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Composite charge distribution

From polarization curves the protectiveness of a passive film in a certain environment can be estimated from the passive current density in figure C2.8.4 which reflects the layer s resistance to ion transport tlirough the film, and chemical dissolution of the film. It is clear that a variety of factors can influence ion transport tlirough the film, such as the film s chemical composition, stmcture, number of grain boundaries and the extent of flaws and pores. The protectiveness and stability of passive films has, for instance, been based on percolation arguments [67, 681, stmctural arguments [69], ion/defect mobility [56, 57] and charge distribution [70, 71]. [Pg.2725]

On the electrode side of the double layer the excess charges are concentrated in the plane of the surface of the electronic conductor. On the electrolyte side of the double layer the charge distribution is quite complex. The potential drop occurs over several atomic dimensions and depends on the specific reactivity and atomic stmcture of the electrode surface and the electrolyte composition. The electrical double layer strongly influences the rate and pathway of electrode reactions. The reader is referred to several excellent discussions of the electrical double layer at the electrode—solution interface (26-28). [Pg.510]

Figure 3 A hydrophobic permeant must negotiate through a complex series of diffu-sional and thermodynamic barriers as it penetrates into a cell. The lipid and protein compositions and charge distribution of the inner and outer leaflets of the membrane lipid bilayer can play limiting roles, particularly at the tight junction. Depending upon the permeant s characteristics, it may remain within the plasma membrane or enter the cytoplasm, possibly in association with cytosolic proteins, and partition into cytoplasmic membranes. Figure 3 A hydrophobic permeant must negotiate through a complex series of diffu-sional and thermodynamic barriers as it penetrates into a cell. The lipid and protein compositions and charge distribution of the inner and outer leaflets of the membrane lipid bilayer can play limiting roles, particularly at the tight junction. Depending upon the permeant s characteristics, it may remain within the plasma membrane or enter the cytoplasm, possibly in association with cytosolic proteins, and partition into cytoplasmic membranes.
There was no change in the conductance, without HC1, in spite of an increase in the temperature of about 10°C due to sonication (Table 9.5b). The ultrasound seemed to have increased the molecular solvation, therefore the activity of SO4-ions did not increase but remained more and more solvated due to complex ionic composition and charge distribution on the SO4 ions (Fig. 9.1). [Pg.234]

Hence, trends in zAH control both the charge distributions and the NBO compositions of these species. [Pg.129]

The reason is that these alleged kp values are mostly composite, comprising the rate constants of propagation of uncomplexed Pn+, paired Pn+ (Pn+A ), and Pn+ complexed with monomer or polymer or both, without or with an associated A" [17]. Even when we will eventually have genuine kp values for solvents other than PhN02, it will not be possible to draw many (or any ) very firm conclusions because the only theoretical treatments of the variation of rate constants with solvent polarity for (ion + molecule) reactions are concerned with spherically symmetrical ions, and the charge distribution in the cations of concern to us is anything but spherically symmetrical. [Pg.488]

In exposures of humans to artificially generated aerosols, where the information is to be relevant to ambient aerosols, several factors are important the particle diameter distribution must be fairly constant and fall within size ranges typical for the given compound in the ambient air, the chemical composition of the aerosol must be stable and predictable, and the electric charge distribution of the aerosol must simulate that of normal atmospheric aerosols. [Pg.393]

In summary, the surface properties of fibers are influenced by the composition of the material, the environment during growth or generation, and the history of the particle. The term history refers to any changes in the surface after the fiber is formated. The charge or charge distribution affects the reactions of a fiber. [Pg.13]

The B3LYP and PWP electronic structures of the OTiCO insertion product appear to be very similar to the BP one [26]. The net charge distribution analysis shows a charge transfer between Ti and O in the Ti-0 bond, and inspection of the molecular orbitals reveals that only two molecular orbitals (15a and 5a") include contributions from all atoms while others have pure TiO or CO character. The composition of 15a and 5a" orbitals shows that the Ti-C bond arises from... [Pg.161]

This attempt at size adjustment between the two types of sheets is illustrated by the fact that very few Fe-rich 2 1 clays contain less than 0.2 tetrahedral R3+. When increased Al in the tetrahedral sheets is compensated by substitution of Mg in the octahedral sheet, the octahedral charge increases and the overall layer charge is increased. This allows strong K-bonds to be developed and exert an influence on layer dimensions. Once the layer charge is larger than 0.7 and predominantly tetrahedral in origin, the Al dominated octahedral sheet represents the stable phase such a clay approaches muscovite in composition and charge distribution and its stability is deter-... [Pg.182]


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