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Tuning Reactivity of Platinum(II) Complexes

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inductive donor capacity and weak π-acceptor ability. Hence, the stronger the trans-<br />

influence, the weaker is the bond. 53 The weakening <strong>of</strong> the M–X bond accelerates rates <strong>of</strong><br />

substitution at the square-planar Pt(<strong>II</strong>) centre. 54<br />

+<br />

+<br />

+<br />

L<br />

-<br />

-<br />

-<br />

+<br />

+<br />

Pt - C l<br />

-<br />

- +<br />

-<br />

The chloride ion trans to the polarisable ligand L is easily<br />

released due to the extra repulsive forces betw een its<br />

negative charge and the induced dipoles <strong>of</strong> the P t(<strong>II</strong>) cation<br />

Scheme 2.4: Distribution <strong>of</strong> charge in induced dipoles in the L–Pt–Cl coordinate <strong>of</strong><br />

trans-[PtA2LX] 35 due to polarisation (where L = non-leaving trans ligand, X<br />

= leaving group e.g. Cl ¯).<br />

Therefore, ligands with stronger trans influence weaken the bond between Pt and the<br />

trans ligand to be displaced and increase the energy <strong>of</strong> ground state accordingly<br />

(polarisation theory by Griberg). 55<br />

In the Pt(<strong>II</strong>) complexes both the σ-donor and π-acceptor capacities are involved in the<br />

trans-effect as illustrated in Figure 2.12. A ligand which exhibits a strong trans-effect is<br />

either a good σ-donor, e.g. H ¯ , CH3 ¯ (Figure 2.12) (a) or a good π-acceptor such as C2H4<br />

(Figure 2.12 (b)) or has both σ-donor and π-acceptor properties like CN ¯ and CO.<br />

Figure 2.12: (a) σ-donation from the filled ligand px orbital to vacant metal 5dx 2 -y 2<br />

orbital. (b) π-back-donation from the filled metal dxz orbital to the<br />

antibonding linear combination <strong>of</strong> carbons’ px orbitals in C2H4. 49<br />

37

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