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Free-energy change characterized

Before we will discuss the electrochemical system, it is important to define the properties and characteristics of each component, especially the electrolyte. In the following, we assume macroscopic amounts of an electrolyte containing various ionic and nonionic components, which might be solvated. In the case that this bulk electrolyte is in thermodynamic equilibrium, each of the species present is characterized by its electrochemical potential, which is defined as the free energy change with respect to the particle number of species i ... [Pg.131]

Almost all problems that require knowledge of free energies are naturally formulated or can be framed in terms of (1.15) or (1.16). Systems 0 and 1 may differ in several ways. For example, they may be characterized by different values of a macroscopic parameter, such as the temperature. Alternatively, they may be defined by two different Hamiltonians, 3%o and 3%, as is the case in studies of free energy changes upon point mutation of one or several amino acids in a protein. Finally, the definitions of 0 and 1 can be naturally extended to describe two different, well-defined macroscopic states of the same system. Then, Q0 is defined as ... [Pg.20]

The simplest way in which a process occurs by itself is when it is under thermodynamic control. The folding of a protein, or the self-assembly of micelles at the critical micelle concentration (cmc) are examples of spontaneous processes the latter are characterized by a negative free-energy change, as the self-orgaiuzed product has a lower energy than the single components. ... [Pg.86]

According to the theory of rubber elasticity, the elastic response of molecular networks is characterized by two mechanisms. The first one is connected with the deformation of the network, and the free energy change is determined by the conformational changes of the elastically active network chains. In the early theories, the free energy change on deformation of polymeric networks has been completely identified with the change of conformational entropy of chains. The molecular structure of the chains... [Pg.57]

Friedman and Krishnan, 1973b). As a result of overlap, some of the solvent co-sphere is displaced and if, for example, the effect of solute j on the solvent dominates the process of overlap, then the overlap can be represented as in Fig. 14(a), the change in the solvent being summarized by the reaction in Fig. 14(b). This mutually destructive overlap can be characterized by the free energy change, Aijt for the solvent reaction, where Ay is related to the thermodynamic energy, and entropy, by the expression A-, - — T. SSj. [Pg.240]

Different analytes are characterized by diverse standard free energy changes (AjU°) thus the dependence of Kle and Kgo on temperature is a function of analyte nature. The following Gibbs equation relates to AH° and AS°, that represent the standard enthalpy and entropy changes, respectively ... [Pg.118]

The second important quantity, the half-wave potential can be a measure of the standard free energy change (AG°) or free energy of activation AG ) associated with the electrolytic process. The value of the half-wave potential depends on the nature of the electroactive species, but also on the composition of the solution in which the electrolysis is carried out. If the composition of the solution electrolysed, consisting of the electroactive substance and a proper supporting electrolyte, often buffered, is kept constant, it is possible to compare the half-wave potentials of various substances. When the mechanism of the electrode process is similar for all compounds compared, the halfwave potential can be considered to be a measure of the reactivity of the compound towards the electrode. Hence the half-wave potentials are physical constants that characterize quantitatively the electrolysed compound, or the composition of the electrolyzed solution. In the application of polarography to reaction kinetics the half-wave potentials are of importance both for slow and fast reactions. For slow reactions a large difference in half-wave potentials makes a simultaneous determination of several components of the reaction mixture possible. In... [Pg.3]

Figure 32 Thermodynamic bases of the fluorescence switching behaviour illustrated in Figure 30. The eT process from the Ni " centre to the nearby photo-excited dansyl subunit (dns ) is characterized by a strongly negative free energy change ACj°eT = —1-93 eW, as calculated through the combination of pertinent photophysical and el ti -chemical quantities. On the other hand, the dns -to-Ni eT process is very disfavoured (AG°eT>0.68 eV). Figure 32 Thermodynamic bases of the fluorescence switching behaviour illustrated in Figure 30. The eT process from the Ni " centre to the nearby photo-excited dansyl subunit (dns ) is characterized by a strongly negative free energy change ACj°eT = —1-93 eW, as calculated through the combination of pertinent photophysical and el ti -chemical quantities. On the other hand, the dns -to-Ni eT process is very disfavoured (AG°eT>0.68 eV).
The Hansen characterization is usually considered a sphere, even although it is really a modified spheroid. The constant 4 in Equation 10.4 modifies the spheroid to a sphere. The cohesion energy parameters of those liquids where affinities are highest are located within the sphere. The center of the sphere has the values of the bpp, and parameters, taken as characteristic for the solute. This may not be quite true because of entropy effects. The radius of the sphere, R, reflects the condition where the free energy change, AG, for the process being considered is zero. This is discussed here in terms of the mixing process, for which reason the superscript M is used. The entropy effects, and enthalpy effects, ATP, are in balance. Thus, on the sphere surface... [Pg.547]


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