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Electrolyte theory

The region of the gradual potential drop from the Helmholtz layer into the bulk of the solution is called the Gouy or diffuse layer (29,30). The Gouy layer has similar characteristics to the ion atmosphere from electrolyte theory. This layer has an almost exponential decay of potential with increasing distance. The thickness of the diffuse layer may be approximated by the Debye length of the electrolyte. [Pg.510]

Thermodynamics of charge carriers weak electrolyte theory... [Pg.84]

Such a chemical approach which links ionic conductivity with thermodynamic characteristics of the dissociating species was initially proposed by Ravaine and Souquet (1977). Since it simply extends to glasses the theory of electrolytic dissociation proposed a century ago by Arrhenius for liquid ionic solutions, this approach is currently called the weak electrolyte theory. The weak electrolyte approach allows, for a glass in which the ionic conductivity is mainly dominated by an MY salt, a simple relationship between the cationic conductivity a+, the electrical mobility u+ of the charge carrier, the dissociation constant and the thermodynamic activity of the salt with a partial molar free energy AG y with respect to an arbitrary reference state ... [Pg.85]

The first attempt to apply microscopic electrolyte theory to study the mobility of protons in PEMs is due to Paddison and co-workers.Because the... [Pg.407]

Resibois, P. M. V. Electrolyte Theory An Elementary Introduction to a Microscopic Approach Harper and Row New York, 1968. [Pg.437]

So far, the discussion of concentrated electrolyte solutions has presumed that ionic relaxation is complete and so is a static correction. Dynamic electrolyte theories are still in their infancy and, in view of the rate of ionic relaxation compared with chemical reaction rates for dilute electrolytes (Sect. 1.6), such effects are probably not very important in concentrated electrolyte solutions containing reactants. The Debye— Falkenhagen [92] theory predicts a change in the relaxation time of electrolyte solutions with concentration, though experimental confirmation is scant [105]. At very high concentrations, small changes in the relaxation time ( 25%) of solvent relaxation can be identified (see also Lestrade et al. [106]). [Pg.60]

We turn now to attempts that aim at an understanding of density and charge fluctuations in ionic fluids. It is fair to say that the extension of conventional electrolyte theories to allow for a description of fluctuations forms one of the major recent achievements in theories of ionic criticality. [Pg.44]

A major ingredient for an RG treatment is a simple and transparent characterization of the molecular forces driving phase separation. This situation calls for mean-field theories of the ionic phase transition. The past decade has indeed seen the development of several approximate mean-field theories that seem to provide a reasonable, albeit not quantitative, picture of the properties of the RPM. Thus, the major forces driving phase separation seem now to be identified. Moreover, the development of a proper description of fluctuations by GDH theory has gone some way to establish a suitable starting point for RG analysis. Needless to say, these developments are also of prime importance in the more general context of electrolyte theory. [Pg.56]

In conclusion, we suggest that the ion dispersion forces were ignored by most (but by no means all) electrolyte theories mainly because they are important only for separations between ions smaller than about 5 A, and the interactions at these distances are not well-known. It is hard to believe that at these distances the interactions can be accurately described by a sum between a hard-wall repulsion, a Coulomb interaction, and a London attraction. Even if the latter would be true, a correction in the local dielectric constant (because of incomplete screening by water molecules) would render again the van der Waals interactions negligible, up to distances of the order of ion diameters. [Pg.445]

Barthel, J. J. Temperature dependence of the properties of electrolyte solutions I a semi-phenomenological approach to an electrolyte theory including short range forces. Ber. Bunsen Ges. Phys. Chem. 1979, 83, 252-257. [Pg.24]

Unfortunately, electrolyte theories which include higher terms must introduce additional parameters for ion sizes and repulsive forces. As yet, none of the theories developed appears capable of making a priori predictions of ion-ion interactions for the higher-valence ions or m the more concentrated solutions. In addition, they lead to unwieldy expressions, which makes their application very tedious (Scatchard, loc. ciL) and, in view of the assumptions included in these theories, of dubious value. [Pg.528]

An important concept that aided in the development of electrolyte theory was the ionic strength, I, introduced by Lewis and Randall (1921) ... [Pg.2300]

The nature of esters or ethereal salts has been fully discussed already in connection with the esters of inorganic acids and alcohols (p. 102). The name salts applies because they are formed by neutralizing an alcohol, acting as a base, with an acid. It must be emphasized, however, that in so terming these compounds salts we do not mean this to apply in a physical chemical sense as describing their properties in solution in accordance with the electrolytic theory of ionic dissociation. We are dealing here with questions of composition and constitution. Ethereal salts differ from metal salts, at least as to the degree of their dissociation into ions when in solution. [Pg.140]

Two properties render electrolyte theories difficult, namely the long-range nature of the Coulomb interactions and the high figures of the Coulomb energy at small ion separations. [Pg.173]

Experiment 2 Molar Conductivity Measurements Considering Arrhenius s electrolytic theory of dissociation, Werner noted that evidence for his coordination theory may be obtained by determining the electrolytic conductivity of the metal complexes in solution. Werner and Jprgensen assumed that acid (ionic) residues bound directly to the metal would not dissociate and would thus behave as nonconductors, while those loosely held would be conductors. Molar conductivities of 0.1 molar percent aqueous solutions of some tetravalent platinum and trivalent cobalt ammines are given in Table 2.3. [Pg.27]


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See also in sourсe #XX -- [ Pg.17 ]




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