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Handbook of Size Exclusion Chromatography and Related ...

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Consider an alternative procedure to Eqs (7). In Eq. (3), replace first<br />

w(V), sUV(V), <strong>and</strong> sDR(V)with wc (V), sc DR (V), <strong>and</strong> sc UV (V), respectively.If the<br />

resulting equation is combined with Eq. (7), then the following can be derived:<br />

w(V)¼<br />

ð<br />

h(V,~V)w c (~V)d~V (8)<br />

Equation(8)suggestsanalternativeprocedureforcalculatingw c (V):(a)use<br />

Eq. (3) to obtain the (broadened) mass “chromatogram” w(V), <strong>and</strong> (b) correct<br />

w(V)for instrumental broadening through Eq. (8). Compared with the normal<br />

procedure <strong>of</strong> inverting Eq. (7), this methodrequires <strong>of</strong> asingle inversion,<strong>and</strong> it is<br />

therefore preferable from the point <strong>of</strong> view <strong>of</strong> the propagation <strong>of</strong> errors.<br />

Equation (8) cannot be extended to pS(V), however. This is because<br />

[unlikeEq.(3)],Eq.(4)isnonlinear.Wehereproposetocalculatep c S (V)asfollows<br />

[see Eq. (1)]:<br />

p c S (V)¼ sc UV (V)<br />

kUVw c (V)<br />

where sc UV (V) is the corrected UV chromatogram [obtained by inversion <strong>of</strong><br />

Eq.(7b)];<strong>and</strong>wc (V)isthecorrectedmass“chromatogram”[obtainedbyinversion<br />

<strong>of</strong> Eq. (8)].<br />

Figure 2b presents the corrected mass “chromatogram” wc (V), when<br />

calculated by inverting w(V) through Eq. (8) with a singular value decomposition<br />

algorithm (53). The corrected UV chromatogram sc UV (V ) <strong>of</strong> Fig. 2a was calculated<br />

from sUV(V) using the same inversion algorithm (53). In the midchromatogram<br />

region, the slope <strong>of</strong> pc S (V) increases steadily with the molar mass. Also, large<br />

errors in pc S (V) are apparent at the chromatogram tails, where compositions larger<br />

than 1 <strong>and</strong> lower than 0 were obtained. The corrected molecular weights<br />

log M c (V) <strong>of</strong> Fig. 2c were calculated by interpolation with pc S (V). From wc (V) <strong>and</strong><br />

log M c (V), the corrected MWD <strong>of</strong> Fig. 2d was found. As expected, this<br />

distribution is narrower than the uncorrected MWD. The change in breadth is<br />

quantified by the (rather large) variation in the polydispersity (from 1.27 without<br />

correction to 1.10 with correction, Fig. 2d).<br />

The CCDs (with <strong>and</strong> without correction for instrumental broadening) are<br />

presented in Fig. 2e. The corrected CCD [wc ( pc S )] was obtained from wc (V) <strong>and</strong><br />

pc S (V). Unlike the MWD, the corrected CCD is broader than the uncorrected CCD.<br />

By assuming accurate measurements <strong>of</strong> the instantaneous mass <strong>and</strong> composition,<br />

the global average composition is unaffected by the instrumental broadening.<br />

For this reason, it seems preferable to calculate the global composition directly<br />

from w(V ) <strong>and</strong> pS(V), rather than from wc (V) <strong>and</strong> pc S (V). The corrected <strong>and</strong><br />

uncorrected global compositions ( pc S <strong>and</strong> pS, respectively) are compared in Fig. 2e.<br />

© 2004 by Marcel Dekker, Inc.<br />

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