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Values Associated with Reactions - Equilibrium Calculations

The objective of this chapter is, by experimentation or computation, on the basis of the values of the main properties, to determine the value of the equilibrium constant of a reaction, or, which is the same thing by virtue of relation [4.2], that of the standard molar Gibbs energy associated with the [Pg.105]

We shall then examine the use of those values to caleulate eomplex equilibria, enabling us to define domains of stability of the phases and the compounds, domains of predominance of components, and to serve the ultimate goal of a transformation within the system. [Pg.105]

In this chapter, we only look at molecular reactions. Ionic equilibria will be studied in Volume 6 of this Set of books. [Pg.105]

In this section, we shall establish a certain number of thermod5mamic relations specific to the reactions, which will be useful to us in this chapter, particularly, for calculating the values. [Pg.105]

Remember that every time we attempt to determine an equilibrium constant, we need to begin by choosing the constant in question (see section 3.1.2) and the reference states. Remember that as a reference, we can choose [Pg.105]


Determination of the Values Associated with Reactions -Equilibrium Calculations... [Pg.105]

Determination of the Values Associated with Reactions - Equilibrium Calculations 137 We shall examine each of these five methods in turn. [Pg.137]

Equation 2.67 indicates that the standard enthalpy and entropy of reaction 2.64 derived from Kc data may be close to the values obtained with molality equilibrium constants. Because Ar// is calculated from the slope of In AT versus l/T, it will be similar to the value derived with Km data provided that the density of the solution remains approximately constant in the experimental temperature range. On the other hand, the error in ArSj calculated with Kc data can be roughly estimated as R In p (from equations 2.57 and 2.67). In the case of water, this is about zero for most solvents, which have p in the range of 0.7-2 kg dm-3, the corrections are smaller (from —3 to 6 J K-1 mol-1) than the usual experimental uncertainties associated with the statistical analysis of the data. [Pg.35]

The methods of experimental determination and the calculation of different values associated with chemical reactions (enthalpies, entropies, calorific capacities, free and constant equilibrium enthalpies) lead to complex equilibrium calculations and their graphical representations in various forms pole figures, generalized Ellingham diagrams, binary, tertiary and quaternary diagrams. [Pg.190]

The following assumptions are made (i) the activated complexes are in equilibrium with the reactants, (ii) the energy of a molecule is not altered when an activated complex is substituted for a nearest neighbour, and (iii) the products do not affect the course of reaction, except to define a boundary in surface processes. The various cases can be recognized from the magnitude of the pre-exponential term and calculated values [515] are summarized in Table 7. Low values of A indicate a tight surface complex whereas higher values are associated with a looser or mobile complex. [Pg.94]

Let us suppose that the acetic acid content of the final aqueous solution is 5%, corresponding to a ratio of approximately 1 mol of CH3COOH to 60 mol of H2O. As the yield of reaction 2.1 will be near 100% (recall that reaction 2.2 is rather exothermic, implying a very high equilibrium constant see section 2.9), the same value will be used for the molar ratio (H2 O) / n (C 2115OII), despite the increased total amount of substance of water in the reaction products. In the present case, the difference of 1 mol of water between the product and the reactant mixtures has a negligible enthalpic effect. The enthalpies associated with the solution of ethanol and acetic acid in 60 mol of water are derived from literature data [17] as Asin//(1) = -10.0 0.1 kJ mol-1 and Asin//(3) = —1.0 0.1 kJ mol-1. This calculation will be detailed in section 2.5. [Pg.11]

Experimental Determination of AG ° for ATP Hydrolysis A direct measurement of the standard free-energy change associated with the hydrolysis of ATP is technically demanding because the minute amount of ATP remaining at equilibrium is difficult to measure accurately The value of AG ° can be calculated indirectly, however, from the equilibrium constants of two other enzymatic reactions having less favorable equilibrium constants ... [Pg.131]

The total overpotential is the sum of these values, namely T] = 12.88 mV, of which only 0.05 mV (0.4%) is associated with the first step. Hence we can consider this step to be effectively at equilibrium. Thus we proceed to calculate the kinetic parameters for the reaction sequence, assuming that all steps other than the rate-determining step are at equilibrium. [Pg.391]

The earlier sections of this chapter discuss the mixed electrode as the interaction of anodic and cathodic reactions at respective anodic and cathodic sites on a metal surface. The mixed electrode is described in terms of the effects of the sizes and distributions of the anodic and cathodic sites on the potential measured as a function of the position of a reference electrode in the adjacent electrolyte and on the distribution of corrosion rates over the surface. For a metal with fine dispersions of anodic and cathodic reactions occurring under Tafel polarization behavior, it is shown (Fig. 4.8) that a single mixed electrode potential, Ecorr, would be measured by a reference electrode at any position in the electrolyte. The counterpart of this mixed electrode potential is the equilibrium potential, E M (or E x), associated with a single half-cell reaction such as Cu in contact with Cu2+ ions under deaerated conditions. The forms of the anodic and cathodic branches of the experimental polarization curves for a single half-cell reaction under charge-transfer control are shown in Fig. 3.11. It is emphasized that the observed experimental curves are curved near i0 and become asymptotic to E M at very low values of the external current. In this section, the experimental polarization of mixed electrodes is interpreted in terms of the polarization parameters of the individual anodic and cathodic reactions establishing the mixed electrode. The interpretation then leads to determination of the corrosion potential, Ecorr, and to determination of the corrosion current density, icorr, from which the corrosion rate can be calculated. [Pg.150]

If the initial oxygen/iron ratio is below the stoichiometric value, then some elemental iron will remain, in association with hematite and gaseous oxygen. The /02 for this assemblage would be 10 - bars (as calculated from the equilibrium constant for reaction (19.69) at 25°C). This is an interesting situation, because hematite and iron are thermodynamically metastable under these conditions with respect to magnetite. [Pg.527]

The enhanced velocities possessed by hot atoms dramatically shorten the time scales associated with nonthermal collisions. Approximate recoil F mean thermalization times, , corresponding to simulated MNR conditions have been calculated (4) using the local equilibrium steady-state hot atom kinetic theory (21,22,41). The values can be compared with the mean reactive lifetimes for thermal Reaction 5, , obtained from absolute and MNR sample composition data. At readily accessible moderator concentrations, the were shown to be tenfold or more larger than the , even for very reactive R species. A calculated [/] ratio of 160 was obtained for C2H6 present at 5.0 X lO" mol fraction in C2F6, showing that hot atom moderation is effectively completed prior to the onset of Reaction 5 in this system. [Pg.216]

It is tricky to experimentally determine the equilibrium conditions, so as much as possible, we use the calculation method to determine the values of the equilibrium constants (or standard Gibbs energies associated with the reactions). Those calculations must restrict the number of experiments as far as possible, or eliminate them altogether. [Pg.136]


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