Literature DB >> 21523138

2-(2,2-Dibromo-ethen-yl)thio-phene.

Sebastien Clément, Laurent Guyard, Michael Knorr, Prisca K Eckert, Carsten Strohmann.   

Abstract

The title compound, C(6)H(4)Br(2)S, represents a versatile building block for the preparation of π-conjugated redox-active thienyl oligomers and metal-mediated cross-coupling reactions. This is due to the presence of an electrochemically active thienyl heterocycle and a reactive dibromo-vinyl substituent, which easily undergoes dehydro-bromination in the presence of n-butyl-lithium to afford 2-ethynyl-thio-phene. In the molecule, the alkenyl unit and the thio-phene ring are almost coplanar with an angle of 3.5 (2)° between the normals of the best planes of the thio-phene ring and the vinyl moiety.

Entities:  

Year:  2011        PMID: 21523138      PMCID: PMC3051600          DOI: 10.1107/S1600536811002522

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

The title compound was first prepared in 1980, see: Bestmann et al. (1980 ▶). For an alternative synthesis using a Corey–Fuchs reaction, see: Beny et al. (1982 ▶). For a structural comparison with 2,2-dibromo­vin­yl[2,2]paracyclo­phane [PCPC(H)=CBr2], (2,2-dibromo­vin­yl)ferrocene [Fc—C(H)=CBr2], and 2-thienyl­methyl­enemalononitrile [C4H3SC(H)=C(CN)2], see: Clément et al. (2007a ▶,b ▶) and Mukherjee et al. (1984 ▶), respectively. For recent applications, see: Herz et al. (1999 ▶); Rao et al. (2010 ▶); Zhang et al. (2010 ▶).

Experimental

Crystal data

C6H4Br2S M = 267.97 Monoclinic, a = 9.6843 (19) Å b = 7.2379 (14) Å c = 11.484 (2) Å β = 109.16 (3)° V = 760.4 (3) Å3 Z = 4 Mo Kα radiation μ = 10.84 mm−1 T = 173 K 0.4 × 0.4 × 0.2 mm

Data collection

Stoe IPDS diffractometer Absorption correction: numerical (FACEIT in IPDS; Stoe & Cie, 1999 ▶) T min = 0.188, T max = 0.658 6492 measured reflections 1667 independent reflections 1444 reflections with I > 2σ(I) R int = 0.064

Refinement

R[F 2 > 2σ(F 2)] = 0.058 wR(F 2) = 0.139 S = 1.04 1667 reflections 82 parameters H-atom parameters not refined Δρmax = 1.36 e Å−3 Δρmin = −1.73 e Å−3 Data collection: EXPOSE in IPDS (Stoe & Cie, 1999 ▶); cell refinement: CELL in IPDS; data reduction: INTEGRATE in IPDS; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶); software used to prepare material for publication: WinGX (Farrugia, 1999 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811002522/im2256sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536811002522/im2256Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C6H4Br2SF(000) = 504
Mr = 267.97Dx = 2.341 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 980 reflections
a = 9.6843 (19) Åθ = 2.2–27.0°
b = 7.2379 (14) ŵ = 10.84 mm1
c = 11.484 (2) ÅT = 173 K
β = 109.16 (3)°Plates, colourless
V = 760.4 (3) Å30.4 × 0.4 × 0.2 mm
Z = 4
Stoe IPDS diffractometer1444 reflections with I > 2σ(I)
graphiteRint = 0.064
φ scansθmax = 27.0°, θmin = 2.2°
Absorption correction: numerical (FACEIT in IPDS; Stoe & Cie, 1999)h = −11→12
Tmin = 0.188, Tmax = 0.658k = −9→9
6492 measured reflectionsl = −14→14
1667 independent reflections
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.058Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.139H-atom parameters not refined
S = 1.04w = 1/[σ2(Fo2) + (0.1099P)2] where P = (Fo2 + 2Fc2)/3
1667 reflections(Δ/σ)max < 0.001
82 parametersΔρmax = 1.36 e Å3
0 restraintsΔρmin = −1.73 e Å3
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.
xyzUiso*/Ueq
Br10.90429 (5)0.69525 (7)0.15399 (5)0.0306 (2)
Br20.75506 (5)0.94572 (7)0.30330 (4)0.0290 (2)
C10.7287 (5)0.7946 (6)0.1647 (4)0.0214 (9)
C20.5999 (5)0.7559 (7)0.0803 (4)0.0225 (9)
H20.60610.68180.01390.027*
C30.4530 (5)0.8068 (6)0.0720 (4)0.0188 (8)
C40.3277 (5)0.7471 (7)−0.0213 (4)0.0225 (9)
H40.33050.6695−0.08730.027*
C50.1970 (6)0.8134 (7)−0.0080 (5)0.0307 (11)
H50.10260.7857−0.06370.037*
C60.2213 (5)0.9216 (7)0.0939 (5)0.0289 (10)
H60.14550.97710.11740.035*
S0.40366 (13)0.94655 (17)0.17497 (12)0.0265 (3)
U11U22U33U12U13U23
Br10.0220 (3)0.0379 (4)0.0324 (3)0.00528 (18)0.0097 (2)−0.0004 (2)
Br20.0268 (3)0.0342 (3)0.0250 (3)−0.00466 (18)0.0072 (2)−0.00800 (17)
C10.024 (2)0.021 (2)0.0202 (19)0.0009 (16)0.0089 (17)0.0037 (16)
C20.024 (2)0.020 (2)0.024 (2)0.0027 (18)0.0104 (18)0.0016 (17)
C30.024 (2)0.0157 (19)0.0183 (19)0.0008 (15)0.0095 (17)0.0015 (15)
C40.024 (2)0.020 (2)0.024 (2)0.0029 (17)0.0083 (18)0.0041 (17)
C50.020 (2)0.034 (3)0.036 (3)−0.0005 (18)0.005 (2)0.006 (2)
C60.022 (2)0.028 (2)0.037 (3)−0.0003 (18)0.011 (2)0.003 (2)
S0.0256 (6)0.0287 (6)0.0277 (6)0.0006 (4)0.0121 (5)−0.0054 (4)
Br1—C11.887 (5)C4—C51.408 (7)
Br2—C11.878 (5)C4—H40.95
C1—C21.335 (7)C5—C61.362 (8)
C2—C31.442 (6)C5—H50.95
C2—H20.95C6—S1.714 (5)
C3—C41.397 (7)C6—H60.95
C3—S1.738 (4)
C2—C1—Br2124.9 (4)C3—C4—H4123.3
C2—C1—Br1121.3 (4)C5—C4—H4123.3
Br2—C1—Br1113.7 (3)C6—C5—C4112.4 (5)
C1—C2—C3131.4 (4)C6—C5—H5123.8
C1—C2—H2114.3C4—C5—H5123.8
C3—C2—H2114.3C5—C6—S112.6 (4)
C4—C3—C2124.1 (4)C5—C6—H6123.7
C4—C3—S109.8 (3)S—C6—H6123.7
C2—C3—S126.1 (3)C6—S—C391.9 (2)
C3—C4—C5113.3 (4)
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