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Tuning Reactivity of Platinum(II) Complexes

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= (k2[B]o + k-2) ([A]t- [A]eq) (2.10)<br />

Separation <strong>of</strong> variables and integration gives:<br />

This results in<br />

ln<br />

[ ] d[<br />

A]<br />

( [ A]<br />

− [ A]<br />

)<br />

t<br />

( [ ] ) dt<br />

A t<br />

∫ [ A]<br />

= − 2 B 0 + k−<br />

[ A ] t - [ A ] e q<br />

[ A ] 0 - [ A ] e q<br />

k 2 ∫<br />

0 0<br />

(2.11)<br />

t eq<br />

= - ( k 2 [ B ] 0 + k -2 ) t<br />

= -k o b s t<br />

w h e r e , k o b s = k 2 [ B ] 0 + k -2<br />

9<br />

( 2 .1 2 )<br />

Under pseudo first-order conditions, the experimental first order rate constant, kobs, is<br />

given by:<br />

-d [M L 3 X ]<br />

d t<br />

w ith<br />

= k o bs [M ]<br />

k o b s = k 2 [Y ] + k -2 (2 .1 3 )<br />

A plot <strong>of</strong> kobs versus the initial concentration <strong>of</strong> the nucleophile, [B]0 = [Y]0, is linear with<br />

a slope equal to the second-order rate constant, k2, and the y-intercept value equal to the<br />

first-order rate constant, k-2. Typical kinetic plots are shown in Figure 2.3. A plot which<br />

passes through zero implies that the forward reaction is irreversible and directly goes to<br />

completion, whereas a non-zero y-intercept signifies a back reaction in which the<br />

nucleophile Y is being substituted from the metal centre by the solvolysis process.

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