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Ptitsyn-Eisner equation

The Mark-Houwink plot for the pullulans is displayed in Figure 9 and indicates a smooth relationship with little scatter. A slope of 0.64 was obtained from the best fit. Figure 10 displays a double logarithmic plot of the radius of gyration versus the molecular weight for pullulans, and this plot has a slope of 0.37. The theoretical values of Rg were calculated by using the Ptitsyn-Eisner equation (as follows) and are shown in the same figure 11) ... [Pg.158]

Figure 10. Double logarithmic plot of radius of gyration versus molecular weight for pullulans. Theoretical slope obtained from Ptitsyn-Eisner equation (see text). Figure 10. Double logarithmic plot of radius of gyration versus molecular weight for pullulans. Theoretical slope obtained from Ptitsyn-Eisner equation (see text).
It appears that for low values of Rg (10-20 nm), the values of Rg that were calculated from the Ptitsyn-Eisner equation were more reliable than those obtained from light scattering in an aqueous medium. Accordingly, for accurate work over a broad range of molecular weights and sizes, a triple detection system is advantageous and recommended. [Pg.164]

This equation indicates that 0 is not strictly constant but decreases with increasing molecular weight and solvent power. A similar conclusion has also been advanced by Ptitsyn and Eisner (277, 218) for essentially the same reason, although their calculation differs in detail. [Pg.218]


See other pages where Ptitsyn-Eisner equation is mentioned: [Pg.151]    [Pg.161]    [Pg.164]    [Pg.151]    [Pg.161]    [Pg.164]   
See also in sourсe #XX -- [ Pg.159 ]




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