organic compounds
(Z,Z)-1,4-Diiodo-1,4-bis(trimethylsilyl)buta-1,3-diene
aInstitut für Organische Chemie, Universität Frankfurt, Max-von-Laue-Strasse 7, D-60438 Frankfurt am Main, Germany, bInstitut für Anorganische Chemie, Universität Frankfurt, Max-von-Laue-Strasse 7, D-60438 Frankfurt am Main, Germany, and cInstitut für Reine und Angewandte Chemie, Universität Oldenburg, Carl-von-Ossietzky-Strasse 9-11, D-26129 Oldenburg, Germany
*Correspondence e-mail: bats@chemie.uni-frankfurt.de
The 10H20I2Si2, contains two half-molecules. Both complete molecules are generated by crystallographic inversion centers located at the mid-points of the central C—C single bonds; the butadiene groups are planar, with a trans conformation about the central C—C bond. The molecules show short intramolecular H⋯I contacts of 2.89 and 2.92 Å. The crystal packing shows no short intermolecular contacts.
of the title compound, CRelated literature
For the synthesis of the title compound, see: Yamaguchi et al. (1998). For related structures, see: Saito et al. (2007); Yamamoto et al. (2002). For van der Waals radii, see: Bondi (1964).
Experimental
Crystal data
|
Refinement
|
Data collection: SMART (Siemens, 1995); cell SMART; data reduction: SAINT (Siemens, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97.
Supporting information
10.1107/S160053680803482X/su2074sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S160053680803482X/su2074Isup2.hkl
The title compound was prepared as described by Yamaguchi et al. (1998), and recrystallized from n-hexane at 153 K.
H atoms were geometrically positioned and treated as riding atoms: Cplanar—H = 0.95 Å, Cmethyl—H=0.98 Å, with Uiso(H)= 1.2Ueq(Cbutene) and = 1.5Ueq(Cmethyl).
Data collection: SMART (Siemens, 1995); cell
SAINT (Siemens, 1995); data reduction: SAINT (Siemens, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).C10H20I2Si2 | Z = 2 |
Mr = 450.24 | F(000) = 428 |
Triclinic, P1 | Dx = 1.795 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 6.3553 (17) Å | Cell parameters from 124 reflections |
b = 11.502 (2) Å | θ = 3–23° |
c = 11.698 (2) Å | µ = 3.89 mm−1 |
α = 103.027 (13)° | T = 155 K |
β = 90.555 (17)° | Block, colorless |
γ = 90.99 (2)° | 0.46 × 0.36 × 0.28 mm |
V = 832.9 (3) Å3 |
Siemens SMART 1K CCD diffractometer | 5837 independent reflections |
Radiation source: normal-focus sealed tube | 5272 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.021 |
ω scans | θmax = 32.5°, θmin = 1.8° |
Absorption correction: multi-scan (SADABS; Sheldrick, 2000) | h = −9→9 |
Tmin = 0.275, Tmax = 0.336 | k = −17→17 |
15331 measured reflections | l = −17→17 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.021 | H-atom parameters constrained |
wR(F2) = 0.059 | w = 1/[σ2(Fo2) + (0.02P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.03 | (Δ/σ)max = 0.002 |
5837 reflections | Δρmax = 1.12 e Å−3 |
134 parameters | Δρmin = −0.94 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.0130 (5) |
C10H20I2Si2 | γ = 90.99 (2)° |
Mr = 450.24 | V = 832.9 (3) Å3 |
Triclinic, P1 | Z = 2 |
a = 6.3553 (17) Å | Mo Kα radiation |
b = 11.502 (2) Å | µ = 3.89 mm−1 |
c = 11.698 (2) Å | T = 155 K |
α = 103.027 (13)° | 0.46 × 0.36 × 0.28 mm |
β = 90.555 (17)° |
Siemens SMART 1K CCD diffractometer | 5837 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 2000) | 5272 reflections with I > 2σ(I) |
Tmin = 0.275, Tmax = 0.336 | Rint = 0.021 |
15331 measured reflections |
R[F2 > 2σ(F2)] = 0.021 | 0 restraints |
wR(F2) = 0.059 | H-atom parameters constrained |
S = 1.03 | Δρmax = 1.12 e Å−3 |
5837 reflections | Δρmin = −0.94 e Å−3 |
134 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 | ||
I1 | 0.631493 (18) | 0.679368 (10) | 0.508829 (10) | 0.02900 (4) | |
I2 | 0.124665 (17) | 0.825214 (9) | 0.402449 (9) | 0.02623 (4) | |
Si1 | 0.76330 (7) | 0.63323 (4) | 0.77198 (4) | 0.02223 (9) | |
Si2 | 0.47343 (7) | 0.86551 (4) | 0.19545 (4) | 0.02225 (9) | |
C1 | 0.9715 (3) | 0.51656 (14) | 0.56130 (13) | 0.0211 (3) | |
H1 | 1.0502 | 0.4804 | 0.6129 | 0.025* | |
C2 | 0.8224 (2) | 0.59143 (13) | 0.61143 (13) | 0.0198 (3) | |
C3 | 0.9030 (3) | 0.53065 (18) | 0.84764 (16) | 0.0321 (4) | |
H3A | 0.8575 | 0.5446 | 0.9293 | 0.048* | |
H3B | 1.0552 | 0.5455 | 0.8458 | 0.048* | |
H3C | 0.8702 | 0.4478 | 0.8077 | 0.048* | |
C4 | 0.8577 (4) | 0.79022 (18) | 0.8278 (2) | 0.0405 (5) | |
H4A | 0.8270 | 0.8157 | 0.9116 | 0.061* | |
H4B | 0.7858 | 0.8422 | 0.7848 | 0.061* | |
H4C | 1.0098 | 0.7953 | 0.8165 | 0.061* | |
C5 | 0.4740 (3) | 0.62065 (18) | 0.79288 (17) | 0.0322 (4) | |
H5A | 0.4456 | 0.6250 | 0.8759 | 0.048* | |
H5B | 0.4206 | 0.5442 | 0.7457 | 0.048* | |
H5C | 0.4037 | 0.6862 | 0.7680 | 0.048* | |
C6 | 0.5181 (3) | 0.98312 (14) | 0.43727 (13) | 0.0221 (3) | |
H6 | 0.6391 | 1.0180 | 0.4103 | 0.027* | |
C7 | 0.4013 (3) | 0.90828 (14) | 0.35421 (13) | 0.0210 (3) | |
C8 | 0.6036 (3) | 0.71790 (16) | 0.16638 (17) | 0.0332 (4) | |
H8A | 0.7252 | 0.7220 | 0.2194 | 0.050* | |
H8B | 0.6506 | 0.6974 | 0.0849 | 0.050* | |
H8C | 0.5034 | 0.6567 | 0.1796 | 0.050* | |
C9 | 0.6592 (3) | 0.98330 (18) | 0.16797 (18) | 0.0361 (4) | |
H9A | 0.7846 | 0.9870 | 0.2182 | 0.054* | |
H9B | 0.5901 | 1.0607 | 0.1859 | 0.054* | |
H9C | 0.7005 | 0.9641 | 0.0854 | 0.054* | |
C10 | 0.2345 (3) | 0.85504 (18) | 0.09994 (16) | 0.0342 (4) | |
H10A | 0.2759 | 0.8370 | 0.0174 | 0.051* | |
H10B | 0.1613 | 0.9312 | 0.1182 | 0.051* | |
H10C | 0.1404 | 0.7914 | 0.1139 | 0.051* |
U11 | U22 | U33 | U12 | U13 | U23 | |
I1 | 0.02999 (7) | 0.03118 (7) | 0.02837 (7) | 0.01194 (4) | 0.00029 (5) | 0.01117 (5) |
I2 | 0.02378 (7) | 0.02802 (7) | 0.02598 (6) | −0.00570 (4) | −0.00083 (4) | 0.00471 (4) |
Si1 | 0.0211 (2) | 0.0241 (2) | 0.01973 (19) | 0.00282 (16) | 0.00184 (15) | 0.00115 (16) |
Si2 | 0.0263 (2) | 0.0217 (2) | 0.01793 (19) | 0.00165 (16) | 0.00037 (16) | 0.00277 (15) |
C1 | 0.0221 (7) | 0.0224 (7) | 0.0191 (6) | 0.0036 (5) | 0.0002 (5) | 0.0049 (5) |
C2 | 0.0193 (7) | 0.0203 (7) | 0.0200 (6) | 0.0019 (5) | −0.0005 (5) | 0.0046 (5) |
C3 | 0.0302 (9) | 0.0438 (10) | 0.0248 (8) | 0.0096 (7) | 0.0031 (7) | 0.0123 (7) |
C4 | 0.0426 (12) | 0.0312 (9) | 0.0408 (11) | −0.0023 (8) | −0.0044 (9) | −0.0063 (8) |
C5 | 0.0224 (9) | 0.0423 (10) | 0.0307 (9) | 0.0045 (7) | 0.0053 (7) | 0.0050 (7) |
C6 | 0.0213 (7) | 0.0223 (7) | 0.0217 (7) | −0.0019 (5) | 0.0011 (5) | 0.0030 (5) |
C7 | 0.0219 (7) | 0.0203 (7) | 0.0207 (7) | 0.0013 (5) | 0.0008 (5) | 0.0045 (5) |
C8 | 0.0414 (11) | 0.0279 (9) | 0.0284 (8) | 0.0081 (7) | −0.0002 (7) | 0.0021 (7) |
C9 | 0.0410 (11) | 0.0339 (9) | 0.0349 (9) | −0.0020 (8) | 0.0109 (8) | 0.0108 (8) |
C10 | 0.0387 (11) | 0.0388 (10) | 0.0245 (8) | 0.0034 (8) | −0.0048 (7) | 0.0060 (7) |
I1—C2 | 2.1207 (16) | C4—H4B | 0.9800 |
I2—C7 | 2.1276 (17) | C4—H4C | 0.9800 |
Si1—C3 | 1.8591 (19) | C5—H5A | 0.9800 |
Si1—C4 | 1.863 (2) | C5—H5B | 0.9800 |
Si1—C5 | 1.8647 (19) | C5—H5C | 0.9800 |
Si1—C2 | 1.8742 (16) | C6—C7 | 1.350 (2) |
Si2—C10 | 1.863 (2) | C6—C6ii | 1.453 (3) |
Si2—C8 | 1.8644 (19) | C6—H6 | 0.9500 |
Si2—C9 | 1.866 (2) | C8—H8A | 0.9800 |
Si2—C7 | 1.8744 (16) | C8—H8B | 0.9800 |
C1—C2 | 1.339 (2) | C8—H8C | 0.9800 |
C1—C1i | 1.450 (3) | C9—H9A | 0.9800 |
C1—H1 | 0.9500 | C9—H9B | 0.9800 |
C3—H3A | 0.9800 | C9—H9C | 0.9800 |
C3—H3B | 0.9800 | C10—H10A | 0.9800 |
C3—H3C | 0.9800 | C10—H10B | 0.9800 |
C4—H4A | 0.9800 | C10—H10C | 0.9800 |
C3—Si1—C4 | 110.85 (10) | Si1—C5—H5A | 109.5 |
C3—Si1—C5 | 109.79 (9) | Si1—C5—H5B | 109.5 |
C4—Si1—C5 | 110.45 (10) | H5A—C5—H5B | 109.5 |
C3—Si1—C2 | 109.04 (8) | Si1—C5—H5C | 109.5 |
C4—Si1—C2 | 107.21 (9) | H5A—C5—H5C | 109.5 |
C5—Si1—C2 | 109.45 (8) | H5B—C5—H5C | 109.5 |
C10—Si2—C8 | 109.30 (9) | C7—C6—C6ii | 128.06 (19) |
C10—Si2—C9 | 110.53 (10) | C7—C6—H6 | 116.0 |
C8—Si2—C9 | 110.39 (10) | C6ii—C6—H6 | 116.0 |
C10—Si2—C7 | 110.61 (9) | C6—C7—Si2 | 123.88 (12) |
C8—Si2—C7 | 108.94 (8) | C6—C7—I2 | 119.83 (12) |
C9—Si2—C7 | 107.04 (8) | Si2—C7—I2 | 116.23 (8) |
C2—C1—C1i | 128.56 (19) | Si2—C8—H8A | 109.5 |
C2—C1—H1 | 115.7 | Si2—C8—H8B | 109.5 |
C1i—C1—H1 | 115.7 | H8A—C8—H8B | 109.5 |
C1—C2—Si1 | 126.01 (12) | Si2—C8—H8C | 109.5 |
C1—C2—I1 | 120.61 (12) | H8A—C8—H8C | 109.5 |
Si1—C2—I1 | 113.35 (8) | H8B—C8—H8C | 109.5 |
Si1—C3—H3A | 109.5 | Si2—C9—H9A | 109.5 |
Si1—C3—H3B | 109.5 | Si2—C9—H9B | 109.5 |
H3A—C3—H3B | 109.5 | H9A—C9—H9B | 109.5 |
Si1—C3—H3C | 109.5 | Si2—C9—H9C | 109.5 |
H3A—C3—H3C | 109.5 | H9A—C9—H9C | 109.5 |
H3B—C3—H3C | 109.5 | H9B—C9—H9C | 109.5 |
Si1—C4—H4A | 109.5 | Si2—C10—H10A | 109.5 |
Si1—C4—H4B | 109.5 | Si2—C10—H10B | 109.5 |
H4A—C4—H4B | 109.5 | H10A—C10—H10B | 109.5 |
Si1—C4—H4C | 109.5 | Si2—C10—H10C | 109.5 |
H4A—C4—H4C | 109.5 | H10A—C10—H10C | 109.5 |
H4B—C4—H4C | 109.5 | H10B—C10—H10C | 109.5 |
C1i—C1—C2—Si1 | −178.07 (17) | C6ii—C6—C7—Si2 | −176.55 (18) |
C1i—C1—C2—I1 | 0.2 (3) | C6ii—C6—C7—I2 | 0.6 (3) |
C3—Si1—C2—C1 | −12.13 (17) | C10—Si2—C7—C6 | −141.69 (15) |
C4—Si1—C2—C1 | 107.93 (16) | C8—Si2—C7—C6 | 98.15 (16) |
C5—Si1—C2—C1 | −132.25 (15) | C9—Si2—C7—C6 | −21.21 (17) |
C3—Si1—C2—I1 | 169.49 (8) | C10—Si2—C7—I2 | 41.11 (11) |
C4—Si1—C2—I1 | −70.44 (11) | C8—Si2—C7—I2 | −79.04 (11) |
C5—Si1—C2—I1 | 49.37 (11) | C9—Si2—C7—I2 | 161.59 (9) |
Symmetry codes: (i) −x+2, −y+1, −z+1; (ii) −x+1, −y+2, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1···I1i | 0.95 | 2.92 | 3.394 (2) | 112 |
C6—H6···I2ii | 0.95 | 2.89 | 3.378 (2) | 113 |
Symmetry codes: (i) −x+2, −y+1, −z+1; (ii) −x+1, −y+2, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C10H20I2Si2 |
Mr | 450.24 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 155 |
a, b, c (Å) | 6.3553 (17), 11.502 (2), 11.698 (2) |
α, β, γ (°) | 103.027 (13), 90.555 (17), 90.99 (2) |
V (Å3) | 832.9 (3) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 3.89 |
Crystal size (mm) | 0.46 × 0.36 × 0.28 |
Data collection | |
Diffractometer | Siemens SMART 1K CCD diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 2000) |
Tmin, Tmax | 0.275, 0.336 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 15331, 5837, 5272 |
Rint | 0.021 |
(sin θ/λ)max (Å−1) | 0.756 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.021, 0.059, 1.03 |
No. of reflections | 5837 |
No. of parameters | 134 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 1.12, −0.94 |
Computer programs: SMART (Siemens, 1995), SAINT (Siemens, 1995), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
C1—H1···I1i | 0.95 | 2.92 | 3.394 (2) | 112 |
C6—H6···I2ii | 0.95 | 2.89 | 3.378 (2) | 113 |
Symmetry codes: (i) −x+2, −y+1, −z+1; (ii) −x+1, −y+2, −z+1. |
References
Bondi, A. (1964). J. Phys. Chem. 68, 441–451. CrossRef CAS Web of Science Google Scholar
Saito, M., Nakamura, M., Tajima, T. & Yoshioka, M. (2007). Angew. Chem. Int. Ed. 46, 1504–1507. Web of Science CSD CrossRef CAS Google Scholar
Sheldrick, G. M. (2000). SADABS. University of Göttingen, Germany. Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Siemens (1995). SMART and SAINT. Siemens Analytical X-ray Instruments Inc., Madison, Wisconsin, USA. Google Scholar
Yamaguchi, S., Jin, R.-Z., Tamao, K. & Sato, F. (1998). J. Org. Chem. 63, 10060–10062. Web of Science CrossRef CAS Google Scholar
Yamamoto, Y., Ohno, T. & Itoh, K. (2002). Chem. Eur. J. 8, 4734–4741. CrossRef PubMed CAS Google Scholar
This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
The title compound crystallized with two independent centrosymmetric molecules in the unit cell (Fig.1). Each molecule has a crystallographic inversion center at the midpoint of the central C—C single bond. The geometrical parameters of both molecules are similar. The butadiene groups are planar with a trans-conformation about the central C—C bond. The trimethylsilyl groups adopt orientations with a methyl group syn-periplanar with the nearest C=C double bond: torsion angles C3—Si1—C2—C1 = -12.1 (2)° and C9—Si2—C7—C6 = -21.2 (2)°. The molecules show intramolecular H···I contacts of 2.89 Å and 2.92 Å (Table 1), which are shorter than the van der Waals contact distance of 3.18 Å (Bondi, 1964).
The crystal packing of the title compound (Fig. 2) shows no short intermolecular contacts. The shortest intermolecular I···I distances of 3.876 (1) Å [I1···I2i; symmetry operation i) = 1+x, y, z] and 3.973 (1) Å [I1···I2] are comparable to the van der Waals contact distance of 3.96 Å.