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Crystal structures of three sterically congested disilanes
In the three sterically congested silanes, C(24)H(38)Si(2) (1) (1,1,2,2-tetraisopropyl-1,2-diphenyldisilane), C(24)H(34)Br4Si(2) (2) [1,1,2,2-tetrakis(2-bromopropan-2-yl)-1,2-diphenyldisilane] and C(32)H(38)Si(2) (3) (1,2-di-tert-butyl-1,1,2,2-tetraphenyldisilane), the Si—Si bond length is...
Autores principales: | , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
International Union of Crystallography
2017
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5347074/ https://www.ncbi.nlm.nih.gov/pubmed/28316829 http://dx.doi.org/10.1107/S2056989017002602 |
Sumario: | In the three sterically congested silanes, C(24)H(38)Si(2) (1) (1,1,2,2-tetraisopropyl-1,2-diphenyldisilane), C(24)H(34)Br4Si(2) (2) [1,1,2,2-tetrakis(2-bromopropan-2-yl)-1,2-diphenyldisilane] and C(32)H(38)Si(2) (3) (1,2-di-tert-butyl-1,1,2,2-tetraphenyldisilane), the Si—Si bond length is shortest in (1) and longest in (2), with (3) having an intermediate value, which parallels the increasing steric congestion. A comparison of the two isopropyl derivatives, (1 and 2), shows a significant increase in the Si—C(ipso) distance with the introduction of bromine. Also, in the brominated compound 2, attractive intermolecular Br⋯Br interactions exist with Br⋯Br separations ca 0.52 Å shorter than the sum of the van der Waals radii. In compound 2, one of the bromoisopropyl groups is rotationally disordered in an 0.8812 (9):0.1188 (9) ratio. Compound 3 exhibits ‘whole molecule’ disorder in a 0.9645 (7):0.0355 (7) ratio with the Si—Si bonds in the two components making an angle of ca 66°. |
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