TY - JOUR
T1 - Breaking an electronically preferred symmetry by steric effects in a series of [Ir(biph)X(QR3)2] compounds (X = Cl or I, Q = P or As)
AU - Ujaque, Gregori
AU - Maseras, Feliu
AU - Eisenstein, Odile
AU - Liable-Sands, Louise
AU - Rheingold, Arnold L.
AU - Yao, Wenbin
AU - Crabtree, Robert H.
PY - 1998/1/1
Y1 - 1998/1/1
N2 - A hybrid quantum mechanical/molecular mechanics IMOMM (B3LYP : MM3) method has been applied to a series of five-coordinate 16-electron d6ML5IrIIIcompounds having a relatively flat potential for a distortion from Y to T geometry and for which crystal structures have been obtained. In this series of type [Ir(biph)X(QPh3)2] (biph = biphenyl-2.2′-diyl; Q = P, X = Cl, 2a; Q = As, X = Cl, 2b; Q = P, X = I, 2c), the halide is found to lie in the (biph)Ir plane but off the C2axis of the {Ir(biph)Q2} fragment by a variable angular distortion φ. While φ = 0 is preferred electronically for [Ir(C4H4)Cl(PH3)2], the steric bulk of the real systems 2a-2c leads to φ taking experimental values of 8.2-17.2°. The observed deviation of the halide from the C2axis is shown by IMOMM to be the result of a direct interaction of the phenyl substituents of the axial ligands with the equatorial ligands and not to an electronic effect. The crystal structures for 2b and 2c have been determined.
AB - A hybrid quantum mechanical/molecular mechanics IMOMM (B3LYP : MM3) method has been applied to a series of five-coordinate 16-electron d6ML5IrIIIcompounds having a relatively flat potential for a distortion from Y to T geometry and for which crystal structures have been obtained. In this series of type [Ir(biph)X(QPh3)2] (biph = biphenyl-2.2′-diyl; Q = P, X = Cl, 2a; Q = As, X = Cl, 2b; Q = P, X = I, 2c), the halide is found to lie in the (biph)Ir plane but off the C2axis of the {Ir(biph)Q2} fragment by a variable angular distortion φ. While φ = 0 is preferred electronically for [Ir(C4H4)Cl(PH3)2], the steric bulk of the real systems 2a-2c leads to φ taking experimental values of 8.2-17.2°. The observed deviation of the halide from the C2axis is shown by IMOMM to be the result of a direct interaction of the phenyl substituents of the axial ligands with the equatorial ligands and not to an electronic effect. The crystal structures for 2b and 2c have been determined.
U2 - 10.1039/a804840a
DO - 10.1039/a804840a
M3 - Article
VL - 22
SP - 1493
EP - 1498
IS - 12
ER -