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Handbook of Size Exclusion Chromatography and Related ...

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globular proteins <strong>and</strong> selected flexible chain polymers were found to elute<br />

predictably when the “viscosity radius”, Rh, (equal to [h]M) was used as the solute<br />

parameter. These authors found that rodlike molecules did not obey this elution<br />

rule, however, <strong>and</strong> concluded that the universal “SEC radius” had not been found.<br />

This may indeed be true for the broad-based SEC <strong>of</strong> biomacromolecules; however,<br />

the RSEC (Dubin’s term) must be similar, if not equal, to the effective<br />

hydrodynamic radius proposed by Cassassa <strong>and</strong> Tagami (34), <strong>and</strong> must occupy the<br />

effective hydrodynamic volume, Vh. For many proteins, Re may be equivalent to<br />

Rh. Yet,Re may also be calculated from known parameters, such as the molecular<br />

weight (from sedimentation equilibrium or gene sequence), molecular dimensions<br />

(from x-ray crystallography), surface hydration (from titration or modeling), <strong>and</strong><br />

partial specific volume (from composition or actual measurement). Following<br />

Oncley’s approach (45), based on an extension <strong>of</strong> the Stokes relationship for a<br />

perfectly spherical protein, f0 ¼ 6phR0, globular proteins may be described more<br />

accurately than as simple spherical, hydrated structures (34). This frictional<br />

coefficient, f , is defined as:<br />

f ¼ 6ph f<br />

f0<br />

3M(n2 þ d1n 0 1 )<br />

4pN<br />

where f =f0 is the frictional ratio, n2 is the protein partial specific volume, n0 1 is the<br />

pure solvent specific volume, d1 is the protein hydration, <strong>and</strong> N is Avogadro’s<br />

number. The product <strong>of</strong> the bracketed quantity in Equation (10) <strong>and</strong> the shape<br />

factor, fe=fo, is the highly protein-specific radius, Re. If needed, the frictional<br />

ratios may be found from experimental data (s, M, <strong>and</strong> n2; where s is the sedimentation<br />

coefficient) or from protein dimensional information, assuming best<br />

fit for x-ray structural data to either prolate or oblate spheroids <strong>of</strong> revolution.<br />

This estimation may be accomplished using the relationships developed long<br />

ago by Perrin (46) <strong>and</strong> modified by Herzog et al. (47). For prolate ellipsoids<br />

(semi-axes a, b, b)<br />

f<br />

f0<br />

1=3<br />

(1 b<br />

¼<br />

2 =a2 ) 1=2<br />

(b=a) 2=3 ln[1 þ (1 b 2 =a2 ) 1=2 ]=(b=a)<br />

<strong>and</strong> for oblate ellipsoids (semi-axes a, a, b):<br />

f<br />

f0<br />

(a<br />

¼<br />

2 =b 2<br />

(a=b) 2=3 tan 1 (a2 =b 2<br />

1) 1=2<br />

1) 1=2<br />

where R0 is the radius <strong>of</strong> a sphere <strong>of</strong> equal volume to the ellipsoid, that is,<br />

4<br />

3pR3 4<br />

0 ¼ 3ab2 (prolate ellipsoid) or 4<br />

3pa2b (oblate ellipsoid).<br />

Unfortunately, these parameters are known accurately for only a relatively<br />

small group <strong>of</strong> globular proteins: the 21 globular proteins reported by Squire <strong>and</strong><br />

Himmel in 1979 (48). The test <strong>of</strong> fit for globular protein elution from SEC based<br />

© 2004 by Marcel Dekker, Inc.<br />

(10)<br />

(11)<br />

(12)

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