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Results from Thermodynamic Data

The standard molar Gibbs energies of transfer of an ion from a source solvent (arbitrarily selected as water, W) to a target solvent, A, G (I, W S), described in Section 4.3.2.1, is the basis for a rough estimation of its preferential solvation in mixtures of these two components. However, the mutual interactions of the two [Pg.210]

Such standard transfer data pertain to infinite dilution of the ions in the solvent mixtures so that the ions dealt with are surrounded by the components of the mixture and are remote from other ions. Several methods have been applied to A jG (l, W - W + S) = f(Xs) data (or the corresponding enthalpies of transfer) to obtain from them the preferential solvation of the ion by the components of the binary solvent mixture. [Pg.211]

The quasi-chemical part of the model considers the numbers of neighboring particles and according to Guggenheim [69]  [Pg.211]

The QLQC expression for the binary solvent mixture is similar to Equation 6.12 and results in the value of as a function of the solvent composition  [Pg.212]

The quantity evp(e Jk T) is obtained from the molar excess Gibbs energy of mixing in the equimolar solvent mixture [68]  [Pg.212]


Turkevich who established the first reproducible standard procedure for the preparation of metal colloids [44] also proposed a mechanism for the stepwise formation of nanoclusters based on nucleation, growth, and agglomeration [45,46]. This model, refined by data from modern analydical techniques and results from thermodynamic and kinetic studies, is in essence stiU valid today (Figure 2) [82]. [Pg.22]

Principal component regression (PCR) is an extension of PCA with the purpose of creating a predictive model of the Y-data using the X or measurement data. For example, if X is composed of temperatures and pressures, Y may be the set of compositions that results from thermodynamic considerations. Piovoso and Kosanovich (1994) used PCR and a priori process knowledge to correlate routine pressure and temperature measurements with laboratory composition measurements to develop a predictive model of the volatile bottoms composition on a vacuum tower. [Pg.35]

Many molecules are composed of functional groups (hat can rotate with respect to the rest of the molecule. The classical example is ethane, as the possibility of rotation of one methyl group against the other was recognized long ego. Because the torsional mode does not result in infrared activity, its frequency was estimated from thermodynamic data. [Pg.125]

The standard potential of the Na+/Na couple can be obtained from these emf values. However, it can also be obtained by calculation from thermodynamic data [2] and the result agrees well with the result by emf measurement. [Pg.89]

For a further verification of this conclusion, we determined equilibrium constant, K, by combining the results of kinetic measurements in the region of r+ > r and in the region of r+ < r, having assumed that v = 1. The agreement of the obtained value with the value known from thermodynamic data (K = 0.0364 atm2 at 530°Q has confirmed that v = 1. This result means that stoichiometric numbers of all nonequilibrium stages of the reaction equal unity. [Pg.246]

The most common approach used by geochemical modeling codes to describe the water-gas-rock-interaction in aquatic systems is the ion dissociation theory outlined briefly in chapter 1.1.2.6.1. However, reliable results can only be expected up to ionic strengths between 0.5 and 1 mol/L. If the ionic strength is exceeding this level, the ion interaction theory (e.g. PITZER equations, chapter 1.1.2.6.2) may solve the problem and computer codes have to be based on this theory. The species distribution can be calculated from thermodynamic data sets using two different approaches (chapter 2.1.4) ... [Pg.67]

The relationships of Equations 5 and 2 are unquestionably valid for unlimited surface coverage on ideal external open (flat, planar, accessible) surfaces ranging from nil at E to infinity at E=0. All of the inherent assumptions (tabulated above) are equally valid as models for physical adsorption in internal constricted regions. These are classically denoted as ultramicropores ( 2 nm), micropores(<2 nm), mesopores (2<1000nm) and macropores (very large and difficult to define with adsorption isotherm). In these instances there are finite concentration limits corresponding to the volume (space, void) size domain(s). Although caution is needed to deduce models from thermodynamic data, we can expect to observe linear relationships over the respective domains. The results will be consistent with, albeit not absolute proof of the models. [Pg.277]

This discussion of the data in Table II demonstrates the importance of obtaining enthalpies and entropies of reaction to gain an understanding of the nature of chelate ring formation in aqueous solution. In the absence of absolute structural proofs, the number of chelate rings formed in solution can only be inferred from thermodynamic data. The examples in Table II show that the ideas resulting from stability data alone may be misleading and can lead to different conclusions than one would draw on the basis of more complete thermodynamic data. [Pg.288]

Therefore the aim of this paper is to calculate the KBIs for aqueous solutions of alcohols from thermodynamic data, to compare the results to those obtained from SAXS measurements, and to examine some specific featmes regarding the structure of aqueous alcohol solutions. [Pg.3]

Models to predict migration data have been developed. (1-4) The available models assume that water intrudes the repository, acts to release the radioactivity by leaching, and transports the radioactivity through the surrounding media to the biosphere. Potential changes in waste properties that result from thermodynamic and kinetic effects are not considered in present models. [Pg.11]

Figure 10 shows the nucleaiity dependence of silver cluster redox potential in water together with the data just presented, the previously published values are reported forn = 1 (3), 2 (23), 5 (5), 10 (24), and 11 (25). The E° values for nuclearities n = 1 and n = 2 resulted from thermodynamic calculations. The value for n = 10 was obtained from electron transfer studies where the clusters were the donor and were corroded by HaO. As a function of the... [Pg.308]

This reaction results in an equilibrium potassium vapor pressure (calculated from thermodynamic data) of 0.714 torr above the LiCl-KCl eutectic at 427°C (700°K). Metallic lithium is rapidly lost, by Reaction 1, from the lithium electrode in open cells exposed to an inert atmosphere of helium (3). However, this reaction has not been evident in hermetically sealed cells. [Pg.195]

The n-pentyl radical is the largest alkyl radical for which Arrhenius parameters have been determined for a gas-phase metathetical reaction. Problems with volatility of reactants and dimer products are considerable in studies involving radicals larger than C4. The few results available for n-pentyl are given in Table 21. but in fact for only the first of the four reactions listed was there an experimental determination the other three results were obtained from data for the reverse reactions and the equilibrium constants derived from thermodynamic data. The selection of the rate coefficient for the n-pentyl dimerization reaction, upon which to base the absolute data for the reaction... [Pg.69]

According to the limitation stated above, our standard functions /u. = pI, T) depend only on temperature and therefore also equilibrium constants depend on temperature only and by (4.474) give restrictions on the values of activities a° in chemical equilibrium (denoted by superscript cf. Sect.4.7). Equations (4.473) and (4.474) permit calculations of chemical equilibria KLp may be calculated from the right-hand side of (4.473) (e.g. from thermodynamic data for pure constituents if they are taken as the standard state) and composition of equilibrium mixture is restricted by (4.474) if we know the relation of activities to composition simple results follow for important case (4.469), which will be used below (4.475). [Pg.249]

Following are descriptions of the preferential solvation in a large variety of binary solvent mixtures, in terms of the preferential solvation parameters. These have been determined mostly by the present anthor, either from KBIs calculated by him from thermodynamic data or from those calculated by other authors. The sources of the thermodynamic data that have been employed for obtaining them are listed in the papers quoted. In the present context, only the results of the application of the fluctuation theory are presented, so that detailed discussions of the chemistry involved in the preferential solvation that was noted for the mixtures dealt with here should be sought in the publications quoted. The temperatures quoted in the following are rounded to integer values. [Pg.70]

Table 1 summarizes some of the most relevant results from thermodynamic studies on platinum single-crystal surfaces. In order to facilitate the comparison of thermodynamic data corresponding to different adsorption reactions, values of the thermodynamic properties at the standard state ( AG , A/T and AS ) are provided. Values of the lateral interaction parameter (a>), and its temperature dependence (dm/dT) are also given in Table 1. While the lateral interaction parameter measures the magnitude of the lateral interactions, its temperature dependence reflects the entropic contributions to the lateral interactions. Therefore, the enthalpic contribution to the lateral interaction energy, can be obtained from - T da/dT. Table 1 summarizes some of the most relevant results from thermodynamic studies on platinum single-crystal surfaces. In order to facilitate the comparison of thermodynamic data corresponding to different adsorption reactions, values of the thermodynamic properties at the standard state ( AG , A/T and AS ) are provided. Values of the lateral interaction parameter (a>), and its temperature dependence (dm/dT) are also given in Table 1. While the lateral interaction parameter measures the magnitude of the lateral interactions, its temperature dependence reflects the entropic contributions to the lateral interactions. Therefore, the enthalpic contribution to the lateral interaction energy, can be obtained from - T da/dT.
The effective charges of the penta- and hexa valent actinyl ions were estimated from thermodynamic data using an extended Born equation (Choppin 1983b, Choppin and Rao 1984). The results obtained were +2.0, +3.3, +3.1 and +3.0 for NpOj", UO ... [Pg.563]


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