The parallel p 3 q 2 alkyne-cluster interaction in compounds of formula H2M3(C0)9(RC2R’ ) (M = Ru, Os) has been studied by means of X-ray diffraction, ‘ H and I3C VT (variable temperature) NMR and UV-PES spectroscopy, and CNDO theoretical techniques. Crystals of H2 0 ~ 3 (C0 ) 9 (CH3C2CH3 ) belong to the monoclinic space group P 2 , / n wi th unit cell dimensions of a = 14.538 (4) A, b = 13.004 ( 4 ) A, c = 9.817 (3) A, ,9 = 100.17 ( 5 ) O , and 2 = 4. Full-matrix least-squares refinement converged to R = 4.95% for 3223 unique reflections. Relevant interatomic distances (A) : Os ( l ) -Os ( 2 ) = 3.016 ( I ) , Os(l)-Os(3) = 2.763 = 2.364 (28), Os(3)-C(43) = 2.263 (27) . The small differences observed between the Os ( l ) -C( 4 2 ) and Os(2)-C(43) distances are thought to reflect the charge imbalance on the metal atoms. The lowest energy dynamic process observed i n the ”C NMR spectra is consistent with an oscillatory motion of the alkyne and of the hydride bridging the Os ( l ) - 0 s ( 2 ) edge (Ha) coupled wi th the edge hopping of the second hydride (Hb). Subtle electronic changes induced by different substituents on the alkyne cause remarkable differences in the 2Jc,H coupling pattern between H, and CO ligands. The results of CNDO calculations have been used for the interpretation of the UV-PE spectra and for discussion of t h e bonding scheme of the studied molecules.
The Alkyne Cluster Interaction - Structural, Theoretical, and Spectroscopic Study On the Parallel Mu-3-eta-2 Bonding Mode In Trinuclear Carbonyl Clusters of Ruthenium and Osmium
BERTONCELLO, RENZO;GRANOZZI, GAETANO;
1986
Abstract
The parallel p 3 q 2 alkyne-cluster interaction in compounds of formula H2M3(C0)9(RC2R’ ) (M = Ru, Os) has been studied by means of X-ray diffraction, ‘ H and I3C VT (variable temperature) NMR and UV-PES spectroscopy, and CNDO theoretical techniques. Crystals of H2 0 ~ 3 (C0 ) 9 (CH3C2CH3 ) belong to the monoclinic space group P 2 , / n wi th unit cell dimensions of a = 14.538 (4) A, b = 13.004 ( 4 ) A, c = 9.817 (3) A, ,9 = 100.17 ( 5 ) O , and 2 = 4. Full-matrix least-squares refinement converged to R = 4.95% for 3223 unique reflections. Relevant interatomic distances (A) : Os ( l ) -Os ( 2 ) = 3.016 ( I ) , Os(l)-Os(3) = 2.763 = 2.364 (28), Os(3)-C(43) = 2.263 (27) . The small differences observed between the Os ( l ) -C( 4 2 ) and Os(2)-C(43) distances are thought to reflect the charge imbalance on the metal atoms. The lowest energy dynamic process observed i n the ”C NMR spectra is consistent with an oscillatory motion of the alkyne and of the hydride bridging the Os ( l ) - 0 s ( 2 ) edge (Ha) coupled wi th the edge hopping of the second hydride (Hb). Subtle electronic changes induced by different substituents on the alkyne cause remarkable differences in the 2Jc,H coupling pattern between H, and CO ligands. The results of CNDO calculations have been used for the interpretation of the UV-PE spectra and for discussion of t h e bonding scheme of the studied molecules.Pubblicazioni consigliate
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