| Literature DB >> 32180927 |
Caroline M Storey1, Audrius Kalpokas2, Matthew R Gyton1, Tobias Krämer2,3, Adrian B Chaplin1.
Abstract
The preparation of a range of tetraaryl-substituted bicyclo[4.2.0]octa-1,5,7-trienes using a one-pot procedure starting from terminal aryl alkynes and catalysed by a rhodium(i) complex is reported. This synthesis proceeds by a reaction sequence involving head-to-tail homocoupling of the terminal alkyne and zipper annulation of the resulting gem-enyne. The rhodium catalyst employed is notable for the incorporation of a flexible NHC-based pincer ligand, which is suggested to interconvert between mer- and fac-coordination modes to fulfil the orthogonal mechanistic demands of the two transformations. Evidence for this interesting auto-tandem action of the catalyst is provided by reactions of the precatalyst with model substrates, corroborating proposed intermediates in both component cycles, and norbornadiene, which reversibly captures the change in pincer ligand coordination mode, along with a DFT-based computational analysis. This journal is © The Royal Society of Chemistry 2020.Entities:
Year: 2020 PMID: 32180927 PMCID: PMC7053420 DOI: 10.1039/c9sc06153c
Source DB: PubMed Journal: Chem Sci ISSN: 2041-6520 Impact factor: 9.825
Fig. 1Sequential reaction protocols and bicyclo[4.2.0]octa-1,5,7-triene synthesis.
Fig. 2Time course analysis of the formation 4a from 2a catalysed by 1·C2H4.
Fig. 3Preparation of bicyclo[4.2.0]octa-1,5,7-trienes from terminal alkynes. Solid-state structures of 4a (not unique, Z′ = 2) and 4d shown with 50% probability thermal ellipsoids.
Fig. 4Proposed auto-tandem catalysed preparation of bicyclo[4.2.0]octa-1,5,7-trienes from terminal alkynes.
Fig. 5Reactivity of 1·C2H4 relevant to the proposed mechanism ([BArF4]– anions omitted). Solid-state structures of the cations of 7, 8 and 9 (not unique, Z′ = 2) shown with 30%, 50% and 50% probability thermal ellipsoids, respectively. Selected data: 7, Rh1–C2, 1.92(2) Å; C2–C3, 1.21(2) Å; Rh1–C2–C3, 179(2)°; Rh1–C4, 2.02(2) Å; C4–C5, 1.30(3) Å; Rh1–N7, 2.15(2) Å; Rh1–C4–C5, 140(2)°; Rh1–N101, 2.25(2) Å; Rh1–C109, 2.01(2) Å; Rh1–C115, 2.01(2) Å; C109–Rh1–C115, 174.5(8)°; 8, Rh1–Cnt(C2,C3), 1.964(2) Å; Rh1–Cnt(C5,C6), 2.144(2) Å; C2–C3, 1.431(4) Å; C5–C6, 1.369(4) Å; N101–Rh1–Cnt(C2,C3), 135.48(8)°; C109–Rh1–Cnt(C2,C3), 140.01(9)°; C115–Rh1–Cnt(C5,C6), 160.86(10)°; Rh1–N101, 2.327(2) Å; Rh1–C109, 2.118(3) Å; Rh1–C115, 2.026(2) Å; C109–Rh1–C115, 103.60(10)°; 9, Rh1–C2, 2.029(2) Å; Rh1–C8, 2.024(2) Å, N101–Rh1–C2, 171.69(8)°; C2–C3, 1.354(3) Å; C3–C7, 1.433(3) Å; C7–C8, 1.345(3) Å; Rh1–N101, 2.242(2) Å; Rh1–C109, 2.049(2) Å; Rh1–C115, 2.063(2) Å; C109–Rh1–C115, 171.92(8)°.
Fig. 6Calculated reaction profile (B3PW91-D3/SDD/6-31G**) for the terminal alkyne coupling of 2b and zipper annulation of 3b. Relative Gibbs free energies (kcal mol–1) are corrected for DFB solvent. Solid traces for elementary steps for which transition states have been calculated.