142 Advances in Polymer Science Editorial Board: A. Abe. A.-C ...
142 Advances in Polymer Science Editorial Board: A. Abe. A.-C ...
142 Advances in Polymer Science Editorial Board: A. Abe. A.-C ...
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Dendrimers and Dendrimer-<strong>Polymer</strong> Hybrids 197<br />
3.2.2<br />
Hydrodynamic Radii<br />
More extensive data are available for the hydrodynamic radii of dendrimers than<br />
for the radii of gyration, because they can be derived from <strong>in</strong>tr<strong>in</strong>sic viscosity<br />
measurements accord<strong>in</strong>g to<br />
R h =(3[h]M) 1/3 (10pN A ) –1/3 (5)<br />
or from the translational diffusion coefficient, D o, accord<strong>in</strong>g to<br />
R h=kT(6ph sD o) –1 (6)<br />
where N A is Avogadro's number, k is the Boltzmann constant, and h s the solvent<br />
viscosity. R h and R h are the radii of the equivalent sphere of constant density.<br />
Equations (5) and (6) may not apply to the smallest dendrimers whose dimensions<br />
are comparable to the dimensions of the solvent molecules. Furthermore,<br />
R h and R h cannot be compared directly to the predictions of the models because<br />
the ratio R h/R g and R h/R g are not <strong>in</strong>dependent of the mass and branch<strong>in</strong>g architecture<br />
of the dendrimers [52]. The earliest hydrodynamic radii have been obta<strong>in</strong>ed<br />
on poly (a,e-L-lys<strong>in</strong>e) dendrimers [72] (see Fig. 3b). For these dendrimers<br />
it was found that [h]=2.5 ml/g <strong>in</strong>dependent of generation. It follows from<br />
Eq. (5) that R h~M 1/3 , this exponent is expected for equal-density spheres and is<br />
unusual for dendrimers and ascribed to the asymmetric nature of the branch<strong>in</strong>g<br />
pattern <strong>in</strong> poly (a,e,-L-lys<strong>in</strong>e) [73]. The experimental ratio R h/R g for these dendrimers<br />
varies between 1.14 and 1.0.<br />
Hydrodynamic radii of poly(benzyl ether) dendrimers are shown <strong>in</strong> Fig. 5.<br />
Data for monodendrons with a hydroxyl focal group and tridendrons fall on the<br />
same curve. The value of the exponent n <strong>in</strong> Eq. (4) is 0.46 of low MW. At high MW<br />
it is 0.26 [48]. Data on low MW l<strong>in</strong>ear polystyrene <strong>in</strong> benzene [74] have been <strong>in</strong>cluded<br />
<strong>in</strong> Fig. 5 for comparison. They highlight the little difference <strong>in</strong> the actual<br />
values of the hydrodynamic radii of l<strong>in</strong>ear polystyrene and low MW poly(benzyl<br />
ether) dendrimers. Deviations are observed only when MW>5·10 3 . Furthermore,<br />
the MW dependence of the radii of polystyrene and poly(benzyl ether)<br />
dendrimers are the same at low MW. This <strong>in</strong>dicates that it rema<strong>in</strong>s impossible to<br />
draw major conclusions about the conformation of the low MW dendrimers<br />
from their global properties. The low values of the hydrodynamic radii of the<br />
high MW dendrimers, on the other hand, attest to their compact conformation.<br />
A similar transition to more compact dendrimers has recently been shown <strong>in</strong> a<br />
direct comparison of l<strong>in</strong>ear and dendritic poly(benzyl ethers) [75].<br />
Recently, Stechemesser and Eimer published hydrodynamic radii obta<strong>in</strong>ed<br />
from translational diffusion coefficients measured by means of recovery after<br />
photobleach<strong>in</strong>g experiments on selected generations of PAMAM dendrimers<br />
[76]. The values of R h obta<strong>in</strong>ed <strong>in</strong> methanol are compared with R g data on the<br />
same dendrimers <strong>in</strong> Fig. 4. It can be calculated that the ratio R h/R g~1.4 for all<br />
but the tenth generation dendrimer. This ratio is somewhat higher than expect-