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_P.-Powell-auth.-Principles-of-Organometallic-Chemistry-Springer-Netherlands-1988

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Molecular orbital theory

6.2 Molecular orbital theory

The bonding of unsaturated organic ligands to transition metals is conveniently

discussed in terms of molecular orbital theory. For significant interaction to occur

(a) metal and ligand orbitals must be of similar energies ( this energy requirement

is met by metal ns, np and (n- l)d and ligand C(2p)n orbitals) and (b) the

symmetry properties of the metal and ligand orbitals must be the same. By

considering the symmetry of a molecule and by applying group theory, it is

possible to deduce which orbitals of the metal and which of the ligands fulfil the

second condition. We concentrate first on one symmetry element, an axis of

rotation which passes through the metal atom and lies perpendicular to the plane

of the ligand. This is defined as the z-axis. Metal and ligand orbitals can be

classified as having CJ, n or 3 symmetry (the last applies only if the rotational

symmetry ofthe molecule is > 2) with respect to this axis. The phase ofthe wave

function of a CJ-orbital does not change sign on rotation through 180° about this

symmetry axis. With a n-orbital the sign changes once, while with a 3-orbital it

changes twice. This division into CJ, n and 3-orbitals is further illustrated in

Fig. 6.7.

As only ligand and metal orbitals of the same symmetry can combine to form

bonding and antibonding molecular orbitals it is often possible through symmetry

considerations to developa qualitative picture ofthe bonding in a molecule. We

contine ourselves here to the valence orbitals of the metal and the p molecular

orbitals of the ligand. Orbitals of similar energy interact more strongly than those

of disparate energy. Estimates of the energies of the interacting metal and ligand

orbitals are obtained from spectroscopic measurements (UV /visible spectra, UVphotoelectron

spectra). The ordering of molecular orbitals in a complex is

deduced from the results of molecular orbital calculations in conjunction with

spectroscopic (especially UV-photoelectron spectral and magnetic data. Even

though more and more powerful computers are becoming available, molecular

Fig. 6.2 Structure of the

anion [C,H.PtCI.J-.

Table 6.2. Symmetry of metal orbitals with respect to

rotation about z-axis (metal-ligand axis).

Symmetry

(J

1[

b

Metal Orbitals

S, p2 , d"z

Px• Py• dzx, dyz

dx'-y'• dxy

Cl y'

1

!

195

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