Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536811002522/im2256sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536811002522/im2256Isup2.hkl |
CCDC reference: 811407
Key indicators
- Single-crystal X-ray study
- T = 173 K
- Mean (C-C) = 0.007 Å
- R factor = 0.058
- wR factor = 0.139
- Data-to-parameter ratio = 20.3
checkCIF/PLATON results
No syntax errors found
Alert level C PLAT341_ALERT_3_C Low Bond Precision on C-C Bonds (x 1000) Ang .. 7 PLAT918_ALERT_3_C Reflection(s) # with I(obs) much smaller I(calc) 1
Alert level G PLAT072_ALERT_2_G SHELXL First Parameter in WGHT Unusually Large. 0.11
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 2 ALERT level C = Check and explain 1 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 2 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion 0 ALERT type 5 Informative message, check
Triphenylphosphine (4.20 g, 16.0 mmol), CBr4 (5.31 g, 16.0 mmol) and zinc dust (1.05 g, 16.0 mmol) were placed in a Schlenk tube and 40 ml of CH2Cl2 were slowly added. The mixture was stirred at room temperature for 28 h. Then, 2-thiophenecarboxaldehyde (0.89 g, 8.00 mmol) in CH2Cl2 (10 ml) was added and stirring was continued for further 2 h. The reaction mixture was extracted with three 50 ml portions of pentane. CH2Cl2 was added when the reaction mixture became too viscous for further extractions. The extracts were filtered and evaporated under reduced pressure. The crude product was purified by column chromatography on silica gel with CH2Cl2/petroleum ether (1:4). Slow evaporation afforded white crystals of 2-(2,2-dibromoethenyl)thiophene (yield: 90%). Characterization data have been previously described in the literature. (Beny et al., 1982)
H atoms were refined using a riding model in their ideal geometric positions using the riding model approximation with Uiso(H) = 1.2Ueq(C) for all H atoms.
Data collection: EXPOSE in IPDS (Stoe & Cie, 1999); cell refinement: CELL in IPDS (Stoe & Cie, 1999); data reduction: INTEGRATE in IPDS (Stoe & Cie, 1999); 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).
C6H4Br2S | F(000) = 504 |
Mr = 267.97 | Dx = 2.341 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 980 reflections |
a = 9.6843 (19) Å | θ = 2.2–27.0° |
b = 7.2379 (14) Å | µ = 10.84 mm−1 |
c = 11.484 (2) Å | T = 173 K |
β = 109.16 (3)° | Plates, colourless |
V = 760.4 (3) Å3 | 0.4 × 0.4 × 0.2 mm |
Z = 4 |
Stoe IPDS diffractometer | 1444 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.064 |
ϕ scans | θmax = 27.0°, θmin = 2.2° |
Absorption correction: numerical (FACEIT in IPDS; Stoe & Cie, 1999) | h = −11→12 |
Tmin = 0.188, Tmax = 0.658 | k = −9→9 |
6492 measured reflections | l = −14→14 |
1667 independent reflections |
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)] = 0.058 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.139 | H-atom parameters not refined |
S = 1.04 | w = 1/[σ2(Fo2) + (0.1099P)2] where P = (Fo2 + 2Fc2)/3 |
1667 reflections | (Δ/σ)max < 0.001 |
82 parameters | Δρmax = 1.36 e Å−3 |
0 restraints | Δρmin = −1.73 e Å−3 |
C6H4Br2S | V = 760.4 (3) Å3 |
Mr = 267.97 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 9.6843 (19) Å | µ = 10.84 mm−1 |
b = 7.2379 (14) Å | T = 173 K |
c = 11.484 (2) Å | 0.4 × 0.4 × 0.2 mm |
β = 109.16 (3)° |
Stoe IPDS diffractometer | 1667 independent reflections |
Absorption correction: numerical (FACEIT in IPDS; Stoe & Cie, 1999) | 1444 reflections with I > 2σ(I) |
Tmin = 0.188, Tmax = 0.658 | Rint = 0.064 |
6492 measured reflections |
R[F2 > 2σ(F2)] = 0.058 | 0 restraints |
wR(F2) = 0.139 | H-atom parameters not refined |
S = 1.04 | Δρmax = 1.36 e Å−3 |
1667 reflections | Δρmin = −1.73 e Å−3 |
82 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Br1 | 0.90429 (5) | 0.69525 (7) | 0.15399 (5) | 0.0306 (2) | |
Br2 | 0.75506 (5) | 0.94572 (7) | 0.30330 (4) | 0.0290 (2) | |
C1 | 0.7287 (5) | 0.7946 (6) | 0.1647 (4) | 0.0214 (9) | |
C2 | 0.5999 (5) | 0.7559 (7) | 0.0803 (4) | 0.0225 (9) | |
H2 | 0.6061 | 0.6818 | 0.0139 | 0.027* | |
C3 | 0.4530 (5) | 0.8068 (6) | 0.0720 (4) | 0.0188 (8) | |
C4 | 0.3277 (5) | 0.7471 (7) | −0.0213 (4) | 0.0225 (9) | |
H4 | 0.3305 | 0.6695 | −0.0873 | 0.027* | |
C5 | 0.1970 (6) | 0.8134 (7) | −0.0080 (5) | 0.0307 (11) | |
H5 | 0.1026 | 0.7857 | −0.0637 | 0.037* | |
C6 | 0.2213 (5) | 0.9216 (7) | 0.0939 (5) | 0.0289 (10) | |
H6 | 0.1455 | 0.9771 | 0.1174 | 0.035* | |
S | 0.40366 (13) | 0.94655 (17) | 0.17497 (12) | 0.0265 (3) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Br1 | 0.0220 (3) | 0.0379 (4) | 0.0324 (3) | 0.00528 (18) | 0.0097 (2) | −0.0004 (2) |
Br2 | 0.0268 (3) | 0.0342 (3) | 0.0250 (3) | −0.00466 (18) | 0.0072 (2) | −0.00800 (17) |
C1 | 0.024 (2) | 0.021 (2) | 0.0202 (19) | 0.0009 (16) | 0.0089 (17) | 0.0037 (16) |
C2 | 0.024 (2) | 0.020 (2) | 0.024 (2) | 0.0027 (18) | 0.0104 (18) | 0.0016 (17) |
C3 | 0.024 (2) | 0.0157 (19) | 0.0183 (19) | 0.0008 (15) | 0.0095 (17) | 0.0015 (15) |
C4 | 0.024 (2) | 0.020 (2) | 0.024 (2) | 0.0029 (17) | 0.0083 (18) | 0.0041 (17) |
C5 | 0.020 (2) | 0.034 (3) | 0.036 (3) | −0.0005 (18) | 0.005 (2) | 0.006 (2) |
C6 | 0.022 (2) | 0.028 (2) | 0.037 (3) | −0.0003 (18) | 0.011 (2) | 0.003 (2) |
S | 0.0256 (6) | 0.0287 (6) | 0.0277 (6) | 0.0006 (4) | 0.0121 (5) | −0.0054 (4) |
Br1—C1 | 1.887 (5) | C4—C5 | 1.408 (7) |
Br2—C1 | 1.878 (5) | C4—H4 | 0.95 |
C1—C2 | 1.335 (7) | C5—C6 | 1.362 (8) |
C2—C3 | 1.442 (6) | C5—H5 | 0.95 |
C2—H2 | 0.95 | C6—S | 1.714 (5) |
C3—C4 | 1.397 (7) | C6—H6 | 0.95 |
C3—S | 1.738 (4) | ||
C2—C1—Br2 | 124.9 (4) | C3—C4—H4 | 123.3 |
C2—C1—Br1 | 121.3 (4) | C5—C4—H4 | 123.3 |
Br2—C1—Br1 | 113.7 (3) | C6—C5—C4 | 112.4 (5) |
C1—C2—C3 | 131.4 (4) | C6—C5—H5 | 123.8 |
C1—C2—H2 | 114.3 | C4—C5—H5 | 123.8 |
C3—C2—H2 | 114.3 | C5—C6—S | 112.6 (4) |
C4—C3—C2 | 124.1 (4) | C5—C6—H6 | 123.7 |
C4—C3—S | 109.8 (3) | S—C6—H6 | 123.7 |
C2—C3—S | 126.1 (3) | C6—S—C3 | 91.9 (2) |
C3—C4—C5 | 113.3 (4) |
Experimental details
Crystal data | |
Chemical formula | C6H4Br2S |
Mr | 267.97 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 173 |
a, b, c (Å) | 9.6843 (19), 7.2379 (14), 11.484 (2) |
β (°) | 109.16 (3) |
V (Å3) | 760.4 (3) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 10.84 |
Crystal size (mm) | 0.4 × 0.4 × 0.2 |
Data collection | |
Diffractometer | Stoe IPDS diffractometer |
Absorption correction | Numerical (FACEIT in IPDS; Stoe & Cie, 1999) |
Tmin, Tmax | 0.188, 0.658 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6492, 1667, 1444 |
Rint | 0.064 |
(sin θ/λ)max (Å−1) | 0.639 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.058, 0.139, 1.04 |
No. of reflections | 1667 |
No. of parameters | 82 |
H-atom treatment | H-atom parameters not refined |
Δρmax, Δρmin (e Å−3) | 1.36, −1.73 |
Computer programs: EXPOSE in IPDS (Stoe & Cie, 1999), CELL in IPDS (Stoe & Cie, 1999), INTEGRATE in IPDS (Stoe & Cie, 1999), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 (Farrugia, 1997), WinGX (Farrugia, 1999).
The title compound (Scheme 1, Fig. 1), which is easily accessible from thiophene-2-carbaldehyde via the Corey-Fuchs reaction, has over the last 30 years become a versatile starting material for a variety of organic transformations and a precursor in material science. This interest is due to the conjugation between the electrochemically active thienyl heterocycle with the reactive halogenated olefin moiety. Originally it was used for the preparation of terthiophenes (Beny et al., 1982). Recent applications include Pd-catalyzed cross-coupling reactions (Herz et al., 1999; Rao et al., 2010) as well as the synthesis of imidazo[1,5-α]pyridines (Zhang et al., 2010).
In the course of our interest in developing new π-conjugated dihalovinyl compounds R—C(H)═CX2 with functional groups (R = imine, ferrocenyl, [2,2]paracyclophane) as substrates for oxidative addition reactions across low-valent noble metals, we have recently reported the synthesis and crystal structures of 4-2',2'-dibromovinyl[2,2]paracyclophane (Clément et al. 2007a) and (2,2-dibromovinyl)ferrocene (Clément et al. 2007b). With this aim in mind, we also prepared the title compound 2-(2,2-dibromoethenyl)thiophene. A survey of the CSD data base revealed that neither 2-vinylthiophene nor a halogenated derivative of the types [C4H3S—C(H)═C(H)X] or [C4H3S—C(H)═CX2] (X = halogen) had been structurally characterized yet. The most related molecule found is 2-thienylmethylenemalononitrile [C4H3S—C(H)═C(CN)2] (Mukherjee et al., 1984). In the latter compound, the angle between the normals of the two planar parts of the molecule, the thiophene cycle and the dicyanovinyl moiety, amounts to 3.6 (5)°. In the title compound, the corresponding angle lies in the same range [3.5 (2)°]. A somewhat larger angle of 10.4° has been determined for (2,2-dibromovinyl)ferrocene [Fc—C(H)═CBr2] (Clément et al., 2007b), whereas in 4-(2',2'-dibromovinyl)[2,2]paracyclophane [PCP—C(H)═CBr2] an angle of 51.1° has been observed significantly deviating from coplanarity (Clément et al., 2007a). The length of the vinylic C1—C2 double bond [1.335 (7) Å] matches well with those of [PCP—C(H)═CBr2] [1.320 (3)°] and [Fc—C(H)═ CBr2] [1.318 (4) Å] (Clément et al., 2007a; Clément et al., 2007b). A similar bond length of 1.353 (5) Å has also been reported for [C4H3S—C(H)═C(CN)2] (Mukherjee et al., 1984).
Bond lenths and angles of the thienyl moiety may be considered as normal and deserve no further comment. The unit cell consists of 4 molecules which are held together by weak interactions only (Fig. 2). These consist of the short Br1—Br2 distance [3.6501 (9) Å, Br1_5-Br2_2] as well as the short distances between Br2 and the carbon atoms of the thiophene ring [3.604 (5) Å, Br2_2-C4; 3.479 (6) Å, Br2_2-C5; 3.624 (5) Å, Br2_2-C6].