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Free energy variation with temperature

Free energy variations with temperature can also be used to estimate reaction enthalpies. However, few studies devoted to the temperature dependence of adsorption phenomena have been published. In one such study of potassium octyl hydroxamate adsorption on barite, calcite and bastnaesite, it was observed that adsorption increased markedly with temperature, which suggested the enthalpies were endothermic (26). The resulting large positive entropies were attributed to loosening of ordered water structure, both at the mineral surface and in the solvent surrounding octyl hydroxamate ions during the adsorption process, as well as hydrophobic chain association effects. [Pg.144]

The most useful expression for describing the variation of standard Gibbs free energy changes with temperature is ... [Pg.8]

The variation in Gibbs-free-energy change with temperature at constant pressure is given by... [Pg.239]

The Gibbs-Helmholtz equation equation gives us the variation of the change in Gibbs free energy, AG, with temperature T. An important part of its derivation requires the differentiation of the quantity AG/T. It is important to reahse that AG does depend upon T, so that this is an example of differentiating a quotient. If AG did not vary with temperature, then the task would be simpler... [Pg.128]

Improved theoretical models for ionic hydration and the variations with temperature of the solvating properties of water so that the free energies can be more accurately extrapolated to elevated temperatures. These models must progress from simple monovalent ions to polyvalent and complex ions, e.g. Cs+, Sr +, Pu " ", ions of Tc, I, etc. [Pg.341]

Thermodynamic calculation results are shown in Table 4.1. For reaction (5), the main parameters are the following free energy variation 5165 kJ, equilibrium constant at 600 °C 3.4 10-3 and the reagent conversion to reaction products is negligibly low. Much less favorable is the equilibrium state in the reaction (6). Therefore, both reactions are not practically executed. Reaction (6) described in the monograph by Zeldovich el al. [39] and in the article by Anbar [40] runs at a temperature above 1273 K with nitric oxide formation by the mechanism, which includes elementary stages with atomic oxygen participation. However, atomic... [Pg.98]

The standard free energy of formation ( AG ) of a compound varies with temperature. The variation with temperature is usually presented by means of a table or some simple equations like... [Pg.127]

FIG. 15 Linear variation of adsorption free energy, —AGa, with experimental temperatures (°Q, measured at infinite dilution. [Pg.431]

The variation of free energy change with variation of temperature and pressure may now be considered G = H-TS since H = V + PV G = U+ PV-TS Upon differentiation this gives... [Pg.3]

Fig. 7.5.3. Variation of the Landau free energy density with the order parameter at temperatures above, at, and below the critical temperature and for changes in direction of the magnetic fields. The heavy dots indicate the value of i) for which the Landau free enei density is minimized. The central row represents a discontinuous first order transition as the temperature is dropped past the its critical value. After Goldenfeld loc. cit. Fig. 7.5.3. Variation of the Landau free energy density with the order parameter at temperatures above, at, and below the critical temperature and for changes in direction of the magnetic fields. The heavy dots indicate the value of i) for which the Landau free enei density is minimized. The central row represents a discontinuous first order transition as the temperature is dropped past the its critical value. After Goldenfeld loc. cit.
Figure 4. Variation with temperature of the complete set of elastic constants for LaPsOn at the mmm < Hm transition (from Carpenter and Salje 1998, after Errandonea 1980). Solid curves are solutions derived from a Landau free energy expansion for a pseudo proper ferroelastic transition. Figure 4. Variation with temperature of the complete set of elastic constants for LaPsOn at the mmm < Hm transition (from Carpenter and Salje 1998, after Errandonea 1980). Solid curves are solutions derived from a Landau free energy expansion for a pseudo proper ferroelastic transition.
Pound RV, Rebka Jr. JA (1960) Variation with temperature of the energy of recoil-free gamma rays from solids. Phys Rev Lett 4 274-277... [Pg.258]

A different approach was made by Dyre et al. (1996) to account for the experimental viscosity variations with temperature as an alternative to VTF and AG models. They considered the flow in viscous liquids to arise from sudden events involving motion and reorganization of several molecules. From the viewpoint of mechanism, the energy required for such flow is minimized if the surrounding liquid is shoved aside to create the necessary volume for rearrangement. This volume is fundamentally different from the volume of the free volume theory and is, in principle, an activation volume. The free energy involved may be written as... [Pg.118]

Of further concern is the possibility that the interfacial free energy associated with the basal plane, a basic assumption in the analysis, may not be constant with crystallization temperature. The change in the crystallization temperature, in practice, gives the variation in crystallite thickness. Because... [Pg.224]

Variation of the Landau free energy density with the order parameter at temperatures above, at, and below the criticai temperature and for changes in direction of the magnetic fields. The heavy dots indicate the value of tj... [Pg.398]

Depiction of a first order transition in terms of the variation of the Landau free energy density with the order parameter at several reduced temperatures. For details see text. Reproduced from N. Goldenfeld, Lectures on Phase Transitions and the Renormalization Group, Copyright (c) July 21, 1992 reprinted with permission of Westview Press of the Perseus books Group. [Pg.400]

To locate the nematic-isotropic transition it is necessary to determine the temperature dependence of the free energy but this is not possible without making further approximations concerning the temperature variation of the segmental interaction parameters X. and This variation with temperature results primarily through their dependence on the orientational order of the system. A rigorous derivation of this dependence is extremely difficult and so we adopt a semi-intuitive approach. As we have seen, the orientational order in a mesophase is characterized by an infinite set of order parameters but the most important of these are the second-rank order parameters, at least close to the nematic-isotropic transition. Indeed for cylindrically symmetric particles both theory and experiment agree that the potential of mean torque is proportional to When the mesophase... [Pg.125]

Figure 11.1 Variation with temperature of the Gibbs free energy per unit volume. Figure 11.1 Variation with temperature of the Gibbs free energy per unit volume.

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See also in sourсe #XX -- [ Pg.64 ]




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