CHARACTERIZATION OF STARBURST DENDRIMERS BY ELECTRON-PARAMAGNETIC-RESONANCE .2. POSITIVELY CHARGED NITROXIDE RADICALS OF VARIABLE CHAIN-LENGTH USED AS SPIN PROBES
Mf. Ottaviani et al., CHARACTERIZATION OF STARBURST DENDRIMERS BY ELECTRON-PARAMAGNETIC-RESONANCE .2. POSITIVELY CHARGED NITROXIDE RADICALS OF VARIABLE CHAIN-LENGTH USED AS SPIN PROBES, Journal of the American Chemical Society, 117(15), 1995, pp. 4387-4398
Electron paramagnetic resonance (EPR) spectroscopy has been used to in
vestigate the structure and binding ability of a novel class of anioni
c macromolecules: half-generation poly(amidoamine) starburst dendrimer
s (n.5-SBDs), which differ systematically in size (generation), and wh
ich are terminated by sodium carboxylated surfaces. The half-generatio
ns in the range 1.5-7.5 have been investigated. To some extent n.5-SBD
s mimic both anionic micelles, in their shape and external surface, an
d biomacromolecules, such as proteins and enzymes, in their internal s
tructure. Positively charged nitroxide radicals attached to carbon cha
ins of different lengths were used to probe hydrophilic and hydrophobi
c binding sites of the SBD structure. Mobility and polarity parameters
were evaluated by means of a computer-aided analysis of the EPR spect
ra of the interacting radicals. The study of these parameters as a fun
ction of pH demonstrated the role of electrostatic interactions in pro
moting binding at the external SBD/water interface. Such interactions
are found to be weaker than those occurring with anionic micelles, due
to the greater hydrophilic character of the internal SBD structure. A
nalysis of the EPR parameters as a function of radical chain length, g
eneration, and carboxylate concentration provided evidence of both hyd
rophilic and hydrophobic interactions between the probe radicals and n
.5-SBDs. The results are consistent with the hypothesis that the radic
al chain may enter the SBD internal structure and interact with hydrop
hobic sites. Analysis of EPR spectra at different temperatures provide
d the activation energies for the rotational motion of the interacting
probe.