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Films structure reduction

Another point of importance about the film structure is the degree to which it can be permeated by various ions and molecules. It is of course essential that supporting electrolyte ions be able to penetrate the film, else the electrical double layer at the electrode/polymer interface could not be charged to potentials that drive electron transfers between the polymer and the electrode. The electroneutrality requirements of porphyrin sites as their electrical charges are changed by oxidation or reduction also could not be satisfied without electrolyte permeation. With the possible exception of the phenolic structure in Fig. 1, this level of permeability seems to be met by the ECP porphyrins. [Pg.412]

Electrochemical deposition of lithium usually forms a fresh Li surface which is exposed to the solution phase. The newly formed surface reacts immediately with the solution species and thus becomes covered by surface films composed of reduction products of solution species. In any event, the surface films that cover these electrodes have a multilayer structure [49], resulting from a delicate balance among several types of possible reduction processes of solution species, dissolution-deposition cycles of surface species, and secondary reactions between surface species and solution components, as explained above. Consequently, the microscopic surface film structure may be mosaiclike, containing different regions of surface species. The structure and composition of these surface films determine the morphology of Li dissolution-deposition processes and, thus, the performance of Li electrodes as battery anodes. Due to the mosaic structure of the surface... [Pg.310]

The partial W reduction is not only obtained at the metal-metal oxide or at the metal oxide-electrolyte interface, but the oxide turns blue immediately throughout the whole layer. This proves the above statement concerning the macromolecular film structure. [Pg.125]

Reduction of the vapor transmittance of latex films as a result of vibrowave influences on the latex, measured by diffusion method, also confirms the change of a film structure under the influence of nonlinear vibrations [8], It is necessary to emphasize, that the influence of vibrowave treatment observed already at a stage of synthesis of polymers [14] is efficient at the subsequent stages of formation of a complex of properties of polymeric composite materials. [Pg.375]

Figure 3 shows typical TEM pictures of such gold colloid containing block copolymer films which were obtained after reduction of PS-b-PEO/LiAuCU complexes in toluene either by BHs/methanol or by N2H4(aq). It was generally observed that reduction with BHs/methanol led to bimodal products containing very small (1.5 nm) and larger (ca. 15 nm) particles in each micelle core (Figure 3A). In contrast, reduction with hydrazine hydrate led to particles with sizes mostly between 6 and 15 nm (Figure 3B). Size and location of the particles was, however, not directly related to a micellar film structure. Figure 3 shows typical TEM pictures of such gold colloid containing block copolymer films which were obtained after reduction of PS-b-PEO/LiAuCU complexes in toluene either by BHs/methanol or by N2H4(aq). It was generally observed that reduction with BHs/methanol led to bimodal products containing very small (1.5 nm) and larger (ca. 15 nm) particles in each micelle core (Figure 3A). In contrast, reduction with hydrazine hydrate led to particles with sizes mostly between 6 and 15 nm (Figure 3B). Size and location of the particles was, however, not directly related to a micellar film structure.
Paulik, M. G., P. A. Brooksby, A. D. Abell, and A. J. Downard. Grafting aryl diazonium cations to polycrystalline gold Insights into film structure using gold oxide reduction, redox probe electrochemistry, and contact angle behavior. J. Phys. Chem. C 111, 2007 7808-7815. [Pg.208]

While Eq. III-18 has been verified for small droplets, attempts to do so for liquids in capillaries (where Rm is negative and there should be a pressure reduction) have led to startling discrepancies. Potential problems include the presence of impurities leached from the capillary walls and allowance for the film of adsorbed vapor that should be present (see Chapter X). There is room for another real effect arising from structural peiturbations in the liquid induced by the vicinity of the solid capillary wall (see Chapter VI). Fisher and Israelachvili [19] review much of the literature on the verification of the Kelvin equation and report confirmatory measurements for liquid bridges between crossed mica cylinders. The situation is similar to that of the meniscus in a capillary since Rm is negative some of their results are shown in Fig. III-3. Studies in capillaries have been reviewed by Melrose [20] who concludes that the Kelvin equation is obeyed for radii at least down to 1 fim. [Pg.54]

In general there are two factors capable of bringing about the reduction in chemical potential of the adsorbate, which is responsible for capillary condensation the proximity of the solid surface on the one hand (adsorption effect) and the curvature of the liquid meniscus on the other (Kelvin effect). From considerations advanced in Chapter 1 the adsorption effect should be limited to a distance of a few molecular diameters from the surface of the solid. Only at distances in excess of this would the film acquire the completely liquid-like properties which would enable its angle of contact with the bulk liquid to become zero thinner films would differ in structure from the bulk liquid and should therefore display a finite angle of contact with it. [Pg.123]

BM Structure, composition, and properties should be similar and (4) the FM-containing elements should be able to bring about chemical reduction/decomposition or physical removal of BM oxide film. [Pg.243]

Here Pyj is the structure factor for the (hkl) diffiaction peak and is related to the atomic arrangements in the material. Specifically, Fjjj is the Fourier transform of the positions of the atoms in one unit cell. Each atom is weighted by its form factor, which is equal to its atomic number Z for small 26, but which decreases as 2d increases. Thus, XRD is more sensitive to high-Z materials, and for low-Z materials, neutron or electron diffraction may be more suitable. The faaor e (called the Debye-Waller factor) accounts for the reduction in intensity due to the disorder in the crystal, and the diffracting volume V depends on p and on the film thickness. For epitaxial thin films and films with preferred orientations, the integrated intensity depends on the orientation of the specimen. [Pg.203]


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See also in sourсe #XX -- [ Pg.317 , Pg.318 , Pg.319 ]




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