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irradiation with 344 nm to reach the trans-cis photostationary state The absorption at the 351-nm band progressively increased with time and the absorption at the 450-nm band decreased with time, indicating the cis-trans thermal isomerization The rate constants were determined according to the rstorder kinetics that ts the experimental data very well There was a small change in the rate constants, that is, from AzoG0 to AzoG3 the rate constants of the cistrans thermal isomerization decreased from 33 10 6 s 1 to 26 10 6 s 1 After the azodendrimers were tethered to the pore walls of the MCM-41 materials, the rate constants of the cis-trans back isomerization were investigated using a similar method The size of the dendrons showed a signi cant effect on the rate constants The AzoG0 dendron with the smallest size exhibited the fastest reverse isomerization (10.

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Metal-solution interfaces lend themselves to the exact study of the double layer better than other types because of the possibility of varying the potential difference between the phases without varying the composition of the solution. This is done through the use of a reference electrode and a potentiometer which fixes the potential difference in question. In favourable cases there is a range of potentials for which a current does not flow across the interface in a system of this kind, the interface being similar to a condenser of large specific capacity. The capacity of this condenser gives a fairly direct measure of the electronic charge on the metallic surface, and this, in turn, leads to other information about the double layer. No such convenient and informative procedure is possible with other types of interfaces. D. C. Grahame, 1947

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2 10 6 s 1), whereas the bulkier AzoG3 dendron had the slowest reaction (26 10 6 s 1) This result is not surprising because the smaller AzoG0 has more freedom to isomerize within the con ned space of the MCM-41 materials The azobenzene derivatives require an extra volume of at least 127 A3 to undergo complete isomerization (Victor and Torkelson, 1987) For the bulky AzoG3 dendron, the con ned space hinders the conformational change of the azobenzene ligands The thermal cis-trans isomerization of the azobenzene ligands con ned in the nanopores has a constant rate constant and exhibits faster isomerization than in solution with the exception of the bulky AzoG3 dendrimer This result is consistent with Brinker and coworkers observation of azobenzene-modi ed nanoporous silica lms and supports their two-rate-constant physical model The nanoporous silica materials prepared by Brinker and coworkers have a cubic (BCC) pore structure.

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In the interphase the cohesion forces binding the individual particles together in the bulk of each condensed phase are significantly reduced. Particles that had a certain number of nearest neighbours in the bulk of the phase have a smaller number of such neighbours at the interface. However, particles from the other phase can also become new neighbours. This change in the equilibrium of forces affecting particles at the interface can lead to a new lateral force, termed the interfacial tension. In addition, the interphase usually has different electrical properties than the bulk phase. The situation becomes relatively simple when the phase is electrically charged. The free charge is then centred in the interphase. Orientation of dipoles in the interphase can also lead to a change in the electrical properties. Further charges can enter the interphase through adsorption of ions and/or dipoles. Excess charge in the interphase resulting from the presence of ions, electrons and dipoles produces an electric field. The region in which these charges are present is termed the electrical double layer. The presence of electrical charge affects the interfacial tension in the interphase. If one of the phases considered is a metal and the other is an electrolyte solution, then the phenomena accompanying a change in the interfacial tension are included under the term of electrocapillarity. While the formation of an electrical double layer at interfaces is a general phenomenon, the electrode-electrolyte solution interface will be considered 198

199 first If the electrode has a charge of <2(m), then this charge is distributed uniformly over the interface with the solution If part of the electrode is not immersed in the solution and is in contact with the air, then the portion of the charge corresponding to the surface in contact with the air is negligible, as this interface has minute capacitance The great majority of the charge is located at the metal-solution interface Excess charge in the metal <2(m) must be compensated in the solution by a charge of the same magnitude but of opposite sign This charge is attracted from the solution by electrostatic forces The general relationship e(m) + G(s) = 0 (41.

The azobenzene ligands positioned on the pore connections have different local environments from those positioned on the spherical pore surfaces Thus the azobenzene ligands isomerize at two different rates fast and slow The MCM-41 nanoporous materials prepared by Zink and coworkers have a hexagonal array pore structure in which all the azobenzene ligands positioned on the channel surfaces have the same local environment Thus simple one-rateconstant rst-order kinetics is suf cient to describe the isomerization process 13323 Photoisomerization of Bridged Azobenzene Ligands in Mesoporous Silica Materials Corriu and coworkers found that for thin lm samples using P123 surfactant templates, BSPA incorporated into a silica matrix exhibited similar reversible photoisomerization to that in solution (Besson et al, 2005).

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