supplementary materials


Acta Cryst. (2009). E65, o265    [ doi:10.1107/S1600536808043985 ]

Butyl 2-(5-bromo-3-methylsulfinyl-1-benzofuran-2-yl)acetate

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

Abstract top

In the title compound, C15H17BrO4S, the methylsulfinyl O atom and the methyl substituents lie on opposite sides of the plane through the benzofuran fragment. The crystal structure is stabilized by [pi]-[pi] interactions between the benzene rings of neighbouring molecules [centroid-centroid distance = 3.698 (4) Å], and by C-H...[pi] interactions between a methylene H atom of the butyl group and the benzene ring of the benzofuran system. Additionally, the crystal structure exhibits weak intermolecular C-H...O contacts. The butyl group is disordered over two positions, with site-occupancy factors, from refinement, of 0.720 (8) and 0.280 (8).

Comment top

This work is related to our previous communications on the synthesis and structure of alkyl 2-(5-bromo-3-methylsulfinyl-1-benzofuran-2-yl)acetate analogues, viz. isopropyl 2-(5-bromo-3-methylsulfinyl-1-benzofuran-2-yl)acetate (Choi et al., 2008a) and methyl 2-(5-bromo-3-methylsulfinyl-1-benzofuran-2-yl)acetate (Choi et al., 2008b). Herein, we describe the crystal structure of the title compound, (I).

The benzofuran unit is essentially planar, with a mean deviation of 0.012 (2) Å from the least-squares plane defined by the nine constituent atoms. The butyl group is disordered over two positions with site-occupancy factors of 0.720 (8) (for atoms labelled B) and 0.280 (8) (B) in Fig. 1. The molecular packing is stabilized by intermolecular ππ interactions: the Cg···Cgii distance is 3.698 (4) Å, where Cg is the centroid of the C2–C7 ring, symmetry code as in Fig. 2. The molecular packing is further stabilized by C—H···π interactions between the methylene-H and the benzene ring of the benzofuran system, with a C12A—H12A···Cgi separation of 2.78 Å, Table 1; Cg is the centroid of the C2–C7 benzene ring. In addition, weak intermolecular C—H···O contacts are observed, Table 1. One C-H···O contact occurs between a benzene-H and the O3-oxygen, and a second between a methylene-H and the O4-oxygen atom.

Related literature top

For the crystal structures of similar alkyl 2-(5-bromo-3-methylsulfinyl-1- benzofuran-2-yl)acetate derivatives. see: Choi et al. (2008a,b).

Experimental top

77% 3-Chloroperoxybenzoic acid (148 mg, 0.66 mmol) was added in small portions to a stirred solution of butyl 2-(5-bromo-3-methylsulfanyl-1-benzofuran-2-yl)acetate (214 mg, 0.6 mmol) in dichloromethane (30 ml) at 273 K. After being stirred for 3 h at room temperature, the mixture was washed with saturated sodium bicarbonate solution and the organic layer separated, dried over magnesium sulfate, filtered and concentrated in vacuum. The residue was purified by column chromatography (hexane-ethyl acetate, 1:2 v/v) to afford (I) as a colorless solid [yield 80%, m.p. 381–382 K; Rf = 0.65 (hexane-ethyl acetate, 1;2 v/v)]. Single crystals were obtained by evaporation of an acetone solution of (I). Spectroscopic analysis: 1H NMR (CDCl3, 400 MHz) δ 0.92 (t, J = 7.32 Hz, 3H), 1.31–1.41 (m, 2H), 1.59–1.67 (m, 2H), 3.07 (s, 3H), 4.04 (s, 2H), 4.15 (t, J = 6.6 Hz, 2H), 7.39 (d, J = 8.8 Hz, 1H), 7.49 (dd, J = 8.8 Hz and J = 2.2 Hz, 1H), 8.11 (d, J = 1.84 Hz, 1H); EI—MS 374 [M+2], 372 [M+].

Refinement top

All H atoms were geometrically positioned and refined using a riding model, with C—H = 0.93 Å for aryl-, 0.97 Å for methylene-, and 0.96 Å for methyl-H atoms, and with Uiso(H) = 1.2Ueq(C) for the aryl- and methylene-H atoms, and 1.5Ueq(C) for methyl-H atoms. The butyl group was found to be disordered over two positions and modelled with site-occupancy factors, from refinement, of 0.720 (8) (C11A–C14A)) and 0.280 (8) (C11B–C14B). The displacement ellipsoids of part B part were restrained using command ISOR (0.01), both sets of C atoms were restrained using the command DELU, and the C—C distances were restrained to 1.480 (2) Å using command DFIX.

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 (I), showing displacement ellipsoids drawn at the 30% probability level. The butyl group is disordered over two positions with the major component having a site occupancy = 0.720 (8).
[Figure 2] Fig. 2. Diagram illustrating the ππ, C—H···π and C—H···O interactions (dotted lines) in the crystal structure of (I). Cg denotes a ring centroid. The disordered component of the butyl group, part B, has been omitted for clarity as have H atoms not involved in intermolecular contacts. Symmetry codes: (i) x + 1, y + 1, z; (ii) -x, 1 - y, -z; (iii) -x + 1, -y + 1, -z + 1; (iv) -x + 1, -y + 2, -z; (v) x - 1, y - 1, z.
Butyl 2-(5-bromo-3-methylsulfinyl-1-benzofuran-2-yl)acetate top
Crystal data top
C15H17BrO4SZ = 2
Mr = 373.26F(000) = 380
Triclinic, P1Dx = 1.522 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 8.420 (1) ÅCell parameters from 3446 reflections
b = 10.255 (1) Åθ = 2.6–27.0°
c = 10.306 (1) ŵ = 2.66 mm1
α = 97.503 (2)°T = 298 K
β = 99.711 (2)°Block, colorless
γ = 108.678 (2)°0.40 × 0.40 × 0.30 mm
V = 814.55 (15) Å3
Data collection top
Bruker SMART CCD
diffractometer
3179 independent reflections
Radiation source: fine-focus sealed tube2645 reflections with I > 2σ(I)
graphiteRint = 0.017
Detector resolution: 10.0 pixels mm-1θmax = 26.0°, θmin = 2.1°
φ and ω scansh = 1010
Absorption correction: multi-scan
(SADABS; Sheldrick, 1999)
k = 1212
Tmin = 0.353, Tmax = 0.451l = 1212
6560 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)] = 0.033Hydrogen site location: difference Fourier map
wR(F2) = 0.089H-atom parameters constrained
S = 1.14 w = 1/[σ2(Fo2) + (0.0442P)2 + 0.2004P]
where P = (Fo2 + 2Fc2)/3
3179 reflections(Δ/σ)max < 0.001
229 parametersΔρmax = 0.30 e Å3
64 restraintsΔρmin = 0.50 e Å3
Crystal data top
C15H17BrO4Sγ = 108.678 (2)°
Mr = 373.26V = 814.55 (15) Å3
Triclinic, P1Z = 2
a = 8.420 (1) ÅMo Kα radiation
b = 10.255 (1) ŵ = 2.66 mm1
c = 10.306 (1) ÅT = 298 K
α = 97.503 (2)°0.40 × 0.40 × 0.30 mm
β = 99.711 (2)°
Data collection top
Bruker SMART CCD
diffractometer
3179 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 1999)
2645 reflections with I > 2σ(I)
Tmin = 0.353, Tmax = 0.451Rint = 0.017
6560 measured reflectionsθmax = 26.0°
Refinement top
R[F2 > 2σ(F2)] = 0.033H-atom parameters constrained
wR(F2) = 0.089Δρmax = 0.30 e Å3
S = 1.14Δρmin = 0.50 e Å3
3179 reflectionsAbsolute structure: ?
229 parametersFlack parameter: ?
64 restraintsRogers parameter: ?
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*/UeqOcc. (<1)
Br0.42599 (4)0.24082 (3)0.12584 (3)0.06775 (14)
S0.32177 (9)0.58854 (7)0.45871 (6)0.04988 (17)
O10.3033 (2)0.46045 (17)0.07725 (15)0.0442 (4)
O20.7594 (3)0.8276 (2)0.2120 (2)0.0686 (6)
O30.5174 (3)0.8291 (2)0.2711 (2)0.0721 (6)
O40.2197 (3)0.4784 (2)0.52321 (18)0.0618 (5)
C10.2665 (3)0.5195 (2)0.2849 (2)0.0413 (5)
C20.0997 (3)0.4347 (2)0.2012 (2)0.0401 (5)
C30.0682 (3)0.3882 (3)0.2186 (2)0.0447 (5)
H30.09410.41080.30100.054*
C40.1944 (3)0.3070 (3)0.1078 (3)0.0472 (6)
C50.1604 (4)0.2716 (3)0.0175 (3)0.0509 (6)
H50.25000.21590.08890.061*
C60.0052 (3)0.3188 (3)0.0354 (2)0.0478 (6)
H60.03070.29660.11810.057*
C70.1318 (3)0.4008 (2)0.0749 (2)0.0414 (5)
C80.3827 (3)0.5320 (2)0.2067 (2)0.0417 (5)
C90.5701 (3)0.6117 (3)0.2310 (3)0.0460 (6)
H9A0.61500.57670.15860.055*
H9B0.62810.59590.31400.055*
C100.6090 (3)0.7675 (3)0.2403 (3)0.0506 (6)
C11A0.8140 (8)0.9810 (14)0.2252 (11)0.087 (3)0.720 (8)
H11A0.81171.02450.31390.104*0.720 (8)
H11B0.73751.00530.15900.104*0.720 (8)
C12A0.9913 (6)1.0302 (6)0.2033 (6)0.0749 (16)0.720 (8)
H12A1.02071.12320.18210.090*0.720 (8)
H12B1.00360.96640.13070.090*0.720 (8)
C13A1.1021 (6)1.0324 (8)0.3331 (7)0.098 (2)0.720 (8)
H13A1.07121.08330.40500.117*0.720 (8)
H13B1.07660.93660.34640.117*0.720 (8)
C14A1.2899 (7)1.0964 (9)0.3450 (10)0.134 (3)0.720 (8)
H14A1.34991.09670.43300.202*0.720 (8)
H14B1.31731.19110.33090.202*0.720 (8)
H14C1.32431.04290.27880.202*0.720 (8)
C11B0.806 (2)0.973 (3)0.183 (2)0.070 (5)0.280 (8)
H11C0.72311.01530.20250.084*0.280 (8)
H11D0.81380.97210.09030.084*0.280 (8)
C12B0.9768 (19)1.049 (2)0.275 (3)0.127 (7)0.280 (8)
H12C0.96141.03610.36450.153*0.280 (8)
H12D1.00031.14750.27460.153*0.280 (8)
C13B1.1377 (19)1.0231 (18)0.2628 (16)0.087 (5)0.280 (8)
H13C1.13200.92700.26220.105*0.280 (8)
H13D1.18841.06010.19150.105*0.280 (8)
C14B1.207 (3)1.117 (2)0.3964 (16)0.124 (6)0.280 (8)
H14D1.33051.15470.41330.186*0.280 (8)
H14E1.17291.06550.46430.186*0.280 (8)
H14F1.16341.19310.39850.186*0.280 (8)
C150.2192 (5)0.7173 (3)0.4576 (3)0.0679 (8)
H15A0.09710.67100.42660.102*
H15B0.26150.77880.39870.102*
H15C0.24420.77100.54680.102*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Br0.04457 (17)0.0686 (2)0.0882 (3)0.01726 (14)0.01642 (15)0.01369 (16)
S0.0507 (4)0.0625 (4)0.0376 (3)0.0229 (3)0.0092 (3)0.0067 (3)
O10.0471 (9)0.0509 (10)0.0400 (9)0.0212 (8)0.0158 (7)0.0093 (7)
O20.0515 (11)0.0466 (11)0.1135 (17)0.0178 (9)0.0256 (11)0.0246 (11)
O30.0637 (13)0.0590 (12)0.1004 (16)0.0315 (11)0.0233 (12)0.0072 (11)
O40.0721 (13)0.0801 (14)0.0466 (10)0.0348 (11)0.0218 (9)0.0265 (9)
C10.0462 (13)0.0449 (13)0.0361 (12)0.0191 (10)0.0103 (10)0.0099 (10)
C20.0474 (13)0.0399 (12)0.0393 (12)0.0203 (10)0.0129 (10)0.0123 (10)
C30.0474 (13)0.0471 (13)0.0471 (14)0.0220 (11)0.0160 (11)0.0146 (11)
C40.0448 (13)0.0421 (13)0.0588 (15)0.0192 (11)0.0119 (11)0.0135 (11)
C50.0537 (15)0.0468 (14)0.0504 (14)0.0221 (12)0.0019 (12)0.0044 (11)
C60.0561 (15)0.0515 (14)0.0400 (13)0.0261 (12)0.0099 (11)0.0061 (11)
C70.0449 (13)0.0420 (12)0.0440 (12)0.0211 (10)0.0134 (10)0.0117 (10)
C80.0462 (13)0.0441 (13)0.0399 (12)0.0209 (10)0.0111 (10)0.0112 (10)
C90.0447 (13)0.0512 (14)0.0480 (14)0.0215 (11)0.0144 (11)0.0132 (11)
C100.0463 (14)0.0517 (15)0.0531 (15)0.0191 (12)0.0068 (11)0.0085 (12)
C11A0.072 (4)0.059 (4)0.137 (7)0.029 (3)0.019 (4)0.032 (5)
C12A0.075 (3)0.044 (2)0.105 (4)0.013 (2)0.022 (3)0.028 (3)
C13A0.072 (3)0.080 (4)0.117 (5)0.002 (3)0.004 (3)0.024 (4)
C14A0.077 (4)0.120 (5)0.175 (7)0.001 (4)0.024 (4)0.018 (5)
C11B0.072 (7)0.040 (8)0.096 (9)0.008 (5)0.016 (6)0.034 (7)
C12B0.110 (8)0.109 (10)0.162 (12)0.054 (8)0.005 (7)0.028 (9)
C13B0.085 (7)0.086 (8)0.089 (8)0.028 (6)0.022 (6)0.012 (6)
C14B0.122 (10)0.135 (10)0.109 (9)0.053 (8)0.012 (7)0.000 (7)
C150.087 (2)0.0654 (19)0.0637 (18)0.0394 (17)0.0291 (16)0.0087 (15)
Geometric parameters (Å, °) top
Br—C41.899 (3)C11A—H11A0.9700
S—O41.491 (2)C11A—H11B0.9700
S—C11.762 (2)C12A—C13A1.489 (2)
S—C151.794 (3)C12A—H12A0.9700
O1—C71.370 (3)C12A—H12B0.9700
O1—C81.376 (3)C13A—C14A1.482 (2)
O2—C101.319 (3)C13A—H13A0.9700
O2—C11A1.471 (14)C13A—H13B0.9700
O2—C11B1.50 (3)C14A—H14A0.9600
O3—C101.199 (3)C14A—H14B0.9600
C1—C81.355 (3)C14A—H14C0.9600
C1—C21.444 (3)C11B—C12B1.481 (2)
C2—C31.391 (3)C11B—H11C0.9700
C2—C71.396 (3)C11B—H11D0.9700
C3—C41.380 (4)C12B—C13B1.483 (2)
C3—H30.9300C12B—H12C0.9700
C4—C51.396 (4)C12B—H12D0.9700
C5—C61.376 (4)C13B—C14B1.481 (2)
C5—H50.9300C13B—H13C0.9700
C6—C71.380 (3)C13B—H13D0.9700
C6—H60.9300C14B—H14D0.9600
C8—C91.486 (3)C14B—H14E0.9600
C9—C101.511 (4)C14B—H14F0.9600
C9—H9A0.9700C15—H15A0.9600
C9—H9B0.9700C15—H15B0.9600
C11A—C12A1.482 (2)C15—H15C0.9600
O4—S—C1106.92 (12)C11A—C12A—H12A110.8
O4—S—C15105.78 (14)C13A—C12A—H12A110.8
C1—S—C1598.46 (13)C11A—C12A—H12B110.8
C7—O1—C8106.62 (17)C13A—C12A—H12B110.8
C10—O2—C11A115.2 (3)H12A—C12A—H12B108.9
C10—O2—C11B120.0 (10)C14A—C13A—C12A115.7 (6)
C11A—O2—C11B16.2 (11)C14A—C13A—H13A108.4
C8—C1—C2107.4 (2)C12A—C13A—H13A108.4
C8—C1—S123.77 (19)C14A—C13A—H13B108.4
C2—C1—S128.70 (18)C12A—C13A—H13B108.4
C3—C2—C7119.5 (2)H13A—C13A—H13B107.4
C3—C2—C1135.8 (2)C13A—C14A—H14A109.5
C7—C2—C1104.6 (2)C13A—C14A—H14B109.5
C4—C3—C2116.8 (2)H14A—C14A—H14B109.5
C4—C3—H3121.6C13A—C14A—H14C109.5
C2—C3—H3121.6H14A—C14A—H14C109.5
C3—C4—C5123.2 (2)H14B—C14A—H14C109.5
C3—C4—Br118.51 (19)O2—C11B—C12B104 (2)
C5—C4—Br118.29 (19)O2—C11B—H11C111.1
C6—C5—C4120.2 (2)C12B—C11B—H11C111.1
C6—C5—H5119.9O2—C11B—H11D111.1
C4—C5—H5119.9C12B—C11B—H11D111.1
C5—C6—C7116.8 (2)H11C—C11B—H11D109.0
C5—C6—H6121.6C11B—C12B—C13B125 (2)
C7—C6—H6121.6C11B—C12B—H12C106.1
O1—C7—C6125.9 (2)C13B—C12B—H12C106.1
O1—C7—C2110.7 (2)C11B—C12B—H12D106.1
C6—C7—C2123.5 (2)C13B—C12B—H12D106.1
C1—C8—O1110.7 (2)H12C—C12B—H12D106.3
C1—C8—C9133.3 (2)C14B—C13B—C12B83.6 (14)
O1—C8—C9115.9 (2)C14B—C13B—H13C114.7
C8—C9—C10112.3 (2)C12B—C13B—H13C114.7
C8—C9—H9A109.1C14B—C13B—H13D114.7
C10—C9—H9A109.1C12B—C13B—H13D114.7
C8—C9—H9B109.1H13C—C13B—H13D111.8
C10—C9—H9B109.1C13B—C14B—H14D109.5
H9A—C9—H9B107.9C13B—C14B—H14E109.5
O3—C10—O2124.3 (3)H14D—C14B—H14E109.5
O3—C10—C9124.9 (3)C13B—C14B—H14F109.5
O2—C10—C9110.8 (2)H14D—C14B—H14F109.5
O2—C11A—C12A107.2 (8)H14E—C14B—H14F109.5
O2—C11A—H11A110.3S—C15—H15A109.5
C12A—C11A—H11A110.3S—C15—H15B109.5
O2—C11A—H11B110.3H15A—C15—H15B109.5
C12A—C11A—H11B110.3S—C15—H15C109.5
H11A—C11A—H11B108.5H15A—C15—H15C109.5
C11A—C12A—C13A104.5 (6)H15B—C15—H15C109.5
O4—S—C1—C8136.3 (2)C2—C1—C8—O10.3 (3)
C15—S—C1—C8114.3 (2)S—C1—C8—O1176.29 (16)
O4—S—C1—C239.5 (2)C2—C1—C8—C9175.7 (2)
C15—S—C1—C269.9 (2)S—C1—C8—C97.8 (4)
C8—C1—C2—C3177.6 (3)C7—O1—C8—C10.3 (2)
S—C1—C2—C36.1 (4)C7—O1—C8—C9177.00 (19)
C8—C1—C2—C70.7 (3)C1—C8—C9—C1073.0 (3)
S—C1—C2—C7175.63 (18)O1—C8—C9—C10102.8 (2)
C7—C2—C3—C41.4 (3)C11A—O2—C10—O32.1 (6)
C1—C2—C3—C4179.5 (2)C11B—O2—C10—O315.4 (11)
C2—C3—C4—C50.3 (3)C11A—O2—C10—C9176.9 (5)
C2—C3—C4—Br179.94 (16)C11B—O2—C10—C9165.7 (10)
C3—C4—C5—C60.5 (4)C8—C9—C10—O324.4 (4)
Br—C4—C5—C6179.14 (18)C8—C9—C10—O2156.7 (2)
C4—C5—C6—C70.1 (4)C10—O2—C11A—C12A174.3 (5)
C8—O1—C7—C6179.6 (2)C11B—O2—C11A—C12A74 (4)
C8—O1—C7—C20.8 (2)O2—C11A—C12A—C13A78.9 (8)
C5—C6—C7—O1178.5 (2)C11A—C12A—C13A—C14A172.1 (9)
C5—C6—C7—C21.1 (4)C10—O2—C11B—C12B128.1 (15)
C3—C2—C7—O1177.69 (19)C11A—O2—C11B—C12B51 (3)
C1—C2—C7—O10.9 (2)O2—C11B—C12B—C13B69 (3)
C3—C2—C7—C61.9 (3)C11B—C12B—C13B—C14B171 (3)
C1—C2—C7—C6179.5 (2)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
C12A—H12A···Cgi0.972.783.698 (5)158
C5—H5···O3ii0.932.553.405 (3)153
C9—H9B···O4iii0.972.303.248 (3)167
Symmetry codes: (i) x+1, y+1, z; (ii) −x, −y+1, −z; (iii) −x+1, −y+1, −z+1.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
C12A—H12A···Cgi0.972.783.698 (5)158
C5—H5···O3ii0.932.553.405 (3)153
C9—H9B···O4iii0.972.303.248 (3)167
Symmetry codes: (i) x+1, y+1, z; (ii) −x, −y+1, −z; (iii) −x+1, −y+1, −z+1.
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. (2008a). Acta Cryst. E64, o2250.

Choi, H. D., Seo, P. J., Son, B. W. & Lee, U. (2008b). Acta Cryst. E64, o2397.

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

Sheldrick, G. M. (1999). SADABS. University of Göttingen, Germany.

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