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Tuning Reactivity of Platinum(II) Complexes

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The light transmitted from the sample can be represented as<br />

I0<br />

T = (2.33)<br />

I<br />

Where I 0 = the intensity <strong>of</strong> the incident light obtained from the solvent reference cell<br />

I = the intensity <strong>of</strong> the transmitted light from the power source after passing<br />

through the analyte cell<br />

The absorbance can then be written as<br />

A = −logT<br />

(2.34)<br />

By measuring the absorbance <strong>of</strong> the reaction mixture at specific time intervals or in a<br />

continuous manner, the concentration-time-resolved spectrum <strong>of</strong> the system can be<br />

determined from the Beer’s law (Equation 2.35). 30<br />

A = εcl<br />

(2.35)<br />

where, A = absorbance<br />

ε = molar absorptivity (L mol-1 cm-1 )<br />

c = Concentration (mol dm-3 )<br />

l = path length (cm)<br />

UV-Visible absorption spectra usually contain broad absorptions that overlap with<br />

other species in the solution, which makes the analysis <strong>of</strong> the product more difficult.<br />

However, kinetic analysis can be done on overlapping absorption spectra. 6<br />

For a given first-order reaction,<br />

k 1<br />

X Y<br />

At any time t, the absorption is then given by<br />

22<br />

(2.36)<br />

= ε [ X ] + ε [ Y ]<br />

(2.37)<br />

At X<br />

Y<br />

where, At = the absorbance at any time, t<br />

ε X , εY<br />

= molar absorptivity <strong>of</strong> X and Y respectively<br />

Once the reaction goes to completion, the absorption is given by<br />

ε + ε<br />

A∞ = X [ X ] 0 Y [ Y ] 0<br />

(2.38)<br />

where A ∞ = absorbance upon completion <strong>of</strong> reaction

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