta Cryst. E63, o4282.

Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.

Politzer, P., Lane, P., Concha, M. C., Ma, Y. & Murray, J. S. (2007). J. Mol. Model. 13, 305–311.

Sheldrick, G. M. (2000). SADABS. University of Gottingen, Germany.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.