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CHEMOMETRICS ASSISTED UV-SPECTROPHOTOMETRIC ...

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4.3. Derivative ratio method<br />

Calculations in this technique rely on the following basis;<br />

Consider a mixture M of two components X and Y. If Beer’s law is obeyed for both<br />

components over the whole wavelength range used and the path length is 1 cm, the<br />

absorption spectrum, of the mixture Ax,y is defined by the Equation<br />

Ax,y = αxi CX + βYi CY .....................................[14]<br />

Where Ax,y is the absorbance of the mixture at wavelength i; αXi and βYi are the A (1%, 1cm)<br />

of X and Y at a given wavelength i ; CX and CY are the concentrations of X and Y<br />

respectively. If such equation 14 is divided by the corresponding equation for the spectrum of<br />

a standard solution of X (the same is correct for the component Y) of concentration C o X, the<br />

following Equation can be written.<br />

Ax,y / αXi C o X = CX / C o X + CY βYi / C o X αXi .................[15]<br />

Which can be simplified to<br />

Ax,y / αXi = CX + CY ( βYi / αXi)........................................[16]<br />

By plotting Ax,y / αXi as a function of βYi / αXi a straight line is obtained. The intercept of<br />

the straight line provides the value of CX and the slope of the straight line is CY . To obtain<br />

the ratio βYi / αXi at each wavelength, the absorption spectra of equimolar standard solutions<br />

of Y and X are measured and the absorbance ratio at each wavelength is calculated. At the<br />

same time the differentiation of equation 15 to its first derivative, give the following<br />

equation:-<br />

d/dλ (AMi / αXi C o X) = (CY / C o X) d/dλ (βYi / αXi)..................[17]<br />

Equation 17 indicates that the derivative ratio spectrum of the mixture is dependent only on<br />

the values of CY and C o X and independent on the values of CX in the mixture. A calibration<br />

graph is obtained by recording and storing the spectra of solution of pure Y at different<br />

concentrations, and the spectrum of a solution of pure X, of concentration C o X. The<br />

amplitudes of Y are then divided (wavelength by wavelength) by the corresponding<br />

amplitudes for X.<br />

41

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