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A de ned stoichiometry is generally not relevant to describe macromolecular complexes, even in dilute regime (ie, with only isolated chains and no polymer polymer aggregates) In practice, the number of bound nanoparticles per polymer chain and the fraction of bound azobenzene are the two primary structural parameters that can be measured (Fig 75b) First, we focus on the binding of the azo chromophores Proton NMR shifts (May et al, 2005), red-shift on the UV spectra (Labarthet et al, 2000), variation of circular dichroism (Shimomura et al, 2002; Suzuki et al, 1991) are among the experimental signals that can be used to probe the solvatation of the chromophore Accordingly, it is possible to determine the fraction of free azobenzene groups and whether the association takes place gradually or not.

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where cH/cu is the ratio of the atomic concentrations of the two isotopes. The separation factor is a function of the overpotential and of the electrode material. The reacting species are H 3 O + and H 2 DO + in solutions with low deuterium concentrations. The S values for mercury electrodes lie between 2.5 and 4, for platinum electrodes with low overpotentials between 3 and 4 and, at large overpotentials, between 7 and 8. The overpotential of hydrogen at a mercury electrode decreases sharply in the presence of readily adsorbed, weak organic bases (especially nitrogen-containing heterocyclic compounds). A peak appears on the polarization curves of these catalytic currents. The hydrogen overpotential is decreased as oxonium ions are replaced in the electrode reaction by the adsorbed cations of these compounds, BH ads + . The product of the reduction is the BHads radical. Recombination of these radicals yields molecular hydrogen and the original base. The evolution of hydrogen through this mechanism occurs more readily than through oxonium ions. The decrease in the catalytic current at negative potentials is a result of the desorption of organic compounds from the electrode surface. The electrode processes of oxygen represent a further important group of electrocatalytic processes. The reduction of oxygen to water O2 + 4H + + 4e<= 2H2O (5.7.6)

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has a standard potential determined by calculation from thermodynamic data as +1.227 V. The extremely low exchange current density prevents direct determination of this value. The simultaneous transfer of four electrons in reaction (5.7.6) is highly improbable; thus the reaction must consist of several partial processes. The non-catalytic electroreduction of oxygen at a mercury electrode will now be compared to the catalytic reduction at a silver electrode. J. Heyrovsky demonstrated that the stable intermediate in the reduction at mercury is hydrogen peroxide. Figure 5.42 depicts the voltammogram (polarographic curve) for the reduction of oxygen at a dropping mercury electrode. The first wave corresponds to the reduction of oxygen to hydrogen peroxide and the second to the reduction

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Our measurements show that the fraction of azobenzene side group that are bound into micelles is most typically signi cantly smaller than 100% Fig 76a gives representative UV-visible spectra of azo-modi ed polymers in water, as a function of the concentration of surfactant The absorbance obviously increases and the main peak is red-shifted with increasing the surfactant concentration, two features that re ect the transfer of azobenzene from water into a less polar environment The presence of isobestic points betrays that the azo groups are either in contact with water or tightly bound to the surfactant and no intermediate solvatation state is detected (not shown) The absorbance at a xed wavelength indicates accordingly the degree of binding of the azobenzene groups In Fig 76b, the absorbance abruptly increases above the critical micelle concentration (Khoukh et al, 2007).

1.01

In the case of other nanoparticles, such as proteins or polymers of CDs, the absorbance increases immediately upon addition of the particles (Pouliquen et al, 2007; Pouliquen and Tribet, 2006) At incipient binding, the association was considered very tight and quantitative, and it has not been possible to estimate a binding constant (not shown) The association was presumably strengthened because of multipoint attachments (see later) A saturation plateau can be reached at high concentrations of the nanoparticles Once normalized by the concentration of azobenzene and a reference shift of extinction coef cient (eg, as measured with azobenzene in water and dodecane), the plateau value should indicate the fraction of bound chromophore In practice, the normalized plateau value depends on the integration level of the azobenzene and intrachain repulsion (as modulated by ionic strength in the case of our azo-modi ed polyelectrolyte).

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