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Handbook of Size Exclusion Chromatography and Related ...

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information regarding appropriate Mark–Houwink coefficients <strong>and</strong>/or the<br />

inability to perform intrinsic viscosity measurements.<br />

Balke, Hamielec et al. described a computer method to determine a<br />

calibration curve expressed by<br />

Ve ¼ C1 C2 log 10 M (15)<br />

where Ve is the elution (or retention) volume <strong>and</strong> M is the molecular weight (16).<br />

Their original method involved a cumbersome, simultaneous search for the constants<br />

C1 <strong>and</strong> C2, which was prone to false convergence. Revised methods featured<br />

a sequential, single-parameter search (17,18). These methods rely on the fact that<br />

the dispersity, D, is a function <strong>of</strong> the slope, C2, alone. Arbitrary values are first<br />

assigned to the two constants. The resulting calibration equation is iteratively<br />

applied to the time slice data while the slope value is optimized to minimize the<br />

difference between the true <strong>and</strong> computed dispersities. Once the slope has been<br />

determined it is fixed <strong>and</strong> the intercept, C1, is optimized to minimize the difference<br />

between the true <strong>and</strong> computed moments (either individually or their sum).<br />

3.4 Universal Calibration<br />

Benoit <strong>and</strong> co-workers demonstrated that it is possible to use a set <strong>of</strong> narrow<br />

polymer st<strong>and</strong>ards <strong>of</strong> one chemical type to provide absolute molecular weight<br />

calibration to a sample <strong>of</strong> a different chemical type (19,20). In order to underst<strong>and</strong><br />

how this is possible, one must first consider the relationship between molecular<br />

weight, intrinsic viscosity <strong>and</strong> hydrodynamic volume, the volume <strong>of</strong> a r<strong>and</strong>om,<br />

freely jointed polymer chain in solution. This relationship has been described by<br />

both the Einstein–Simha viscosity law for spherical particles in suspension<br />

[h] ¼ C Vh<br />

M<br />

<strong>and</strong> the Flory–Fox equation for linear polymers in solution<br />

[h] ¼ F ks2l 3=2<br />

!<br />

M<br />

(16)<br />

(17)<br />

where [h] is the intrinsic viscosity, Vh, is the hydrodynamic volume, ks 2 l 1=2 is<br />

the root-mean-square radius <strong>of</strong> gyration <strong>of</strong> the polymer chain, <strong>and</strong> C <strong>and</strong> F are<br />

constants (21). If either equation is multiplied by M, the molecular weight,<br />

the resulting product, [h]M, is seen as proportional to hydrodynamic volume.<br />

(Note that the cube <strong>of</strong> the root-mean-square radius <strong>of</strong> gyration is also proportional<br />

to volume.) Benoit <strong>and</strong> co-workers plotted this product versus elution volume for a<br />

number <strong>of</strong> chemically different polymers investigated under identical SEC<br />

© 2004 by Marcel Dekker, Inc.

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