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Handbook of Size Exclusion Chromatography and Related ...

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3. Calculate the g 0 branching parameter from the ratio (at any givenmolar<br />

mass) between the intrinsic viscosity <strong>of</strong> the branched polymer <strong>and</strong> the<br />

intrinsic viscosity <strong>of</strong> the linear homolog, yielding:<br />

g 0 (M)¼ [h](M)<br />

KM a 1 (11)<br />

where K <strong>and</strong> a are the Mark–Houwink parameters <strong>of</strong> the linear<br />

homolog.<br />

4. Calculate the gbranching parameter (which is based on the radii <strong>of</strong><br />

gyration), which is related to g 0 through the following empirical<br />

expression:<br />

[g(M)] 1 ¼g 0 (M) (12)<br />

where 1depends on the polymer, the solvent, <strong>and</strong> the temperature, <strong>and</strong><br />

is generally unknown for copolymers.<br />

5. Calculate bn(M)by inverting the following nonlinear equation, which<br />

was theoretically derived for trifunctional branching points (9,12):<br />

" # 1=2<br />

g(M)¼ 1þ bn(M)<br />

7<br />

1=2<br />

þ 4bn(M)<br />

9p<br />

1 (13)<br />

An SEC analysis may be improved when measurements are compared with<br />

predictions produced by representative polymerization models. For the<br />

investigated graft copolymer, the 1exponent <strong>of</strong> Eq. (12) was adjusted from<br />

comparing SEC measurements <strong>of</strong> g 0 (M)with theoretical predictions <strong>of</strong> g(M)<br />

provided by apolymerization model (11,12,54). For THF at 258C, the exponent<br />

resultedin1ffi2(12).For thesamesolvent<strong>and</strong>temperature,theMark–Houwink<br />

parameters <strong>of</strong> alinear SB diblock copolymer with asimilar global composition<br />

<strong>and</strong> equivalent molecular weight range were taken from the literature, yielding<br />

K¼3:2 10 4 dL/g <strong>and</strong> a¼0:693 (23).<br />

The IV <strong>and</strong> DR chromatograms are presented in Fig. 3a. From the ratio<br />

sDR(V)=sUV(V) <strong>and</strong> Eq. (4), an almost constant pS(V) was observed. For this<br />

reason, the DR signal was made proportional to the instantaneous mass. The<br />

intrinsic viscosity [h](V) was calculated from Eq. (10), but is not presented here.<br />

The universal calibration resulted in log M(V) [h](V) ¼ 18:09 0:3041 V<br />

(12). The experimental MWD <strong>of</strong> Fig. 3c was determined from [h](V ) <strong>and</strong> the<br />

universal calibration. The experimental BD was estimated from Eqs (10)–(13)<br />

(Fig. 3d). This function is represented by a continuous curve in Fig. 3d, but with<br />

the data points concentrated at integer values <strong>of</strong> the number <strong>of</strong> branches.<br />

Finally, compare the SEC results with theoretical predictions by a<br />

polymerization model (Figs. 3b, c, <strong>and</strong> d). For the total copolymer, the following<br />

© 2004 by Marcel Dekker, Inc.

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