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Handbook of Size Exclusion Chromatography and Related ...

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shifts to applied laser light, which may be monitored via the autocorrelation<br />

function G 2(t) [Eq. (26)].<br />

G2(t) ¼ 1<br />

T<br />

ð t<br />

0<br />

I(t)I(t þt)dt (26)<br />

where T¼temperature [K], t¼time, I¼intensity <strong>of</strong> scattered laser light, <strong>and</strong><br />

t¼correlation period.<br />

Indirect Laplace transformation <strong>of</strong> G2(t) yields G2(t), which contains the<br />

translational diffusion coefficient (DT) (72) [Eq. (27)].<br />

G2(t) ¼A 1þCi<br />

" #<br />

ð tmax<br />

tmin<br />

DT(t)<br />

t2 e ( t=t) 2<br />

dt<br />

with t¼ 1<br />

DTh 2<br />

(27)<br />

where D T¼translational diffusion coefficient, h¼scattering vector, <strong>and</strong> A,<br />

C¼coefficients.<br />

According to Stokes/Einstein [Eq. (28)] DT <strong>of</strong> observed glucans <strong>and</strong><br />

glucan aggregates may be correlated with radius RH or diameter (d)<strong>of</strong> amoving<br />

equivalent sphere.Inthecase <strong>of</strong>glucan aggregates,diameterdrather isthelength<br />

<strong>of</strong> coherent segments <strong>and</strong>, thus, dfor glucans is used as coherence length lcoh <strong>of</strong><br />

molecular <strong>and</strong>/or supermolecular glucan segments.<br />

DT ¼ kBT<br />

!lcoh<br />

6phRH<br />

(28)<br />

where kB ¼Boltzman constant, T¼temperature [K], <strong>and</strong> h¼viscosity <strong>of</strong><br />

solution.<br />

Results from mobility investigations within glucan solutions by means <strong>of</strong><br />

photon correlation spectroscopy reflect asituation having two main populations:<br />

. Amajor mass fraction (Fig. 30a) with dimensions (lcoh) in the range<br />

10–30 nm, which represents the molecular dissolved starch glucans;<br />

. A minor, but not negligible, fraction (Fig. 30b) with dimensions (lcoh)in<br />

the range 100–800 nm representing glucan aggregates.<br />

Additionally, translational diffusion coefficient analysis <strong>of</strong> starch glucan<br />

solutions shows the source <strong>of</strong> many problems in the analysis <strong>of</strong> these materials.<br />

Depending on the applied principle <strong>of</strong> observation, (mass-sensitive refractive<br />

index variations or volume-square <strong>of</strong> coherent objects by scattering intensities)<br />

either individual glucan molecules (Fig. 30a) or glucan aggregates (Fig. 30b)<br />

dominate the experimental data. If this fact is not considered, SEC-DRI/LS<br />

experiments <strong>of</strong> starch glucans in particular provide information about supermolecular<br />

aggregates <strong>and</strong> not about constituent glucan molecular weights.<br />

© 2004 by Marcel Dekker, Inc.

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